예제 #1
0
# Define boundary condition on left and right boundary
u0 = Constant(0.0)
bc = DirichletBC(V, u0, boundary)

# Define variational problem, simply copied from FEniCS demo
u = TrialFunction(V)
v = TestFunction(V)
f = Expression("10*exp(-(pow(x[0] - 0.5, 2) + pow(x[1] - 0.5, 2)) / 0.02)",
               degree=2)
g = Expression("sin(5*x[0])", degree=2)
a = inner(grad(u), grad(v)) * dx
L = f * v * dx + g * v * ds

while precice.is_coupling_ongoing(
):  # potential time loop, currently only one timestep is done

    # Compute solution
    u = Function(V)
    solve(a == L, u, bc)

    # Save solution in VTK format
    file = File("poisson.pvd")
    file << u

    # write data to preCICE and advance coupling
    precice.write_data(u)
    precice.advance(precice_dt)

precice.finalize()
예제 #2
0
        precice.store_checkpoint(u_n, t, n)

    read_data = precice.read_data()

    # Update the coupling expression with the new read data
    precice.update_coupling_expression(coupling_expression, read_data)

    dt.assign(np.min([fenics_dt, precice_dt]))

    # Compute solution
    solve(a == L, u_np1, bcs)

    # Dirichlet problem obtains flux from solution and sends flux on boundary to Neumann problem
    determine_heat_flux(V_g, u_np1, k, fluxes)
    fluxes_y = fluxes.sub(1)  # only exchange y component of flux.
    precice.write_data(fluxes_y)

    precice_dt = precice.advance(dt(0))

    if precice.is_action_required(precice.action_read_iteration_checkpoint()
                                  ):  # roll back to checkpoint
        u_cp, t_cp, n_cp = precice.retrieve_checkpoint()
        u_n.assign(u_cp)
        t = t_cp
        n = n_cp
    else:  # update solution
        u_n.assign(u_np1)
        t += float(dt)
        n += 1

    if precice.is_time_window_complete():
예제 #3
0
        # See https://github.com/precice/fenics-adapter/issues/113 for details.
        read_data[(0, 0)] = u_D(0, 0)

    # Update the coupling expression with the new read data
    precice.update_coupling_expression(coupling_expression, read_data)

    dt.assign(np.min([fenics_dt, precice_dt]))

    # Compute solution u^n+1, use bcs u_D^n+1, u^n and coupling bcs
    solve(a == L, u_np1, bcs)

    # Write data to preCICE according to which problem is being solved
    if problem is ProblemType.DIRICHLET:
        # Dirichlet problem reads temperature and writes flux on boundary to Neumann problem
        determine_gradient(V_g, u_np1, flux)
        precice.write_data(flux)
    elif problem is ProblemType.NEUMANN:
        # Neumann problem reads flux and writes temperature on boundary to Dirichlet problem
        precice.write_data(u_np1)

    precice_dt = precice.advance(dt(0))

    if precice.is_action_required(precice.action_read_iteration_checkpoint()):  # roll back to checkpoint
        u_cp, t_cp, n_cp = precice.retrieve_checkpoint()
        u_n.assign(u_cp)
        t = t_cp
        n = n_cp
    else:  # update solution
        u_n.assign(u_np1)
        t += float(dt)
        n += 1
예제 #4
0
    for ps in forces_x:
        ps.apply(b_forces)
    for ps in forces_y:
        ps.apply(b_forces)
    for ps in forces_z:
        ps.apply(b_forces)

    assert (b is not b_forces)
    solve(A, u_np1.vector(), b_forces)

    dt = Constant(np.min([precice_dt, fenics_dt]))

    # Write relative displacements to preCICE
    u_delta.vector()[:] = u_np1.vector()[:] - u_n.vector()[:]
    precice.write_data(u_delta)

    # Call to advance coupling, also returns the optimum time step value
    precice_dt = precice.advance(dt(0))

    # Either revert to old step if timestep has not converged or move to next timestep
    if precice.is_action_required(precice.action_read_iteration_checkpoint()
                                  ):  # roll back to checkpoint
        u_cp, t_cp, n_cp = precice.retrieve_checkpoint()
        u_n.assign(u_cp)
        t = t_cp
        n = n_cp
    else:
        u_n.assign(u_np1)
        t += float(dt)
        n += 1