Example #1
0
    def test_apply_scalar(n_threads, halo, grid, loop):
        n_dims = len(grid)
        if n_dims == 1 and n_threads > 1:
            return

        # arrange
        traversals = Traversals(grid, halo, jit_flags, n_threads)
        sut = traversals.apply_scalar(loop=loop)

        scl_null_arg_impl = ScalarField.make_null(n_dims).impl
        vec_null_arg_impl = VectorField.make_null(n_dims).impl

        out = ScalarField(np.zeros(grid), halo,
                          [ConstantBoundaryCondition(np.nan)] * n_dims)

        # act
        sut(_cell_id_scalar, _cell_id_scalar, *out.impl[0],
            *vec_null_arg_impl[0], *vec_null_arg_impl[1],
            *scl_null_arg_impl[0], *scl_null_arg_impl[1],
            *scl_null_arg_impl[0], *scl_null_arg_impl[1],
            *scl_null_arg_impl[0], *scl_null_arg_impl[1])

        # assert
        data = out.get()
        assert data.shape == grid
        focus = (-halo, -halo)
        for i in range(halo, halo + grid[0]):
            for j in (-1, ) if n_dims == 1 else range(halo, halo + grid[1]):
                value = indexers[n_dims].at[0](focus, data, i, j)
                assert value == (n_dims if loop else 1) * cell_id(i, j)
        assert scl_null_arg_impl[0][0][meta_halo_valid]
        assert vec_null_arg_impl[0][0][meta_halo_valid]
        assert not out.impl[0][0][meta_halo_valid]
Example #2
0
    def test_make_upwind(self):
        # Arrange
        psi_data = np.array((0, 1, 0))
        flux_data = np.array((0, 0, 1, 0))

        options = Options()
        halo = options.n_halo
        traversals = Traversals(grid=psi_data.shape,
                                halo=halo,
                                jit_flags={},
                                n_threads=1)
        upwind = make_upwind(options=options,
                             non_unit_g_factor=False,
                             traversals=traversals)

        bc = [PeriodicBoundaryCondition()]
        psi = ScalarField(psi_data, halo, bc)
        psi_impl = psi.impl
        flux_impl = VectorField((flux_data, ), halo, bc).impl
        null_impl = ScalarField.make_null(len(psi_data.shape)).impl

        # Act
        upwind(psi_impl[0], *flux_impl, *null_impl)

        # Assert
        np.testing.assert_array_equal(psi.get(), np.roll(psi_data, 1))
    def test_vector_1d(self, data, halo, side):
        # arrange
        field = VectorField((data, ), halo, (PeriodicBoundaryCondition(), ))
        meta_and_data, fill_halos = field.impl
        traversals = Traversals(grid=(data.shape[0] - 1, ),
                                halo=halo,
                                jit_flags={},
                                n_threads=1)
        sut = traversals._fill_halos_vector
        thread_id = 0

        # act
        sut(thread_id, *meta_and_data, *fill_halos)

        # assert
        if halo == 1:
            return
        if side == LEFT:
            np.testing.assert_array_equal(field.data[0][:(halo - 1)],
                                          data[-(halo - 1):])
        elif side == RIGHT:
            np.testing.assert_array_equal(field.data[0][-(halo - 1):],
                                          data[:(halo - 1)])
        else:
            raise ValueError()
Example #4
0
def make_laplacian(non_unit_g_factor: bool, options: Options,
                   traversals: Traversals):
    if not options.non_zero_mu_coeff:

        @numba.njit(**options.jit_flags)
        def apply(_1, _2, _3, _4, _5):
            return
    else:
        idx = indexers[traversals.n_dims]
        apply_vector = traversals.apply_vector()

        formulae_laplacian = tuple([
            __make_laplacian(options.jit_flags, idx.at[i], options.epsilon,
                             non_unit_g_factor)
            if i < traversals.n_dims else None for i in range(MAX_DIM_NUM)
        ])

        @numba.njit(**options.jit_flags)
        def apply(advector, advectee, advectee_bc, null_vecfield_bc):
            null_vecfield = advector
            null_scalarfield = advectee
            return apply_vector(*formulae_laplacian, *advector, *advectee,
                                *advectee_bc, *null_vecfield,
                                *null_vecfield_bc, *null_scalarfield,
                                *null_vecfield_bc)

    return apply
Example #5
0
    def test_vector_2d(self, halo, n_threads):
        # arrange
        grid = (4, 2)
        data = (np.array([
            [1, 6],
            [2, 7],
            [3, 8],
            [4, 9],
            [5, 10],
        ]), np.array([
            [1, 5, 9],
            [2, 6, 10],
            [3, 7, 11],
            [4, 8, 12],
        ]))
        bc = (PeriodicBoundaryCondition(), PolarBoundaryCondition(grid, 0, 1))
        field = VectorField(data, halo, bc)
        meta_and_data, fill_halos = field.impl
        traversals = Traversals(grid=grid,
                                halo=halo,
                                jit_flags={},
                                n_threads=n_threads)
        sut = traversals._fill_halos_vector

        # act
        for thread_id in numba.prange(n_threads):
            sut(thread_id, *meta_and_data, *fill_halos)

        # assert
        print(field.data[0].shape)
        print(field.data[0])
        print(field.data[1].shape)
        print(field.data[1])
Example #6
0
def make_laplacian(non_unit_g_factor: bool, options: Options,
                   traversals: Traversals):
    if not options.non_zero_mu_coeff:

        @numba.njit(**options.jit_flags)
        def apply(_flux, _psi, _psi_bc, _GC_corr, _vec_bc):
            return
    else:
        idx = indexers[traversals.n_dims]
        apply_vector = traversals.apply_vector()

        formulae_laplacian = tuple([
            __make_laplacian(options.jit_flags, idx.at[i], options.epsilon,
                             non_unit_g_factor, traversals.n_dims)
            if i < traversals.n_dims else null_vector_formula
            for i in range(MAX_DIM_NUM)
        ])

        @numba.njit(**options.jit_flags)
        def apply(GC_phys, psi, psi_bc, null_vecfield_bc):
            null_vecfield = GC_phys
            null_scalarfield = psi
            return apply_vector(*formulae_laplacian, *GC_phys, *psi, *psi_bc,
                                *null_vecfield, *null_vecfield_bc,
                                *null_scalarfield, *null_vecfield_bc)

    return apply
Example #7
0
    def test_scalar_1d(self, data, halo, side):
        # arrange
        field = ScalarField(data, halo, (PeriodicBoundaryCondition(),))
        meta_and_data, fill_halos = field.impl
        traversals = Traversals(grid=data.shape, halo=halo, jit_flags={})
        sut, _ = traversals.make_boundary_conditions()

        # act
        sut(*meta_and_data, *fill_halos)

        # assert
        if side == LEFT:
            np.testing.assert_array_equal(field.data[:halo], data[-halo:])
        elif side == RIGHT:
            np.testing.assert_array_equal(field.data[-halo:], data[:halo])
        else:
            raise ValueError()
Example #8
0
    def test_apply_vector(n_threads, halo, grid):
        n_dims = len(grid)
        if n_dims == 1 and n_threads > 1:
            return

        # arrange
        traversals = Traversals(grid, halo, jit_flags, n_threads)
        sut = traversals.apply_vector()

        scl_null_arg_impl = ScalarField.make_null(n_dims).impl
        vec_null_arg_impl = VectorField.make_null(n_dims).impl

        if n_dims == 1:
            data = (np.zeros(grid[0] + 1), )
        elif n_dims == 2:
            data = (np.zeros(
                (grid[0] + 1, grid[1])), np.zeros((grid[0], grid[1] + 1)))
        else:
            raise NotImplementedError()

        out = VectorField(data, halo,
                          [ConstantBoundaryCondition(np.nan)] * n_dims)

        # act
        sut(_cell_id_vector, _cell_id_vector, *out.impl[0],
            *scl_null_arg_impl[0], *scl_null_arg_impl[1],
            *vec_null_arg_impl[0], *vec_null_arg_impl[1],
            *scl_null_arg_impl[0], *scl_null_arg_impl[1])

        # assert
        halos = ((halo - 1, halo), (halo, halo - 1))
        for d in range(n_dims):
            data = out.get_component(d)
            focus = tuple(-halos[d][i] for i in range(n_dims))
            for i in range(halos[d][0], halos[d][0] + data.shape[0]):
                for j in (-1, ) if n_dims == 1 else range(
                        halos[d][1], halos[d][1] + data.shape[1]):
                    value = indexers[n_dims].at[0](focus, data, i, j)
                    assert value == cell_id(i, j)

        assert scl_null_arg_impl[0][0][meta_halo_valid]
        assert vec_null_arg_impl[0][0][meta_halo_valid]
        assert not out.impl[0][0][meta_halo_valid]
Example #9
0
    def test_scalar_2d(self, halo, n_threads):
        # arrange
        data = np.array([[1, 6], [2, 7], [3, 8], [4, 9]])
        bc = (PeriodicBoundaryCondition(),
              PolarBoundaryCondition(data.shape, 0, 1))
        field = ScalarField(data, halo, bc)
        meta_and_data, fill_halos = field.impl
        traversals = Traversals(grid=data.shape,
                                halo=halo,
                                jit_flags={},
                                n_threads=n_threads)
        sut = traversals._fill_halos_scalar

        # act
        for thread_id in numba.prange(n_threads):
            sut(thread_id, *meta_and_data, *fill_halos)

        # assert
        np.testing.assert_array_equal(
            field.data[halo:-halo, :halo],
            np.roll(field.get()[:, :halo], data.shape[0] // 2, axis=0))
        np.testing.assert_array_equal(
            field.data[halo:-halo, -halo:],
            np.roll(field.get()[:, -halo:], data.shape[0] // 2, axis=0))
Example #10
0
def make_step_impl(options, non_unit_g_factor, grid, n_threads):
    n_iters = options.n_iters
    n_dims = len(grid)
    halo = options.n_halo
    non_zero_mu_coeff = options.non_zero_mu_coeff
    flux_corrected_transport = options.flux_corrected_transport

    traversals = Traversals(grid, halo, options.jit_flags, n_threads=n_threads)

    upwind = make_upwind(options, non_unit_g_factor, traversals)
    flux_first_pass = make_flux_first_pass(options, traversals)
    flux_subsequent = make_flux_subsequent(options, traversals)
    antidiff = make_antidiff(non_unit_g_factor, options, traversals)
    laplacian = make_laplacian(non_unit_g_factor, options, traversals)
    fct_psi_min = make_psi_extremum(min, options, traversals)
    fct_psi_max = make_psi_extremum(max, options, traversals)
    fct_beta_down = make_beta(min, non_unit_g_factor, options, traversals)
    fct_beta_up = make_beta(max, non_unit_g_factor, options, traversals)
    fct_correction = make_correction(options, traversals)

    @numba.njit(**options.jit_flags)
    def axpy(out_meta, out0, out1, a, x_meta, x0, x1, y_meta, y0, y1):
        out0[:] = a[0] * x0[:] + y0[:]
        if n_dims > 1:
            out1[:] = a[1] * x1[:] + y1[:]
        out_meta[meta_halo_valid] = False

    @numba.njit(**options.jit_flags)
    def step(nt, mu_coeff, advectee, advectee_bc, advector, advector_bc,
             g_factor, g_factor_bc, vectmp_a, vectmp_a_bc, vectmp_b,
             vectmp_b_bc, vectmp_c, vectmp_c_bc, psi_min, psi_min_bc, psi_max,
             psi_max_bc, beta_up, beta_up_bc, beta_down, beta_down_bc):
        vec_bc = advector_bc
        null_vecfield = advector
        null_vecfield_bc = vec_bc

        time = clock()
        for _ in range(nt):
            if non_zero_mu_coeff:
                advector_orig = advector
                advector = vectmp_c
            for it in range(n_iters):
                if it == 0:
                    if flux_corrected_transport:
                        fct_psi_min(psi_min, advectee, advectee_bc,
                                    null_vecfield, null_vecfield_bc)
                        fct_psi_max(psi_max, advectee, advectee_bc,
                                    null_vecfield, null_vecfield_bc)
                    if non_zero_mu_coeff:
                        laplacian(advector, advectee, advectee_bc,
                                  null_vecfield_bc)
                        axpy(*advector, mu_coeff, *advector, *advector_orig)
                    flux_first_pass(vectmp_a, advector, advectee, advectee_bc,
                                    vec_bc)
                    flux = vectmp_a
                else:
                    if it == 1:
                        advector_oscilatory = advector
                        advector_nonoscilatory = vectmp_a
                        flux = vectmp_b
                    elif it % 2 == 0:
                        advector_oscilatory = vectmp_a
                        advector_nonoscilatory = vectmp_b
                        flux = vectmp_a
                    else:
                        advector_oscilatory = vectmp_b
                        advector_nonoscilatory = vectmp_a
                        flux = vectmp_b
                    antidiff(advector_nonoscilatory, advectee, advectee_bc,
                             advector_oscilatory, vec_bc, g_factor,
                             g_factor_bc)
                    flux_subsequent(flux, advectee, advectee_bc,
                                    advector_nonoscilatory, vec_bc)
                    if flux_corrected_transport:
                        fct_beta_down(beta_down, flux, vec_bc, advectee,
                                      advectee_bc, psi_min, psi_min_bc,
                                      g_factor, g_factor_bc)
                        fct_beta_up(beta_up, flux, vec_bc, advectee,
                                    advectee_bc, psi_max, psi_max_bc, g_factor,
                                    g_factor_bc)
                        fct_correction(advector_nonoscilatory, vec_bc,
                                       beta_down, beta_down_bc, beta_up,
                                       beta_up_bc)
                        flux_subsequent(flux, advectee, advectee_bc,
                                        advector_nonoscilatory, vec_bc)
                upwind(advectee, flux, vec_bc, g_factor, g_factor_bc)
            if non_zero_mu_coeff:
                advector = advector_orig
        return (clock() - time) / nt

    return step
Example #11
0
def make_step_impl(options, non_unit_g_factor, grid):
    n_iters = options.n_iters
    n_dims = len(grid)
    halo = options.n_halo
    non_zero_mu_coeff = options.non_zero_mu_coeff
    flux_corrected_transport = options.flux_corrected_transport

    traversals = Traversals(grid, halo, options.jit_flags)

    upwind = make_upwind(options, non_unit_g_factor, traversals)
    flux_first_pass = make_flux_first_pass(options, traversals)
    flux_subsequent = make_flux_subsequent(options, traversals)
    antidiff = make_antidiff(non_unit_g_factor, options, traversals)
    laplacian = make_laplacian(non_unit_g_factor, options, traversals)
    fct_psi_min = make_psi_extremum(min, options, traversals)
    fct_psi_max = make_psi_extremum(max, options, traversals)
    fct_beta_down = make_beta(min, non_unit_g_factor, options, traversals)
    fct_beta_up = make_beta(max, non_unit_g_factor, options, traversals)
    fct_correction = make_correction(options, traversals)

    @numba.njit(**options.jit_flags)
    def axpy(out_meta, out0, out1, a, x_meta, x0, x1, y_meta, y0, y1):
        out0[:] = a * x0[:] + y0[:]
        if n_dims > 1:
            out1[:] = a * x1[:] + y1[:]
        out_meta[meta_halo_valid] = False

    @numba.njit(**options.jit_flags)
    def step(nt, mu_coeff,
             psi, psi_bc,
             GC_phys, GC_phys_bc,
             g_factor, g_factor_bc,
             vectmp_a, vectmp_a_bc,
             vectmp_b, vectmp_b_bc,
             vectmp_c, vectmp_c_bc,
             psi_min, psi_min_bc,
             psi_max, psi_max_bc,
             beta_up, beta_up_bc,
             beta_down, beta_down_bc
             ):
        vec_bc = GC_phys_bc
        null_vecfield = GC_phys
        null_vecfield_bc = vec_bc

        for _ in range(nt):
            if non_zero_mu_coeff:
                GC_orig = GC_phys
                GC_phys = vectmp_c
            for it in range(n_iters):
                if it == 0:
                    if flux_corrected_transport:
                        fct_psi_min(psi_min, psi, psi_bc, null_vecfield, null_vecfield_bc)
                        fct_psi_max(psi_max, psi, psi_bc, null_vecfield, null_vecfield_bc)
                    if non_zero_mu_coeff:
                        laplacian(GC_phys, psi, psi_bc, null_vecfield_bc)
                        axpy(*GC_phys, mu_coeff, *GC_phys, *GC_orig)
                    flux_first_pass(vectmp_a, GC_phys, psi, psi_bc, vec_bc)
                    flux = vectmp_a
                else:
                    if it == 1:
                        GC_unco = GC_phys
                        GC_corr = vectmp_a
                        flux = vectmp_b
                    elif it % 2 == 0:
                        GC_unco = vectmp_a
                        GC_corr = vectmp_b
                        flux = vectmp_a
                    else:
                        GC_unco = vectmp_b
                        GC_corr = vectmp_a
                        flux = vectmp_b
                    antidiff(GC_corr, psi, psi_bc, GC_unco, vec_bc, g_factor, g_factor_bc)
                    flux_subsequent(flux, psi, psi_bc, GC_corr, vec_bc)
                    if flux_corrected_transport:
                        fct_beta_down(beta_down, flux, vec_bc, psi, psi_bc, psi_min, psi_min_bc, g_factor, g_factor_bc)
                        fct_beta_up(beta_up, flux, vec_bc, psi, psi_bc, psi_max, psi_max_bc, g_factor, g_factor_bc)
                        fct_correction(GC_corr, vec_bc, beta_down, beta_down_bc, beta_up, beta_up_bc)
                        flux_subsequent(flux, psi, psi_bc, GC_corr, vec_bc)
                upwind(psi, flux, vec_bc, g_factor, g_factor_bc)
            if non_zero_mu_coeff:
                GC_phys = GC_orig

    return step