def form_fluid_adjoint(
displacement_fluid_adjoint,
velocity_fluid_adjoint,
xi_fluid,
eta_fluid,
fluid: Space,
param: Parameters,
):
return (
param.NU
* dot(grad(eta_fluid), grad(displacement_fluid_adjoint))
* fluid.dx
+ dot(param.BETA, grad(eta_fluid))
* displacement_fluid_adjoint
* fluid.dx
+ dot(grad(xi_fluid), grad(velocity_fluid_adjoint)) * fluid.dx
- dot(grad(xi_fluid), fluid.normal_vector)
* velocity_fluid_adjoint
* fluid.ds(1)
- param.NU
* dot(grad(eta_fluid), fluid.normal_vector)
* displacement_fluid_adjoint
* fluid.ds(1)
+ param.GAMMA
/ fluid.cell_size
* xi_fluid
* velocity_fluid_adjoint
* fluid.ds(1)
+ param.GAMMA
/ fluid.cell_size
* eta_fluid
* displacement_fluid_adjoint
* fluid.ds(1)
)
def _construct_eigenproblem(self, u: ufl.Argument, v: ufl.Argument) \
-> Tuple[ufl.algebra.Operator, ufl.algebra.Operator]:
"""Construct left- and right-hand sides of eigenvalue problem.
Parameters
----------
u : ufl.Argument
A function belonging to the function space under consideration.
v : ufl.Argument
A function belonging to the function space under consideration.
Returns
-------
a : ufl.algebra.Operator
Left hand side form.
b : ufl.algebra.Operator
Right hand side form.
"""
g = self.metric_tensor
sqrt_g = fenics.sqrt(fenics.det(g))
inv_g = fenics.inv(g)
# $a(u, v) = \int_M \nabla u \cdot g^{-1} \nabla v \, \sqrt{\det(g)} \, d x$.
a = fenics.dot(fenics.grad(u), inv_g * fenics.grad(v)) * sqrt_g
# $b(u, v) = \int_M u \, v \, \sqrt{\det(g)} \, d x$.
b = fenics.dot(u, v) * sqrt_g
return a, b
def functional_fluid_adjoint_initial(
displacement_fluid_adjoint_old,
velocity_fluid_adjoint_old,
displacement_fluid_adjoint_interface,
velocity_fluid_adjoint_interface,
displacement_fluid_adjoint_old_interface,
velocity_fluid_adjoint_old_interface,
xi_fluid,
eta_fluid,
fluid: Space,
param: Parameters,
time,
time_step,
microtimestep_before: MicroTimeStep,
microtimestep: MicroTimeStep,
):
return (
0.5
* time_step
* param.NU
* dot(grad(eta_fluid), fluid.normal_vector)
* displacement_fluid_adjoint_interface
* fluid.ds(1)
+ 2.0 * param.NU
* characteristic_function_fluid(param)
* dot(
goal_functional(
microtimestep_before, microtimestep, "primal_velocity"
)[1],
grad(eta_fluid),
)
* fluid.dx
)
def form_fluid(
displacement_fluid,
velocity_fluid,
phi_fluid,
psi_fluid,
fluid: Space,
param: Parameters,
):
return (
param.NU * dot(grad(velocity_fluid), grad(phi_fluid)) * fluid.dx
+ dot(param.BETA, grad(velocity_fluid)) * phi_fluid * fluid.dx
+ dot(grad(displacement_fluid), grad(psi_fluid)) * fluid.dx
- dot(grad(displacement_fluid), fluid.normal_vector)
* psi_fluid
* fluid.ds(1)
- param.NU
* dot(grad(velocity_fluid), fluid.normal_vector)
* phi_fluid
* fluid.ds(1)
+ param.GAMMA
/ fluid.cell_size
* displacement_fluid
* psi_fluid
* fluid.ds(1)
+ param.GAMMA
/ fluid.cell_size
* velocity_fluid
* phi_fluid
* fluid.ds(1)
)
def defineWeakSystemDomain():
"""Define system of equations of the weak formulation of
the second-orderformulation of the PN equations on the domain .
"""
sMD = importlib.import_module(
"systemMatricesDomain_d_%d_k_%s_N_%d" %
(par['spatialDimension'], par['kernelName'], N_PN))
systemMatricesDomain = sMD.getSystemMatricesDomain(par)
lhs = 0.0 * v[0] * fe.dx(V)
for i in range(nEvenMoments):
for j in range(nEvenMoments):
if (par['spatialDimension'] == 1):
lhs += systemMatricesDomain['Kzz'][i][j] * fe.dot(
fe.grad(u[j])[0],
fe.grad(v[i])[0]) * fe.dx(V)
elif (par['spatialDimension'] == 2):
lhs += systemMatricesDomain['Kxx'][i][j] * fe.dot(
fe.grad(u[j])[0],
fe.grad(v[i])[0]) * fe.dx(V)
lhs += systemMatricesDomain['Kxy'][i][j] * fe.dot(
fe.grad(u[j])[1],
fe.grad(v[i])[0]) * fe.dx(V)
lhs += systemMatricesDomain['Kyx'][i][j] * fe.dot(
fe.grad(u[j])[0],
fe.grad(v[i])[1]) * fe.dx(V)
lhs += systemMatricesDomain['Kyy'][i][j] * fe.dot(
fe.grad(u[j])[1],
fe.grad(v[i])[1]) * fe.dx(V)
else:
raise ValueError(
'Only spatial dimensions <= 2 implemented!')
lhs += systemMatricesDomain['S'][i][j] * u[j] * v[i] * fe.dx(V)
return lhs
def plot_diffusion_coef(self, entries='01'):
indices = [int(entry) for entry in entries]
vector = np.zeros(2)
vector[indices] = 1
print(vector)
fevec = fe.Constant(vector)
val = fe.dot(self.composed_diff_coef, fevec)
val = fe.dot(fevec, val)
fe.plot(val, mesh=self.mesh)
plt.show()
def solve(self):
"""Evoke FEniCS FEM solver.
Returns
-------
uij : (Ni,) ndarray
potential at Ni grid points
nij : (M,Nij) ndarray
concentrations of M species at Ni grid points
lamj: (L,) ndarray
value of L Lagrange multipliers
"""
# weak form and FEM scheme:
# in the weak form, u and v are the trial and test functions associated
# with the Poisson part, p and q the trial and test functions associated
# with the Nernst-Planck part. lam and mu are trial and test fuctions
# associated to constraints introduced via Lagrange multipliers.
# w is the whole set of trial functions [u,p,lam]
# W is the space all w live in.
rho = 0
for i in range(self.M):
rho += self.z[i] * self.p[i]
source = -0.5 * rho * self.v * fn.dx
laplace = fn.dot(fn.grad(self.u), fn.grad(self.v)) * fn.dx
poisson = laplace + source
nernst_planck = 0
for i in range(self.M):
nernst_planck += fn.dot(
-fn.grad(self.p[i]) - self.z[i] * self.p[i] * fn.grad(self.u),
fn.grad(self.q[i])) * fn.dx
# constraints set up elsewhere
F = poisson + nernst_planck + self.constraints
fn.solve(F == 0, self.w, self.boundary_conditions)
# store results:
wij = np.array([self.w(x) for x in self.X]).T
self.uij = wij[0, :] # potential
self.nij = wij[1:(self.M + 1), :] # concentrations
self.lamj = wij[(self.M + 1):] # Lagrange multipliers
return self.uij, self.nij, self.lamj
def goal_functional_solid(
displacement_solid_array,
velocity_solid_array,
solid,
solid_timeline,
param,
):
global_result = 0.0
macrotimestep = solid_timeline.head
global_size = solid_timeline.size
m = 1
for n in range(global_size):
microtimestep = macrotimestep.head.after
local_size = macrotimestep.size - 1
for k in range(local_size):
print(f"Current contribution: {m}")
result = 0.0
time_step = microtimestep.before.dt
gauss_1, gauss_2 = gauss(microtimestep)
result += (
0.5 * time_step * param.ZETA *
characteristic_function_solid(param) * dot(
grad(
linear_extrapolation(displacement_solid_array, m,
gauss_1, microtimestep)),
grad(
linear_extrapolation(displacement_solid_array, m,
gauss_1, microtimestep)),
) * solid.dx)
result += (
0.5 * time_step * param.ZETA *
characteristic_function_solid(param) * dot(
grad(
linear_extrapolation(displacement_solid_array, m,
gauss_2, microtimestep)),
grad(
linear_extrapolation(displacement_solid_array, m,
gauss_2, microtimestep)),
) * solid.dx)
m += 1
microtimestep = microtimestep.after
global_result += assemble(result)
macrotimestep = macrotimestep.after
return global_result
def project_gradient_neumann(
f0,
degree=None,
mesh=None,
solver_type='gmres',
preconditioner_type='default'
):
"""Find an approximation to f0 that has the same gradient
The resulting function also satisfies homogeneous Neumann boundary
conditions.
Parameters:
f0: the function to approximate
mesh=None: the mesh on which to approximate it If not provided, the
mesh is extracted from f0.
degree=None: degree of the polynomial approximation. extracted
from f0 if not provided.
solver_type='gmres': The linear solver type to use.
preconditioner_type='default': Preconditioner type to use
"""
if not mesh: mesh = f0.function_space().mesh()
element = f0.ufl_element()
if not degree:
degree = element.degree()
CE = FiniteElement('CG', mesh.ufl_cell(), degree)
CS = FunctionSpace(mesh, CE)
DE = FiniteElement('DG', mesh.ufl_cell(), degree)
DS = FunctionSpace(mesh, DE)
CVE = VectorElement('CG', mesh.ufl_cell(), degree - 1)
CV = FunctionSpace(mesh, CVE)
RE = FiniteElement('R', mesh.ufl_cell(), 0)
R = FunctionSpace(mesh, RE)
CRE = MixedElement([CE, RE])
CR = FunctionSpace(mesh, CRE)
f = fe.project(f0, CS,
solver_type=solver_type,
preconditioner_type=preconditioner_type)
g = fe.project(fe.grad(f), CV,
solver_type=solver_type,
preconditioner_type=preconditioner_type)
lf = fe.project(fe.nabla_div(g), CS,
solver_type=solver_type,
preconditioner_type=preconditioner_type)
tf, tc = TrialFunction(CR)
wf, wc = TestFunctions(CR)
dx = Measure('dx', domain=mesh,
metadata={'quadrature_degree': min(degree, 10)})
a = (fe.dot(fe.grad(tf), fe.grad(wf)) + tc * wf + tf * wc) * dx
L = (f * wc - lf * wf) * dx
igc = Function(CR)
fe.solve(a == L, igc,
solver_parameters={'linear_solver': solver_type,
'preconditioner': preconditioner_type}
)
ig, c = igc.sub(0), igc.sub(1)
igd = fe.project(ig, DS,
solver_type=solver_type,
preconditioner_type=preconditioner_type)
return igd
def solver(f, u_D, bc_funs, ndim, length, nx, ny, nz=None, degree=1):
"""Fenics 求解器
Args:
f (Expression): [description]
u_D (Expression): [description]
bc_funs (List[Callable]): [description]
ndim (int): [description]
length (float): [description]
nx (int): [description]
ny (int): [description]
nz (int, optional): [description]. Defaults to None.
degree (int, optional): [description]. Defaults to 1.
Returns:
Function: 解 u
"""
mesh = get_mesh(length, nx, ny, nz)
V = fs.FunctionSpace(mesh, "P", degree)
bcs = [fs.DirichletBC(V, u_D, bc) for bc in bc_funs]
u = fs.TrialFunction(V)
v = fs.TestFunction(V)
FF = fs.dot(fs.grad(u), fs.grad(v)) * fs.dx - f * v * fs.dx
a = fs.lhs(FF)
L = fs.rhs(FF)
u = fs.Function(V)
fs.solve(a == L, u, bcs)
return u
def construct_variation_problem(self) -> Tuple[Form, Form]:
p = self.params
u_t = (p.T - p.T_prev) / p.dt
f = p.Q_pc + p.Q_sw + p.Q_mm
F = p.P_s * p.c_s * u_t * p.v * dx + p.k_e * dot(grad(p.T), grad(
p.v)) * dx - f * p.v * dx
return lhs(F), rhs(F)
def __call__(self, u_test, return_sol=False, return_permeability=False):
# Variables
x, y = sym.symbols('x[0], x[1]', real=True, positive=True)
# Diffusivities
diff_1 = np.exp(u_test[0])
diff_2 = np.exp(u_test[1])
# Interfaces
ix = u_test[2]
iy = u_test[3]
# Diffusivity
diff = sym.Piecewise((sym.Piecewise(
(diff_1, y <= iy), (diff_2, True)), x <= ix), (diff_2, True))
# if return_permeability:
# return sym.lambdify((x, y), diff)
ccode_coeff = sym.ccode(diff)
diff = fen.Expression(ccode_coeff, degree=2)
if return_permeability:
return diff
# Define bilinear form in variational problem
a_bil = diff * fen.dot(fen.grad(self.trial_f), fen.grad(
self.test_f)) * fen.dx
# Compute solution
sol = fen.Function(self.f_space)
fen.solve(a_bil == self.lin_func, sol, self.bound_cond)
evaluations = [sol(xi, yi) for xi, yi in zip(self.x_obs, self.y_obs)]
return sol if return_sol else np.array(evaluations)
def solve_pde(self):
u = fe.Function(self.function_space)
v = fe.TestFunction(self.function_space)
u_old = fe.project(self.u_0, self.function_space)
# Todo: Average right hand side if we choose it non-constant
flux = self.dt * fe.dot(
self.composed_diff_coef *
(fe.grad(u) + self.drift_function(u)), fe.grad(v)) * fe.dx
bilin_part = u * v * fe.dx + flux
funtional_part = self.rhs * v * self.dt * fe.dx + u_old * v * fe.dx
full_form = bilin_part - funtional_part
num_steps = int(self.T / self.dt) + 1
bc = fe.DirichletBC(self.function_space, self.u_boundary,
MembraneSimulator.full_boundary)
for n in range(num_steps):
print("Step %d" % n)
self.time += self.dt
fe.solve(full_form == 0, u, bc)
# fe.plot(u)
# plt.show()
# print(fe.errornorm(u_old, u))
u_old.assign(u)
self.file << (u, self.time)
f = fe.plot(u)
plt.rc('text', usetex=True)
plt.colorbar(f, format='%.0e')
plt.title(r'Macroscopic density profile of $u(x,t)$ at $t=1$')
plt.xlabel(r'$x_1$')
plt.ylabel(r'$x_2$')
plt.show()
def effective_field(m, volume=None):
w_Zeeman = - mu0 * Ms * fe.dot(m, H)
w_exchange = A * fe.inner(fe.grad(m), fe.grad(m))
w_DMI = D * fe.inner(m, fe.curl(m))
w_ani = - K * fe.inner(m, ea)**2
w = w_Zeeman + w_exchange + w_DMI + w_ani
return -1/(mu0*Ms) * fe.derivative(w*fe.dx, m)
def form_solid(
displacement_solid,
velocity_solid,
phi_solid,
psi_solid,
solid: Space,
param: Parameters,
):
return (
param.ZETA * dot(grad(displacement_solid), grad(phi_solid)) * solid.dx
+ param.DELTA * dot(grad(velocity_solid), grad(phi_solid)) * solid.dx
- velocity_solid * psi_solid * solid.dx
- param.DELTA
* dot(grad(velocity_solid), solid.normal_vector)
* phi_solid
* solid.ds(1)
)
def test_formulation_1_extrap_1_material():
'''
Test function formulation() with 1 extrinsic trap
and 1 material
'''
dt = 1
traps = [{
"energy": 1,
"materials": [1],
"type": "extrinsic"
}]
materials = [{
"alpha": 1,
"beta": 2,
"density": 3,
"borders": [0, 1],
"E_diff": 4,
"D_0": 5,
"id": 1
}]
mesh = fenics.UnitIntervalMesh(10)
V = fenics.VectorFunctionSpace(mesh, 'P', 1, 2)
W = fenics.FunctionSpace(mesh, 'P', 1)
u = fenics.Function(V)
u_n = fenics.Function(V)
v = fenics.TestFunction(V)
n = fenics.interpolate(fenics.Expression('1', degree=0), W)
solutions = list(fenics.split(u))
previous_solutions = list(fenics.split(u_n))
testfunctions = list(fenics.split(v))
extrinsic_traps = [n]
mf = fenics.MeshFunction('size_t', mesh, 1, 1)
dx = fenics.dx(subdomain_data=mf)
temp = fenics.Expression("300", degree=0)
flux_ = fenics.Expression("10000", degree=0)
F, expressions = FESTIM.formulation(
traps, extrinsic_traps, solutions, testfunctions,
previous_solutions, dt, dx, materials, temp, flux_)
expected_form = ((solutions[0] - previous_solutions[0]) / dt) * \
testfunctions[0]*dx
expected_form += 5 * fenics.exp(-4/8.6e-5/temp) * \
fenics.dot(
fenics.grad(solutions[0]), fenics.grad(testfunctions[0]))*dx(1)
expected_form += -flux_*testfunctions[0]*dx + \
((solutions[1] - previous_solutions[1]) / dt) * \
testfunctions[1]*dx
expected_form += - 5 * fenics.exp(-4/8.6e-5/temp)/1/1/2 * \
solutions[0] * (extrinsic_traps[0] - solutions[1]) * \
testfunctions[1]*dx(1)
expected_form += 1e13*fenics.exp(-1/8.6e-5/temp)*solutions[1] * \
testfunctions[1]*dx(1)
expected_form += ((solutions[1] - previous_solutions[1]) / dt) * \
testfunctions[0]*dx
assert expected_form.equals(F) is True
def get_F(u, v, dt):
dx = fenics.dx
F = (u * v * dx
+ dt * (sigma**2 / 2)
* fenics.dot(fenics.grad(u**2), fenics.grad(v)) * dx
- (1 / theta) * dt * u * (1 - u) * v * dx
- u_n * v * dx
)
return F
def _solve_pde(self, diff_coef):
# Actual PDE solver for any coefficient diff_coef
u = fe.TrialFunction(self.function_space)
v = fe.TestFunction(self.function_space)
a = fe.dot(diff_coef * fe.grad(u), fe.grad(v)) * fe.dx
L = self.f * v * fe.dx
bc = fe.DirichletBC(self.function_space, self.bc_function,
PoissonSolver.boundary)
fe.solve(a == L, self.solution, bc)
def fenics_p_electric(self, my_d):
"""
@description:
Solve poisson equation to get potential and electric field
@Modify:
2021/08/31
"""
if "plugin3D" in self.det_model:
bc_l = []
bc_l = self.boundary_definition_3D(my_d, "Possion")
elif "planar3D" in self.det_model:
bc_l = self.boundary_definition_2D(my_d, "Possion")
u = fenics.TrialFunction(self.V)
v = fenics.TestFunction(self.V)
if self.det_dic['name'] == "lgad3D":
if self.det_dic['part'] == 2:
bond = self.det_dic['bond1']
doping_avalanche = self.f_value(my_d, self.det_dic['doping1'])
doping = self.f_value(my_d, self.det_dic['doping2'])
f = fenics.Expression('x[2] < width ? doping1 : doping2',
degree=1,
width=bond,
doping1=doping_avalanche,
doping2=doping)
elif self.det_dic['part'] == 3:
bond1 = self.det_dic['bond1']
bond2 = self.det_dic['bond2']
doping1 = self.f_value(my_d, self.det_dic['doping1'])
doping2 = self.f_value(my_d, self.det_dic['doping2'])
doping3 = self.f_value(my_d, self.det_dic['doping3'])
f = fenics.Expression(
'x[2] < bonda ? dopinga : x[2] > bondb ? dopingc : dopingb',
degree=1,
bonda=bond1,
bondb=bond2,
dopinga=doping1,
dopingb=doping2,
dopingc=doping3)
else:
print("The structure of lgad is wrong.")
else:
f = fenics.Constant(self.f_value(my_d))
a = fenics.dot(fenics.grad(u), fenics.grad(v)) * fenics.dx
L = f * v * fenics.dx
# Compute solution
self.u = fenics.Function(self.V)
fenics.solve(a == L,
self.u,
bc_l,
solver_parameters=dict(linear_solver='gmres',
preconditioner='ilu'))
#calculate electric field
W = fenics.VectorFunctionSpace(self.mesh3D, 'P', 1)
self.E_field = fenics.project(
fenics.as_vector((self.u.dx(0), self.u.dx(1), self.u.dx(2))), W)
def construct_variation_problem(self) -> Tuple[Form, Form]:
p = self.params
ds = self.make_ds(p.mesh)
u_t = (p.u - p.P_prev) / p.dt
term = p.alpha_th * p.u * p.P_d * (p.my_v + p.my_d)**2 / (
(p.P_prev + p.P_d) * p.my_v * p.my_d) / p.T_s * grad(p.T_s)
F = p.theta_a * u_t * p.v * dx + p.theta_a * p.D_e * dot(
grad(p.u) - term, grad(
p.v)) * dx - p.M_mm * p.v * dx + p.q_h * p.v * ds(1)
return lhs(F), rhs(F)
def _compute_effective_diffusion(self):
# Uses the solutions of the cell problems to compute the harmonic average of the diffusivity
for i, j in np.ndindex((self.dim, self.dim)):
integrand_ij = fe.project(
self.a_y *
fe.dot(self.e_is[i] + fe.grad(self.cell_solutions[i]),
self.e_is[j] + fe.grad(self.cell_solutions[j])),
self.function_space)
self.eff_diff[i, j] = fe.assemble(integrand_ij * fe.dx)
return fe.Constant(self.eff_diff)
def _solve_cell_problems(self):
# Solves the cell problems (one for each space dimension)
w = fe.TrialFunction(self.function_space)
v = fe.TestFunction(self.function_space)
a = self.a_y * fe.dot(fe.grad(w), fe.grad(v)) * fe.dx
for i in range(self.dim):
L = fe.div(self.a_y * self.e_is[i]) * v * fe.dx
bc = fe.DirichletBC(self.function_space, self.bc_function,
PoissonSolver.boundary)
fe.solve(a == L, self.cell_solutions[i], bc)
fe.plot(self.cell_solutions[i])
def __compute_shape_derivative(self):
"""Computes the shape derivative.
Returns
-------
None
Notes
-----
This only works properly if differential operators only
act on state and adjoint variables, else the results are incorrect.
A corresponding warning whenever this could be the case is issued.
"""
# Shape derivative of Lagrangian w/o regularization and pull-backs
self.shape_derivative = fenics.derivative(
self.lagrangian.lagrangian_form,
fenics.SpatialCoordinate(self.mesh), self.test_vector_field)
# Add pull-backs
if self.use_pull_back:
self.state_adjoint_ids = [coeff.id() for coeff in self.states] + [
coeff.id() for coeff in self.adjoints
]
self.material_derivative_coeffs = []
for coeff in self.lagrangian.lagrangian_form.coefficients():
if coeff.id() in self.state_adjoint_ids:
pass
else:
if not (coeff.ufl_element().family() == 'Real'):
self.material_derivative_coeffs.append(coeff)
if len(self.material_derivative_coeffs) > 0:
warning(
'Shape derivative might be wrong, if differential operators act on variables other than states and adjoints. \n'
'You can check for correctness of the shape derivative with cashocs.verification.shape_gradient_test\n'
)
for coeff in self.material_derivative_coeffs:
# temp_space = fenics.FunctionSpace(self.mesh, coeff.ufl_element())
# placeholder = fenics.Function(temp_space)
# temp_form = fenics.derivative(self.lagrangian.lagrangian_form, coeff, placeholder)
# material_derivative = replace(temp_form, {placeholder : fenics.dot(fenics.grad(coeff), self.test_vector_field)})
material_derivative = fenics.derivative(
self.lagrangian.lagrangian_form, coeff,
fenics.dot(fenics.grad(coeff), self.test_vector_field))
material_derivative = expand_derivatives(material_derivative)
self.shape_derivative += material_derivative
# Add regularization
self.shape_derivative += self.regularization.compute_shape_derivative()
def create_bilinear_form_and_rhs(self):
# Define variational problem
u = fe.TrialFunction(self.function_space)
v = fe.TestFunction(self.function_space)
self.bilinear_form = (1 + self.lam * self.dt) *\
(u * v * fe.dx) + self.dt * self.diffusion_coefficient *\
(fe.dot(fe.grad(u), fe.grad(v)) * fe.dx)
self.rhs = (self.u_n + self.dt * self.rhs_fun * self.u_n) * v * fe.dx
def functional_solid(
displacement_solid_old,
velocity_solid_old,
displacement_solid_interface,
velocity_solid_interface,
displacement_solid_old_interface,
velocity_solid_old_interface,
phi_solid,
psi_solid,
solid: Space,
param: Parameters,
time,
time_step,
):
return (
velocity_solid_old * phi_solid * solid.dx
+ displacement_solid_old * psi_solid * solid.dx
- 0.5
* time_step
* form_solid(
displacement_solid_old,
velocity_solid_old,
phi_solid,
psi_solid,
solid,
param,
)
- 0.5
* time_step
* param.NU
* dot(grad(velocity_solid_interface), solid.normal_vector)
* phi_solid
* solid.ds(1)
- 0.5
* time_step
* param.NU
* dot(grad(velocity_solid_old_interface), solid.normal_vector)
* phi_solid
* solid.ds(1)
)
def create_bilinear_form_and_rhs(self):
# Define variational problem
u = fe.TrialFunction(self.function_space)
v = fe.TestFunction(self.function_space)
if self.dimension == 1:
diffusion_tensor = self.diffusion_matrix
self.bilinear_form = (1 + self.lam * self.dt) * (u * v * fe.dx) +\
self.dt * (fe.dot(\
diffusion_tensor * fe.grad(u),\
fe.grad(v)) * fe.dx)
if self.dimension == 2:
diffusion_tensor = fe.as_matrix(self.diffusion_matrix)
self.bilinear_form = (1 + self.lam * self.dt) * (u * v * fe.dx) +\
self.dt * (fe.dot(\
fe.dot(diffusion_tensor, fe.grad(u)),\
fe.grad(v)) * fe.dx)
self.rhs = (self.u_n + self.dt * self.rhs_fun) * v * fe.dx
def get_tangential_component(self, t, E):
E_t = fn.dot(E, t)
E_t = Poisson.block_project(E_t,
self.mesh,
self.restrictions_dict['interface_rtc'],
self.boundaries,
self.boundaries_ids['Interface'],
space_type='scalar',
boundary_type='internal',
sign=t.side(),
restricted=True)
return E_t
def solve_wave_equation(u0, u1, u_boundary, f, domain, mesh, degree):
"""Solving the wave equation using CG-CG method.
Args:
u0: Initial data.
u1: Initial velocity.
u_boundary: Dirichlet boundary condition.
f: Right-hand side.
domain: Space-time domain.
mesh: Computational mesh.
degree: CG(degree) will be used as the finite element.
Outputs:
uh: Numerical solution.
"""
# Element
V = FunctionSpace(mesh, "CG", degree)
# Measures on the initial and terminal slice
mask = MeshFunction("size_t", mesh, mesh.topology().dim() - 1, 0)
domain.get_initial_slice().mark(mask, 1)
ends = ds(subdomain_data=mask)
# Form
g = Constant(((-1.0, 0.0), (0.0, 1.0)))
u = TrialFunction(V)
v = TestFunction(V)
a = dot(grad(v), dot(g, grad(u))) * dx
L = f * v * dx + u1 * v * ends(1)
# Assembled matrices
A = assemble(a, keep_diagonal=True)
b = assemble(L, keep_diagonal=True)
# Spatial boundary condition
bc = DirichletBC(V, u_boundary, domain.get_spatial_boundary())
bc.apply(A, b)
# Temporal boundary conditions (by hand)
(A, b) = apply_time_boundary_conditions(domain, V, u0, A, b)
# Solve
solver = LUSolver()
solver.set_operator(A)
uh = Function(V)
solver.solve(uh.vector(), b)
return uh
def compute_dmdt(m):
"""Convenience function that does all in one go"""
# Assemble RHS
b = fe.assemble(Heff_form)
# Project onto Heff
LU.solve(Heff.vector(), b)
LLG = -gamma/(1+alpha*alpha)*fe.cross(m, Heff) - alpha*gamma/(1+alpha*alpha)*fe.cross(m, fe.cross(m, Heff))
result = fe.assemble(fe.dot(LLG, v)*fe.dP)
return result.array()
def form_solid_adjoint(
displacement_solid_adjoint,
velocity_solid_adjoint,
xi_solid,
eta_solid,
solid: Space,
param: Parameters,
):
return (
param.ZETA
* dot(grad(xi_solid), grad(displacement_solid_adjoint))
* solid.dx
+ param.DELTA
* dot(grad(eta_solid), grad(displacement_solid_adjoint))
* solid.dx
- eta_solid * velocity_solid_adjoint * solid.dx
- param.DELTA
* dot(grad(eta_solid), solid.normal_vector)
* displacement_solid_adjoint
* solid.ds(1)
)
def solve(self):
# TODO: when FEniCS ported to Python3, this should be exist_ok
try:
os.makedirs('results')
except OSError:
pass
z, w = (self.z, self.w)
u0 = d.Constant(0.0)
# Define the linear and bilinear forms
L = u0 * w * dx
# Define useful functions
cond = d.Function(self.DV)
U = d.Function(self.V)
# Initialize the max_e vector, that will store the cumulative max e values
max_e = d.Function(self.V)
max_e.vector()[:] = 0.0
max_e.rename("max_E", "Maximum energy deposition by location")
max_e_file = d.File("results/%s-max_e.pvd" % input_mesh)
max_e_per_step = d.Function(self.V)
max_e_per_step_file = d.File("results/%s-max_e_per_step.pvd" % input_mesh)
self.es = {}
self.max_es = {}
fi = d.File("results/%s-cond.pvd" % input_mesh)
potential_file = d.File("results/%s-potential.pvd" % input_mesh)
# Loop through the voltages and electrode combinations
for i, (anode, cathode, voltage) in enumerate(v.electrode_triples):
print("Electrodes %d (%lf) -> %d (0)" % (anode, voltage, cathode))
cond = d.project(self.sigma_start, V=self.DV)
# Define the Dirichlet boundary conditions on the active needles
uV = d.Constant(voltage)
term1_bc = d.DirichletBC(self.V, uV, self.patches, v.needles[anode])
term2_bc = d.DirichletBC(self.V, u0, self.patches, v.needles[cathode])
e = d.Function(self.V)
e.vector()[:] = max_e.vector()
# Re-evaluate conductivity
self.increase_conductivity(cond, e)
for j in range(v.max_restarts):
# Update the bilinear form
a = d.inner(d.nabla_grad(z), cond * d.nabla_grad(w)) * dx
# Solve again
print(" [solving...")
d.solve(a == L, U, bcs=[term1_bc, term2_bc])
print(" ....solved]")
# Extract electric field norm
for k in range(len(U.vector())):
if N.isnan(U.vector()[k]):
U.vector()[k] = 1e5
e_new = d.project(d.sqrt(d.dot(d.grad(U), d.grad(U))), self.V)
# Take the max of the new field and the established electric field
e.vector()[:] = N.array([max(*X) for X in zip(e.vector(), e_new.vector())])
# Re-evaluate conductivity
fi << cond
self.increase_conductivity(cond, e)
potential_file << U
# Save the max e function to a VTU
max_e_per_step.vector()[:] = e.vector()[:]
max_e_per_step_file << max_e_per_step
# Store this electric field norm, for this triple, for later reference
self.es[i] = e
# Store the max of this electric field norm and that for all previous triples
max_e_array = N.array([max(*X) for X in zip(max_e.vector(), e.vector())])
max_e.vector()[:] = max_e_array
# Create a new max_e function for storage, or it will be overwritten by the next iteration
max_e_new = d.Function(self.V)
max_e_new.vector()[:] = max_e_array
# Store this max e function for the cumulative coverage curve calculation later
self.max_es[i] = max_e_new
# Save the max e function to a VTU
max_e_file << max_e
self.max_e_count = i