Source code for pde.solvers.explicit_mpi

"""Defines an explicit solver using multiprocessing via MPI.

TODO: Implement this not as a separate solver but as a separate numba_mpi backend

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

from __future__ import annotations

import copy
from typing import TYPE_CHECKING, Literal

import numpy as np

from ..tools.math import OnlineStatistics
from .euler import EulerSolver

if TYPE_CHECKING:
    from ..backends.base import BackendBase
    from ..pdes.base import PDEBase
    from ..tools.typing import StepperType, TField


[docs] class ExplicitMPISolver(EulerSolver): """Explicit Euler solver using MPI. Warning: This solver can only be used if MPI is properly installed. In particular, python scripts then need to be started using :code:`mpirun` or :code:`mpiexec`. Please refer to the documentation of your MPI distribution for details. The main idea of the solver is to take the full initial state in the main node (ID 0) and split the grid into roughly equal subgrids. The main node then distributes these subfields to all other nodes and each node creates the right hand side of the PDE for itself (and independently). Each node then advances the PDE independently, ensuring proper coupling to neighboring nodes via special boundary conditions, which exchange field values between sub grids. This is implemented by the :meth:`get_boundary_conditions` method of the sub grids, which takes the boundary conditions for the full grid and creates conditions suitable for the specific sub grid on the given node. The trackers (and thus all input and output) are only handled on the main node. Warning: The function providing the right hand side of the PDE needs to support MPI. This is automatically the case for local evaluations (which only use the field value at the current position), for the differential operators provided by :mod:`pde`, and integration of fields. Similarly, `post_step_hook` can only be used to do local modifications since the field data supplied to the function is local to each MPI node. Example: A minimal example using the MPI solver is .. code-block:: python from pde import DiffusionPDE, ScalarField, UnitGrid grid = UnitGrid([64, 64]) state = ScalarField.random_uniform(grid, 0.2, 0.3) eq = DiffusionPDE(diffusivity=0.1) result = eq.solve(state, t_range=10, dt=0.1, solver="explicit_mpi") if result is not None: # restrict the output to the main node result.plot() Saving this script as `multiprocessing.py`, a parallel simulation is started by .. code-block:: bash mpiexec -n 2 python3 multiprocessing.py Here, the number `2` determines the number of cores that will be used. Note that macOS might require an additional hint on how to connect the processes even when they are run on the same machine (e.g., your workstation). It might help to run :code:`mpiexec -n 2 -host localhost python3 multiprocessing.py` in this case """ name = "explicit_mpi" mpi_run = True def __init__( self, pde: PDEBase, # scheme: Literal["euler", "runge-kutta", "rk", "rk45"] = "euler", decomposition: Literal["auto"] | int | list[int] = "auto", *, backend: str | BackendBase = "auto", adaptive: bool = False, tolerance: float = 1e-4, ): """ Args: pde (:class:`~pde.pdes.base.PDEBase`): The partial differential equation that should be solved decomposition (str, int, or list of ints): Number of subdivision in each direction. Should be a list of length `grid.num_axes` specifying the number of nodes for this axis. If one value is `-1`, its value will be determined from the number of available nodes. A single integer is interpreted as the number of subdivisions along one axis. The default value `auto` tries to determine an optimal decomposition by minimizing communication between nodes. backend (str): The backend used for numerical operations adaptive (bool): Whether to use adaptive time stepping tolerance (float): Error tolerance for adaptive time stepping """ pde._mpi_synchronization = self._mpi_synchronization super().__init__(pde, backend=backend, adaptive=adaptive, tolerance=tolerance) self.decomposition = decomposition @property def _mpi_synchronization(self) -> bool: # type: ignore """Flag indicating whether MPI synchronization is required.""" from ..tools import mpi return mpi.parallel_run def _init_post_step_data(self) -> None: """Initialize the post step data for all nodes.""" from ..tools import mpi if mpi.is_main: self.info["post_step_data_list"] = [ copy.deepcopy(self.info["post_step_data"]) for _ in range(len(self.mesh)) ] else: self.info["post_step_data_list"] = None
[docs] def make_stepper(self, state: TField, dt=None) -> StepperType: """Create the executable stepping function produced by this solver. Args: state (:class:`~pde.fields.base.FieldBase`): An example for the state from which the grid and other information can be extracted dt (float): Initial time step. If `None`, this solver specifies 1e-3 as a default value. Returns: Function that can be called to advance the `state` from time `t_start` to time `t_end`. The function call signature is `(state: numpy.ndarray, t_start: float, t_end: float)` """ from ..grids._mesh import GridMesh from ..tools import mpi if not mpi.parallel_run: self._logger.warning( "Using `ExplicitMPISolver` without a proper multiprocessing run. " "Scripts need to be started with `mpiexec` to use multiple cores." ) if dt is None: # support `None` as a default value, so the controller can signal that # the solver should use a default time step dt = 1e-3 if not self.adaptive: self._logger.warning( "Explicit solver configured for fixed time stepping did not " "receive any initial value for `dt`. Using dt=%g, but specifying " "a value or enabling adaptive stepping is advisable.", dt, ) self._select_backend(state) self.info["dt"] = float(dt) self.info["dt_adaptive"] = self.adaptive self.info["dt_statistics"] = OnlineStatistics() self.info["steps"] = 0 self.info["stochastic"] = getattr(self.pde, "is_sde", False) self.info["use_mpi"] = True # decompose the state into multiple cells self.mesh: GridMesh = GridMesh.from_grid(state.grid, self.decomposition) sub_state = self.mesh.extract_subfield(state) self.info["grid_decomposition"] = self.mesh.shape # create the inner stepping function # TODO: Use backend compilation inner_stepper = self._make_inner_stepper(sub_state) self._init_post_step_data() def wrapped_stepper(state: TField, t_start: float, t_end: float) -> float: """Advance `state` from `t_start` to `t_end` using the stepping function.""" nonlocal dt # `dt` stores value for the next call # retrieve last post_step_data and continue with this self.info["post_step_data"] = self.mesh.scatter( self.info["post_step_data_list"] ) # distribute the end time and the field to all nodes t_end = self.mesh.broadcast(t_end) substate_data = self.mesh.split_field_data_mpi(state.data) # Evolve the sub-state on each individual node. The nodes synchronize # field data via special boundary conditions and they synchronize the # maximal error via the error synchronizer. Apart from that, all nodes # work independently. t_last = inner_stepper(substate_data, t_start, t_end) # check whether t_last is the same for all processes t_list = self.mesh.gather(t_last) if t_list is not None and not np.isclose(min(t_list), max(t_list)): msg = f"Processes went out of sync: t_last={t_list}" raise RuntimeError(msg) # collect the data from all nodes post_step_data_list = self.mesh.gather(self.info["post_step_data"]) self.mesh.combine_field_data_mpi(substate_data, out=state.data) if mpi.is_main: self.info["post_step_data_list"] = post_step_data_list return t_last return wrapped_stepper # type: ignore