Op_Diff_PolyMAC_HFV_Elem.cpp

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#include <Echange_contact_PolyMAC_HFV.h>
#include <Op_Diff_PolyMAC_HFV_Elem.h>
#include <Champ_Elem_PolyMAC_HFV.h>
#include <Echange_externe_impose.h>
#include <Domaine_PolyMAC_HFV.h>
#include <Domaine_Cl_PolyMAC_family.h>
#include <Flux_parietal_base.h>
#include <Pb_Multiphase.h>
#include <Matrix_tools.h>
#include <Array_tools.h>
#include <deque>
#include <Perf_counters.h>
 
Implemente_instanciable_sans_constructeur(Op_Diff_PolyMAC_HFV_Elem, "Op_Diff_PolyMAC_HFV_Elem|Op_Diff_PolyMAC_HFV_var_Elem", Op_Diff_PolyMAC_HFV_base);
 
Op_Diff_PolyMAC_HFV_Elem::Op_Diff_PolyMAC_HFV_Elem()
{
  declare_support_masse_volumique(1);
}
 
Sortie& Op_Diff_PolyMAC_HFV_Elem::printOn(Sortie& os) const { return Op_Diff_PolyMAC_HFV_base::printOn(os); }
 
Entree& Op_Diff_PolyMAC_HFV_Elem::readOn(Entree& is) { return Op_Diff_PolyMAC_HFV_base::readOn(is); }
 
void Op_Diff_PolyMAC_HFV_Elem::completer()
{
  Op_Diff_PolyMAC_HFV_base::completer();
  Equation_base& eq = equation();
  Champ_Elem_PolyMAC_HFV& ch = ref_cast(Champ_Elem_PolyMAC_HFV, le_champ_inco ? le_champ_inco.valeur() : eq.inconnue());
  ch.init_auxiliary_variables();
  const Domaine_PolyMAC_HFV& domaine = ref_cast(Domaine_PolyMAC_HFV, le_dom_poly_.valeur());
  if (domaine.domaine().nb_joints() && domaine.domaine().joint(0).epaisseur() < 1)
    {
      Cerr << "Op_Diff_PolyMAC_HFV_Elem : largeur de joint insuffisante (minimum 1)!" << finl;
      Process::exit();
    }
  flux_bords_.resize(domaine.premiere_face_int(), ch.valeurs().line_size());
}
 
void Op_Diff_PolyMAC_HFV_Elem::init_op_ext() const
{
  if (op_ext.size())
    return; //deja fait
  /* recherche d'operateurs connectes par des Echange_Contact_PolyMAC_HFV (eventuellement indirectement) */
  std::set<const Op_Diff_PolyMAC_HFV_Elem*> ops_tbd = { this }, ops; //operateurs a scanner pour remplir op_ext, operateurs trouves
  while (ops_tbd.size())
    {
      const Op_Diff_PolyMAC_HFV_Elem *op = *ops_tbd.begin();
      ops_tbd.erase(ops_tbd.begin()), ops.insert(op);
      const Conds_lim& cls = op->equation().domaine_Cl_dis().les_conditions_limites();
      for (const auto &itr : cls)
        if (sub_type(Echange_contact_PolyMAC_HFV, itr.valeur()))
          {
            const Echange_contact_PolyMAC_HFV& cl = ref_cast(Echange_contact_PolyMAC_HFV, itr.valeur());
            cl.init_op();
            if (!ops.count(&cl.o_diff.valeur()))
              ops_tbd.insert(&cl.o_diff.valeur()); //on a un nouvel operateur a scanner
          }
    }
  op_ext = { this };
  for (auto &&op : ops)
    if (op != this)
      op_ext.push_back(op); /* remplissage de op_ext avec l'operateur local en 1er */
 
  /* remplissage des o_idx des Echange_Contact_PolyMAC_HFV connectes */
  const Conds_lim& cls = equation().domaine_Cl_dis().les_conditions_limites();
  for (int i = 0; i < cls.size(); i++)
    if (sub_type(Echange_contact_PolyMAC_HFV, cls[i].valeur()))
      {
        const Echange_contact_PolyMAC_HFV& cl = ref_cast(Echange_contact_PolyMAC_HFV, cls[i].valeur());
        cl.o_idx = (int) (std::find(op_ext.begin(), op_ext.end(), &cl.o_diff.valeur()) - op_ext.begin());
      }
}
 
double Op_Diff_PolyMAC_HFV_Elem::calculer_dt_stab() const
{
  const Domaine_PolyMAC_HFV& domaine = ref_cast(Domaine_PolyMAC_HFV, le_dom_poly_.valeur());
  const IntTab& e_f = domaine.elem_faces();
  const DoubleTab& nf = domaine.face_normales(), *alp = sub_type(Pb_Multiphase, equation().probleme()) ? &ref_cast(Pb_Multiphase, equation().probleme()).equation_masse().inconnue().passe() : nullptr, &diffu =
                                                          diffusivite_pour_pas_de_temps().valeurs(), &lambda = diffusivite().valeurs();
  const DoubleVect& pe = equation().milieu().porosite_elem(), &vf = domaine.volumes_entrelaces(), &ve = domaine.volumes();
  update_nu();
 
  int i, e, f, n, N = equation().inconnue().valeurs().dimension(1), cD = diffu.dimension(0) == 1, cL = lambda.dimension(0) == 1;
  double dt = 1e10;
  DoubleTrav flux(N);
  for (e = 0; e < domaine.nb_elem(); e++)
    {
      for (flux = 0, i = 0; i < e_f.dimension(1) && (f = e_f(e, i)) >= 0; i++)
        for (n = 0; n < N; n++)
          flux(n) += domaine.nu_dot(&nu_, e, n, &nf(f, 0), &nf(f, 0)) / vf(f);
      for (n = 0; n < N; n++)
        if ((!alp || (*alp)(e, n) > 1e-3) && flux(n)) /* sous 0.5e-6, on suppose que l'evanescence fait le job */
          dt = std::min(dt, pe(e) * ve(e) * (alp ? (*alp)(e, n) : 1) * (lambda(!cL * e, n) / diffu(!cD * e, n)) / flux(n));
      if (dt < 0)
        abort();
    }
  return Process::mp_min(dt);
}
 
void Op_Diff_PolyMAC_HFV_Elem::dimensionner_blocs_ext(int aux_only, matrices_t matrices, const tabs_t& semi_impl) const
{
  init_op_ext();
  const std::string& nom_inco = (le_champ_inco ? le_champ_inco.valeur() : equation().inconnue()).le_nom().getString();
  int i, j, k, l, e, o_e, f, o_f, fb, m, n, M, n_ext = (int) op_ext.size(), n_sten = 0, semi = (int) semi_impl.count(nom_inco);
  long p;
  std::vector<Matrice_Morse*> mat(n_ext); //matrices
  std::vector<int> N, ne_tot; //composantes, nombre d'elements total par pb
  std::vector<std::reference_wrapper<const Domaine_PolyMAC_HFV>> domaine; //domaines
  std::vector<std::reference_wrapper<const Conds_lim>> cls; //conditions aux limites
  std::vector<std::reference_wrapper<const IntTab>> fcl, e_f, f_e; //tableaux "fcl", "elem_faces", "faces_voisins"
  std::vector<std::reference_wrapper<const DoubleTab>> diffu, inco; //inconnues, normales aux faces, positions elems / faces / sommets
  std::deque<ConstDoubleTab_parts> v_part; //blocs de chaque inconnue
  std::vector<Stencil> stencil(n_ext); //stencils par matrice
  for (i = 0, M = 0; i < n_ext; M = std::max(M, N[i]), i++)
    {
      std::string nom_mat = i ? nom_inco + "/" + op_ext[i]->equation().probleme().le_nom().getString() : nom_inco;
      mat[i] = matrices.count(nom_mat) ? matrices.at(nom_mat) : nullptr;
      domaine.push_back(std::ref(ref_cast(Domaine_PolyMAC_HFV, op_ext[i]->equation().domaine_dis())));
      f_e.push_back(std::ref(domaine[i].get().face_voisins())), e_f.push_back(std::ref(domaine[i].get().elem_faces()));
      cls.push_back(std::ref(op_ext[i]->equation().domaine_Cl_dis().les_conditions_limites()));
      diffu.push_back(ref_cast(Op_Diff_PolyMAC_HFV_Elem, *op_ext[i]).nu());
      const Champ_Elem_PolyMAC_HFV& ch = ref_cast(Champ_Elem_PolyMAC_HFV, op_ext[i]->has_champ_inco() ? op_ext[i]->mon_inconnue() : op_ext[i]->equation().inconnue());
 
      N.push_back(ch.valeurs().line_size()), fcl.push_back(std::ref(ch.fcl())), ne_tot.push_back(domaine[i].get().nb_elem_tot());
      inco.push_back(ch.valeurs()), v_part.emplace_back(ch.valeurs());
      stencil[i].resize(0, 2);
 
    }
 
  IntTrav tpfa(0, N[0]); //pour suivre quels flux sont a deux points
  domaine[0].get().creer_tableau_faces(tpfa), tpfa = 1;
 
  if (!aux_only)
    Cerr << "Op_Diff_PolyMAC_HFV_Elem::dimensionner() : ";
  DoubleTrav w2;
  /* probleme local */
  for (e = 0; e < ne_tot[0]; e++)
    {
      domaine[0].get().W2(&diffu[0].get(), e, w2); //interpolation : [n_ef.nu grad T]_f = w2_{ff'} (T_f' - T_e)
      //element <-> toutes ses faces (non Dirichlet)
      if (!aux_only && !semi)
        for (i = 0; i < w2.dimension(0); i++)
          if (!semi && fcl[0](f = e_f[0](e, i), 0) < 6)
            {
              if (e < domaine[0].get().nb_elem())
                for (n = 0; n < N[0]; n++)
                  stencil[0].append_line(N[0] * e + n, N[0] * (ne_tot[0] + f) + n);
              if (f < domaine[0].get().nb_faces())
                for (n = 0; n < N[0]; n++)
                  stencil[0].append_line(N[0] * (ne_tot[0] + f) + n, N[0] * e + n);
            }
      //face <-> face (si les deux sont non Dirichlet)
      for (i = 0; i < w2.dimension(0); i++)
        if ((f = e_f[0](e, i)) >= domaine[0].get().nb_faces())
          continue; //face virtuelle -> rien
        else if (semi || fcl[0](f = e_f[0](e, i), 0) > 5)
          for (n = 0; n < N[0]; n++) //Dirichlet ou semi-implicite -> diagonale
            stencil[0].append_line(N[0] * (!aux_only * ne_tot[0] + f) + n, N[0] * (!aux_only * ne_tot[0] + f) + n);
        else
          for (j = 0; j < w2.dimension(1); j++)
            for (fb = e_f[0](e, j), n = 0; n < N[0]; n++) //cas reel
              if (fcl[0](fb, 0) < 6 && w2(i, j, n))
                stencil[0].append_line(N[0] * (!aux_only * ne_tot[0] + f) + n, N[0] * (!aux_only * ne_tot[0] + fb) + n), tpfa(f, n) &= (i == j);
    }
  /* problemes distants : pour les Echange_contact */
  const Echange_contact_PolyMAC_HFV *pcl;
  if (!semi)
    for (i = 0; i < cls[0].get().size(); i++)
      if ((pcl = sub_type(Echange_contact_PolyMAC_HFV, cls[0].get()[i].valeur()) ? &ref_cast(Echange_contact_PolyMAC_HFV, cls[0].get()[i].valeur()) : nullptr))
        for (pcl->init_f_dist(), j = 0, p = std::find(op_ext.begin(), op_ext.end(), &pcl->o_diff.valeur()) - op_ext.begin(); j < pcl->fvf->nb_faces(); j++)
          {
            f = pcl->fvf->num_face(j), o_f = pcl->f_dist(j), o_e = f_e[p](o_f, 0); //faces cote local/distant, elem cote distant
            domaine[p].get().W2(&diffu[p].get(), o_e, w2); //matrice w2 de l'autre cote
            k = (int) (std::find(&e_f[p](o_e, 0), &e_f[p](o_e, 0) + w2.dimension(0), o_f) - &e_f[p](o_e, 0)); //indice de o_f dans o_e
            if (!aux_only)
              for (n = 0; n < N[0]; n++)
                for (m = (N[0] == N[p]) * n; m < (N[0] == N[p] ? n + 1 : N[p]); m++)
                  stencil[p].append_line(N[0] * (ne_tot[0] + f) + n, N[p] * o_e + m); //face <-> elem : compo par compo si N[0] == N[p], tout sinon
            for (l = 0; l < w2.dimension(0); l++)
              if (fcl[p](fb = e_f[p](o_e, l), 0) < 6)
                for (n = 0; n < N[0]; n++)
                  for (m = (N[0] == N[p]) * n; m < (N[0] == N[p] ? n + 1 : N[p]); m++)
                    if (w2(k, l, m))
                      stencil[p].append_line(N[0] * (!aux_only * ne_tot[0] + f) + n, N[p] * (!aux_only * ne_tot[p] + fb) + m);
          }
 
  for (i = 0; i < n_ext; i++)
    if (mat[i])
      {
        tableau_trier_retirer_doublons(stencil[i]);
        Matrice_Morse mat2;
        Matrix_tools::allocate_morse_matrix(aux_only ? v_part[0][1].size_totale() : inco[0].get().size_totale(), aux_only ? v_part[i][1].size_totale() : inco[i].get().size_totale(), stencil[i], mat2);
        mat[i]->nb_colonnes() ? *mat[i] += mat2 : *mat[i] = mat2;
      }
 
  for (auto &&st : stencil)
    n_sten += st.dimension(0); //n_sten : nombre total de points du stencil de l'operateur
  if (!aux_only)
    {
      const double elem_face_t = static_cast<double>(domaine[0].get().mdv_elems_faces->nb_items_seq_tot()),
                   face_t = static_cast<double>(domaine[0].get().md_vector_faces()->nb_items_seq_tot());
      Cerr << "width " << mp_sum_as_double(n_sten) / (N[0] * elem_face_t) << " "
           << mp_somme_vect_as_double(tpfa) * 100. / (N[0] * face_t) << "% TPFA " << finl;
    }
}
 
void Op_Diff_PolyMAC_HFV_Elem::ajouter_blocs_ext(int aux_only, matrices_t matrices, DoubleTab& secmem, const tabs_t& semi_impl) const
{
  init_op_ext();
  const std::string& nom_inco = (le_champ_inco ? le_champ_inco.valeur() : equation().inconnue()).le_nom().getString();
  int i, j, k1, k2, e, f, fb, n, M, n_ext = (int) op_ext.size(), semi = (int) semi_impl.count(nom_inco), d, D = dimension;
  std::vector<Matrice_Morse*> mat(n_ext); //matrices
  std::vector<int> N, ne_tot; //composantes
  std::vector<std::reference_wrapper<const Domaine_PolyMAC_HFV>> domaine; //domaines
  std::vector<std::reference_wrapper<const Conds_lim>> cls; //conditions aux limites
  std::vector<std::reference_wrapper<const IntTab>> fcl, e_f, f_e, f_s; //tableaux "fcl", "elem_faces", "faces_voisins"
  std::vector<std::reference_wrapper<const DoubleVect>> fs, pf, pe, ve; //surfaces
  std::vector<std::reference_wrapper<const DoubleTab>> inco, xp, xv, diffu, v_aux; //inconnues, normales aux faces, positions elems / faces / sommets
  std::deque<ConstDoubleTab_parts> v_part; //blocs de chaque inconnue
  std::vector<const Flux_parietal_base*> corr; //correlations de flux parietal (si elles existent)
  for (i = 0, M = 0; i < n_ext; M = std::max(M, N[i]), i++)
    {
      std::string nom_mat = i ? nom_inco + "/" + op_ext[i]->equation().probleme().le_nom().getString() : nom_inco;
      mat[i] = matrices.count(nom_mat) ? matrices.at(nom_mat) : nullptr;
      domaine.push_back(std::ref(ref_cast(Domaine_PolyMAC_HFV, op_ext[i]->equation().domaine_dis())));
      f_e.push_back(std::ref(domaine[i].get().face_voisins())), e_f.push_back(std::ref(domaine[i].get().elem_faces())), f_s.push_back(std::ref(domaine[i].get().face_sommets()));
      fs.push_back(std::ref(domaine[i].get().face_surfaces()));
      xp.push_back(std::ref(domaine[i].get().xp())), xv.push_back(std::ref(domaine[i].get().xv()));
      pe.push_back(std::ref(equation().milieu().porosite_elem())), pf.push_back(std::ref(equation().milieu().porosite_face())), ve.push_back(std::ref(domaine[i].get().volumes()));
      cls.push_back(std::ref(op_ext[i]->equation().domaine_Cl_dis().les_conditions_limites()));
      diffu.push_back(ref_cast(Op_Diff_PolyMAC_HFV_Elem, *op_ext[i]).nu());
      const Champ_Elem_PolyMAC_HFV& ch = ref_cast(Champ_Elem_PolyMAC_HFV, op_ext[i]->has_champ_inco() ? op_ext[i]->mon_inconnue() : op_ext[i]->equation().inconnue());
      inco.push_back(std::ref(semi_impl.count(nom_mat) ? semi_impl.at(nom_mat) : ch.valeurs())), v_part.emplace_back(inco.back());
      corr.push_back(
        sub_type(Energie_Multiphase, op_ext[i]->equation()) && op_ext[i]->equation().probleme().has_correlation("flux_parietal") ?
        &ref_cast(Flux_parietal_base, op_ext[i]->equation().probleme().get_correlation("flux_parietal")) : nullptr);
      N.push_back(inco[i].get().line_size()), ne_tot.push_back(domaine[i].get().nb_elem_tot()), fcl.push_back(std::ref(ch.fcl()));
    }
 
  /* que faire avec les variables auxiliaires ? */
  double t = equation().schema_temps().temps_courant(), dt = equation().schema_temps().pas_de_temps(), fac, prefac;
  if (aux_only)
    use_aux_ = 0; /* 1) on est en train d'assembler le systeme de resolution des variables auxiliaires lui-meme */
  else if (mat[0] && !semi)
    t_last_aux_ = t + dt, use_aux_ = 0; /* 2) on est en implicite complet : pas besoin de mat_aux / var_aux, on aura les variables a t + dt */
  else if (t_last_aux_ < t)
    update_aux(t); /* 3) premier pas a ce temps en semi-implicite : on calcule les variables auxiliaires a t et on les stocke dans var_aux */
  for (i = 0; i < n_ext; i++)
    v_aux.push_back(use_aux_ ? ref_cast(Op_Diff_PolyMAC_HFV_Elem, *op_ext[i]).var_aux : v_part[i][1]); /* les variables auxiliaires peuvent etre soit dans inco/semi_impl (cas 1), soit dans var_aux (cas 2) */
 
  DoubleTrav w2, flux(N[0]), acc(N[0]);
  for (e = 0; e < ne_tot[0]; e++)
    {
      domaine[0].get().W2(&diffu[0].get(), e, w2); //interpolation : [n_ef.nu grad T]_f = w2_{ff'} (T_f' - T_e)
 
      for (i = 0; i < w2.dimension(0); i++) //seconds membres
        {
          for (f = e_f[0](e, i), flux = 0, j = 0; j < w2.dimension(1); j++)
            for (fb = e_f[0](e, j), n = 0; n < N[0]; n++)
              flux(n) += w2(i, j, n) * (v_aux[0](fb, n) - inco[0](e, n));
          if (!semi && fcl[0](f, 0) < 6)
            for (n = 0; n < N[0]; n++)
              secmem(!aux_only * ne_tot[0] + f, n) -= flux(n);
          if (!aux_only)
            for (n = 0; n < N[0]; n++)
              secmem(e, n) += flux(n);
          if (!aux_only && f < domaine[0].get().premiere_face_int())
            for (n = 0; n < N[0]; n++)
              flux_bords_(f, n) = flux(n); //flux aux bords
        }
 
      if (semi || !mat[0])
        continue;
      //matrice: elem-elem
      for (acc = 0, i = 0; i < w2.dimension(0); i++)
        for (j = 0; j < w2.dimension(1); j++)
          for (n = 0; n < N[0]; n++)
            acc(n) += w2(i, j, n);
      if (!aux_only && e < domaine[0].get().nb_elem())
        for (n = 0; n < N[0]; n++)
          (*mat[0])(N[0] * e + n, N[0] * e + n) += acc(n);
      //matrice: elem-face
      if (!aux_only)
        for (i = 0; i < w2.dimension(0); i++)
          if (fcl[0](f = e_f[0](e, i), 0) < 6)
            {
              for (acc = 0, j = 0; j < w2.dimension(1); j++)
                for (n = 0; n < N[0]; n++)
                  acc(n) += w2(i, j, n);
              if (f < domaine[0].get().nb_faces())
                for (n = 0; n < N[0]; n++)
                  (*mat[0])(N[0] * (ne_tot[0] + f) + n, N[0] * e + n) -= acc(n);
              if (e < domaine[0].get().nb_elem())
                for (n = 0; n < N[0]; n++)
                  (*mat[0])(N[0] * e + n, N[0] * (ne_tot[0] + f) + n) -= acc(n);
            }
      //matrice : face-face
      for (i = 0; i < w2.dimension(0); i++)
        if (fcl[0](f = e_f[0](e, i), 0) < 6 && f < domaine[0].get().nb_faces())
          for (j = 0; j < w2.dimension(1); j++)
            if (fcl[0](fb = e_f[0](e, j), 0) < 6)
              for (n = 0; n < N[0]; n++)
                if (w2(i, j, n))
                  (*mat[0])(N[0] * (!aux_only * ne_tot[0] + f) + n, N[0] * (!aux_only * ne_tot[0] + fb) + n) += w2(i, j, n);
    }
 
  //contributions restantes aux equations aux faces
  for (f = 0; f < domaine[0].get().nb_faces(); f++)
    if (!aux_only && semi && mat[0])
      for (n = 0; n < N[0]; n++) //semi-implicite : T_f^+ = var_aux
        secmem(ne_tot[0] + f, n) += v_aux[0](f, n) - (le_champ_inco ? le_champ_inco->valeurs() : equation().inconnue().valeurs())(ne_tot[0] + f, n), (*mat[0])(N[0] * (ne_tot[0] + f) + n,
                                    N[0] * (ne_tot[0] + f) + n)++;
    else if (fcl[0](f, 0) == 0 || fcl[0](f, 0) == 5)
      continue; //face interne ou Neumann_val_ext -> rien
    else if (corr[0]) //Pb_Multiphase avec flux parietal -> on ne traite (pour le moment) que Dirichlet et Echange_contact
      {
        if (fcl[0](f, 0) == 2)
          abort(); //Echange_global_impose -> on ne sait pas faire (que vaut T_paroi dans l'element?)
        const Echange_contact_PolyMAC_HFV *ech = fcl[0](f, 0) == 3 ? &ref_cast(Echange_contact_PolyMAC_HFV, cls[0].get()[fcl[0](f, 1)].valeur()) : nullptr;
        int o_p = ech ? ech->o_idx : -1, o_f = ech ? ech->f_dist(fcl[0](f, 2)) : -1;
        const Pb_Multiphase& pbm = ref_cast(Pb_Multiphase, equation().probleme());
        const DoubleTab& alpha = pbm.equation_masse().inconnue().passe(), &dh = pbm.milieu().diametre_hydraulique_elem(),
                         &press = ref_cast(QDM_Multiphase, pbm.equation_qdm()).pression().passe(), &vit = pbm.equation_qdm().inconnue().passe(),
                          &lambda = pbm.milieu().conductivite().passe(), &mu = ref_cast(Fluide_base, pbm.milieu()).viscosite_dynamique().passe(), &rho = pbm.milieu().masse_volumique().passe(), &Cp =
                                                                                 pbm.milieu().capacite_calorifique().passe();
        Flux_parietal_base::input_t in;
        Flux_parietal_base::output_t out;
        DoubleTrav qpk(N[0]), dTf_qpk(N[0], N[0]), dTp_qpk(N[0]), qpi(N[0], N[0]), dTf_qpi(N[0], N[0], N[0]), dTp_qpi(N[0], N[0]), v(N[0], D), nv(N[0]);
        in.N = N[0], in.f = f, in.D_h = dh(e), in.D_ch = dh(e), in.alpha = &alpha(e, 0), in.T = &v_aux[0](f, 0), in.p = press(e), in.v = nv.addr(), in.lambda = &lambda(e, 0), in.mu = &mu(e, 0), in.rho =
                                                                                                                          &rho(e, 0), in.Cp = &Cp(e, 0);
        out.qpk = &qpk, out.dTf_qpk = &dTf_qpk, out.dTp_qpk = &dTp_qpk, out.qpi = &qpi, out.dTf_qpi = &dTf_qpi, out.dTp_qpi = &dTp_qpi;
        for (e = f_e[0](f, 0), i = 0; i < e_f[0].get().dimension(1) && (fb = e_f[0](e, i)) >= 0; i++)
          for (prefac = fs[0](fb) * pf[0](fb) * (e == f_e[0](fb, 0) ? 1 : -1) / (pe[0](e) * ve[0](e)), n = 0; n < N[0]; n++)
            for (fac = prefac * vit(fb, n), d = 0; d < D; d++)
              v(n, d) += fac * (xv[0](fb, d) - xp[0](e, d));
        for (n = 0; n < N[0]; n++)
          nv(n) = sqrt(domaine[0].get().dot(&v(n, 0), &v(n, 0)));
        //Tparoi : estimation initiale + Newton si on ne la connait pas
        double h_imp = fcl[0](f, 0) == 1 ? ref_cast(Echange_impose_base, cls[0].get()[fcl[0](f, 1)].valeur()).h_imp(fcl[0](f, 2), 0) : 0, T_ext =
                         fcl[0](f, 0) == 1 ? ref_cast(Echange_impose_base, cls[0].get()[fcl[0](f, 1)].valeur()).T_ext(fcl[0](f, 2), 0) : 0, dTp, FT, dFTp;
        in.Tp = ech ? v_aux[o_p](o_f, 0) : fcl[0](f, 0) == 5 ? 0 : fcl[0](f, 0) == 6 ? ref_cast(Dirichlet, cls[0].get()[fcl[0](f, 1)].valeur()).val_imp(fcl[0](f, 2), 0) :
                fcl[0](f, 0) == 1 ? T_ext : v_aux[0](f, 0);
        //appel : on n'est implicite qu'en les temperatures
        dTp = 0;
        for (int it = 0; it < 10 && (!it || std::abs(dTp) > 1e-5); in.Tp += dTp, it++)
          {
            corr[0]->qp(in, out);
            for (FT = 0, dFTp = 0; n < N[0]; n++)
              FT += qpk(n), dFTp += dTp_qpk(n);
            dTp = fcl[0](f, 0) == 5 ? (ref_cast(Neumann, cls[0].get()[fcl[0](f, 1)].valeur()).flux_impose(fcl[0](f, 2), 0) - FT) / dFTp :
                  fcl[0](f, 0) == 1 ? (h_imp * (T_ext - in.Tp) - FT) / (dFTp + h_imp) : 0;
          }
        for (n = 0; n < N[0]; n++)
          secmem(!aux_only * ne_tot[0] + f, n) += fs[0](f) * qpk(n); //second membre
        if (mat[0])
          for (k1 = 0; k1 < N[0]; k1++)
            for (k2 = 0; k2 < N[0]; k2++) //derivees en Tfluide
              (*mat[0])(N[0] * (!aux_only * ne_tot[0] + f) + k1, N[0] * (!aux_only * ne_tot[0] + f) + k2) -= fs[0](f) * dTf_qpk(k1, k2);
        if (ech && mat[o_p])
          for (n = 0; n < N[0]; n++) /* derivees en Tparoi (si Echange_contact) */
            (*mat[o_p])(N[0] * (!aux_only * ne_tot[0] + f) + n, !aux_only * ne_tot[o_p] + o_f) -= fs[0](f) * dTp_qpk(n);
      }
    else if (fcl[0](f, 0) > 5)
      for (n = 0; n < N[0]; n++) //Dirichlet : T_f^+ = T_b
        {
          secmem(!aux_only * ne_tot[0] + f, n) += (fcl[0](f, 0) == 6 ? ref_cast(Dirichlet, cls[0].get()[fcl[0](f, 1)].valeur()).val_imp(fcl[0](f, 2), n) : 0) - v_aux[0](f, n);
          if (mat[0])
            (*mat[0])(N[0] * (!aux_only * ne_tot[0] + f) + n, N[0] * (!aux_only * ne_tot[0] + f) + n)++;
        }
    else if (fcl[0](f, 0) == 3) //Echange_contact
      {
        const Echange_contact_PolyMAC_HFV& ech = ref_cast(Echange_contact_PolyMAC_HFV, cls[0].get()[fcl[0](f, 1)].valeur());
        int o_p = ech.o_idx, o_f = ech.f_dist(fcl[0](f, 2)), o_e = f_e[o_p](o_f, 0); //autre pb/face/elem
        if (corr[o_p] || N[o_p] != N[0]) /* correlation de l'autre cote */
          {
            const Pb_Multiphase& pbm = ref_cast(Pb_Multiphase, op_ext[o_p]->equation().probleme());
            const DoubleTab& alpha = pbm.equation_masse().inconnue().passe(), &dh = pbm.milieu().diametre_hydraulique_elem(),
                             &press = ref_cast(QDM_Multiphase, pbm.equation_qdm()).pression().passe(), &vit = pbm.equation_qdm().inconnue().passe(),
                              &lambda = pbm.milieu().conductivite().passe(), &mu = ref_cast(Fluide_base, pbm.milieu()).viscosite_dynamique().passe(), &rho = pbm.milieu().masse_volumique().passe(), &Cp =
                                                                                     pbm.milieu().capacite_calorifique().passe();
            DoubleTrav qpk(N[o_p]), dTf_qpk(N[o_p], N[o_p]), dTp_qpk(N[o_p]), qpi(N[o_p], N[o_p]), dTf_qpi(N[o_p], N[o_p], N[o_p]), dTp_qpi(N[o_p], N[o_p]), v(N[o_p], D), nv(N[o_p]);
            for (i = 0; i < e_f[o_p].get().dimension(1) && (fb = e_f[o_p](o_e, i)) >= 0; i++)
              for (prefac = fs[o_p](fb) * pf[o_p](fb) * (o_e == f_e[o_p](fb, 0) ? 1 : -1) / (pe[o_p](o_e) * ve[o_p](o_e)), n = 0; n < N[o_p]; n++)
                for (fac = prefac * vit(fb, n), d = 0; d < D; d++)
                  v(n, d) += fac * (xv[o_p](fb, d) - xp[o_p](o_e, d));
            for (n = 0; n < N[o_p]; n++)
              nv(n) = sqrt(domaine[0].get().dot(&v(n, 0), &v(n, 0)));
            //appel : on n'est implicite qu'en les temperatures
            Flux_parietal_base::input_t in;
            Flux_parietal_base::output_t out;
 
            in.N = N[o_p], in.f = o_f, in.D_h = dh(o_e), in.D_ch = dh(o_e), in.alpha = &alpha(o_e, 0), in.T = &v_aux[o_p](o_f, 0), in.p = press(e), in.v = nv.addr(), in.Tp = v_aux[0](f, 0), in.lambda =
                                                                                                                &lambda(o_e, 0), in.mu = &mu(o_e, 0), in.rho = &rho(o_e, 0), in.Cp = &Cp(o_e, 0);
            out.qpk = &qpk, out.dTf_qpk = &dTf_qpk, out.dTp_qpk = &dTp_qpk, out.qpi = &qpi, out.dTf_qpi = &dTf_qpi, out.dTp_qpi = &dTp_qpi, out.nonlinear = &j;
            corr[o_p]->qp(in, out);
            for (n = 0; n < N[o_p]; n++)
              secmem(!aux_only * ne_tot[0] + f, 0) -= fs[0](f) * qpk(n); //second membre
            if (mat[o_p])
              for (k1 = 0; k1 < N[o_p]; k1++)
                for (k2 = 0; k2 < N[o_p]; k2++) //derivees en Tfluide
                  (*mat[o_p])(!aux_only * ne_tot[0] + f, N[o_p] * (!aux_only * ne_tot[o_p] + o_f) + k2) += fs[0](f) * dTf_qpk(k1, k2);
            if (mat[0])
              for (n = 0; n < N[o_p]; n++) /* derivees en Tparoi */
                (*mat[0])(!aux_only * ne_tot[0] + f, !aux_only * ne_tot[0] + f) += fs[0](f) * dTp_qpk(n);
          }
        else if (ech.invh_paroi)
          for (n = 0; n < N[0]; n++)/* resistance de la paroi -> ajout du h(T'-T) */
            {
              secmem(!aux_only * ne_tot[0] + f, n) -= fs[0](f) / ech.invh_paroi * (v_aux[0](f, n) - v_aux[o_p](o_f, n)); //second membre
              if (mat[0])
                (*mat[0])(N[0] * (!aux_only * ne_tot[0] + f) + n, N[0] * (!aux_only * ne_tot[0] + f) + n) += fs[0](f) / ech.invh_paroi; //derivees
              if (mat[o_p])
                (*mat[o_p])(N[0] * (!aux_only * ne_tot[0] + f) + n, N[o_p] * (!aux_only * ne_tot[o_p] + o_f) + n) -= fs[0](f) / ech.invh_paroi;
            }
        else
          for (domaine[o_p].get().W2(&diffu[o_p].get(), o_e, w2), i = 0; i < w2.dimension(0); i++) /* pas de resistance -> ajout du flux de l'autre cote */
            if (e_f[o_p](o_e, i) == o_f)
              for (j = 0; j < w2.dimension(1); j++)
                for (n = 0; n < N[0]; n++)
                  if (w2(i, j, n))
                    {
                      secmem(!aux_only * ne_tot[0] + f, n) -= w2(i, j, n) * (v_aux[o_p * (j != i)](j != i ? e_f[o_p](o_e, j) : f, n) - inco[o_p](o_e, n)); //second membre
                      if (mat[o_p * (j != i)] && (j == i || fcl[o_p](o_f, 0) < 6)) //autre face: on substitue T_fb par T_f
                        (*mat[o_p * (j != i)])(N[0] * (!aux_only * ne_tot[0] + f) + n, N[0] * (!aux_only * ne_tot[o_p * (j != i)] + (j != i ? e_f[o_p](o_e, j) : f)) + n) += w2(i, j, n);
                      if (!aux_only && mat[o_p])
                        (*mat[o_p])(N[0] * (ne_tot[0] + f) + n, N[0] * o_e + n) -= w2(i, j, n); //autre element
                    }
      }
    else if (fcl[0](f, 0) == 4)
      for (n = 0; n < N[0]; n++) //Neumann
        secmem(!aux_only * ne_tot[0] + f, n) += fs[0](f) * ref_cast(Neumann, cls[0].get()[fcl[0](f, 1)].valeur()).flux_impose(fcl[0](f, 2), n);
    else if (fcl[0](f, 0) && fcl[0](f, 0) < 3)
      for (e = f_e[0](f, 0), n = 0; n < N[0]; n++) //Echange_global_impose
        {
          const Echange_impose_base& ech = ref_cast(Echange_impose_base, cls[0].get()[fcl[0](f, 1)].valeur());
          double h = ech.h_imp(fcl[0](f, 2), n), T = ech.T_ext(fcl[0](f, 2), n);
          secmem(!aux_only * ne_tot[0] + f, n) -= fs[0](f) * h * ((fcl[0](f, 0) == 1 ? v_aux[0](f, n) : inco[0](e, n)) - T);
          if (mat[0] && fcl[0](f, 0) == 1)
            (*mat[0])(N[0] * (!aux_only * ne_tot[0] + f) + n, N[0] * (!aux_only * ne_tot[0] + f) + n) += h * fs[0](f);
          if (mat[0] && fcl[0](f, 0) == 2 && !aux_only)
            (*mat[0])(N[0] * (ne_tot[0] + f) + n, N[0] * e + n) += h * fs[0](f);
        }
}