def _mats_default( self ):
# Material model construction
mats = MATS1D5Bond( mats_phase1 = self.mats_m,
mats_phase2 = self.mats_f,
mats_ifslip = self.mats_b,
mats_ifopen = MATS1DElastic( E = 0 ) # elastic function of open - inactive
)
return mats
def _get_mats_fb(self):
# Material model construction
return MATS1D5Bond(
mats_phase1=MATS1DElastic(E=0),
mats_phase2=self.mats_f,
mats_ifslip=self.mats_b,
mats_ifopen=MATS1DElastic(
E=0) # elastic function of open - inactive
)
def example():
from ibvpy.api import \
TStepper as TS, RTDofGraph, RTraceDomainListField, TLoop, \
TLine, IBVPSolve as IS, DOTSEval, BCSlice
from ibvpy.mesh.fe_grid import FEGrid
from mathkit.mfn import MFnLineArray
stiffness_concrete = 34000 * 0.03 * 0.03
A_fiber = 1.
E_fiber = 1.
stiffness_fiber = E_fiber * A_fiber
d = 2 * sqrt(Pi)
tau_max = 0.1 * d * Pi
G = 100
u_max = 0.023
f_max = 0.2
mats_eval = MATS1D5Bond(mats_phase1=MATS1DElastic(E=stiffness_fiber),
mats_phase2=MATS1DElastic(E=0),
mats_ifslip=MATS1DPlastic(E=G,
sigma_y=tau_max,
K_bar=0.,
H_bar=0.),
mats_ifopen=MATS1DElastic(E=0))
fets_eval = FETS1D52L4ULRH(mats_eval=mats_eval)
domain = FEGrid(coord_max=(1., 0.2),
shape=(16, 1),
fets_eval=fets_eval)
end_dof = domain[-1, 0, -1, 0].dofs[0, 0, 0]
ts = TS(dof_resultants=True,
sdomain=domain,
# conversion to list (square brackets) is only necessary for slicing of
# single dofs, e.g "get_left_dofs()[0,1]"
bcond_list=[
BCSlice(var='u', value=0., dims=[0],
slice=domain[:, :, :, -1]),
BCSlice(var='u', value=0., dims=[1],
slice=domain[:, :, :, :]),
BCSlice(var='f', value=f_max, dims=[0],
slice=domain[-1, 0, -1, 0])
],
rtrace_list=[RTDofGraph(name='Fi,right over u_right (iteration)',
var_y='F_int', idx_y=end_dof,
var_x='U_k', idx_x=end_dof),
RTraceDomainListField(name='slip',
var='slip', idx=0),
RTraceDomainListField(name='eps1',
var='eps1', idx=0),
RTraceDomainListField(name='eps2',
var='eps2', idx=0),
RTraceDomainListField(name='shear_flow',
var='shear_flow', idx=0),
RTraceDomainListField(name='sig1',
var='sig1', idx=0),
RTraceDomainListField(name='sig2',
var='sig2', idx=0),
RTraceDomainListField(name='Displacement',
var='u', idx=0)
])
# Add the time-loop control
tloop = TLoop(tstepper=ts, KMAX=30, debug=False,
tline=TLine(min=0.0, step=0.1, max=1.0))
print(tloop.eval())
# Put the whole stuff into the simulation-framework to map the
# individual pieces of definition into the user interface.
#
from ibvpy.plugins.ibvpy_app import IBVPyApp
app = IBVPyApp(ibv_resource=tloop)
app.main()
from mayavi.sources.api import VTKDataSource, VTKFileReader
from ibvpy.fets.fets1D5 import FETS1D52L4ULRH
from ibvpy.mats.mats1D import MATS1DElastic
from ibvpy.mats.mats1D5.mats1D5_bond import MATS1D5Bond
from ibvpy.mesh.fe_grid import FEGrid
from mathkit.matrix_la.sys_mtx_assembly import SysMtxAssembly
import numpy as np
if __name__ == '__main__':
#=========================================================================
# Material matrix
#=========================================================================
mats_eval = MATS1D5Bond(mats_phase1=MATS1DElastic(E=10.),
mats_phase2=MATS1DElastic(E=20.),
mats_ifslip=MATS1DElastic(E=5.),
mats_ifopen=MATS1DElastic(E=1.))
D_el = np.diag(np.array([10., 0.1, 1., 10.]))
n_s = D_el.shape[0]
#=========================================================================
# Element definition
#=========================================================================
fets_eval = FETS1D52L4ULRH(mats_eval=mats_eval)
n_geo_r, n_dim_geo = fets_eval.geo_r.shape
n_dof_r, n_dim_dof = fets_eval.dof_r.shape
n_ip = fets_eval.n_gp
n_el_dofs = n_dof_r * n_dim_dof
#[ d, i]
r_ip = fets_eval.ip_coords[:, :-1].T