Add Minimal Multi-Material hydro scheme (untested WIP)

configure.ac

@@ -779,7 +779,7 @@ fi
 # Hydro scheme.
 AC_ARG_WITH([hydro],
    [AS_HELP_STRING([--with-hydro=<scheme>],
-      [Hydro dynamics to use @<:@gadget2, minimal, hopkins, default, gizmo, shadowfax debug default: gadget2@:>@]
+      [Hydro dynamics to use @<:@gadget2, minimal, hopkins, default, gizmo, shadowfax, minimal-multi-mat debug default: gadget2@:>@]
    )],
    [with_hydro="$withval"],
    [with_hydro="gadget2"]
@@ -803,6 +803,9 @@ case "$with_hydro" in
    shadowfax)
       AC_DEFINE([SHADOWFAX_SPH], [1], [Shadowfax SPH])
    ;;
+   minimal-multi-mat)
+      AC_DEFINE([MINIMAL_MULTI_MAT_SPH], [1], [Minimal Multiple Material SPH])
+   ;;
 
    *)
       AC_MSG_ERROR([Unknown hydrodynamics scheme: $with_hydro])
@@ -890,7 +893,7 @@ esac
 #  Equation of state
 AC_ARG_WITH([equation-of-state],
    [AS_HELP_STRING([--with-equation-of-state=<EoS>],
-      [equation of state @<:@ideal-gas, isothermal-gas, tillotson-iron default: ideal-gas@:>@]
+      [equation of state @<:@ideal-gas, isothermal-gas, tillotson default: ideal-gas@:>@]
    )],
    [with_eos="$withval"],
    [with_eos="ideal-gas"]
@@ -902,8 +905,8 @@ case "$with_eos" in
    isothermal-gas)
       AC_DEFINE([EOS_ISOTHERMAL_GAS], [1], [Isothermal gas equation of state])
    ;;
-   tillotson-iron)
-      AC_DEFINE([EOS_TILLOTSON_IRON], [1], [Tillotson iron equation of state])
+   tillotson)
+      AC_DEFINE([EOS_TILLOTSON], [1], [Tillotson equation of state])
    ;;
    *)
       AC_MSG_ERROR([Unknown equation of state: $with_eos])

src/debug.c

@@ -52,6 +52,8 @@
 #include "./hydro/Gizmo/hydro_debug.h"
 #elif defined(SHADOWFAX_SPH)
 #include "./hydro/Shadowswift/hydro_debug.h"
+#elif defined(MINIMAL_MULTI_MAT_SPH)
+#include "./hydro/MinimalMultiMat/hydro_debug.h"
 #else
 #error "Invalid choice of SPH variant"
 #endif

src/hydro.h

@@ -52,6 +52,10 @@
 #include "./hydro/Shadowswift/hydro_iact.h"
 #define SPH_IMPLEMENTATION \
   "Shadowfax moving mesh (Vandenbroucke and De Rijcke 2016)"
+#elif defined(MINIMAL_MULTI_MAT_SPH)
+#include "./hydro/MinimalMultiMat/hydro.h"
+#include "./hydro/MinimalMultiMat/hydro_iact.h"
+#define SPH_IMPLEMENTATION "Minimal version of SPH with multiple materials"
 #else
 #error "Invalid choice of SPH variant"
 #endif

src/hydro/MinimalMultiMat/hydro_debug.h

+/*******************************************************************************
+ * This file is part of SWIFT.
+ * Coypright (c) 2016 Matthieu Schaller (matthieu.schaller@durham.ac.uk)
+ *
+ * This program is free software: you can redistribute it and/or modify
+ * it under the terms of the GNU Lesser General Public License as published
+ * by the Free Software Foundation, either version 3 of the License, or
+ * (at your option) any later version.
+ *
+ * This program is distributed in the hope that it will be useful,
+ * but WITHOUT ANY WARRANTY; without even the implied warranty of
+ * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
+ * GNU General Public License for more details.
+ *
+ * You should have received a copy of the GNU Lesser General Public License
+ * along with this program.  If not, see <http://www.gnu.org/licenses/>.
+ *
+ ******************************************************************************/
+#ifndef SWIFT_MINIMAL_MULTI_MAT_HYDRO_DEBUG_H
+#define SWIFT_MINIMAL_MULTI_MAT_HYDRO_DEBUG_H
+
+/**
+ * @file MinimalMultiMat/hydro_debug.h
+ * @brief MinimalMultiMat conservative implementation of SPH (Debugging routines)
+ *
+ * The thermal variable is the internal energy (u). Simple constant
+ * viscosity term without switches is implemented. No thermal conduction
+ * term is implemented.
+ *
+ * This corresponds to equations (43), (44), (45), (101), (103)  and (104) with
+ * \f$\beta=3\f$ and \f$\alpha_u=0\f$ of
+ * Price, D., Journal of Computational Physics, 2012, Volume 231, Issue 3,
+ * pp. 759-794.
+ */
+
+__attribute__((always_inline)) INLINE static void hydro_debug_particle(
+    const struct part* p, const struct xpart* xp) {
+  printf(
+      "x=[%.3e,%.3e,%.3e], "
+      "v=[%.3e,%.3e,%.3e],v_full=[%.3e,%.3e,%.3e] \n a=[%.3e,%.3e,%.3e], "
+      "u=%.3e, du/dt=%.3e v_sig=%.3e, P=%.3e\n"
+      "h=%.3e, dh/dt=%.3e wcount=%d, m=%.3e, dh_drho=%.3e, rho=%.3e, "
+      "time_bin=%d, mat_id=%d\n",
+      p->x[0], p->x[1], p->x[2], p->v[0], p->v[1], p->v[2], xp->v_full[0],
+      xp->v_full[1], xp->v_full[2], p->a_hydro[0], p->a_hydro[1], p->a_hydro[2],
+      p->u, p->u_dt, p->force.v_sig, hydro_get_comoving_pressure(p), p->h,
+      p->force.h_dt, (int)p->density.wcount, p->mass, p->density.rho_dh, p->rho,
+      p->time_bin, p->mat_id);
+}
+
+#endif /* SWIFT_MINIMAL_MULTI_MAT_HYDRO_DEBUG_H */

src/hydro/MinimalMultiMat/hydro_iact.h

+/*******************************************************************************
+ * This file is part of SWIFT.
+ * Copyright (c) 2016 Matthieu Schaller (matthieu.schaller@durham.ac.uk)
+ *
+ * This program is free software: you can redistribute it and/or modify
+ * it under the terms of the GNU Lesser General Public License as published
+ * by the Free Software Foundation, either version 3 of the License, or
+ * (at your option) any later version.
+ *
+ * This program is distributed in the hope that it will be useful,
+ * but WITHOUT ANY WARRANTY; without even the implied warranty of
+ * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
+ * GNU General Public License for more details.
+ *
+ * You should have received a copy of the GNU Lesser General Public License
+ * along with this program.  If not, see <http://www.gnu.org/licenses/>.
+ *
+ ******************************************************************************/
+#ifndef SWIFT_MINIMAL_MULTI_MAT_HYDRO_IACT_H
+#define SWIFT_MINIMAL_MULTI_MAT_HYDRO_IACT_H
+
+/**
+ * @file MinimalMultiMat/hydro_iact.h
+ * @brief MinimalMultiMat conservative implementation of SPH (Neighbour loop equations)
+ *
+ * The thermal variable is the internal energy (u). Simple constant
+ * viscosity term without switches is implemented. No thermal conduction
+ * term is implemented.
+ *
+ * This corresponds to equations (43), (44), (45), (101), (103)  and (104) with
+ * \f$\beta=3\f$ and \f$\alpha_u=0\f$ of Price, D., Journal of Computational
+ * Physics, 2012, Volume 231, Issue 3, pp. 759-794.
+ */
+
+#include "adiabatic_index.h"
+#include "minmax.h"
+
+/**
+ * @brief Density interaction between two particles.
+ *
+ * @param r2 Comoving square distance between the two particles.
+ * @param dx Comoving vector separating both particles (pi - pj).
+ * @param hi Comoving smoothing-length of particle i.
+ * @param hj Comoving smoothing-length of particle j.
+ * @param pi First particle.
+ * @param pj Second particle.
+ * @param a Current scale factor.
+ * @param H Current Hubble parameter.
+ */
+__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 wi, wj, wi_dx, wj_dx;
+
+  /* Get r. */
+  const float r_inv = 1.0f / sqrtf(r2);
+  const float r = r2 * r_inv;
+
+  /* Get the masses. */
+  const float mi = pi->mass;
+  const float mj = pj->mass;
+
+  /* Compute density of pi. */
+  const float hi_inv = 1.f / hi;
+  const float ui = r * hi_inv;
+  kernel_deval(ui, &wi, &wi_dx);
+
+  pi->rho += mj * wi;
+  pi->density.rho_dh -= mj * (hydro_dimension * wi + ui * wi_dx);
+  pi->density.wcount += wi;
+  pi->density.wcount_dh -= (hydro_dimension * wi + ui * wi_dx);
+
+  /* Compute density of pj. */
+  const float hj_inv = 1.f / hj;
+  const float uj = r * hj_inv;
+  kernel_deval(uj, &wj, &wj_dx);
+
+  pj->rho += mi * wj;
+  pj->density.rho_dh -= mi * (hydro_dimension * wj + uj * wj_dx);
+  pj->density.wcount += wj;
+  pj->density.wcount_dh -= (hydro_dimension * wj + uj * wj_dx);
+}
+
+/**
+ * @brief Density interaction between two particles (non-symmetric).
+ *
+ * @param r2 Comoving square distance between the two particles.
+ * @param dx Comoving vector separating both particles (pi - pj).
+ * @param hi Comoving smoothing-length of particle i.
+ * @param hj Comoving smoothing-length of particle j.
+ * @param pi First particle.
+ * @param pj Second particle (not updated).
+ * @param a Current scale factor.
+ * @param H Current Hubble parameter.
+ */
+__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 wi, wi_dx;
+
+  /* Get the masses. */
+  const float mj = pj->mass;
+
+  /* Get r. */
+  const float r_inv = 1.0f / sqrtf(r2);
+  const float r = r2 * r_inv;
+
+  const float h_inv = 1.f / hi;
+  const float ui = r * h_inv;
+  kernel_deval(ui, &wi, &wi_dx);
+
+  pi->rho += mj * wi;
+  pi->density.rho_dh -= mj * (hydro_dimension * wi + ui * wi_dx);
+  pi->density.wcount += wi;
+  pi->density.wcount_dh -= (hydro_dimension * wi + ui * wi_dx);
+}
+
+/**
+ * @brief Force interaction between two particles.
+ *
+ * @param r2 Comoving square distance between the two particles.
+ * @param dx Comoving vector separating both particles (pi - pj).
+ * @param hi Comoving smoothing-length of particle i.
+ * @param hj Comoving smoothing-length of particle j.
+ * @param pi First particle.
+ * @param pj Second particle.
+ * @param a Current scale factor.
+ * @param H Current Hubble parameter.
+ */
+__attribute__((always_inline)) INLINE static void runner_iact_force(
+    float r2, const float *dx, float hi, float hj, struct part *restrict pi,
+    struct part *restrict pj, float a, float H) {
+
+  /* Cosmological factors entering the EoMs */
+  const float fac_mu = pow_three_gamma_minus_five_over_two(a);
+  const float a2_Hubble = a * a * H;
+
+  /* Get r and r inverse. */
+  const float r_inv = 1.0f / sqrtf(r2);
+  const float r = r2 * r_inv;
+
+  /* Recover some data */
+  const float mi = pi->mass;
+  const float mj = pj->mass;
+  const float rhoi = pi->rho;
+  const float rhoj = pj->rho;
+  const float pressurei = pi->force.pressure;
+  const float pressurej = pj->force.pressure;
+
+  /* Get the kernel for hi. */
+  const float hi_inv = 1.0f / hi;
+  const float hid_inv = pow_dimension_plus_one(hi_inv); /* 1/h^(d+1) */
+  const float xi = r * hi_inv;
+  float wi, wi_dx;
+  kernel_deval(xi, &wi, &wi_dx);
+  const float wi_dr = hid_inv * wi_dx;
+
+  /* Get the kernel for hj. */
+  const float hj_inv = 1.0f / hj;
+  const float hjd_inv = pow_dimension_plus_one(hj_inv); /* 1/h^(d+1) */
+  const float xj = r * hj_inv;
+  float wj, wj_dx;
+  kernel_deval(xj, &wj, &wj_dx);
+  const float wj_dr = hjd_inv * wj_dx;
+
+  /* Compute gradient terms */
+  const float P_over_rho2_i = pressurei / (rhoi * rhoi) * pi->force.f;
+  const float P_over_rho2_j = pressurej / (rhoj * rhoj) * pj->force.f;
+
+  /* Compute dv dot r. */
+  const 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] + a2_Hubble * r2;
+
+  /* Are the particles moving towards each others ? */
+  const float omega_ij = min(dvdr, 0.f);
+  const float mu_ij = fac_mu * r_inv * omega_ij; /* This is 0 or negative */
+
+  /* Compute sound speeds and signal velocity */
+  const float ci = pi->force.soundspeed;
+  const float cj = pj->force.soundspeed;
+  const float v_sig = ci + cj - 3.f * mu_ij;
+
+  /* Construct the full viscosity term */
+  const float rho_ij = 0.5f * (rhoi + rhoj);
+  const float visc = -0.5f * const_viscosity_alpha * v_sig * mu_ij / rho_ij;
+
+  /* Convolve with the kernel */
+  const float visc_acc_term = 0.5f * visc * (wi_dr + wj_dr) * r_inv;
+
+  /* SPH acceleration term */
+  const float sph_acc_term =
+      (P_over_rho2_i * wi_dr + P_over_rho2_j * wj_dr) * r_inv;
+
+  /* Assemble the acceleration */
+  const float acc = sph_acc_term + visc_acc_term;
+
+  /* Use the force Luke ! */
+  pi->a_hydro[0] -= mj * acc * dx[0];
+  pi->a_hydro[1] -= mj * acc * dx[1];
+  pi->a_hydro[2] -= mj * acc * dx[2];
+
+  pj->a_hydro[0] += mi * acc * dx[0];
+  pj->a_hydro[1] += mi * acc * dx[1];
+  pj->a_hydro[2] += mi * acc * dx[2];
+
+  /* Get the time derivative for u. */
+  const float sph_du_term_i = P_over_rho2_i * dvdr * r_inv * wi_dr;
+  const float sph_du_term_j = P_over_rho2_j * dvdr * r_inv * wj_dr;
+
+  /* Viscosity term */
+  const float visc_du_term = 0.5f * visc_acc_term * dvdr;
+
+  /* Assemble the energy equation term */
+  const float du_dt_i = sph_du_term_i + visc_du_term;
+  const float du_dt_j = sph_du_term_j + visc_du_term;
+
+  /* Internal energy time derivatibe */
+  pi->u_dt += du_dt_i * mj;
+  pj->u_dt += du_dt_j * mi;
+
+  /* Get the time derivative for h. */
+  pi->force.h_dt -= mj * dvdr * r_inv / rhoj * wi_dr;
+  pj->force.h_dt -= mi * dvdr * r_inv / rhoi * wj_dr;
+
+  /* Update the signal velocity. */
+  pi->force.v_sig = max(pi->force.v_sig, v_sig);
+  pj->force.v_sig = max(pj->force.v_sig, v_sig);
+}
+
+/**
+ * @brief Force interaction between two particles (non-symmetric).
+ *
+ * @param r2 Comoving square distance between the two particles.
+ * @param dx Comoving vector separating both particles (pi - pj).
+ * @param hi Comoving smoothing-length of particle i.
+ * @param hj Comoving smoothing-length of particle j.
+ * @param pi First particle.
+ * @param pj Second particle (not updated).
+ * @param a Current scale factor.
+ * @param H Current Hubble parameter.
+ */
+__attribute__((always_inline)) INLINE static void runner_iact_nonsym_force(
+    float r2, const float *dx, float hi, float hj, struct part *restrict pi,
+    const struct part *restrict pj, float a, float H) {
+
+  /* Cosmological factors entering the EoMs */
+  const float fac_mu = pow_three_gamma_minus_five_over_two(a);
+  const float a2_Hubble = a * a * H;
+
+  /* Get r and r inverse. */
+  const float r_inv = 1.0f / sqrtf(r2);
+  const float r = r2 * r_inv;
+
+  /* Recover some data */
+  // const float mi = pi->mass;
+  const float mj = pj->mass;
+  const float rhoi = pi->rho;
+  const float rhoj = pj->rho;
+  const float pressurei = pi->force.pressure;
+  const float pressurej = pj->force.pressure;
+
+  /* Get the kernel for hi. */
+  const float hi_inv = 1.0f / hi;
+  const float hid_inv = pow_dimension_plus_one(hi_inv); /* 1/h^(d+1) */
+  const float xi = r * hi_inv;
+  float wi, wi_dx;
+  kernel_deval(xi, &wi, &wi_dx);
+  const float wi_dr = hid_inv * wi_dx;
+
+  /* Get the kernel for hj. */
+  const float hj_inv = 1.0f / hj;
+  const float hjd_inv = pow_dimension_plus_one(hj_inv); /* 1/h^(d+1) */
+  const float xj = r * hj_inv;
+  float wj, wj_dx;
+  kernel_deval(xj, &wj, &wj_dx);
+  const float wj_dr = hjd_inv * wj_dx;
+
+  /* Compute gradient terms */
+  const float P_over_rho2_i = pressurei / (rhoi * rhoi) * pi->force.f;
+  const float P_over_rho2_j = pressurej / (rhoj * rhoj) * pj->force.f;
+
+  /* Compute dv dot r. */
+  const 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] + a2_Hubble * r2;
+
+  /* Are the particles moving towards each others ? */
+  const float omega_ij = min(dvdr, 0.f);
+  const float mu_ij = fac_mu * r_inv * omega_ij; /* This is 0 or negative */
+
+  /* Compute sound speeds and signal velocity */
+  const float ci = pi->force.soundspeed;
+  const float cj = pj->force.soundspeed;
+  const float v_sig = ci + cj - 3.f * mu_ij;
+
+  /* Construct the full viscosity term */
+  const float rho_ij = 0.5f * (rhoi + rhoj);
+  const float visc = -0.5f * const_viscosity_alpha * v_sig * mu_ij / rho_ij;
+
+  /* Convolve with the kernel */
+  const float visc_acc_term = 0.5f * visc * (wi_dr + wj_dr) * r_inv;
+
+  /* SPH acceleration term */
+  const float sph_acc_term =
+      (P_over_rho2_i * wi_dr + P_over_rho2_j * wj_dr) * r_inv;
+
+  /* Assemble the acceleration */
+  const float acc = sph_acc_term + visc_acc_term;
+
+  /* Use the force Luke ! */
+  pi->a_hydro[0] -= mj * acc * dx[0];
+  pi->a_hydro[1] -= mj * acc * dx[1];
+  pi->a_hydro[2] -= mj * acc * dx[2];
+
+  /* Get the time derivative for u. */
+  const float sph_du_term_i = P_over_rho2_i * dvdr * r_inv * wi_dr;
+
+  /* Viscosity term */
+  const float visc_du_term = 0.5f * visc_acc_term * dvdr;
+
+  /* Assemble the energy equation term */
+  const float du_dt_i = sph_du_term_i + visc_du_term;
+
+  /* Internal energy time derivatibe */
+  pi->u_dt += du_dt_i * mj;
+
+  /* Get the time derivative for h. */
+  pi->force.h_dt -= mj * dvdr * r_inv / rhoj * wi_dr;
+
+  /* Update the signal velocity. */
+  pi->force.v_sig = max(pi->force.v_sig, v_sig);
+}
+
+#endif /* SWIFT_MINIMAL_MULTI_MAT_HYDRO_IACT_H */

src/hydro/MinimalMultiMat/hydro_io.h

+/*******************************************************************************
+ * This file is part of SWIFT.
+ * Coypright (c) 2016 Matthieu Schaller (matthieu.schaller@durham.ac.uk)
+ *
+ * This program is free software: you can redistribute it and/or modify
+ * it under the terms of the GNU Lesser General Public License as published
+ * by the Free Software Foundation, either version 3 of the License, or
+ * (at your option) any later version.
+ *
+ * This program is distributed in the hope that it will be useful,
+ * but WITHOUT ANY WARRANTY; without even the implied warranty of
+ * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
+ * GNU General Public License for more details.
+ *
+ * You should have received a copy of the GNU Lesser General Public License
+ * along with this program.  If not, see <http://www.gnu.org/licenses/>.
+ *
+ ******************************************************************************/
+#ifndef SWIFT_MINIMAL_MULTI_MAT_HYDRO_IO_H
+#define SWIFT_MINIMAL_MULTI_MAT_HYDRO_IO_H
+
+/**
+ * @file MinimalMultiMat/hydro_io.h
+ * @brief MinimalMultiMat conservative implementation of SPH (i/o routines)
+ *
+ * The thermal variable is the internal energy (u). Simple constant
+ * viscosity term without switches is implemented. No thermal conduction
+ * term is implemented.
+ *
+ * This corresponds to equations (43), (44), (45), (101), (103)  and (104) with
+ * \f$\beta=3\f$ and \f$\alpha_u=0\f$ of
+ * Price, D., Journal of Computational Physics, 2012, Volume 231, Issue 3,
+ * pp. 759-794.
+ */
+
+#include "adiabatic_index.h"
+#include "hydro.h"
+#include "io_properties.h"
+#include "kernel_hydro.h"
+
+/**
+ * @brief Specifies which particle fields to read from a dataset
+ *
+ * @param parts The particle array.
+ * @param list The list of i/o properties to read.
+ * @param num_fields The number of i/o fields to read.
+ */
+void hydro_read_particles(struct part* parts, struct io_props* list,
+                          int* num_fields) {
+
+  *num_fields = 8;
+
+  /* List what we want to read */
+  list[0] = io_make_input_field("Coordinates", DOUBLE, 3, COMPULSORY,
+                                UNIT_CONV_LENGTH, parts, x);
+  list[1] = io_make_input_field("Velocities", FLOAT, 3, COMPULSORY,
+                                UNIT_CONV_SPEED, parts, v);
+  list[2] = io_make_input_field("Masses", FLOAT, 1, COMPULSORY, UNIT_CONV_MASS,
+                                parts, mass);
+  list[3] = io_make_input_field("SmoothingLength", FLOAT, 1, COMPULSORY,
+                                UNIT_CONV_LENGTH, parts, h);
+  list[4] = io_make_input_field("InternalEnergy", FLOAT, 1, COMPULSORY,
+                                UNIT_CONV_ENERGY_PER_UNIT_MASS, parts, u);
+  list[5] = io_make_input_field("ParticleIDs", ULONGLONG, 1, COMPULSORY,
+                                UNIT_CONV_NO_UNITS, parts, id);
+  list[6] = io_make_input_field("Accelerations", FLOAT, 3, OPTIONAL,
+                                UNIT_CONV_ACCELERATION, parts, a_hydro);
+  list[7] = io_make_input_field("Density", FLOAT, 1, OPTIONAL,
+                                UNIT_CONV_DENSITY, parts, rho);
+  list[8] = io_make_input_field("MaterialID", INT, 1, OPTIONAL, 1, parts,
+                                mat_id);
+}
+
+void convert_S(const struct engine* e, const struct part* p,
+               const struct xpart* xp, float* ret) {
+
+  ret[0] = hydro_get_comoving_entropy(p);
+}
+
+void convert_P(const struct engine* e, const struct part* p,
+               const struct xpart* xp, float* ret) {
+
+  ret[0] = hydro_get_comoving_pressure(p);
+}
+
+void convert_part_pos(const struct engine* e, const struct part* p,
+                      const struct xpart* xp, double* ret) {
+
+  if (e->s->periodic) {
+    ret[0] = box_wrap(p->x[0], 0.0, e->s->dim[0]);
+    ret[1] = box_wrap(p->x[1], 0.0, e->s->dim[1]);
+    ret[2] = box_wrap(p->x[2], 0.0, e->s->dim[2]);
+  } else {
+    ret[0] = p->x[0];
+    ret[1] = p->x[1];
+    ret[2] = p->x[2];
+  }
+}
+
+void convert_part_vel(const struct engine* e, const struct part* p,
+                      const struct xpart* xp, float* ret) {
+
+  const int with_cosmology = (e->policy & engine_policy_cosmology);
+  const struct cosmology* cosmo = e->cosmology;
+  const integertime_t ti_current = e->ti_current;
+  const double time_base = e->time_base;
+
+  const integertime_t ti_beg = get_integer_time_begin(ti_current, p->time_bin);
+  const integertime_t ti_end = get_integer_time_end(ti_current, p->time_bin);
+
+  /* Get time-step since the last kick */
+  float dt_kick_grav, dt_kick_hydro;
+  if (with_cosmology) {
+    dt_kick_grav = cosmology_get_grav_kick_factor(cosmo, ti_beg, ti_current);
+    dt_kick_grav -=
+        cosmology_get_grav_kick_factor(cosmo, ti_beg, (ti_beg + ti_end) / 2);
+    dt_kick_hydro = cosmology_get_hydro_kick_factor(cosmo, ti_beg, ti_current);
+    dt_kick_hydro -=
+        cosmology_get_hydro_kick_factor(cosmo, ti_beg, (ti_beg + ti_end) / 2);
+  } else {
+    dt_kick_grav = (ti_current - ((ti_beg + ti_end) / 2)) * time_base;
+    dt_kick_hydro = (ti_current - ((ti_beg + ti_end) / 2)) * time_base;
+  }
+
+  /* Extrapolate the velocites to the current time */
+  hydro_get_drifted_velocities(p, xp, dt_kick_hydro, dt_kick_grav, ret);
+
+  /* Conversion from internal units to peculiar velocities */
+  ret[0] *= cosmo->a2_inv;
+  ret[1] *= cosmo->a2_inv;
+  ret[2] *= cosmo->a2_inv;
+}
+
+void convert_part_potential(const struct engine* e, const struct part* p,
+                            const struct xpart* xp, float* ret) {
+
+  if (p->gpart != NULL)
+    ret[0] = gravity_get_comoving_potential(p->gpart);
+  else
+    ret[0] = 0.f;
+}
+
+/**
+ * @brief Specifies which particle fields to write to a dataset
+ *
+ * @param parts The particle array.
+ * @param xparts The extended particle array.
+ * @param list The list of i/o properties to write.
+ * @param num_fields The number of i/o fields to write.
+ */
+void hydro_write_particles(const struct part* parts, const struct xpart* xparts,
+