2D case - Figures 9-10: FEM comparison#
Two-parameter 2D problem - Comparison with the FEM reference and plot of the solution for different parametric configurations
Libraries import#
import sys
import torch
import torch.nn as nn
from neurom.HiDeNN_PDE import MeshNN, NeuROM, MeshNN_2D, MeshNN_1D
import neurom.src.Pre_processing as pre
from neurom.src.PDE_Library import Strain, Stress,VonMises_plain_strain
from neurom.src.Training import Training_NeuROM_multi_level
import neurom.Post.Plots as Pplot
import time
import os
import torch._dynamo as dynamo
from importlib import reload
import tomllib
import numpy as np
import argparse
torch.manual_seed(0)
Load the config file#
Configuration_file = 'Configurations/config_2D_ROM.toml'
with open(Configuration_file, mode="rb") as file:
config = tomllib.load(file)
Definition of the space domain and mechanical proprieties of the structure#
The initial Material parameters, the geometry, mesh and the boundary conditions are set.
# Material parameters definition
Mat = pre.Material( flag_lame = False, # If True should input lmbda and mu instead of E and nu
coef1 = config["material"]["E"], # Young Modulus
coef2 = config["material"]["nu"] # Poisson's ratio
)
MaxElemSize2D = config["interpolation"]["MaxElemSize2D"] = 0.125
# Create mesh object
MaxElemSize = pre.ElementSize(
dimension = config["interpolation"]["dimension"],
L = config["geometry"]["L"],
order = config["interpolation"]["order"],
np = config["interpolation"]["np"],
MaxElemSize2D = config["interpolation"]["MaxElemSize2D"]
)
Excluded = []
Mesh_object = pre.Mesh(
config["geometry"]["Name"], # Create the mesh object
MaxElemSize,
config["interpolation"]["order"],
config["interpolation"]["dimension"]
)
Mesh_object.AddBorders(config["Borders"]["Borders"])
Mesh_object.AddBCs( # Include Boundary physical domains infos (BCs+volume)
config["geometry"]["Volume_element"],
Excluded,
config["DirichletDictionryList"]
)
Mesh_object.MeshGeo() # Mesh the .geo file if .msh does not exist
Mesh_object.ReadMesh()
Mesh_object.ExportMeshVtk()
Parametric study definition#
The hypercube describing the parametric domain used for the tensor decomposition is set-up here
ParameterHypercube = torch.tensor([ [ config["parameters"]["para_1_min"],
config["parameters"]["para_1_max"],
config["parameters"]["N_para_1"]],
[ config["parameters"]["para_2_min"],
config["parameters"]["para_2_max"],
config["parameters"]["N_para_2"]]])
Initialisation of the surrogate model#
ROM_model = NeuROM( # Build the surrogate (reduced-order) model
Mesh_object,
ParameterHypercube,
config,
config["solver"]["n_modes_ini"],
config["solver"]["n_modes_max"]
)
Training the model#
# ROM_model.Freeze_Mesh() # Set space mesh coordinates as untrainable
# ROM_model.Freeze_MeshPara() # Set parameters mesh coordinates as untrainable
# ROM_model.TrainingParameters(
# loss_decrease_c = config["training"]["loss_decrease_c"],
# Max_epochs = config["training"]["n_epochs"],
# learning_rate = config["training"]["learning_rate"]
# )
# ROM_model.train() # Put the model in training mode
# ROM_model, Mesh_object = Training_NeuROM_multi_level(ROM_model,config, Mat)
ROM_model.load_state_dict(torch.load('Pretrained_models/2D_ROM', weights_only=False))
Pyvista plots#
Plot the solution and the error with regard to the Finite Element solution
eval_coord_file = "GroundTruth/nodal_coordinates.npy"
E_vect = [0.0038,0.00314,0.00462]
theta_vect = [4.21,0,0.82]
error_vect = []
for i in range(len(E_vect)):
num_displ_file = "GroundTruth/nodal_num_displacement_E="+str(E_vect[i])+"_theta="+str(theta_vect[i])+".npy"
eval_coord = torch.tensor(np.load(eval_coord_file), dtype=torch.float64, requires_grad=True)
num_displ = torch.tensor(np.load(num_displ_file))
theta = torch.tensor([theta_vect[i]],dtype=torch.float64)
theta = theta[:,None]
E = torch.tensor([E_vect[i]],dtype=torch.float64)
E = E[:,None]
Para_coord_list = nn.ParameterList((E,theta))
ROM_model.eval() # Put model in evaluation mode
u_sol = ROM_model(eval_coord,Para_coord_list) # Evaluate model
u_sol_x = u_sol[0,:,0,0]
u_sol_y = u_sol[1,:,0,0]
u_ref_x = num_displ[:,0]
u_ref_y = num_displ[:,1]
u_ref_tot = torch.hstack((u_ref_x,u_ref_y))
u_sol_tot = torch.hstack((u_sol_x,u_sol_y))
error_u_tot = (torch.linalg.vector_norm(u_sol_tot - u_ref_tot)/torch.linalg.vector_norm(u_ref_tot)).item()
error_vect.append(error_u_tot)
import pyvista as pv
import numpy as np
import matplotlib.pyplot as plt
from matplotlib.backends.backend_pdf import PdfPages
from matplotlib import cm
from matplotlib.colorbar import ColorbarBase
from matplotlib.colors import Normalize
import torch.nn as nn
pv.global_theme.font.family = 'times' # Arial, courier or times
pv.global_theme.font.size = 40
pv.global_theme.font.title_size = 40
pv.global_theme.font.label_size = 40
pv.global_theme.font.fmt = '%.2e'
filename = 'Geometries/'+Mesh_object.name_mesh # Load mesh (used for projecting the solution only)
mesh = pv.read(filename) # Create pyvista mesh
Nodes = np.stack(Mesh_object.Nodes)
import matplotlib
matplotlib.rcParams["font.size"] = "25"
First parameters set#
#Fig a)
name = 'a'
theta_i = theta_vect[0]
E_i = E_vect[0]
print(f'E = {E_i}, theta = {theta_i}, theta_deg = {theta_i*180/np.pi}')
num_displ_file = "GroundTruth/nodal_num_displacement_E="+str(E_i)+"_theta="+str(theta_i)+".npy"
num_displ = torch.tensor(np.load(num_displ_file))
theta = torch.tensor([theta_i],dtype=torch.float64)
theta = theta[:,None]
E = torch.tensor([E_i],dtype=torch.float64)
E = E[:,None]
Para_coord_list = nn.ParameterList((E,theta))
ROM_model.eval() # Put model in evaluation mode
u_sol = ROM_model(eval_coord,Para_coord_list) # Evaluate model
u = torch.stack([(u_sol[0,:,0,0]),(u_sol[1,:,0,0]),torch.zeros(u_sol[0,:,0,0].shape[0])],dim=1)
u_ref = torch.stack([(num_displ[:,0]),(num_displ[:,1]),torch.zeros(u_sol[0,:,0,0].shape[0])],dim=1)
error_ref = torch.abs(u-u_ref)
mesh.point_data['U'] = u.data
mesh.point_data['U_norm'] = torch.norm(u, dim=1).data
mesh.point_data['Ux'] = u[:,0].data
mesh.point_data['Uy'] = u[:,1].data
mesh.point_data['Uz'] = u[:,2].data
mesh.point_data['error'] = error_ref.data
mesh.point_data['error_norm'] = torch.norm(error_ref, dim=1).data
## Result a)
plotter = pv.Plotter(off_screen=True)
plotter.add_mesh(mesh.warp_by_vector(vectors="U",factor=20,inplace=False), scalars='U_norm', cmap='viridis', show_scalar_bar=False)
plotter.view_xy()
import matplotlib
image = plotter.screenshot(transparent_background=True,return_img=True, window_size=[3200, 1800]) # Return image as array for Matplotlib
with PdfPages('Results/Fig_pyvista_'+name+'.pdf') as pdf:
fig, ax = plt.subplots(figsize=(8, 9), dpi = 300)
plt.imshow(image)
plt.xlim(900, 2500)
plt.ylim(1500,250)
# ax.imshow(image)
plt.axis('off')
# fig.subplots_adjust(right=1)
cbar_ax = fig.add_axes([0.81, 0.25, 0.03, 0.5])
# Normalize scalar field values for the color bar
norm = Normalize(vmin=mesh.point_data['U_norm'].min(), vmax=mesh.point_data['U_norm'].max())
# cmap = cm.get_cmap('viridis')
cmap = matplotlib.colormaps['viridis']
# Add a color bar based on the normalization and the colormap
cbar = ColorbarBase(cbar_ax, cmap=cmap, norm=norm)
cbar.set_label('Displacement (mm)', fontsize=25)
cbar.formatter.set_powerlimits((-2, 2)) # Use scientific notation for ticks outside this range
cbar.update_ticks() # Update the ticks after setting the formatter
# Save the figure as a vectorized PDF
pdf.savefig(fig,bbox_inches = 'tight',pad_inches = 0)
plt.show(fig)
plt.close(fig)
## Error a)
plotter = pv.Plotter(off_screen=True)
# plotter.add_mesh(mesh.warp_by_vector(vectors="error",factor=20,inplace=False), scalars='error_norm', cmap='viridis', clim=[0, 0.05],show_scalar_bar=False)
plotter.add_mesh(mesh.warp_by_vector(vectors="error",factor=20,inplace=False), scalars='error_norm', cmap='viridis',show_scalar_bar=False)
plotter.view_xy()
import matplotlib
image = plotter.screenshot(transparent_background=True,return_img=True, window_size=[3200, 1800]) # Return image as array for Matplotlib
with PdfPages('Results/Fig_pyvista_error_'+name+'.pdf') as pdf:
fig, ax = plt.subplots(figsize=(8, 9), dpi = 300)
plt.imshow(image)
plt.xlim(900, 2500)
plt.ylim(1500,250)
# ax.imshow(image)
plt.axis('off')
# fig.subplots_adjust(right=1)
cbar_ax = fig.add_axes([0.85, 0.25, 0.03, 0.5])
# Normalize scalar field values for the color bar
norm = Normalize(vmin=mesh.point_data['error_norm'].min(), vmax=mesh.point_data['error_norm'].max())
# cmap = cm.get_cmap('viridis')
cmap = matplotlib.colormaps['viridis']
# Add a color bar based on the normalization and the colormap
cbar = ColorbarBase(cbar_ax, cmap=cmap, norm=norm)
cbar.set_label('Error (mm)', fontsize=25)
cbar.formatter.set_powerlimits((-2, 2)) # Use scientific notation for ticks outside this range
cbar.update_ticks() # Update the ticks after setting the formatter
# Save the figure as a vectorized PDF
pdf.savefig(fig,bbox_inches = 'tight')
plt.show(fig)
plt.close(fig)
E = 0.0038, theta = 4.21, theta_deg = 241.21523175007655
Second parameters set#
#Fig b)
name = 'b'
theta_i = theta_vect[1]
E_i = E_vect[1]
print(f'E = {E_i}, theta = {theta_i}, theta_deg = {theta_i*180/np.pi}')
num_displ_file = "GroundTruth/nodal_num_displacement_E="+str(E_i)+"_theta="+str(theta_i)+".npy"
num_displ = torch.tensor(np.load(num_displ_file))
theta = torch.tensor([theta_i],dtype=torch.float64)
theta = theta[:,None]
E = torch.tensor([E_i],dtype=torch.float64)
E = E[:,None]
Para_coord_list = nn.ParameterList((E,theta))
ROM_model.eval() # Put model in evaluation mode
u_sol = ROM_model(eval_coord,Para_coord_list) # Evaluate model
u = torch.stack([(u_sol[0,:,0,0]),(u_sol[1,:,0,0]),torch.zeros(u_sol[0,:,0,0].shape[0])],dim=1)
u_ref = torch.stack([(num_displ[:,0]),(num_displ[:,1]),torch.zeros(u_sol[0,:,0,0].shape[0])],dim=1)
error_ref = torch.abs(u-u_ref)
mesh.point_data['U'] = u.data
mesh.point_data['U_norm'] = torch.norm(u, dim=1).data
mesh.point_data['Ux'] = u[:,0].data
mesh.point_data['Uy'] = u[:,1].data
mesh.point_data['Uz'] = u[:,2].data
mesh.point_data['error'] = error_ref.data
mesh.point_data['error_norm'] = torch.norm(error_ref, dim=1).data
## Result b)
plotter = pv.Plotter(off_screen=True)
plotter.add_mesh(mesh.warp_by_vector(vectors="U",factor=20,inplace=False), scalars='U_norm', cmap='viridis', show_scalar_bar=False)
plotter.view_xy()
import matplotlib
image = plotter.screenshot(transparent_background=True,return_img=True, window_size=[3200, 1800]) # Return image as array for Matplotlib
with PdfPages('Results/Fig_pyvista_'+name+'.pdf') as pdf:
fig, ax = plt.subplots(figsize=(8, 9), dpi = 300)
plt.imshow(image)
plt.xlim(900, 2500)
plt.ylim(1500,250)
# ax.imshow(image)
plt.axis('off')
# fig.subplots_adjust(right=1)
cbar_ax = fig.add_axes([0.81, 0.25, 0.03, 0.5])
# Normalize scalar field values for the color bar
norm = Normalize(vmin=mesh.point_data['U_norm'].min(), vmax=mesh.point_data['U_norm'].max())
# cmap = cm.get_cmap('viridis')
cmap = matplotlib.colormaps['viridis']
# Add a color bar based on the normalization and the colormap
cbar = ColorbarBase(cbar_ax, cmap=cmap, norm=norm)
cbar.set_label('Displacement (mm)', fontsize=25)
cbar.formatter.set_powerlimits((-2, 2)) # Use scientific notation for ticks outside this range
cbar.update_ticks() # Update the ticks after setting the formatter
# Save the figure as a vectorized PDF
pdf.savefig(fig,bbox_inches = 'tight',pad_inches = 0)
plt.show(fig)
plt.close(fig)
## Error a)
plotter = pv.Plotter(off_screen=True)
# plotter.add_mesh(mesh.warp_by_vector(vectors="error",factor=20,inplace=False), scalars='error_norm', cmap='viridis', clim=[0, 0.05],show_scalar_bar=False)
plotter.add_mesh(mesh.warp_by_vector(vectors="error",factor=20,inplace=False), scalars='error_norm', cmap='viridis',show_scalar_bar=False)
plotter.view_xy()
import matplotlib
image = plotter.screenshot(transparent_background=True,return_img=True, window_size=[3200, 1800]) # Return image as array for Matplotlib
with PdfPages('Results/Fig_pyvista_error_'+name+'.pdf') as pdf:
fig, ax = plt.subplots(figsize=(8, 9), dpi = 300)
plt.imshow(image)
plt.xlim(900, 2500)
plt.ylim(1500,250)
# ax.imshow(image)
plt.axis('off')
# fig.subplots_adjust(right=1)
cbar_ax = fig.add_axes([0.85, 0.25, 0.03, 0.5])
# Normalize scalar field values for the color bar
norm = Normalize(vmin=mesh.point_data['error_norm'].min(), vmax=mesh.point_data['error_norm'].max())
# cmap = cm.get_cmap('viridis')
cmap = matplotlib.colormaps['viridis']
# Add a color bar based on the normalization and the colormap
cbar = ColorbarBase(cbar_ax, cmap=cmap, norm=norm)
cbar.set_label('Error (mm)', fontsize=25)
cbar.formatter.set_powerlimits((-2, 2)) # Use scientific notation for ticks outside this range
cbar.update_ticks() # Update the ticks after setting the formatter
# Save the figure as a vectorized PDF
pdf.savefig(fig,bbox_inches = 'tight')
plt.show(fig)
plt.close(fig)
E = 0.00314, theta = 0, theta_deg = 0.0
Third parameters set#
#Fig c)
name = 'c'
theta_i = theta_vect[2]
E_i = E_vect[2]
print(f'E = {E_i}, theta = {theta_i}, theta_deg = {theta_i*180/np.pi}')
num_displ_file = "GroundTruth/nodal_num_displacement_E="+str(E_i)+"_theta="+str(theta_i)+".npy"
num_displ = torch.tensor(np.load(num_displ_file))
theta = torch.tensor([theta_i],dtype=torch.float64)
theta = theta[:,None]
E = torch.tensor([E_i],dtype=torch.float64)
E = E[:,None]
Para_coord_list = nn.ParameterList((E,theta))
ROM_model.eval() # Put model in evaluation mode
u_sol = ROM_model(eval_coord,Para_coord_list) # Evaluate model
u = torch.stack([(u_sol[0,:,0,0]),(u_sol[1,:,0,0]),torch.zeros(u_sol[0,:,0,0].shape[0])],dim=1)
u_ref = torch.stack([(num_displ[:,0]),(num_displ[:,1]),torch.zeros(u_sol[0,:,0,0].shape[0])],dim=1)
error_ref = torch.abs(u-u_ref)
mesh.point_data['U'] = u.data
mesh.point_data['U_norm'] = torch.norm(u, dim=1).data
mesh.point_data['Ux'] = u[:,0].data
mesh.point_data['Uy'] = u[:,1].data
mesh.point_data['Uz'] = u[:,2].data
mesh.point_data['error'] = error_ref.data
mesh.point_data['error_norm'] = torch.norm(error_ref, dim=1).data
## Result c)
plotter = pv.Plotter(off_screen=True)
plotter.add_mesh(mesh.warp_by_vector(vectors="U",factor=20,inplace=False), scalars='U_norm', cmap='viridis', show_scalar_bar=False)
plotter.view_xy()
import matplotlib
image = plotter.screenshot(transparent_background=True,return_img=True, window_size=[3200, 1800]) # Return image as array for Matplotlib
with PdfPages('Results/Fig_pyvista_'+name+'.pdf') as pdf:
fig, ax = plt.subplots(figsize=(8, 9), dpi = 300)
plt.imshow(image)
plt.xlim(900, 2500)
plt.ylim(1500,250)
# ax.imshow(image)
plt.axis('off')
# fig.subplots_adjust(right=1)
cbar_ax = fig.add_axes([0.81, 0.25, 0.03, 0.5])
# Normalize scalar field values for the color bar
norm = Normalize(vmin=mesh.point_data['U_norm'].min(), vmax=mesh.point_data['U_norm'].max())
# cmap = cm.get_cmap('viridis')
cmap = matplotlib.colormaps['viridis']
# Add a color bar based on the normalization and the colormap
cbar = ColorbarBase(cbar_ax, cmap=cmap, norm=norm)
cbar.set_label('Displacement (mm)', fontsize=25)
cbar.formatter.set_powerlimits((-2, 2)) # Use scientific notation for ticks outside this range
cbar.update_ticks() # Update the ticks after setting the formatter
# Save the figure as a vectorized PDF
pdf.savefig(fig,bbox_inches = 'tight',pad_inches = 0)
plt.show(fig)
plt.close(fig)
## Error a)
plotter = pv.Plotter(off_screen=True)
# plotter.add_mesh(mesh.warp_by_vector(vectors="error",factor=20,inplace=False), scalars='error_norm', cmap='viridis', clim=[0, 0.05],show_scalar_bar=False)
plotter.add_mesh(mesh.warp_by_vector(vectors="error",factor=20,inplace=False), scalars='error_norm', cmap='viridis',show_scalar_bar=False)
plotter.view_xy()
import matplotlib
image = plotter.screenshot(transparent_background=True,return_img=True, window_size=[3200, 1800]) # Return image as array for Matplotlib
with PdfPages('Results/Fig_pyvista_error_'+name+'.pdf') as pdf:
fig, ax = plt.subplots(figsize=(8, 9), dpi = 300)
plt.imshow(image)
plt.xlim(900, 2500)
plt.ylim(1500,250)
# ax.imshow(image)
plt.axis('off')
# fig.subplots_adjust(right=1)
cbar_ax = fig.add_axes([0.85, 0.25, 0.03, 0.5])
# Normalize scalar field values for the color bar
norm = Normalize(vmin=mesh.point_data['error_norm'].min(), vmax=mesh.point_data['error_norm'].max())
# cmap = cm.get_cmap('viridis')
cmap = matplotlib.colormaps['viridis']
# Add a color bar based on the normalization and the colormap
cbar = ColorbarBase(cbar_ax, cmap=cmap, norm=norm)
cbar.set_label('Error (mm)', fontsize=25)
cbar.formatter.set_powerlimits((-2, 2)) # Use scientific notation for ticks outside this range
cbar.update_ticks() # Update the ticks after setting the formatter
# Save the figure as a vectorized PDF
pdf.savefig(fig,bbox_inches = 'tight')
plt.show(fig)
plt.close(fig)
E = 0.00462, theta = 0.82, theta_deg = 46.9825392007275
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