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Commit e3ae510d authored by Matthieu Schaller's avatar Matthieu Schaller
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Use the equation of state functions in a few more places in the gizmo code to...

Use the equation of state functions in a few more places in the gizmo code to be more robust to changes.
parent 882305fe
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......@@ -24,6 +24,7 @@
#include "approx_math.h"
#include "equation_of_state.h"
#include "hydro_gradients.h"
#include "hydro_properties.h"
#include "hydro_space.h"
#include "hydro_unphysical.h"
#include "hydro_velocities.h"
......@@ -130,8 +131,9 @@ __attribute__((always_inline)) INLINE static void hydro_first_init_part(
/* remember that we store the total thermal energy, not the specific thermal
energy (as in Gadget) */
#if defined(EOS_ISOTHERMAL_GAS)
/* this overwrites the internal energy from the initial condition file */
p->conserved.energy = mass * eos.isothermal_internal_energy;
/* this overwrites the internal energy from the initial condition file
* Note that we call the EoS function just to get the constant u here. */
p->conserved.energy = mass * gas_internal_energy_from_entropy(0.f, 0.f);
#else
p->conserved.energy *= mass;
#endif
......@@ -608,7 +610,9 @@ __attribute__((always_inline)) INLINE static void hydro_kick_extra(
p->conserved.momentum[1] += p->conserved.flux.momentum[1];
p->conserved.momentum[2] += p->conserved.flux.momentum[2];
#if defined(EOS_ISOTHERMAL_GAS)
p->conserved.energy = p->conserved.mass * eos.isothermal_internal_energy;
/* We use the EoS equation in a sneaky way here just to get the constant u */
p->conserved.energy =
p->conserved.mass * gas_internal_energy_from_entropy(0.f, 0.f);
#else
p->conserved.energy += p->conserved.flux.energy;
#endif
......@@ -707,15 +711,11 @@ __attribute__((always_inline)) INLINE static void hydro_kick_extra(
__attribute__((always_inline)) INLINE static float hydro_get_internal_energy(
const struct part* restrict p) {
if (p->primitives.rho > 0.) {
#ifdef EOS_ISOTHERMAL_GAS
return eos.isothermal_internal_energy;
#else
return p->primitives.P / hydro_gamma_minus_one / p->primitives.rho;
#endif
} else {
if (p->primitives.rho > 0.)
return gas_internal_energy_from_pressure(p->primitives.rho,
p->primitives.P);
else
return 0.;
}
}
/**
......@@ -727,7 +727,7 @@ __attribute__((always_inline)) INLINE static float hydro_get_entropy(
const struct part* restrict p) {
if (p->primitives.rho > 0.) {
return p->primitives.P / pow_gamma(p->primitives.rho);
return gas_entropy_from_pressure(p->primitives.rho, p->primitives.P);
} else {
return 0.;
}
......@@ -741,16 +741,10 @@ __attribute__((always_inline)) INLINE static float hydro_get_entropy(
__attribute__((always_inline)) INLINE static float hydro_get_soundspeed(
const struct part* restrict p) {
if (p->primitives.rho > 0.) {
#ifdef EOS_ISOTHERMAL_GAS
return sqrtf(eos.isothermal_internal_energy * hydro_gamma *
hydro_gamma_minus_one);
#else
return sqrtf(hydro_gamma * p->primitives.P / p->primitives.rho);
#endif
} else {
if (p->primitives.rho > 0.)
return gas_soundspeed_from_pressure(p->primitives.rho, p->primitives.P);
else
return 0.;
}
}
/**
......
......@@ -18,7 +18,7 @@
******************************************************************************/
#include "adiabatic_index.h"
#include "equation_of_state.h"
#include "hydro.h"
#include "hydro_flux_limiters.h"
#include "hydro_gradients.h"
#include "hydro_slope_limiters.h"
......@@ -72,15 +72,7 @@ void hydro_read_particles(struct part* parts, struct io_props* list,
* @return Internal energy of the particle
*/
float convert_u(struct engine* e, struct part* p) {
if (p->primitives.rho > 0.) {
#ifdef EOS_ISOTHERMAL_GAS
return eos.isothermal_internal_energy;
#else
return p->primitives.P / hydro_gamma_minus_one / p->primitives.rho;
#endif
} else {
return 0.;
}
return hydro_get_internal_energy(p);
}
/**
......@@ -91,11 +83,7 @@ float convert_u(struct engine* e, struct part* p) {
* @return Entropic function of the particle
*/
float convert_A(struct engine* e, struct part* p) {
if (p->primitives.rho > 0.) {
return p->primitives.P / pow_gamma(p->primitives.rho);
} else {
return 0.;
}
return hydro_get_entropy(p);
}
/**
......
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