def __init__(self, physics="flow", coupling=None):
self.physics = physics
self.discr = DualSource(self.physics)
self.discr_ndof = self.discr.ndof
self.coupling_conditions = coupling
self.solver = Coupler(self.discr, self.coupling_conditions)
SolverMixedDim.__init__(self)
def __init__(self, physics='flow'):
self.physics = physics
self.discr = Integral(self.physics)
self.discr_ndof = self.discr.ndof
self.coupling_conditions = None
self.solver = Coupler(self.discr)
SolverMixedDim.__init__(self)
def __init__(self, physics="flow"):
self.physics = physics
self.discr = P1Source(self.physics)
self.discr_ndof = self.discr.ndof
self.coupling_conditions = None
self.solver = Coupler(self.discr)
SolverMixedDim.__init__(self)
def __init__(self, dim_max, physics='flow'):
# NOTE: There is no flow along the intersections of the fractures.
self.physics = physics
self.dim_max = dim_max
self.discr = Tpfa(self.physics)
self.coupling_conditions = TpfaCouplingDFN(self.discr)
kwargs = {"discr_ndof": self.discr.ndof,
"discr_fct": self.__matrix_rhs__}
self.solver = Coupler(coupling = self.coupling_conditions, **kwargs)
SolverMixedDim.__init__(self)
def __init__(self, dim_max, physics='flow'):
# NOTE: There is no flow along the intersections of the fractures.
# In this case a mixed solver is considered. We assume only two
# (contiguous) dimensions active. In the higher dimensional grid the
# physical problem is discretise with a vem solver and in the lower
# dimensional grid Lagrange multiplier are used to "glue" the velocity
# dof at the interface between the fractures.
# For this reason the matrix_rhs and ndof need to be carefully taking
# care.
self.physics = physics
self.dim_max = dim_max
self.discr = DualSource(self.physics)
self.coupling_conditions = None
kwargs = {"discr_ndof": self.__ndof__,
"discr_fct": self.__matrix_rhs__}
self.solver = Coupler(coupling = None, **kwargs)
SolverMixedDim.__init__(self)