r""" .. _ref_elasticity_center_cracked_displacement_controlled: Displacement Controlled Center Cracked Specimen ----------------------------------------------- Purely elastic Finite Element model under displacement loading. To improve computational efficiency, a quarter-symmetry model is employed. The crack is explicitly defined in the mesh by adjusting the boundary conditions. A series of simulations are run, each with a different pre-defined crack length. .. code-block:: # u/\/\/\/\/\/\ u/\/\/\/\/\/\ # |||||||||||| |||||||||||| # *----------* o|\ *----------* # | | o|/ | | # | 2a=a0 | o|\ | a=a0 | # | ---- | o|/ *----------* # | | /_\/_\ # | | oo oo oo # *----------* # /_\/_\/_\/_\ # |Y ///////////// # | # *---X The Young's modulus, Poisson's ratio, and the critical energy release rate are given in the table :ref:`Properties `. Young's modulus $E$ and Poisson's ratio $\nu$ can be represented with the Lamé parameters as: $\lambda=\frac{E\nu}{(1+\nu)(1-2\nu)}$; $\mu=\frac{E}{2(1+\nu)}$. Material Properties ------------------- The material properties are summarized in the table below: +----+---------+--------+ | | VALUE | UNITS | +====+=========+========+ | E | 210 | kN/mm2 | +----+---------+--------+ | nu | 0.3 | [-] | +----+---------+--------+ """ ############################################################################### # Import necessary libraries # -------------------------- import numpy as np import pyvista as pv import pandas as pd import matplotlib.pyplot as plt import matplotlib.image as mpimg import sys import os sys.path.insert(0, os.path.abspath('../../')) plt.style.use('../../graph.mplstyle') import plot_config as pcfg import dolfinx import mpi4py import petsc4py import os img = mpimg.imread('images/symmetry_central_cracked.png') # or .jpg, .tif, etc. plt.imshow(img) plt.axis('off') ############################################################################### # Import from phasefieldx package # ------------------------------- from phasefieldx.Element.Elasticity.Input import Input from phasefieldx.Element.Elasticity.solver.solver import solve from phasefieldx.Boundary.boundary_conditions import bc_x, bc_y, get_ds_bound_from_marker from phasefieldx.PostProcessing.ReferenceResult import AllResults results_folder = "results_center_cracked_displacement_control" if not os.path.exists(results_folder): os.makedirs(results_folder) def run_simulations(i, a0): Data = Input(E=210.0, nu=0.3, save_solution_xdmf=False, save_solution_vtu=True, results_folder_name=os.path.join(results_folder,str(i))) divx, divy = 200, 600 lx, ly = 1.0, 3.0 msh = dolfinx.mesh.create_rectangle(mpi4py.MPI.COMM_WORLD, [np.array([0, 0]), np.array([lx, ly])], [divx, divy], cell_type=dolfinx.mesh.CellType.quadrilateral) def bottom(x): return np.logical_and(np.isclose(x[1], 0), np.greater_equal(x[0], a0)) def top(x): return np.isclose(x[1], ly) def left(x): return np.isclose(x[0], 0) fdim = msh.topology.dim - 1 # Dimension of the mesh facets bottom_facet_marker = dolfinx.mesh.locate_entities_boundary(msh, fdim, bottom) top_facet_marker = dolfinx.mesh.locate_entities_boundary(msh, fdim, top) left_facet_marker = dolfinx.mesh.locate_entities_boundary(msh, fdim, left) ds_top = get_ds_bound_from_marker(top_facet_marker, msh, fdim) ds_bottom = get_ds_bound_from_marker(bottom_facet_marker, msh, fdim) ds_left = get_ds_bound_from_marker(left_facet_marker, msh, fdim) ds_list = np.array([ [ds_top, "top"], [ds_bottom, "bottom"], [ds_left, "left"], ]) V_u = dolfinx.fem.functionspace(msh, ("Lagrange", 1, (msh.geometry.dim, ))) bc_top = bc_y(top_facet_marker, V_u, fdim, value=0.0) bc_bottom = bc_y(bottom_facet_marker, V_u, fdim, value=0.0) bc_left = bc_x(left_facet_marker, V_u, fdim, value=0.0) bcs_list_u = [bc_top, bc_bottom, bc_left] bcs_list_u_names = ["top", "bottom", "left"] def update_boundary_conditions(bcs, time): val = 1 bcs[0].g.value[...] = petsc4py.PETSc.ScalarType(val) return 0, val, 0 T_list_u = None update_loading = None f = None final_time = 1.0 dt = 1.0 solve(Data, msh, final_time, V_u, bcs_list_u, update_boundary_conditions, f, T_list_u, update_loading, ds_list, dt, path=None, quadrature_degree=2, bcs_list_u_names=bcs_list_u_names) da=0.01 a = np.arange(0.0, 0.95+da, da) run_simulation_bool = False if run_simulation_bool: for i in range(0,len(a)): run_simulations(i, a[i]) ############################################################################### # Load results # ------------ compliance = np.zeros(len(a)) E = np.zeros(len(a)) for i in range(0,len(a)): print(f"Loading results for simulation {i} with crack length {a[i]} mm") simulation_folder = os.path.join(results_folder,str(i)) S = AllResults(simulation_folder) compliance[i] = 2*S.energy_files["total.energy"]["E"][0]/S.reaction_files["bottom.reaction"]["Ry"]**2 # %% # For this symmetric model, the compliance calculated here for the full specimen # is equivalent to that of a quarter-symmetry model, due to boundary conditions and loading. # Note: The variable 'a_saved' stores the half-crack length 'a' (not the total crack length 2a), # which is consistent with the convention used in the documentation and manuals. a_saved = a stiffness_complete_model = abs(1/compliance) # %% # Save processed results to file header = ["crack_length", "stiffness"] data_save = np.column_stack((a_saved, stiffness_complete_model)) save_path = os.path.join(results_folder, "results.elasticity") np.savetxt(save_path, data_save, fmt="%.6e", delimiter="\t", header="\t".join(header), comments="") else: # Load processed results from file save_path = os.path.join(results_folder, "results.elasticity") data_loaded = pd.read_csv(save_path, delim_whitespace=True, comment="#") a_saved = data_loaded["crack_length"].to_numpy() stiffness_complete_model = data_loaded["stiffness"].to_numpy() ############################################################################### # Crack length vs stiffness # ------------------------- fig, ax0 = plt.subplots() ax0.plot(a_saved, stiffness_complete_model, 'k-') ax0.set_xlabel(pcfg.crack_length_label) ax0.set_ylabel(pcfg.stiffness_label) ax0.legend() plt.show() ############################################################################## # Visualization of Results # ------------------------- # The following section visualizes the mesh and displacement field for two # different simulations (indices 20 and 50). The mesh is shown first, followed # by the displacement field, which is warped by the displacement vector for # better visualization. pv.start_xvfb() file_vtu_1 = pv.read(os.path.join(results_folder, "20", "paraview-solutions_vtu", "phasefieldx_p0_000000.vtu")) file_vtu_2 = pv.read(os.path.join(results_folder, "80", "paraview-solutions_vtu", "phasefieldx_p0_000000.vtu")) ############################################################################## # Plot: Mesh # ---------- # Display the mesh for the first simulation (index 20). file_vtu_1.plot(cpos='xy', color='white', show_edges=True) ############################################################################## # Plot: Displacement (Simulation 20) # ----------------------------------- # Warp the mesh by the displacement vector for the first simulation and plot # the displacement field. warped_1 = file_vtu_1.warp_by_vector('u', factor=1.0) warped_1.plot(scalars='u', cpos='xy', show_scalar_bar=True, show_edges=False) ############################################################################## # Plot: Displacement (Simulation 50) # ----------------------------------- # Warp the mesh by the displacement vector for the second simulation and plot # the displacement field. warped_2 = file_vtu_2.warp_by_vector('u', factor=1.0) warped_2.plot(scalars='u', cpos='xy', show_scalar_bar=True, show_edges=False)