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Commit f32fd3df authored by Matthieu Schaller's avatar Matthieu Schaller
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General speed-up improvements to the GIZMO interaction functions.

parent b87add90
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src/const.h
View file @ f32fd3df
......@@ -68,7 +68,9 @@
#define GIZMO_UNPHYSICAL_RESCUE
/* Show a warning message if an unphysical value was reset (only works if
GIZMO_UNPHYSICAL_RESCUE is also selected). */
#ifdef SWIFT_DEBUG_CHECKS
#define GIZMO_UNPHYSICAL_WARNING
#endif
/* Parameters that control how GIZMO handles pathological particle
configurations. */
......
src/hydro/Gizmo/hydro_gradients.h
View file @ f32fd3df
......@@ -93,17 +93,16 @@ __attribute__((always_inline)) INLINE static void hydro_gradients_finalize(
*/
__attribute__((always_inline)) INLINE static void hydro_gradients_predict(
struct part* restrict pi, struct part* restrict pj, float hi, float hj,
const float* dx, float r, float* xij_i, float* Wi, float* Wj) {
const float* dx, float r, const float* xij_i, float* Wi, float* Wj) {
float dWi[5], dWj[5];
float xij_j[3];
/* perform gradient reconstruction in space and time */
/* Compute interface position (relative to pj, since we don't need the actual
* position) eqn. (8) */
const float xfac = hj / (hi + hj);
for (int k = 0; k < 3; k++) xij_j[k] = xfac * dx[k];
const float xij_j[3] = {xfac * dx[0], xfac * dx[1], xfac * dx[2]};
float dWi[5];
dWi[0] = pi->primitives.gradients.rho[0] * xij_i[0] +
pi->primitives.gradients.rho[1] * xij_i[1] +
pi->primitives.gradients.rho[2] * xij_i[2];
......@@ -120,6 +119,7 @@ __attribute__((always_inline)) INLINE static void hydro_gradients_predict(
pi->primitives.gradients.P[1] * xij_i[1] +
pi->primitives.gradients.P[2] * xij_i[2];
float dWj[5];
dWj[0] = pj->primitives.gradients.rho[0] * xij_j[0] +
pj->primitives.gradients.rho[1] * xij_j[1] +
pj->primitives.gradients.rho[2] * xij_j[2];
......
src/hydro/Gizmo/hydro_iact.h
View file @ f32fd3df
......@@ -51,15 +51,14 @@ __attribute__((always_inline)) INLINE static void runner_iact_density(
float r2, const float *dx, float hi, float hj, struct part *restrict pi,
struct part *restrict pj, float a, float H) {
float r = sqrtf(r2);
float xi, xj;
float h_inv;
float wi, wj, wi_dx, wj_dx;
int k, l;
/* Get r and h inverse. */
const float r = sqrtf(r2);
/* Compute density of pi. */
h_inv = 1.f / hi;
xi = r * h_inv;
const float hi_inv = 1.f / hi;
const float xi = r * hi_inv;
kernel_deval(xi, &wi, &wi_dx);
pi->density.wcount += wi;
......@@ -67,16 +66,17 @@ __attribute__((always_inline)) INLINE static void runner_iact_density(
/* these are eqns. (1) and (2) in the summary */
pi->geometry.volume += wi;
for (k = 0; k < 3; k++)
for (l = 0; l < 3; l++) pi->geometry.matrix_E[k][l] += dx[k] * dx[l] * wi;
for (int k = 0; k < 3; k++)
for (int l = 0; l < 3; l++)
pi->geometry.matrix_E[k][l] += dx[k] * dx[l] * wi;
pi->geometry.centroid[0] -= dx[0] * wi;
pi->geometry.centroid[1] -= dx[1] * wi;
pi->geometry.centroid[2] -= dx[2] * wi;
/* Compute density of pj. */
h_inv = 1.f / hj;
xj = r * h_inv;
const float hj_inv = 1.f / hj;
const float xj = r * hj_inv;
kernel_deval(xj, &wj, &wj_dx);
pj->density.wcount += wj;
......@@ -84,8 +84,9 @@ __attribute__((always_inline)) INLINE static void runner_iact_density(
/* these are eqns. (1) and (2) in the summary */
pj->geometry.volume += wj;
for (k = 0; k < 3; k++)
for (l = 0; l < 3; l++) pj->geometry.matrix_E[k][l] += dx[k] * dx[l] * wj;
for (int k = 0; k < 3; k++)
for (int l = 0; l < 3; l++)
pj->geometry.matrix_E[k][l] += dx[k] * dx[l] * wj;
pj->geometry.centroid[0] += dx[0] * wj;
pj->geometry.centroid[1] += dx[1] * wj;
......@@ -117,17 +118,13 @@ __attribute__((always_inline)) INLINE static void runner_iact_nonsym_density(
float r2, const float *dx, float hi, float hj, struct part *restrict pi,
const struct part *restrict pj, float a, float H) {
float r;
float xi;
float h_inv;
float wi, wi_dx;
int k, l;
/* Get r and r inverse. */
r = sqrtf(r2);
/* Get r and h inverse. */
const float r = sqrtf(r2);
h_inv = 1.f / hi;
xi = r * h_inv;
const float hi_inv = 1.f / hi;
const float xi = r * hi_inv;
kernel_deval(xi, &wi, &wi_dx);
pi->density.wcount += wi;
......@@ -135,8 +132,9 @@ __attribute__((always_inline)) INLINE static void runner_iact_nonsym_density(
/* these are eqns. (1) and (2) in the summary */
pi->geometry.volume += wi;
for (k = 0; k < 3; k++)
for (l = 0; l < 3; l++) pi->geometry.matrix_E[k][l] += dx[k] * dx[l] * wi;
for (int k = 0; k < 3; k++)
for (int l = 0; l < 3; l++)
pi->geometry.matrix_E[k][l] += dx[k] * dx[l] * wi;
pi->geometry.centroid[0] -= dx[0] * wi;
pi->geometry.centroid[1] -= dx[1] * wi;
......@@ -222,34 +220,24 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
float r2, const float *dx, float hi, float hj, struct part *restrict pi,
struct part *restrict pj, int mode, float a, float H) {
float r = sqrtf(r2);
float xi, xj;
float hi_inv, hi_inv_dim;
float hj_inv, hj_inv_dim;
float wi, wj, wi_dx, wj_dx;
int k, l;
float A[3];
float Anorm;
float Bi[3][3];
float Bj[3][3];
float Vi, Vj;
float xij_i[3], xfac, xijdotdx;
float vmax, dvdotdx;
float vi[3], vj[3], vij[3];
float Wi[5], Wj[5];
float n_unit[3];
const float r_inv = 1.f / sqrtf(r2);
const float r = r2 * r_inv;
/* Initialize local variables */
for (k = 0; k < 3; k++) {
for (l = 0; l < 3; l++) {
float Bi[3][3];
float Bj[3][3];
float vi[3], vj[3];
for (int k = 0; k < 3; k++) {
for (int l = 0; l < 3; l++) {
Bi[k][l] = pi->geometry.matrix_E[k][l];
Bj[k][l] = pj->geometry.matrix_E[k][l];
}
vi[k] = pi->v[k]; /* particle velocities */
vj[k] = pj->v[k];
}
Vi = pi->geometry.volume;
Vj = pj->geometry.volume;
const float Vi = pi->geometry.volume;
const float Vj = pj->geometry.volume;
float Wi[5], Wj[5];
Wi[0] = pi->primitives.rho;
Wi[1] = pi->primitives.v[0];
Wi[2] = pi->primitives.v[1];
......@@ -262,56 +250,63 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
Wj[4] = pj->primitives.P;
/* calculate the maximal signal velocity */
float vmax;
if (Wi[0] > 0.0f && Wj[0] > 0.0f) {
vmax =
sqrtf(hydro_gamma * Wi[4] / Wi[0]) + sqrtf(hydro_gamma * Wj[4] / Wj[0]);
} else {
const float ci = gas_soundspeed_from_pressure(Wi[0], Wi[4]);
const float cj = gas_soundspeed_from_pressure(Wj[0], Wj[4]);
vmax = ci + cj;
} else
vmax = 0.0f;
}
dvdotdx = (Wi[1] - Wj[1]) * dx[0] + (Wi[2] - Wj[2]) * dx[1] +
(Wi[3] - Wj[3]) * dx[2];
dvdotdx = min(dvdotdx, (vi[0] - vj[0]) * dx[0] + (vi[1] - vj[1]) * dx[1] +
(vi[2] - vj[2]) * dx[2]);
if (dvdotdx < 0.) {
/* the magical factor 3 also appears in Gadget2 */
vmax -= 3.f * dvdotdx / r;
}
float dvdr = (pi->v[0] - pj->v[0]) * dx[0] + (pi->v[1] - pj->v[1]) * dx[1] +
(pi->v[2] - pj->v[2]) * dx[2];
/* Velocity on the axis linking the particles */
float dvdotdx = (Wi[1] - Wj[1]) * dx[0] + (Wi[2] - Wj[2]) * dx[1] +
(Wi[3] - Wj[3]) * dx[2];
dvdotdx = min(dvdotdx, dvdr);
/* We only care about this velocity for particles moving towards each others
*/
dvdotdx = min(dvdotdx, 0.f);
/* Get the signal velocity */
/* the magical factor 3 also appears in Gadget2 */
vmax -= 3.f * dvdotdx * r_inv;
/* Store the signal velocity */
pi->timestepvars.vmax = max(pi->timestepvars.vmax, vmax);
if (mode == 1) {
pj->timestepvars.vmax = max(pj->timestepvars.vmax, vmax);
}
if (mode == 1) pj->timestepvars.vmax = max(pj->timestepvars.vmax, vmax);
/* Compute kernel of pi. */
hi_inv = 1.f / hi;
hi_inv_dim = pow_dimension(hi_inv);
xi = r * hi_inv;
float wi, wi_dx;
const float hi_inv = 1.f / hi;
const float hi_inv_dim = pow_dimension(hi_inv);
const float xi = r * hi_inv;
kernel_deval(xi, &wi, &wi_dx);
/* Compute kernel of pj. */
hj_inv = 1.f / hj;
hj_inv_dim = pow_dimension(hj_inv);
xj = r * hj_inv;
float wj, wj_dx;
const float hj_inv = 1.f / hj;
const float hj_inv_dim = pow_dimension(hj_inv);
const float xj = r * hj_inv;
kernel_deval(xj, &wj, &wj_dx);
/* Compute h_dt. We are going to use an SPH-like estimate of div_v for that */
float dvdr = (pi->v[0] - pj->v[0]) * dx[0] + (pi->v[1] - pj->v[1]) * dx[1] +
(pi->v[2] - pj->v[2]) * dx[2];
float ri = 1.0f / r;
float hidp1 = pow_dimension_plus_one(hi_inv);
float hjdp1 = pow_dimension_plus_one(hj_inv);
float wi_dr = hidp1 * wi_dx;
float wj_dr = hjdp1 * wj_dx;
dvdr *= ri;
if (pj->primitives.rho > 0.) {
const float hidp1 = pow_dimension_plus_one(hi_inv);
const float hjdp1 = pow_dimension_plus_one(hj_inv);
const float wi_dr = hidp1 * wi_dx;
const float wj_dr = hjdp1 * wj_dx;
dvdr *= r_inv;
if (pj->primitives.rho > 0.)
pi->force.h_dt -= pj->conserved.mass * dvdr / pj->primitives.rho * wi_dr;
}
if (mode == 1 && pi->primitives.rho > 0.) {
if (mode == 1 && pi->primitives.rho > 0.)
pj->force.h_dt -= pi->conserved.mass * dvdr / pi->primitives.rho * wj_dr;
}
/* Compute area */
/* Compute (square of) area */
/* eqn. (7) */
Anorm = 0.0f;
float Anorm2 = 0.0f;
float A[3];
if (pi->density.wcorr > const_gizmo_min_wcorr &&
pj->density.wcorr > const_gizmo_min_wcorr) {
/* in principle, we use Vi and Vj as weights for the left and right
......@@ -327,30 +322,31 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
Xj = Xi;
}
#endif
for (k = 0; k < 3; k++) {
for (int k = 0; k < 3; k++) {
/* we add a minus sign since dx is pi->x - pj->x */
A[k] = -Xi * (Bi[k][0] * dx[0] + Bi[k][1] * dx[1] + Bi[k][2] * dx[2]) *
wi * hi_inv_dim -
Xj * (Bj[k][0] * dx[0] + Bj[k][1] * dx[1] + Bj[k][2] * dx[2]) *
wj * hj_inv_dim;
Anorm += A[k] * A[k];
Anorm2 += A[k] * A[k];
}
} else {
/* ill condition gradient matrix: revert to SPH face area */
Anorm = -(hidp1 * Vi * Vi * wi_dx + hjdp1 * Vj * Vj * wj_dx) * ri;
const float Anorm =
-(hidp1 * Vi * Vi * wi_dx + hjdp1 * Vj * Vj * wj_dx) * r_inv;
A[0] = -Anorm * dx[0];
A[1] = -Anorm * dx[1];
A[2] = -Anorm * dx[2];
Anorm *= Anorm * r2;
Anorm2 = Anorm * Anorm * r2;
}
if (Anorm == 0.f) {
/* if the interface has no area, nothing happens and we return */
/* continuing results in dividing by zero and NaN's... */
return;
}
/* if the interface has no area, nothing happens and we return */
/* continuing results in dividing by zero and NaN's... */
if (Anorm2 == 0.f) return;
Anorm = sqrtf(Anorm);
/* Compute the area */
const float Anorm_inv = 1. / sqrtf(Anorm2);
const float Anorm = Anorm2 * Anorm_inv;
#ifdef SWIFT_DEBUG_CHECKS
/* For stability reasons, we do require A and dx to have opposite
......@@ -358,29 +354,32 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
always points from particle i to particle j, as it would in a real
moving-mesh code). If not, our scheme is no longer upwind and hence can
become unstable. */
float dA_dot_dx = A[0] * dx[0] + A[1] * dx[1] + A[2] * dx[2];
const float dA_dot_dx = A[0] * dx[0] + A[1] * dx[1] + A[2] * dx[2];
/* In GIZMO, Phil Hopkins reverts to an SPH integration scheme if this
happens. We curently just ignore this case and display a message. */
const float rdim = pow_dimension(r);
if (dA_dot_dx > 1.e-6 * rdim) {
if (dA_dot_dx > 1.e-6f * rdim) {
message("Ill conditioned gradient matrix (%g %g %g %g %g)!", dA_dot_dx,
Anorm, Vi, Vj, r);
}
#endif
/* compute the normal vector of the interface */
for (k = 0; k < 3; k++) n_unit[k] = A[k] / Anorm;
const float n_unit[3] = {A[0] * Anorm_inv, A[1] * Anorm_inv,
A[2] * Anorm_inv};
/* Compute interface position (relative to pi, since we don't need the actual
* position) */
/* eqn. (8) */
xfac = hi / (hi + hj);
for (k = 0; k < 3; k++) xij_i[k] = -xfac * dx[k];
* position) eqn. (8) */
const float xfac = -hi / (hi + hj);
const float xij_i[3] = {xfac * dx[0], xfac * dx[1], xfac * dx[2]};
/* Compute interface velocity */
/* eqn. (9) */
xijdotdx = xij_i[0] * dx[0] + xij_i[1] * dx[1] + xij_i[2] * dx[2];
for (k = 0; k < 3; k++) vij[k] = vi[k] + (vi[k] - vj[k]) * xijdotdx / r2;
float xijdotdx = xij_i[0] * dx[0] + xij_i[1] * dx[1] + xij_i[2] * dx[2];
xijdotdx *= r_inv * r_inv;
const float vij[3] = {vi[0] + (vi[0] - vj[0]) * xijdotdx,
vi[1] + (vi[1] - vj[1]) * xijdotdx,
vi[2] + (vi[2] - vj[2]) * xijdotdx};
/* complete calculation of position of interface */
/* NOTE: dx is not necessarily just pi->x - pj->x but can also contain
......@@ -388,8 +387,7 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
we have to use xij w.r.t. the actual particle.
=> we need a separate xij for pi and pj... */
/* tldr: we do not need the code below, but we do need the same code as above
but then
with i and j swapped */
but then with i and j swapped */
// for ( k = 0 ; k < 3 ; k++ )
// xij[k] += pi->x[k];
......@@ -418,10 +416,10 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
totflux[4] *= Anorm;
/* Store mass flux */
float mflux = totflux[0];
pi->gravity.mflux[0] += mflux * dx[0];
pi->gravity.mflux[1] += mflux * dx[1];
pi->gravity.mflux[2] += mflux * dx[2];
const float mflux_i = totflux[0];
pi->gravity.mflux[0] += mflux_i * dx[0];
pi->gravity.mflux[1] += mflux_i * dx[1];
pi->gravity.mflux[2] += mflux_i * dx[2];
/* Update conserved variables */
/* eqn. (16) */
......@@ -432,13 +430,13 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
pi->conserved.flux.energy -= totflux[4];
#ifndef GIZMO_TOTAL_ENERGY
float ekin = 0.5f * (pi->primitives.v[0] * pi->primitives.v[0] +
pi->primitives.v[1] * pi->primitives.v[1] +
pi->primitives.v[2] * pi->primitives.v[2]);
const float ekin_i = 0.5f * (pi->primitives.v[0] * pi->primitives.v[0] +
pi->primitives.v[1] * pi->primitives.v[1] +
pi->primitives.v[2] * pi->primitives.v[2]);
pi->conserved.flux.energy += totflux[1] * pi->primitives.v[0];
pi->conserved.flux.energy += totflux[2] * pi->primitives.v[1];
pi->conserved.flux.energy += totflux[3] * pi->primitives.v[2];
pi->conserved.flux.energy -= totflux[0] * ekin;
pi->conserved.flux.energy -= totflux[0] * ekin_i;
#endif
/* Note that this used to be much more complicated in early implementations of
......@@ -448,10 +446,10 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
* for the flux over the entire time step. */
if (mode == 1) {
/* Store mass flux */
mflux = totflux[0];
pj->gravity.mflux[0] -= mflux * dx[0];
pj->gravity.mflux[1] -= mflux * dx[1];
pj->gravity.mflux[2] -= mflux * dx[2];
const float mflux_j = totflux[0];
pj->gravity.mflux[0] -= mflux_j * dx[0];
pj->gravity.mflux[1] -= mflux_j * dx[1];
pj->gravity.mflux[2] -= mflux_j * dx[2];
pj->conserved.flux.mass += totflux[0];
pj->conserved.flux.momentum[0] += totflux[1];
......@@ -460,13 +458,13 @@ __attribute__((always_inline)) INLINE static void runner_iact_fluxes_common(
pj->conserved.flux.energy += totflux[4];
#ifndef GIZMO_TOTAL_ENERGY
ekin = 0.5f * (pj->primitives.v[0] * pj->primitives.v[0] +
pj->primitives.v[1] * pj->primitives.v[1] +
pj->primitives.v[2] * pj->primitives.v[2]);
const float ekin_j = 0.5f * (pj->primitives.v[0] * pj->primitives.v[0] +
pj->primitives.v[1] * pj->primitives.v[1] +
pj->primitives.v[2] * pj->primitives.v[2]);
pj->conserved.flux.energy -= totflux[1] * pj->primitives.v[0];
pj->conserved.flux.energy -= totflux[2] * pj->primitives.v[1];
pj->conserved.flux.energy -= totflux[3] * pj->primitives.v[2];
pj->conserved.flux.energy += totflux[0] * ekin;
pj->conserved.flux.energy += totflux[0] * ekin_j;
#endif
}
}
......
src/hydro/Gizmo/hydro_slope_limiters_face.h
View file @ f32fd3df
......@@ -88,7 +88,7 @@ hydro_slope_limit_face_quantity(float phi_i, float phi_j, float phi_mid0,
* @param r Distance between particle i and particle j.
*/
__attribute__((always_inline)) INLINE static void hydro_slope_limit_face(
float *Wi, float *Wj, float *dWi, float *dWj, float *xij_i, float *xij_j,
float *Wi, float *Wj, float *dWi, float *dWj, const float *xij_i, const float *xij_j,
float r) {
const float xij_i_norm =
......
src/riemann/riemann_exact.h
View file @ f32fd3df
......@@ -47,14 +47,14 @@
* @param W The left or right state vector
* @param a The left or right sound speed
*/
__attribute__((always_inline)) INLINE static float riemann_fb(float p, float* W,
__attribute__((always_inline)) INLINE static float riemann_fb(float p,
const float* W,
float a) {
float fval = 0.;
float A, B;
float fval;
if (p > W[4]) {
A = hydro_two_over_gamma_plus_one / W[0];
B = hydro_gamma_minus_one_over_gamma_plus_one * W[4];
const float A = hydro_two_over_gamma_plus_one / W[0];
const float B = hydro_gamma_minus_one_over_gamma_plus_one * W[4];
fval = (p - W[4]) * sqrtf(A / (p + B));
} else {
fval = hydro_two_over_gamma_minus_one * a *
......@@ -75,7 +75,8 @@ __attribute__((always_inline)) INLINE static float riemann_fb(float p, float* W,
* @param aR The right sound speed
*/
__attribute__((always_inline)) INLINE static float riemann_f(
float p, float* WL, float* WR, float vL, float vR, float aL, float aR) {
float p, const float* WL, const float* WR, float vL, float vR, float aL,
float aR) {
return riemann_fb(p, WL, aL) + riemann_fb(p, WR, aR) + (vR - vL);
}
......@@ -87,15 +88,13 @@ __attribute__((always_inline)) INLINE static float riemann_f(
* @param W The left or right state vector
* @param a The left or right sound speed
*/
__attribute__((always_inline)) INLINE static float riemann_fprimeb(float p,
float* W,
float a) {
__attribute__((always_inline)) INLINE static float riemann_fprimeb(
float p, const float* W, float a) {
float fval = 0.;
float A, B;
float fval;
if (p > W[4]) {
A = hydro_two_over_gamma_plus_one / W[0];
B = hydro_gamma_minus_one_over_gamma_plus_one * W[4];
const float A = hydro_two_over_gamma_plus_one / W[0];
const float B = hydro_gamma_minus_one_over_gamma_plus_one * W[4];
fval = (1.0f - 0.5f * (p - W[4]) / (B + p)) * sqrtf(A / (p + B));
} else {
fval = 1.0f / W[0] / a * pow_minus_gamma_plus_one_over_two_gamma(p / W[4]);
......@@ -113,7 +112,7 @@ __attribute__((always_inline)) INLINE static float riemann_fprimeb(float p,
* @param aR The right sound speed
*/
__attribute__((always_inline)) INLINE static float riemann_fprime(
float p, float* WL, float* WR, float aL, float aR) {
float p, const float* WL, const float* WR, float aL, float aR) {
return riemann_fprimeb(p, WL, aL) + riemann_fprimeb(p, WR, aR);
}
......@@ -125,11 +124,10 @@ __attribute__((always_inline)) INLINE static float riemann_fprime(
* @param W The left or right state vector
*/
__attribute__((always_inline)) INLINE static float riemann_gb(float p,
float* W) {
const float* W) {
float A, B;
A = hydro_two_over_gamma_plus_one / W[0];
B = hydro_gamma_minus_one_over_gamma_plus_one * W[4];
const float A = hydro_two_over_gamma_plus_one / W[0];
const float B = hydro_gamma_minus_one_over_gamma_plus_one * W[4];
return sqrtf(A / (p + B));
}
......@@ -147,7 +145,7 @@ __attribute__((always_inline)) INLINE static float riemann_gb(float p,
* @param aR The right sound speed
*/
__attribute__((always_inline)) INLINE static float riemann_guess_p(
float* WL, float* WR, float vL, float vR, float aL, float aR) {
const float* WL, const float* WR, float vL, float vR, float aL, float aR) {
float pguess, pmin, pmax, qmax;
float ppv;
......@@ -199,8 +197,8 @@ __attribute__((always_inline)) INLINE static float riemann_guess_p(
*/
__attribute__((always_inline)) INLINE static float riemann_solve_brent(
float lower_limit, float upper_limit, float lowf, float upf,
float error_tol, float* WL, float* WR, float vL, float vR, float aL,
float aR) {
float error_tol, const float* WL, const float* WR, float vL, float vR,
float aL, float aR) {
float a, b, c, d, s;
float fa, fb, fc, fs;
......@@ -306,7 +304,7 @@ __attribute__((always_inline)) INLINE static float riemann_solve_brent(
* @param n_unit Normal vector of the interface
*/
__attribute__((always_inline)) INLINE static void riemann_solver_solve(
float* WL, float* WR, float* Whalf, float* n_unit) {
const float* WL, const float* WR, float* Whalf, const float* n_unit) {
/* velocity of the left and right state in a frame aligned with n_unit */
float vL, vR, vhalf;
......@@ -510,7 +508,8 @@ __attribute__((always_inline)) INLINE static void riemann_solver_solve(
}
__attribute__((always_inline)) INLINE static void riemann_solve_for_flux(
float* Wi, float* Wj, float* n_unit, float* vij, float* totflux) {
const float* Wi, const float* Wj, const float* n_unit, const float* vij,
float* totflux) {
float Whalf[5];
float flux[5][3];
......
src/riemann/riemann_hllc.h
View file @ f32fd3df
......@@ -38,7 +38,8 @@
#endif
__attribute__((always_inline)) INLINE static void riemann_solve_for_flux(
float *WL, float *WR, float *n, float *vij, float *totflux) {
const float *WL, const float *WR, const float *n, const float *vij,
float *totflux) {
/* Handle pure vacuum */
if (!WL[0] && !WR[0]) {
......
src/riemann/riemann_trrs.h
View file @ f32fd3df
......@@ -52,7 +52,7 @@
* @param n_unit Normal vector of the interface
*/
__attribute__((always_inline)) INLINE static void riemann_solver_solve(
float* WL, float* WR, float* Whalf, float* n_unit) {
const float* WL, const float* WR, float* Whalf, const float* n_unit) {
float aL, aR;
float PLR;
float vL, vR;
......@@ -160,7 +160,8 @@ __attribute__((always_inline)) INLINE static void riemann_solver_solve(
}
__attribute__((always_inline)) INLINE static void riemann_solve_for_flux(
float* Wi, float* Wj, float* n_unit, float* vij, float* totflux) {
const float* Wi, const float* Wj, const float* n_unit, const float* vij,
float* totflux) {
float Whalf[5];
float flux[5][3];
......
src/riemann/riemann_vacuum.h
View file @ f32fd3df
......@@ -24,7 +24,7 @@
* @brief Check if the given input states are vacuum or will generate vacuum
*/
__attribute__((always_inline)) INLINE static int riemann_is_vacuum(
float* WL, float* WR, float vL, float vR, float aL, float aR) {