def __init__(self, keyword, grids):
if isinstance(grids, list):
self._grids = grids
else:
self._grids = [grids]
dim = np.unique([g[0].dim for g in grids])
low_dim_grids = [g[1] for g in grids]
if not dim.size == 1:
raise ValueError("Expected unique dimension of grids with contact problems")
self._discretization = pp.ColoumbContact(
keyword, ambient_dimension=dim[0], discr_h=pp.Mpsa(keyword)
)
self._name = "Biot stabilization term"
self.keyword = keyword
self.traction: _MergedOperator
self.displacement: _MergedOperator
self.rhs: _MergedOperator
_wrap_discretization(
self, self._discretization, grids, mat_dict_grids=low_dim_grids
)
def assign_discretizations(self):
"""
Assign discretizations to the nodes and edges of the grid bucket.
"""
# For the Nd domain we solve linear elasticity with mpsa.
Nd = self.Nd
gb = self.gb
mpsa = pp.Mpsa(self.mechanics_parameter_key)
# We need a void discretization for the contact traction variable defined on
# the fractures.
empty_discr = pp.VoidDiscretization(self.mechanics_parameter_key, ndof_cell=Nd)
for g, d in gb:
if g.dim == Nd:
d[pp.DISCRETIZATION] = {self.displacement_variable: {"mpsa": mpsa}}
elif g.dim == Nd - 1:
d[pp.DISCRETIZATION] = {
self.contact_traction_variable: {"empty": empty_discr}
}
# Define the contact condition on the mortar grid
coloumb = pp.ColoumbContact(self.mechanics_parameter_key, Nd, mpsa)
contact = pp.PrimalContactCoupling(self.mechanics_parameter_key, mpsa, coloumb)
for e, d in gb.edges():
g_l, g_h = gb.nodes_of_edge(e)
if g_h.dim == Nd:
d[pp.COUPLING_DISCRETIZATION] = {
self.friction_coupling_term: {
g_h: (self.displacement_variable, "mpsa"),
g_l: (self.contact_traction_variable, "empty"),
(g_h, g_l): (self.mortar_displacement_variable, contact),
}
}
def setup(self):
g = pp.CartGrid([5, 5])
g.compute_geometry()
stiffness = pp.FourthOrderTensor(np.ones(g.num_cells),
np.ones(g.num_cells))
bnd = pp.BoundaryConditionVectorial(g)
specified_data = {
"fourth_order_tensor": stiffness,
"bc": bnd,
"inverter": "python",
}
keyword = "mechanics"
data = pp.initialize_default_data(g, {},
keyword,
specified_parameters=specified_data)
discr = pp.Mpsa(keyword)
discr.discretize(g, data)
stress = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.stress_matrix_key]
bound_stress = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.bound_stress_matrix_key]
return g, stiffness, bnd, stress, bound_stress
def test_cart_2d(self):
g = pp.CartGrid([2, 1], physdims=(1, 1))
g.compute_geometry()
right = g.face_centers[0] > 1 - 1e-10
top = g.face_centers[1] > 1 - 1e-10
bc = pp.BoundaryConditionVectorial(g)
bc.is_dir[:, top] = True
bc.is_dir[0, right] = True
bc.is_neu[bc.is_dir] = False
g = true_2d(g)
subcell_topology = pp.fvutils.SubcellTopology(g)
# Mat boundary to subfaces
bc = pp.fvutils.boundary_to_sub_boundary(bc, subcell_topology)
bound_exclusion = pp.fvutils.ExcludeBoundaries(subcell_topology, bc,
g.dim)
cell_node_blocks = np.array([[0, 0, 0, 0, 1, 1, 1, 1],
[0, 1, 3, 4, 1, 2, 4, 5]])
ncasym_np = np.arange(32 * 32).reshape((32, 32))
ncasym = sps.csr_matrix(ncasym_np)
pp.Mpsa("")._eliminate_ncasym_neumann(ncasym, subcell_topology,
bound_exclusion,
cell_node_blocks, 2)
eliminate_ind = np.array([0, 1, 16, 17, 26, 27])
ncasym_np[eliminate_ind] = 0
self.assertTrue(np.allclose(ncasym.A, ncasym_np))
def test_structured_triang(self):
nx = 1
ny = 1
g = pp.StructuredTriangleGrid([nx, ny], physdims=[1, 1])
g.compute_geometry()
bot = g.face_centers[1] < 1e-10
top = g.face_centers[1] > 1 - 1e-10
left = g.face_centers[0] < 1e-10
right = g.face_centers[0] > 1 - 1e-10
is_dir = left
is_neu = top
is_rob = right + bot
bnd = pp.BoundaryConditionVectorial(g)
bnd.is_neu[:] = False
bnd.is_dir[:, is_dir] = True
bnd.is_rob[:, is_rob] = True
bnd.is_neu[:, is_neu] = True
sc_top = pp.fvutils.SubcellTopology(g)
bnd = pp.fvutils.boundary_to_sub_boundary(bnd, sc_top)
bnd_excl = pp.fvutils.ExcludeBoundaries(sc_top, bnd, g.dim)
rhs = pp.Mpsa("")._create_bound_rhs(bnd, bnd_excl, sc_top, g, True)
hf2f = pp.fvutils.map_hf_2_f(sc_top.fno_unique, sc_top.subfno_unique,
g.dim)
rhs = rhs * hf2f.T
rhs_known = np.array([
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0],
[1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0],
[0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0],
[0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
[0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0],
])
self.assertTrue(np.all(np.abs(rhs_known - rhs) < 1e-12))
def reconstruct_stress(self, previous_iterate: bool = False) -> None:
"""
Compute the stress in the highest-dimensional grid based on the displacement
states in that grid, adjacent interfaces and global boundary conditions.
The stress is stored in the data dictionary of the highest-dimensional grid,
in [pp.STATE]['stress'].
Parameters:
previous_iterate (boolean, optional): If True, use values from previous
iteration to compute the stress. Defaults to False.
"""
# Highest-dimensional grid and its data
g = self._nd_grid()
d = self.gb.node_props(g)
# Pick the relevant displacemnet field
if previous_iterate:
u = d[pp.STATE][pp.ITERATE][self.displacement_variable]
else:
u = d[pp.STATE][self.displacement_variable]
matrix_dictionary: Dict[str, sps.spmatrix] = d[
pp.DISCRETIZATION_MATRICES][self.mechanics_parameter_key]
# Make a discretization object to get hold of the right keys to access the
# matrix_dictionary
mpsa = pp.Mpsa(self.mechanics_parameter_key)
# Stress contribution from internal cell center displacements
stress: np.ndarray = matrix_dictionary[mpsa.stress_matrix_key] * u
# Contributions from global boundary conditions
bound_stress_discr: sps.spmatrix = matrix_dictionary[
mpsa.bound_stress_matrix_key]
global_bc_val: np.ndarray = d[pp.PARAMETERS][
self.mechanics_parameter_key]["bc_values"]
stress += bound_stress_discr * global_bc_val
# Contributions from the mortar displacement variables
for e, d_e in self.gb.edges():
# Only contributions from interfaces to the highest dimensional grid
mg: pp.MortarGrid = d_e["mortar_grid"]
if mg.dim == self._Nd - 1:
if previous_iterate:
u_e: np.ndarray = d_e[pp.STATE][pp.ITERATE][
self.mortar_displacement_variable]
else:
u_e = d_e[pp.STATE][self.mortar_displacement_variable]
stress += (bound_stress_discr *
mg.mortar_to_primary_avg(nd=self._Nd) * u_e)
d[pp.STATE]["stress"] = stress
def test_mpsa(self):
self.setup()
g, g_larger = self.g, self.g_larger
specified_data = {
"inverter": "python",
}
keyword = "mechanics"
data_small = pp.initialize_default_data(
g, {}, keyword, specified_parameters=specified_data)
discr = pp.Mpsa(keyword)
# Discretization on a small problem
discr.discretize(g, data_small)
# Perturb one node
g_larger.nodes[0, 2] += 0.2
# Faces that have their geometry changed
update_faces = np.array([2, 21, 22])
# Perturb the permeability in some cells on the larger grid
mu, lmbda = np.ones(g_larger.num_cells), np.ones(g_larger.num_cells)
high_coeff_cells = np.array([7, 12])
stiff_larger = pp.FourthOrderTensor(mu, lmbda)
specified_data_larger = {"fourth_order_tensor": stiff_larger}
# Do a full discretization on the larger grid
data_full = pp.initialize_default_data(
g_larger, {}, keyword, specified_parameters=specified_data_larger)
discr.discretize(g_larger, data_full)
# Cells that will be marked as updated, either due to changed parameters or
# the newly defined topology
update_cells = np.union1d(self.new_cells, high_coeff_cells)
updates = {
"modified_cells": update_cells,
# "modified_faces": update_faces,
"map_cells": self.cell_map,
"map_faces": self.face_map,
}
# Data dictionary for the two-step discretization
data_partial = pp.initialize_default_data(
g_larger, {}, keyword, specified_parameters=specified_data_larger)
data_partial["update_discretization"] = updates
self._update_and_compare(data_small, data_partial, data_full, g_larger,
[keyword], discr)
def _assign_discretizations(self) -> None:
"""
Assign discretizations to the nodes and edges of the grid bucket.
Note the attribute subtract_fracture_pressure: Indicates whether or not to
subtract the fracture pressure contribution for the contact traction. This
should not be done if the scalar variable is temperature.
"""
super()._assign_discretizations()
# Shorthand
key_s, key_m = self.scalar_parameter_key, self.mechanics_parameter_key
var_s, var_d = self.scalar_variable, self.displacement_variable
# Define discretization
# For the Nd domain we solve linear elasticity with mpsa.
mpsa = pp.Mpsa(key_m)
mass_disc_s = pp.MassMatrix(key_s)
source_disc_s = pp.ScalarSource(key_s)
# Coupling discretizations
# Assign node discretizations
for g, d in self.gb:
if g.dim == self.Nd:
mpsa = d[pp.DISCRETIZATION][var_d]["mpsa"]
elif g.dim == self.Nd - 1:
d[pp.DISCRETIZATION].update({
var_s: {
"mass": mass_disc_s,
"source": source_disc_s,
},
})
fracture_scalar_to_force_balance = pp.FractureScalarToForceBalance(
mpsa, mass_disc_s)
for e, d in self.gb.edges():
g_l, g_h = self.gb.nodes_of_edge(e)
if g_h.dim == self.Nd:
d[pp.COUPLING_DISCRETIZATION].update({
"fracture_scalar_to_force_balance": {
g_h: (var_d, "mpsa"),
g_l: (var_s, "mass"),
e: (
self.mortar_displacement_variable,
fracture_scalar_to_force_balance,
),
}
})
def reconstruct_stress(self, previous_iterate: bool = False) -> None:
"""
Compute the stress in the highest-dimensional grid based on the displacement
states in that grid, adjacent interfaces and global boundary conditions.
The stress is stored in the data dictionary of the highest-dimensional grid,
in [pp.STATE]['stress'].
Parameters:
previous_iterate (boolean, optional): If True, use values from previous
iteration to compute the stress. Defaults to False.
"""
g = self._nd_grid()
d = self.gb.node_props(g)
mpsa = pp.Mpsa(self.mechanics_parameter_key)
if previous_iterate:
u = d[pp.STATE][pp.ITERATE][self.displacement_variable]
else:
u = d[pp.STATE][self.displacement_variable]
matrix_dictionary = d[pp.DISCRETIZATION_MATRICES][
self.mechanics_parameter_key]
# Stress contribution from internal cell center displacements
stress = matrix_dictionary[mpsa.stress_matrix_key] * u
# Contributions from global boundary conditions
bound_stress_discr = matrix_dictionary[mpsa.bound_stress_matrix_key]
global_bc_val = d[pp.PARAMETERS][
self.mechanics_parameter_key]["bc_values"]
stress += bound_stress_discr * global_bc_val
# Contributions from the mortar displacement variables
for e, d_e in self.gb.edges():
# Only contributions from interfaces to the highest dimensional grid
mg = d_e["mortar_grid"]
if mg.dim == self.Nd - 1:
if previous_iterate:
u_e = d_e[pp.STATE][pp.ITERATE][
self.mortar_displacement_variable]
else:
u_e = d_e[pp.STATE][self.mortar_displacement_variable]
stress += bound_stress_discr * mg.mortar_to_master_avg(
nd=self.Nd) * u_e
d[pp.STATE]["stress"] = stress
def assign_mechanics_discretizations(self) -> None:
"""
Assign discretizations to the nodes and edges of the grid bucket.
"""
gb = self.gb
nd = self.Nd
# Shorthand
key_m, var_m = self.mechanics_parameter_key, self.displacement_variable
var_contact = self.contact_traction_variable
var_mortar = self.mortar_displacement_variable
discr_key, coupling_discr_key = pp.DISCRETIZATION, pp.COUPLING_DISCRETIZATION
# For the Nd domain we solve linear elasticity with mpsa.
mpsa = pp.Mpsa(key_m)
# We need a void discretization for the contact traction variable defined on
# the fractures.
empty_discr = pp.VoidDiscretization(key_m, ndof_cell=nd)
# Assign node discretizations
for g, d in gb:
add_nonpresent_dictionary(d, discr_key)
if g.dim == nd:
d[discr_key].update(
{var_m: {"mpsa": mpsa},}
)
elif g.dim == nd - 1:
d[discr_key].update(
{var_contact: {"empty": empty_discr},}
)
# Define the contact condition on the mortar grid
coloumb = pp.ColoumbContact(key_m, nd, mpsa)
contact = pp.PrimalContactCoupling(key_m, mpsa, coloumb)
for e, d in gb.edges():
g_l, g_h = gb.nodes_of_edge(e)
add_nonpresent_dictionary(d, coupling_discr_key)
if g_h.dim == nd:
d[coupling_discr_key].update(
{
self.friction_coupling_term: {
g_h: (var_m, "mpsa"),
g_l: (var_contact, "empty"),
e: (var_mortar, contact),
},
}
)
def reconstruct_stress(self, previous_iterate: bool = False) -> None:
""" Compute the stress in the highest-dimensional grid based on the displacement
states in that grid, adjacent interfaces and global boundary conditions.
The stress is stored in the data dictionary of the highest-dimensional grid,
in [pp.STATE]["stress"].
Parameters:
previous_iterate : bool
If True, use values from previous iteration to compute the stress.
Default: False.
"""
# TODO: Currently 'reconstruct_stress' does not work if 'previous_iterate = True'
# since the displacement variable on Nd-grid is not stored in pp.ITERATE.
if previous_iterate is True:
raise ValueError("Not yet implemented.")
g = self._nd_grid()
d = self.gb.node_props(g)
key_m = self.mechanics_parameter_key
var_m = self.displacement_variable
var_mortar = self.mortar_displacement_variable
mpsa = pp.Mpsa(self.mechanics_parameter_key)
if previous_iterate:
u = d[pp.STATE][pp.ITERATE][var_m]
else:
u = d[pp.STATE][var_m]
matrix_dictionary = d[pp.DISCRETIZATION_MATRICES][key_m]
# Stress contribution from internal cell center displacements
stress = matrix_dictionary[mpsa.stress_matrix_key] * u
# Contributions from global boundary conditions
bound_stress_discr = matrix_dictionary[mpsa.bound_stress_matrix_key]
global_bc_val = d[pp.PARAMETERS][key_m]["bc_values"]
stress += bound_stress_discr * global_bc_val
# Contributions from the mortar displacement variables
for e, d_e in self.gb.edges():
# Only contributions from interfaces to the highest dimensional grid
mg: pp.MortarGrid = d_e["mortar_grid"]
if mg.dim == self.Nd - 1:
u_e = d_e[pp.STATE][var_mortar]
stress += bound_stress_discr * mg.mortar_to_master_avg(nd=self.Nd) * u_e
d[pp.STATE]["stress"] = stress
def test_bound_cell_node_keyword(self):
# Compute update for a single cell on the
g, stiffness, bnd, stress, bound_stress = self.setup()
# inner_cell = 10
nodes_of_cell = np.array([12, 13, 18, 19])
faces_of_cell = np.array([12, 13, 40, 45])
bnd = pp.BoundaryConditionVectorial(g)
specified_data = {
"fourth_order_tensor": stiffness,
"bc": bnd,
"inverter": "python",
"specified_nodes": np.array([nodes_of_cell]),
}
keyword = "mechanics"
data = pp.initialize_default_data(g, {},
keyword,
specified_parameters=specified_data)
discr = pp.Mpsa(keyword)
discr.discretize(g, data)
partial_stress = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.stress_matrix_key]
partial_bound = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.bound_stress_matrix_key]
active_faces = data[pp.PARAMETERS][keyword]["active_faces"]
self.assertTrue(faces_of_cell.size == active_faces.size)
self.assertTrue(
np.all(np.sort(faces_of_cell) == np.sort(active_faces)))
faces_of_cell = self.expand_indices_nd(faces_of_cell, g.dim)
diff_stress = (stress - partial_stress).todense()
diff_bound = (bound_stress - partial_bound).todense()
self.assertTrue(np.max(np.abs(diff_stress[faces_of_cell])) == 0)
self.assertTrue(np.max(np.abs(diff_bound[faces_of_cell])) == 0)
# Only the faces of the central cell should be non-zero.
pp.fvutils.remove_nonlocal_contribution(faces_of_cell, 1,
partial_stress, partial_bound)
self.assertTrue(np.max(np.abs(partial_stress.data)) == 0)
self.assertTrue(np.max(np.abs(partial_bound.data)) == 0)
def __init__(self, keyword, grids):
if isinstance(grids, list):
self._grids = grids
else:
self._grids = [grids]
self._discretization = pp.Mpsa(keyword)
self._name = "Mpsa"
self.keyword = keyword
# Declear attributes, these will be initialized by the below call to the
# discretization wrapper.
self.stress: _MergedOperator
self.bound_stress: _MergedOperator
self.bound_displacement_cell: _MergedOperator
self.bound_displacement_face: _MergedOperator
_wrap_discretization(self, self._discretization, grids)
def set_parameters(self, g, data_node, mg, data_edge):
"""
Set the parameters for the simulation. The stress is given in GPa.
"""
# Define the finite volume sub grid
s_t = pp.fvutils.SubcellTopology(g)
# Rock parameters
rock = pp.Granite()
lam = rock.LAMBDA * np.ones(g.num_cells) / self.pressure_scale
mu = rock.MU * np.ones(g.num_cells) / self.pressure_scale
F = self._friction_coefficient(g, mg, data_edge, s_t)
k = pp.FourthOrderTensor(g.dim, mu, lam)
# Define boundary regions
top = g.face_centers[g.dim - 1] > np.max(g.nodes[1]) - 1e-9
bot = g.face_centers[g.dim - 1] < np.min(g.nodes[1]) + 1e-9
top_hf = top[s_t.fno_unique]
bot_hf = bot[s_t.fno_unique]
# Define boundary condition on sub_faces
bc = pp.BoundaryConditionVectorial(g, top + bot, 'dir')
bc = pp.fvutils.boundary_to_sub_boundary(bc, s_t)
# Set the boundary values
u_bc = np.zeros((g.dim, s_t.num_subfno_unique))
u_bc[1, top_hf] = -0.002
u_bc[0, top_hf] = 0.005
# Find the continuity points
eta = 1 / 3
eta_vec = eta * np.ones(s_t.num_subfno_unique)
cont_pnt = g.face_centers[:g.dim, s_t.fno_unique] + eta_vec * (
g.nodes[:g.dim, s_t.nno_unique] -
g.face_centers[:g.dim, s_t.fno_unique])
# collect parameters in dictionary
key = 'mech'
key_m = 'mech'
data_node = pp.initialize_data(
g, data_node, key, {
'bc': bc,
'bc_values': u_bc.ravel('F'),
'source': 0,
'fourth_order_tensor': k,
'mpsa_eta': eta_vec,
'cont_pnt': cont_pnt,
'rock': rock,
})
pp.initialize_data(mg, data_edge, key_m, {
'friction_coeff': F,
'c': 100
})
# Define discretization
# For the 2D domain we solve linear elasticity with mpsa.
mpsa = pp.Mpsa(key)
data_node[pp.PRIMARY_VARIABLES] = {'u': {'cells': g.dim}}
data_node[pp.DISCRETIZATION] = {'u': {'mpsa': mpsa}}
# And define a Robin condition on the mortar grid
contact = pp.numerics.interface_laws.elliptic_interface_laws.RobinContact(
key_m, mpsa)
data_edge[pp.PRIMARY_VARIABLES] = {'lam': {'cells': g.dim}}
data_edge[pp.COUPLING_DISCRETIZATION] = {
'robin_disc': {
g: ('u', 'mpsa'),
g: ('u', 'mpsa'),
(g, g): ('lam', contact),
}
}
return key, key_m
def _assign_discretizations(self) -> None:
"""
Assign discretizations to the nodes and edges of the grid bucket.
"""
# For the Nd domain we solve linear elasticity with mpsa.
Nd = self._Nd
gb = self.gb
if not self._use_ad:
mpsa = pp.Mpsa(self.mechanics_parameter_key)
# We need a void discretization for the contact traction variable defined on
# the fractures.
empty_discr = pp.VoidDiscretization(self.mechanics_parameter_key,
ndof_cell=Nd)
for g, d in gb:
if g.dim == Nd:
d[pp.DISCRETIZATION] = {
self.displacement_variable: {
"mpsa": mpsa
}
}
elif g.dim == Nd - 1:
d[pp.DISCRETIZATION] = {
self.contact_traction_variable: {
"empty": empty_discr
}
}
# Define the contact condition on the mortar grid
coloumb = pp.ColoumbContact(self.mechanics_parameter_key, Nd, mpsa)
contact = pp.PrimalContactCoupling(self.mechanics_parameter_key,
mpsa, coloumb)
for e, d in gb.edges():
g_l, g_h = gb.nodes_of_edge(e)
if g_h.dim == Nd:
d[pp.COUPLING_DISCRETIZATION] = {
self.friction_coupling_term: {
g_h: (self.displacement_variable, "mpsa"),
g_l: (self.contact_traction_variable, "empty"),
(g_h, g_l):
(self.mortar_displacement_variable, contact),
}
}
else:
dof_manager = pp.DofManager(gb)
eq_manager = pp.ad.EquationManager(gb, dof_manager)
g_primary: pp.Grid = gb.grids_of_dimension(Nd)[0]
g_frac: List[pp.Grid] = gb.grids_of_dimension(Nd - 1).tolist()
num_frac_cells = np.sum([g.num_cells for g in g_frac])
if len(gb.grids_of_dimension(Nd)) != 1:
raise NotImplementedError("This will require further work")
edge_list = [(g_primary, g) for g in g_frac]
mortar_proj = pp.ad.MortarProjections(edges=edge_list,
gb=gb,
nd=self._Nd)
subdomain_proj = pp.ad.SubdomainProjections(gb=gb, nd=self._Nd)
tangential_proj_lists = [
gb.node_props(
gf,
"tangential_normal_projection").project_tangential_normal(
gf.num_cells) for gf in g_frac
]
tangential_proj = pp.ad.Matrix(
sps.block_diag(tangential_proj_lists))
mpsa_ad = mpsa_ad = pp.ad.MpsaAd(self.mechanics_parameter_key,
g_primary)
bc_ad = pp.ad.BoundaryCondition(self.mechanics_parameter_key,
grids=[g_primary])
div = pp.ad.Divergence(grids=[g_primary], dim=g_primary.dim)
# Primary variables on Ad form
u = eq_manager.variable(g_primary, self.displacement_variable)
u_mortar = eq_manager.merge_variables([
(e, self.mortar_displacement_variable) for e in edge_list
])
contact_force = eq_manager.merge_variables([
(g, self.contact_traction_variable) for g in g_frac
])
u_mortar_prev = u_mortar.previous_timestep()
# Stress in g_h
stress = (mpsa_ad.stress * u + mpsa_ad.bound_stress * bc_ad +
mpsa_ad.bound_stress *
subdomain_proj.face_restriction(g_primary) *
mortar_proj.mortar_to_primary_avg * u_mortar)
# momentum balance equation in g_h
momentum_eq = pp.ad.Expression(div * stress,
dof_manager,
name="momentuum",
grid_order=[g_primary])
coloumb_ad = pp.ad.ColoumbContactAd(self.mechanics_parameter_key,
edge_list)
jump_rotate = (tangential_proj *
subdomain_proj.cell_restriction(g_frac) *
mortar_proj.mortar_to_secondary_avg *
mortar_proj.sign_of_mortar_sides)
# Contact conditions
jump_discr = coloumb_ad.displacement * jump_rotate * u_mortar
tmp = np.ones(num_frac_cells * self._Nd)
tmp[self._Nd - 1::self._Nd] = 0
exclude_normal = pp.ad.Matrix(
sps.dia_matrix((tmp, 0), shape=(tmp.size, tmp.size)))
# Rhs of contact conditions
rhs = (coloumb_ad.rhs + exclude_normal * coloumb_ad.displacement *
jump_rotate * u_mortar_prev)
contact_conditions = coloumb_ad.traction * contact_force + jump_discr - rhs
contact_eq = pp.ad.Expression(contact_conditions,
dof_manager,
grid_order=g_frac,
name="contact")
# Force balance
mat = None
for _, d in gb.edges():
mg: pp.MortarGrid = d["mortar_grid"]
if mg.dim < self._Nd - 1:
continue
faces_on_fracture_surface = mg.primary_to_mortar_int().tocsr(
).indices
m = pp.grid_utils.switch_sign_if_inwards_normal(
g_primary, self._Nd, faces_on_fracture_surface)
if mat is None:
mat = m
else:
mat += m
sign_switcher = pp.ad.Matrix(mat)
# Contact from primary grid and mortar displacements (via primary grid)
contact_from_primary_mortar = (
mortar_proj.primary_to_mortar_int *
subdomain_proj.face_prolongation(g_primary) * sign_switcher *
stress)
contact_from_secondary = (
mortar_proj.sign_of_mortar_sides *
mortar_proj.secondary_to_mortar_int *
subdomain_proj.cell_prolongation(g_frac) *
tangential_proj.transpose() * contact_force)
force_balance_eq = pp.ad.Expression(
contact_from_primary_mortar + contact_from_secondary,
dof_manager,
name="force_balance",
grid_order=edge_list,
)
# eq2 = pp.ad.Equation(contact_from_secondary, dof_manager).to_ad(gb)
eq_manager.equations += [momentum_eq, contact_eq, force_balance_eq]
self._eq_manager = eq_manager
def test_cart_2d(self):
nx = 1
ny = 1
g = pp.CartGrid([nx, ny], physdims=[2, 2])
g.compute_geometry()
g = make_true_2d(g)
sc_top = pp.fvutils.SubcellTopology(g)
D_g, CC = pp.Mpsa("")._reconstruct_displacement(g, sc_top, eta=0)
D_g_known = np.array([
[
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1.0,
0.0,
],
[
0.0,
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1.0,
],
])
CC_known = np.array([
[1, 0.0],
[0, 1.0],
[1, 0.0],
[0, 1.0],
[1, 0.0],
[0, 1.0],
[1, 0.0],
[0, 1.0],
[1, 0.0],
[0, 1.0],
[1, 0.0],
[0, 1.0],
[1, 0.0],
[0, 1.0],
[1, 0.0],
[0, 1.0],
])
self.assertTrue(np.all(np.abs(D_g - D_g_known) < 1e-12))
self.assertTrue(np.all(np.abs(CC - CC_known) < 1e-12))
def test_cart_3d(self):
g = pp.CartGrid([1, 1, 1], physdims=[2, 2, 2])
g.compute_geometry()
sc_top = pp.fvutils.SubcellTopology(g)
D_g, CC = pp.Mpsa("")._reconstruct_displacement(g, sc_top, eta=1)
data = np.array([
-1.0,
-1.0,
-1.0,
-1.0,
-1.0,
-1.0,
-1.0,
-1.0,
-1.0,
1.0,
-1.0,
-1.0,
1.0,
-1.0,
-1.0,
1.0,
-1.0,
-1.0,
-1.0,
1.0,
-1.0,
-1.0,
1.0,
-1.0,
-1.0,
1.0,
-1.0,
1.0,
1.0,
-1.0,
1.0,
1.0,
-1.0,
1.0,
1.0,
-1.0,
-1.0,
-1.0,
1.0,
-1.0,
-1.0,
1.0,
-1.0,
-1.0,
1.0,
1.0,
-1.0,
1.0,
1.0,
-1.0,
1.0,
1.0,
-1.0,
1.0,
-1.0,
1.0,
1.0,
-1.0,
1.0,
1.0,
-1.0,
1.0,
1.0,
1.0,
1.0,
1.0,
1.0,
1.0,
1.0,
1.0,
1.0,
1.0,
])
indices = np.array([
0,
24,
48,
1,
25,
49,
2,
26,
50,
12,
33,
51,
13,
34,
52,
14,
35,
53,
3,
36,
57,
4,
37,
58,
5,
38,
59,
15,
45,
54,
16,
46,
55,
17,
47,
56,
9,
27,
60,
10,
28,
61,
11,
29,
62,
21,
30,
63,
22,
31,
64,
23,
32,
65,
6,
39,
69,
7,
40,
70,
8,
41,
71,
18,
42,
66,
19,
43,
67,
20,
44,
68,
])
indptr = np.array([
0,
1,
2,
3,
4,
5,
6,
7,
8,
9,
10,
11,
12,
13,
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27,
28,
29,
30,
31,
32,
33,
34,
35,
36,
37,
38,
39,
40,
41,
42,
43,
44,
45,
46,
47,
48,
49,
50,
51,
52,
53,
54,
55,
56,
57,
58,
59,
60,
61,
62,
63,
64,
65,
66,
67,
68,
69,
70,
71,
72,
])
CC_known = np.array([
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
[1.0, 0.0, 0.0],
[0.0, 1.0, 0.0],
[0.0, 0.0, 1.0],
])
D_g_known = sps.csc_matrix((data, indices, indptr))
self.assertTrue(np.all(np.abs(D_g - D_g_known).A < 1e-12))
self.assertTrue(np.all(np.abs(CC - CC_known) < 1e-12))
def set_parameters(self, g, data_node, mg, data_edge):
"""
Set the parameters for the simulation. The stress is given in GPa.
"""
# Define the finite volume sub grid
s_t = pp.fvutils.SubcellTopology(g)
# Rock parameters
rock = pp.Granite()
lam = rock.LAMBDA * np.ones(g.num_cells) / self.pressure_scale
mu = rock.MU * np.ones(g.num_cells) / self.pressure_scale
k = pp.FourthOrderTensor(g.dim, mu, lam)
F = self._friction_coefficient(g, mg, data_edge, s_t)
# Define boundary regions
east = g.face_centers[0] > np.max(g.nodes[0]) - 1e-9
west = g.face_centers[0] < np.min(g.nodes[0]) + 1e-9
north = g.face_centers[1] > np.max(g.nodes[1]) - 1e-9
south = g.face_centers[1] < np.min(g.nodes[1]) + 1e-9
top = g.face_centers[2] > np.max(g.nodes[2]) - 1e-9
bot = g.face_centers[2] < np.min(g.nodes[2]) + 1e-9
top_hf = top[s_t.fno_unique]
bot_hf = bot[s_t.fno_unique]
# define boundary condition
bc = pp.BoundaryConditionVectorial(g)
bc.is_dir[0, east] = True # Rolling
bc.is_dir[0, west] = True # Rolling
bc.is_dir[1, north] = True # Rolling
bc.is_dir[1, south] = True # Rolling
bc.is_dir[:, bot] = True # Dirichlet
bc.is_neu[bc.is_dir + bc.is_rob] = False
# extract boundary condition to subcells
bc = pp.fvutils.boundary_to_sub_boundary(bc, s_t)
# Give boundary condition values
A = g.face_areas[s_t.fno_unique][top_hf] / 3 #* pp.length_scale**g.dim
u_bc = np.zeros((g.dim, s_t.num_subfno_unique))
u_bc[2, top_hf] = -4.5 * pp.MEGA * pp.PASCAL / self.pressure_scale * A
# Find the continuity points
eta = 1 / 3
eta_vec = eta * np.ones(s_t.num_subfno_unique)
cont_pnt = g.face_centers[:g.dim, s_t.fno_unique] + eta_vec * (
g.nodes[:g.dim, s_t.nno_unique] -
g.face_centers[:g.dim, s_t.fno_unique])
# collect parameters in dictionary
key = 'mech'
key_m = 'mech'
data_node = pp.initialize_data(
g, data_node, key, {
'bc': bc,
'bc_values': u_bc.ravel('F'),
'source': 0,
'fourth_order_tensor': k,
'mpsa_eta': eta_vec,
'cont_pnt': cont_pnt,
'rock': rock,
})
pp.initialize_data(
mg, data_edge, key_m, {
'friction_coeff': F,
'c': 100 * pp.GIGA * pp.PASCAL / self.pressure_scale
})
# Define discretization
# Solve linear elasticity with mpsa
mpsa = pp.Mpsa(key)
data_node[pp.PRIMARY_VARIABLES] = {'u': {'cells': g.dim}}
data_node[pp.DISCRETIZATION] = {'u': {'mpsa': mpsa}}
# Add a Robin condition to the mortar grid
contact = pp.numerics.interface_laws.elliptic_interface_laws.RobinContact(
key_m, mpsa)
data_edge[pp.PRIMARY_VARIABLES] = {'lam': {'cells': g.dim}}
data_edge[pp.COUPLING_DISCRETIZATION] = {
'robin_disc': {
g: ('u', 'mpsa'),
g: ('u', 'mpsa'),
(g, g): ('lam', contact),
}
}
return key, key_m
def test_simplex_2d(self):
nx = 1
ny = 1
g = pp.StructuredTriangleGrid([nx, ny], physdims=[1, 1])
g.compute_geometry()
g = make_true_2d(g)
sc_top = pp.fvutils.SubcellTopology(g)
D_g, CC = pp.Mpsa("")._reconstruct_displacement(g, sc_top, eta=0)
D_g_known = np.array([
[
-1 / 6,
-1 / 3,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
-1 / 6,
-1 / 3,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
-1 / 6,
-1 / 3,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1 / 6,
-1 / 3,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1 / 3,
-1 / 6,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1 / 3,
-1 / 6,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1 / 3,
-1 / 6,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1 / 3,
-1 / 6,
0.0,
0.0,
0.0,
0.0,
],
[
-1 / 12,
1 / 12,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 12,
-1 / 12,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
-1 / 12,
1 / 12,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 12,
-1 / 12,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1 / 12,
1 / 12,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 12,
-1 / 12,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
-1 / 12,
1 / 12,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 12,
-1 / 12,
],
[
0.0,
0.0,
0.0,
0.0,
1 / 3,
1 / 6,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 3,
1 / 6,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 3,
1 / 6,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 3,
1 / 6,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 6,
1 / 3,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 6,
1 / 3,
0.0,
0.0,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 6,
1 / 3,
0.0,
0.0,
],
[
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
0.0,
1 / 6,
1 / 3,
],
])
CC_known = np.array([
[1.0, 0.0, 0.0, 0.0],
[0.0, 1.0, 0.0, 0.0],
[1.0, 0.0, 0.0, 0.0],
[0.0, 1.0, 0.0, 0.0],
[0.0, 0.0, 1.0, 0.0],
[0.0, 0.0, 0.0, 1.0],
[0.0, 0.0, 1.0, 0.0],
[0.0, 0.0, 0.0, 1.0],
[0.5, 0.0, 0.5, 0.0],
[0.0, 0.5, 0.0, 0.5],
[0.5, 0.0, 0.5, 0.0],
[0.0, 0.5, 0.0, 0.5],
[1.0, 0.0, 0.0, 0.0],
[0.0, 1.0, 0.0, 0.0],
[1.0, 0.0, 0.0, 0.0],
[0.0, 1.0, 0.0, 0.0],
[0.0, 0.0, 1.0, 0.0],
[0.0, 0.0, 0.0, 1.0],
[0.0, 0.0, 1.0, 0.0],
[0.0, 0.0, 0.0, 1.0],
])
self.assertTrue(np.all(np.abs(D_g - D_g_known).A < 1e-12))
self.assertTrue(np.all(np.abs(CC - CC_known) < 1e-12))
def set_parameters(self, g, data_node, mg, data_edge):
"""
Set the parameters for the simulation. The stress is given in GPa.
"""
# First set the parameters used in the pure elastic simulation
key_m, key_c = super().set_parameters(g, data_node, mg, data_edge)
key_f = 'flow'
if not key_m == key_c:
raise ValueError('Mechanics keyword must equal contact keyword')
self.key_m = key_m
self.key_f = key_f
# Set fluid parameters
kxx = self.k * np.ones(g.num_cells) / self.length_scale**2
viscosity = self.viscosity / self.pressure_scale
K = pp.SecondOrderTensor(g.dim, kxx / viscosity)
# Define Biot parameters
alpha = 1
dt = self.end_time / 20
# Define the finite volume sub grid
s_t = pp.fvutils.SubcellTopology(g)
# Define boundary conditions for flow
top = g.face_centers[2] > np.max(g.nodes[2]) - 1e-9
bot = g.face_centers[2] < np.min(g.nodes[2]) + 1e-9
east = g.face_centers[0] > np.max(g.nodes[0]) - 1e-9
bc_flow = pp.BoundaryCondition(g, top, 'dir')
bc_flow = pp.fvutils.boundary_to_sub_boundary(bc_flow, s_t)
# Set boundary condition values.
p_bc = self.bc_values(g, dt, key_f)
# Set initial solution
u0 = np.zeros(g.dim * g.num_cells)
p0 = np.zeros(g.num_cells)
lam_u0 = np.zeros(g.dim * mg.num_cells)
u_bc0 = self.bc_values(g, 0, key_m)
u_bc = self.bc_values(g, dt, key_m)
# Collect parameters in dictionaries
# Add biot parameters to mechanics
data_node[pp.PARAMETERS][key_m]['biot_alpha'] = alpha
data_node[pp.PARAMETERS][key_m]['time_step'] = dt
data_node[pp.PARAMETERS][key_m]['bc_values'] = u_bc
data_node[pp.PARAMETERS][key_m]['state'] = {
'displacement': u0,
'bc_values': u_bc0
}
data_edge[pp.PARAMETERS][key_c]['state'] = lam_u0
# Add fluid flow dictionary
data_node = pp.initialize_data(
g, data_node, key_f, {
'bc': bc_flow,
'bc_values': p_bc.ravel('F'),
'second_order_tensor': K,
'mass_weight': self.S,
'aperture': np.ones(g.num_cells),
'biot_alpha': alpha,
'time_step': dt,
'state': p0,
})
# Define discretization.
# For the domain we solve linear elasticity with mpsa and fluid flow with mpfa.
# In addition we add a storage term (ImplicitMassMatrix) to the fluid mass balance.
# The coupling terms are:
# BiotStabilization, pressure contribution to the div u term.
# GrapP, pressure contribution to stress equation.
# div_u, displacement contribution to div u term.
data_node[pp.PRIMARY_VARIABLES] = {
"u": {
"cells": g.dim
},
"p": {
"cells": 1
}
}
mpfa_disc = discretizations.ImplicitMpfa(key_f)
data_node[pp.DISCRETIZATION] = {
"u": {
"div_sigma": pp.Mpsa(key_m)
},
"p": {
"flux": mpfa_disc,
"mass": discretizations.ImplicitMassMatrix(key_f),
"stab": pp.BiotStabilization(key_f),
},
"u_p": {
"grad_p": pp.GradP(key_m)
},
"p_u": {
"div_u": pp.DivD(key_m)
},
}
# On the mortar grid we define two variables and sets of equations. The first
# adds a Robin condition to the elasticity equation. The second enforces full
# fluid pressure and flux continuity over the fractures. We also have to be
# carefull to obtain the contribution of the coupling discretizations gradP on
# the Robin contact condition, and the contribution from the mechanical mortar
# variable on the div_u term.
# Contribution from fluid pressure on displacement jump at fractures
gradP_disp = pp.numerics.interface_laws.elliptic_interface_laws.RobinContactBiotPressure(
key_m, pp.numerics.fv.biot.GradP(key_m))
# Contribution from mechanics mortar on div_u term
div_u_lam = pp.numerics.interface_laws.elliptic_interface_laws.DivU_StressMortar(
key_m, pp.numerics.fv.biot.DivD(key_m))
# gradP_disp and pp.RobinContact will now give the correct Robin contact
# condition.
# div_u (from above) and div_u_lam will now give the correct div u term in the
# fluid mass balance
data_edge[pp.PRIMARY_VARIABLES] = {"lam_u": {"cells": g.dim}}
data_edge[pp.COUPLING_DISCRETIZATION] = {
"robin_discretization": {
g: ("u", "div_sigma"),
g: ("u", "div_sigma"),
(g, g): ("lam_u", pp.RobinContact(key_m, pp.Mpsa(key_m))),
},
"p_contribution_to_displacement": {
g: ("p", "flux"
), # "flux" should be "grad_p", but the assembler does not
g: ("p", "flux"
), # support this. However, in FV this is not used anyway.
(g, g): ("lam_u", gradP_disp),
},
"lam_u_contr_2_div_u": {
g: ("p", "flux"), # "flux" -> "div_u"
g: ("p", "flux"),
(g, g): ("lam_u", div_u_lam),
},
}
# Discretize with biot
pp.Biot(key_m, key_f).discretize(g, data_node)
return key_m, key_f
def test_assemble_biot(self):
""" Test the assembly of the Biot problem using the assembler.
The test checks whether the discretization matches that of the Biot class.
"""
gb = pp.meshing.cart_grid([], [2, 1])
g = gb.grids_of_dimension(2)[0]
d = gb.node_props(g)
# Parameters identified by two keywords
kw_m = "mechanics"
kw_f = "flow"
variable_m = "displacement"
variable_f = "pressure"
bound_mech, bound_flow = self.make_boundary_conditions(g)
initial_disp, initial_pressure, initial_state = self.make_initial_conditions(
g, x0=0, y0=0, p0=0)
state = {
variable_f: initial_pressure,
variable_m: initial_disp,
kw_m: {
"bc_values": np.zeros(g.num_faces * g.dim)
},
}
parameters_m = {"bc": bound_mech, "biot_alpha": 1}
parameters_f = {"bc": bound_flow, "biot_alpha": 1}
pp.initialize_default_data(g, d, kw_m, parameters_m)
pp.initialize_default_data(g, d, kw_f, parameters_f)
pp.set_state(d, state)
# Discretize the mechanics related terms using the Biot class
biot_discretizer = pp.Biot()
biot_discretizer._discretize_mech(g, d)
# Set up the structure for the assembler. First define variables and equation
# term names.
v_0 = variable_m
v_1 = variable_f
term_00 = "stress_divergence"
term_01 = "pressure_gradient"
term_10 = "displacement_divergence"
term_11_0 = "fluid_mass"
term_11_1 = "fluid_flux"
term_11_2 = "stabilization"
d[pp.PRIMARY_VARIABLES] = {v_0: {"cells": g.dim}, v_1: {"cells": 1}}
d[pp.DISCRETIZATION] = {
v_0: {
term_00: pp.Mpsa(kw_m)
},
v_1: {
term_11_0: pp.MassMatrix(kw_f),
term_11_1: pp.Mpfa(kw_f),
term_11_2: pp.BiotStabilization(kw_f),
},
v_0 + "_" + v_1: {
term_01: pp.GradP(kw_m)
},
v_1 + "_" + v_0: {
term_10: pp.DivU(kw_m)
},
}
# Assemble. Also discretizes the flow terms (fluid_mass and fluid_flux)
general_assembler = pp.Assembler(gb)
general_assembler.discretize(term_filter=["fluid_mass", "fluid_flux"])
A, b = general_assembler.assemble_matrix_rhs()
# Re-discretize and assemble using the Biot class
A_class, b_class = biot_discretizer.matrix_rhs(g, d, discretize=False)
# Make sure the variable ordering of the matrix assembled by the assembler
# matches that of the Biot class.
grids = [g, g]
variables = [v_0, v_1]
A, b = permute_matrix_vector(
A,
b,
general_assembler.block_dof,
general_assembler.full_dof,
grids,
variables,
)
# Compare the matrices and rhs vectors
self.assertTrue(np.all(np.isclose(A.A, A_class.A)))
self.assertTrue(np.all(np.isclose(b, b_class)))
def test_cart_3d(self):
g = pp.CartGrid([1, 1, 1])
g.compute_geometry()
bot = g.face_centers[2] < 1e-10
top = g.face_centers[2] > 1 - 1e-10
south = g.face_centers[1] < 1e-10
north = g.face_centers[1] > 1 - 1e-10
west = g.face_centers[0] < 1e-10
east = g.face_centers[0] > 1 - 1e-10
is_dir = south + top
is_neu = east + west
is_rob = north + bot
bnd = pp.BoundaryConditionVectorial(g)
bnd.is_neu[:] = False
bnd.is_dir[:, is_dir] = True
bnd.is_rob[:, is_rob] = True
bnd.is_neu[:, is_neu] = True
sc_top = pp.fvutils.SubcellTopology(g)
bnd = pp.fvutils.boundary_to_sub_boundary(bnd, sc_top)
bnd_excl = pp.fvutils.ExcludeBoundaries(sc_top, bnd, g.dim)
rhs = pp.Mpsa("")._create_bound_rhs(bnd, bnd_excl, sc_top, g, True)
hf2f = pp.fvutils.map_hf_2_f(sc_top.fno_unique, sc_top.subfno_unique,
g.dim)
rhs = rhs * hf2f.T
rhs_indptr = np.array(
[
0,
1,
2,
3,
4,
5,
6,
7,
8,
9,
10,
11,
12,
13,
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27,
28,
29,
30,
31,
32,
33,
34,
35,
36,
37,
38,
39,
40,
41,
42,
43,
44,
45,
46,
47,
48,
49,
50,
51,
52,
53,
54,
55,
56,
57,
58,
59,
60,
61,
62,
63,
64,
65,
66,
67,
68,
69,
70,
71,
72,
],
dtype=np.int32,
)
rhs_indices = np.array(
[
0,
0,
0,
0,
3,
3,
3,
3,
1,
1,
1,
1,
4,
4,
4,
4,
2,
2,
2,
2,
5,
5,
5,
5,
9,
9,
9,
9,
12,
12,
12,
12,
10,
10,
10,
10,
13,
13,
13,
13,
11,
11,
11,
11,
14,
14,
14,
14,
6,
6,
6,
6,
15,
15,
15,
15,
7,
7,
7,
7,
16,
16,
16,
16,
8,
8,
8,
8,
17,
17,
17,
17,
],
dtype=np.int32,
)
rhs_data = np.array([
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
1,
-1.0,
-1.0,
-1.0,
-1.0,
1.0,
1.0,
1.0,
1.0,
-1.0,
-1.0,
-1.0,
-1.0,
1.0,
1.0,
1.0,
1.0,
-1.0,
-1.0,
-1.0,
-1.0,
1.0,
1.0,
1.0,
1.0,
])
rhs_known = sps.csr_matrix((rhs_data, rhs_indices, rhs_indptr),
shape=(72, 18))
self.assertTrue(np.all(np.abs((rhs_known - rhs).data) < 1e-12))
def test_mixed_condition(self):
nx = 2
ny = 1
g = pp.CartGrid([nx, ny], physdims=[1, 1])
g.compute_geometry()
bot = g.face_centers[1] < 1e-10
top = g.face_centers[1] > 1 - 1e-10
left = g.face_centers[0] < 1e-10
right = g.face_centers[0] > 1 - 1e-10
bnd = pp.BoundaryConditionVectorial(g)
bnd.is_neu[:] = False
bnd.is_dir[0, left] = True
bnd.is_neu[1, left] = True
bnd.is_rob[0, right] = True
bnd.is_dir[1, right] = True
bnd.is_neu[0, bot] = True
bnd.is_rob[1, bot] = True
bnd.is_rob[0, top] = True
bnd.is_dir[1, top] = True
sc_top = pp.fvutils.SubcellTopology(g)
bnd = pp.fvutils.boundary_to_sub_boundary(bnd, sc_top)
bnd_excl = pp.fvutils.ExcludeBoundaries(sc_top, bnd, g.dim)
rhs = pp.Mpsa("")._create_bound_rhs(bnd, bnd_excl, sc_top, g, True)
hf2f = pp.fvutils.map_hf_2_f(sc_top.fno_unique, sc_top.subfno_unique,
g.dim)
rhs = rhs * hf2f.T
rhs_known = np.array([
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
1.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
1.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0,
0.0, 0.0
],
[
-1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
-1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 1.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 1.0,
0.0, 0.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 1.0
],
[
0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 1.0
],
])
self.assertTrue(np.all(np.abs(rhs_known - rhs) < 1e-12))
def discretize(
grid_bucket,
data_dictionary,
parameter_keyword_flow,
parameter_keyword_mechanics,
variable_flow,
variable_mechanics,
):
"""
Discretize the problem.
Parameters:
grid_bucket (PorePy object): Grid bucket
data_dictionary (Dict): Model's data dictionary
parameter_keyword_flow (String): Keyword for the flow parameter
parameter_keyword_mechanics (String): Keyword for the mechanics parameter
variable_flow (String): Primary variable of the flow problem
variable_mechanics (String): Primary variable of the mechanics problem
Output:
assembler (PorePy object): Assembler containing discretization
"""
# The Mpfa discretization assumes unit viscosity. Hence we need to
# overwrite the class to include it.
class ImplicitMpfa(pp.Mpfa):
def assemble_matrix_rhs(self, g, d):
"""
Overwrite MPFA method to be consistent with Biot's
time discretization and inclusion of viscosity in Darcy's law
"""
viscosity = d[pp.PARAMETERS][self.keyword]["viscosity"]
a, b = super().assemble_matrix_rhs(g, d)
dt = d[pp.PARAMETERS][self.keyword]["time_step"]
return a * (1 / viscosity) * dt, b * (1 / viscosity) * dt
# Redefining input parameters
gb = grid_bucket
g = gb.grids_of_dimension(2)[0]
d = data_dictionary
kw_f = parameter_keyword_flow
kw_m = parameter_keyword_mechanics
v_0 = variable_mechanics
v_1 = variable_flow
# Discretize the subproblems using Biot's class, which employs
# MPSA for the mechanics problem and MPFA for the flow problem
biot_discretizer = pp.Biot(kw_m, kw_f, v_0, v_1)
biot_discretizer._discretize_mech(g, d) # discretize mech problem
biot_discretizer._discretize_flow(g, d) # discretize flow problem
# Names of the five terms of the equation + additional stabilization term.
####################################### Term in the Biot equation:
term_00 = "stress_divergence" ######## div symmetric grad u
term_01 = "pressure_gradient" ######## alpha grad p
term_10 = "displacement_divergence" ## d/dt alpha div u
term_11_0 = "fluid_mass" ############# d/dt beta p
term_11_1 = "fluid_flux" ############# div (rho g - K grad p)
term_11_2 = "stabilization" ##########
# Store in the data dictionary and specify discretization objects.
d[pp.PRIMARY_VARIABLES] = {v_0: {"cells": g.dim}, v_1: {"cells": 1}}
d[pp.DISCRETIZATION] = {
v_0: {
term_00: pp.Mpsa(kw_m)
},
v_1: {
term_11_0: ImplicitMassMatrix(kw_f, v_1),
term_11_1: ImplicitMpfa(kw_f),
term_11_2: pp.BiotStabilization(kw_f, v_1),
},
v_0 + "_" + v_1: {
term_01: pp.GradP(kw_m)
},
v_1 + "_" + v_0: {
term_10: pp.DivU(kw_m, kw_f, v_0)
},
}
assembler = pp.Assembler(gb)
# Discretize the flow and accumulation terms - the other are already handled
# by the biot_discretizer
assembler.discretize(term_filter=[term_11_0, term_11_1])
return assembler
gb = pp.meshing.cart_grid(frac, [9, 3])
split_scheme = [[np.array([1]), np.array([8])], [np.array([49]), np.array([55])]]
return gb, split_scheme
# The main test function
@pytest.mark.parametrize(
"geometry",
[
_two_fractures_overlapping_regions,
_two_fractures_non_overlapping_regions,
_two_fractures_regions_become_overlapping,
],
)
@pytest.mark.parametrize(
"method", [pp.Mpfa("flow"), pp.Mpsa("mechanics"), pp.Biot("mechanics", "flow")]
)
def test_propagation(geometry, method):
# Method to test partial discretization (aimed at finite volume methods) under
# fracture propagation. The test is based on first discretizing, and then do one
# or several fracture propagation steps. after each step, we do a partial
# update of the discretization scheme, and compare with a full discretization on
# the newly split grid. The test fails unless all discretization matrices generated
# are identical.
#
# NOTE: Only the highest-dimensional grid in the GridBucket is used.
# Get GridBucket and splitting schedule
gb, faces_to_split = geometry()
g = gb.grids_of_dimension(gb.dim_max())[0]
def assign_discretisations(self):
"""
Assign discretizations to the nodes and edges of the grid bucket.
Note the attribute subtract_fracture_pressure: Indicates whether or not to
subtract the fracture pressure contribution for the contact traction. This
should not be done if the scalar variable is temperature.
"""
# Shorthand
key_s, key_m = self.scalar_parameter_key, self.mechanics_parameter_key
var_s, var_d = self.scalar_variable, self.displacement_variable
# Define discretization
# For the Nd domain we solve linear elasticity with mpsa.
mpsa = pp.Mpsa(key_m)
empty_discr = pp.VoidDiscretization(key_m, ndof_cell=self.Nd)
# Scalar discretizations (all dimensions)
diff_disc_s = IE_discretizations.ImplicitMpfa(key_s)
mass_disc_s = IE_discretizations.ImplicitMassMatrix(key_s, var_s)
source_disc_s = pp.ScalarSource(key_s)
# Coupling discretizations
# All dimensions
div_u_disc = pp.DivU(
key_m,
key_s,
variable=var_d,
mortar_variable=self.mortar_displacement_variable,
)
# Nd
grad_p_disc = pp.GradP(key_m)
stabilization_disc_s = pp.BiotStabilization(key_s, var_s)
# Assign node discretizations
for g, d in self.gb:
if g.dim == self.Nd:
d[pp.DISCRETIZATION] = {
var_d: {
"mpsa": mpsa
},
var_s: {
"diffusion": diff_disc_s,
"mass": mass_disc_s,
"stabilization": stabilization_disc_s,
"source": source_disc_s,
},
var_d + "_" + var_s: {
"grad_p": grad_p_disc
},
var_s + "_" + var_d: {
"div_u": div_u_disc
},
}
elif g.dim == self.Nd - 1:
d[pp.DISCRETIZATION] = {
self.contact_traction_variable: {
"empty": empty_discr
},
var_s: {
"diffusion": diff_disc_s,
"mass": mass_disc_s,
"source": source_disc_s,
},
}
# Define edge discretizations for the mortar grid
contact_law = pp.ColoumbContact(self.mechanics_parameter_key, self.Nd)
contact_discr = pp.PrimalContactCoupling(self.mechanics_parameter_key,
mpsa, contact_law)
# Account for the mortar displacements effect on scalar balance in the matrix,
# as an internal boundary contribution, fracture, aperture changes appear as a
# source contribution.
div_u_coupling = pp.DivUCoupling(self.displacement_variable,
div_u_disc, div_u_disc)
# Account for the pressure contributions to the force balance on the fracture
# (see contact_discr).
# This discretization needs the keyword used to store the grad p discretization:
grad_p_key = key_m
matrix_scalar_to_force_balance = pp.MatrixScalarToForceBalance(
grad_p_key, mass_disc_s, mass_disc_s)
if self.subtract_fracture_pressure:
fracture_scalar_to_force_balance = pp.FractureScalarToForceBalance(
mass_disc_s, mass_disc_s)
for e, d in self.gb.edges():
g_l, g_h = self.gb.nodes_of_edge(e)
if g_h.dim == self.Nd:
d[pp.COUPLING_DISCRETIZATION] = {
self.friction_coupling_term: {
g_h: (var_d, "mpsa"),
g_l: (self.contact_traction_variable, "empty"),
(g_h, g_l):
(self.mortar_displacement_variable, contact_discr),
},
self.scalar_coupling_term: {
g_h: (var_s, "diffusion"),
g_l: (var_s, "diffusion"),
e: (
self.mortar_scalar_variable,
pp.RobinCoupling(key_s, diff_disc_s),
),
},
"div_u_coupling": {
g_h: (
var_s,
"mass",
), # This is really the div_u, but this is not implemented
g_l: (var_s, "mass"),
e: (self.mortar_displacement_variable, div_u_coupling),
},
"matrix_scalar_to_force_balance": {
g_h: (var_s, "mass"),
g_l: (var_s, "mass"),
e: (
self.mortar_displacement_variable,
matrix_scalar_to_force_balance,
),
},
}
if self.subtract_fracture_pressure:
d[pp.COUPLING_DISCRETIZATION].update({
"matrix_scalar_to_force_balance": {
g_h: (var_s, "mass"),
g_l: (var_s, "mass"),
e: (
self.mortar_displacement_variable,
fracture_scalar_to_force_balance,
),
}
})
else:
raise ValueError(
"assign_discretizations assumes no fracture intersections."
)
def test_one_cell_a_time_node_keyword(self):
# Update one and one cell, and verify that the result is the same as
# with a single computation. The test is similar to what will happen
# with a memory-constrained splitting.
g = pp.CartGrid([3, 3])
g.compute_geometry()
# Assign random permeabilities, for good measure
np.random.seed(42)
mu = np.random.random(g.num_cells)
lmbda = np.random.random(g.num_cells)
stiffness = pp.FourthOrderTensor(mu=mu, lmbda=lmbda)
stress = sps.csr_matrix((g.num_faces * g.dim, g.num_cells * g.dim))
bound_stress = sps.csr_matrix(
(g.num_faces * g.dim, g.num_faces * g.dim))
faces_covered = np.zeros(g.num_faces, np.bool)
bnd = pp.BoundaryConditionVectorial(g)
specified_data = {
"fourth_order_tensor": stiffness,
"bc": bnd,
"inverter": "python",
}
keyword = "mechanics"
data = pp.initialize_default_data(g, {},
keyword,
specified_parameters=specified_data)
discr = pp.Mpsa(keyword)
discr.discretize(g, data)
stress_full = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.stress_matrix_key]
bound_stress_full = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.bound_stress_matrix_key]
cn = g.cell_nodes()
for ci in range(g.num_cells):
ind = np.zeros(g.num_cells)
ind[ci] = 1
nodes = np.squeeze(np.where(cn * ind > 0))
data[pp.PARAMETERS][keyword]["specified_nodes"] = nodes
discr.discretize(g, data)
partial_stress = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.stress_matrix_key]
partial_bound = data[pp.DISCRETIZATION_MATRICES][keyword][
discr.bound_stress_matrix_key]
active_faces = data[pp.PARAMETERS][keyword]["active_faces"]
if np.any(faces_covered):
del_faces = self.expand_indices_nd(
np.where(faces_covered)[0], g.dim)
# del_faces is already expanded, set dimension to 1
pp.fvutils.remove_nonlocal_contribution(
del_faces, 1, partial_stress, partial_bound)
faces_covered[active_faces] = True
stress += partial_stress
bound_stress += partial_bound
self.assertTrue((stress_full - stress).max() < 1e-8)
self.assertTrue((stress_full - stress).min() > -1e-8)
self.assertTrue((bound_stress - bound_stress_full).max() < 1e-8)
self.assertTrue((bound_stress - bound_stress_full).min() > -1e-8)
return gb, split_scheme
# The main test function
@pytest.mark.parametrize(
"geometry",
[
_two_fractures_overlapping_regions,
_two_fractures_non_overlapping_regions,
_two_fractures_regions_become_overlapping,
],
)
@pytest.mark.parametrize(
"method",
[pp.Mpfa("flow"),
pp.Mpsa("mechanics"),
pp.Biot("mechanics", "flow")])
def test_propagation(geometry, method):
# Method to test partial discretization (aimed at finite volume methods) under
# fracture propagation. The test is based on first discretizing, and then do one
# or several fracture propagation steps. after each step, we do a partial
# update of the discretization scheme, and compare with a full discretization on
# the newly split grid. The test fails unless all discretization matrices generated
# are identical.
#
# NOTE: Only the highest-dimensional grid in the GridBucket is used.
# Get GridBucket and splitting schedule
gb, faces_to_split = geometry()
g = gb.grids_of_dimension(gb.dim_max())[0]
def _assign_discretizations(self) -> None:
"""
Assign discretizations to the nodes and edges of the grid bucket.
Note the attribute subtract_fracture_pressure: Indicates whether or not to
subtract the fracture pressure contribution for the contact traction. This
should not be done if the scalar variable is temperature.
"""
if not self._use_ad:
# Shorthand
key_s, key_m = self.scalar_parameter_key, self.mechanics_parameter_key
var_s, var_d = self.scalar_variable, self.displacement_variable
# Define discretization
# For the Nd domain we solve linear elasticity with mpsa.
mpsa = pp.Mpsa(key_m)
empty_discr = pp.VoidDiscretization(key_m, ndof_cell=self._Nd)
# Scalar discretizations (all dimensions)
diff_disc_s = IE_discretizations.ImplicitMpfa(key_s)
mass_disc_s = IE_discretizations.ImplicitMassMatrix(key_s, var_s)
source_disc_s = pp.ScalarSource(key_s)
# Coupling discretizations
# All dimensions
div_u_disc = pp.DivU(
key_m,
key_s,
variable=var_d,
mortar_variable=self.mortar_displacement_variable,
)
# Nd
grad_p_disc = pp.GradP(key_m)
stabilization_disc_s = pp.BiotStabilization(key_s, var_s)
# Assign node discretizations
for g, d in self.gb:
if g.dim == self._Nd:
d[pp.DISCRETIZATION] = {
var_d: {"mpsa": mpsa},
var_s: {
"diffusion": diff_disc_s,
"mass": mass_disc_s,
"stabilization": stabilization_disc_s,
"source": source_disc_s,
},
var_d + "_" + var_s: {"grad_p": grad_p_disc},
var_s + "_" + var_d: {"div_u": div_u_disc},
}
elif g.dim == self._Nd - 1:
d[pp.DISCRETIZATION] = {
self.contact_traction_variable: {"empty": empty_discr},
var_s: {
"diffusion": diff_disc_s,
"mass": mass_disc_s,
"source": source_disc_s,
},
}
else:
d[pp.DISCRETIZATION] = {
var_s: {
"diffusion": diff_disc_s,
"mass": mass_disc_s,
"source": source_disc_s,
}
}
# Define edge discretizations for the mortar grid
contact_law = pp.ColoumbContact(
self.mechanics_parameter_key, self._Nd, mpsa
)
contact_discr = pp.PrimalContactCoupling(
self.mechanics_parameter_key, mpsa, contact_law
)
# Account for the mortar displacements effect on scalar balance in the matrix,
# as an internal boundary contribution, fracture, aperture changes appear as a
# source contribution.
div_u_coupling = pp.DivUCoupling(
self.displacement_variable, div_u_disc, div_u_disc
)
# Account for the pressure contributions to the force balance on the fracture
# (see contact_discr).
# This discretization needs the keyword used to store the grad p discretization:
grad_p_key = key_m
matrix_scalar_to_force_balance = pp.MatrixScalarToForceBalance(
grad_p_key, mass_disc_s, mass_disc_s
)
if self.subtract_fracture_pressure:
fracture_scalar_to_force_balance = pp.FractureScalarToForceBalance(
mass_disc_s, mass_disc_s
)
for e, d in self.gb.edges():
g_l, g_h = self.gb.nodes_of_edge(e)
if g_h.dim == self._Nd:
d[pp.COUPLING_DISCRETIZATION] = {
self.friction_coupling_term: {
g_h: (var_d, "mpsa"),
g_l: (self.contact_traction_variable, "empty"),
(g_h, g_l): (
self.mortar_displacement_variable,
contact_discr,
),
},
self.scalar_coupling_term: {
g_h: (var_s, "diffusion"),
g_l: (var_s, "diffusion"),
e: (
self.mortar_scalar_variable,
pp.RobinCoupling(key_s, diff_disc_s),
),
},
"div_u_coupling": {
g_h: (
var_s,
"mass",
), # This is really the div_u, but this is not implemented
g_l: (var_s, "mass"),
e: (self.mortar_displacement_variable, div_u_coupling),
},
"matrix_scalar_to_force_balance": {
g_h: (var_s, "mass"),
g_l: (var_s, "mass"),
e: (
self.mortar_displacement_variable,
matrix_scalar_to_force_balance,
),
},
}
if self.subtract_fracture_pressure:
d[pp.COUPLING_DISCRETIZATION].update(
{
"fracture_scalar_to_force_balance": {
g_h: (var_s, "mass"),
g_l: (var_s, "mass"),
e: (
self.mortar_displacement_variable,
fracture_scalar_to_force_balance,
),
}
}
)
else:
d[pp.COUPLING_DISCRETIZATION] = {
self.scalar_coupling_term: {
g_h: (var_s, "diffusion"),
g_l: (var_s, "diffusion"),
e: (
self.mortar_scalar_variable,
pp.RobinCoupling(key_s, diff_disc_s),
),
}
}
else:
gb = self.gb
Nd = self._Nd
dof_manager = pp.DofManager(gb)
eq_manager = pp.ad.EquationManager(gb, dof_manager)
g_primary = gb.grids_of_dimension(Nd)[0]
g_frac = gb.grids_of_dimension(Nd - 1).tolist()
grid_list = [
g_primary,
*g_frac,
*gb.grids_of_dimension(Nd - 2),
*gb.grids_of_dimension(Nd - 3),
]
if len(gb.grids_of_dimension(Nd)) != 1:
raise NotImplementedError("This will require further work")
edge_list_highest = [(g_primary, g) for g in g_frac]
edge_list = [e for e, _ in gb.edges()]
mortar_proj_scalar = pp.ad.MortarProjections(edges=edge_list, gb=gb, nd=1)
mortar_proj_vector = pp.ad.MortarProjections(
edges=edge_list_highest, gb=gb, nd=self._Nd
)
subdomain_proj_scalar = pp.ad.SubdomainProjections(gb=gb)
subdomain_proj_vector = pp.ad.SubdomainProjections(gb=gb, nd=self._Nd)
tangential_normal_proj_list = []
normal_proj_list = []
for gf in g_frac:
proj = gb.node_props(gf, "tangential_normal_projection")
tangential_normal_proj_list.append(
proj.project_tangential_normal(gf.num_cells)
)
normal_proj_list.append(proj.project_normal(gf.num_cells))
tangential_normal_proj = pp.ad.Matrix(
sps.block_diag(tangential_normal_proj_list)
)
normal_proj = pp.ad.Matrix(sps.block_diag(normal_proj_list))
# Ad representation of discretizations
mpsa_ad = pp.ad.BiotAd(self.mechanics_parameter_key, g_primary)
grad_p_ad = pp.ad.GradPAd(self.mechanics_parameter_key, g_primary)
mpfa_ad = pp.ad.MpfaAd(self.scalar_parameter_key, grid_list)
mass_ad = pp.ad.MassMatrixAd(self.scalar_parameter_key, grid_list)
robin_ad = pp.ad.RobinCouplingAd(self.scalar_parameter_key, edge_list)
div_u_ad = pp.ad.DivUAd(
self.mechanics_parameter_key,
grids=g_primary,
mat_dict_keyword=self.scalar_parameter_key,
)
stab_biot_ad = pp.ad.BiotStabilizationAd(
self.scalar_parameter_key, g_primary
)
coloumb_ad = pp.ad.ColoumbContactAd(
self.mechanics_parameter_key, edge_list_highest
)
bc_ad = pp.ad.BoundaryCondition(
self.mechanics_parameter_key, grids=[g_primary]
)
div_vector = pp.ad.Divergence(grids=[g_primary], dim=g_primary.dim)
# Primary variables on Ad form
u = eq_manager.variable(g_primary, self.displacement_variable)
u_mortar = eq_manager.merge_variables(
[(e, self.mortar_displacement_variable) for e in edge_list_highest]
)
contact_force = eq_manager.merge_variables(
[(g, self.contact_traction_variable) for g in g_frac]
)
p = eq_manager.merge_variables(
[(g, self.scalar_variable) for g in grid_list]
)
mortar_flux = eq_manager.merge_variables(
[(e, self.mortar_scalar_variable) for e in edge_list]
)
u_prev = u.previous_timestep()
u_mortar_prev = u_mortar.previous_timestep()
p_prev = p.previous_timestep()
# Reference pressure, corresponding to an initial stress free state
p_reference = pp.ad.ParameterArray(
param_keyword=self.mechanics_parameter_key,
array_keyword="p_reference",
grids=[g_primary],
gb=gb,
)
# Stress in g_h
stress = (
mpsa_ad.stress * u
+ mpsa_ad.bound_stress * bc_ad
+ mpsa_ad.bound_stress
* subdomain_proj_vector.face_restriction(g_primary)
* mortar_proj_vector.mortar_to_primary_avg
* u_mortar
+ grad_p_ad.grad_p
* subdomain_proj_scalar.cell_restriction(g_primary)
* p
# The reference pressure is only defined on g_primary, thus there is no need
# for a subdomain projection.
- grad_p_ad.grad_p * p_reference
)
momentum_eq = pp.ad.Expression(
div_vector * stress, dof_manager, "momentuum", grid_order=[g_primary]
)
jump = (
subdomain_proj_vector.cell_restriction(g_frac)
* mortar_proj_vector.mortar_to_secondary_avg
* mortar_proj_vector.sign_of_mortar_sides
)
jump_rotate = tangential_normal_proj * jump
# Contact conditions
num_frac_cells = np.sum([g.num_cells for g in g_frac])
jump_discr = coloumb_ad.displacement * jump_rotate * u_mortar
tmp = np.ones(num_frac_cells * self._Nd)
tmp[self._Nd - 1 :: self._Nd] = 0
exclude_normal = pp.ad.Matrix(
sps.dia_matrix((tmp, 0), shape=(tmp.size, tmp.size))
)
# Rhs of contact conditions
rhs = (
coloumb_ad.rhs
+ exclude_normal * coloumb_ad.displacement * jump_rotate * u_mortar_prev
)
contact_conditions = coloumb_ad.traction * contact_force + jump_discr - rhs
contact_eq = pp.ad.Expression(
contact_conditions, dof_manager, "contact", grid_order=g_frac
)
# Force balance
mat = None
for _, d in gb.edges():
mg: pp.MortarGrid = d["mortar_grid"]
if mg.dim < self._Nd - 1:
continue
faces_on_fracture_surface = mg.primary_to_mortar_int().tocsr().indices
m = pp.grid_utils.switch_sign_if_inwards_normal(
g_primary, self._Nd, faces_on_fracture_surface
)
if mat is None:
mat = m
else:
mat += m
sign_switcher = pp.ad.Matrix(mat)
# Contact from primary grid and mortar displacements (via primary grid)
contact_from_primary_mortar = (
mortar_proj_vector.primary_to_mortar_int
* subdomain_proj_vector.face_prolongation(g_primary)
* sign_switcher
* stress
)
contact_from_secondary = (
mortar_proj_vector.sign_of_mortar_sides
* mortar_proj_vector.secondary_to_mortar_int
* subdomain_proj_vector.cell_prolongation(g_frac)
* tangential_normal_proj.transpose()
* contact_force
)
if self.subtract_fracture_pressure:
# This gives an error because of -=
mat = []
for e in edge_list_highest:
mg = gb.edge_props(e, "mortar_grid")
faces_on_fracture_surface = (
mg.primary_to_mortar_int().tocsr().indices
)
sgn, _ = g_primary.signs_and_cells_of_boundary_faces(
faces_on_fracture_surface
)
fracture_normals = g_primary.face_normals[
: self._Nd, faces_on_fracture_surface
]
outwards_fracture_normals = sgn * fracture_normals
data = outwards_fracture_normals.ravel("F")
row = np.arange(g_primary.dim * mg.num_cells)
col = np.tile(np.arange(mg.num_cells), (g_primary.dim, 1)).ravel(
"F"
)
n_dot_I = sps.csc_matrix((data, (row, col)))
# i) The scalar contribution to the contact stress is mapped to
# the mortar grid and multiplied by n \dot I, with n being the
# outwards normals on the two sides.
# Note that by using different normals for the two sides, we do not need to
# adjust the secondary pressure with the corresponding signs by applying
# sign_of_mortar_sides as done in PrimalContactCoupling.
# iii) The contribution should be subtracted so that we balance the primary
# forces by
# T_contact - n dot I p,
# hence the minus.
mat.append(n_dot_I * mg.secondary_to_mortar_int(nd=1))
# May need to do this as for tangential projections, additive that is
normal_matrix = pp.ad.Matrix(sps.block_diag(mat))
p_frac = subdomain_proj_scalar.cell_restriction(g_frac) * p
contact_from_secondary2 = normal_matrix * p_frac
force_balance_eq = pp.ad.Expression(
contact_from_primary_mortar
+ contact_from_secondary
+ contact_from_secondary2,
dof_manager,
"force_balance",
grid_order=edge_list_highest,
)
bc_val_scalar = pp.ad.BoundaryCondition(
self.scalar_parameter_key, grid_list
)
div_scalar = pp.ad.Divergence(grids=grid_list)
dt = self.time_step
# FIXME: Need bc for div_u term, including previous time step
accumulation_primary = (
div_u_ad.div_u * (u - u_prev)
+ stab_biot_ad.stabilization
* subdomain_proj_scalar.cell_restriction(g_primary)
* (p - p_prev)
+ div_u_ad.bound_div_u
* subdomain_proj_vector.face_restriction(g_primary)
* mortar_proj_vector.mortar_to_primary_int
* (u_mortar - u_mortar_prev)
)
# Accumulation term on the fractures.
frac_vol = np.hstack([g.cell_volumes for g in g_frac])
vol_mat = pp.ad.Matrix(
sps.dia_matrix((frac_vol, 0), shape=(num_frac_cells, num_frac_cells))
)
accumulation_fracs = (
vol_mat * normal_proj * jump * (u_mortar - u_mortar_prev)
)
accumulation_all = mass_ad.mass * (p - p_prev)
flux = (
mpfa_ad.flux * p
+ mpfa_ad.bound_flux * bc_val_scalar
+ mpfa_ad.bound_flux
* mortar_proj_scalar.mortar_to_primary_int
* mortar_flux
)
flow_md = (
dt
* ( # Time scaling of flux terms, both inter-dimensional and from
# the higher dimension
div_scalar * flux
- mortar_proj_scalar.mortar_to_secondary_int * mortar_flux
)
+ accumulation_all
+ subdomain_proj_scalar.cell_prolongation(g_primary)
* accumulation_primary
+ subdomain_proj_scalar.cell_prolongation(g_frac) * accumulation_fracs
)
interface_flow_eq = robin_ad.mortar_scaling * (
mortar_proj_scalar.primary_to_mortar_avg
* mpfa_ad.bound_pressure_cell
* p
+ mortar_proj_scalar.primary_to_mortar_avg
* mpfa_ad.bound_pressure_face
* (
mortar_proj_scalar.mortar_to_primary_int * mortar_flux
+ bc_val_scalar
)
- mortar_proj_scalar.secondary_to_mortar_avg * p
+ robin_ad.mortar_discr * mortar_flux
)
flow_eq = pp.ad.Expression(
flow_md, dof_manager, "flow on nodes", grid_order=grid_list
)
interface_eq = pp.ad.Expression(
interface_flow_eq,
dof_manager,
"flow on interface",
grid_order=edge_list,
)
eq_manager.equations += [
momentum_eq,
contact_eq,
force_balance_eq,
flow_eq,
interface_eq,
]
self._eq_manager = eq_manager
def test_assemble_biot_rhs_transient(self):
""" Test the assembly of a Biot problem with a non-zero rhs using the assembler.
The test checks whether the discretization matches that of the Biot class and
that the solution reaches the expected steady state.
"""
gb = pp.meshing.cart_grid([], [3, 3], physdims=[1, 1])
g = gb.grids_of_dimension(2)[0]
d = gb.node_props(g)
# Parameters identified by two keywords. Non-default parameters of somewhat
# arbitrary values are assigned to make the test more revealing.
kw_m = "mechanics"
kw_f = "flow"
variable_m = "displacement"
variable_f = "pressure"
bound_mech, bound_flow = self.make_boundary_conditions(g)
val_mech = np.ones(g.dim * g.num_faces)
val_flow = np.ones(g.num_faces)
initial_disp, initial_pressure, initial_state = self.make_initial_conditions(
g, x0=1, y0=2, p0=0)
dt = 1e0
biot_alpha = 0.6
state = {
variable_f: initial_pressure,
variable_m: initial_disp,
kw_m: {
"bc_values": val_mech
},
}
parameters_m = {
"bc": bound_mech,
"bc_values": val_mech,
"time_step": dt,
"biot_alpha": biot_alpha,
}
parameters_f = {
"bc": bound_flow,
"bc_values": val_flow,
"time_step": dt,
"biot_alpha": biot_alpha,
"mass_weight": 0.1 * np.ones(g.num_cells),
}
pp.initialize_default_data(g, d, kw_m, parameters_m)
pp.initialize_default_data(g, d, kw_f, parameters_f)
pp.set_state(d, state)
# Initial condition fot the Biot class
# d["state"] = initial_state
# Set up the structure for the assembler. First define variables and equation
# term names.
v_0 = variable_m
v_1 = variable_f
term_00 = "stress_divergence"
term_01 = "pressure_gradient"
term_10 = "displacement_divergence"
term_11_0 = "fluid_mass"
term_11_1 = "fluid_flux"
term_11_2 = "stabilization"
d[pp.PRIMARY_VARIABLES] = {v_0: {"cells": g.dim}, v_1: {"cells": 1}}
d[pp.DISCRETIZATION] = {
v_0: {
term_00: pp.Mpsa(kw_m)
},
v_1: {
term_11_0: IE_discretizations.ImplicitMassMatrix(kw_f, v_1),
term_11_1: IE_discretizations.ImplicitMpfa(kw_f),
term_11_2: pp.BiotStabilization(kw_f),
},
v_0 + "_" + v_1: {
term_01: pp.GradP(kw_m)
},
v_1 + "_" + v_0: {
term_10: pp.DivU(kw_m)
},
}
# Discretize the mechanics related terms using the Biot class
biot_discretizer = pp.Biot()
biot_discretizer._discretize_mech(g, d)
general_assembler = pp.Assembler(gb)
# Discretize terms that are not handled by the call to biot_discretizer
general_assembler.discretize(term_filter=["fluid_mass", "fluid_flux"])
times = np.arange(5)
for _ in times:
# Assemble. Also discretizes the flow terms (fluid_mass and fluid_flux)
A, b = general_assembler.assemble_matrix_rhs()
# Assemble using the Biot class
A_class, b_class = biot_discretizer.matrix_rhs(g,
d,
discretize=False)
# Make sure the variable ordering of the matrix assembled by the assembler
# matches that of the Biot class.
grids = [g, g]
variables = [v_0, v_1]
A, b = permute_matrix_vector(
A,
b,
general_assembler.block_dof,
general_assembler.full_dof,
grids,
variables,
)
# Compare the matrices and rhs vectors
self.assertTrue(np.all(np.isclose(A.A, A_class.A)))
self.assertTrue(np.all(np.isclose(b, b_class)))
# Store the current solution for the next time step.
x_i = sps.linalg.spsolve(A_class, b_class)
u_i = x_i[:(g.dim * g.num_cells)]
p_i = x_i[(g.dim * g.num_cells):]
state = {variable_f: p_i, variable_m: u_i}
pp.set_state(d, state)
# Check that the solution has converged to the expected, uniform steady state
# dictated by the BCs.
self.assertTrue(
np.all(np.isclose(x_i, np.ones((g.dim + 1) * g.num_cells))))