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Cahn-Hilliad¤

exponax.reaction.CahnHilliard ¤

Bases: BaseStepper

Source code in exponax/reaction/_cahn_hilliard.py 
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class CahnHilliard(BaseStepper):
    diffusivity: float
    gamma: float
    first_order_coefficient: float
    third_order_coefficient: float
    dealiasing_fraction: float

    def __init__(
        self,
        num_spatial_dims: int,
        domain_extent: float,
        num_points: int,
        dt: float,
        *,
        diffusivity: float = 1e-2,
        gamma: float = 1e-3,
        first_order_coefficient: float = -1.0,
        third_order_coefficient: float = 1.0,
        order: int = 2,
        # Needs lower value due to cubic nonlinearity
        dealiasing_fraction: float = 1 / 2,
        num_circle_points: int = 16,
        circle_radius: float = 1.0,
    ):
        """
        Timestepper for the d-dimensional (`d ∈ {1, 2, 3}`) Cahn-Hilliard
        reaction-diffusion equation on periodic boundary conditions. This model
        is related to the Allen-Cahn equation. In 1d, it reads

        ```
            uₜ = ν ∂ₓₓ (c₃ u³ + c₁ u − γ uₓₓ)
        ```

        with `ν` the diffusivity, `c₁` the first order coefficient, `c₃` the
        third order coefficient, and `γ` the gamma parameter. The state always
        only has one channel. In higher dimensions, the equation reads

        ```
            uₜ = ν Δ (c₃ u³ + c₁ u - γ Δu)
        ```

        Since the Laplace operator is self-multiplied, there will be spatial
        mixing.

        **Arguments:**

        - `num_spatial_dims`: The number of spatial dimensions `d`.
        - `domain_extent`: The size of the domain `L`; in higher dimensions
            the domain is assumed to be a scaled hypercube `Ω = (0, L)ᵈ`.
        - `num_points`: The number of points `N` used to discretize the
            domain. This **includes** the left boundary point and **excludes**
            the right boundary point. In higher dimensions; the number of points
            in each dimension is the same. Hence, the total number of degrees of
            freedom is `Nᵈ`.
        - `dt`: The timestep size `Δt` between two consecutive states.
        - `diffusivity`: The diffusivity `ν`.
        - `gamma`: The gamma parameter `γ`.
        - `first_order_coefficient`: The first order coefficient `c₁`.
        - `third_order_coefficient`: The third order coefficient `c₃`.
        - `dealiasing_fraction`: The fraction of the highest wavenumbers to
            dealias. Default is `1/2` because the default polynomial has a
            highest degree of 3.
        - `order`: The order of the Exponential Time Differencing Runge
            Kutta method. Must be one of {0, 1, 2, 3, 4}. The option `0` only
            solves the linear part of the equation. Use higher values for higher
            accuracy and stability. The default choice of `2` is a good
            compromise for single precision floats.
        - `num_circle_points`: How many points to use in the complex contour
            integral method to compute the coefficients of the exponential time
            differencing Runge Kutta method. Default: 16.
        - `circle_radius`: The radius of the contour used to compute the
            coefficients of the exponential time differencing Runge Kutta
            method. Default: 1.0.

        **Notes:**

        - See
            https://github.com/chebfun/chebfun/blob/db207bc9f48278ca4def15bf90591bfa44d0801d/spin.m#L89
            for an example IC of the Cahn-Hilliard in 1d.
        """
        self.diffusivity = diffusivity
        self.gamma = gamma
        self.first_order_coefficient = first_order_coefficient
        self.third_order_coefficient = third_order_coefficient
        self.dealiasing_fraction = dealiasing_fraction
        super().__init__(
            num_spatial_dims=num_spatial_dims,
            domain_extent=domain_extent,
            num_points=num_points,
            dt=dt,
            num_channels=1,
            order=order,
            num_circle_points=num_circle_points,
            circle_radius=circle_radius,
        )

    def _build_linear_operator(
        self,
        derivative_operator: Complex[Array, "D ... (N//2)+1"],
    ) -> Complex[Array, "1 ... (N//2)+1"]:
        laplace = build_laplace_operator(derivative_operator, order=2)
        linear_operator = (
            self.diffusivity
            * laplace
            * (self.first_order_coefficient - self.gamma * laplace)
        )
        return linear_operator

    def _build_nonlinear_fun(
        self,
        derivative_operator: Complex[Array, "D ... (N//2)+1"],
    ) -> CahnHilliardNonlinearFun:
        return CahnHilliardNonlinearFun(
            self.num_spatial_dims,
            self.num_points,
            derivative_operator=derivative_operator,
            dealiasing_fraction=self.dealiasing_fraction,
            scale=self.diffusivity * self.third_order_coefficient,
        )
__init__ ¤
__init__(
    num_spatial_dims: int,
    domain_extent: float,
    num_points: int,
    dt: float,
    *,
    diffusivity: float = 0.01,
    gamma: float = 0.001,
    first_order_coefficient: float = -1.0,
    third_order_coefficient: float = 1.0,
    order: int = 2,
    dealiasing_fraction: float = 1 / 2,
    num_circle_points: int = 16,
    circle_radius: float = 1.0
)

Timestepper for the d-dimensional (d ∈ {1, 2, 3}) Cahn-Hilliard reaction-diffusion equation on periodic boundary conditions. This model is related to the Allen-Cahn equation. In 1d, it reads

    uₜ = ν ∂ₓₓ (c₃ u³ + c₁ u − γ uₓₓ)

with ν the diffusivity, c₁ the first order coefficient, c₃ the third order coefficient, and γ the gamma parameter. The state always only has one channel. In higher dimensions, the equation reads

    uₜ = ν Δ (c₃ u³ + c₁ u - γ Δu)

Since the Laplace operator is self-multiplied, there will be spatial mixing.

Arguments:

  • num_spatial_dims: The number of spatial dimensions d.
  • domain_extent: The size of the domain L; in higher dimensions the domain is assumed to be a scaled hypercube Ω = (0, L)ᵈ.
  • num_points: The number of points N used to discretize the domain. This includes the left boundary point and excludes the right boundary point. In higher dimensions; the number of points in each dimension is the same. Hence, the total number of degrees of freedom is Nᵈ.
  • dt: The timestep size Δt between two consecutive states.
  • diffusivity: The diffusivity ν.
  • gamma: The gamma parameter γ.
  • first_order_coefficient: The first order coefficient c₁.
  • third_order_coefficient: The third order coefficient c₃.
  • dealiasing_fraction: The fraction of the highest wavenumbers to dealias. Default is 1/2 because the default polynomial has a highest degree of 3.
  • order: The order of the Exponential Time Differencing Runge Kutta method. Must be one of {0, 1, 2, 3, 4}. The option 0 only solves the linear part of the equation. Use higher values for higher accuracy and stability. The default choice of 2 is a good compromise for single precision floats.
  • num_circle_points: How many points to use in the complex contour integral method to compute the coefficients of the exponential time differencing Runge Kutta method. Default: 16.
  • circle_radius: The radius of the contour used to compute the coefficients of the exponential time differencing Runge Kutta method. Default: 1.0.

Notes:

  • See https://github.com/chebfun/chebfun/blob/db207bc9f48278ca4def15bf90591bfa44d0801d/spin.m#L89 for an example IC of the Cahn-Hilliard in 1d.
Source code in exponax/reaction/_cahn_hilliard.py 
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def __init__(
    self,
    num_spatial_dims: int,
    domain_extent: float,
    num_points: int,
    dt: float,
    *,
    diffusivity: float = 1e-2,
    gamma: float = 1e-3,
    first_order_coefficient: float = -1.0,
    third_order_coefficient: float = 1.0,
    order: int = 2,
    # Needs lower value due to cubic nonlinearity
    dealiasing_fraction: float = 1 / 2,
    num_circle_points: int = 16,
    circle_radius: float = 1.0,
):
    """
    Timestepper for the d-dimensional (`d ∈ {1, 2, 3}`) Cahn-Hilliard
    reaction-diffusion equation on periodic boundary conditions. This model
    is related to the Allen-Cahn equation. In 1d, it reads

    ```
        uₜ = ν ∂ₓₓ (c₃ u³ + c₁ u − γ uₓₓ)
    ```

    with `ν` the diffusivity, `c₁` the first order coefficient, `c₃` the
    third order coefficient, and `γ` the gamma parameter. The state always
    only has one channel. In higher dimensions, the equation reads

    ```
        uₜ = ν Δ (c₃ u³ + c₁ u - γ Δu)
    ```

    Since the Laplace operator is self-multiplied, there will be spatial
    mixing.

    **Arguments:**

    - `num_spatial_dims`: The number of spatial dimensions `d`.
    - `domain_extent`: The size of the domain `L`; in higher dimensions
        the domain is assumed to be a scaled hypercube `Ω = (0, L)ᵈ`.
    - `num_points`: The number of points `N` used to discretize the
        domain. This **includes** the left boundary point and **excludes**
        the right boundary point. In higher dimensions; the number of points
        in each dimension is the same. Hence, the total number of degrees of
        freedom is `Nᵈ`.
    - `dt`: The timestep size `Δt` between two consecutive states.
    - `diffusivity`: The diffusivity `ν`.
    - `gamma`: The gamma parameter `γ`.
    - `first_order_coefficient`: The first order coefficient `c₁`.
    - `third_order_coefficient`: The third order coefficient `c₃`.
    - `dealiasing_fraction`: The fraction of the highest wavenumbers to
        dealias. Default is `1/2` because the default polynomial has a
        highest degree of 3.
    - `order`: The order of the Exponential Time Differencing Runge
        Kutta method. Must be one of {0, 1, 2, 3, 4}. The option `0` only
        solves the linear part of the equation. Use higher values for higher
        accuracy and stability. The default choice of `2` is a good
        compromise for single precision floats.
    - `num_circle_points`: How many points to use in the complex contour
        integral method to compute the coefficients of the exponential time
        differencing Runge Kutta method. Default: 16.
    - `circle_radius`: The radius of the contour used to compute the
        coefficients of the exponential time differencing Runge Kutta
        method. Default: 1.0.

    **Notes:**

    - See
        https://github.com/chebfun/chebfun/blob/db207bc9f48278ca4def15bf90591bfa44d0801d/spin.m#L89
        for an example IC of the Cahn-Hilliard in 1d.
    """
    self.diffusivity = diffusivity
    self.gamma = gamma
    self.first_order_coefficient = first_order_coefficient
    self.third_order_coefficient = third_order_coefficient
    self.dealiasing_fraction = dealiasing_fraction
    super().__init__(
        num_spatial_dims=num_spatial_dims,
        domain_extent=domain_extent,
        num_points=num_points,
        dt=dt,
        num_channels=1,
        order=order,
        num_circle_points=num_circle_points,
        circle_radius=circle_radius,
    )
__call__ ¤
__call__(
    u: Float[Array, "C ... N"]
) -> Float[Array, "C ... N"]

Performs a check

Source code in exponax/_base_stepper.py 
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def __call__(
    self,
    u: Float[Array, "C ... N"],
) -> Float[Array, "C ... N"]:
    """
    Performs a check
    """
    expected_shape = (self.num_channels,) + spatial_shape(
        self.num_spatial_dims, self.num_points
    )
    if u.shape != expected_shape:
        raise ValueError(
            f"Expected shape {expected_shape}, got {u.shape}. For batched operation use `jax.vmap` on this function."
        )
    return self.step(u)