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Merge pull request #5882 from isaaclegred/FixEquilibriumEoS
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Fix a bug in Equilibrium3D EoS
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nilsdeppe authored Apr 1, 2024
2 parents aead616 + f0e6981 commit eabf7be
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39 changes: 37 additions & 2 deletions src/PointwiseFunctions/Hydro/EquationsOfState/EquationOfState.hpp
Original file line number Diff line number Diff line change
Expand Up @@ -641,12 +641,47 @@ class EquationOfState<IsRelativistic, 3> : public PUP::able {
* Computes adiabatic sound speed squared
* \f[
* c_s^2 \equiv \frac{\partial p}{\partial e} |_{s, Y_e} =
* \frac{\rho}{h}\frac{\partial p}{\rho} |_{e, Y_e} +
* \frac{\rho}{h}\frac{\partial p}{\partial \rho} |_{e, Y_e} +
* \frac{\partial p}{\partial e}|_{\rho, Y_e}
* \f].
* With \f$p, e\f$ the pressure and energy density respectively,
* \f$s\f$ the entropy density, \f$Y_e\f$ the electron fraction
* and \f$\rho\f$ the rest-mass density.
* \f$\rho\f$ the rest-mass density, and \f$h\f$ the enthalpy density.
* Note that \f$e\f$ is the total energy density and not the internal energy,
* therefore
* \f[
* \frac{\partial p}{\partial \rho} |_{e, Y_e} \neq \chi \equiv \frac{\partial
* p}{\partial \rho} |_{\epsilon, Y_e}
* \f]
* as defined in the 2-d EoS above. By definition
* \f$ e = (1+\epsilon) \rho \f$ so holding \f$e\f$ constant
* \f[
* 0 = \frac{d e}{d \rho} = \frac{\partial e}{\partial \rho} +
* \frac{\partial e}{\partial \epsilon} \frac{\partial \epsilon}{\rho}.
* \f]
* (where we have suppressed \f$ Y_e\f$ dependence)
* So \f$ \partial \epsilon / \partial \rho |_{e} = (1 + \epsilon)/\rho \f$
* and we can expand
* \f[
* \frac{\partial p}{\partial \rho} |_{e, Y_e} = \frac{\partial e}{\partial
* \rho}_{\epsilon, Y_e} + \frac{(1 + \epsilon)}{\rho} \frac{\partial
* e}{\partial \epsilon}|_{\rho, Y_e}
* \f]
* Finally, we can rewrite the entire sound speed using only the rest-mass
* density, specific internal energy, and electron fraction as variables,
* by using \f$ \frac{\partial e}{\partial \epsilon}|_{\rho, Y_e} = 1 \f$
* \f[
* c_s^2 =
* \frac{\rho}{h}\frac{\partial p}{\partial \rho} |_{\epsilon, Y_e} +
* \frac{1}{\rho} \frac{\partial p}{\partial \epsilon}|_{\rho, Y_e} \left(
* 1 - \frac{(1 + \epsilon)\rho}{h}\right)
* \f]
* Which reduces to our preferred form
* \f[
* c_s^2 =
* \frac{\rho}{h}(\chi + \kappa)
* \f]
*
* Computed as a function of temperature, rest-mass density and electron
* fraction. Note that this will break thermodynamic consistency if the
* pressure and internal energy interpolated separately. The precise impact of
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14 changes: 6 additions & 8 deletions src/PointwiseFunctions/Hydro/EquationsOfState/Equilibrium3D.cpp
Original file line number Diff line number Diff line change
Expand Up @@ -119,14 +119,12 @@ Equilibrium3D<EquilEos>::sound_speed_squared_from_density_and_temperature_impl(
// Cold part plus temperature dependent part, see the 3D EoS documentation for
// expression.
return Scalar<DataType>{
get(rest_mass_density) *
get(underlying_eos_.chi_from_density_and_energy(
rest_mass_density, specific_internal_energy)) /
enthalpy_density +
get(rest_mass_density) / pressure *
get(underlying_eos_
.kappa_times_p_over_rho_squared_from_density_and_energy(
rest_mass_density, specific_internal_energy))};
get(rest_mass_density) / enthalpy_density *
(get(underlying_eos_.chi_from_density_and_energy(
rest_mass_density, specific_internal_energy)) +
get(underlying_eos_
.kappa_times_p_over_rho_squared_from_density_and_energy(
rest_mass_density, specific_internal_energy)))};
}

template class Equilibrium3D<HybridEos<PolytropicFluid<true>>>;
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Original file line number Diff line number Diff line change
Expand Up @@ -16,15 +16,22 @@
#include "PointwiseFunctions/Hydro/EquationsOfState/EquationOfState.hpp"
#include "PointwiseFunctions/Hydro/EquationsOfState/Equilibrium3D.hpp"
#include "PointwiseFunctions/Hydro/EquationsOfState/Factory.hpp"
#include "PointwiseFunctions/Hydro/EquationsOfState/IdealFluid.hpp"
#include "Utilities/Serialization/RegisterDerivedClassesWithCharm.hpp"


SPECTRE_TEST_CASE("Unit.PointwiseFunctions.EquationsOfState.Equilibrium3D",
"[Unit][EquationsOfState]") {
namespace EoS = EquationsOfState;
const EoS::PolytropicFluid<true> cold_eos{100.0, 2.0};
const EoS::HybridEos<EoS::PolytropicFluid<true>> underlying_eos{cold_eos,
2.0};

const double ideal_adiabatic_index = 2.0;
const double cold_polytropic_index = 2.0;
const EoS::PolytropicFluid<true> cold_eos{100.0, cold_polytropic_index};
const EoS::IdealFluid<true> eos_ideal_fluid{ideal_adiabatic_index};

EoS::Equilibrium3D<EoS::IdealFluid<true>> eos_ideal_fluid_3d{eos_ideal_fluid};
const EoS::HybridEos<EoS::PolytropicFluid<true>> underlying_eos{
cold_eos, ideal_adiabatic_index};
EoS::Equilibrium3D<EoS::HybridEos<EoS::PolytropicFluid<true>>> eos{
underlying_eos};
CHECK(eos.rest_mass_density_lower_bound() ==
Expand Down Expand Up @@ -83,22 +90,32 @@ SPECTRE_TEST_CASE("Unit.PointwiseFunctions.EquationsOfState.Equilibrium3D",
eos.temperature_from_density_and_energy(
rest_mass_density, specific_internal_energy, electron_fraction),
temperature);
}
{
const Scalar<DataVector> rest_mass_density{
DataVector{1e-10, 1e-6, 1e-4, 1e-3, 1e-2, 1.0}};
// electron fraction should be irrelevant
const Scalar<DataVector> electron_fraction{
DataVector{1e-10, 1e-6, 1e-4, 1e-3, 1e-2, 1.0}};
const Scalar<DataVector> temperature{
DataVector{1e-10, 1e-6, 1e-4, 1e-3, 1e-2, 1.0}};
// For the ideal fluid the sound speed can be computed analytically
const Scalar<DataVector> pressure =
eos_ideal_fluid_3d.pressure_from_density_and_temperature(
rest_mass_density, temperature, electron_fraction);
const Scalar<DataVector> specific_internal_energy =
eos_ideal_fluid_3d
.specific_internal_energy_from_density_and_temperature(
rest_mass_density, temperature, electron_fraction);
const DataVector enthalpy_density =
get(rest_mass_density) * (1.0 + get(specific_internal_energy)) +
get(pressure);

CHECK_ITERABLE_APPROX(
get(eos.sound_speed_squared_from_density_and_temperature(
get(eos_ideal_fluid_3d.sound_speed_squared_from_density_and_temperature(
rest_mass_density, temperature, electron_fraction)),
get(rest_mass_density) *
get(underlying_eos.chi_from_density_and_energy(
rest_mass_density, specific_internal_energy)) /
enthalpy_density +
get(rest_mass_density) / get(pressure) *
get(underlying_eos
.kappa_times_p_over_rho_squared_from_density_and_energy(
rest_mass_density, specific_internal_energy)));
(ideal_adiabatic_index)*get(pressure) / enthalpy_density);
}

{
// double functions
const Scalar<double> rest_mass_density{{1e-3}};
Expand All @@ -121,42 +138,39 @@ SPECTRE_TEST_CASE("Unit.PointwiseFunctions.EquationsOfState.Equilibrium3D",
rest_mass_density, specific_internal_energy, electron_fraction) ==
underlying_eos.temperature_from_density_and_energy(
rest_mass_density, specific_internal_energy));
}
{
// Using the ideal fluid for sound speed computations
const Scalar<double> rest_mass_density{{1e-3}};
// temperature and electron fraction should be irrelevant
const Scalar<double> electron_fraction{{1e-1}};
const Scalar<double> temperature{{1e-1}};
const Scalar<double> pressure =
eos_ideal_fluid_3d.pressure_from_density_and_temperature(
rest_mass_density, temperature, electron_fraction);
const Scalar<double> specific_internal_energy =
eos_ideal_fluid_3d
.specific_internal_energy_from_density_and_temperature(
rest_mass_density, temperature, electron_fraction);

const double enthalpy_density =
get(rest_mass_density) * (1.0 + get(specific_internal_energy)) +
get(pressure);
CHECK(
get(eos.sound_speed_squared_from_density_and_temperature(
rest_mass_density, temperature, electron_fraction)) ==
approx(
get(rest_mass_density) *
get(underlying_eos.chi_from_density_and_energy(
rest_mass_density, specific_internal_energy)) /
enthalpy_density +
get(rest_mass_density) / get(pressure) *
get(underlying_eos
.kappa_times_p_over_rho_squared_from_density_and_energy(
rest_mass_density, specific_internal_energy))));
// IdealFluid value is known analytically
CHECK_ITERABLE_APPROX(
get(eos_ideal_fluid_3d.sound_speed_squared_from_density_and_temperature(
rest_mass_density, temperature, electron_fraction)),
(ideal_adiabatic_index)*get(pressure) / enthalpy_density);
// Check that the sound speed calculation works at zero temperature
CHECK_ITERABLE_APPROX(
get(eos.sound_speed_squared_from_density_and_temperature(
rest_mass_density, Scalar<double>{0.0}, electron_fraction)) -
get(rest_mass_density) /
get(cold_eos.pressure_from_density(rest_mass_density)) *
get(underlying_eos
.kappa_times_p_over_rho_squared_from_density_and_energy(
rest_mass_density,
cold_eos.specific_internal_energy_from_density(
rest_mass_density))),
get(rest_mass_density) *
get(underlying_eos.chi_from_density_and_energy(
rest_mass_density,
cold_eos.specific_internal_energy_from_density(
rest_mass_density))) /
(get(rest_mass_density) +
get(cold_eos.pressure_from_density(rest_mass_density)) +
get(cold_eos.specific_internal_energy_from_density(
rest_mass_density)) *
get(rest_mass_density)));
rest_mass_density, Scalar<double>{0.0}, electron_fraction)),
get(rest_mass_density) /
(get(cold_eos.pressure_from_density(rest_mass_density)) +
get(rest_mass_density) *
(1.0 + get(cold_eos.specific_internal_energy_from_density(
rest_mass_density)))) *
get(cold_eos.chi_from_density(rest_mass_density)));
}
{
register_derived_classes_with_charm<EoS::EquationOfState<true, 3>>();
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