From a90f9247571e75c236a5edfc790bfc63f341f9f8 Mon Sep 17 00:00:00 2001 From: Raul Bravo Date: Wed, 10 Jan 2024 14:33:47 +0100 Subject: [PATCH] Adding all files for generating paper results (in branch) --- .../Untitled-checkpoint.ipynb | 74 + ...cationKratosStructuredMeshWorkingRicc.mdpa | 0 .../Example1/Affine/ProblemFiles/FOM.py | 280 + .../Affine/ProblemFiles/FOM_TestTrajectory.py | 164 + .../Affine}/ProblemFiles/FluidMaterials.json | 0 .../ProblemFiles/HROM_TestTrajectory.py | 126 + .../ProblemFiles/ProjectParameters.json | 162 + .../Affine/ProblemFiles/ROM_TestTrajectory.py | 144 + .../Example1/Affine/ProblemFiles/Run_HROM.py | 97 + .../Example1/Affine/ProblemFiles/Run_ROM.py | 272 + .../Affine/ProblemFiles/TrainHROM_Step1.py | 90 + .../Affine/ProblemFiles/TrainHROM_Step2.py | 76 + .../Affine/ProblemFiles/analytic_mapping.py | 65 + .../ProblemFiles/overlapping_strategies.py | 323 + .../ProblemFiles/simulation_trajectories.py | 50 + .../ProblemFiles/test_ALE_ROM_stage4.py | 128 + 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rom_application/ContractionExpansionChannel/SelectedResults/Example_4/FFD_RBF/y_velocity_ROM_1e-06.npy create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/FFD_RBF/y_velocity_ROM_test_0.0001.npy create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/FFD_RBF/y_velocity_ROM_test_0.001.npy create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/FFD_RBF/y_velocity_ROM_test_1e-05.npy create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/FFD_RBF/y_velocity_ROM_test_1e-06.npy create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/hysteresis_rom_vs_hrom_0.0001_test.pdf create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/hysteresis_rom_vs_hrom_0.001_test.pdf create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/hysteresis_rom_vs_hrom_1e-05_test.pdf create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/hysteresis_rom_vs_hrom_1e-06_test.pdf create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/Example_4/plot_results.py create mode 100644 rom_application/ContractionExpansionChannel/SelectedResults/launch_plots.py diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/.ipynb_checkpoints/Untitled-checkpoint.ipynb b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/.ipynb_checkpoints/Untitled-checkpoint.ipynb new file mode 100644 index 00000000..73bc0b45 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/.ipynb_checkpoints/Untitled-checkpoint.ipynb @@ -0,0 +1,74 @@ +{ + "cells": [ + { + "cell_type": "code", + "execution_count": null, + "id": "bbeaaa45", + "metadata": {}, + "outputs": [], + "source": [ + "# Copy the RomPython folder to your own drive and run this cell to use the notebook in google colab\n", + "\n", + "from google.colab import drive\n", + "drive.mount('/content/drive/')" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "a2a6c2f6", + "metadata": {}, + "outputs": [], + "source": [ + "!pip install KratosMultiphysics\n", + "!pip install KratosRomApplication\n", + "!pip install KratosStructuralMechanicsApplication\n", + "!pip install KratosLinearSolversApplication\n", + "!pip install KratosConstitutiveLawsApplication" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "af25d338", + "metadata": {}, + "outputs": [], + "source": [ + "from KratosMultiphysics.StructuralMechanicsApplication.structural_mechanics_analysis import StructuralMechanicsAnalysis\n", + "from KratosMultiphysics.RomApplication.rom_testing_utilities import SetUpSimulationInstance\n", + "import KratosMultiphysics" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "98750e24", + "metadata": {}, + "outputs": [], + "source": [ + "with open(\"/content/drive/MyDrive/WinterSchool2023_Examples_test/stanford_bunny/ProjectParameters.json\",'r') as parameter_file:\n", + " parameters = KratosMultiphysics.Parameters(parameter_file.read())\n", + "model = KratosMultiphysics.Model()\n", + "simulation = StructuralMechanicsAnalysis(model,parameters)\n", + "simulation.Run()" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "e5bd6eb5", + "metadata": {}, + "outputs": [], + "source": [] + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 3", + "language": "python", + "name": "python3" + } + }, + "nbformat": 4, + "nbformat_minor": 5 +} diff --git a/rom_application/ContractionExpansionChannel/Affine_Mapping/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc.mdpa b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc.mdpa similarity index 100% rename from rom_application/ContractionExpansionChannel/Affine_Mapping/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc.mdpa rename to rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc.mdpa diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FOM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FOM.py new file mode 100644 index 00000000..0d10f137 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FOM.py @@ -0,0 +1,280 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis + +import json + +import numpy as np + +#for checking if paths exits +import os + +#importing training trajectory +from simulation_trajectories import TrainingTrajectory + + + +class FOM_Class(FluidDynamicsAnalysis): + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.control_point = 538 #a node around the middle of the geometry to capture the bufurcation + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.time_step_solution_container = [] + self.reynolds_number_container = [] + + + def InitialMeshPosition(self): + self.training_trajectory = TrainingTrajectory(self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble()) + self.w = self.training_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.InitialMeshPosition() + + + + def MovePart(self, part_name, jacobian, centering_vector, extra_centering): + x_original = [] + y_original = [] + # first loop + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(1,-1) + y_original = np.array(y_original).reshape(1,-1) + matrix_of_coordinates = np.r_[x_original, y_original] + modified_matrix_of_coordinates = np.linalg.inv(jacobian) @ (matrix_of_coordinates - centering_vector) + modified_matrix_of_coordinates += centering_vector + extra_centering #re-locating + # second loop + i = 0 + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = modified_matrix_of_coordinates[0,i] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = modified_matrix_of_coordinates[1,i] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + # node = self.model.GetModelPart("FluidModelPart").GetNode(self.control_point) + # self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + # self.narrowing_width.append(self.w) + for node in self.model.GetModelPart("FluidModelPart.GENERIC_Meassure").Nodes: + pass + #node = self.model.GetModelPart("Meassure").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.narrowing_width.append(self.w) + + + def MoveAllPartsAccordingToW(self): + ############################# + #### FREE ALL NODES #### + ############################# + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + #### FIXING OUTSIDE PART #### + ############################# + for node in self.model.GetModelPart("FluidModelPart.GENERIC_not_moving").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + ### MOVE EACH SUB-PART ### + ############################# + self.MovePart('GENERIC_green', np.array([[1,0],[0,1/self.w]]), np.array([[0],[1.5]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_up', np.array([[1,0],[0, (2/(3-self.w))]]), np.array([[0],[3]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_down', np.array([[1,0],[0, 2/(3-self.w)]]), np.array([[0],[0]]), np.array([[0],[0]])) + self.MovePart('GENERIC_blue', np.array([[1,0],[(self.w-1)/2, 1]]), np.array([[0],[0]]), np.array([[0],[(self.w-1)/4]])) + self.MovePart('GENERIC_grey', np.array([[1,0],[(1-self.w)/2, 1]]), np.array([[0],[0]]), np.array([[0],[- (self.w-1)/4]])) + + + + def UpdateNarrowing(self): + self.w = self.training_trajectory.UpdateW(self.w) + + + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + print('The current Reynolds Number is: ', self.GetReynolds()) + + + + def GetReynolds(self): + #TODO Make values agree with papers. Parameter to modify: dunamic viscosity niu + velocities = [] + for node in self.model.GetModelPart("FluidModelPart.GENERIC_narrowing_zone").Nodes: + velocities.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + vel_np = np.array(velocities) + + vx = np.max(vel_np) #np.mean(vel_np) + Re = (vx*self.w) / 0.1 #TODO retrieve dynamic viscosity in a more robust way + return Re + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + self.reynolds_number_container.append(self.GetReynolds()) + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + def GetBifuracationData(self): + return np.array(self.velocity_y_at_control_point) , np.array(self.narrowing_width) + + def GetReynoldsData(self): + return np.array(self.reynolds_number_container) + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + + + + + + + + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + +def Train_ROM(): + + if not os.path.exists(f'./Results/FOM.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing = simulation.GetBifuracationData() + reynolds = simulation.GetReynoldsData() + np.save('Results/reynolds.npy', reynolds) + np.save('Results/narrowing.npy', narrowing) + np.save('Results/Velocity_y.npy', velocity_y) + np.save('Results/SnapshotMatrix.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + Train_ROM() \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FOM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FOM_TestTrajectory.py new file mode 100644 index 00000000..4b2093f8 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FOM_TestTrajectory.py @@ -0,0 +1,164 @@ +import KratosMultiphysics +from FOM import FOM_Class + + + +import KratosMultiphysics.RomApplication as romapp +import json + +import numpy as np + +#for checking if paths exits +import os + + +#importing testing trajectory +from simulation_trajectories import TestingTrajectory + + + + +class FOM_Class_test(FOM_Class): + + def InitialMeshPosition(self): + self.testing_trajectory = TestingTrajectory(self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble()) + self.w = self.testing_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + + def UpdateNarrowing(self): + self.w = self.testing_trajectory.UpdateW(self.w) + + + def InitializeSolutionStep(self): + super(FOM_Class, self).InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + print('The current Reynolds Number is: ', self.GetReynolds()) + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM_test' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + + + + + +def FOM_test(): + + if not os.path.exists(f'./Results/FOM_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class_test(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing = simulation.GetBifuracationData() + reynolds = simulation.GetReynoldsData() + np.save('Results/reynolds_test.npy', reynolds) + np.save('Results/narrowing_test.npy', narrowing) + np.save('Results/Velocity_y_test.npy', velocity_y) + np.save('Results/SnapshotMatrix_test.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + FOM_test() + + + + + + + + + + + + + + diff --git a/rom_application/ContractionExpansionChannel/Affine_Mapping/ProblemFiles/FluidMaterials.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FluidMaterials.json similarity index 100% rename from rom_application/ContractionExpansionChannel/Affine_Mapping/ProblemFiles/FluidMaterials.json rename to rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/FluidMaterials.json diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/HROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/HROM_TestTrajectory.py new file mode 100644 index 00000000..e3ade411 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/HROM_TestTrajectory.py @@ -0,0 +1,126 @@ +import KratosMultiphysics +from ROM_TestTrajectory import ROM_Class_test + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt +import os + + + + + + +class HROMClass_test(ROM_Class_test): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 4916 #TODO, get rid of this, load both elements and condition sets + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + + + + + + + + + + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass_test(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + + vy_rom, w_rom = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + + + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}_test' + updated_project_parameters["output_processes"]["vtk_output"][0]["Parameters"]["output_path"] = working_path +f'/Results/vtk_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}_test' + + + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/ProjectParameters.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/ProjectParameters.json new file mode 100644 index 00000000..254fa63f --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/ProjectParameters.json @@ -0,0 +1,162 @@ +{ + "analysis_stage": "KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis", + "problem_data" : { + "problem_name" : "2DFlowBifurcationKratosStructuredMeshWorkingRicc", + "parallel_type" : "OpenMP", + "echo_level" : 0, + "start_time" : 0.0, + "end_time" : 244 + }, + "output_processes" : { + "gid_output" : [{ + "python_module" : "gid_output_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "GiDOutputProcess", + "help" : "This process writes postprocessing files for GiD", + "Parameters" : { + "model_part_name" : "FluidModelPart.fluid_computational_model_part", + "output_name" : "2DFlowBifurcationKratosStructuredMeshWorkingRicc", + "postprocess_parameters" : { + "result_file_configuration" : { + "gidpost_flags" : { + "GiDPostMode" : "GiD_PostBinary", + "WriteDeformedMeshFlag" : "WriteDeformed", + "WriteConditionsFlag" : "WriteConditions", + "MultiFileFlag" : "SingleFile" + }, + "file_label" : "time", + "output_control_type" : "time", + "output_interval" : 0.5, + "body_output" : true, + "node_output" : false, + "skin_output" : false, + "plane_output" : [], + "nodal_results" : ["VELOCITY","PRESSURE","MESH_DISPLACEMENT"], + "gauss_point_results" : [], + "nodal_nonhistorical_results" : [] + }, + "point_data_configuration" : [] + } + } + }], + "vtk_output" : [{ + "python_module" : "vtk_output_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "VtkOutputProcess", + "help" : "This process writes postprocessing files for Paraview", + "Parameters" : { + "model_part_name" : "FluidModelPart.fluid_computational_model_part", + "output_control_type" : "step", + "output_interval" : 1, + "file_format" : "ascii", + "output_precision" : 7, + "output_sub_model_parts" : false, + "output_path" : "vtk_output", + "save_output_files_in_folder" : true, + "nodal_solution_step_data_variables" : ["VELOCITY","PRESSURE"], + "nodal_data_value_variables" : [], + "element_data_value_variables" : ["HROM_WEIGHT"], + "condition_data_value_variables" : [], + "gauss_point_variables_extrapolated_to_nodes" : [] + } + }], + "rom_output" : [] + }, + "solver_settings" : { + "solver_type": "ale_fluid", + "ale_boundary_parts": [], + "mesh_motion_solver_settings" : { + "solver_type" : "structural_similarity" + }, + "fluid_solver_settings": { + "model_part_name" : "FluidModelPart", + "domain_size" : 2, + "solver_type" : "Monolithic", + "model_import_settings" : { + "input_type" : "mdpa", + "input_filename" : "2DFlowBifurcationKratosStructuredMeshWorkingRicc" + }, + "material_import_settings" : { + "materials_filename" : "FluidMaterials.json" + }, + "echo_level" : 0, + "compute_reactions" : false, + "maximum_iterations" : 10, + "relative_velocity_tolerance" : 1e-8, + "absolute_velocity_tolerance" : 1e-8, + "relative_pressure_tolerance" : 1e-8, + "absolute_pressure_tolerance" : 1e-8, + "volume_model_part_name" : "FluidParts_Volume", + "skin_parts" : ["Outlet2D_Outlet","NoSlip2D_Wall"], + "no_skin_parts" : ["VelocityConstraints2D_Inlet-Total"], + "time_scheme" : "bdf2", + "time_stepping" : { + "automatic_time_step" : false, + "time_step" : 0.1 + }, + "formulation" : { + "element_type" : "weakly_compressible", + "dynamic_tau" : 1.0 + }, + "reform_dofs_at_each_step" : false + } + }, + "processes" : { + "initial_conditions_process_list" : [], + "boundary_conditions_process_list" : [{ + "python_module" : "apply_outlet_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyOutletProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.Outlet2D_Outlet", + "variable_name" : "PRESSURE", + "constrained" : true, + "value" : 0.0, + "hydrostatic_outlet" : false, + "h_top" : 0.0 + } + },{ + "python_module" : "apply_noslip_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyNoSlipProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.NoSlip2D_Wall" + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name" : "VELOCITY", + "interval" : [0.0,1], + "constrained" : [true,true,true], + "value" : ["y*(3-y)*sin(pi*t*0.5)",0.0,0.0] + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name" : "VELOCITY", + "interval" : [0.0,"End"], + "constrained" : [true,true,true], + "value" : ["y*(3-y)",0.0,0.0] + } + }], + "gravity" : [{ + "python_module" : "assign_vector_by_direction_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorByDirectionProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "variable_name" : "BODY_FORCE", + "modulus" : 0.0, + "constrained" : false, + "direction" : [0.0,-1.0,0.0] + } + }], + "auxiliar_process_list" : [] + } +} diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/ROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/ROM_TestTrajectory.py new file mode 100644 index 00000000..1ad3f03b --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/ROM_TestTrajectory.py @@ -0,0 +1,144 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + + +import KratosMultiphysics.RomApplication as romapp +import json + + +import numpy as np +import os + + +#importing testing trajectory +from simulation_trajectories import TestingTrajectory + + + +class ROM_Class_test(ROM_Class): + + + def InitialMeshPosition(self): + self.testing_trajectory = TestingTrajectory(self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble()) + self.w = self.testing_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + + def UpdateNarrowing(self): + self.w = self.testing_trajectory.UpdateW(self.w) + + + + + def InitializeSolutionStep(self): + super(ROM_Class, self).InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + + + + + + + + + + + + + + + + + +def prepare_files(working_path,svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_{svd_truncation_tolerance}_test' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(hard_impose_currect_cluster = False, Number_Of_Clusters=1, svd_truncation_tolerance=1e-4): + + + if not os.path.exists(f'./Results/ROM_{svd_truncation_tolerance}_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class_test(global_model, parameters, correct_clusters, hard_impose_currect_cluster, bases) + simulation.Run() + np.save(f'Results/ROM_snapshots_{svd_truncation_tolerance}_test.npy',simulation.GetSnapshotsMatrix()) + vy_rom,w_rom = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_ROM_{svd_truncation_tolerance}_test.npy', vy_rom) + np.save(f'Results/narrowing_ROM_{svd_truncation_tolerance}_test.npy', w_rom) + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path,svd_truncation_tolerance) + + + ROM(hard_impose_currect_cluster = True, Number_Of_Clusters=Number_Of_Clusters, svd_truncation_tolerance=svd_truncation_tolerance) + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/Run_HROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/Run_HROM.py new file mode 100644 index 00000000..1268863d --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/Run_HROM.py @@ -0,0 +1,97 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + +import KratosMultiphysics.RomApplication as romapp +import json + + + +import numpy as np +import os + + + +class HROMClass(ROM_Class): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance,hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 4916 + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.post.bin'): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + vy_rom, w_rom = simulation.GetBifuracationData() + np.save(f'Results/y_velocity_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + updated_project_parameters["output_processes"]["vtk_output"][0]["Parameters"]["output_path"] = working_path +f'/Results/vtk_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/Run_ROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/Run_ROM.py new file mode 100644 index 00000000..f108fb0a --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/Run_ROM.py @@ -0,0 +1,272 @@ +import KratosMultiphysics +from KratosMultiphysics.RomApplication.fluid_dynamics_analysis_rom import FluidDynamicsAnalysisROM + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np + + + + +import os.path + + + +#importing training trajectory +from simulation_trajectories import TrainingTrajectory + + + + + + + +class ROM_Class(FluidDynamicsAnalysisROM): + + def __init__(self, model, project_parameters, correct_cluster = None, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, hrom) + self.bases = bases + self.w = 1 # original narrowing size + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.delta_w = 0.025 * time_step_size # this ensures to obtain a maximum narrowing size of 2.9 and a minimum of 0.1 + self.maximum = 2.9 + self.minimum = 0.1 + self.control_point = None + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.tttime = 0 #fake time step, useful to impose the correct cluster + self.time_step_solution_container = [] + + + def InitialMeshPosition(self): + self.training_trajectory = TrainingTrajectory(self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble()) + self.w = self.training_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.InitialMeshPosition() + + + def MovePart(self, part_name, jacobian, centering_vector, extra_centering): + x_original = [] + y_original = [] + # first loop + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(1,-1) + y_original = np.array(y_original).reshape(1,-1) + matrix_of_coordinates = np.r_[x_original, y_original] + modified_matrix_of_coordinates = np.linalg.inv(jacobian) @ (matrix_of_coordinates - centering_vector) + modified_matrix_of_coordinates += centering_vector + extra_centering #re-locating + # second loop + i = 0 + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = modified_matrix_of_coordinates[0,i] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = modified_matrix_of_coordinates[1,i] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + def MoveAllPartsAccordingToW(self): + ############################# + #### FREE ALL NODES #### + ############################# + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + #### FIXING OUTSIDE PART #### + ############################# + for node in self.model.GetModelPart("FluidModelPart.GENERIC_not_moving").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + ### MOVE EACH SUB-PART ### + ############################# + self.MovePart('GENERIC_green', np.array([[1,0],[0,1/self.w]]), np.array([[0],[1.5]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_up', np.array([[1,0],[0, (2/(3-self.w))]]), np.array([[0],[3]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_down', np.array([[1,0],[0, 2/(3-self.w)]]), np.array([[0],[0]]), np.array([[0],[0]])) + self.MovePart('GENERIC_blue', np.array([[1,0],[(self.w-1)/2, 1]]), np.array([[0],[0]]), np.array([[0],[(self.w-1)/4]])) + self.MovePart('GENERIC_grey', np.array([[1,0],[(1-self.w)/2, 1]]), np.array([[0],[0]]), np.array([[0],[- (self.w-1)/4]])) + + + def StoreBifurcationData(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_Meassure").Nodes: + pass + #node = self.model.GetModelPart("Meassure").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.narrowing_width.append(self.w) + + + def UpdateNarrowing(self): + self.w = self.training_trajectory.UpdateW(self.w) + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + self.tttime += 1 + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + +def prepare_files(working_path,svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_{svd_truncation_tolerance}' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(hard_impose_currect_cluster = False, Number_Of_Clusters=1, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/ROM_{svd_truncation_tolerance}.post.bin'): + if not os.path.exists(f'./ROM/'): + os.mkdir('./ROM') + basis = f'./ROM/Phi_{svd_truncation_tolerance}.npy' + if os.path.exists(basis): + u = np.load(basis) + else: + u,s,_,_ = RandomizedSingularValueDecomposition().Calculate(np.load(f'./Results/SnapshotMatrix.npy'), svd_truncation_tolerance) + np.save(basis,u) + + ### Saving the nodal basis ### (Need to make this more robust, hard coded here) + basis_POD={"rom_settings":{},"nodal_modes":{}} + basis_POD["rom_settings"]["nodal_unknowns"] = ["VELOCITY_X","VELOCITY_Y","PRESSURE"] + basis_POD["rom_settings"]["number_of_rom_dofs"] = np.shape(u)[1] + Dimensions = len(basis_POD["rom_settings"]["nodal_unknowns"]) + N_nodes=np.shape(u)[0]/Dimensions + N_nodes = int(N_nodes) + node_Id=np.linspace(1,N_nodes,N_nodes) + i = 0 + for j in range (0,N_nodes): + basis_POD["nodal_modes"][int(node_Id[j])] = (u[i:i+Dimensions].tolist()) + i=i+Dimensions + + with open('ProblemFiles/RomParameters.json', 'w') as f: + json.dump(basis_POD,f, indent=2) + + print('\n\nNodal basis printed in json format\n\n') + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class(global_model, parameters, correct_clusters, hard_impose_currect_cluster, bases) + simulation.Run() + np.save(f'./Results/ROM_snapshots_{svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom = simulation.GetBifuracationData() + + np.save(f'./Results/y_velocity_ROM_{svd_truncation_tolerance}.npy', vy_rom) + np.save(f'./Results/narrowing_ROM_{svd_truncation_tolerance}.npy', w_rom) + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path,svd_truncation_tolerance) + + + ROM(hard_impose_currect_cluster = True, Number_Of_Clusters=Number_Of_Clusters, svd_truncation_tolerance=svd_truncation_tolerance) + + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/TrainHROM_Step1.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/TrainHROM_Step1.py new file mode 100644 index 00000000..5c1e8f3e --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/TrainHROM_Step1.py @@ -0,0 +1,90 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + + +import KratosMultiphysics.RomApplication as romapp +import json +import numpy as np + + + + +import os.path + + +class TrainHROMClass(ROM_Class): + + def __init__(self, model, project_parameters,svd_truncation_tolerance): + super().__init__(model, project_parameters, hrom="EmpiricalCubature") + self.svd_truncation_tolerance = svd_truncation_tolerance + + + + + + + +def Train_HROM(svd_truncation_tolerance): + + projected_residuals = f'HROM/Sr_{svd_truncation_tolerance}.npy' + + + if not os.path.exists(projected_residuals): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + #loading the bases + bases = [] + bases = None + simulation = TrainHROMClass(global_model, parameters, svd_truncation_tolerance) + simulation.Run() + + + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"] = [] + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path) + + Train_HROM(svd_truncation_tolerance) + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/TrainHROM_Step2.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/TrainHROM_Step2.py new file mode 100644 index 00000000..f7d869c0 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/TrainHROM_Step2.py @@ -0,0 +1,76 @@ +import numpy as np +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition +from matplotlib import pyplot as plt + +import os.path + +def get_global_norm(number_bases): + norm = 0 + for i in range(number_bases): + norm_a = np.linalg.norm(np.load(f'HROM/Sr_{i}.npy')) + norm = np.sqrt(np.power(norm_a, 2) + np.power(norm, 2)) + return norm + + +def get_bases(number_bases, global_norm, tol, relative=False): + bases = [] + for i in range(number_bases): + if relative: + u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=False).Calculate( np.load(f'HROM/Sr_{i}.npy'), tol* global_norm) #* global_norm + else: + u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr_{i}.npy'), tol) #* global_norm + bases.append(u) + + return bases + +def select_elements(svd_truncation_tolerance, residuals_svd_truncation_tolerance): + + weights = f'HROM/WeightsMatrix_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + elements = f'HROM/Elementsvector_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + + if not os.path.exists(weights) and not os.path.exists(elements): + #u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr.npy'), tol) # HEAVY!!! + u = np.load(f'HROM/basis_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy') + + hyper_reduction_element_selector = EmpiricalCubatureMethod() + hyper_reduction_element_selector.SetUp(u) #add again z + hyper_reduction_element_selector.Initialize() + hyper_reduction_element_selector.Calculate() + + + w = np.squeeze(hyper_reduction_element_selector.w) + z = np.squeeze(hyper_reduction_element_selector.z) + + WeightsMatrix = w.reshape(np.size(z),1) + + np.save(weights, WeightsMatrix ) + np.save(elements, z) + + +def get_basis(svd_truncation_tolerance, tol): + + basis = f'HROM/basis_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + + if not os.path.exists(basis): + u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr_{svd_truncation_tolerance}.npy'), tol) + np.save( basis,u) + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance = float(argv[7]) + residuals_svd_relative_to_global_residuals_snapshots = bool(argv[8]) + + + get_basis(svd_truncation_tolerance, residuals_svd_truncation_tolerance) + select_elements(svd_truncation_tolerance, residuals_svd_truncation_tolerance) + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/analytic_mapping.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/analytic_mapping.py new file mode 100644 index 00000000..f23a1702 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/analytic_mapping.py @@ -0,0 +1,65 @@ +import KratosMultiphysics +import numpy as np + +#Not working + + + +def MovePart(simulation, part_name, jacobian, centering_vector, extra_centering): + x_original = [] + y_original = [] + # first loop + for node in simulation.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(1,-1) + y_original = np.array(y_original).reshape(1,-1) + matrix_of_coordinates = np.r_[x_original, y_original] + modified_matrix_of_coordinates = np.linalg.inv(jacobian) @ (matrix_of_coordinates - centering_vector) + modified_matrix_of_coordinates += centering_vector + extra_centering #re-locating + # second loop + i = 0 + for node in simulation.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = modified_matrix_of_coordinates[0,i] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = modified_matrix_of_coordinates[1,i] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + +def phi(simulation): + ############################# + #### FREE ALL NODES #### + ############################# + for node in simulation.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + #### FIXING OUTSIDE PART #### + ############################# + for node in simulation.model.GetModelPart("FluidModelPart.GENERIC_not_moving").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + ### MOVE EACH SUB-PART ### + ############################# + simulation.MovePart('GENERIC_green', np.array([[1,0],[0,1/simulation.w]]), np.array([[0],[1.5]]), np.array([[0],[0]])) + simulation.MovePart('GENERIC_yellow_up', np.array([[1,0],[0, (2/(3-simulation.w))]]), np.array([[0],[3]]), np.array([[0],[0]])) + simulation.MovePart('GENERIC_yellow_down', np.array([[1,0],[0, 2/(3-simulation.w)]]), np.array([[0],[0]]), np.array([[0],[0]])) + simulation.MovePart('GENERIC_blue', np.array([[1,0],[(simulation.w-1)/2, 1]]), np.array([[0],[0]]), np.array([[0],[(simulation.w-1)/4]])) + simulation.MovePart('GENERIC_grey', np.array([[1,0],[(1-simulation.w)/2, 1]]), np.array([[0],[0]]), np.array([[0],[- (simulation.w-1)/4]])) + + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/overlapping_strategies.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/overlapping_strategies.py new file mode 100644 index 00000000..638238bf --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/overlapping_strategies.py @@ -0,0 +1,323 @@ +import numpy as np +from matplotlib import pyplot as plt +from sklearn.cluster import KMeans + +def time_clustering(S, time_clusters = 3, overlaping_snapshots = 1 ): + total_time_steps = S.shape[1] + if time_clusters > total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #get list containing snapshots to add to each overlapped cluster + if overlaping_snapshots is not 0: + snapshots_to_add = {} + for i in range(time_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == time_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(time_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + + +def ismember(A, B): + if isinstance(A, np.int_): + return [ np.sum(A == B) ] + else: + return [ np.sum(a == B) for a in A ] + +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + kmeans = KMeans(n_clusters=narrowing_clusters, random_state=0).fit(narrowing.reshape(-1,1)) + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(narrowing_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + correct_cluster = kmeans.labels_ + centroids = kmeans.cluster_centers_ + + if narrowing_clusters>1: + #try and use as is solution manifold neighbor identification + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + narrowing = narrowing.reshape(1,-1) + for i in range(np.shape(narrowing)[1]): + this_matrix = (kmeans.cluster_centers_).T - narrowing[:,i].reshape(np.shape(narrowing)[0], 1) + distance = np.zeros((narrowing_clusters)) + for j in range(narrowing_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + #get list containing snapshots to add to each overlapped cluster + if True: + #if overlaping_snapshots is not 0: + + snapshots_to_add = [] + for j in range(narrowing_clusters): + N_neighbors = len(neighbors[j]) + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + ith_narrowing_cluster = narrowing[:,kmeans.labels_==neighbors[j][i]] + this_matrix = ith_narrowing_cluster - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(narrowing)[0], 1) + distance = np.linalg.norm(this_matrix, axis = 0) + #distance = np.zeros(np.shape(ith_narrowing_cluster[1])) + #for k in range(len(distance)): + # distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + + return sub_snapshots, correct_cluster + + +def solution_manifold_clustering(): + pass + + + +if __name__=='__main__': + #S = np.load('SnapshotMatrix.npy') + #narrowing = np.load('narrowing.npy') + narrowing = np.linspace(0,1,12) + S = np.array([[1,2,3,4,5,6,7,8,9,10,11,12],[1,2,3,4,5,6,7,8,9,10,11,12]]) + #a = narrowing.reshape(1,-1) + #S = np.r_[a, a , a, a] + sub_snapshots, correct_cluster = time_clustering(S, 3,0) + #sub_snapshots, correct_cluster = narrowing_clustering(S, narrowing, 3, 2) + #sub_snapshots, correct_cluster = solution_manifold_clustering(S) + #sub_snapshots, correct_cluster = time_clustering(S) + kkk = 5 + + # + + +""" + +def solution_manifold_clustering(S, solution_manifold_clusters = 3, overlaping_snapshots = 1 ): + #S = np.load('SnapshotMatrix.npy') + kmeans = KMeans(n_clusters = solution_manifold_clusters, random_state=0).fit(S.T) + correct_cluster = kmeans.labels_ + + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(solution_manifold_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + for i in range(np.shape(S)[1]): + this_matrix = (kmeans.cluster_centers_).T - S[:,i].reshape(np.shape(S)[0], 1) + distance = np.zeros((solution_manifold_clusters)) + for j in range(solution_manifold_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + snapshots_to_add = [] + + for j in range(solution_manifold_clusters): + N_snaps = np.shape(sub_snapshots[j])[1] + N_neighbors = len(neighbors[j]) + + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + this_matrix = sub_snapshots[neighbors[j][i]] - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(S)[0], 1) + distance = np.zeros(np.shape(sub_snapshots[neighbors[j][i]][1])) + for k in range(len(distance)): + distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(solution_manifold_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + + +""" +This is wrong, but save for now as reference +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + # wrong implementation :( + # MINE (no k-means) + #S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + #narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + correct_cluster = np.empty(narrowing.shape) + for i in range(narrowing_clusters): + # In this implementation, I just shuffle (order) the snapshots to match the narrowing width. No time-relation whatsoever + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + correct_cluster[intersection] = i + ith_narrowing = narrowing[intersection] + ith_indexes_ordered = np.argsort(ith_narrowing) + sub_snapshots[i] = S[:,ith_indexes_ordered] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + # storing centroids + if i==0: + centroids = np.sum(ith_narrowing)/(ith_narrowing.shape[0]) + else: + centroids = np.c_[centroids, np.sum(ith_narrowing)/(ith_narrowing.shape[0])] + np.save('cluster_centroid.npy', centroids) + #overlapping after correct cluster definition + + #get list containing snapshots to add to each overlapped cluster + snapshots_to_add = {} + for i in range(narrowing_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == narrowing_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + +""" +def time_clustering(time_clusters = 5, overlaping_snapshots = 1 ): + #it works, but no overlapping + S = np.load('SnapshotMatrix.npy') + total_time_steps = S.shape[1] + if time_clusters > total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + + return sub_snapshots, correct_cluster +""" + + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + #no overlapping. MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + return sub_snapshots, correct_cluster +""" + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + # MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + #overlapping after correct cluster definition + # In this implementation, I just shuffle the snapshots to match the narrowing width. No time relation whatsoever + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + if i == 0: + ith_narrowing = narrowing[intersection] + + ith_indexes = np.argsort(ith_narrowing) + ith_narrowing_ordered = ith_narrowing[ith_indexes] + plt.plot(ith_narrowing, 'b') + plt.plot(ith_narrowing_ordered, 'r') + plt.show() + + elif i == narrowing_clusters-1: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + else: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + sub_snapshots[i] = np.c_[sub_snapshots[i] , sub_snapshots[i+1][:, :overlaping_snapshots] ] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster +""" + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/simulation_trajectories.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/simulation_trajectories.py new file mode 100644 index 00000000..ca9b8ef1 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/simulation_trajectories.py @@ -0,0 +1,50 @@ +class TrainingTrajectory(): + + def __init__(self, time_step_size): + self.min_or_max_reached_flag = False + self.maximum = 2.9 + self.minimum = 0.1 + self.delta_w = 0.025 * time_step_size # this ensures to obtain a maximum narrowing size of 2.9 and a minimum of 0.1 for a total time T=244 + + def SetUpInitialNarrowing(self): + return 2.9 # starting with a wide narrowing + + def UpdateW(self, w): + ####Train trajectory#### + if not self.min_or_max_reached_flag: #contraction + w -= self.delta_w + if w < self.minimum: + w =self.minimum + self.min_or_max_reached_flag = True + else: #expansion + w += self.delta_w + if w > self.maximum: + w = self.maximum + return w + + + +class TestingTrajectory(): + + def __init__(self, time_step_size): + self.min_or_max_reached_flag = False + self.maximum = 2.9 + self.minimum = 0.1 + self.delta_w = 0.025 * time_step_size # this ensures to obtain a maximum narrowing size of 2.9 and a minimum of 0.1 for a total time T=244 + + def SetUpInitialNarrowing(self): + return 0.1 # starting with a narrow narrowing + + def UpdateW(self, w): + ####Test trajectory#### + if not self.min_or_max_reached_flag:#expansion + w += self.delta_w + if w > self.maximum: + w = self.maximum + self.min_or_max_reached_flag = True + else: #contraction + w -= self.delta_w + if w < self.minimum: + w =self.minimum + return w + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/test_ALE_ROM_stage4.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/test_ALE_ROM_stage4.py new file mode 100644 index 00000000..978729c2 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/ProblemFiles/test_ALE_ROM_stage4.py @@ -0,0 +1,128 @@ +import KratosMultiphysics +from test_ALE_ROM_stage2 import ROM_Class + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt + + + + + + + +class HROMClass(ROM_Class): + + def __init__(self, model, project_parameters, correct_cluster, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 4916 + WeightsMatrix = np.load('HROM_Local/WeightsMatrix.npy') + ElementsVector = np.load('HROM_Local/Elementsvector.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + + + + + + + + + + + +def HROM(hard_impose_currect_cluster = False, Number_Of_Clusters=1, residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + #loading the bases + bases = [] + bases = None + simulation = HROMClass(global_model, parameters, correct_clusters, hard_impose_currect_cluster, bases) + simulation.Run() + np.save(f'Results/HROM_snapshots_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + return simulation.GetBifuracationData() + + + + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + updated_project_parameters["output_processes"]["vtk_output"][0]["Parameters"]["output_path"] = working_path +f'/Results/vtk_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + vy_rom, w_rom = HROM(hard_impose_currect_cluster = True, Number_Of_Clusters=Number_Of_Clusters, residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) + + np.save(f'Results/y_velocity_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + + + +4916 \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/launch_ale_rom.sh b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/launch_ale_rom.sh new file mode 100755 index 00000000..62fd38ff --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Affine/launch_ale_rom.sh @@ -0,0 +1,102 @@ +#!/bin/sh +#SBATCH -N 1 # nodes requested +#SBATCH -n 1 # tasks requested +#SBATCH -c 16 # cores requested +#SBATCH -t 20:00:00 # time requested in hour:minute:second +#SBATCH --constraint='highmem' + + +export OMP_NUM_THREADS=16 +export PROBLEMS_PATH=$PWD/ProblemFiles +export LANGUAGE=en_GB.utf8 +export LC_ALL=en_GB.utf8 + + +FOM=True #(storing results) +FOM_test=True #(storing results) +Run_ROM=True #3 (storing results) +ROM_test=True #4 = (storing results) +Train_HROM_Step1=True #5 = (creating projected residuals matrices {Sr_i}_i=1^k (one per basis)) +Train_HROM_Step2=True #6 = ontain a reduced set of elements and weights starting from the projected residuals matrices Sr_i +Run_HROM=True #7 = RunHROM Train Trajectory +HROM_test=True #8 = RunHROM Test Trajectory + +plot_partial_hysteresis=False + +#parameters used in Local POD: + +# parameters for the simulations +Launch_Simulation=1 +Number_Of_Clusters=1 #not used in global POD +svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +clustering="narrowing" #time # +overlapping=30 +residuals_svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +residuals_svd_relative_to_global_residuals_snapshots=1 + + +if [ $FOM = True ] + then + #### LAUNCH FOM TRAIN TRAJECTORY #### + # MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLauching FOM \n\n\n\n\n\n" + python3 ProblemFiles/FOM.py $PWD +fi +if [ $FOM_test = True ] + then + # NEW MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching FOM test trajectory \n\n\n\n\n\n" + python3 ProblemFiles/FOM_TestTrajectory.py $PWD +fi +for j in ${svd_truncation_tolerance_list[@]} +do + svd_truncation_tolerance=$j + if [ $Run_ROM = True ] + then + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching ROM \n\n\n\n\n\n" + python3 ProblemFiles/Run_ROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $ROM_test = True ] + then + #### LAUNCH ROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\nlaunching ROM test\n\n\n\n' + python3 ProblemFiles/ROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $Train_HROM_Step1 = True ] + then + #### TrainHROM (Creating Matrix of projected resduals Sr) #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\nlaunching TrainHROM train\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step1.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + for k in ${residuals_svd_truncation_tolerance_list[@]} + do + residuals_svd_truncation_tolerance=$k + if [ $Train_HROM_Step2 = True ] + then + ### Obtain Reduced Elements and Weights #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nlaunching HROM elements and Weights\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step2.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $Run_HROM = True ] + then + #### LAUNCH HROM TRAIN TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nLaunching HROM train\n\n\n\n\n\n\n' + python3 ProblemFiles/Run_HROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $HROM_test = True ] + then + #### LAUNCH HROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo 'Launching HROM test' + python3 ProblemFiles/HROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + done +done + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FOM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FOM.py new file mode 100644 index 00000000..740ccada --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FOM.py @@ -0,0 +1,480 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt + +#importing overlapping strategies +from overlapping_strategies import time_clustering, narrowing_clustering, solution_manifold_clustering + +#for checking if paths exits +import os + +#importing PyGeM tools +from pygem import FFD, RBF + +import pdb + + +class FOM_Class(FluidDynamicsAnalysis): + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.deformation_multiplier = 1 # original narrowing size + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.delta_deformation = time_step_size # this ensures to obtain the same deformation independently of the time step used + self.control_point = 854 #a node around the middle of the geometry to capture the bufurcation + self.maximum = 11 + self.minimum = 0 + ### ### ### + self.node_up = 412 #nodes to obtain the narrowing width + self.node_down = 673 + ### ### ### + self.time_step_solution_container = [] + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.deformation_multiplier_list = [] + self.matrix_of_free_coordinates = None + self.deformation_multiplier = 0 + + + def MoveInnerNodesWithRBF(self): + # first loop, ONLY ENTERED ONCE + if self.matrix_of_free_coordinates is None: + x_original = [] + y_original = [] + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(-1,1) + y_original = np.array(y_original).reshape(-1,1) + self.matrix_of_free_coordinates = np.c_[x_original, y_original, np.ones((y_original.shape[0],1))] + self.matrix_of_modified_coordinates = self.rbf(self.matrix_of_free_coordinates) + + # second loop + i = 0 + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = self.matrix_of_modified_coordinates[i,0] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = self.matrix_of_modified_coordinates[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + node = self.model.GetModelPart("FluidModelPart").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.deformation_multiplier_list.append(self.deformation_multiplier) + node_up = self.model.GetModelPart("FluidModelPart").GetNode(self.node_up) + node_down = self.model.GetModelPart("FluidModelPart").GetNode(self.node_down) + self.narrowing_width.append(node_up.Y - node_down.Y) + + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.IdentifyNodes() + self.SetUpFreeFormDeformation() + + + + def IdentifyNodes(self): + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + fixed_walls= self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls") + + number_of_nodes_walls = fixed_walls.NumberOfNodes() + number_of_nodes_down = control_down.NumberOfNodes() + number_of_nodes_up = control_down.NumberOfNodes() + + #get matrix of original coordinates + walls_coordinates = np.ones((int(number_of_nodes_walls),3)) + up_coordinates = np.ones((int(number_of_nodes_up),3)) + down_coordinates = np.ones((int(number_of_nodes_down),3)) + + counter = 0 + for node in control_down.Nodes: + down_coordinates[counter, 0] = node.X0 + down_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in control_up.Nodes: + up_coordinates[counter, 0] = node.X0 + up_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in fixed_walls.Nodes: + walls_coordinates[counter, 0] = node.X0 + walls_coordinates[counter, 1] = node.Y0 + counter+=1 + + self.walls = walls_coordinates + + self.up = up_coordinates + at_3_y = np.where(self.up[:,1] == 3) + self.up = np.delete(self.up,at_3_y, 0) + + self.down = down_coordinates + at_0_y = np.where(self.down[:,1] == 0) + self.down = np.delete(self.down,at_0_y, 0) + + self.fixed_coordinates = np.r_[walls_coordinates, self.down, self.up] + + + + + def SetUpFreeFormDeformation(self): + #creating a free form deformation object for each control domain + self.ffd_up = FFD([2,5,2]) #3D box of control points + self.ffd_down = FFD([2,5,2]) #3D box of control points + + #setting the centre and size of the upper box of control points + self.ffd_down.box_origin = np.array([1.25, 0, 0.5]) + self.ffd_down.box_length = np.array([1, 1.25, 1]) + + #setting the centre and size of the lower box of control points + self.ffd_up.box_origin = np.array([1.25, 1.75, 0.5]) + self.ffd_up.box_length = np.array([1, 1.25, 1]) + + self.list_of_ffds = [self.ffd_up, self.ffd_down] + + + + + def MoveControlPoints(self, scale_of_deformation=1): + + self.ffd_down.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + + self.ffd_down.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + self.ffd_up.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[0, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[0, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + + self.ffd_up.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[1, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[1, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + moved_up = self.ffd_up(self.up) + moved_down = self.ffd_down(self.down) + + + #Moving lower part + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + i=0 + for node in control_down.Nodes: + if node.Y0 != 0: + x_disp = moved_down[i,0] - node.X0 + y_disp = moved_down[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + node.X = node.X0 + x_disp + node.Y = node.Y0 + y_disp + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + #moving upper part + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + i=0 + for node in control_up.Nodes: + if node.Y0 != 3: + x_disp = moved_up[i,0] - node.X0 + y_disp = moved_up[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + node.X = node.X0 + x_disp + node.Y = node.Y0 + y_disp + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.moved_coordinates = np.r_[self.walls, moved_down, moved_up] + + + + def UpdateRBF(self): + self.rbf = RBF(original_control_points = self.fixed_coordinates, deformed_control_points = + self.moved_coordinates, radius=0.75) + + + def LockOuterWalls(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0 ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + def UpdateDeformationMultiplier(self): + ####Train trajectory#### + if self.time>10.0 and self.time<=21.0: # start modifying narrowing from 10 seconds onwards + self.deformation_multiplier+=self.delta_deformation + if self.deformation_multiplier > self.maximum: + self.deformation_multiplier = self.maximum + elif self.time>31.0 and self.time<41.9: # start modifying narrowing from 10 seconds onwards + self.deformation_multiplier-=self.delta_deformation + if self.deformation_multiplier < self.minimum: + self.deformation_multiplier = self.minimum + + + + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width, self.deformation_multiplier_list + + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + + + + + + + + + + + + +def Train_ROM(): + + if not os.path.exists(f'./Results/FOM.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing, deformation_multiplier = simulation.GetBifuracationData() + #reynolds = simulation.GetReynoldsData() + #np.save('Results/reynolds.npy', reynolds) + np.save('Results/deformation_multiplier.npy', deformation_multiplier) + np.save('Results/narrowing.npy', narrowing) + np.save('Results/Velocity_y.npy', velocity_y) + np.save('Results/SnapshotMatrix.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + + Train_ROM() + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FOM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FOM_TestTrajectory.py new file mode 100644 index 00000000..0ed0f912 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FOM_TestTrajectory.py @@ -0,0 +1,180 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis + +from FOM import FOM_Class + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt + +#importing overlapping strategies +from overlapping_strategies import time_clustering, narrowing_clustering, solution_manifold_clustering + +#for checking if paths exits +import os + + + +#importing PyGeM tools +from pygem import FFD, RBF + + + + + +class FOM_Class_test(FOM_Class): + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.deformation_multiplier = 11 + + + + + def UpdateDeformationMultiplier(self): + #### Test trajectory#### + + if self.time>10.0 and self.time<=21.0: # start modifying narrowing from 1 second onwards + self.deformation_multiplier-= self.delta_deformation + if self.deformation_multiplier < self.minimum: + self.deformation_multiplier = self.minimum + elif self.time>31.0 and self.time<41.9: + self.deformation_multiplier+= self.delta_deformation + if self.deformation_multiplier > self.maximum: + self.deformation_multiplier = self.maximum + + + def InitializeSolutionStep(self): + super(FluidDynamicsAnalysis, self).InitializeSolutionStep() + + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM_test' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + + + + + + + + + + + + +def Train_ROM(): + + if not os.path.exists(f'./Results/FOM_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class_test(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing, deformation_multiplier = simulation.GetBifuracationData() + #reynolds = simulation.GetReynoldsData() + #np.save('Results/reynolds.npy', reynolds) + np.save('Results/deformation_multiplier_test.npy', deformation_multiplier) + np.save('Results/narrowing_test.npy', narrowing) + np.save('Results/Velocity_y_test.npy', velocity_y) + np.save('Results/SnapshotMatrix_test.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + + Train_ROM() + diff --git a/rom_application/ContractionExpansionChannel/FFD_plus_RBF/ProblemFiles/FluidMaterials.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FluidMaterials.json similarity index 100% rename from rom_application/ContractionExpansionChannel/FFD_plus_RBF/ProblemFiles/FluidMaterials.json rename to rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/FluidMaterials.json diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/HROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/HROM_TestTrajectory.py new file mode 100644 index 00000000..92fc4938 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/HROM_TestTrajectory.py @@ -0,0 +1,133 @@ +import KratosMultiphysics +from ROM_TestTrajectory import ROM_Class_test + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt + +import os + + + + + +class HROMClass_test(ROM_Class_test): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 5152 #TODO, get rid of this, load both elements and condition sets + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + + + + + + + + + + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass_test(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom, deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_ROM_test_{svd_truncation_tolerance}.npy', deformation_multiplier) + + + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/MainKratos.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/MainKratos.py new file mode 100644 index 00000000..7922e43b --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/MainKratos.py @@ -0,0 +1,383 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis +from KratosMultiphysics.RomApplication.fluid_dynamics_analysis_rom import FluidDynamicsAnalysisROM + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt + + +#importing PyGeM tools +from pygem import FFD, RBF + +#Function from PyGeM tutorial +def scatter3d(arr, figsize=(8,8), s=10, draw=True, ax=None, alpha=1, labels=None, title=None): + if ax is None: + fig = plt.figure(figsize=figsize) + ax = fig.add_subplot(projection='3d') + + for idx,a in enumerate(arr): + if labels is not None: + ax.scatter(*a.T, s=s, alpha=alpha, label=labels[idx]) + else: + ax.scatter(*a.T, s=s, alpha=alpha) + + if draw: + if labels is not None: + plt.legend() + if title is not None: + plt.title(title) + plt.show() + else: + return ax + + +class FOM_Class(FluidDynamicsAnalysis): + + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.w = 1 # original narrowing size + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.control_point = 363 #a node around the middle of the geometry to capture the bufurcation + self.time_step_solution_container = [] + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.matrix_of_free_coordinates = None + self.deformation_multiplier = 0 + + + def MoveInnerNodesWithRBF(self): + # first loop, ONLY ENTERED ONCE + if self.matrix_of_free_coordinates is None: + x_original = [] + y_original = [] + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(-1,1) + y_original = np.array(y_original).reshape(-1,1) + self.matrix_of_free_coordinates = np.c_[x_original, y_original, np.ones((y_original.shape[0],1))] + self.matrix_of_modified_coordinates = self.rbf(self.matrix_of_free_coordinates) + + # second loop + i = 0 + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = self.matrix_of_modified_coordinates[i,0] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = self.matrix_of_modified_coordinates[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + node = self.model.GetModelPart("FluidModelPart").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.narrowing_width.append(self.deformation_multiplier) + + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.IdentifyNodes() + self.SetUpFreeFormDeformation() + + + + def IdentifyNodes(self): + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + fixed_walls= self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls") + + number_of_nodes_walls = fixed_walls.NumberOfNodes() + number_of_nodes_down = control_down.NumberOfNodes() + number_of_nodes_up = control_down.NumberOfNodes() + + #get matrix of original coordinates + walls_coordinates = np.ones((int(number_of_nodes_walls),3)) + up_coordinates = np.ones((int(number_of_nodes_up),3)) + down_coordinates = np.ones((int(number_of_nodes_down),3)) + + counter = 0 + for node in control_down.Nodes: + down_coordinates[counter, 0] = node.X0 + down_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in control_up.Nodes: + up_coordinates[counter, 0] = node.X0 + up_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in fixed_walls.Nodes: + walls_coordinates[counter, 0] = node.X0 + walls_coordinates[counter, 1] = node.Y0 + counter+=1 + + self.walls = walls_coordinates + + self.up = up_coordinates + at_3_y = np.where(self.up[:,1] == 3) + self.up = np.delete(self.up,at_3_y, 0) + + self.down = down_coordinates + at_0_y = np.where(self.down[:,1] == 0) + self.down = np.delete(self.down,at_0_y, 0) + + self.fixed_coordinates = np.r_[walls_coordinates, self.down, self.up] + + + + + def SetUpFreeFormDeformation(self): + #creating a free form deformation object for each control domain + self.ffd_up = FFD([2,5,2]) #3D box of control points + self.ffd_down = FFD([2,5,2]) #3D box of control points + + #setting the centre and size of the upper box of control points + self.ffd_down.box_origin = np.array([1.25, 0, 0.5]) + self.ffd_down.box_length = np.array([1, 1.25, 1]) + + #setting the centre and size of the lower box of control points + self.ffd_up.box_origin = np.array([1.25, 1.75, 0.5]) + self.ffd_up.box_length = np.array([1, 1.25, 1]) + + self.list_of_ffds = [self.ffd_up, self.ffd_down] + + + + + def MoveControlPoints(self, scale_of_deformation=1): + + self.ffd_down.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + + self.ffd_down.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + self.ffd_up.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[0, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[0, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + + self.ffd_up.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[1, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[1, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + moved_up = self.ffd_up(self.up) + moved_down = self.ffd_down(self.down) + + + #Moving lower part + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + i=0 + for node in control_down.Nodes: + if node.Y0 != 0: + print(node.Y0) + x_disp = moved_down[i,0] - node.X0 + y_disp = moved_down[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + #moving upper part + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + i=0 + for node in control_up.Nodes: + if node.Y0 != 3: + print(node.Y0) + x_disp = moved_up[i,0] - node.X0 + y_disp = moved_up[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.moved_coordinates = np.r_[self.walls, moved_down, moved_up] + + + + def UpdateRBF(self): + self.rbf = RBF(original_control_points = self.fixed_coordinates, deformed_control_points = + self.moved_coordinates, radius=0.75) + + + def LockOuterWalls(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0 ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + if self.time>1.0 and self.time<16.0: # start modifying narrowing from 1 second onwards + self.deformation_multiplier+=.1 + elif self.time>21.0 and self.time<36: + self.deformation_multiplier-=.1 + + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width + + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + +def Train_ROM(): + with open("ProjectParameters.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + + global_model = KratosMultiphysics.Model() + simulation = FOM_Class(global_model, parameters) + simulation.Run() + return simulation.GetBifuracationData() + + + + + + + +if __name__ == "__main__": + #Train_ROM() + vy, w = Train_ROM() + + plt.plot(vy, w, 'k-', label = 'FOM', linewidth = 3) + plt.legend() + plt.xlabel('velocity y', size=20) + plt.ylabel('narrowing w',size=20) + plt.show() diff --git a/rom_application/ContractionExpansionChannel/FFD_plus_RBF/ProblemFiles/NonlinearInGiD.mdpa b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/NonlinearInGiD.mdpa similarity index 100% rename from rom_application/ContractionExpansionChannel/FFD_plus_RBF/ProblemFiles/NonlinearInGiD.mdpa rename to rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/NonlinearInGiD.mdpa diff --git a/rom_application/ContractionExpansionChannel/FFD_plus_RBF/ProblemFiles/ProjectParameters.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/ProjectParameters.json similarity index 100% rename from rom_application/ContractionExpansionChannel/FFD_plus_RBF/ProblemFiles/ProjectParameters.json rename to rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/ProjectParameters.json diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/ROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/ROM_TestTrajectory.py new file mode 100644 index 00000000..600b9745 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/ROM_TestTrajectory.py @@ -0,0 +1,152 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + +import KratosMultiphysics.RomApplication as romapp +import json + +import numpy as np + + +#importing PyGeM tools +from pygem import FFD, RBF + +import os + + + + + + + + + + + +class ROM_Class_test(ROM_Class): + + def __init__(self, model, project_parameters, correct_cluster = None, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, hrom) + self.deformation_multiplier = 11 + + + + + def UpdateDeformationMultiplier(self): + #### Test trajectory#### + if self.time>10.0 and self.time<=21.0: # start modifying narrowing from 1 second onwards + self.deformation_multiplier-=self.delta_deformation + if self.deformation_multiplier < self.minimum: + self.deformation_multiplier = self.minimum + elif self.time>31.0 and self.time<41.9: + self.deformation_multiplier+=self.delta_deformation + if self.deformation_multiplier > self.maximum: + self.deformation_multiplier = self.maximum + + + + def InitializeSolutionStep(self): + super(ROM_Class, self).InitializeSolutionStep() + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + + + + +def prepare_files(working_path, svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_test_{svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(svd_truncation_tolerance): + + + if not os.path.exists(f'./Results/ROM_test_{svd_truncation_tolerance}.post.bin'): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class_test(global_model, parameters) + simulation.Run() + + + np.save(f'Results/ROM_snapshots_test_{svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom, deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_ROM_test_{svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_ROM_test_{svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_ROM_test_{svd_truncation_tolerance}.npy', deformation_multiplier) + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path, svd_truncation_tolerance) + + + ROM(svd_truncation_tolerance) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/Run_HROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/Run_HROM.py new file mode 100644 index 00000000..28bc60c8 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/Run_HROM.py @@ -0,0 +1,102 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + +import KratosMultiphysics.RomApplication as romapp +import json + + +import os +import numpy as np + + + +class HROMClass(ROM_Class): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance,hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 5152 + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + + + if not os.path.exists(f'./Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom, deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', deformation_multiplier) + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/Run_ROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/Run_ROM.py new file mode 100644 index 00000000..65f59ec1 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/Run_ROM.py @@ -0,0 +1,465 @@ +import KratosMultiphysics +from KratosMultiphysics.RomApplication.fluid_dynamics_analysis_rom import FluidDynamicsAnalysisROM + +import os.path + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np + + +#importing PyGeM tools +from pygem import FFD, RBF + + + + + + + +class ROM_Class(FluidDynamicsAnalysisROM): + + def __init__(self, model, project_parameters, correct_cluster = None, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, hrom) + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.delta_deformation = time_step_size # this ensures to obtain the same deformation independently of the time step used + self.control_point = 854 #a node around the middle of the geometry to capture the bufurcation + self.maximum = 11 + self.minimum = 0 + ### ### ### + self.node_up = 412 #nodes to obtain the narrowing width + self.node_down = 673 + ### ### ### + self.deformation_multiplier_list = [] + self.time_step_solution_container = [] + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.matrix_of_free_coordinates = None + self.deformation_multiplier = 0 + + + def MoveInnerNodesWithRBF(self): + # first loop, ONLY ENTERED ONCE + if self.matrix_of_free_coordinates is None: + x_original = [] + y_original = [] + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(-1,1) + y_original = np.array(y_original).reshape(-1,1) + self.matrix_of_free_coordinates = np.c_[x_original, y_original, np.ones((y_original.shape[0],1))] + self.matrix_of_modified_coordinates = self.rbf(self.matrix_of_free_coordinates) + + # second loop + i = 0 + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = self.matrix_of_modified_coordinates[i,0] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = self.matrix_of_modified_coordinates[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + node = self.model.GetModelPart("FluidModelPart").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.deformation_multiplier_list.append(self.deformation_multiplier) + node_up = self.model.GetModelPart("FluidModelPart").GetNode(self.node_up) + node_down = self.model.GetModelPart("FluidModelPart").GetNode(self.node_down) + self.narrowing_width.append(node_up.Y - node_down.Y) + + + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.IdentifyNodes() + self.SetUpFreeFormDeformation() + + + + def IdentifyNodes(self): + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + fixed_walls= self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls") + + number_of_nodes_walls = fixed_walls.NumberOfNodes() + number_of_nodes_down = control_down.NumberOfNodes() + number_of_nodes_up = control_down.NumberOfNodes() + + #get matrix of original coordinates + walls_coordinates = np.ones((int(number_of_nodes_walls),3)) + up_coordinates = np.ones((int(number_of_nodes_up),3)) + down_coordinates = np.ones((int(number_of_nodes_down),3)) + + counter = 0 + for node in control_down.Nodes: + down_coordinates[counter, 0] = node.X0 + down_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in control_up.Nodes: + up_coordinates[counter, 0] = node.X0 + up_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in fixed_walls.Nodes: + walls_coordinates[counter, 0] = node.X0 + walls_coordinates[counter, 1] = node.Y0 + counter+=1 + + self.walls = walls_coordinates + + self.up = up_coordinates + at_3_y = np.where(self.up[:,1] == 3) + self.up = np.delete(self.up,at_3_y, 0) + + self.down = down_coordinates + at_0_y = np.where(self.down[:,1] == 0) + self.down = np.delete(self.down,at_0_y, 0) + + self.fixed_coordinates = np.r_[walls_coordinates, self.down, self.up] + + + + + def SetUpFreeFormDeformation(self): + #creating a free form deformation object for each control domain + self.ffd_up = FFD([2,5,2]) #3D box of control points + self.ffd_down = FFD([2,5,2]) #3D box of control points + + #setting the centre and size of the upper box of control points + self.ffd_down.box_origin = np.array([1.25, 0, 0.5]) + self.ffd_down.box_length = np.array([1, 1.25, 1]) + + #setting the centre and size of the lower box of control points + self.ffd_up.box_origin = np.array([1.25, 1.75, 0.5]) + self.ffd_up.box_length = np.array([1, 1.25, 1]) + + self.list_of_ffds = [self.ffd_up, self.ffd_down] + + + + + def MoveControlPoints(self, scale_of_deformation=1): + + self.ffd_down.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + + self.ffd_down.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + self.ffd_up.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[0, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[0, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + + self.ffd_up.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[1, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[1, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + moved_up = self.ffd_up(self.up) + moved_down = self.ffd_down(self.down) + + + #Moving lower part + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + i=0 + for node in control_down.Nodes: + if node.Y0 != 0: + x_disp = moved_down[i,0] - node.X0 + y_disp = moved_down[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + #moving upper part + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + i=0 + for node in control_up.Nodes: + if node.Y0 != 3: + x_disp = moved_up[i,0] - node.X0 + y_disp = moved_up[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.moved_coordinates = np.r_[self.walls, moved_down, moved_up] + + + + def UpdateRBF(self): + self.rbf = RBF(original_control_points = self.fixed_coordinates, deformed_control_points = + self.moved_coordinates, radius=0.75) + + + def LockOuterWalls(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0 ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + + def UpdateDeformationMultiplier(self): + ####Train trajectory#### + if self.time>10.0 and self.time<=21.0: # start modifying narrowing from 10 seconds onwards + self.deformation_multiplier+=self.delta_deformation + if self.deformation_multiplier > self.maximum: + self.deformation_multiplier = self.maximum + elif self.time>31.0 and self.time<41.9: # start modifying narrowing from 10 seconds onwards + self.deformation_multiplier-=self.delta_deformation + if self.deformation_multiplier < self.minimum: + self.deformation_multiplier = self.minimum + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width, self.deformation_multiplier_list + + + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + +def prepare_files(working_path, svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_{svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(svd_truncation_tolerance): + + if not os.path.exists(f'./Results/ROM_{svd_truncation_tolerance}.post.bin'): + + basis = f'ROM/{svd_truncation_tolerance}.npy' + + if os.path.exists(basis): + u = np.load(basis) + else: + if not os.path.exists(f'./ROM/'): + os.mkdir(f'./ROM/') + u,s,_,_ = RandomizedSingularValueDecomposition().Calculate(np.load(f'Results/SnapshotMatrix.npy'), svd_truncation_tolerance) + np.save(basis,u) + + ### Saving the nodal basis ### (Need to make this more robust, hard coded here) + basis_POD={"rom_settings":{},"nodal_modes":{}} + basis_POD["rom_settings"]["nodal_unknowns"] = ["VELOCITY_X","VELOCITY_Y","PRESSURE"] + basis_POD["rom_settings"]["number_of_rom_dofs"] = np.shape(u)[1] + Dimensions = len(basis_POD["rom_settings"]["nodal_unknowns"]) + N_nodes=np.shape(u)[0]/Dimensions + N_nodes = int(N_nodes) + node_Id=np.linspace(1,N_nodes,N_nodes) + i = 0 + for j in range (0,N_nodes): + basis_POD["nodal_modes"][int(node_Id[j])] = (u[i:i+Dimensions].tolist()) + i=i+Dimensions + + with open('ProblemFiles/RomParameters.json', 'w') as f: + json.dump(basis_POD,f, indent=2) + + print('\n\nNodal basis printed in json format\n\n') + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class(global_model, parameters) + simulation.Run() + + np.save(f'Results/ROM_snapshots_{svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom,w_rom,deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_ROM_{svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_ROM_{svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_{svd_truncation_tolerance}.npy', deformation_multiplier) + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + prepare_files(working_path, svd_truncation_tolerance) + + ROM(svd_truncation_tolerance) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/TrainHROM_Step1.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/TrainHROM_Step1.py new file mode 100644 index 00000000..3fe72a60 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/TrainHROM_Step1.py @@ -0,0 +1,104 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + + +import KratosMultiphysics.RomApplication as romapp +import json +import numpy as np + + + + +import os.path + + +class TrainHROMClass(ROM_Class): + + def __init__(self, model, project_parameters,svd_truncation_tolerance): + super().__init__(model, project_parameters, hrom="EmpiricalCubature") + self.svd_truncation_tolerance = svd_truncation_tolerance + + + + + + + +def Train_HROM(svd_truncation_tolerance): + + projected_residuals = f'HROM/Sr_{svd_truncation_tolerance}.npy' + + + if not os.path.exists(projected_residuals): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + #loading the bases + bases = [] + bases = None + simulation = TrainHROMClass(global_model, parameters, svd_truncation_tolerance) + simulation.Run() + + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path) + + Train_HROM(svd_truncation_tolerance) + + # np.save(f'Results/y_velocity_{Number_Of_Clusters}_clusters.npy', vy_rom) + # np.save(f'Results/narrowing_{Number_Of_Clusters}_clusters.npy', w_rom) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/TrainHROM_Step2.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/TrainHROM_Step2.py new file mode 100644 index 00000000..f7d869c0 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/TrainHROM_Step2.py @@ -0,0 +1,76 @@ +import numpy as np +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition +from matplotlib import pyplot as plt + +import os.path + +def get_global_norm(number_bases): + norm = 0 + for i in range(number_bases): + norm_a = np.linalg.norm(np.load(f'HROM/Sr_{i}.npy')) + norm = np.sqrt(np.power(norm_a, 2) + np.power(norm, 2)) + return norm + + +def get_bases(number_bases, global_norm, tol, relative=False): + bases = [] + for i in range(number_bases): + if relative: + u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=False).Calculate( np.load(f'HROM/Sr_{i}.npy'), tol* global_norm) #* global_norm + else: + u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr_{i}.npy'), tol) #* global_norm + bases.append(u) + + return bases + +def select_elements(svd_truncation_tolerance, residuals_svd_truncation_tolerance): + + weights = f'HROM/WeightsMatrix_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + elements = f'HROM/Elementsvector_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + + if not os.path.exists(weights) and not os.path.exists(elements): + #u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr.npy'), tol) # HEAVY!!! + u = np.load(f'HROM/basis_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy') + + hyper_reduction_element_selector = EmpiricalCubatureMethod() + hyper_reduction_element_selector.SetUp(u) #add again z + hyper_reduction_element_selector.Initialize() + hyper_reduction_element_selector.Calculate() + + + w = np.squeeze(hyper_reduction_element_selector.w) + z = np.squeeze(hyper_reduction_element_selector.z) + + WeightsMatrix = w.reshape(np.size(z),1) + + np.save(weights, WeightsMatrix ) + np.save(elements, z) + + +def get_basis(svd_truncation_tolerance, tol): + + basis = f'HROM/basis_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + + if not os.path.exists(basis): + u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr_{svd_truncation_tolerance}.npy'), tol) + np.save( basis,u) + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance = float(argv[7]) + residuals_svd_relative_to_global_residuals_snapshots = bool(argv[8]) + + + get_basis(svd_truncation_tolerance, residuals_svd_truncation_tolerance) + select_elements(svd_truncation_tolerance, residuals_svd_truncation_tolerance) + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/overlapping_strategies.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/overlapping_strategies.py new file mode 100644 index 00000000..638238bf --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/overlapping_strategies.py @@ -0,0 +1,323 @@ +import numpy as np +from matplotlib import pyplot as plt +from sklearn.cluster import KMeans + +def time_clustering(S, time_clusters = 3, overlaping_snapshots = 1 ): + total_time_steps = S.shape[1] + if time_clusters > total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #get list containing snapshots to add to each overlapped cluster + if overlaping_snapshots is not 0: + snapshots_to_add = {} + for i in range(time_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == time_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(time_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + + +def ismember(A, B): + if isinstance(A, np.int_): + return [ np.sum(A == B) ] + else: + return [ np.sum(a == B) for a in A ] + +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + kmeans = KMeans(n_clusters=narrowing_clusters, random_state=0).fit(narrowing.reshape(-1,1)) + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(narrowing_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + correct_cluster = kmeans.labels_ + centroids = kmeans.cluster_centers_ + + if narrowing_clusters>1: + #try and use as is solution manifold neighbor identification + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + narrowing = narrowing.reshape(1,-1) + for i in range(np.shape(narrowing)[1]): + this_matrix = (kmeans.cluster_centers_).T - narrowing[:,i].reshape(np.shape(narrowing)[0], 1) + distance = np.zeros((narrowing_clusters)) + for j in range(narrowing_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + #get list containing snapshots to add to each overlapped cluster + if True: + #if overlaping_snapshots is not 0: + + snapshots_to_add = [] + for j in range(narrowing_clusters): + N_neighbors = len(neighbors[j]) + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + ith_narrowing_cluster = narrowing[:,kmeans.labels_==neighbors[j][i]] + this_matrix = ith_narrowing_cluster - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(narrowing)[0], 1) + distance = np.linalg.norm(this_matrix, axis = 0) + #distance = np.zeros(np.shape(ith_narrowing_cluster[1])) + #for k in range(len(distance)): + # distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + + return sub_snapshots, correct_cluster + + +def solution_manifold_clustering(): + pass + + + +if __name__=='__main__': + #S = np.load('SnapshotMatrix.npy') + #narrowing = np.load('narrowing.npy') + narrowing = np.linspace(0,1,12) + S = np.array([[1,2,3,4,5,6,7,8,9,10,11,12],[1,2,3,4,5,6,7,8,9,10,11,12]]) + #a = narrowing.reshape(1,-1) + #S = np.r_[a, a , a, a] + sub_snapshots, correct_cluster = time_clustering(S, 3,0) + #sub_snapshots, correct_cluster = narrowing_clustering(S, narrowing, 3, 2) + #sub_snapshots, correct_cluster = solution_manifold_clustering(S) + #sub_snapshots, correct_cluster = time_clustering(S) + kkk = 5 + + # + + +""" + +def solution_manifold_clustering(S, solution_manifold_clusters = 3, overlaping_snapshots = 1 ): + #S = np.load('SnapshotMatrix.npy') + kmeans = KMeans(n_clusters = solution_manifold_clusters, random_state=0).fit(S.T) + correct_cluster = kmeans.labels_ + + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(solution_manifold_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + for i in range(np.shape(S)[1]): + this_matrix = (kmeans.cluster_centers_).T - S[:,i].reshape(np.shape(S)[0], 1) + distance = np.zeros((solution_manifold_clusters)) + for j in range(solution_manifold_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + snapshots_to_add = [] + + for j in range(solution_manifold_clusters): + N_snaps = np.shape(sub_snapshots[j])[1] + N_neighbors = len(neighbors[j]) + + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + this_matrix = sub_snapshots[neighbors[j][i]] - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(S)[0], 1) + distance = np.zeros(np.shape(sub_snapshots[neighbors[j][i]][1])) + for k in range(len(distance)): + distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(solution_manifold_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + + +""" +This is wrong, but save for now as reference +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + # wrong implementation :( + # MINE (no k-means) + #S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + #narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + correct_cluster = np.empty(narrowing.shape) + for i in range(narrowing_clusters): + # In this implementation, I just shuffle (order) the snapshots to match the narrowing width. No time-relation whatsoever + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + correct_cluster[intersection] = i + ith_narrowing = narrowing[intersection] + ith_indexes_ordered = np.argsort(ith_narrowing) + sub_snapshots[i] = S[:,ith_indexes_ordered] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + # storing centroids + if i==0: + centroids = np.sum(ith_narrowing)/(ith_narrowing.shape[0]) + else: + centroids = np.c_[centroids, np.sum(ith_narrowing)/(ith_narrowing.shape[0])] + np.save('cluster_centroid.npy', centroids) + #overlapping after correct cluster definition + + #get list containing snapshots to add to each overlapped cluster + snapshots_to_add = {} + for i in range(narrowing_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == narrowing_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + +""" +def time_clustering(time_clusters = 5, overlaping_snapshots = 1 ): + #it works, but no overlapping + S = np.load('SnapshotMatrix.npy') + total_time_steps = S.shape[1] + if time_clusters > total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + + return sub_snapshots, correct_cluster +""" + + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + #no overlapping. MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + return sub_snapshots, correct_cluster +""" + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + # MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + #overlapping after correct cluster definition + # In this implementation, I just shuffle the snapshots to match the narrowing width. No time relation whatsoever + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + if i == 0: + ith_narrowing = narrowing[intersection] + + ith_indexes = np.argsort(ith_narrowing) + ith_narrowing_ordered = ith_narrowing[ith_indexes] + plt.plot(ith_narrowing, 'b') + plt.plot(ith_narrowing_ordered, 'r') + plt.show() + + elif i == narrowing_clusters-1: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + else: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + sub_snapshots[i] = np.c_[sub_snapshots[i] , sub_snapshots[i+1][:, :overlaping_snapshots] ] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster +""" + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/plot_bifurcation.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/plot_bifurcation.py new file mode 100644 index 00000000..8b56aa1e --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/plot_bifurcation.py @@ -0,0 +1,65 @@ +import numpy as np +from matplotlib import pyplot as plt + + + +if __name__=='__main__': + #library for passing arguments to the script from bash + from sys import argv + + + Number_Of_Clusters= int(argv[1]) + + + + vy = np.load('Results/Velocity_y.npy') + w = np.load('Results/narrowing.npy') + vy_rom = np.load(f'Results/y_velocity_ROM.npy') + w_rom = np.load(f'Results/narrowing_ROM.npy') + + + #plt.title(r'Singular Values for matrix $ S^{(2)} $', fontsize=15, fontweight='bold') + #plt.title(r'$\alpha $ \textbf{AA}!', fontsize=16, color='r') + #plt.title(f'ROM VS FOM') + + plt.rc('text', usetex=True) + plt.rc('font', family='serif') + + plt.plot(vy, w, 'b', label = 'FOM', linewidth = 3, alpha=0.5) #linewidth = 3 + plt.plot(vy_rom, w_rom, 'r', label = 'ROM', linewidth = 3, alpha=0.5) + #plt.title(r'FOM vs ROM', fontsize=20, fontweight='bold') + plt.legend() + #plt.grid() + # plt.xticks(np.arange(-3.5,0.25,0.25)) #TODO the ticks are not easily beautyfied, do it later :) + # plt.yticks(np.arange(0,3.1,0.25)) + plt.xlabel(r'$v_y^*$', size=15, fontweight='bold') + plt.ylabel(r'$w_c$',size=15,fontweight='bold') + + plt.savefig('Results/fom_vs_rom') + plt.show() + + + + + # import numpy as np + # import matplotlib.pyplot as plt + + + # # Example data + # t = np.arange(0.0, 1.0 + 0.01, 0.01) + # s = np.cos(4 * np.pi * t) + 2 + + # plt.rc('text', usetex=True) + # plt.rc('font', family='serif') + # plt.plot(t, s) + + # plt.xlabel(r'\textbf{time} (s)') + # plt.ylabel(r'\textit{voltage} (mV)',fontsize=16) + # plt.title(r"\TeX\ is Number " + # r"$\displaystyle\sum_{n=1}^\infty\frac{-e^{i\pi}}{2^n}$!", + # fontsize=16, color='gray') + # # Make room for the ridiculously large title. + # plt.subplots_adjust(top=0.8) + + # plt.savefig('tex_demo') + # plt.show() \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/plot_full_bifurcation.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/plot_full_bifurcation.py new file mode 100644 index 00000000..9c96c6c6 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/ProblemFiles/plot_full_bifurcation.py @@ -0,0 +1,31 @@ +import numpy as np +from matplotlib import pyplot as plt + + + +if __name__=='__main__': + + + vy = np.load('Results/Velocity_y.npy') + w = np.load('Results/narrowing.npy') + vy_rom = np.load(f'Results/y_velocity_ROM.npy') + w_rom = np.load(f'Results/narrowing_ROM.npy') + vy_hrom = np.load(f'Results/y_velocity_HROM.npy') + w_hrom = np.load(f'Results/narrowing_HROM.npy') + + plt.rc('text', usetex=True) + plt.rc('font', family='serif') + + plt.plot(vy, w, 'b', label = 'FOM', linewidth = 3, alpha=0.5) #linewidth = 3 + plt.plot(vy_rom, w_rom, 'r', label = 'ROM', linewidth = 3, alpha=0.5) + plt.plot(vy_hrom, w_hrom, 'm', label = 'HROM', linewidth = 3, alpha=0.5) + + plt.legend() + #plt.grid() + # plt.xticks(np.arange(-3.5,0.25,0.25)) #TODO the ticks are not easily beautyfied, do it later :) + # plt.yticks(np.arange(0,3.1,0.25)) + plt.xlabel(r'$v_y^*$', size=15, fontweight='bold') + plt.ylabel(r'$w_c$',size=15,fontweight='bold') + + plt.savefig('Results/fom_vs_rom_vs_hrom') + plt.show() \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/launch_ale_rom.sh b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/launch_ale_rom.sh new file mode 100755 index 00000000..0fd2edd5 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example1/Nonaffine/launch_ale_rom.sh @@ -0,0 +1,102 @@ +#!/bin/sh +#SBATCH -N 1 # nodes requested +#SBATCH -n 1 # tasks requested +#SBATCH -c 16 # cores requested +#SBATCH -t 20:00:00 # time requested in hour:minute:second +##### --constraint='highmem' + + +export OMP_NUM_THREADS=16 +export PROBLEMS_PATH=$PWD/ProblemFiles +export LANGUAGE=en_GB.utf8 +export LC_ALL=en_GB.utf8 + + +FOM=True #(storing results) +FOM_test=True #(storing results) +Run_ROM=True #3 (storing results) +ROM_test=True #4 = (storing results) +Train_HROM_Step1=True #5 = (creating projected residuals matrices {Sr_i}_i=1^k (one per basis)) +Train_HROM_Step2=True #6 = ontain a reduced set of elements and weights starting from the projected residuals matrices Sr_i +Run_HROM=True #7 = RunHROM Train Trajectory +HROM_test=True #8 = RunHROM Test Trajectory + +plot_partial_hysteresis=False + +#parameters used in Local POD: + +# parameters for the simulations +Launch_Simulation=1 +Number_Of_Clusters=1 #not used in global POD +svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +clustering="narrowing" #time # +overlapping=30 +residuals_svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +residuals_svd_relative_to_global_residuals_snapshots=1 + + +if [ $FOM = True ] + then + #### LAUNCH FOM TRAIN TRAJECTORY #### + # MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLauching FOM \n\n\n\n\n\n" + python3 ProblemFiles/FOM.py $PWD +fi +if [ $FOM_test = True ] + then + # NEW MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching FOM test trajectory \n\n\n\n\n\n" + python3 ProblemFiles/FOM_TestTrajectory.py $PWD +fi +for j in ${svd_truncation_tolerance_list[@]} +do + svd_truncation_tolerance=$j + if [ $Run_ROM = True ] + then + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching ROM \n\n\n\n\n\n" + python3 ProblemFiles/Run_ROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $ROM_test = True ] + then + #### LAUNCH ROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\nlaunching ROM test\n\n\n\n' + python3 ProblemFiles/ROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $Train_HROM_Step1 = True ] + then + #### TrainHROM (Creating Matrix of projected resduals Sr) #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\nlaunching TrainHROM train\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step1.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + for k in ${residuals_svd_truncation_tolerance_list[@]} + do + residuals_svd_truncation_tolerance=$k + if [ $Train_HROM_Step2 = True ] + then + ### Obtain Reduced Elements and Weights #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nlaunching HROM elements and Weights\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step2.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $Run_HROM = True ] + then + #### LAUNCH HROM TRAIN TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nLaunching HROM train\n\n\n\n\n\n\n' + python3 ProblemFiles/Run_HROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $HROM_test = True ] + then + #### LAUNCH HROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo 'Launching HROM test' + python3 ProblemFiles/HROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + done +done + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/.ipynb_checkpoints/Untitled-checkpoint.ipynb b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/.ipynb_checkpoints/Untitled-checkpoint.ipynb new file mode 100644 index 00000000..73bc0b45 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/.ipynb_checkpoints/Untitled-checkpoint.ipynb @@ -0,0 +1,74 @@ +{ + "cells": [ + { + "cell_type": "code", + "execution_count": null, + "id": "bbeaaa45", + "metadata": {}, + "outputs": [], + "source": [ + "# Copy the RomPython folder to your own drive and run this cell to use the notebook in google colab\n", + "\n", + "from google.colab import drive\n", + "drive.mount('/content/drive/')" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "a2a6c2f6", + "metadata": {}, + "outputs": [], + "source": [ + "!pip install KratosMultiphysics\n", + "!pip install KratosRomApplication\n", + "!pip install KratosStructuralMechanicsApplication\n", + "!pip install KratosLinearSolversApplication\n", + "!pip install KratosConstitutiveLawsApplication" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "af25d338", + "metadata": {}, + "outputs": [], + "source": [ + "from KratosMultiphysics.StructuralMechanicsApplication.structural_mechanics_analysis import StructuralMechanicsAnalysis\n", + "from KratosMultiphysics.RomApplication.rom_testing_utilities import SetUpSimulationInstance\n", + "import KratosMultiphysics" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "98750e24", + "metadata": {}, + "outputs": [], + "source": [ + "with open(\"/content/drive/MyDrive/WinterSchool2023_Examples_test/stanford_bunny/ProjectParameters.json\",'r') as parameter_file:\n", + " parameters = KratosMultiphysics.Parameters(parameter_file.read())\n", + "model = KratosMultiphysics.Model()\n", + "simulation = StructuralMechanicsAnalysis(model,parameters)\n", + "simulation.Run()" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "e5bd6eb5", + "metadata": {}, + "outputs": [], + "source": [] + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 3", + "language": "python", + "name": "python3" + } + }, + "nbformat": 4, + "nbformat_minor": 5 +} diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc.mdpa b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc.mdpa new file mode 100644 index 00000000..eab2848c --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc.mdpa @@ -0,0 +1,18765 @@ +Begin 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100644 index 00000000..46e2c6b3 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/FOM.py @@ -0,0 +1,274 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis + +import json + +import numpy as np + +#for checking if paths exits +import os + +#importing training trajectory +from simulation_trajectories import TrainingTrajectory + + + +class FOM_Class(FluidDynamicsAnalysis): + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.time_step_solution_container = [] + self.reynolds_number_container = [] + + + def InitialMeshPosition(self): + self.training_trajectory = TrainingTrajectory(self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble()) + self.w = self.training_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.InitialMeshPosition() + + + + def MovePart(self, part_name, jacobian, centering_vector, extra_centering): + x_original = [] + y_original = [] + # first loop + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(1,-1) + y_original = np.array(y_original).reshape(1,-1) + matrix_of_coordinates = np.r_[x_original, y_original] + modified_matrix_of_coordinates = np.linalg.inv(jacobian) @ (matrix_of_coordinates - centering_vector) + modified_matrix_of_coordinates += centering_vector + extra_centering #re-locating + # second loop + i = 0 + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = modified_matrix_of_coordinates[0,i] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = modified_matrix_of_coordinates[1,i] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_Meassure").Nodes: + pass + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.narrowing_width.append(self.w) + + + def MoveAllPartsAccordingToW(self): + ############################# + #### FREE ALL NODES #### + ############################# + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + #### FIXING OUTSIDE PART #### + ############################# + for node in self.model.GetModelPart("FluidModelPart.GENERIC_not_moving").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + ### MOVE EACH SUB-PART ### + ############################# + self.MovePart('GENERIC_green', np.array([[1,0],[0,1/self.w]]), np.array([[0],[1.5]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_up', np.array([[1,0],[0, (2/(3-self.w))]]), np.array([[0],[3]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_down', np.array([[1,0],[0, 2/(3-self.w)]]), np.array([[0],[0]]), np.array([[0],[0]])) + self.MovePart('GENERIC_blue', np.array([[1,0],[(self.w-1)/2, 1]]), np.array([[0],[0]]), np.array([[0],[(self.w-1)/4]])) + self.MovePart('GENERIC_grey', np.array([[1,0],[(1-self.w)/2, 1]]), np.array([[0],[0]]), np.array([[0],[- (self.w-1)/4]])) + + + + def UpdateNarrowing(self): + self.w = self.training_trajectory.UpdateW(self.w) + + + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + print('The current Reynolds Number is: ', self.GetReynolds()) + + + + def GetReynolds(self): + velocities = [] + for node in self.model.GetModelPart("FluidModelPart.GENERIC_narrowing_zone").Nodes: + velocities.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + vel_np = np.array(velocities) + + vx = np.max(vel_np) #np.mean(vel_np) + Re = (vx*self.w) / 0.1 #TODO retrieve dynamic viscosity in a more robust way + return Re + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + self.reynolds_number_container.append(self.GetReynolds()) + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + def GetBifuracationData(self): + return np.array(self.velocity_y_at_control_point) , np.array(self.narrowing_width) + + def GetReynoldsData(self): + return np.array(self.reynolds_number_container) + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + + + + + + + + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + +def Train_ROM(): + + if not os.path.exists(f'./Results/FOM.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing = simulation.GetBifuracationData() + reynolds = simulation.GetReynoldsData() + np.save('Results/reynolds.npy', reynolds) + np.save('Results/narrowing.npy', narrowing) + np.save('Results/Velocity_y.npy', velocity_y) + np.save('Results/SnapshotMatrix.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + Train_ROM() \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/FOM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/FOM_TestTrajectory.py new file mode 100644 index 00000000..984fac93 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/FOM_TestTrajectory.py @@ -0,0 +1,163 @@ +import KratosMultiphysics +from FOM import FOM_Class + + + +import KratosMultiphysics.RomApplication as romapp +import json + +import numpy as np + +#for checking if paths exits +import os + + +#importing testing trajectory +from simulation_trajectories import TestingTrajectory2 + + +class FOM_Class_test(FOM_Class): + + def InitialMeshPosition(self): + self.testing_trajectory = TestingTrajectory2() + self.w = self.testing_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + + def UpdateNarrowing(self): + self.w = self.testing_trajectory.UpdateW(self.time-10) + + + def InitializeSolutionStep(self): + super(FOM_Class, self).InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + print('The current Reynolds Number is: ', self.GetReynolds()) + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM_test' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + + + + + +def FOM_test(): + + if not os.path.exists(f'./Results/FOM_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class_test(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing = simulation.GetBifuracationData() + reynolds = simulation.GetReynoldsData() + np.save('Results/reynolds_test.npy', reynolds) + np.save('Results/narrowing_test.npy', narrowing) + np.save('Results/Velocity_y_test.npy', velocity_y) + np.save('Results/SnapshotMatrix_test.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + FOM_test() + + + + + + + + + + + + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/FluidMaterials.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/FluidMaterials.json new file mode 100644 index 00000000..24e1bedf --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/FluidMaterials.json @@ -0,0 +1,16 @@ +{ + "properties" : [{ + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "properties_id" : 1, + "Material" : { + "constitutive_law" : { + "name" : "Newtonian2DLaw" + }, + "Variables" : { + "DENSITY" : 1.0, + "DYNAMIC_VISCOSITY" : 0.1 + }, + "Tables" : {} + } + }] +} diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/HROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/HROM_TestTrajectory.py new file mode 100644 index 00000000..e3ade411 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/HROM_TestTrajectory.py @@ -0,0 +1,126 @@ +import KratosMultiphysics +from ROM_TestTrajectory import ROM_Class_test + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt +import os + + + + + + +class HROMClass_test(ROM_Class_test): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 4916 #TODO, get rid of this, load both elements and condition sets + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + + + + + + + + + + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass_test(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + + vy_rom, w_rom = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + + + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}_test' + updated_project_parameters["output_processes"]["vtk_output"][0]["Parameters"]["output_path"] = working_path +f'/Results/vtk_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}_test' + + + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/ProjectParameters.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/ProjectParameters.json new file mode 100644 index 00000000..c4bc9c92 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/ProjectParameters.json @@ -0,0 +1,162 @@ +{ + "analysis_stage": "KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis", + "problem_data" : { + "problem_name" : "2DFlowBifurcationKratosStructuredMeshWorkingRicc", + "parallel_type" : "OpenMP", + "echo_level" : 0, + "start_time" : 0.0, + "end_time" : 244 + }, + "output_processes" : { + "gid_output" : [{ + "python_module" : "gid_output_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "GiDOutputProcess", + "help" : "This process writes postprocessing files for GiD", + "Parameters" : { + "model_part_name" : "FluidModelPart.fluid_computational_model_part", + "output_name" : "2DFlowBifurcationKratosStructuredMeshWorkingRicc", + "postprocess_parameters" : { + "result_file_configuration" : { + "gidpost_flags" : { + "GiDPostMode" : "GiD_PostBinary", + "WriteDeformedMeshFlag" : "WriteDeformed", + "WriteConditionsFlag" : "WriteConditions", + "MultiFileFlag" : "SingleFile" + }, + "file_label" : "time", + "output_control_type" : "time", + "output_interval" : 0.5, + "body_output" : true, + "node_output" : false, + "skin_output" : false, + "plane_output" : [], + "nodal_results" : ["VELOCITY","PRESSURE","MESH_DISPLACEMENT"], + "gauss_point_results" : [], + "nodal_nonhistorical_results" : [] + }, + "point_data_configuration" : [] + } + } + }], + "vtk_output" : [{ + "python_module" : "vtk_output_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "VtkOutputProcess", + "help" : "This process writes postprocessing files for Paraview", + "Parameters" : { + "model_part_name" : "FluidModelPart.fluid_computational_model_part", + "output_control_type" : "step", + "output_interval" : 1, + "file_format" : "binary", + "output_precision" : 7, + "output_sub_model_parts" : false, + "output_path" : "vtk_output", + "save_output_files_in_folder" : true, + "nodal_solution_step_data_variables" : ["VELOCITY","PRESSURE"], + "nodal_data_value_variables" : [], + "element_data_value_variables" : ["HROM_WEIGHT"], + "condition_data_value_variables" : [], + "gauss_point_variables_extrapolated_to_nodes" : [] + } + }], + "rom_output" : [] + }, + "solver_settings" : { + "solver_type": "ale_fluid", + "ale_boundary_parts": [], + "mesh_motion_solver_settings" : { + "solver_type" : "structural_similarity" + }, + "fluid_solver_settings": { + "model_part_name" : "FluidModelPart", + "domain_size" : 2, + "solver_type" : "Monolithic", + "model_import_settings" : { + "input_type" : "mdpa", + "input_filename" : "2DFlowBifurcationKratosStructuredMeshWorkingRicc" + }, + "material_import_settings" : { + "materials_filename" : "FluidMaterials.json" + }, + "echo_level" : 0, + "compute_reactions" : false, + "maximum_iterations" : 10, + "relative_velocity_tolerance" : 1e-8, + "absolute_velocity_tolerance" : 1e-8, + "relative_pressure_tolerance" : 1e-8, + "absolute_pressure_tolerance" : 1e-8, + "volume_model_part_name" : "FluidParts_Volume", + "skin_parts" : ["Outlet2D_Outlet","NoSlip2D_Wall"], + "no_skin_parts" : ["VelocityConstraints2D_Inlet-Total"], + "time_scheme" : "bdf2", + "time_stepping" : { + "automatic_time_step" : false, + "time_step" : 0.1 + }, + "formulation" : { + "element_type" : "weakly_compressible", + "dynamic_tau" : 1.0 + }, + "reform_dofs_at_each_step" : false + } + }, + "processes" : { + "initial_conditions_process_list" : [], + "boundary_conditions_process_list" : [{ + "python_module" : "apply_outlet_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyOutletProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.Outlet2D_Outlet", + "variable_name" : "PRESSURE", + "constrained" : true, + "value" : 0.0, + "hydrostatic_outlet" : false, + "h_top" : 0.0 + } + },{ + "python_module" : "apply_noslip_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyNoSlipProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.NoSlip2D_Wall" + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name" : "VELOCITY", + "interval" : [0.0,1], + "constrained" : [true,true,true], + "value" : ["y*(3-y)*sin(pi*t*0.5)",0.0,0.0] + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name" : "VELOCITY", + "interval" : [0.0,"End"], + "constrained" : [true,true,true], + "value" : ["y*(3-y)",0.0,0.0] + } + }], + "gravity" : [{ + "python_module" : "assign_vector_by_direction_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorByDirectionProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "variable_name" : "BODY_FORCE", + "modulus" : 0.0, + "constrained" : false, + "direction" : [0.0,-1.0,0.0] + } + }], + "auxiliar_process_list" : [] + } +} diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/ROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/ROM_TestTrajectory.py new file mode 100644 index 00000000..4a93c581 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/ROM_TestTrajectory.py @@ -0,0 +1,145 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + + +import KratosMultiphysics.RomApplication as romapp +import json + + +import numpy as np +import os + + +#importing testing trajectory +from simulation_trajectories import TestingTrajectory2 + + + +class ROM_Class_test(ROM_Class): + + + def InitialMeshPosition(self): + self.testing_trajectory = TestingTrajectory2() + self.w = self.testing_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + + + def UpdateNarrowing(self): + self.w = self.testing_trajectory.UpdateW(self.time-10) + + + + + def InitializeSolutionStep(self): + super(ROM_Class, self).InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + + + + + + + + + + + + + + + + + +def prepare_files(working_path,svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_{svd_truncation_tolerance}_test' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(hard_impose_currect_cluster = False, Number_Of_Clusters=1, svd_truncation_tolerance=1e-4): + + + if not os.path.exists(f'./Results/ROM_{svd_truncation_tolerance}_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class_test(global_model, parameters, correct_clusters, hard_impose_currect_cluster, bases) + simulation.Run() + np.save(f'Results/ROM_snapshots_{svd_truncation_tolerance}_test.npy',simulation.GetSnapshotsMatrix()) + vy_rom,w_rom = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_ROM_{svd_truncation_tolerance}_test.npy', vy_rom) + np.save(f'Results/narrowing_ROM_{svd_truncation_tolerance}_test.npy', w_rom) + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path,svd_truncation_tolerance) + + + ROM(hard_impose_currect_cluster = True, Number_Of_Clusters=Number_Of_Clusters, svd_truncation_tolerance=svd_truncation_tolerance) + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/Run_HROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/Run_HROM.py new file mode 100644 index 00000000..1268863d --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/Run_HROM.py @@ -0,0 +1,97 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + +import KratosMultiphysics.RomApplication as romapp +import json + + + +import numpy as np +import os + + + +class HROMClass(ROM_Class): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance,hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 4916 + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.post.bin'): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + vy_rom, w_rom = simulation.GetBifuracationData() + np.save(f'Results/y_velocity_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + updated_project_parameters["output_processes"]["vtk_output"][0]["Parameters"]["output_path"] = working_path +f'/Results/vtk_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/Run_ROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/Run_ROM.py new file mode 100644 index 00000000..73fad925 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/Run_ROM.py @@ -0,0 +1,272 @@ +import KratosMultiphysics +from KratosMultiphysics.RomApplication.fluid_dynamics_analysis_rom import FluidDynamicsAnalysisROM + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np + + + + +import os.path + + + +#importing training trajectory +from simulation_trajectories import TrainingTrajectory + + + + + + + +class ROM_Class(FluidDynamicsAnalysisROM): + + def __init__(self, model, project_parameters, correct_cluster = None, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, hrom) + self.bases = bases + self.w = 1 # original narrowing size + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.delta_w = 0.025 * time_step_size # this ensures to obtain a maximum narrowing size of 2.9 and a minimum of 0.1 + self.maximum = 2.9 + self.minimum = 0.1 + self.control_point = None + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.tttime = 0 #fake time step, useful to impose the correct cluster + self.time_step_solution_container = [] + + + def InitialMeshPosition(self): + self.training_trajectory = TrainingTrajectory() + self.w = self.training_trajectory.SetUpInitialNarrowing() + self.MoveAllPartsAccordingToW() + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.InitialMeshPosition() + + + def MovePart(self, part_name, jacobian, centering_vector, extra_centering): + x_original = [] + y_original = [] + # first loop + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(1,-1) + y_original = np.array(y_original).reshape(1,-1) + matrix_of_coordinates = np.r_[x_original, y_original] + modified_matrix_of_coordinates = np.linalg.inv(jacobian) @ (matrix_of_coordinates - centering_vector) + modified_matrix_of_coordinates += centering_vector + extra_centering #re-locating + # second loop + i = 0 + for node in self.model.GetModelPart(f"FluidModelPart.{part_name}").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = modified_matrix_of_coordinates[0,i] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = modified_matrix_of_coordinates[1,i] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + def MoveAllPartsAccordingToW(self): + ############################# + #### FREE ALL NODES #### + ############################# + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + #### FIXING OUTSIDE PART #### + ############################# + for node in self.model.GetModelPart("FluidModelPart.GENERIC_not_moving").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + ############################# + ### MOVE EACH SUB-PART ### + ############################# + self.MovePart('GENERIC_green', np.array([[1,0],[0,1/self.w]]), np.array([[0],[1.5]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_up', np.array([[1,0],[0, (2/(3-self.w))]]), np.array([[0],[3]]), np.array([[0],[0]])) + self.MovePart('GENERIC_yellow_down', np.array([[1,0],[0, 2/(3-self.w)]]), np.array([[0],[0]]), np.array([[0],[0]])) + self.MovePart('GENERIC_blue', np.array([[1,0],[(self.w-1)/2, 1]]), np.array([[0],[0]]), np.array([[0],[(self.w-1)/4]])) + self.MovePart('GENERIC_grey', np.array([[1,0],[(1-self.w)/2, 1]]), np.array([[0],[0]]), np.array([[0],[- (self.w-1)/4]])) + + + def StoreBifurcationData(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_Meassure").Nodes: + pass + #node = self.model.GetModelPart("Meassure").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.narrowing_width.append(self.w) + + + def UpdateNarrowing(self): + self.w = self.training_trajectory.UpdateW(self.w) + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + if self.time>10.0: # start modifying narrowing from 10 seconds onwards (How long does it take to close????) + self.UpdateNarrowing() + self.MoveAllPartsAccordingToW() + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + self.tttime += 1 + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + +def prepare_files(working_path,svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_{svd_truncation_tolerance}' + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(hard_impose_currect_cluster = False, Number_Of_Clusters=1, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/ROM_{svd_truncation_tolerance}.post.bin'): + if not os.path.exists(f'./ROM/'): + os.mkdir('./ROM') + basis = f'./ROM/Phi_{svd_truncation_tolerance}.npy' + if os.path.exists(basis): + u = np.load(basis) + else: + u,s,_,_ = RandomizedSingularValueDecomposition().Calculate(np.load(f'./Results/SnapshotMatrix.npy'), svd_truncation_tolerance) + np.save(basis,u) + + ### Saving the nodal basis ### (Need to make this more robust, hard coded here) + basis_POD={"rom_settings":{},"nodal_modes":{}} + basis_POD["rom_settings"]["nodal_unknowns"] = ["VELOCITY_X","VELOCITY_Y","PRESSURE"] + basis_POD["rom_settings"]["number_of_rom_dofs"] = np.shape(u)[1] + Dimensions = len(basis_POD["rom_settings"]["nodal_unknowns"]) + N_nodes=np.shape(u)[0]/Dimensions + N_nodes = int(N_nodes) + node_Id=np.linspace(1,N_nodes,N_nodes) + i = 0 + for j in range (0,N_nodes): + basis_POD["nodal_modes"][int(node_Id[j])] = (u[i:i+Dimensions].tolist()) + i=i+Dimensions + + with open('ProblemFiles/RomParameters.json', 'w') as f: + json.dump(basis_POD,f, indent=2) + + print('\n\nNodal basis printed in json format\n\n') + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class(global_model, parameters, correct_clusters, hard_impose_currect_cluster, bases) + simulation.Run() + np.save(f'./Results/ROM_snapshots_{svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom = simulation.GetBifuracationData() + + np.save(f'./Results/y_velocity_ROM_{svd_truncation_tolerance}.npy', vy_rom) + np.save(f'./Results/narrowing_ROM_{svd_truncation_tolerance}.npy', w_rom) + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path,svd_truncation_tolerance) + + + ROM(hard_impose_currect_cluster = True, Number_Of_Clusters=Number_Of_Clusters, svd_truncation_tolerance=svd_truncation_tolerance) + + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/TrainHROM_Step1.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/TrainHROM_Step1.py new file mode 100644 index 00000000..5c1e8f3e --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/TrainHROM_Step1.py @@ -0,0 +1,90 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + + +import KratosMultiphysics.RomApplication as romapp +import json +import numpy as np + + + + +import os.path + + +class TrainHROMClass(ROM_Class): + + def __init__(self, model, project_parameters,svd_truncation_tolerance): + super().__init__(model, project_parameters, hrom="EmpiricalCubature") + self.svd_truncation_tolerance = svd_truncation_tolerance + + + + + + + +def Train_HROM(svd_truncation_tolerance): + + projected_residuals = f'HROM/Sr_{svd_truncation_tolerance}.npy' + + + if not os.path.exists(projected_residuals): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + #loading the bases + bases = [] + bases = None + simulation = TrainHROMClass(global_model, parameters, svd_truncation_tolerance) + simulation.Run() + + + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"] = [] + updated_project_parameters["output_processes"]["vtk_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path) + + Train_HROM(svd_truncation_tolerance) + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/TrainHROM_Step2.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/TrainHROM_Step2.py new file mode 100644 index 00000000..ac50c49c --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/TrainHROM_Step2.py @@ -0,0 +1,155 @@ +import numpy as np +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition +from matplotlib import pyplot as plt + +import os.path +import os + + + + +def select_elements(svd_truncation_tolerance, residuals_svd_truncation_tolerance): + + weights = f'HROM/WeightsMatrix_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + elements = f'HROM/Elementsvector_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + + if not os.path.exists(weights) and not os.path.exists(elements): + #u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr.npy'), tol) # HEAVY!!! + u = np.load(f'HROM/basis_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy') + + hyper_reduction_element_selector = EmpiricalCubatureMethod() + hyper_reduction_element_selector.SetUp(u) #add again z + hyper_reduction_element_selector.Initialize() + hyper_reduction_element_selector.Calculate() + + + w = np.squeeze(hyper_reduction_element_selector.w) + z = np.squeeze(hyper_reduction_element_selector.z) + + WeightsMatrix = w.reshape(np.size(z),1) + + np.save(weights, WeightsMatrix ) + np.save(elements, z) + + + +def split_matrix_in_columns(svd_truncation_tolerance): + + array_name = f'HROM/Sr_{svd_truncation_tolerance}' + + if not os.path.exists(array_name + '/column_block1.npy'): + + #load array + array = np.load(array_name+'.npy') + + + # Create a folder with the given name + if not os.path.exists(array_name): + os.makedirs(array_name) + + # Create the spliting of the matrix inside the folder + if not os.path.exists(array_name + '/column_block1.npy'): + n_rows, n_cols = array.shape + block_size = n_rows + + start_col = 0 + block_number = 1 + + while start_col < n_cols: + end_col = min(start_col + block_size, n_cols) + + # Check if the remaining columns are too few; if so, merge with the previous block + if n_cols - end_col < block_size / 2 and start_col != 0: + end_col = n_cols + + # Slice the array and save + block = array[:, start_col:end_col] + np.save(os.path.join(array_name, f'column_block{block_number}.npy'), block) + + start_col = end_col + block_number += 1 + + os.remove(array_name+'.npy') + + +def get_global_basis(svd_truncation_tolerance): + + if not os.path.exists(f'HROM/global_basis_{svd_truncation_tolerance}.npy'): + + array_name = f'HROM/Sr_{svd_truncation_tolerance}' + + # List all .npy files in the folder + files = [f for f in os.listdir(array_name) if f.endswith('.npy')] + + u = None + + for file in files: + file_path = os.path.join(array_name, file) + + # Load the file + data = np.load(file_path) + + if u is None: + u, s ,_ = np.linalg.svd(data, full_matrices=False) + else: + print('updating basis') + u2, s2, _ = np.linalg.svd(data, full_matrices=False) + u, s, _ = np.linalg.svd(np.c_[u*s, u2*s2], full_matrices=False) + + #store global basis and global singular values + np.save(f'HROM/global_basis_{svd_truncation_tolerance}.npy',u) + np.save(f'HROM/global_singular_values_{svd_truncation_tolerance}.npy',s) + + + +def truncated_svd(u,s,epsilon=0): + tol = np.finfo(float).eps*max(s)/2 + R = np.sum(s > tol) # Definition of numerical rank + if epsilon == 0: + K = R + else: + SingVsq = np.multiply(s,s) + SingVsq.sort() + normEf2 = np.sqrt(np.cumsum(SingVsq)) + epsilon = epsilon*normEf2[-1] #relative tolerance + T = (sum(normEf2 total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #get list containing snapshots to add to each overlapped cluster + if overlaping_snapshots is not 0: + snapshots_to_add = {} + for i in range(time_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == time_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(time_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + + +def ismember(A, B): + if isinstance(A, np.int_): + return [ np.sum(A == B) ] + else: + return [ np.sum(a == B) for a in A ] + +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + kmeans = KMeans(n_clusters=narrowing_clusters, random_state=0).fit(narrowing.reshape(-1,1)) + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(narrowing_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + correct_cluster = kmeans.labels_ + centroids = kmeans.cluster_centers_ + + if narrowing_clusters>1: + #try and use as is solution manifold neighbor identification + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + narrowing = narrowing.reshape(1,-1) + for i in range(np.shape(narrowing)[1]): + this_matrix = (kmeans.cluster_centers_).T - narrowing[:,i].reshape(np.shape(narrowing)[0], 1) + distance = np.zeros((narrowing_clusters)) + for j in range(narrowing_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + #get list containing snapshots to add to each overlapped cluster + if True: + #if overlaping_snapshots is not 0: + + snapshots_to_add = [] + for j in range(narrowing_clusters): + N_neighbors = len(neighbors[j]) + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + ith_narrowing_cluster = narrowing[:,kmeans.labels_==neighbors[j][i]] + this_matrix = ith_narrowing_cluster - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(narrowing)[0], 1) + distance = np.linalg.norm(this_matrix, axis = 0) + #distance = np.zeros(np.shape(ith_narrowing_cluster[1])) + #for k in range(len(distance)): + # distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + + return sub_snapshots, correct_cluster + + +def solution_manifold_clustering(): + pass + + + +if __name__=='__main__': + #S = np.load('SnapshotMatrix.npy') + #narrowing = np.load('narrowing.npy') + narrowing = np.linspace(0,1,12) + S = np.array([[1,2,3,4,5,6,7,8,9,10,11,12],[1,2,3,4,5,6,7,8,9,10,11,12]]) + #a = narrowing.reshape(1,-1) + #S = np.r_[a, a , a, a] + sub_snapshots, correct_cluster = time_clustering(S, 3,0) + #sub_snapshots, correct_cluster = narrowing_clustering(S, narrowing, 3, 2) + #sub_snapshots, correct_cluster = solution_manifold_clustering(S) + #sub_snapshots, correct_cluster = time_clustering(S) + kkk = 5 + + # + + +""" + +def solution_manifold_clustering(S, solution_manifold_clusters = 3, overlaping_snapshots = 1 ): + #S = np.load('SnapshotMatrix.npy') + kmeans = KMeans(n_clusters = solution_manifold_clusters, random_state=0).fit(S.T) + correct_cluster = kmeans.labels_ + + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(solution_manifold_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + for i in range(np.shape(S)[1]): + this_matrix = (kmeans.cluster_centers_).T - S[:,i].reshape(np.shape(S)[0], 1) + distance = np.zeros((solution_manifold_clusters)) + for j in range(solution_manifold_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + snapshots_to_add = [] + + for j in range(solution_manifold_clusters): + N_snaps = np.shape(sub_snapshots[j])[1] + N_neighbors = len(neighbors[j]) + + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + this_matrix = sub_snapshots[neighbors[j][i]] - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(S)[0], 1) + distance = np.zeros(np.shape(sub_snapshots[neighbors[j][i]][1])) + for k in range(len(distance)): + distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(solution_manifold_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + + +""" +This is wrong, but save for now as reference +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + # wrong implementation :( + # MINE (no k-means) + #S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + #narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + correct_cluster = np.empty(narrowing.shape) + for i in range(narrowing_clusters): + # In this implementation, I just shuffle (order) the snapshots to match the narrowing width. No time-relation whatsoever + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + correct_cluster[intersection] = i + ith_narrowing = narrowing[intersection] + ith_indexes_ordered = np.argsort(ith_narrowing) + sub_snapshots[i] = S[:,ith_indexes_ordered] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + # storing centroids + if i==0: + centroids = np.sum(ith_narrowing)/(ith_narrowing.shape[0]) + else: + centroids = np.c_[centroids, np.sum(ith_narrowing)/(ith_narrowing.shape[0])] + np.save('cluster_centroid.npy', centroids) + #overlapping after correct cluster definition + + #get list containing snapshots to add to each overlapped cluster + snapshots_to_add = {} + for i in range(narrowing_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == narrowing_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + +""" +def time_clustering(time_clusters = 5, overlaping_snapshots = 1 ): + #it works, but no overlapping + S = np.load('SnapshotMatrix.npy') + total_time_steps = S.shape[1] + if time_clusters > total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + + return sub_snapshots, correct_cluster +""" + + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + #no overlapping. MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + return sub_snapshots, correct_cluster +""" + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + # MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + #overlapping after correct cluster definition + # In this implementation, I just shuffle the snapshots to match the narrowing width. No time relation whatsoever + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + if i == 0: + ith_narrowing = narrowing[intersection] + + ith_indexes = np.argsort(ith_narrowing) + ith_narrowing_ordered = ith_narrowing[ith_indexes] + plt.plot(ith_narrowing, 'b') + plt.plot(ith_narrowing_ordered, 'r') + plt.show() + + elif i == narrowing_clusters-1: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + else: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + sub_snapshots[i] = np.c_[sub_snapshots[i] , sub_snapshots[i+1][:, :overlaping_snapshots] ] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster +""" + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/plot_bifurcation.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/plot_bifurcation.py new file mode 100644 index 00000000..5a0e5ce2 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/plot_bifurcation.py @@ -0,0 +1,84 @@ +import numpy as np +from matplotlib import pyplot as plt + + + +if __name__=='__main__': + #library for passing arguments to the script from bash + from sys import argv + + + tol_svd= argv[1] + to_svd_res= argv[2] + + print(tol_svd) + print(to_svd_res) + + + tol_svd = [1e-3] + to_svd_res = [1e-4,1e-5,1e-6]#1e-3, + + + + + + #plt.title(r'Singular Values for matrix $ S^{(2)} $', fontsize=15, fontweight='bold') + #plt.title(r'$\alpha $ \textbf{AA}!', fontsize=16, color='r') + #plt.title(f'ROM VS FOM') + + + plt.rc('text', usetex=True) + plt.rc('font', family='serif') + + + vy = np.load('Results/Velocity_y.npy') + w = np.load('Results/narrowing.npy') + plt.plot(vy, w, 'b', label = 'FOM', linewidth = 1.5 ) #linewidth = 3, alpha=0.5 + markers=['s','^','+','H','*'] + counter = 0 + for svd in tol_svd: + vy_rom = np.load(f'Results/y_velocity_ROM_{svd}.npy') + w_rom = np.load(f'Results/narrowing_ROM_{svd}.npy') + plt.plot(vy_rom, w_rom, label = f"ROM\_{svd}", linewidth = 1.5) #alpha=0.5 + for res in to_svd_res: + vy_rom = np.load(f'Results/y_velocity_HROM_{svd}_{res}.npy') + w_rom = np.load(f'Results/narrowing_HROM_{svd}_{res}.npy') + plt.plot(vy_rom, w_rom, marker=markers[counter],markevery=50,label = f"HROM\_{svd}\_{res}", linewidth = 1.5) #alpha=0.5 + counter+=1 + + #plt.title(r'FOM vs ROM', fontsize=20, fontweight='bold') + plt.legend() + plt.grid() + # plt.xticks(np.arange(-3.5,0.25,0.25)) #TODO the ticks are not easily beautyfied, do it later :) + # plt.yticks(np.arange(0,3.1,0.25)) + plt.xlabel(r'$v_y^*$', size=15, fontweight='bold') + plt.ylabel(r'$w_c$',size=15,fontweight='bold') + + plt.savefig('Results/fom_vs_rom') + plt.show() + + + + + # import numpy as np + # import matplotlib.pyplot as plt + + + # # Example data + # t = np.arange(0.0, 1.0 + 0.01, 0.01) + # s = np.cos(4 * np.pi * t) + 2 + + # plt.rc('text', usetex=True) + # plt.rc('font', family='serif') + # plt.plot(t, s) + + # plt.xlabel(r'\textbf{time} (s)') + # plt.ylabel(r'\textit{voltage} (mV)',fontsize=16) + # plt.title(r"\TeX\ is Number " + # r"$\displaystyle\sum_{n=1}^\infty\frac{-e^{i\pi}}{2^n}$!", + # fontsize=16, color='gray') + # # Make room for the ridiculously large title. + # plt.subplots_adjust(top=0.8) + + # plt.savefig('tex_demo') + # plt.show() \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/plot_full_bifurcation.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/plot_full_bifurcation.py new file mode 100644 index 00000000..6e89133c --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/plot_full_bifurcation.py @@ -0,0 +1,24 @@ +import numpy as np +from matplotlib import pyplot as plt + + + +if __name__=='__main__': + + + vy = np.load('Results/Velocity_y.npy') + w = np.load('Results/narrowing.npy') + vy_rom = np.load(f'Results/y_velocity_ROM.npy') + w_rom = np.load(f'Results/narrowing_ROM.npy') + vy_hrom = np.load(f'Results/y_velocity_HROM.npy') + w_hrom = np.load(f'Results/narrowing_HROM.npy') + + + plt.plot(vy, w, 'k*-', label = 'FOM', linewidth = 3) + plt.plot(vy_rom, w_rom, 'b*-', label = 'ROM') + plt.plot(vy_hrom, w_hrom, 'r*-', label = 'HROM') + plt.title(f'ROMs VS FOM') + plt.legend() + plt.xlabel('velocity y', size=20) + plt.ylabel('narrowing w',size=20) + plt.show() diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/simulation_trajectories.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/simulation_trajectories.py new file mode 100644 index 00000000..23d7a09f --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/ProblemFiles/simulation_trajectories.py @@ -0,0 +1,71 @@ +import numpy as np +from matplotlib import pyplot as plt + +class TrainingTrajectory(): + + def __init__(self, time_step_size): + self.min_or_max_reached_flag = False + self.maximum = 2.9 + self.minimum = 0.1 + self.delta_w = 0.025 * time_step_size # this ensures to obtain a maximum narrowing size of 2.9 and a minimum of 0.1 for a total time T=244 + + def SetUpInitialNarrowing(self): + return self.maximum # starting with a wide narrowing + + def UpdateW(self, w): + ####Train trajectory#### + if not self.min_or_max_reached_flag: #contraction + w -= self.delta_w + if w < self.minimum: + w =self.minimum + self.min_or_max_reached_flag = True + else: #expansion + w += self.delta_w + if w > self.maximum: + w = self.maximum + return w + + + +class TestingTrajectory(): + + def __init__(self, time_step_size): + self.min_or_max_reached_flag = False + self.maximum = 2.9 + self.minimum = 0.1 + self.delta_w = 0.025 * time_step_size # this ensures to obtain a maximum narrowing size of 2.9 and a minimum of 0.1 for a total time T=244 + + def SetUpInitialNarrowing(self): + return self.minimum # starting with a narrow narrowing + + def UpdateW(self, w): + ####Test trajectory#### + if not self.min_or_max_reached_flag:#expansion + w += self.delta_w + if w > self.maximum: + w = self.maximum + self.min_or_max_reached_flag = True + else: #contraction + w -= self.delta_w + if w < self.minimum: + w =self.minimum + return w + + + + +class TestingTrajectory2(): + + + def SetUpInitialNarrowing(self): + return self.UpdateW(0) + + + def UpdateW(self, time, T=100): + # Normalizing time t to the range [0, 2*pi] + fixed_deformation_factor = 2.8 + normalized_t = (2 * np.pi * time) / T + + # Defining the function using a combination of sine and cosine functions + # with a phase shift and frequency adjustments for more variations + return 0.1 + (0.5 * (1 + np.sin(normalized_t - np.pi/2) * np.cos(3 * normalized_t)) * fixed_deformation_factor) diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/launch_ale_rom_nord3.sh b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/launch_ale_rom_nord3.sh new file mode 100755 index 00000000..8fa73bf3 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Affine/launch_ale_rom_nord3.sh @@ -0,0 +1,102 @@ +#!/bin/sh +#SBATCH -N 1 # nodes requested +#SBATCH -n 1 # tasks requested +#SBATCH -c 16 # cores requested +#SBATCH -t 20:00:00 # time requested in hour:minute:second +####3#SBATCH --constraint='highmem' + + +export OMP_NUM_THREADS=16 +export PROBLEMS_PATH=$PWD/ProblemFiles +export LANGUAGE=en_GB.utf8 +export LC_ALL=en_GB.utf8 + + +FOM=False #(storing results) +FOM_test=True #(storing results) +Run_ROM=False #3 (storing results) +ROM_test=True #4 = (storing results) +Train_HROM_Step1=False #5 = (creating projected residuals matrices {Sr_i}_i=1^k (one per basis)) +Train_HROM_Step2=False #6 = ontain a reduced set of elements and weights starting from the projected residuals matrices Sr_i +Run_HROM=False #7 = RunHROM Train Trajectory +HROM_test=True #8 = RunHROM Test Trajectory + +plot_partial_hysteresis=False + +#parameters used in Local POD: + +# parameters for the simulations +Launch_Simulation=1 +Number_Of_Clusters=1 #not used in global POD +svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +clustering="narrowing" #time # +overlapping=30 +residuals_svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +residuals_svd_relative_to_global_residuals_snapshots=1 + + +if [ $FOM = True ] + then + #### LAUNCH FOM TRAIN TRAJECTORY #### + # MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLauching FOM \n\n\n\n\n\n" + python3 ProblemFiles/FOM.py $PWD +fi +if [ $FOM_test = True ] + then + # NEW MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching FOM test trajectory \n\n\n\n\n\n" + python3 ProblemFiles/FOM_TestTrajectory.py $PWD +fi +for j in ${svd_truncation_tolerance_list[@]} +do + svd_truncation_tolerance=$j + if [ $Run_ROM = True ] + then + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching ROM \n\n\n\n\n\n" + python3 ProblemFiles/Run_ROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $ROM_test = True ] + then + #### LAUNCH ROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\nlaunching ROM test\n\n\n\n' + python3 ProblemFiles/ROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $Train_HROM_Step1 = True ] + then + #### TrainHROM (Creating Matrix of projected resduals Sr) #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\nlaunching TrainHROM train\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step1.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + for k in ${residuals_svd_truncation_tolerance_list[@]} + do + residuals_svd_truncation_tolerance=$k + if [ $Train_HROM_Step2 = True ] + then + ### Obtain Reduced Elements and Weights #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nlaunching HROM elements and Weights\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step2.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $Run_HROM = True ] + then + #### LAUNCH HROM TRAIN TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nLaunching HROM train\n\n\n\n\n\n\n' + python3 ProblemFiles/Run_HROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $HROM_test = True ] + then + #### LAUNCH HROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo 'Launching HROM test' + python3 ProblemFiles/HROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + done +done + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FOM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FOM.py new file mode 100644 index 00000000..682122e2 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FOM.py @@ -0,0 +1,365 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis + + +import json + +import numpy as np + + +#for checking if paths exits +import os + +#importing PyGeM tools +from pygem import FFD, RBF + + +#importing training trajectory +from simulation_trajectories import training_trajectory + +#importing the nonlinear mapping +from nonlinear_mapping import set_up_phi, phi + + + + +class FOM_Class(FluidDynamicsAnalysis): + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.deformation_multiplier = 1 # original narrowing size + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.delta_deformation = time_step_size # this ensures to obtain the same deformation independently of the time step used + self.control_point = 854 #a node around the middle of the geometry to capture the bufurcation + self.maximum = 11 + self.minimum = 0 + ### ### ### + self.node_up = 412 #nodes to obtain the narrowing width + self.node_down = 673 + ### ### ### + self.time_step_solution_container = [] + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.deformation_multiplier_list = [] + self.matrix_of_free_coordinates = None + self.deformation_multiplier = 11 + + + def MoveInnerNodesWithRBF(self): + # first loop, ONLY ENTERED ONCE + if self.matrix_of_free_coordinates is None: + x_original = [] + y_original = [] + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(-1,1) + y_original = np.array(y_original).reshape(-1,1) + self.matrix_of_free_coordinates = np.c_[x_original, y_original, np.ones((y_original.shape[0],1))] + self.matrix_of_modified_coordinates = self.rbf(self.matrix_of_free_coordinates) + + # second loop + i = 0 + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = self.matrix_of_modified_coordinates[i,0] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = self.matrix_of_modified_coordinates[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + node = self.model.GetModelPart("FluidModelPart").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.deformation_multiplier_list.append(self.deformation_multiplier) + node_up = self.model.GetModelPart("FluidModelPart").GetNode(self.node_up) + node_down = self.model.GetModelPart("FluidModelPart").GetNode(self.node_down) + self.narrowing_width.append(node_up.Y - node_down.Y) + + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.IdentifyNodes() + self.SetUpFreeFormDeformation() + + + + def IdentifyNodes(self): + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + fixed_walls= self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls") + + number_of_nodes_walls = fixed_walls.NumberOfNodes() + number_of_nodes_down = control_down.NumberOfNodes() + number_of_nodes_up = control_down.NumberOfNodes() + + #get matrix of original coordinates + walls_coordinates = np.ones((int(number_of_nodes_walls),3)) + up_coordinates = np.ones((int(number_of_nodes_up),3)) + down_coordinates = np.ones((int(number_of_nodes_down),3)) + + counter = 0 + for node in control_down.Nodes: + down_coordinates[counter, 0] = node.X0 + down_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in control_up.Nodes: + up_coordinates[counter, 0] = node.X0 + up_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in fixed_walls.Nodes: + walls_coordinates[counter, 0] = node.X0 + walls_coordinates[counter, 1] = node.Y0 + counter+=1 + + self.walls = walls_coordinates + + self.up = up_coordinates + at_3_y = np.where(self.up[:,1] == 3) + self.up = np.delete(self.up,at_3_y, 0) + + self.down = down_coordinates + at_0_y = np.where(self.down[:,1] == 0) + self.down = np.delete(self.down,at_0_y, 0) + + self.fixed_coordinates = np.r_[walls_coordinates, self.down, self.up] + + + def SetUpFreeFormDeformation(self): + # #creating a free form deformation object for each control domain + self.ffd_up, self.ffd_down = set_up_phi() + + + def MoveControlPoints(self, scale_of_deformation=1): + + moved_up, moved_down, _, _ = phi(self.up,self.down,self.ffd_down,self.ffd_up, + self.deformation_multiplier,scale_of_deformation) + + + #Moving lower part + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + i=0 + for node in control_down.Nodes: + if node.Y0 != 0: + x_disp = moved_down[i,0] - node.X0 + y_disp = moved_down[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + node.X = node.X0 + x_disp + node.Y = node.Y0 + y_disp + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + #moving upper part + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + i=0 + for node in control_up.Nodes: + if node.Y0 != 3: + x_disp = moved_up[i,0] - node.X0 + y_disp = moved_up[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + node.X = node.X0 + x_disp + node.Y = node.Y0 + y_disp + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.moved_coordinates = np.r_[self.walls, moved_down, moved_up] + + + + def UpdateRBF(self): + self.rbf = RBF(original_control_points = self.fixed_coordinates, deformed_control_points = + self.moved_coordinates, radius=0.75) + + + def LockOuterWalls(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0 ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + def UpdateDeformationMultiplier(self): + self.deformation_multiplier = training_trajectory( self.time, self.deformation_multiplier, self.delta_deformation, self.maximum, self.minimum) + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width, self.deformation_multiplier_list + + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + + + + + + + + + + + + +def Train_ROM(): + + if not os.path.exists(f'./Results/FOM.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing, deformation_multiplier = simulation.GetBifuracationData() + #reynolds = simulation.GetReynoldsData() + #np.save('Results/reynolds.npy', reynolds) + np.save('Results/deformation_multiplier.npy', deformation_multiplier) + np.save('Results/narrowing.npy', narrowing) + np.save('Results/Velocity_y.npy', velocity_y) + np.save('Results/SnapshotMatrix.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + + Train_ROM() + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FOM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FOM_TestTrajectory.py new file mode 100644 index 00000000..813d6ace --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FOM_TestTrajectory.py @@ -0,0 +1,159 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis + +from FOM import FOM_Class + +import json + +import numpy as np + + +#for checking if paths exits +import os + + +#importing testing trajectory +from simulation_trajectories import second_testing_trajectory + + +class FOM_Class_test(FOM_Class): + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.deformation_multiplier = 11 + + + def UpdateDeformationMultiplier(self): + self.deformation_multiplier = second_testing_trajectory( self.time ) + + + + def InitializeSolutionStep(self): + super(FluidDynamicsAnalysis, self).InitializeSolutionStep() + + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +'/Results/FOM_test' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + +def convert_to_nd(SnapshotsMatrix, number_of_dimensions=2): + for i in range(np.shape(SnapshotsMatrix)[1]): + column_mean = np.mean( SnapshotsMatrix[:,i].reshape(-1,number_of_dimensions).reshape(-1,number_of_dimensions),0).reshape(-1,1) + if i ==0: + columns_means = column_mean + else: + columns_means = np.c_[columns_means,column_mean] + + return columns_means + + + + + + + + + + + + + + + + + + + + + + + + + + + + +def Train_ROM(): + + if not os.path.exists(f'./Results/FOM_test.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + simulation = FOM_Class_test(global_model, parameters) + simulation.Run() + SnapshotsMatrix = simulation.GetSnapshotsMatrix() + velocity_y, narrowing, deformation_multiplier = simulation.GetBifuracationData() + #reynolds = simulation.GetReynoldsData() + #np.save('Results/reynolds.npy', reynolds) + np.save('Results/deformation_multiplier_test.npy', deformation_multiplier) + np.save('Results/narrowing_test.npy', narrowing) + np.save('Results/Velocity_y_test.npy', velocity_y) + np.save('Results/SnapshotMatrix_test.npy', SnapshotsMatrix ) + + + + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + #library for passing arguments to the script from bash + from sys import argv + + working_path = argv[1] + + prepare_files(working_path) + + + Train_ROM() + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FluidMaterials.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FluidMaterials.json new file mode 100644 index 00000000..24e1bedf --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/FluidMaterials.json @@ -0,0 +1,16 @@ +{ + "properties" : [{ + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "properties_id" : 1, + "Material" : { + "constitutive_law" : { + "name" : "Newtonian2DLaw" + }, + "Variables" : { + "DENSITY" : 1.0, + "DYNAMIC_VISCOSITY" : 0.1 + }, + "Tables" : {} + } + }] +} diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/HROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/HROM_TestTrajectory.py new file mode 100644 index 00000000..92fc4938 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/HROM_TestTrajectory.py @@ -0,0 +1,133 @@ +import KratosMultiphysics +from ROM_TestTrajectory import ROM_Class_test + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt + +import os + + + + + +class HROMClass_test(ROM_Class_test): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 5152 #TODO, get rid of this, load both elements and condition sets + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + + + + + + + + + + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + if not os.path.exists(f'./Results/HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass_test(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom, deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_ROM_test_{svd_truncation_tolerance}.npy', deformation_multiplier) + + + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_test_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/MainKratos.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/MainKratos.py new file mode 100644 index 00000000..7922e43b --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/MainKratos.py @@ -0,0 +1,383 @@ +import KratosMultiphysics +from KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis import FluidDynamicsAnalysis +from KratosMultiphysics.RomApplication.fluid_dynamics_analysis_rom import FluidDynamicsAnalysisROM + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np +from matplotlib import pyplot as plt + + +#importing PyGeM tools +from pygem import FFD, RBF + +#Function from PyGeM tutorial +def scatter3d(arr, figsize=(8,8), s=10, draw=True, ax=None, alpha=1, labels=None, title=None): + if ax is None: + fig = plt.figure(figsize=figsize) + ax = fig.add_subplot(projection='3d') + + for idx,a in enumerate(arr): + if labels is not None: + ax.scatter(*a.T, s=s, alpha=alpha, label=labels[idx]) + else: + ax.scatter(*a.T, s=s, alpha=alpha) + + if draw: + if labels is not None: + plt.legend() + if title is not None: + plt.title(title) + plt.show() + else: + return ax + + +class FOM_Class(FluidDynamicsAnalysis): + + + def __init__(self, model, project_parameters): + super().__init__(model, project_parameters) + self.w = 1 # original narrowing size + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.control_point = 363 #a node around the middle of the geometry to capture the bufurcation + self.time_step_solution_container = [] + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.matrix_of_free_coordinates = None + self.deformation_multiplier = 0 + + + def MoveInnerNodesWithRBF(self): + # first loop, ONLY ENTERED ONCE + if self.matrix_of_free_coordinates is None: + x_original = [] + y_original = [] + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(-1,1) + y_original = np.array(y_original).reshape(-1,1) + self.matrix_of_free_coordinates = np.c_[x_original, y_original, np.ones((y_original.shape[0],1))] + self.matrix_of_modified_coordinates = self.rbf(self.matrix_of_free_coordinates) + + # second loop + i = 0 + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = self.matrix_of_modified_coordinates[i,0] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = self.matrix_of_modified_coordinates[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + node = self.model.GetModelPart("FluidModelPart").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.narrowing_width.append(self.deformation_multiplier) + + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.IdentifyNodes() + self.SetUpFreeFormDeformation() + + + + def IdentifyNodes(self): + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + fixed_walls= self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls") + + number_of_nodes_walls = fixed_walls.NumberOfNodes() + number_of_nodes_down = control_down.NumberOfNodes() + number_of_nodes_up = control_down.NumberOfNodes() + + #get matrix of original coordinates + walls_coordinates = np.ones((int(number_of_nodes_walls),3)) + up_coordinates = np.ones((int(number_of_nodes_up),3)) + down_coordinates = np.ones((int(number_of_nodes_down),3)) + + counter = 0 + for node in control_down.Nodes: + down_coordinates[counter, 0] = node.X0 + down_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in control_up.Nodes: + up_coordinates[counter, 0] = node.X0 + up_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in fixed_walls.Nodes: + walls_coordinates[counter, 0] = node.X0 + walls_coordinates[counter, 1] = node.Y0 + counter+=1 + + self.walls = walls_coordinates + + self.up = up_coordinates + at_3_y = np.where(self.up[:,1] == 3) + self.up = np.delete(self.up,at_3_y, 0) + + self.down = down_coordinates + at_0_y = np.where(self.down[:,1] == 0) + self.down = np.delete(self.down,at_0_y, 0) + + self.fixed_coordinates = np.r_[walls_coordinates, self.down, self.up] + + + + + def SetUpFreeFormDeformation(self): + #creating a free form deformation object for each control domain + self.ffd_up = FFD([2,5,2]) #3D box of control points + self.ffd_down = FFD([2,5,2]) #3D box of control points + + #setting the centre and size of the upper box of control points + self.ffd_down.box_origin = np.array([1.25, 0, 0.5]) + self.ffd_down.box_length = np.array([1, 1.25, 1]) + + #setting the centre and size of the lower box of control points + self.ffd_up.box_origin = np.array([1.25, 1.75, 0.5]) + self.ffd_up.box_length = np.array([1, 1.25, 1]) + + self.list_of_ffds = [self.ffd_up, self.ffd_down] + + + + + def MoveControlPoints(self, scale_of_deformation=1): + + self.ffd_down.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + + self.ffd_down.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_down.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_down.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_down.array_mu_y[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_down.array_mu_y[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_down.array_mu_y[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_down.array_mu_y[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_down.array_mu_y[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_down.array_mu_y[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.02 + self.ffd_down.array_mu_y[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.025 + + self.ffd_up.array_mu_x[0, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[0, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[0, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[0, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[0, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[0, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[0, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[0, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[0, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[0, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + + self.ffd_up.array_mu_x[1, 0, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 0] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 0] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 0] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 0, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + self.ffd_up.array_mu_x[1, 1, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 2, 1] = self.deformation_multiplier*scale_of_deformation * 0.06 + self.ffd_up.array_mu_x[1, 3, 1] = self.deformation_multiplier*scale_of_deformation * 0.04 + self.ffd_up.array_mu_x[1, 4, 1] = self.deformation_multiplier*scale_of_deformation * 0.0 + + self.ffd_up.array_mu_y[1, 0, 0] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 0] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 0] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 0] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 0] = -self.deformation_multiplier*scale_of_deformation * 0.00 + self.ffd_up.array_mu_y[1, 0, 1] = -self.deformation_multiplier*scale_of_deformation * 0.025 + self.ffd_up.array_mu_y[1, 1, 1] = -self.deformation_multiplier*scale_of_deformation * 0.020 + self.ffd_up.array_mu_y[1, 2, 1] = -self.deformation_multiplier*scale_of_deformation * 0.015 + self.ffd_up.array_mu_y[1, 3, 1] = -self.deformation_multiplier*scale_of_deformation * 0.01 + self.ffd_up.array_mu_y[1, 4, 1] = -self.deformation_multiplier*scale_of_deformation * 0.00 + + moved_up = self.ffd_up(self.up) + moved_down = self.ffd_down(self.down) + + + #Moving lower part + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + i=0 + for node in control_down.Nodes: + if node.Y0 != 0: + print(node.Y0) + x_disp = moved_down[i,0] - node.X0 + y_disp = moved_down[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + #moving upper part + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + i=0 + for node in control_up.Nodes: + if node.Y0 != 3: + print(node.Y0) + x_disp = moved_up[i,0] - node.X0 + y_disp = moved_up[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.moved_coordinates = np.r_[self.walls, moved_down, moved_up] + + + + def UpdateRBF(self): + self.rbf = RBF(original_control_points = self.fixed_coordinates, deformed_control_points = + self.moved_coordinates, radius=0.75) + + + def LockOuterWalls(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0 ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + if self.time>1.0 and self.time<16.0: # start modifying narrowing from 1 second onwards + self.deformation_multiplier+=.1 + elif self.time>21.0 and self.time<36: + self.deformation_multiplier-=.1 + + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width + + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + +def Train_ROM(): + with open("ProjectParameters.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + + global_model = KratosMultiphysics.Model() + simulation = FOM_Class(global_model, parameters) + simulation.Run() + return simulation.GetBifuracationData() + + + + + + + +if __name__ == "__main__": + #Train_ROM() + vy, w = Train_ROM() + + plt.plot(vy, w, 'k-', label = 'FOM', linewidth = 3) + plt.legend() + plt.xlabel('velocity y', size=20) + plt.ylabel('narrowing w',size=20) + plt.show() diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/NonlinearInGiD.mdpa b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/NonlinearInGiD.mdpa new file mode 100644 index 00000000..ec99bbdb --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/NonlinearInGiD.mdpa @@ -0,0 +1,17117 @@ +Begin ModelPartData +// VARIABLE_NAME value +End ModelPartData + +Begin Properties 0 +End Properties + +Begin Nodes + 1 0.0000000000 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// Group Inlet//Custom2 // Subtree VelocityConstraints2D + Begin SubModelPartNodes + 1 + 2 + 5 + 11 + 18 + 26 + 35 + 48 + 62 + 79 + 95 + 115 + 135 + 160 + 185 + 209 + 237 + 261 + 281 + 305 + 330 + 361 + 399 + 439 + 482 + 528 + 572 + 615 + 661 + 708 + 750 + End SubModelPartNodes + Begin SubModelPartElements + End SubModelPartElements + Begin SubModelPartConditions + End SubModelPartConditions +End SubModelPart diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ProjectParameters.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ProjectParameters.json new file mode 100644 index 00000000..52628b5b --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ProjectParameters.json @@ -0,0 +1,163 @@ +{ + "analysis_stage": "KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis", + "problem_data" : { + "problem_name" : "NonlinearInGiD", + "parallel_type" : "OpenMP", + "echo_level" : 0, + "start_time" : 0.0, + "end_time" : 52 + }, + "output_processes" : { + "gid_output" : [{ + "python_module" : "gid_output_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "GiDOutputProcess", + "help" : "This process writes postprocessing files for GiD", + "Parameters" : { + "model_part_name" : "FluidModelPart.fluid_computational_model_part", + "output_name" : "NonlinearInGiD", + "postprocess_parameters" : { + "result_file_configuration" : { + "gidpost_flags" : { + "GiDPostMode" : "GiD_PostBinary", + "WriteDeformedMeshFlag" : "WriteDeformed", + "WriteConditionsFlag" : "WriteConditions", + "MultiFileFlag" : "SingleFile" + }, + "file_label" : "time", + "output_control_type" : "time", + "output_interval" : 0.1, + "body_output" : true, + "node_output" : false, + "skin_output" : false, + "plane_output" : [], + "nodal_results" : ["VELOCITY","PRESSURE","MESH_DISPLACEMENT"], + "gauss_point_results" : [], + "nodal_nonhistorical_results" : [] + }, + "point_data_configuration" : [] + } + } + }], + "vtk_output" : [{ + "python_module" : "vtk_output_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "VtkOutputProcess", + "help" : "This process writes postprocessing files for Paraview", + "Parameters" : { + "model_part_name" : "FluidModelPart.fluid_computational_model_part", + "output_control_type" : "step", + "output_interval" : 50, + "file_format" : "binary", + "output_precision" : 7, + "output_sub_model_parts" : false, + "output_path" : "vtk_output", + "save_output_files_in_folder" : true, + "nodal_solution_step_data_variables" : ["VELOCITY","PRESSURE"], + "nodal_data_value_variables" : [], + "element_data_value_variables" : ["HROM_WEIGHT"], + "condition_data_value_variables" : [], + "gauss_point_variables_extrapolated_to_nodes" : [] + } + }] + }, + "solver_settings" : { + "solver_type": "ale_fluid", + "ale_boundary_parts": [], + "mesh_motion_solver_settings" : { + "solver_type" : "structural_similarity" + }, + "fluid_solver_settings": { + "model_part_name" : "FluidModelPart", + "domain_size" : 2, + "solver_type" : "Monolithic", + "model_import_settings" : { + "input_type" : "mdpa", + "input_filename" : "NonlinearInGiD" + }, + "material_import_settings" : { + "materials_filename" : "FluidMaterials.json" + }, + "echo_level" : 0, + "compute_reactions" : false, + "maximum_iterations" : 10, + "relative_velocity_tolerance" : 0.001, + "absolute_velocity_tolerance" : 1e-5, + "relative_pressure_tolerance" : 0.001, + "absolute_pressure_tolerance" : 1e-5, + "volume_model_part_name" : "FluidParts_Volume", + "skin_parts" : ["Outlet2D_Outlet","NoSlip2D_No_Slip_Auto1"], + "no_skin_parts" : ["VelocityConstraints2D_Inlet-Total","VelocityConstraints2D_Inlet-Custom2"], + "time_scheme" : "bossak", + "time_stepping" : { + "automatic_time_step" : false, + "time_step" : 0.05 + }, + "formulation" : { + "element_type" : "qsvms", + "use_orthogonal_subscales" : false, + "dynamic_tau" : 1.0 + }, + "reform_dofs_at_each_step" : false + } + + }, + "processes" :{ + "initial_conditions_process_list" : [], + "boundary_conditions_process_list" : [{ + "python_module" : "apply_outlet_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyOutletProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.Outlet2D_Outlet", + "variable_name" : "PRESSURE", + "constrained" : true, + "value" : 0.0, + "hydrostatic_outlet" : false, + "h_top" : 0.0 + } + },{ + "python_module" : "apply_noslip_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyNoSlipProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.NoSlip2D_No_Slip_Auto1" + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name" : "VELOCITY", + "interval" : [0.0,1.0], + "constrained" : [true,true,true], + "value" : ["y*(3-y)*sin(pi*t*0.5)",0.0,0.0] + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Custom2", + "variable_name" : "VELOCITY", + "interval" : [1.0,"End"], + "constrained" : [true,true,true], + "value" : ["y*(3-y)",0.0,0.0] + } + }], + "gravity" : [{ + "python_module" : "assign_vector_by_direction_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorByDirectionProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "variable_name" : "BODY_FORCE", + "modulus" : 0.0, + "constrained" : false, + "direction" : [0.0,-1.0,0.0] + } + }], + "auxiliar_process_list" : [] + } +} diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ProjectParameters_modified.json b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ProjectParameters_modified.json new file mode 100644 index 00000000..dcb01c06 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ProjectParameters_modified.json @@ -0,0 +1,214 @@ +{ + "analysis_stage": "KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis", + "problem_data": { + "problem_name": "NonlinearInGiD", + "parallel_type": "OpenMP", + "echo_level": 0, + "start_time": 0.0, + "end_time": 52 + }, + "output_processes": { + "gid_output": [ + { + "python_module": "gid_output_process", + "kratos_module": "KratosMultiphysics", + "process_name": "GiDOutputProcess", + "help": "This process writes postprocessing files for GiD", + "Parameters": { + "model_part_name": "FluidModelPart.fluid_computational_model_part", + "output_name": "/gpfs/projects/bsc44/bsc44011/KratosSimulations/FinalNarrowing/example_3/FFD_plus_RBF/Results/HROM_test_1e-06_1e-06", + "postprocess_parameters": { + "result_file_configuration": { + "gidpost_flags": { + "GiDPostMode": "GiD_PostBinary", + "WriteDeformedMeshFlag": "WriteDeformed", + "WriteConditionsFlag": "WriteConditions", + "MultiFileFlag": "SingleFile" + }, + "file_label": "time", + "output_control_type": "time", + "output_interval": 0.1, + "body_output": true, + "node_output": false, + "skin_output": false, + "plane_output": [], + "nodal_results": [ + "VELOCITY", + "PRESSURE", + "MESH_DISPLACEMENT" + ], + "gauss_point_results": [], + "nodal_nonhistorical_results": [] + }, + "point_data_configuration": [] + } + } + } + ], + "vtk_output": [ + { + "python_module": "vtk_output_process", + "kratos_module": "KratosMultiphysics", + "process_name": "VtkOutputProcess", + "help": "This process writes postprocessing files for Paraview", + "Parameters": { + "model_part_name": "FluidModelPart.fluid_computational_model_part", + "output_control_type": "step", + "output_interval": 50, + "file_format": "binary", + "output_precision": 7, + "output_sub_model_parts": false, + "output_path": "vtk_output", + "save_output_files_in_folder": true, + "nodal_solution_step_data_variables": [ + "VELOCITY", + "PRESSURE" + ], + "nodal_data_value_variables": [], + "element_data_value_variables": [ + "HROM_WEIGHT" + ], + "condition_data_value_variables": [], + "gauss_point_variables_extrapolated_to_nodes": [] + } + } + ] + }, + "solver_settings": { + "solver_type": "ale_fluid", + "ale_boundary_parts": [], + "mesh_motion_solver_settings": { + "solver_type": "structural_similarity" + }, + "fluid_solver_settings": { + "model_part_name": "FluidModelPart", + "domain_size": 2, + "solver_type": "Monolithic", + "model_import_settings": { + "input_type": "mdpa", + "input_filename": "/gpfs/projects/bsc44/bsc44011/KratosSimulations/FinalNarrowing/example_3/FFD_plus_RBF/ProblemFiles/NonlinearInGiD" + }, + "material_import_settings": { + "materials_filename": "/gpfs/projects/bsc44/bsc44011/KratosSimulations/FinalNarrowing/example_3/FFD_plus_RBF/ProblemFiles/FluidMaterials.json" + }, + "echo_level": 0, + "compute_reactions": false, + "maximum_iterations": 10, + "relative_velocity_tolerance": 0.001, + "absolute_velocity_tolerance": 1e-05, + "relative_pressure_tolerance": 0.001, + "absolute_pressure_tolerance": 1e-05, + "volume_model_part_name": "FluidParts_Volume", + "skin_parts": [ + "Outlet2D_Outlet", + "NoSlip2D_No_Slip_Auto1" + ], + "no_skin_parts": [ + "VelocityConstraints2D_Inlet-Total", + "VelocityConstraints2D_Inlet-Custom2" + ], + "time_scheme": "bossak", + "time_stepping": { + "automatic_time_step": false, + "time_step": 0.05 + }, + "formulation": { + "element_type": "qsvms", + "use_orthogonal_subscales": false, + "dynamic_tau": 1.0 + }, + "reform_dofs_at_each_step": false + } + }, + "processes": { + "initial_conditions_process_list": [], + "boundary_conditions_process_list": [ + { + "python_module": "apply_outlet_process", + "kratos_module": "KratosMultiphysics.FluidDynamicsApplication", + "process_name": "ApplyOutletProcess", + "Parameters": { + "model_part_name": "FluidModelPart.Outlet2D_Outlet", + "variable_name": "PRESSURE", + "constrained": true, + "value": 0.0, + "hydrostatic_outlet": false, + "h_top": 0.0 + } + }, + { + "python_module": "apply_noslip_process", + "kratos_module": "KratosMultiphysics.FluidDynamicsApplication", + "process_name": "ApplyNoSlipProcess", + "Parameters": { + "model_part_name": "FluidModelPart.NoSlip2D_No_Slip_Auto1" + } + }, + { + "python_module": "assign_vector_variable_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorVariableProcess", + "Parameters": { + "model_part_name": "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name": "VELOCITY", + "interval": [ + 0.0, + 1.0 + ], + "constrained": [ + true, + true, + true + ], + "value": [ + "y*(3-y)*sin(pi*t*0.5)", + 0.0, + 0.0 + ] + } + }, + { + "python_module": "assign_vector_variable_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorVariableProcess", + "Parameters": { + "model_part_name": "FluidModelPart.VelocityConstraints2D_Inlet-Custom2", + "variable_name": "VELOCITY", + "interval": [ + 1.0, + "End" + ], + "constrained": [ + true, + true, + true + ], + "value": [ + "y*(3-y)", + 0.0, + 0.0 + ] + } + } + ], + "gravity": [ + { + "python_module": "assign_vector_by_direction_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorByDirectionProcess", + "Parameters": { + "model_part_name": "FluidModelPart.FluidParts_Volume", + "variable_name": "BODY_FORCE", + "modulus": 0.0, + "constrained": false, + "direction": [ + 0.0, + -1.0, + 0.0 + ] + } + } + ], + "auxiliar_process_list": [] + } +} \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ROM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ROM_TestTrajectory.py new file mode 100644 index 00000000..8db31aa8 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/ROM_TestTrajectory.py @@ -0,0 +1,144 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + +import KratosMultiphysics.RomApplication as romapp +import json + +import numpy as np + + +#importing PyGeM tools +from pygem import FFD, RBF + +import os + + + +#importing testing trajectory +from simulation_trajectories import second_testing_trajectory + + + + + + + +class ROM_Class_test(ROM_Class): + + def __init__(self, model, project_parameters, correct_cluster = None, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, hrom) + self.deformation_multiplier = 11 + + + def UpdateDeformationMultiplier(self): + self.deformation_multiplier = second_testing_trajectory( self.time ) + + + def InitializeSolutionStep(self): + super(ROM_Class, self).InitializeSolutionStep() + + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + + + + +def prepare_files(working_path, svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_test_{svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(svd_truncation_tolerance): + + + if not os.path.exists(f'./Results/ROM_test_{svd_truncation_tolerance}.post.bin'): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class_test(global_model, parameters) + simulation.Run() + + + np.save(f'Results/ROM_snapshots_test_{svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom, deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_ROM_test_{svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_ROM_test_{svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_ROM_test_{svd_truncation_tolerance}.npy', deformation_multiplier) + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path, svd_truncation_tolerance) + + + ROM(svd_truncation_tolerance) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/Run_HROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/Run_HROM.py new file mode 100644 index 00000000..28bc60c8 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/Run_HROM.py @@ -0,0 +1,102 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + +import KratosMultiphysics.RomApplication as romapp +import json + + +import os +import numpy as np + + + +class HROMClass(ROM_Class): + + def __init__(self, model, project_parameters, correct_cluster, svd_truncation_tolerance, residuals_svd_truncation_tolerance,hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, correct_cluster, hard_impose_correct_cluster, bases, hrom) + self.svd_truncation_tolerance = svd_truncation_tolerance + self.residuals_svd_truncation_tolerance = residuals_svd_truncation_tolerance + + + def ModifyInitialGeometry(self): + """Here is the place where the HROM_WEIGHTS are assigned to the selected elements and conditions""" + super().ModifyInitialGeometry() + computing_model_part = self._solver.GetComputingModelPart() + OriginalNumberOfElements = 5152 + WeightsMatrix = np.load(f'HROM/WeightsMatrix_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + ElementsVector = np.load(f'HROM/Elementsvector_{self.svd_truncation_tolerance}_{self.residuals_svd_truncation_tolerance}.npy') + + for i in range(WeightsMatrix.shape[0]): + if ElementsVector[i] < OriginalNumberOfElements: + computing_model_part.GetElement(int( ElementsVector[i])+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + else: + computing_model_part.GetCondition(int( ElementsVector[i] - OriginalNumberOfElements)+1).SetValue(romapp.HROM_WEIGHT, WeightsMatrix[i,0] ) + + + +def HROM(residuals_svd_truncation_tolerance=1e-4, svd_truncation_tolerance=1e-4): + + + + if not os.path.exists(f'./Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.post.bin'): + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = HROMClass(global_model, parameters, correct_clusters, svd_truncation_tolerance, residuals_svd_truncation_tolerance, hard_impose_correct_cluster = False, bases=None, hrom=None ) + simulation.Run() + np.save(f'Results/HROM_snapshots_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom, w_rom, deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy', deformation_multiplier) + + + + +def prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/HROM_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + residuals_svd_truncation_tolerance=float(argv[7]) + + prepare_files(working_path,svd_truncation_tolerance,residuals_svd_truncation_tolerance) + + HROM(residuals_svd_truncation_tolerance=residuals_svd_truncation_tolerance, svd_truncation_tolerance=svd_truncation_tolerance) + + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/Run_ROM.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/Run_ROM.py new file mode 100644 index 00000000..15caa56a --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/Run_ROM.py @@ -0,0 +1,355 @@ +import KratosMultiphysics +from KratosMultiphysics.RomApplication.fluid_dynamics_analysis_rom import FluidDynamicsAnalysisROM + +import os.path + + +import KratosMultiphysics.RomApplication as romapp +import json + +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition + +import numpy as np + +#importing training trajectory +from simulation_trajectories import training_trajectory + +#importing the nonlinear mapping +from nonlinear_mapping import set_up_phi, phi + +#importing PyGeM tools +from pygem import FFD, RBF + + +class ROM_Class(FluidDynamicsAnalysisROM): + + def __init__(self, model, project_parameters, correct_cluster = None, hard_impose_correct_cluster = False, bases=None, hrom=None): + super().__init__(model, project_parameters, hrom) + time_step_size = self.project_parameters["solver_settings"]["fluid_solver_settings"]["time_stepping"]["time_step"].GetDouble() + self.delta_deformation = time_step_size # this ensures to obtain the same deformation independently of the time step used + self.control_point = 854 #a node around the middle of the geometry to capture the bufurcation + self.maximum = 11 + self.minimum = 0 + ### ### ### + self.node_up = 412 #nodes to obtain the narrowing width + self.node_down = 673 + ### ### ### + self.deformation_multiplier_list = [] + self.time_step_solution_container = [] + self.velocity_y_at_control_point = [] + self.narrowing_width = [] + self.matrix_of_free_coordinates = None + self.deformation_multiplier = 11 + + + def MoveInnerNodesWithRBF(self): + # first loop, ONLY ENTERED ONCE + if self.matrix_of_free_coordinates is None: + x_original = [] + y_original = [] + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_original.append(node.X0) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_original.append(node.Y0) + x_original = np.array(x_original).reshape(-1,1) + y_original = np.array(y_original).reshape(-1,1) + self.matrix_of_free_coordinates = np.c_[x_original, y_original, np.ones((y_original.shape[0],1))] + self.matrix_of_modified_coordinates = self.rbf(self.matrix_of_free_coordinates) + + # second loop + i = 0 + for node in self.model.GetModelPart("FluidModelPart").Nodes: + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_X): + x_disp = self.matrix_of_modified_coordinates[i,0] - node.X0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + if not node.IsFixed(KratosMultiphysics.MESH_DISPLACEMENT_Y): + y_disp = self.matrix_of_modified_coordinates[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + def StoreBifurcationData(self): + node = self.model.GetModelPart("FluidModelPart").GetNode(self.control_point) + self.velocity_y_at_control_point.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y)) + self.deformation_multiplier_list.append(self.deformation_multiplier) + node_up = self.model.GetModelPart("FluidModelPart").GetNode(self.node_up) + node_down = self.model.GetModelPart("FluidModelPart").GetNode(self.node_down) + self.narrowing_width.append(node_up.Y - node_down.Y) + + + + + def ModifyInitialGeometry(self): + super().ModifyInitialGeometry() + self.IdentifyNodes() + self.SetUpFreeFormDeformation() + + + + def IdentifyNodes(self): + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + fixed_walls= self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls") + + number_of_nodes_walls = fixed_walls.NumberOfNodes() + number_of_nodes_down = control_down.NumberOfNodes() + number_of_nodes_up = control_down.NumberOfNodes() + + #get matrix of original coordinates + walls_coordinates = np.ones((int(number_of_nodes_walls),3)) + up_coordinates = np.ones((int(number_of_nodes_up),3)) + down_coordinates = np.ones((int(number_of_nodes_down),3)) + + counter = 0 + for node in control_down.Nodes: + down_coordinates[counter, 0] = node.X0 + down_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in control_up.Nodes: + up_coordinates[counter, 0] = node.X0 + up_coordinates[counter, 1] = node.Y0 + counter+=1 + + counter = 0 + for node in fixed_walls.Nodes: + walls_coordinates[counter, 0] = node.X0 + walls_coordinates[counter, 1] = node.Y0 + counter+=1 + + self.walls = walls_coordinates + + self.up = up_coordinates + at_3_y = np.where(self.up[:,1] == 3) + self.up = np.delete(self.up,at_3_y, 0) + + self.down = down_coordinates + at_0_y = np.where(self.down[:,1] == 0) + self.down = np.delete(self.down,at_0_y, 0) + + self.fixed_coordinates = np.r_[walls_coordinates, self.down, self.up] + + def SetUpFreeFormDeformation(self): + # #creating a free form deformation object for each control domain + self.ffd_up, self.ffd_down = set_up_phi() + + + def MoveControlPoints(self, scale_of_deformation=1): + + moved_up, moved_down, _, _ = phi(self.up,self.down,self.ffd_down,self.ffd_up, + self.deformation_multiplier,scale_of_deformation) + + + #Moving lower part + control_down = self.model.GetModelPart("FluidModelPart.GENERIC_ControlDown") + i=0 + for node in control_down.Nodes: + if node.Y0 != 0: + x_disp = moved_down[i,0] - node.X0 + y_disp = moved_down[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + node.X = node.X0 + x_disp + node.Y = node.Y0 + y_disp + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + #moving upper part + control_up = self.model.GetModelPart("FluidModelPart.GENERIC_ControlUp") + i=0 + for node in control_up.Nodes: + if node.Y0 != 3: + x_disp = moved_up[i,0] - node.X0 + y_disp = moved_up[i,1] - node.Y0 + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, x_disp ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, y_disp ) + node.X = node.X0 + x_disp + node.Y = node.Y0 + y_disp + i +=1 + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.moved_coordinates = np.r_[self.walls, moved_down, moved_up] + + + def UpdateRBF(self): + self.rbf = RBF(original_control_points = self.fixed_coordinates, deformed_control_points = + self.moved_coordinates, radius=0.75) + + + def LockOuterWalls(self): + for node in self.model.GetModelPart("FluidModelPart.GENERIC_FixedWalls").Nodes: + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_X,0, 0 ) + node.SetSolutionStepValue(KratosMultiphysics.MESH_DISPLACEMENT_Y,0, 0) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Fix(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + + + + def UpdateDeformationMultiplier(self): + self.deformation_multiplier = training_trajectory( self.time, self.deformation_multiplier, self.delta_deformation, self.maximum, self.minimum) + + + + + def InitializeSolutionStep(self): + super().InitializeSolutionStep() + #free all nodes + for node in self.model.GetModelPart("FluidModelPart").Nodes: + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_X) + node.Free(KratosMultiphysics.MESH_DISPLACEMENT_Y) + + self.UpdateDeformationMultiplier() + self.MoveControlPoints() + self.LockOuterWalls() + + + + + + + def FinalizeSolutionStep(self): + super().FinalizeSolutionStep() + self.StoreBifurcationData() + + ArrayOfResults = [] + for node in self._GetSolver().fluid_solver.GetComputingModelPart().Nodes: + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_X, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.VELOCITY_Y, 0)) + ArrayOfResults.append(node.GetSolutionStepValue(KratosMultiphysics.PRESSURE, 0)) + self.time_step_solution_container.append(ArrayOfResults) + + + + + def GetBifuracationData(self): + return self.velocity_y_at_control_point , self.narrowing_width, self.deformation_multiplier_list + + + + + def GetSnapshotsMatrix(self): + SnapshotMatrix = np.zeros((len(self.time_step_solution_container[0]), len(self.time_step_solution_container))) + for i in range(len(self.time_step_solution_container)): + Snapshot_i= np.array(self.time_step_solution_container[i]) + SnapshotMatrix[:,i] = Snapshot_i.transpose() + return SnapshotMatrix + + + + + + + + +def prepare_files(working_path, svd_truncation_tolerance): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] = working_path +f'/Results/ROM_{svd_truncation_tolerance}' + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + +def ROM(svd_truncation_tolerance): + + if not os.path.exists(f'./Results/ROM_{svd_truncation_tolerance}.post.bin'): + + basis = f'ROM/{svd_truncation_tolerance}.npy' + + if os.path.exists(basis): + u = np.load(basis) + else: + if not os.path.exists(f'./ROM/'): + os.mkdir(f'./ROM/') + u,s,_,_ = RandomizedSingularValueDecomposition().Calculate(np.load(f'Results/SnapshotMatrix.npy'), svd_truncation_tolerance) + np.save(basis,u) + + ### Saving the nodal basis ### (Need to make this more robust, hard coded here) + basis_POD={"rom_settings":{},"nodal_modes":{}} + basis_POD["rom_settings"]["nodal_unknowns"] = ["VELOCITY_X","VELOCITY_Y","PRESSURE"] + basis_POD["rom_settings"]["number_of_rom_dofs"] = np.shape(u)[1] + Dimensions = len(basis_POD["rom_settings"]["nodal_unknowns"]) + N_nodes=np.shape(u)[0]/Dimensions + N_nodes = int(N_nodes) + node_Id=np.linspace(1,N_nodes,N_nodes) + i = 0 + for j in range (0,N_nodes): + basis_POD["nodal_modes"][int(node_Id[j])] = (u[i:i+Dimensions].tolist()) + i=i+Dimensions + + with open('ProblemFiles/RomParameters.json', 'w') as f: + json.dump(basis_POD,f, indent=2) + + print('\n\nNodal basis printed in json format\n\n') + + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + #loading the bases + bases = [] + bases = None + simulation = ROM_Class(global_model, parameters) + simulation.Run() + + np.save(f'Results/ROM_snapshots_{svd_truncation_tolerance}.npy',simulation.GetSnapshotsMatrix()) + + vy_rom,w_rom,deformation_multiplier = simulation.GetBifuracationData() + + np.save(f'Results/y_velocity_ROM_{svd_truncation_tolerance}.npy', vy_rom) + np.save(f'Results/narrowing_ROM_{svd_truncation_tolerance}.npy', w_rom) + np.save(f'Results/deformation_multiplier_{svd_truncation_tolerance}.npy', deformation_multiplier) + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= 1 + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + prepare_files(working_path, svd_truncation_tolerance) + + ROM(svd_truncation_tolerance) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/TrainHROM_Step1.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/TrainHROM_Step1.py new file mode 100644 index 00000000..3fe72a60 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/TrainHROM_Step1.py @@ -0,0 +1,104 @@ +import KratosMultiphysics +from Run_ROM import ROM_Class + + +import KratosMultiphysics.RomApplication as romapp +import json +import numpy as np + + + + +import os.path + + +class TrainHROMClass(ROM_Class): + + def __init__(self, model, project_parameters,svd_truncation_tolerance): + super().__init__(model, project_parameters, hrom="EmpiricalCubature") + self.svd_truncation_tolerance = svd_truncation_tolerance + + + + + + + +def Train_HROM(svd_truncation_tolerance): + + projected_residuals = f'HROM/Sr_{svd_truncation_tolerance}.npy' + + + if not os.path.exists(projected_residuals): + with open("ProblemFiles/ProjectParameters_modified.json", 'r') as parameter_file: + parameters = KratosMultiphysics.Parameters(parameter_file.read()) + global_model = KratosMultiphysics.Model() + correct_clusters = None + + + #loading the bases + bases = [] + bases = None + simulation = TrainHROMClass(global_model, parameters, svd_truncation_tolerance) + simulation.Run() + + + + + + + + + +def prepare_files(working_path): + """pre-pending the absolut path of the files in the Project Parameters""" + with open(working_path+'/ProblemFiles/ProjectParameters.json','r') as f: + updated_project_parameters = json.load(f) + file_input_name = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] + materials_filename = updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] + gid_output_name = updated_project_parameters["output_processes"]["gid_output"][0]["Parameters"]["output_name"] + + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["model_import_settings"]["input_filename"] = working_path + '/ProblemFiles/'+ file_input_name + updated_project_parameters["solver_settings"]["fluid_solver_settings"]["material_import_settings"]["materials_filename"] = working_path +'/ProblemFiles/'+ materials_filename + updated_project_parameters["output_processes"]["gid_output"] = [] + + with open(working_path+'/ProblemFiles/ProjectParameters_modified.json','w') as f: + json.dump(updated_project_parameters, f, indent = 4) + + + + + + + + + + + + + + + + + +if __name__=="__main__": + + #library for passing arguments to the script from bash + from sys import argv + + Launch_Simulation = bool(int(argv[1])) + Number_Of_Clusters= int(argv[2]) + svd_truncation_tolerance= float(argv[3]) + clustering= argv[4] + overlapping = int(argv[5]) + working_path = argv[6] + + + prepare_files(working_path) + + Train_HROM(svd_truncation_tolerance) + + # np.save(f'Results/y_velocity_{Number_Of_Clusters}_clusters.npy', vy_rom) + # np.save(f'Results/narrowing_{Number_Of_Clusters}_clusters.npy', w_rom) + + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/TrainHROM_Step2.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/TrainHROM_Step2.py new file mode 100644 index 00000000..ac50c49c --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/TrainHROM_Step2.py @@ -0,0 +1,155 @@ +import numpy as np +from KratosMultiphysics.RomApplication.empirical_cubature_method import EmpiricalCubatureMethod +from KratosMultiphysics.RomApplication.randomized_singular_value_decomposition import RandomizedSingularValueDecomposition +from matplotlib import pyplot as plt + +import os.path +import os + + + + +def select_elements(svd_truncation_tolerance, residuals_svd_truncation_tolerance): + + weights = f'HROM/WeightsMatrix_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + elements = f'HROM/Elementsvector_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy' + + if not os.path.exists(weights) and not os.path.exists(elements): + #u,_,_,_ = RandomizedSingularValueDecomposition(RELATIVE_SVD=True).Calculate( np.load(f'HROM/Sr.npy'), tol) # HEAVY!!! + u = np.load(f'HROM/basis_{svd_truncation_tolerance}_{residuals_svd_truncation_tolerance}.npy') + + hyper_reduction_element_selector = EmpiricalCubatureMethod() + hyper_reduction_element_selector.SetUp(u) #add again z + hyper_reduction_element_selector.Initialize() + hyper_reduction_element_selector.Calculate() + + + w = np.squeeze(hyper_reduction_element_selector.w) + z = np.squeeze(hyper_reduction_element_selector.z) + + WeightsMatrix = w.reshape(np.size(z),1) + + np.save(weights, WeightsMatrix ) + np.save(elements, z) + + + +def split_matrix_in_columns(svd_truncation_tolerance): + + array_name = f'HROM/Sr_{svd_truncation_tolerance}' + + if not os.path.exists(array_name + '/column_block1.npy'): + + #load array + array = np.load(array_name+'.npy') + + + # Create a folder with the given name + if not os.path.exists(array_name): + os.makedirs(array_name) + + # Create the spliting of the matrix inside the folder + if not os.path.exists(array_name + '/column_block1.npy'): + n_rows, n_cols = array.shape + block_size = n_rows + + start_col = 0 + block_number = 1 + + while start_col < n_cols: + end_col = min(start_col + block_size, n_cols) + + # Check if the remaining columns are too few; if so, merge with the previous block + if n_cols - end_col < block_size / 2 and start_col != 0: + end_col = n_cols + + # Slice the array and save + block = array[:, start_col:end_col] + np.save(os.path.join(array_name, f'column_block{block_number}.npy'), block) + + start_col = end_col + block_number += 1 + + os.remove(array_name+'.npy') + + +def get_global_basis(svd_truncation_tolerance): + + if not os.path.exists(f'HROM/global_basis_{svd_truncation_tolerance}.npy'): + + array_name = f'HROM/Sr_{svd_truncation_tolerance}' + + # List all .npy files in the folder + files = [f for f in os.listdir(array_name) if f.endswith('.npy')] + + u = None + + for file in files: + file_path = os.path.join(array_name, file) + + # Load the file + data = np.load(file_path) + + if u is None: + u, s ,_ = np.linalg.svd(data, full_matrices=False) + else: + print('updating basis') + u2, s2, _ = np.linalg.svd(data, full_matrices=False) + u, s, _ = np.linalg.svd(np.c_[u*s, u2*s2], full_matrices=False) + + #store global basis and global singular values + np.save(f'HROM/global_basis_{svd_truncation_tolerance}.npy',u) + np.save(f'HROM/global_singular_values_{svd_truncation_tolerance}.npy',s) + + + +def truncated_svd(u,s,epsilon=0): + tol = np.finfo(float).eps*max(s)/2 + R = np.sum(s > tol) # Definition of numerical rank + if epsilon == 0: + K = R + else: + SingVsq = np.multiply(s,s) + SingVsq.sort() + normEf2 = np.sqrt(np.cumsum(SingVsq)) + epsilon = epsilon*normEf2[-1] #relative tolerance + T = (sum(normEf2 total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #get list containing snapshots to add to each overlapped cluster + if overlaping_snapshots is not 0: + snapshots_to_add = {} + for i in range(time_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == time_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(time_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + + +def ismember(A, B): + if isinstance(A, np.int_): + return [ np.sum(A == B) ] + else: + return [ np.sum(a == B) for a in A ] + +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + kmeans = KMeans(n_clusters=narrowing_clusters, random_state=0).fit(narrowing.reshape(-1,1)) + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(narrowing_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + correct_cluster = kmeans.labels_ + centroids = kmeans.cluster_centers_ + + if narrowing_clusters>1: + #try and use as is solution manifold neighbor identification + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + narrowing = narrowing.reshape(1,-1) + for i in range(np.shape(narrowing)[1]): + this_matrix = (kmeans.cluster_centers_).T - narrowing[:,i].reshape(np.shape(narrowing)[0], 1) + distance = np.zeros((narrowing_clusters)) + for j in range(narrowing_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + #get list containing snapshots to add to each overlapped cluster + if True: + #if overlaping_snapshots is not 0: + + snapshots_to_add = [] + for j in range(narrowing_clusters): + N_neighbors = len(neighbors[j]) + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + ith_narrowing_cluster = narrowing[:,kmeans.labels_==neighbors[j][i]] + this_matrix = ith_narrowing_cluster - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(narrowing)[0], 1) + distance = np.linalg.norm(this_matrix, axis = 0) + #distance = np.zeros(np.shape(ith_narrowing_cluster[1])) + #for k in range(len(distance)): + # distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + + return sub_snapshots, correct_cluster + + +def solution_manifold_clustering(): + pass + + + +if __name__=='__main__': + #S = np.load('SnapshotMatrix.npy') + #narrowing = np.load('narrowing.npy') + narrowing = np.linspace(0,1,12) + S = np.array([[1,2,3,4,5,6,7,8,9,10,11,12],[1,2,3,4,5,6,7,8,9,10,11,12]]) + #a = narrowing.reshape(1,-1) + #S = np.r_[a, a , a, a] + sub_snapshots, correct_cluster = time_clustering(S, 3,0) + #sub_snapshots, correct_cluster = narrowing_clustering(S, narrowing, 3, 2) + #sub_snapshots, correct_cluster = solution_manifold_clustering(S) + #sub_snapshots, correct_cluster = time_clustering(S) + kkk = 5 + + # + + +""" + +def solution_manifold_clustering(S, solution_manifold_clusters = 3, overlaping_snapshots = 1 ): + #S = np.load('SnapshotMatrix.npy') + kmeans = KMeans(n_clusters = solution_manifold_clusters, random_state=0).fit(S.T) + correct_cluster = kmeans.labels_ + + #split snapshots into sub-sets + sub_snapshots={} + neighbors={} + for i in range(solution_manifold_clusters): + sub_snapshots[i] = S[:,kmeans.labels_==i] + neighbors[i] = [] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns before overlapping') + + #identify the two nearest cluster centroids to state i and mark these clusters as neighbors + for i in range(np.shape(S)[1]): + this_matrix = (kmeans.cluster_centers_).T - S[:,i].reshape(np.shape(S)[0], 1) + distance = np.zeros((solution_manifold_clusters)) + for j in range(solution_manifold_clusters): + distance[j] = np.linalg.norm(this_matrix[:,j]) + second_nearest_idx = np.argsort(distance)[1] + if not(sum(ismember(neighbors[kmeans.labels_[i]],second_nearest_idx))): + neighbors[kmeans.labels_[i]].append(second_nearest_idx) + + snapshots_to_add = [] + + for j in range(solution_manifold_clusters): + N_snaps = np.shape(sub_snapshots[j])[1] + N_neighbors = len(neighbors[j]) + + N_add = overlaping_snapshots #number of snapshots to add to subset i (on each direction) + for i in range(N_neighbors): + print('adding neighbors from ', neighbors[j][i], 'to cluster ', j ) + this_matrix = sub_snapshots[neighbors[j][i]] - ((kmeans.cluster_centers_[j]).T).reshape(np.shape(S)[0], 1) + distance = np.zeros(np.shape(sub_snapshots[neighbors[j][i]][1])) + for k in range(len(distance)): + distance[k] = np.linalg.norm(this_matrix[:,k]) + indices_to_add = np.argsort(distance) + if i==0: + snapshots_to_add.append(sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]]) + else: + snapshots_to_add[j] = np.c_[ snapshots_to_add[j] , sub_snapshots[neighbors[j][i]][:,indices_to_add[:N_add]] ] + + for j in range(solution_manifold_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + + +""" +This is wrong, but save for now as reference +def narrowing_clustering(S, narrowing, narrowing_clusters = 3, overlaping_snapshots = 1 ): + # wrong implementation :( + # MINE (no k-means) + #S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + #narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + correct_cluster = np.empty(narrowing.shape) + for i in range(narrowing_clusters): + # In this implementation, I just shuffle (order) the snapshots to match the narrowing width. No time-relation whatsoever + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + correct_cluster[intersection] = i + ith_narrowing = narrowing[intersection] + ith_indexes_ordered = np.argsort(ith_narrowing) + sub_snapshots[i] = S[:,ith_indexes_ordered] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + # storing centroids + if i==0: + centroids = np.sum(ith_narrowing)/(ith_narrowing.shape[0]) + else: + centroids = np.c_[centroids, np.sum(ith_narrowing)/(ith_narrowing.shape[0])] + np.save('cluster_centroid.npy', centroids) + #overlapping after correct cluster definition + + #get list containing snapshots to add to each overlapped cluster + snapshots_to_add = {} + for i in range(narrowing_clusters): + if i == 0: + snapshots_to_add[0] = sub_snapshots[1][:,:overlaping_snapshots] + elif i == narrowing_clusters-1: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + else: + snapshots_to_add[i] = sub_snapshots[i-1][:, -overlaping_snapshots:] + snapshots_to_add[i] = np.c_[snapshots_to_add[i], sub_snapshots[i+1][:, :overlaping_snapshots] ] + + #actually enlarging sub_snapshots + for j in range(narrowing_clusters): + sub_snapshots[j] = np.c_[sub_snapshots[j], snapshots_to_add[j]] + print(f'{j}\'th sub-snapshot contains',(np.shape(sub_snapshots[j])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster + +""" + + +""" +def time_clustering(time_clusters = 5, overlaping_snapshots = 1 ): + #it works, but no overlapping + S = np.load('SnapshotMatrix.npy') + total_time_steps = S.shape[1] + if time_clusters > total_time_steps: + raise error + sub_snapshots = np.array_split(S,time_clusters, axis=1) + + for i in range(time_clusters): + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + + return sub_snapshots, correct_cluster +""" + + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + #no overlapping. MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + return sub_snapshots, correct_cluster +""" + +""" +def narrowing_clustering(narrowing_clusters = 3, overlaping_snapshots = 1 ): + # MINE (no k-means) + S = np.load('SnapshotMatrix.npy') + total_snapshots = S.shape[1] + narrowing = np.load('narrowing.npy') + MAX = np.max(narrowing) + MIN = np.min(narrowing) + print('the maximum is ',MAX, ' and the minimum is: ', MIN) + sub_snapshots = {} + step = (MAX - MIN)/ (narrowing_clusters + 1) + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + sub_snapshots[i] = S[:,intersection] + if i == 0: + correct_cluster = np.full((sub_snapshots[0].shape[1],), 0 ) + else: + correct_cluster = np.r_[correct_cluster, np.full((sub_snapshots[i].shape[1],), i )] + print(f'the {i}th subsnapsht has shape: ',sub_snapshots[i].shape) + print('with minimum value: ',np.min(narrowing[intersection])) + print('with maximum value: ', np.max(narrowing[intersection]),'\n') + + #overlapping after correct cluster definition + # In this implementation, I just shuffle the snapshots to match the narrowing width. No time relation whatsoever + for i in range(narrowing_clusters): + lower_bounds = np.where(narrowing > (MIN + (step*(i) )))[0] + uppper_bounds = np.where(narrowing < (MIN + (step*(i+1) )))[0] + intersection = np.intersect1d(lower_bounds, uppper_bounds) + if i == 0: + ith_narrowing = narrowing[intersection] + + ith_indexes = np.argsort(ith_narrowing) + ith_narrowing_ordered = ith_narrowing[ith_indexes] + plt.plot(ith_narrowing, 'b') + plt.plot(ith_narrowing_ordered, 'r') + plt.show() + + elif i == narrowing_clusters-1: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + else: + sub_snapshots[i] = np.c_[sub_snapshots[i-1][:, -overlaping_snapshots:], sub_snapshots[i]] + sub_snapshots[i] = np.c_[sub_snapshots[i] , sub_snapshots[i+1][:, :overlaping_snapshots] ] + print(f'{i}\'th sub-snapshot contains',(np.shape(sub_snapshots[i])[1]), 'columns after overlapping') + + return sub_snapshots, correct_cluster +""" + diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/plot_bifurcation.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/plot_bifurcation.py new file mode 100644 index 00000000..8b56aa1e --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/plot_bifurcation.py @@ -0,0 +1,65 @@ +import numpy as np +from matplotlib import pyplot as plt + + + +if __name__=='__main__': + #library for passing arguments to the script from bash + from sys import argv + + + Number_Of_Clusters= int(argv[1]) + + + + vy = np.load('Results/Velocity_y.npy') + w = np.load('Results/narrowing.npy') + vy_rom = np.load(f'Results/y_velocity_ROM.npy') + w_rom = np.load(f'Results/narrowing_ROM.npy') + + + #plt.title(r'Singular Values for matrix $ S^{(2)} $', fontsize=15, fontweight='bold') + #plt.title(r'$\alpha $ \textbf{AA}!', fontsize=16, color='r') + #plt.title(f'ROM VS FOM') + + plt.rc('text', usetex=True) + plt.rc('font', family='serif') + + plt.plot(vy, w, 'b', label = 'FOM', linewidth = 3, alpha=0.5) #linewidth = 3 + plt.plot(vy_rom, w_rom, 'r', label = 'ROM', linewidth = 3, alpha=0.5) + #plt.title(r'FOM vs ROM', fontsize=20, fontweight='bold') + plt.legend() + #plt.grid() + # plt.xticks(np.arange(-3.5,0.25,0.25)) #TODO the ticks are not easily beautyfied, do it later :) + # plt.yticks(np.arange(0,3.1,0.25)) + plt.xlabel(r'$v_y^*$', size=15, fontweight='bold') + plt.ylabel(r'$w_c$',size=15,fontweight='bold') + + plt.savefig('Results/fom_vs_rom') + plt.show() + + + + + # import numpy as np + # import matplotlib.pyplot as plt + + + # # Example data + # t = np.arange(0.0, 1.0 + 0.01, 0.01) + # s = np.cos(4 * np.pi * t) + 2 + + # plt.rc('text', usetex=True) + # plt.rc('font', family='serif') + # plt.plot(t, s) + + # plt.xlabel(r'\textbf{time} (s)') + # plt.ylabel(r'\textit{voltage} (mV)',fontsize=16) + # plt.title(r"\TeX\ is Number " + # r"$\displaystyle\sum_{n=1}^\infty\frac{-e^{i\pi}}{2^n}$!", + # fontsize=16, color='gray') + # # Make room for the ridiculously large title. + # plt.subplots_adjust(top=0.8) + + # plt.savefig('tex_demo') + # plt.show() \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/plot_full_bifurcation.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/plot_full_bifurcation.py new file mode 100644 index 00000000..9c96c6c6 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/plot_full_bifurcation.py @@ -0,0 +1,31 @@ +import numpy as np +from matplotlib import pyplot as plt + + + +if __name__=='__main__': + + + vy = np.load('Results/Velocity_y.npy') + w = np.load('Results/narrowing.npy') + vy_rom = np.load(f'Results/y_velocity_ROM.npy') + w_rom = np.load(f'Results/narrowing_ROM.npy') + vy_hrom = np.load(f'Results/y_velocity_HROM.npy') + w_hrom = np.load(f'Results/narrowing_HROM.npy') + + plt.rc('text', usetex=True) + plt.rc('font', family='serif') + + plt.plot(vy, w, 'b', label = 'FOM', linewidth = 3, alpha=0.5) #linewidth = 3 + plt.plot(vy_rom, w_rom, 'r', label = 'ROM', linewidth = 3, alpha=0.5) + plt.plot(vy_hrom, w_hrom, 'm', label = 'HROM', linewidth = 3, alpha=0.5) + + plt.legend() + #plt.grid() + # plt.xticks(np.arange(-3.5,0.25,0.25)) #TODO the ticks are not easily beautyfied, do it later :) + # plt.yticks(np.arange(0,3.1,0.25)) + plt.xlabel(r'$v_y^*$', size=15, fontweight='bold') + plt.ylabel(r'$w_c$',size=15,fontweight='bold') + + plt.savefig('Results/fom_vs_rom_vs_hrom') + plt.show() \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/simulation_trajectories.py b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/simulation_trajectories.py new file mode 100644 index 00000000..80f2221d --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/ProblemFiles/simulation_trajectories.py @@ -0,0 +1,44 @@ +import numpy as np + +def training_trajectory(time, deformation_multiplier, delta_deformation, maximum, minimum): + #THIS IS INVERTED W.R.T. THE FIRST EXAMPLE IN THE PAPER + #### Test trajectory#### + if time>10.0 and time<=31.0: # start modifying narrowing from 10 seconds onwards + deformation_multiplier-= delta_deformation + if deformation_multiplier < minimum: + deformation_multiplier = minimum + elif time>31.0: + deformation_multiplier+= delta_deformation + if deformation_multiplier > maximum: + deformation_multiplier = maximum + return deformation_multiplier + + +def testing_trajectory(time, deformation_multiplier, delta_deformation, maximum, minimum): + #THIS IS INVERTED W.R.T. THE FIRST EXAMPLE IN THE PAPER + ####Train trajectory#### + if time>10.0 and time<=31.0: # start modifying narrowing from 10 seconds onwards + deformation_multiplier+=delta_deformation + if deformation_multiplier > maximum: + deformation_multiplier = maximum + elif time>31.0: + deformation_multiplier-=delta_deformation + if deformation_multiplier < minimum: + deformation_multiplier = minimum + return deformation_multiplier + + +def second_testing_trajectory(t, T=100): + """ + A further adjusted time-dependent function using trigonometric functions. + This function starts at 1 when t=0, reaches 0 several times in the range t ∈ [0, 100], + and includes more ups and downs without being noisy. + The function takes a time parameter 't' and a period 'T'. + """ + # Normalizing time t to the range [0, 2*pi] + fixed_deformation_factor = 11 + normalized_t = (2 * np.pi * t) / T + + # Defining the function using a combination of sine and cosine functions + # with a phase shift and frequency adjustments for more variations + return (1 - (0.5 * (1 + np.sin(normalized_t - np.pi/2) * np.cos(3 * normalized_t)))) * fixed_deformation_factor diff --git a/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/launch_ale_romnord3.sh b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/launch_ale_romnord3.sh new file mode 100755 index 00000000..67db8d41 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/AllFiles_requireKratosBranch/Example2/Nonaffine/launch_ale_romnord3.sh @@ -0,0 +1,102 @@ +#!/bin/sh +#SBATCH -N 1 # nodes requested +#SBATCH -n 1 # tasks requested +#SBATCH -c 16 # cores requested +#SBATCH -t 20:00:00 # time requested in hour:minute:second + + + +export OMP_NUM_THREADS=16 +export PROBLEMS_PATH=$PWD/ProblemFiles +export LANGUAGE=en_GB.utf8 +export LC_ALL=en_GB.utf8 + + +FOM=False #(storing results) +FOM_test=True #(storing results) +Run_ROM=False #3 (storing results) +ROM_test=True #4 = (storing results) +Train_HROM_Step1=False #5 = (creating projected residuals matrices {Sr_i}_i=1^k (one per basis)) +Train_HROM_Step2=False #6 = ontain a reduced set of elements and weights starting from the projected residuals matrices Sr_i +Run_HROM=False #7 = RunHROM Train Trajectory +HROM_test=True #8 = RunHROM Test Trajectory + +plot_partial_hysteresis=False + +#parameters used in Local POD: + +# parameters for the simulations +Launch_Simulation=1 +Number_Of_Clusters=1 #not used in global POD +svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +clustering="narrowing" #time # +overlapping=30 +residuals_svd_truncation_tolerance_list=(1e-3 1e-4 1e-5 1e-6) +residuals_svd_relative_to_global_residuals_snapshots=1 + + +if [ $FOM = True ] + then + #### LAUNCH FOM TRAIN TRAJECTORY #### + # MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLauching FOM \n\n\n\n\n\n" + python3 ProblemFiles/FOM.py $PWD +fi +if [ $FOM_test = True ] + then + # NEW MASTER + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/KratosMaster/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching FOM test trajectory \n\n\n\n\n\n" + python3 ProblemFiles/FOM_TestTrajectory.py $PWD +fi +for j in ${svd_truncation_tolerance_list[@]} +do + svd_truncation_tolerance=$j + if [ $Run_ROM = True ] + then + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo "\n\n\n\n\n\nLaunching ROM \n\n\n\n\n\n" + python3 ProblemFiles/Run_ROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $ROM_test = True ] + then + #### LAUNCH ROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\nlaunching ROM test\n\n\n\n' + python3 ProblemFiles/ROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + if [ $Train_HROM_Step1 = True ] + then + #### TrainHROM (Creating Matrix of projected resduals Sr) #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\nlaunching TrainHROM train\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step1.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD + fi + for k in ${residuals_svd_truncation_tolerance_list[@]} + do + residuals_svd_truncation_tolerance=$k + if [ $Train_HROM_Step2 = True ] + then + ### Obtain Reduced Elements and Weights #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nlaunching HROM elements and Weights\n\n\n\n\n\n' + python3 ProblemFiles/TrainHROM_Step2.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $Run_HROM = True ] + then + #### LAUNCH HROM TRAIN TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo '\n\n\n\n\n\nLaunching HROM train\n\n\n\n\n\n\n' + python3 ProblemFiles/Run_HROM.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + if [ $HROM_test = True ] + then + #### LAUNCH HROM TEST TRAJECTORY #### + source /gpfs/projects/bsc44/bsc44011/KratosInstallations/UpdatedKratosALE/Kratos_POD_ALE/Kratos/scripts/Kratos_env.sh + echo 'Launching HROM test' + python3 ProblemFiles/HROM_TestTrajectory.py $Launch_Simulation $Number_Of_Clusters $svd_truncation_tolerance $clustering $overlapping $PWD $residuals_svd_truncation_tolerance $residuals_svd_relative_to_global_residuals_snapshots + fi + done +done + diff --git a/rom_application/ContractionExpansionChannel/Affine_Mapping/FOM.py b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/FOM.py similarity index 100% rename from rom_application/ContractionExpansionChannel/Affine_Mapping/FOM.py rename to rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/FOM.py diff --git a/rom_application/ContractionExpansionChannel/Affine_Mapping/FOM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/FOM_TestTrajectory.py similarity index 100% rename from rom_application/ContractionExpansionChannel/Affine_Mapping/FOM_TestTrajectory.py rename to rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/FOM_TestTrajectory.py diff --git 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669 + 709 + End SubModelPartNodes + Begin SubModelPartElements + End SubModelPartElements + Begin SubModelPartConditions + End SubModelPartConditions +End SubModelPart diff --git a/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/FluidMaterials.json b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/FluidMaterials.json new file mode 100644 index 00000000..24e1bedf --- /dev/null +++ b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/FluidMaterials.json @@ -0,0 +1,16 @@ +{ + "properties" : [{ + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "properties_id" : 1, + "Material" : { + "constitutive_law" : { + "name" : "Newtonian2DLaw" + }, + "Variables" : { + "DENSITY" : 1.0, + "DYNAMIC_VISCOSITY" : 0.1 + }, + "Tables" : {} + } + }] +} diff --git a/rom_application/ContractionExpansionChannel/Affine_Mapping/ProblemFiles/ProjectParameters.json b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/ProjectParameters.json similarity index 100% rename from rom_application/ContractionExpansionChannel/Affine_Mapping/ProblemFiles/ProjectParameters.json rename to rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/ProjectParameters.json diff --git a/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/ProjectParameters_modified.json b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/ProjectParameters_modified.json new file mode 100644 index 00000000..f7357135 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/ProjectParameters_modified.json @@ -0,0 +1,187 @@ +{ + "analysis_stage": "KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis", + "problem_data": { + "problem_name": "2DFlowBifurcationKratosStructuredMeshWorkingRicc", + "parallel_type": "OpenMP", + "echo_level": 0, + "start_time": 0.0, + "end_time": 244 + }, + "output_processes": { + "gid_output": [ + { + "python_module": "gid_output_process", + "kratos_module": "KratosMultiphysics", + "process_name": "GiDOutputProcess", + "help": "This process writes postprocessing files for GiD", + "Parameters": { + "model_part_name": "FluidModelPart.fluid_computational_model_part", + "output_name": "/home/jbravo/OtherRepos/Examples/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/Results/FOM", + "postprocess_parameters": { + "result_file_configuration": { + "gidpost_flags": { + "GiDPostMode": "GiD_PostBinary", + "WriteDeformedMeshFlag": "WriteDeformed", + "WriteConditionsFlag": "WriteConditions", + "MultiFileFlag": "SingleFile" + }, + "file_label": "time", + "output_control_type": "time", + "output_interval": 0.5, + "body_output": true, + "node_output": false, + "skin_output": false, + "plane_output": [], + "nodal_results": [ + "VELOCITY", + "PRESSURE", + "MESH_DISPLACEMENT" + ], + "gauss_point_results": [], + "nodal_nonhistorical_results": [] + }, + "point_data_configuration": [] + } + } + } + ], + "vtk_output": [], + "rom_output": [] + }, + "solver_settings": { + "solver_type": "ale_fluid", + "ale_boundary_parts": [], + "mesh_motion_solver_settings": { + "solver_type": "structural_similarity" + }, + "fluid_solver_settings": { + "model_part_name": "FluidModelPart", + "domain_size": 2, + "solver_type": "Monolithic", + "model_import_settings": { + "input_type": "mdpa", + "input_filename": "/home/jbravo/OtherRepos/Examples/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/2DFlowBifurcationKratosStructuredMeshWorkingRicc" + }, + "material_import_settings": { + "materials_filename": "/home/jbravo/OtherRepos/Examples/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/ProblemFiles/FluidMaterials.json" + }, + "echo_level": 0, + "compute_reactions": false, + "maximum_iterations": 10, + "relative_velocity_tolerance": 1e-08, + "absolute_velocity_tolerance": 1e-08, + "relative_pressure_tolerance": 1e-08, + "absolute_pressure_tolerance": 1e-08, + "volume_model_part_name": "FluidParts_Volume", + "skin_parts": [ + "Outlet2D_Outlet", + "NoSlip2D_Wall" + ], + "no_skin_parts": [ + "VelocityConstraints2D_Inlet-Total" + ], + "time_scheme": "bossak", + "time_stepping": { + "automatic_time_step": false, + "time_step": 0.1 + }, + "formulation": { + "element_type": "qsvms", + "use_orthogonal_subscales": false, + "dynamic_tau": 1.0 + }, + "reform_dofs_at_each_step": false + } + }, + "processes": { + "initial_conditions_process_list": [], + "boundary_conditions_process_list": [ + { + "python_module": "apply_outlet_process", + "kratos_module": "KratosMultiphysics.FluidDynamicsApplication", + "process_name": "ApplyOutletProcess", + "Parameters": { + "model_part_name": "FluidModelPart.Outlet2D_Outlet", + "variable_name": "PRESSURE", + "constrained": true, + "value": 0.0, + "hydrostatic_outlet": false, + "h_top": 0.0 + } + }, + { + "python_module": "apply_noslip_process", + "kratos_module": "KratosMultiphysics.FluidDynamicsApplication", + "process_name": "ApplyNoSlipProcess", + "Parameters": { + "model_part_name": "FluidModelPart.NoSlip2D_Wall" + } + }, + { + "python_module": "assign_vector_variable_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorVariableProcess", + "Parameters": { + "model_part_name": "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name": "VELOCITY", + "interval": [ + 0.0, + 1 + ], + "constrained": [ + true, + true, + true + ], + "value": [ + "y*(3-y)*sin(pi*t*0.5)", + 0.0, + 0.0 + ] + } + }, + { + "python_module": "assign_vector_variable_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorVariableProcess", + "Parameters": { + "model_part_name": "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name": "VELOCITY", + "interval": [ + 0.0, + "End" + ], + "constrained": [ + true, + true, + true + ], + "value": [ + "y*(3-y)", + 0.0, + 0.0 + ] + } + } + ], + "gravity": [ + { + "python_module": "assign_vector_by_direction_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorByDirectionProcess", + "Parameters": { + "model_part_name": "FluidModelPart.FluidParts_Volume", + "variable_name": "BODY_FORCE", + "modulus": 0.0, + "constrained": false, + "direction": [ + 0.0, + -1.0, + 0.0 + ] + } + } + ], + "auxiliar_process_list": [] + } +} \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/Affine_Mapping/simulation_trajectories.py b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/simulation_trajectories.py similarity index 100% rename from rom_application/ContractionExpansionChannel/Affine_Mapping/simulation_trajectories.py rename to rom_application/ContractionExpansionChannel/FilesInKratosMaster/Affine_Mapping/simulation_trajectories.py diff --git a/rom_application/ContractionExpansionChannel/FFD_plus_RBF/FOM.py b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/FOM.py similarity index 100% rename from rom_application/ContractionExpansionChannel/FFD_plus_RBF/FOM.py rename to rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/FOM.py diff --git a/rom_application/ContractionExpansionChannel/FFD_plus_RBF/FOM_TestTrajectory.py b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/FOM_TestTrajectory.py similarity index 100% rename from rom_application/ContractionExpansionChannel/FFD_plus_RBF/FOM_TestTrajectory.py rename to rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/FOM_TestTrajectory.py diff --git a/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/FluidMaterials.json b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/FluidMaterials.json new file mode 100644 index 00000000..24e1bedf --- /dev/null +++ b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/FluidMaterials.json @@ -0,0 +1,16 @@ +{ + "properties" : [{ + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "properties_id" : 1, + "Material" : { + "constitutive_law" : { + "name" : "Newtonian2DLaw" + }, + "Variables" : { + "DENSITY" : 1.0, + "DYNAMIC_VISCOSITY" : 0.1 + }, + "Tables" : {} + } + }] +} diff --git a/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/NonlinearInGiD.mdpa b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/NonlinearInGiD.mdpa new file mode 100644 index 00000000..ec99bbdb --- /dev/null +++ b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/NonlinearInGiD.mdpa @@ -0,0 +1,17117 @@ +Begin ModelPartData +// VARIABLE_NAME value +End ModelPartData + +Begin Properties 0 +End Properties + +Begin Nodes + 1 0.0000000000 3.0000000000 0.0000000000 + 2 0.0000000000 2.9000000000 0.0000000000 + 3 0.1000000000 3.0000000000 0.0000000000 + 4 0.1027312675 2.8660123659 0.0000000000 + 5 0.0000000000 2.8000000000 0.0000000000 + 6 0.2000000000 3.0000000000 0.0000000000 + 7 0.1996673628 2.9159025624 0.0000000000 + 8 0.1155849631 2.7642454797 0.0000000000 + 9 0.2011352789 2.8159261534 0.0000000000 + 10 0.3000000000 3.0000000000 0.0000000000 + 11 0.0000000000 2.7000000000 0.0000000000 + 12 0.2869617884 2.8671468409 0.0000000000 + 13 0.2032025607 2.7161528072 0.0000000000 + 14 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Group Inlet//Total // Subtree VelocityConstraints2D + Begin SubModelPartNodes + 1 + 2 + 5 + 11 + 18 + 26 + 35 + 48 + 62 + 79 + 95 + 115 + 135 + 160 + 185 + 209 + 237 + 261 + 281 + 305 + 330 + 361 + 399 + 439 + 482 + 528 + 572 + 615 + 661 + 708 + 750 + End SubModelPartNodes + Begin SubModelPartElements + End SubModelPartElements + Begin SubModelPartConditions + End SubModelPartConditions +End SubModelPart +Begin SubModelPart VelocityConstraints2D_Inlet-Custom2 // Group Inlet//Custom2 // Subtree VelocityConstraints2D + Begin SubModelPartNodes + 1 + 2 + 5 + 11 + 18 + 26 + 35 + 48 + 62 + 79 + 95 + 115 + 135 + 160 + 185 + 209 + 237 + 261 + 281 + 305 + 330 + 361 + 399 + 439 + 482 + 528 + 572 + 615 + 661 + 708 + 750 + End SubModelPartNodes + Begin SubModelPartElements + End SubModelPartElements + Begin SubModelPartConditions + End SubModelPartConditions +End SubModelPart diff --git a/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/ProjectParameters.json b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/ProjectParameters.json new file mode 100644 index 00000000..28091bcf --- /dev/null +++ b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/ProjectParameters.json @@ -0,0 +1,143 @@ +{ + "analysis_stage": "KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis", + "problem_data" : { + "problem_name" : "NonlinearInGiD", + "parallel_type" : "OpenMP", + "echo_level" : 0, + "start_time" : 0.0, + "end_time" : 52 + }, + "output_processes" : { + "gid_output" : [{ + "python_module" : "gid_output_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "GiDOutputProcess", + "help" : "This process writes postprocessing files for GiD", + "Parameters" : { + "model_part_name" : "FluidModelPart.fluid_computational_model_part", + "output_name" : "NonlinearInGiD", + "postprocess_parameters" : { + "result_file_configuration" : { + "gidpost_flags" : { + "GiDPostMode" : "GiD_PostBinary", + "WriteDeformedMeshFlag" : "WriteDeformed", + "WriteConditionsFlag" : "WriteConditions", + "MultiFileFlag" : "SingleFile" + }, + "file_label" : "time", + "output_control_type" : "time", + "output_interval" : 0.1, + "body_output" : true, + "node_output" : false, + "skin_output" : false, + "plane_output" : [], + "nodal_results" : ["VELOCITY","PRESSURE","MESH_DISPLACEMENT"], + "gauss_point_results" : [], + "nodal_nonhistorical_results" : [] + }, + "point_data_configuration" : [] + } + } + }], + "vtk_output" : [] + }, + "solver_settings" : { + "solver_type": "ale_fluid", + "ale_boundary_parts": [], + "mesh_motion_solver_settings" : { + "solver_type" : "structural_similarity" + }, + "fluid_solver_settings": { + "model_part_name" : "FluidModelPart", + "domain_size" : 2, + "solver_type" : "Monolithic", + "model_import_settings" : { + "input_type" : "mdpa", + "input_filename" : "NonlinearInGiD" + }, + "material_import_settings" : { + "materials_filename" : "FluidMaterials.json" + }, + "echo_level" : 0, + "compute_reactions" : false, + "maximum_iterations" : 10, + "relative_velocity_tolerance" : 0.001, + "absolute_velocity_tolerance" : 1e-5, + "relative_pressure_tolerance" : 0.001, + "absolute_pressure_tolerance" : 1e-5, + "volume_model_part_name" : "FluidParts_Volume", + "skin_parts" : ["Outlet2D_Outlet","NoSlip2D_No_Slip_Auto1"], + "no_skin_parts" : ["VelocityConstraints2D_Inlet-Total","VelocityConstraints2D_Inlet-Custom2"], + "time_scheme" : "bossak", + "time_stepping" : { + "automatic_time_step" : false, + "time_step" : 0.05 + }, + "formulation" : { + "element_type" : "qsvms", + "use_orthogonal_subscales" : false, + "dynamic_tau" : 1.0 + }, + "reform_dofs_at_each_step" : false + } + + }, + "processes" :{ + "initial_conditions_process_list" : [], + "boundary_conditions_process_list" : [{ + "python_module" : "apply_outlet_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyOutletProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.Outlet2D_Outlet", + "variable_name" : "PRESSURE", + "constrained" : true, + "value" : 0.0, + "hydrostatic_outlet" : false, + "h_top" : 0.0 + } + },{ + "python_module" : "apply_noslip_process", + "kratos_module" : "KratosMultiphysics.FluidDynamicsApplication", + "process_name" : "ApplyNoSlipProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.NoSlip2D_No_Slip_Auto1" + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name" : "VELOCITY", + "interval" : [0.0,1.0], + "constrained" : [true,true,true], + "value" : ["y*(3-y)*sin(pi*t*0.5)",0.0,0.0] + } + },{ + "python_module" : "assign_vector_variable_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorVariableProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.VelocityConstraints2D_Inlet-Custom2", + "variable_name" : "VELOCITY", + "interval" : [1.0,"End"], + "constrained" : [true,true,true], + "value" : ["y*(3-y)",0.0,0.0] + } + }], + "gravity" : [{ + "python_module" : "assign_vector_by_direction_process", + "kratos_module" : "KratosMultiphysics", + "process_name" : "AssignVectorByDirectionProcess", + "Parameters" : { + "model_part_name" : "FluidModelPart.FluidParts_Volume", + "variable_name" : "BODY_FORCE", + "modulus" : 0.0, + "constrained" : false, + "direction" : [0.0,-1.0,0.0] + } + }], + "auxiliar_process_list" : [] + } +} diff --git a/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/ProjectParameters_modified.json b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/ProjectParameters_modified.json new file mode 100644 index 00000000..766f6e24 --- /dev/null +++ b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/ProjectParameters_modified.json @@ -0,0 +1,187 @@ +{ + "analysis_stage": "KratosMultiphysics.FluidDynamicsApplication.fluid_dynamics_analysis", + "problem_data": { + "problem_name": "NonlinearInGiD", + "parallel_type": "OpenMP", + "echo_level": 0, + "start_time": 0.0, + "end_time": 52 + }, + "output_processes": { + "gid_output": [ + { + "python_module": "gid_output_process", + "kratos_module": "KratosMultiphysics", + "process_name": "GiDOutputProcess", + "help": "This process writes postprocessing files for GiD", + "Parameters": { + "model_part_name": "FluidModelPart.fluid_computational_model_part", + "output_name": "/home/jbravo/OtherRepos/Examples/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/Results/FOM", + "postprocess_parameters": { + "result_file_configuration": { + "gidpost_flags": { + "GiDPostMode": "GiD_PostBinary", + "WriteDeformedMeshFlag": "WriteDeformed", + "WriteConditionsFlag": "WriteConditions", + "MultiFileFlag": "SingleFile" + }, + "file_label": "time", + "output_control_type": "time", + "output_interval": 0.1, + "body_output": true, + "node_output": false, + "skin_output": false, + "plane_output": [], + "nodal_results": [ + "VELOCITY", + "PRESSURE", + "MESH_DISPLACEMENT" + ], + "gauss_point_results": [], + "nodal_nonhistorical_results": [] + }, + "point_data_configuration": [] + } + } + } + ], + "vtk_output": [] + }, + "solver_settings": { + "solver_type": "ale_fluid", + "ale_boundary_parts": [], + "mesh_motion_solver_settings": { + "solver_type": "structural_similarity" + }, + "fluid_solver_settings": { + "model_part_name": "FluidModelPart", + "domain_size": 2, + "solver_type": "Monolithic", + "model_import_settings": { + "input_type": "mdpa", + "input_filename": "/home/jbravo/OtherRepos/Examples/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/NonlinearInGiD" + }, + "material_import_settings": { + "materials_filename": "/home/jbravo/OtherRepos/Examples/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/ProblemFiles/FluidMaterials.json" + }, + "echo_level": 0, + "compute_reactions": false, + "maximum_iterations": 10, + "relative_velocity_tolerance": 0.001, + "absolute_velocity_tolerance": 1e-05, + "relative_pressure_tolerance": 0.001, + "absolute_pressure_tolerance": 1e-05, + "volume_model_part_name": "FluidParts_Volume", + "skin_parts": [ + "Outlet2D_Outlet", + "NoSlip2D_No_Slip_Auto1" + ], + "no_skin_parts": [ + "VelocityConstraints2D_Inlet-Total", + "VelocityConstraints2D_Inlet-Custom2" + ], + "time_scheme": "bossak", + "time_stepping": { + "automatic_time_step": false, + "time_step": 0.05 + }, + "formulation": { + "element_type": "qsvms", + "use_orthogonal_subscales": false, + "dynamic_tau": 1.0 + }, + "reform_dofs_at_each_step": false + } + }, + "processes": { + "initial_conditions_process_list": [], + "boundary_conditions_process_list": [ + { + "python_module": "apply_outlet_process", + "kratos_module": "KratosMultiphysics.FluidDynamicsApplication", + "process_name": "ApplyOutletProcess", + "Parameters": { + "model_part_name": "FluidModelPart.Outlet2D_Outlet", + "variable_name": "PRESSURE", + "constrained": true, + "value": 0.0, + "hydrostatic_outlet": false, + "h_top": 0.0 + } + }, + { + "python_module": "apply_noslip_process", + "kratos_module": "KratosMultiphysics.FluidDynamicsApplication", + "process_name": "ApplyNoSlipProcess", + "Parameters": { + "model_part_name": "FluidModelPart.NoSlip2D_No_Slip_Auto1" + } + }, + { + "python_module": "assign_vector_variable_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorVariableProcess", + "Parameters": { + "model_part_name": "FluidModelPart.VelocityConstraints2D_Inlet-Total", + "variable_name": "VELOCITY", + "interval": [ + 0.0, + 1.0 + ], + "constrained": [ + true, + true, + true + ], + "value": [ + "y*(3-y)*sin(pi*t*0.5)", + 0.0, + 0.0 + ] + } + }, + { + "python_module": "assign_vector_variable_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorVariableProcess", + "Parameters": { + "model_part_name": "FluidModelPart.VelocityConstraints2D_Inlet-Custom2", + "variable_name": "VELOCITY", + "interval": [ + 1.0, + "End" + ], + "constrained": [ + true, + true, + true + ], + "value": [ + "y*(3-y)", + 0.0, + 0.0 + ] + } + } + ], + "gravity": [ + { + "python_module": "assign_vector_by_direction_process", + "kratos_module": "KratosMultiphysics", + "process_name": "AssignVectorByDirectionProcess", + "Parameters": { + "model_part_name": "FluidModelPart.FluidParts_Volume", + "variable_name": "BODY_FORCE", + "modulus": 0.0, + "constrained": false, + "direction": [ + 0.0, + -1.0, + 0.0 + ] + } + } + ], + "auxiliar_process_list": [] + } +} \ No newline at end of file diff --git a/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/nonlinear_mapping.py b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/nonlinear_mapping.py new file mode 100644 index 00000000..21b4f09d --- /dev/null +++ b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/nonlinear_mapping.py @@ -0,0 +1,122 @@ +#importing PyGeM tools +from pygem import FFD, RBF + +import numpy as np + +def set_up_phi(): + #creating a free form deformation object for each control domain + ffd_up = FFD([2,5,2]) #3D box of control points + ffd_down = FFD([2,5,2]) #3D box of control points + + #setting the centre and size of the upper box of control points + ffd_down.box_origin = np.array([1.25, 0, 0.5]) + ffd_down.box_length = np.array([1, 1.25, 1]) + + #setting the centre and size of the lower box of control points + ffd_up.box_origin = np.array([1.25, 1.75, 0.5]) + ffd_up.box_length = np.array([1, 1.25, 1]) + + return ffd_up, ffd_down + + +def phi(up,down,ffd_down,ffd_up,deformation_multiplier,scale_of_deformation): + + ### moving down free-form-deformation ### + + ffd_down.array_mu_x[0, 0, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_x[0, 1, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[0, 2, 0] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_down.array_mu_x[0, 3, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[0, 4, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_x[0, 0, 1] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_x[0, 1, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[0, 2, 1] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_down.array_mu_x[0, 3, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[0, 4, 1] = deformation_multiplier*scale_of_deformation * 0.0 + + ffd_down.array_mu_y[0, 0, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_y[0, 1, 0] = deformation_multiplier*scale_of_deformation * 0.01 + ffd_down.array_mu_y[0, 2, 0] = deformation_multiplier*scale_of_deformation * 0.015 + ffd_down.array_mu_y[0, 3, 0] = deformation_multiplier*scale_of_deformation * 0.02 + ffd_down.array_mu_y[0, 4, 0] = deformation_multiplier*scale_of_deformation * 0.025 + ffd_down.array_mu_y[0, 0, 1] = deformation_multiplier*scale_of_deformation * 0.00 + ffd_down.array_mu_y[0, 1, 1] = deformation_multiplier*scale_of_deformation * 0.01 + ffd_down.array_mu_y[0, 2, 1] = deformation_multiplier*scale_of_deformation * 0.015 + ffd_down.array_mu_y[0, 3, 1] = deformation_multiplier*scale_of_deformation * 0.02 + ffd_down.array_mu_y[0, 4, 1] = deformation_multiplier*scale_of_deformation * 0.025 + + ffd_down.array_mu_x[1, 0, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_x[1, 1, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[1, 2, 0] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_down.array_mu_x[1, 3, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[1, 4, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_x[1, 0, 1] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_x[1, 1, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[1, 2, 1] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_down.array_mu_x[1, 3, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_down.array_mu_x[1, 4, 1] = deformation_multiplier*scale_of_deformation * 0.0 + + ffd_down.array_mu_y[1, 0, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_down.array_mu_y[1, 1, 0] = deformation_multiplier*scale_of_deformation * 0.01 + ffd_down.array_mu_y[1, 2, 0] = deformation_multiplier*scale_of_deformation * 0.015 + ffd_down.array_mu_y[1, 3, 0] = deformation_multiplier*scale_of_deformation * 0.02 + ffd_down.array_mu_y[1, 4, 0] = deformation_multiplier*scale_of_deformation * 0.025 + ffd_down.array_mu_y[1, 0, 1] = deformation_multiplier*scale_of_deformation * 0.00 + ffd_down.array_mu_y[1, 1, 1] = deformation_multiplier*scale_of_deformation * 0.01 + ffd_down.array_mu_y[1, 2, 1] = deformation_multiplier*scale_of_deformation * 0.015 + ffd_down.array_mu_y[1, 3, 1] = deformation_multiplier*scale_of_deformation * 0.02 + ffd_down.array_mu_y[1, 4, 1] = deformation_multiplier*scale_of_deformation * 0.025 + + + ### moving up free-form-deformation ### + + ffd_up.array_mu_x[0, 0, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_up.array_mu_x[0, 1, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[0, 2, 0] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_up.array_mu_x[0, 3, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[0, 4, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_up.array_mu_x[0, 0, 1] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_up.array_mu_x[0, 1, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[0, 2, 1] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_up.array_mu_x[0, 3, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[0, 4, 1] = deformation_multiplier*scale_of_deformation * 0.0 + + ffd_up.array_mu_y[0, 0, 0] = -deformation_multiplier*scale_of_deformation * 0.025 + ffd_up.array_mu_y[0, 1, 0] = -deformation_multiplier*scale_of_deformation * 0.020 + ffd_up.array_mu_y[0, 2, 0] = -deformation_multiplier*scale_of_deformation * 0.015 + ffd_up.array_mu_y[0, 3, 0] = -deformation_multiplier*scale_of_deformation * 0.01 + ffd_up.array_mu_y[0, 4, 0] = -deformation_multiplier*scale_of_deformation * 0.00 + ffd_up.array_mu_y[0, 0, 1] = -deformation_multiplier*scale_of_deformation * 0.025 + ffd_up.array_mu_y[0, 1, 1] = -deformation_multiplier*scale_of_deformation * 0.020 + ffd_up.array_mu_y[0, 2, 1] = -deformation_multiplier*scale_of_deformation * 0.015 + ffd_up.array_mu_y[0, 3, 1] = -deformation_multiplier*scale_of_deformation * 0.01 + ffd_up.array_mu_y[0, 4, 1] = -deformation_multiplier*scale_of_deformation * 0.00 + + ffd_up.array_mu_x[1, 0, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_up.array_mu_x[1, 1, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[1, 2, 0] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_up.array_mu_x[1, 3, 0] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[1, 4, 0] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_up.array_mu_x[1, 0, 1] = deformation_multiplier*scale_of_deformation * 0.0 + ffd_up.array_mu_x[1, 1, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[1, 2, 1] = deformation_multiplier*scale_of_deformation * 0.06 + ffd_up.array_mu_x[1, 3, 1] = deformation_multiplier*scale_of_deformation * 0.04 + ffd_up.array_mu_x[1, 4, 1] = deformation_multiplier*scale_of_deformation * 0.0 + + ffd_up.array_mu_y[1, 0, 0] = -deformation_multiplier*scale_of_deformation * 0.025 + ffd_up.array_mu_y[1, 1, 0] = -deformation_multiplier*scale_of_deformation * 0.020 + ffd_up.array_mu_y[1, 2, 0] = -deformation_multiplier*scale_of_deformation * 0.015 + ffd_up.array_mu_y[1, 3, 0] = -deformation_multiplier*scale_of_deformation * 0.01 + ffd_up.array_mu_y[1, 4, 0] = -deformation_multiplier*scale_of_deformation * 0.00 + ffd_up.array_mu_y[1, 0, 1] = -deformation_multiplier*scale_of_deformation * 0.025 + ffd_up.array_mu_y[1, 1, 1] = -deformation_multiplier*scale_of_deformation * 0.020 + ffd_up.array_mu_y[1, 2, 1] = -deformation_multiplier*scale_of_deformation * 0.015 + ffd_up.array_mu_y[1, 3, 1] = -deformation_multiplier*scale_of_deformation * 0.01 + ffd_up.array_mu_y[1, 4, 1] = -deformation_multiplier*scale_of_deformation * 0.00 + + + moved_up = ffd_up(up) + moved_down = ffd_down(down) + + return moved_up, moved_down, ffd_up , ffd_down + diff --git a/rom_application/ContractionExpansionChannel/FFD_plus_RBF/simulation_trajectories.py b/rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/simulation_trajectories.py similarity index 100% rename from rom_application/ContractionExpansionChannel/FFD_plus_RBF/simulation_trajectories.py rename to rom_application/ContractionExpansionChannel/FilesInKratosMaster/FFD_plus_RBF/simulation_trajectories.py diff --git a/rom_application/ContractionExpansionChannel/SelectedResults/Example_1/Affine/Velocity_y.npy b/rom_application/ContractionExpansionChannel/SelectedResults/Example_1/Affine/Velocity_y.npy new file mode 100644 index 0000000000000000000000000000000000000000..5affe577dffbd97f76f8ca9eab91423f36b34527 GIT binary 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np.max(v) + + if np.max(w)>max_y: + max_y = np.max(w) + + if np.min(v)-4: + min_x = np.min(v) + + if np.min(w)','d','8','H'] + + + + + for svd in tol_svd: + + vy_FOM = np.load(resuts_path+f'Velocity_y{add_to_name}.npy') + w_FOM = np.load(resuts_path+f'narrowing{add_to_name}.npy') + + min_x = 0 + max_x = 0 + min_y=0.7 + max_y=0.7 + + min_x, min_y, max_x, max_y = update_plot_ranges(min_x, min_y, max_x, max_y, vy_FOM,w_FOM) + + vy_rom, w_rom = load_rom_data(resuts_path, add_to_name, svd) + + min_x, min_y, max_x, max_y = update_plot_ranges(min_x, min_y, max_x, max_y, vy_rom,w_rom) + counter=0 + plt.plot(vy_FOM, w_FOM, 'k', label = 'FOM', linewidth = 5, alpha=0.4) #linewidth = 3, alpha=0.5 + plt.plot(vy_rom, w_rom, colours[counter], marker=markers[counter], markevery=50,label = r"$ROM \ \epsilon_{SOL}=$" + "{:.0e}".format(svd), alpha=0.9) #alpha=0.5, #alpha=0.5 + for res in to_svd_res: + vy_rom,w_rom = load_hrom_data(resuts_path, add_to_name, svd, res) + # vy_rom = np.load(resuts_path+f'y_velocity_HROM{add_to_name}_{svd}_{res}.npy') + # w_rom = np.load(resuts_path+f'narrowing_HROM{add_to_name}_{svd}_{res}.npy') + min_x, min_y, max_x, max_y = update_plot_ranges(min_x, min_y, max_x, max_y, vy_rom,w_rom) #do not consider the HROM for the ranges, as some of them explote + if np.max(np.abs(vy_rom))>10: + alpha = 0.4 + else: + alpha = 1 + plt.plot(vy_rom, w_rom, markevery=80+counter*15, + label = r"$HROM \ \epsilon_{SOL}=$ " + "{:.0e}".format(svd) + r" ; $\epsilon_{RES}=$ "+"{:.0e}".format(res), + linewidth = 1.5, marker=markers[counter], alpha=alpha) #alpha=0.5 marker=markers[counter] + counter+=1 + counter+=1 + plt.xlabel(r'$v_y^*$', size=15) + plt.ylabel(r'$w_c$',size=15) + plt.xlim([min_x-0.05,max_x+0.05]) + plt.ylim([min_y-0.05,max_y+0.05]) + plt.grid() + plt.legend(loc='upper left') + plt.savefig(f'hysteresis_rom_vs_hrom_{svd}_{trajectory}.pdf') + plt.show() + + + +if __name__=='__main__': + + resuts_path = './Affine/' #'./Nonlinear/' './Affine/' + trajectory = "train" # test or train + + tol_svd = [1e-3, 1e-4, 1e-5, 1e-6] + to_svd_res = [1e-3, 1e-4, 1e-5, 1e-6] + + + reviewed_plot_hysteresis_rom_hrom(tol_svd,to_svd_res,resuts_path, trajectory) + + diff --git a/rom_application/ContractionExpansionChannel/SelectedResults/Example_2/Affine/Velocity_y.npy b/rom_application/ContractionExpansionChannel/SelectedResults/Example_2/Affine/Velocity_y.npy new file mode 100644 index 0000000000000000000000000000000000000000..bc9d2926237f039de03010bb040723637dfe50d3 GIT binary patch literal 19656 zcmbSR`9Ia)^S5O!r4mYu6e1)=DVgYGc&hNpEEjZ!O6kq@Rq%FndQio)z~3>)aj7y z-W{?|G^Q)lo@z^DUb_6h?|SxR)@A&iXQg$1*B$cM1? zvYV|#8CzxxUNXvotDE!XZKrSWzQg2dsPQC>e6_d{);I&*(@JM2E2n{on%UoD`5AEekcC%z68NTc34wRHv&nw@QHI+xIAbFt9q1P-Dn%i8g)I1eF|dOP|= zBp+c}d()oQCqUT!WmoiV6e6zrl_n2779xt4=gw*`2oVmst4`h+5+W+z)9kY1goxea z-+E;B3K0$GcV2tbDoA7!rLXgR1&Lov(k)yng2cn1k^FO$0>l=1RMq@UfH3~_(p5A` zfXK{bHN$lQf+uj^geO{nc(W8ImW01QuH5Oh@K}Jjtre!et5JXmvXs-fI3hrNcyRON 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b/rom_application/ContractionExpansionChannel/SelectedResults/Example_2/plot_results.py @@ -0,0 +1,132 @@ +import numpy as np +from matplotlib import pyplot as plt +plt.rc('text', usetex=True) +plt.rc('font', family='serif') + + + + + +def update_plot_ranges(min_x, min_y, max_x, max_y, v,w): + + if np.max(v)>max_x and np.max(v)<4: + max_x = np.max(v) + + if np.max(w)>max_y: + max_y = np.max(w) + + if np.min(v)-4: + min_x = np.min(v) + + if np.min(w)','d','8','H'] + + + + + for svd in tol_svd: + + vy_FOM = np.load(resuts_path+f'Velocity_y{add_to_name}.npy') + w_FOM = np.load(resuts_path+f'narrowing{add_to_name}.npy') + + min_x = 0 + max_x = 0 + min_y=0.7 + max_y=0.7 + + min_x, min_y, max_x, max_y = update_plot_ranges(min_x, min_y, max_x, max_y, vy_FOM,w_FOM) + + vy_rom, w_rom = load_rom_data(resuts_path, add_to_name, svd) + + min_x, min_y, max_x, max_y = update_plot_ranges(min_x, min_y, max_x, max_y, vy_rom,w_rom) + counter=0 + plt.plot(vy_FOM, w_FOM, 'k', label = 'FOM', linewidth = 5, alpha=0.4) #linewidth = 3, alpha=0.5 + plt.plot(vy_rom, w_rom, colours[counter], marker=markers[counter], markevery=50,label = r"$ROM \ \epsilon_{SOL}=$" + "{:.0e}".format(svd), alpha=0.9) #alpha=0.5, #alpha=0.5 + for res in to_svd_res: + vy_rom,w_rom = load_hrom_data(resuts_path, add_to_name, svd, res) + # vy_rom = np.load(resuts_path+f'y_velocity_HROM{add_to_name}_{svd}_{res}.npy') + # w_rom = np.load(resuts_path+f'narrowing_HROM{add_to_name}_{svd}_{res}.npy') + min_x, min_y, max_x, max_y = update_plot_ranges(min_x, min_y, max_x, max_y, vy_rom,w_rom) #do not consider the HROM for the ranges, as some of them explote + if np.max(np.abs(vy_rom))>10: + alpha = 0.4 + else: + alpha = 1 + plt.plot(vy_rom, w_rom, markevery=80+counter*15, + label = r"$HROM \ \epsilon_{SOL}=$ " + "{:.0e}".format(svd) + r" ; $\epsilon_{RES}=$ "+"{:.0e}".format(res), + linewidth = 1.5, marker=markers[counter], alpha=alpha) #alpha=0.5 marker=markers[counter] + counter+=1 + counter+=1 + plt.xlabel(r'$v_y^*$', size=15) + plt.ylabel(r'$w_c$',size=15) + plt.xlim([min_x-0.05,max_x+0.05]) + plt.ylim([min_y-0.05,max_y+0.05]) + plt.grid() + plt.legend(loc='upper left') + plt.savefig(f'hysteresis_rom_vs_hrom_{svd}_{trajectory}.pdf') + plt.show() + + + +if __name__=='__main__': + + resuts_path = './Affine/' #'./Nonlinear/' './Affine/' + trajectory = "train" # test or train + + tol_svd = [1e-3, 1e-4, 1e-5, 1e-6] + to_svd_res = [1e-3, 1e-4, 1e-5, 1e-6] + + + reviewed_plot_hysteresis_rom_hrom(tol_svd,to_svd_res,resuts_path, trajectory) + + diff --git a/rom_application/ContractionExpansionChannel/SelectedResults/Example_3/Affine/Velocity_y.npy b/rom_application/ContractionExpansionChannel/SelectedResults/Example_3/Affine/Velocity_y.npy new file mode 100644 index 0000000000000000000000000000000000000000..4eafac306ccd080230414196f72cdde49a6bdddd GIT binary patch literal 19656 zcmbSR`9Iaq_qRo8QxQd3A`ucH={+|@l*&>eS<80!d%5;~jUrMCMG8@bY#~P_S;~?^ 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