Exemple #1
0
def test_ft():
    plot = Plot()
    vb = Verbose()

    # =============================================================================
    # Parameters
    # =============================================================================
    #
    # Flow
    #

    # permeability field
    phi = Constant(1)  # porosity
    D = Constant(0.0252)  # dispersivity
    K = Constant(1)  # permeability

    # =============================================================================
    # Mesh and Elements
    # =============================================================================
    # Mesh
    mesh = QuadMesh(resolution=(30, 30))

    # Mark left and right regions
    mesh.mark_region('left',
                     lambda x, y: np.abs(x) < 1e-9,
                     entity_type='half_edge')
    mesh.mark_region('right',
                     lambda x, y: np.abs(x - 1) < 1e-9,
                     entity_type='half_edge')

    # Elements
    p_element = QuadFE(2, 'Q1')  # element for pressure
    c_element = QuadFE(2, 'Q1')  # element for concentration

    # Dofhandlers
    p_dofhandler = DofHandler(mesh, p_element)
    c_dofhandler = DofHandler(mesh, c_element)

    p_dofhandler.distribute_dofs()
    c_dofhandler.distribute_dofs()

    # Basis functions
    p_ux = Basis(p_dofhandler, 'ux')
    p_uy = Basis(p_dofhandler, 'uy')
    p_u = Basis(p_dofhandler, 'u')

    p_inflow = lambda x, y: np.ones(shape=x.shape)
    p_outflow = lambda x, y: np.zeros(shape=x.shape)
    c_inflow = lambda x, y: np.zeros(shape=x.shape)

    # =============================================================================
    # Solve the steady state flow equations
    # =============================================================================
    vb.comment('Solving flow equations')

    # Define problem
    flow_problem = [
        Form(1, test=p_ux, trial=p_ux),
        Form(1, test=p_uy, trial=p_uy),
        Form(0, test=p_u)
    ]

    # Assemble
    vb.tic('assembly')
    assembler = Assembler(flow_problem)
    assembler.add_dirichlet('left', 1)
    assembler.add_dirichlet('right', 0)
    assembler.assemble()
    vb.toc()

    # Solve linear system
    vb.tic('solve')
    A = assembler.get_matrix().tocsr()
    b = assembler.get_vector()
    x0 = assembler.assembled_bnd()

    # Interior nodes
    pa = np.zeros((p_u.n_dofs(), 1))
    int_dofs = assembler.get_dofs('interior')
    pa[int_dofs, 0] = spla.spsolve(A, b - x0)

    # Resolve Dirichlet conditions
    dir_dofs, dir_vals = assembler.get_dirichlet(asdict=False)
    pa[dir_dofs] = dir_vals
    vb.toc()

    # Pressure function
    pfn = Nodal(data=pa, basis=p_u)

    px = pfn.differentiate((1, 0))
    py = pfn.differentiate((1, 1))

    #plot.contour(px)
    #plt.show()

    # =============================================================================
    # Transport Equations
    # =============================================================================
    # Specify initial condition
    c0 = Constant(1)
    dt = 1e-1
    T = 6
    N = int(np.ceil(T / dt))

    c = Basis(c_dofhandler, 'c')
    cx = Basis(c_dofhandler, 'cx')
    cy = Basis(c_dofhandler, 'cy')

    print('assembling transport equations')
    k_phi = Kernel(f=phi)
    k_advx = Kernel(f=[K, px], F=lambda K, px: -K * px)
    k_advy = Kernel(f=[K, py], F=lambda K, py: -K * py)
    tht = 1
    m = [Form(kernel=k_phi, test=c, trial=c)]
    s = [
        Form(kernel=k_advx, test=c, trial=cx),
        Form(kernel=k_advy, test=c, trial=cy),
        Form(kernel=Kernel(D), test=cx, trial=cx),
        Form(kernel=Kernel(D), test=cy, trial=cy)
    ]

    problems = [m, s]
    assembler = Assembler(problems)
    assembler.add_dirichlet('left', 0, i_problem=0)
    assembler.add_dirichlet('left', 0, i_problem=1)
    assembler.assemble()

    x0 = assembler.assembled_bnd()

    # Interior nodes
    int_dofs = assembler.get_dofs('interior')

    # Dirichlet conditions
    dir_dofs, dir_vals = assembler.get_dirichlet(asdict=False)

    # System matrices
    M = assembler.get_matrix(i_problem=0)
    S = assembler.get_matrix(i_problem=1)

    # Initialize c0 and cp
    c0 = np.ones((c.n_dofs(), 1))
    cp = np.zeros((c.n_dofs(), 1))
    c_fn = Nodal(data=c0, basis=c)

    #
    # Compute solution
    #
    print('time stepping')
    for i in range(N):

        # Build system
        A = M + tht * dt * S
        b = M.dot(c0[int_dofs]) - (1 - tht) * dt * S.dot(c0[int_dofs])

        # Solve linear system
        cp[int_dofs, 0] = spla.spsolve(A, b)

        # Add Dirichlet conditions
        cp[dir_dofs] = dir_vals

        # Record current iterate
        c_fn.add_samples(data=cp)

        # Update c0
        c0 = cp.copy()

        #plot.contour(c_fn, n_sample=i)

    #
    # Quantity of interest
    #
    def F(c, px, py, entity=None):
        """
        Compute c(x,y,t)*(grad p * n)
        """
        n = entity.unit_normal()
        return c * (px * n[0] + py * n[1])

    px.set_subsample(i=np.arange(41))
    py.set_subsample(i=np.arange(41))

    #kernel = Kernel(f=[c_fn,px,py], F=F)
    kernel = Kernel(c_fn)

    #print(kernel.n_subsample())
    form = Form(kernel, flag='right', dmu='ds')
    assembler = Assembler(form, mesh=mesh)
    assembler.assemble()
    QQ = assembler.assembled_forms()[0].aggregate_data()['array']

    Q = np.array([assembler.get_scalar(i_sample=i) for i in np.arange(N + 1)])
    t = np.linspace(0, T, N + 1)
    plt.plot(t, Q)
    plt.show()
    print(Q)