Source code for struphy.propagators.current_coupling_5d_density

import logging
from dataclasses import dataclass

from feectools.ddm.mpi import mpi as MPI
from feectools.linalg.solvers import inverse
from line_profiler import profile

from struphy.feec import preconditioner
from struphy.io.options import LiteralOptions, OptionsBase
from struphy.linear_algebra.solver import SolverParameters
from struphy.models.variables import FEECVariable, PICVariable
from struphy.pic.accumulation import accum_kernels_gc
from struphy.pic.accumulation.filter import FilterParameters
from struphy.pic.accumulation.particles_to_grid import Accumulator
from struphy.propagators.base import Propagator
from struphy.utils.pyccel import Pyccelkernel
from struphy.utils.utils import check_option

logger = logging.getLogger("struphy")


[docs] class CurrentCoupling5DDensity(Propagator): r""":ref:`FEEC <gempic>` discretization of the following equations: find :math:`\mathbf U \in \{H(\textnormal{curl}), H(\textnormal{div}), (H^1)^3\}` and :math:`\mathbf B \in H(\textnormal{div})` such that .. math:: \int \rho_0 \frac{\partial \tilde{\mathbf U}}{\partial t} \cdot \mathbf V \, \textnormal{d} \mathbf{x} = \frac{A_\textnormal{h}}{A_b} \frac{1}{\epsilon} \iiint f^\text{vol} \left(1 - \frac{B_\parallel}{B^*_\parallel}\right) \tilde{\mathbf U} \times \mathbf B_f \cdot \mathbf V \, \textnormal{d} \mathbf{x} \textnormal{d} v_\parallel \textnormal{d} \mu \quad \forall \,\mathbf V \in \{H(\textnormal{curl}), H(\textnormal{div}), (H^1)^3\}\,, FE coefficients update: .. math:: \mathbf u^{n+1} - \mathbf u^n = -\frac{A_\textnormal{h}}{A_b} \frac{1}{\epsilon} \mathbb{L}²{\mathbb{B}}^\times_f \mathbb{N}(1/g) \mathbb{W} \mathbb{N}\left(1- \frac{\hat B^0_\parallel}{\hat B^{*0} _\parallel}\right) (\mathbb{L}²)^\top \frac{\Delta t}{2} \cdot (\mathbf u^{n+1} + \mathbf u^n) \,. For the detail explanation of the notations, see `2022_DriftKineticCurrentCoupling <https://gitlab.mpcdf.mpg.de/struphy/struphy-projects/-/blob/main/running-projects/2022_DriftKineticCurrentCoupling.md?ref_type=heads>`_. """
[docs] class Variables: """Container for variables advanced by :class:`CurrentCoupling5DDensity`. Attributes ---------- u : FEECVariable Fluid-like FEEC variable in one of ``"Hcurl"``, ``"Hdiv"``, or ``"H1vec"``. """ def __init__(self): self._u: FEECVariable = None @property def u(self) -> FEECVariable: return self._u @u.setter def u(self, new): assert isinstance(new, FEECVariable) assert new.space in ("Hcurl", "Hdiv", "H1vec") self._u = new
def __init__( self, energetic_ions: PICVariable = None, b_tilde: FEECVariable = None, ): """ Parameters ---------- energetic_ions : PICVariable, default=None Energetic-ion particle distribution (``"Particles5D"`` space) providing the density source term. b_tilde : FEECVariable, default=None Magnetic perturbation 1-form (``"Hcurl"`` space) entering the coupling term. If ``None``, only the equilibrium field is used. """ self.variables = self.Variables() self.energetic_ions = energetic_ions self.b_tilde = b_tilde
[docs] @dataclass(repr=False) class Options(OptionsBase): """Configuration options for :class:`CurrentCoupling5DDensity`. Parameters ---------- ep_scale : float, default=1.0 Scaling factor applied in the energetic-particle accumulation kernel. u_space : LiteralOptions.OptsVecSpace, default="Hdiv" FEEC space used for the unknown ``u`` variable. solver : LiteralOptions.OptsSymmSolver, default="pcg" Symmetric iterative solver used for the linear system. precond : LiteralOptions.OptsMassPrecond, default="MassMatrixPreconditioner" Preconditioner applied to the FEEC mass matrix. solver_params : SolverParameters, default=None Iterative-solver controls. If ``None``, defaults to ``SolverParameters()``. filter_params : FilterParameters, default=None Particle-to-grid filtering parameters used by the accumulator. If ``None``, defaults to ``FilterParameters()``. """ # propagator options ep_scale: float = 1.0 u_space: LiteralOptions.OptsVecSpace = "Hdiv" solver: LiteralOptions.OptsSymmSolver = "pcg" precond: LiteralOptions.OptsMassPrecond = "MassMatrixPreconditioner" solver_params: SolverParameters = None filter_params: FilterParameters = None def __post_init__(self): # checks check_option(self.u_space, LiteralOptions.OptsVecSpace) check_option(self.solver, LiteralOptions.OptsSymmSolver) check_option(self.precond, LiteralOptions.OptsMassPrecond) assert isinstance(self.ep_scale, float) # defaults if self.solver_params is None: self.solver_params = SolverParameters() if self.filter_params is None: self.filter_params = FilterParameters()
@property def options(self) -> Options: if not hasattr(self, "_options"): self._options = self.Options() return self._options @options.setter def options(self, new): assert isinstance(new, self.Options) self._options = new logger.info(f"\nNew options for propagator '{self.__class__.__name__}':\n{self._options}") @profile def allocate(self): if self.options.u_space == "H1vec": self._u_form_int = 0 else: self._u_form_int = int(self.derham.space_to_form[self.options.u_space]) # call operatros id_M = "M" + self.derham.space_to_form[self.options.u_space] + "n" self._A = getattr(self.mass_ops, id_M) # magnetic equilibrium field unit_b1 = self.projected_equil.unit_b1 curl_unit_b1 = self.projected_equil.curl_unit_b1 self._b2 = self.projected_equil.b2 # scaling factor epsilon = self.energetic_ions.species.equation_params.epsilon # temporary vectors to avoid memory allocation self._b_full = self._b2.space.zeros() self._rhs_v = self.variables.u.spline.vector.space.zeros() self._u_new = self.variables.u.spline.vector.space.zeros() # define Accumulator and arguments self._ACC = Accumulator( self.energetic_ions.particles, self.options.u_space, Pyccelkernel(accum_kernels_gc.cc_lin_mhd_5d_D), self.mass_ops, self.domain.args_domain, add_vector=False, symmetry="asym", filter_params=self.options.filter_params, ) self._args_accum_kernel = ( epsilon, self.options.ep_scale, self._b_full[0]._data, self._b_full[1]._data, self._b_full[2]._data, unit_b1[0]._data, unit_b1[1]._data, unit_b1[2]._data, curl_unit_b1[0]._data, curl_unit_b1[1]._data, curl_unit_b1[2]._data, self._u_form_int, ) # Preconditioner if self.options.precond is None: pc = None else: pc_class = getattr(preconditioner, self.options.precond) pc = pc_class(getattr(self.mass_ops, id_M)) # linear solver self._A_inv = inverse( self._A, self.options.solver, pc=pc, tol=self.options.solver_params.tol, maxiter=self.options.solver_params.maxiter, verbose=self.options.solver_params.verbose, ) def __call__(self, dt): # current FE coeffs un = self.variables.u.spline.vector # sum up total magnetic field b_full1 = b_eq + b_tilde (in-place) b_full = self._b2.copy(out=self._b_full) b_full += self.b_tilde.spline.vector b_full.update_ghost_regions() self._ACC( *self._args_accum_kernel, ) # define system (M - dt/2 * A)*u^(n + 1) = (M + dt/2 * A)*u^n lhs = self._A - dt / 2 * self._ACC.operators[0] rhs = self._A + dt / 2 * self._ACC.operators[0] # solve linear system for updated u coefficients (in-place) rhs = rhs.dot(un, out=self._rhs_v) self._A_inv.linop = lhs _u = self._A_inv.solve(rhs, out=self._u_new) info = self._A_inv._info diffs = self.update_feec_variables(u=_u) if self.options.solver_params.info and MPI.COMM_WORLD.Get_rank() == 0: logger.info(f"Status for CurrentCoupling5DDensity: {info['success']}") logger.info(f"Iterations for CurrentCoupling5DDensity: {info['niter']}") logger.info(f"Maxdiff up for CurrentCoupling5DDensity: {diffs['u']}") logger.info("")