Source code for pde.solvers.crank_nicolson

"""Defines a Crank-Nicolson solver.

.. codeauthor:: David Zwicker <david.zwicker@ds.mpg.de>
"""

from __future__ import annotations

from typing import TYPE_CHECKING, Callable

import numba as nb
import numpy as np

from .base import ConvergenceError, SolverBase

if TYPE_CHECKING:
    from ..fields.base import FieldBase
    from ..pdes.base import PDEBase
    from ..tools.typing import BackendType, NumericArray


[docs] class CrankNicolsonSolver(SolverBase): """Crank-Nicolson solver.""" name = "crank-nicolson" def __init__( self, pde: PDEBase, *, maxiter: int = 100, maxerror: float = 1e-4, explicit_fraction: float = 0, backend: BackendType = "auto", ): """ Args: pde (:class:`~pde.pdes.base.PDEBase`): The partial differential equation that should be solved maxiter (int): The maximal number of iterations per step maxerror (float): The maximal error that is permitted in each step explicit_fraction (float): Hyperparameter determining the fraction of explicit time stepping in the implicit step. `explicit_fraction == 0` is the simple Crank-Nicolson scheme, while `explicit_fraction == 1` reduces to the explicit Euler method. Intermediate values can improve convergence. backend (str): Determines how the function is created. Accepted values are 'numpy` and 'numba'. Alternatively, 'auto' lets the code decide for the most optimal backend. """ super().__init__(pde, backend=backend) self.maxiter = maxiter self.maxerror = maxerror self.explicit_fraction = explicit_fraction def _make_single_step_fixed_dt( self, state: FieldBase, dt: float ) -> Callable[[NumericArray, float], None]: """Return a function doing a single step with an implicit Euler scheme. Args: state (:class:`~pde.fields.base.FieldBase`): An example for the state from which the grid and other information can be extracted dt (float): Time step of the implicit step """ if self.pde.is_sde: msg = "Cannot use implicit stepper with stochastic equation" raise RuntimeError(msg) self.info["function_evaluations"] = 0 self.info["scheme"] = "implicit-euler" self.info["stochastic"] = False rhs = self._make_pde_rhs(state, backend=self.backend) maxiter = int(self.maxiter) maxerror2 = self.maxerror**2 α = self.explicit_fraction # handle deterministic version of the pde def crank_nicolson_step(state_data: NumericArray, t: float) -> None: """Compiled inner loop for speed.""" nfev = 0 # count function evaluations # keep values at the current time t point used in iteration state_t = state_data.copy() rate_t = rhs(state_t, t) # new state is weighted average of explicit and Crank-Nicolson steps state_cn = state_t + dt / 2 * (rhs(state_data, t + dt) + rate_t) state_data[:] = α * state_data + (1 - α) * state_cn state_prev = np.empty_like(state_data) # fixed point iteration for improving state after dt for n in range(maxiter): state_prev[:] = state_data # keep previous state to judge convergence # new state is weighted average of explicit and Crank-Nicolson steps state_cn = state_t + dt / 2 * (rhs(state_data, t + dt) + rate_t) state_data[:] = α * state_data + (1 - α) * state_cn # calculate mean squared error err = 0.0 for j in range(state_data.size): diff: NumericArray = state_data.flat[j] - state_prev.flat[j] err += (diff.conjugate() * diff).real err /= state_data.size if err < maxerror2: # fix point iteration converged break else: with nb.objmode: self._logger.warning( "Crank-Nicolson step did not converge after %d iterations " "at t=%g (error=%g)", maxiter, t, err, ) msg = "Crank-Nicolson step did not converge." raise ConvergenceError(msg) nfev += n + 2 return crank_nicolson_step