Source code for struphy.models.variational_compressible_fluid

import copy

import cunumpy as xp
from feectools.ddm.mpi import mpi as MPI

from struphy.feec.mass import L2Projector
from struphy.feec.variational_utilities import (
    InternalEnergyEvaluator,
)
from struphy.io.options import BaseUnits, LiteralOptions
from struphy.models.base import StruphyModel
from struphy.models.scalars import BilinearEnergyFEEC, FunctionScalarFEEC, Scalars
from struphy.models.species import (
    FluidSpecies,
)
from struphy.models.variables import FEECVariable
from struphy.propagators.base import Propagator
from struphy.propagators.variational_density_evolve import VariationalDensityEvolve
from struphy.propagators.variational_entropy_evolve import VariationalEntropyEvolve
from struphy.propagators.variational_momentum_advection import VariationalMomentumAdvection

rank = MPI.COMM_WORLD.Get_rank()


[docs] class VariationalCompressibleFluid(StruphyModel): """Fully compressible fluid equations discretized with a variational method. Parameters ---------- base_units: BaseUnits Base units for normalization (default: BaseUnits()) mass_number: float Mass number (in units of Proton mass) of the fluid species (default: 1.0) """ @classmethod def model_type(cls) -> LiteralOptions.ModelTypes: return "Fluid" ## species class Fluid(FluidSpecies): def __init__(self, mass_number: float = 1.0): self.density = FEECVariable(space="L2") self.velocity = FEECVariable(space="H1vec") self.entropy = FEECVariable(space="L2") self.init_variables(mass_number=mass_number) ## propagators class Propagators: def __init__( self, s: FEECVariable = None, rho: FEECVariable = None, ): self.variat_dens = VariationalDensityEvolve(s=s) self.variat_mom = VariationalMomentumAdvection() self.variat_ent = VariationalEntropyEvolve(rho=rho) ## abstract methods def __init__(self, base_units: BaseUnits = BaseUnits(), mass_number: float = 1.0): # 0. store input parameters self.params = copy.deepcopy(locals()) # 1. instantiate all species self.fluid = self.Fluid(mass_number=mass_number) # 2. derive units (must be done after instantiating species to access charge and mass numbers) self.setup_equation_params(base_units=base_units) # 3. instantiate all propagators self.propagators = self.Propagators(s=self.fluid.entropy, rho=self.fluid.density) # 4. assign variables to propagators self.propagators.variat_dens.variables.rho = self.fluid.density self.propagators.variat_dens.variables.u = self.fluid.velocity self.propagators.variat_mom.variables.u = self.fluid.velocity self.propagators.variat_ent.variables.s = self.fluid.entropy self.propagators.variat_ent.variables.u = self.fluid.velocity # 5. define scalars to be tracked during simulation kinetic_energy = BilinearEnergyFEEC(self.fluid.velocity, bilinear_form_name="WMMnew") thermo_energy = FunctionScalarFEEC(self.update_thermo_energy) total_energy = kinetic_energy + thermo_energy self.scalars = Scalars( en_U=kinetic_energy, en_thermo=thermo_energy, en_tot=total_energy, ) @property def bulk_species(self): return self.fluid @property def velocity_scale(self): return "alfvén" def allocate_helpers(self): projV3 = L2Projector("L2", Propagator.mass_ops) def f(e1, e2, e3): return 1 f = xp.vectorize(f) self._integrator = projV3(f) self._energy_evaluator = InternalEnergyEvaluator(Propagator.derham, self.propagators.variat_ent.options.gamma) # default parameters def generate_default_parameter_file(self, path=None, prompt=True): params_path = super().generate_default_parameter_file(path=path, prompt=prompt) new_file = [] with open(params_path, "r") as f: for line in f: if "variat_dens.Options" in line: new_file += [ "model.propagators.variat_dens.options = model.propagators.variat_dens.Options(model='full')\n", ] elif "entropy.add_background" in line: new_file += ["model.fluid.density.add_background(FieldsBackground())\n"] new_file += [line] else: new_file += [line] with open(params_path, "w") as f: for line in new_file: f.write(line) def update_thermo_energy(self): """Reuse tmp used in VariationalEntropyEvolve to compute the thermodynamical energy. :meta private: """ en_prop = self.propagators.variat_ent self._energy_evaluator.sf.vector = self.fluid.entropy.spline.vector self._energy_evaluator.rhof.vector = self.fluid.density.spline.vector sf_values = self._energy_evaluator.sf.eval_tp_fixed_loc( self._energy_evaluator.integration_grid_spans, self._energy_evaluator.integration_grid_bd, out=self._energy_evaluator._sf_values, ) rhof_values = self._energy_evaluator.rhof.eval_tp_fixed_loc( self._energy_evaluator.integration_grid_spans, self._energy_evaluator.integration_grid_bd, out=self._energy_evaluator._rhof_values, ) e = self.__ener ener_values = en_prop._proj_rho2_metric_term * e(rhof_values, sf_values) en_prop._get_L2dofs_V3(ener_values, dofs=en_prop._linear_form_dl_ds) en_thermo = self._integrator.inner(en_prop._linear_form_dl_ds) return en_thermo def __ener(self, rho, s): """Themodynamical energy as a function of rho and s, usign the perfect gaz hypothesis E(rho, s) = rho^gamma*exp(s/rho)""" return xp.power(rho, self.propagators.variat_ent.options.gamma) * xp.exp(s / rho)
[docs] @classmethod def doc_pde(cls): r"""**PDEs solved by model:** Continuity: .. math:: \partial_t \rho + \nabla \cdot (\rho \mathbf{u}) = 0 Momentum: .. math:: \partial_t (\rho \mathbf{u}) + \nabla \cdot (\rho \mathbf{u} \otimes \mathbf{u}) + \rho \nabla \frac{(\rho \mathcal{U}(\rho, s))}{\partial \rho} + s \nabla \frac{(\rho \mathcal{U}(\rho, s))}{\partial s} = 0 Entropy: .. math:: \partial_t s + \nabla \cdot (s \mathbf{u}) = 0 where the internal energy per unit mass is :math:`\mathcal U(\rho) = \rho^{\gamma-1} \exp(s / \rho)`. """
[docs] @classmethod def doc_normalization(cls): r"""The model uses Alfvén-speed scaling for the flow variables together with separate units for internal energy and entropy: .. math:: \hat u = \hat v_A,\qquad \hat{\mathcal U}=K,\qquad \hat s=\hat\rho C_v. """
[docs] @classmethod def doc_scalar_quantities(cls): r"""**The following scalars are tracked during simulation:** - Kinetic energy: ``en_U`` - Thermodynamic energy: ``en_thermo`` - Total energy: ``en_tot``"""
[docs] @classmethod def doc_discretization(cls): """Time integration is performed by the following propagators (in sequence): 1. :class:`~struphy.propagators.variational_density_evolve.VariationalDensityEvolve` 2. :class:`~struphy.propagators.variational_momentum_advection.VariationalMomentumAdvection` 3. :class:`~struphy.propagators.variational_entropy_evolve.VariationalEntropyEvolve` """ doc = rf"""**1. VariationalDensityEvolve:** {VariationalDensityEvolve.__doc__} **2. VariationalMomentumAdvection:** {VariationalMomentumAdvection.__doc__} **3. VariationalEntropyEvolve:** {VariationalEntropyEvolve.__doc__} """ return doc
[docs] @classmethod def doc_long_description(cls): r"""VariationalCompressibleFluid is the entropy-based compressible fluid model in the variational family. It is the natural non-magnetic counterpart to the full variational MHD models."""
[docs] @classmethod def doc_examples(cls): r"""Create and initialize a variational compressible-fluid model: .. code-block:: python from struphy.models import VariationalCompressibleFluid model = VariationalCompressibleFluid() model.fluid.density model.fluid.velocity model.fluid.entropy """
[docs] @classmethod def doc_use_cases(cls): r"""This model is appropriate for: - compressible fluid benchmarks with entropy transport - testing the variational fluid propagator stack - non-magnetic hydrodynamics with conservative thermodynamics"""
[docs] @classmethod def doc_cannot_be_used_for(cls): r"""This model is not suitable for: - magnetic-field evolution or MHD coupling - pressureless or barotropic-only reductions - kinetic or particle-based transport physics"""