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R11910/mechanical_model/netcdf2h5_hea.py
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netcdf2h5_hea.py
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#!/usr/bin/env python3
# -*- coding: utf-8 -*-
"""
Created on Tue Aug 2 13:47:04 2022
@author: ekinkubilay
"""
#from netCDF4 import Dataset
"""
nc_file_name = 'spectral_3D_output.nc'
data = Dataset(nc_file_name, 'r')
print(data)
grad = data.variables['grad'][:,:,:,:,:,:]
nx = data.dimensions['nx']
print(type(grad))
hf = h5py.File('data.h5', 'w')
hf.create_dataset('dataset_1', data=grad)
hf.close()
"""
import os
import sys
import h5py
sys.path.insert(0, os.path.join(os.getcwd(), "/home/kubilay/software/muspectre/build/language_bindings/python"))
sys.path.insert(0, os.path.join(os.getcwd(), "/home/kubilay/software/muspectre/build/language_bindings/libmufft/python"))
sys.path.insert(0, os.path.join(os.getcwd(), "/home/kubilay/software/muspectre/build/language_bindings/libmugrid/python"))
sys.path.insert(0, os.path.join(os.getcwd(), "/home/kubilay/software/muspectre/build/language_bindings/python/muSpectre"))
print("current working directory: '{}'".format(os.getcwd()))
import muFFT
import muSpectre as msp
import numpy as np
import matplotlib.pyplot as plt
import muGrid
from muFFT import Stencils2D
from muFFT import Stencils3D
import cProfile, pstats
import time as timer
import fenics
from petsc4py import PETSc
import argparse
from muSpectre.gradient_integration import get_complemented_positions_class_solver
def parse_args():
"""
Function to handle arguments
"""
parser = argparse.ArgumentParser(description='Run given layer')
parser.add_argument("layer_no", type=int, help='layer_number')
parser.add_argument("factor", type=float, help='factor for material parametric analysis')
parser.add_argument("target_directory", help='target directory for output/input files')
args = parser.parse_args()
return args
def read_data_of_step(file_io_object_read, cell, solver, read_netcdf, material, read_frame=-1):
nb_quad = cell.nb_quad_pts
nb_domain_grid_pts = cell.nb_domain_grid_pts
dim = cell.dims
alpha_thermal = material.alpha_thermal
T_m = material.T_m
epsilon_sat = 0.35
sigma_for = 1.200 #GPa
if read_netcdf:
file_io_object_read.read(
frame=read_frame,
field_names=["flux", "grad", "epsilon_bar", "epsilon_plastic", "temperature", "vacuum_strain", "melt_pool", "material2"])
material_arr = cell.get_fields().get_field('material2').array().reshape((1, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((1, 1, -1), order='F').T.swapaxes(1, 2)
flux_arr = cell.get_fields().get_field('flux').array().reshape((dim, dim, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, dim, -1), order='F').T.swapaxes(1, 2)
flux_arr_2 = np.array(flux_arr, copy=True)
grad_arr = cell.get_fields().get_field('grad').array().reshape((dim, dim, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, dim, -1), order='F').T.swapaxes(1, 2)
epsilon_plastic = cell.get_globalised_current_real_field("epsilon_plastic").array().reshape((dim, dim, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, dim, -1), order='F').T.swapaxes(1, 2)
epsilon_bar = cell.get_globalised_current_real_field("epsilon_bar").array().reshape((1, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((1, 1, -1), order='F').T.swapaxes(1, 2)
vacuum_strain = cell.get_globalised_internal_real_field("vacuum_strain").array().reshape((dim, dim, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, dim, -1), order='F').T.swapaxes(1, 2)
temperature_material = cell.get_globalised_internal_real_field("temperature").array().reshape((1, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((1, 1, -1), order='F').T.swapaxes(1, 2)
melt_pool = cell.get_globalised_internal_int_field("melt_pool").array().reshape((1, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((1, 1, -1), order='F').T.swapaxes(1, 2)
thermal_strain = np.zeros_like(grad_arr)
thermal_strain_value = (temperature_material[:,0,0] - T_m)*alpha_thermal
for i in range(3):
thermal_strain[:,i,i] = np.array([thermal_strain_value])
elastic_strain = grad_arr - epsilon_plastic - vacuum_strain - thermal_strain
total_actual_strain = grad_arr - vacuum_strain
sigma_forest = np.zeros_like(temperature_material)
sigma_forest = sigma_for*(1-np.exp(-epsilon_bar[:,0,0]/epsilon_sat))*(1- temperature_material[:,0,0]/T_m)**0.5
stress_deviatoric = np.zeros_like(flux_arr)
trace_array = (flux_arr[:,0,0] + flux_arr[:,1,1] + flux_arr[:,2,2])/3
stress_deviatoric += flux_arr
for i in range(3):
stress_deviatoric[:,i,i] -= trace_array
sigma_vonmises = np.sqrt((3/2)*np.sum(stress_deviatoric*stress_deviatoric, axis=(1,2)))
#flux_integral = np.repeat(np.expand_dims(solver.projection.integrate(solver.flux.field).array(), 2), 6, axis=2).reshape((dim, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, 1, -1), order='F').T.swapaxes(1, 2)
#flux_integral_nonaffine = np.repeat(np.expand_dims(solver.projection.integrate_nonaffine_displacements(solver.flux.field).array(), 2), 6, axis=2).reshape((dim, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, 1, -1), order='F').T.swapaxes(1, 2)
grad_integral = np.repeat(np.expand_dims(solver.projection.integrate(solver.grad.field).array(), 2), 6, axis=2).reshape((dim, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, 1, -1), order='F').T.swapaxes(1, 2)
grad_integral_nonaffine = np.repeat(np.expand_dims(solver.projection.integrate_nonaffine_displacements(solver.grad.field).array(), 2), 6, axis=2).reshape((dim, 1, nb_quad) + tuple(nb_domain_grid_pts),order='f').reshape((dim, 1, -1), order='F').T.swapaxes(1, 2)
solver.projection.apply_projection(solver.flux.field)
c_data = {
"material": np.array([material_arr]),
"stress": np.array([flux_arr_2]),
"strain": np.array([grad_arr]),
"epsilon_plastic": np.array([epsilon_plastic]),
"epsilon_bar": np.array([epsilon_bar]),
"vacuum_strain": np.array([vacuum_strain]),
"temperature_material": np.array([temperature_material]),
"melt_pool": np.array([melt_pool]),
"epsilon_elastic": np.array([elastic_strain]),
"sigma_forest": np.array([sigma_forest]),
"sigma_vonmises": np.array([sigma_vonmises]),
"stress_deviatoric": np.array([stress_deviatoric]),
"total_actual_strain": np.array([total_actual_strain]),
"projection": np.array([flux_arr]),
#"flux_integral": np.array([flux_integral]),
"grad_integral": np.array([grad_integral]),
#"flux_integral_nonaffine": np.array([flux_integral_nonaffine]),
"grad_integral_nonaffine": np.array([grad_integral_nonaffine])
}
strain_field = cell.get_fields().get_field("grad")
material_field = cell.get_fields().get_field("material2")
strain_field_alias = np.array(strain_field, copy=False)
strain_field_alias[material_field == 0] = 0
#strain_field_alias[:,:,:,-1,:,:] = 0
#strain_field_alias[:,:,:,:,-1,:] = 0
#strain_field_alias[:,:,:,:,:,-1] = 0
#strain_field_alias[:,:,:,:,:,0] = 0
#strain_field_alias[:,:,:,:,:,:] = np.roll(strain_field_alias, (nb_domain_grid_pts[0]//2, nb_domain_grid_pts[1]//2, nb_domain_grid_pts[2]//2), (3,4,5))
[x_0, y_0, z_0], [x_displ, y_displ, z_displ] = get_complemented_positions_class_solver("0n", cell, solver, np.eye(3), periodically_complemented=True)
#x_displ = np.roll(x_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
#y_displ = np.roll(y_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
#z_displ = np.roll(z_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
total_displacement = np.transpose([x_displ.ravel(order='F'), y_displ.ravel(order='F'), z_displ.ravel(order='F')])
#file_io_object_read.read(frame=read_frame,field_names=["grad"])
strain_field = cell.get_fields().get_field("grad")
strain_field_alias = np.array(strain_field, copy=False)
vacuum_strain_field = cell.get_globalised_internal_real_field("vacuum_strain").array().reshape((dim, dim, nb_quad) + tuple(nb_domain_grid_pts),order='f')
strain_field_alias -= vacuum_strain_field
#strain_field_alias[:,:,:,-1,:,:] = 0
#strain_field_alias[:,:,:,:,-1,:] = 0
#strain_field_alias[:,:,:,:,:,-1] = 0
#strain_field_alias[:,:,:,:,:,:] = np.roll(strain_field_alias, (nb_domain_grid_pts[0]//2, nb_domain_grid_pts[1]//2, nb_domain_grid_pts[2]//2), (3,4,5))
[x_0, y_0, z_0], [x_displ, y_displ, z_displ] = get_complemented_positions_class_solver("0n", cell, solver, np.eye(3), periodically_complemented=True)
#x_displ = np.roll(x_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
#y_displ = np.roll(y_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
#z_displ = np.roll(z_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
actual_displacement = np.transpose([x_displ.ravel(order='F'), y_displ.ravel(order='F'), z_displ.ravel(order='F')])
strain_field = cell.get_fields().get_field("grad")
strain_field_alias = np.array(strain_field, copy=False)
#strain_field_alias[:,:,:,-1,:,:] = 0
#strain_field_alias[:,:,:,:,-1,:] = 0
#strain_field_alias[:,:,:,:,:,-1] = 0
#strain_field_alias[:,:,:,:,:,:] = np.roll(strain_field_alias, (nb_domain_grid_pts[0]//2, nb_domain_grid_pts[1]//2, nb_domain_grid_pts[2]//2), (3,4,5))
strain_field_alias[:,:,:,:,:] = cell.get_globalised_current_real_field("epsilon_plastic").array().reshape((dim, dim, nb_quad) + tuple(nb_domain_grid_pts),order='f')[:,:,:,:,:]
[x_0, y_0, z_0], [x_displ, y_displ, z_displ] = get_complemented_positions_class_solver("0n", cell, solver, np.eye(3), periodically_complemented=True)
#x_displ = np.roll(x_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
#y_displ = np.roll(y_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
#z_displ = np.roll(z_displ, (-(nb_domain_grid_pts[0]+1)//2, -(nb_domain_grid_pts[1]+1)//2, -(nb_domain_grid_pts[2]+1)//2), (0,1,2))
plastic_displacement = np.transpose([x_displ.ravel(order='F'), y_displ.ravel(order='F'), z_displ.ravel(order='F')])
point_data = {'actual_displacement' : actual_displacement, 'total_displacement': total_displacement, 'plastic_displacement': plastic_displacement}
file_io_object_read.read(frame=-1,field_names=["grad", "material2"])
return c_data, point_data
def main():
args = parse_args()
layer_no = args.layer_no
factor = args.factor
target_directory = args.target_directory
from mpi4py import MPI
comm_py = MPI.COMM_WORLD
comm = muGrid.Communicator(comm_py)
#rank = comm.rank
#procs = comm.size
#os.chdir('/scratch/kubilay/mechanical_model/results/mu_layer')
os.chdir(target_directory)
#get the geometry via fenics
mesh = fenics.Mesh()
filename = "/work/lammm/kubilay/mesh/layer_"+str(layer_no).zfill(3)+".xdmf"
temperature_filename = "/work/lammm/kubilay/results/temperature/temperature_layer_"+str(layer_no).zfill(3)+".h5"
f = fenics.XDMFFile(filename)
f.read(mesh)
fenics.MeshTransformation.rescale(mesh, 1e-3, fenics.Point(0,0,0)) #in m
f.close()
bounding_box = mesh.bounding_box_tree()
#nb_steps = 20
dim = 3
nb_quad = 6
x_max = np.max(mesh.coordinates()[:,0])
x_min = np.min(mesh.coordinates()[:,0])
y_max = np.max(mesh.coordinates()[:,1])
y_min = np.min(mesh.coordinates()[:,1])
z_max = np.max(mesh.coordinates()[:,2])
z_min = np.min(mesh.coordinates()[:,2])
xmax = np.array([np.NAN])
ymax = np.array([np.NAN])
zmax = np.array([np.NAN])
xmin = np.array([np.NAN])
ymin = np.array([np.NAN])
zmin = np.array([np.NAN])
dx, dy, dz = 0.00045, 0.0005, 0.00003
z_lim = 0.00801
#x_lim = 0.05496
#x_lim_min = -0.00004
x_lim = 0.05505
x_lim_min = 0.00005
element_dimensions = [dx, dy, dz]
#nb_domain_grid_pts = [11,11,11]
domain_lengths = [x_lim-x_lim_min,y_max-y_min,z_max-z_lim]
nb_domain_grid_pts = list(np.array(domain_lengths)/np.array(element_dimensions))
nb_domain_grid_pts = [round(i) for i in nb_domain_grid_pts]
#domain_lengths = [x_max-x_min,y_max-y_min,z_max-z_min]
#domain_lengths = [x_max-x_min,y_max-y_min,z_max-z_min]
#element_dimensions = np.array(domain_lengths)/np.array(nb_domain_grid_pts-np.ones(dim))
#define constant material properties
young = 162 #GPa
poisson = 0.277 #unitless
alpha_s = 0.55 #unitless
Delta_E_bs = 1.13*factor**(2/3) #eV
epsilon_sat = 0.35 # unitless
sigma_gb = 0.150 #GPa
sigma_s0 = 0.254*factor**(4/3) #GPa
sigma_f = 1.200 #GPa
## define the convergence tolerance for the Newton-Raphson increment
newton_tol = 1e-12
equil_tol = newton_tol
## tolerance for the solver of the linear cell
cg_tol = -1e-2
maxiter = 10000 # for linear cell solver
#bulk = np.load("bulk.npy")
#coords = np.load("coords.npy")
#nb_domain_grid_pts = np.load("nb_domain_grid_pts.npy")
#domain_lengths = np.load("domain_lengths.npy")
bulk = np.ones(nb_domain_grid_pts)
#x_dim = np.linspace(x_min, x_lim, nb_domain_grid_pts[0])
#y_dim = np.linspace(y_min, y_max, nb_domain_grid_pts[1])
#z_dim = np.linspace(z_lim, z_max, nb_domain_grid_pts[2])
#assign material
#for i,x in enumerate(x_dim):
# for j,y in enumerate(y_dim):
# for k,z in enumerate(z_dim):
# if len(bounding_box.compute_collisions(fenics.Point(x+0.5*dx,y+0.5*dy,z+0.5*dz))) != 0:
# bulk[i,j,k] = 1
#add base plate at the bottom and vacuum on top and sides
# bulk = np.insert(bulk, nb_domain_grid_pts[2], 0, axis=2)
# nb_domain_grid_pts[2] += 1
# domain_lengths[2] += element_dimensions[2]
# bulk = np.insert(bulk, nb_domain_grid_pts[1], 0, axis=1)
# nb_domain_grid_pts[1] += 1
# domain_lengths[1] += element_dimensions[1]
# bulk = np.insert(bulk, nb_domain_grid_pts[0], 0, axis=0)
# nb_domain_grid_pts[0] += 1
# domain_lengths[0] += element_dimensions[0]
#bulk[:,:,0] *= 2
#add base plate at the bottom and vacuum on top and sides
#increase the number of grid points and total domain length in each dimension
bulk = np.insert(bulk, 0, 2, axis=2)
nb_domain_grid_pts[2] += 1
domain_lengths[2] += element_dimensions[2]
bulk = np.insert(bulk, 0, 2, axis=2)
nb_domain_grid_pts[2] += 1
domain_lengths[2] += element_dimensions[2]
bulk = np.insert(bulk, nb_domain_grid_pts[2], 0, axis=2)
nb_domain_grid_pts[2] += 1
domain_lengths[2] += element_dimensions[2]
bulk = np.insert(bulk, nb_domain_grid_pts[1], 0, axis=1)
nb_domain_grid_pts[1] += 1
domain_lengths[1] += element_dimensions[1]
bulk = np.insert(bulk, 0, 0, axis=1)
nb_domain_grid_pts[1] += 1
domain_lengths[1] += element_dimensions[1]
bulk = np.insert(bulk, nb_domain_grid_pts[0], 0, axis=0)
nb_domain_grid_pts[0] += 1
domain_lengths[0] += element_dimensions[0]
bulk = np.insert(bulk, 0, 0, axis=0)
nb_domain_grid_pts[0] += 1
domain_lengths[0] += element_dimensions[0]
bulk = np.insert(bulk, 0, 2, axis=2)
nb_domain_grid_pts[2] += 1
domain_lengths[2] += element_dimensions[2]
bulk = np.insert(bulk, 0, 2, axis=2)
nb_domain_grid_pts[2] += 1
domain_lengths[2] += element_dimensions[2]
#domain discretisation TO DO:muspectre has this array already
x_dim = np.linspace(x_lim_min-element_dimensions[0], x_lim, nb_domain_grid_pts[0])+0.5*dx
y_dim = np.linspace(ymin-element_dimensions[1], ymax, nb_domain_grid_pts[1])+0.5*dy
z_dim = np.linspace(z_lim-4*element_dimensions[2], zmax, nb_domain_grid_pts[2])+0.5*dz
coords = np.zeros([nb_domain_grid_pts[0],nb_domain_grid_pts[1],nb_domain_grid_pts[2],3])
temperature_array = np.zeros((1,nb_quad)+tuple(nb_domain_grid_pts))
bulk_array = np.zeros_like(temperature_array)
for i in range(nb_domain_grid_pts[0]):
coords[i,:,:,0] = x_dim[i]
for i in range(nb_domain_grid_pts[1]):
coords[:,i,:,1] = y_dim[i]
for i in range(nb_domain_grid_pts[2]):
coords[:,:,i,2] = z_dim[i]
#s_list = [(0.005, 0.065)]
s_list = [(i,i+0.001) for i in np.linspace(0.005,0.050, 26)]
support_mask = np.ones_like(x_dim)
for i,x in enumerate(x_dim):
loc = x
for j,s in enumerate(s_list):
if loc>s[0] and loc<s[1]:
support_mask[i] = 0
#bulk[:,:,0] = 2
#bulk[:,-1,1] = 0
#bulk[-1,:,1] = 0
#for j,y in enumerate(y_dim):
# bulk[:,j,0] = bulk[:,j,0]*support_mask
cell = msp.cell.CellData.make(list(nb_domain_grid_pts), list(domain_lengths))
cell.nb_quad_pts = nb_quad
cell.get_fields().set_nb_sub_pts("quad", nb_quad)
#define materials
material = msp.material.MaterialHEA_3d.make(cell, "material", young, poisson, alpha_s, Delta_E_bs, epsilon_sat, sigma_gb, sigma_s0, sigma_f)
vacuum = msp.material.MaterialLinearElastic1_3d.make(cell, "vacuum", 0.0, poisson)
base = msp.material.MaterialLinearElastic1_3d.make(cell, "base", 20*young, poisson)
for pixel_index, pixel in enumerate(cell.pixels):
if bulk[tuple(pixel)]==1:
material.add_pixel(pixel_index)
bulk_array[0,:,pixel[0], pixel[1], pixel[2]] = 1
elif bulk[tuple(pixel)]==0:
vacuum.add_pixel(pixel_index)
elif bulk[tuple(pixel)]==2:
base.add_pixel(pixel_index)
gradient = Stencils3D.linear_finite_elements_6_regular
weights = nb_quad*[1]
material.T_m = 1600
material.alpha_thermal = 22e-6
material.identify_temperature_loaded_quad_pts(cell, bulk_array.reshape(-1,1, order="F"))
## use solver
krylov_solver = msp.solvers.KrylovSolverCG(cg_tol, maxiter, msp.Verbosity.Full)
solver = msp.solvers.SolverNewtonCG(cell, krylov_solver, msp.Verbosity.Full, newton_tol, equil_tol, maxiter, gradient, weights, msp.solvers.MeanControl.stress_control)
solver.formulation = msp.Formulation.small_strain
solver.initialise_cell()
output_filename = "layer_"+str(layer_no).zfill(3)+".nc"
file_io_object_read = muGrid.FileIONetCDF(output_filename,
muGrid.FileIONetCDF.OpenMode.Read,
comm)
cell.get_fields().set_nb_sub_pts("quad", nb_quad)
material_phase = cell.get_fields().register_int_field("material2", 1, 'quad')
material_phase_alias = np.array(material_phase, copy=False)
#coordinates = cell.get_fields().register_real_field("coordinates", 3, 'quad')
#temperature = cell.get_fields().register_real_field("temperature2", 1 , 'quad')
#vacuum_strain_field = cell.get_fields().register_real_field("vacuum_strain2", (3,3), "quad")
file_io_object_read.register_field_collection(field_collection=cell.get_fields(),field_names=cell.get_field_names())
file_io_object_read.register_field_collection(field_collection=material.collection)
# register global fields of the cell which you want to write
# print("cell field names:\n", cell.get_field_names())
#cell_field_names = cell.get_field_names()
sub_domain_loc = cell.subdomain_locations
# register global fields of the cell which you want to write
#print("cell field names:\n", cell.get_field_names())
#cell_field_names = cell.get_field_names()
#file_io_object_read.register_field_collection(field_collection=cell.get_fields(),field_names=["coordinates", "flux",
# "grad",
# "incrF",
# "material2",
# "rhs",
# "tangent", "temperature2", "vacuum_strain2"])
#file_io_object_read.register_field_collection(field_collection=material.collection, field_names=["epsilon_bar"])
#mat_fields = material.list_fields()
#file_io_object_read.register_field_collection(field_collection=material.collection)
# sub_domain_loc = cell.subdomain_locations
# #material_phase = cell.get_fields().register_int_field("material", 1, 'quad')
# material_phase_alias = np.array(material_phase, copy=False)
# coordinates_alias = np.array(coordinates, copy=False)
# for pixel_id, pixel_coord in cell.pixels.enumerate():
# i, j, k = pixel_coord[0], pixel_coord[1], pixel_coord[2]
# pix_mat = int(bulk[i, j, k])
# for q in range(nb_quad):
# # local coordinates on the processor
# a = i - sub_domain_loc[0]
# b = j - sub_domain_loc[1]
# c = k - sub_domain_loc[2]
# material_phase_alias[a, b, c] = pix_mat
# coordinates_alias[0, 0, a, b, c] = i
# coordinates_alias[1, 0, a, b, c] = j
# coordinates_alias[2, 0, a, b, c] = k
timestamp_arr = file_io_object_read.read_global_attribute('timestamp')
#print(timestamp_arr)
nb_steps = len(timestamp_arr)
start = timer.time()
import meshio
points = msp.linear_finite_elements.get_position_3d_helper(cell, solver=solver)
nx, ny, nz = cell.nb_domain_grid_pts
xc, yc, zc = np.mgrid[:nx, :ny, :nz]
# Global node indices
def c2i(xp, yp, zp):
return xp + (nx+1) * (yp + (ny+1) * zp)
cells = cells = np.swapaxes(
[[c2i(xc, yc, zc), c2i(xc+1, yc, zc),
c2i(xc+1, yc+1, zc), c2i(xc+1, yc+1, zc+1)],
[c2i(xc, yc, zc), c2i(xc+1, yc, zc),
c2i(xc+1, yc, zc+1), c2i(xc+1, yc+1, zc+1)],
[c2i(xc, yc, zc), c2i(xc, yc+1, zc),
c2i(xc+1, yc+1, zc), c2i(xc+1, yc+1, zc+1)],
[c2i(xc, yc, zc), c2i(xc, yc+1, zc),
c2i(xc, yc+1, zc+1), c2i(xc+1, yc+1, zc+1)],
[c2i(xc, yc, zc), c2i(xc, yc, zc+1),
c2i(xc+1, yc, zc+1), c2i(xc+1, yc+1, zc+1)],
[c2i(xc, yc, zc), c2i(xc, yc, zc+1),
c2i(xc, yc+1, zc+1), c2i(xc+1, yc+1, zc+1)]],
0, 1)
cells = cells.reshape((4, -1), order='F').T
T_m = 1600
alpha_thermal = 22e-6
epsilon_sat = 0.35
sigma_for = 1.200
with meshio.xdmf.TimeSeriesWriter('mu_layer_'+str(layer_no).zfill(3)+'.xdmf') as writer:
writer.write_points_cells(points, {"tetra": cells})
c_data, point_data = read_data_of_step(file_io_object_read, cell, solver, True, material, read_frame=0)
writer.write_data(timestamp_arr[0], cell_data=c_data, point_data=point_data)
if layer_no == 333:
c_data, point_data = read_data_of_step(file_io_object_read, cell, solver, True, material, read_frame=1)
writer.write_data(timestamp_arr[1], cell_data=c_data, point_data=point_data)
material.dt = 3000
res = solver.solve_load_increment(np.zeros((3,3)))
c_data, point_data = read_data_of_step(file_io_object_read, cell, solver, False, material)
writer.write_data(timestamp_arr[1]+material.dt, cell_data=c_data, point_data=point_data)
#for i in range(1):
# print('=== STEP {}/{} ==='.format(i+1, nb_steps))
# if layer_no == 333:
#flux_arr = cell.get_fields().get_field('flux').array()
#grad_arr = cell.get_fields().get_field('grad').array()
#vacuum_strain_arr = cell.get_globalised_internal_real_field("vacuum_strain").array()
#flux_arr_alias = np.array(flux_arr, copy=False)
#grad_arr_alias = np.array(grad_arr, copy=False)
#vacuum_strain_arr_alias = np.array(vacuum_strain_arr, copy=False)
#flux_arr_alias[:,:,:,:,:] = 0
#grad_arr_alias[:,:,:,:,:] = 0
#vacuum_strain_arr_alias[:,:,:,:,:] = 0
#material.update_vacuum_strain_field(cell, vacuum_strain_arr_alias.reshape(-1,1, order="F"))
# material.update_temperature_field(cell, 293*np.ones_like(bulk_array.reshape(-1,1,order="F")))
# material.dt = 3000
#material.alpha_thermal = 0.0
# res = solver.solve_load_increment(np.zeros((3,3)))
#msp.linear_finite_elements.write_3d_class(
#"ekin_tutorial_3D_spectral_output_{}.xdmf".format(i), cell, solver, cell_data=c_data)
comm_py.barrier()
#stress = cell.get_fields().get_field('flux').array()
#strain = cell.get_fields().get_field('grad').array()
#temperature = cell.get_fields().get_field('temperature').array()
#np.savez('previous_fields.npz', stress=stress, strain= strain, temperature=temperature)
file_io_object_read.close()
if __name__=='__main__':
main()
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