IBIceModel.cc

Go to the documentation of this file.

#include <iostream>
#include <limits>
#include <memory>
#include <string>
 
#include "pism/energy/BedThermalUnit.hh"
#include "pism/util/EnthalpyConverter.hh"
#include "pism/util/io/File.hh"
#include "pism/util/io/io_helpers.hh"
 
#include "pism/icebin/IBIceModel.hh"
#include "pism/icebin/IBSurfaceModel.hh"
#include "pism/coupler/ocean/Factory.hh"
#include "pism/energy/EnergyModel.hh"
 
namespace pism {
namespace icebin {
 
static double const NaN = std::numeric_limits<double>::quiet_NaN();
 
// ================================
 
IBIceModel::IBIceModel(std::shared_ptr<pism::Grid> grid, const std::shared_ptr<Context> &context,
                       IBIceModel::Params const &_params)
    : pism::IceModel(grid, context),
      params(_params),
      // FIXME: should `prefix` be empty below?
      base(grid, ""),
      cur(grid, ""),
      rate(grid, ""),
      ice_top_senth(grid, "ice_top_senth"),
      elevmask_ice(grid, "elevmask_ice"),
      elevmask_land(grid, "elevmask_land") {
 
  std::cout << "IBIceModel Conservation Formulas:" << std::endl;
  cur.print_formulas(std::cout);
}
IBIceModel::IBIceModel(std::shared_ptr<pism::Grid> grid, const std::shared_ptr<Context> &context, {…}
 
IBIceModel::~IBIceModel() {
  // empty
}
IBIceModel::~IBIceModel() {…}
 
 
void IBIceModel::allocate_subglacial_hydrology() {
  if (pism::IceModel::m_subglacial_hydrology) {
    // indicates it has already been allocated
    return;
  }
 
  m_subglacial_hydrology.reset(new pism::icebin::NullTransportHydrology(m_grid));
}
void IBIceModel::allocate_subglacial_hydrology() {…}
 
 
void IBIceModel::allocate_couplers() {
  super::allocate_couplers();
 
  m_log->message(2, "# Allocating the icebin surface model...\n");
  m_surface = std::make_shared<IBSurfaceModel>(m_grid);
  m_submodels["surface process model"] = m_surface.get();
}
void IBIceModel::allocate_couplers() {…}
 
void IBIceModel::massContPreHook() {
#if 0 // Avoid warnings until we put something in this method
 
    // Enthalpy and mass continuity are stepped with different timesteps.
    // Fish out the timestep relevant to US.
    const double my_t0 = m_grid.time->current();
    const double my_dt = this->dt;
#endif
}
void IBIceModel::massContPreHook() {…}
 
 
void IBIceModel::massContPostHook() {
#if 0 // Avoid warnings until we put something in this method
 
    // Enthalpy and mass continuity are stepped with different timesteps.
    // Fish out the timestep relevant to US.
    const double my_t0 = m_grid.time->current();
    const double my_dt = this->dt;
#endif
}
void IBIceModel::massContPostHook() {…}
 
 
void IBIceModel::energy_step() {
 
  printf("BEGIN IBIceModel::energyStep(t=%f, dt=%f)\n", t_TempAge, dt_TempAge);
 
  // Enthalpy and mass continuity are stepped with different timesteps.
  // Fish out the timestep relevant to US.
  // const double my_t0 = t_TempAge;          // Time at beginning of timestep
  const double my_dt = dt_TempAge;
 
  // =========== BEFORE Energy Step
 
  // =========== The Energy Step Itself
  super::energy_step();
 
  // =========== AFTER Energy Step
 
  // We need to integrate over strain_heating and geothermal_flux, which
  // are given in PISM as rates.
 
 
  // --------- Upward Geothermal Flux
  // Use actual geothermal flux, not the long-term average..
  // See: file:///Users/rpfische/git/pism/build/doc/browser/html/classPISMBedThermalUnit.html#details
  { cur.upward_geothermal_flux.add(my_dt, m_btu->flux_through_top_surface()); }
 
  // ----------- Geothermal Flux
  cur.geothermal_flux.add(my_dt, m_btu->flux_through_bottom_surface());
 
  // ---------- Basal Frictional Heating (see iMenthalpy.cc l. 220)
  array::Scalar const &Rb(m_stress_balance->basal_frictional_heating());
  cur.basal_frictional_heating.add(my_dt, Rb);
 
  // NOTE: strain_heating is inf at the coastlines.
  // See: https://github.com/pism/pism/issues/292
  // ------------ Volumetric Strain Heating
  // strain_heating_sum += my_dt * sum_columns(strainheating3p)
  const auto &strain_heating3 = m_stress_balance->volumetric_strain_heating();
 
  array::sum_columns(strain_heating3, 1.0, my_dt, cur.strain_heating);
}
void IBIceModel::energy_step() {…}
 
void IBIceModel::massContExplicitStep() {
 
  printf("BEGIN IBIceModel::MassContExplicitStep()\n");
 
  m_ice_density              = m_config->get_number("constants.ice.density");
  m_meter_per_s_to_kg_per_m2 = m_dt * m_ice_density;
 
 
  // =========== The Mass Continuity Step Itself
  // This will call through to accumulateFluxes_massContExplicitStep()
  // in the inner loop.  We must open access to variables we will use
  // in that subroutine.
  {
    array::AccessScope access{ &cur.pism_smb,           &cur.melt_grounded, &cur.melt_floating,
                               &cur.internal_advection, &cur.href_to_h,     &cur.nonneg_rule };
 
    // FIXME: update to use PISM's current mass transport code
    // super::massContExplicitStep();
  }
 
  // =========== AFTER the Mass Continuity Step
 
  // ----------- SMB: Pass inputs through to outputs.
  // They are needed to participate in mass/energy budget
  // This allows them to be used in the MassEnergyBudget computation.
  IBSurfaceModel *ib_surface = ib_surface_model();
 
  {
    array::AccessScope access{ &ib_surface->massxfer, &ib_surface->enthxfer, &ib_surface->deltah,
                               &cur.smb, &cur.deltah };
 
    for (auto p = m_grid->points(); p; p.next()) {
      const int i = p.i(), j = p.j();
 
      cur.smb.mass(i, j) += m_dt * ib_surface->massxfer(i, j);
      cur.smb.enth(i, j) += m_dt * ib_surface->enthxfer(i, j);
      cur.deltah(i, j) += m_dt * ib_surface->deltah(i, j);
    }
  }
}
void IBIceModel::massContExplicitStep() {…}
 
 
/** This is called IMMEDIATELY after ice is gained/lost in
iMgeometry.cc (massContExplicitStep()).  Here we can record the same
values that PISM saw when moving ice around. */
void IBIceModel::accumulateFluxes_massContExplicitStep(
    int i, int j,
    double surface_mass_balance, // [m s-1] ice equivalent
    double basal_melt_rate,      // [m s-1] ice equivalent
    double divQ_SIA,             // [m s-1] ice equivalent
    double divQ_SSA,             // [m s-1] ice equivalent
    double Href_to_H_flux,       // [m] ice equivalent
    double nonneg_rule_flux)     // [m] ice equivalent
{
  EnthalpyConverter::Ptr EC = ctx()->enthalpy_converter();
 
  const auto &ice_thickness = m_geometry.ice_thickness;
 
  const auto &ice_enthalpy = m_energy_model->enthalpy();
 
  // -------------- Melting
  double p_basal             = EC->pressure(ice_thickness(i, j));
  double T                   = EC->melting_temperature(p_basal);
  double specific_enth_basal = EC->enthalpy_permissive(T, 1.0, p_basal);
  double mass;
 
  // ------- Melting at base of ice sheet
  mass = -basal_melt_rate * m_meter_per_s_to_kg_per_m2;
  // TODO: Change this to just cur.melt_rate
  cur.melt_grounded.mass(i, j) += mass;
  cur.melt_grounded.enth(i, j) += mass * specific_enth_basal;
 
  // -------------- internal_advection
  const int ks             = m_grid->kBelowHeight(ice_thickness(i, j));
  const double *Enth       = ice_enthalpy.get_column(i, j);
  double specific_enth_top = Enth[ks]; // Approximate, we will use the enthalpy of the top layer...
 
  mass = -(divQ_SIA + divQ_SSA) * m_meter_per_s_to_kg_per_m2;
 
  cur.internal_advection.mass(i, j) += mass;
  cur.internal_advection.enth(i, j) += mass * specific_enth_top;
 
 
  // -------------- Get the easy variables out of the way...
  mass = surface_mass_balance * m_meter_per_s_to_kg_per_m2;
  cur.pism_smb.mass(i, j) += mass;
  cur.pism_smb.enth(i, j) += mass * specific_enth_top;
  cur.nonneg_rule(i, j) -= nonneg_rule_flux * m_ice_density;
  cur.href_to_h(i, j) += Href_to_H_flux * m_ice_density;
}
void IBIceModel::accumulateFluxes_massContExplicitStep( {…}
 
/** Differences and divides by accumulated time over coupling timestep.
Eg, to convert [kg m-2] --> [kg m-2 s-1]
@param t0 Time of last time we coupled. */
void IBIceModel::set_rate(double dt) {
 
  if (dt == 0)
    throw RuntimeError(PISM_ERROR_LOCATION, "Coupling timestep has size dt=0");
 
  double by_dt = 1.0 / dt;
  printf("IBIceModel::set_rate(dt=%f)\n", dt);
 
  compute_enth2(cur.total.enth, cur.total.mass);
  cur.set_epsilon();
 
  // Compute differences, and set base = cur
  auto base_ii(base.all_vecs.begin());
  auto cur_ii(cur.all_vecs.begin());
  auto rate_ii(rate.all_vecs.begin());
  for (; base_ii != base.all_vecs.end(); ++base_ii, ++cur_ii, ++rate_ii) {
    array::Scalar &vbase(base_ii->vec);
    array::Scalar &vcur(cur_ii->vec);
    array::Scalar &vrate(rate_ii->vec);
 
    {
      array::AccessScope access{ &vbase, &vcur, &vrate };
      for (auto p = m_grid->points(); p; p.next()) {
        const int i = p.i(), j = p.j();
 
        // rate = cur - base: Just for DELTA and EPSILON flagged vectors
        if (base_ii->flags & (MassEnergyBudget::DELTA | MassEnergyBudget::EPSILON)) {
          vrate(i, j) = (vcur(i, j) - vbase(i, j)) * by_dt;
        } else {
          // Or else just copy the to "rate"
          vrate(i, j) = vcur(i, j);
        }
      }
    }
  }
}
void IBIceModel::set_rate(double dt) {…}
 
void IBIceModel::reset_rate() {
  // Compute differences, and set base = cur
  auto base_ii(base.all_vecs.begin());
  auto cur_ii(cur.all_vecs.begin());
  for (; base_ii != base.all_vecs.end(); ++base_ii, ++cur_ii) {
    array::Scalar &vbase(base_ii->vec);
    array::Scalar &vcur(cur_ii->vec);
 
    // This cannot go in the loop above with PETSc because
    // vbase is needed on the RHS of the equations above.
    array::AccessScope access{ &vbase, &vcur };
    for (auto p = m_grid->points(); p; p.next()) {
      const int i = p.i(), j = p.j();
      // base = cur: For ALL vectors
      vbase(i, j) = vcur(i, j);
    }
  }
}
void IBIceModel::reset_rate() {…}
 
void IBIceModel::prepare_outputs(double time_s) {
  (void)time_s;
 
  EnthalpyConverter::Ptr EC = ctx()->enthalpy_converter();
 
  // --------- ice_surface_enth from m_ice_enthalpy
  const auto &ice_surface_elevation = m_geometry.ice_surface_elevation;
  const auto &cell_type = m_geometry.cell_type;
  const auto &ice_enthalpy = m_energy_model->enthalpy();
  const auto &ice_thickness         = m_geometry.ice_thickness;
 
  array::AccessScope access{ &ice_enthalpy,          &ice_thickness, // INPUTS
                             &ice_surface_elevation, &cell_type,     &ice_top_senth,
                             &elevmask_ice,          &elevmask_land }; // OUTPUT
  for (int i = m_grid->xs(); i < m_grid->xs() + m_grid->xm(); ++i) {
    for (int j = m_grid->ys(); j < m_grid->ys() + m_grid->ym(); ++j) {
      double const *Enth = ice_enthalpy.get_column(i, j);
 
      // Top Layer
      auto ks             = m_grid->kBelowHeight(ice_thickness(i, j));
      double senth        = Enth[ks]; // [J kg-1]
      ice_top_senth(i, j) = senth;
 
      // elevmask_ice and elevmask_land: Used by IceBin for elevation and masking
      switch ((int)cell_type(i, j)) {
      case MASK_GROUNDED:
      case MASK_FLOATING:
        elevmask_ice(i, j)  = ice_surface_elevation(i, j);
        elevmask_land(i, j) = ice_surface_elevation(i, j);
        break;
      case MASK_ICE_FREE_BEDROCK:
        elevmask_ice(i, j)  = NaN;
        elevmask_land(i, j) = ice_surface_elevation(i, j);
        break;
      case MASK_ICE_FREE_OCEAN:
      case MASK_UNKNOWN:
        elevmask_ice(i, j)  = NaN;
        elevmask_land(i, j) = NaN;
        break;
      }
    }
  }
 
  // ====================== Write to the post_energy.nc file (OPTIONAL)
}
void IBIceModel::prepare_outputs(double time_s) {…}
 
void IBIceModel::dumpToFile(const std::string &filename) const {
  File file(m_grid->com, filename,
            string_to_backend(m_config->get_string("output.format")), io::PISM_READWRITE_MOVE);
 
  write_metadata(file, WRITE_MAPPING, PREPEND_HISTORY);
  write_run_stats(file, run_stats());
 
  // assume that "dumpToFile" is expected to save the model state *only*.
  save_variables(file, INCLUDE_MODEL_STATE, {}, m_time->current());
}
void IBIceModel::dumpToFile(const std::string &filename) const  {…}
 
void IBIceModel::time_setup() {
  // super::m_grid_setup() trashes m_time->start().  Now set it correctly.
  m_time->set_start(params.time_start_s);
  m_time->set(params.time_start_s);
 
  m_log->message(2, "* Run time: [%s, %s]  (%s years, using the '%s' calendar)\n",
                 m_time->date(m_time->start()).c_str(), m_time->date(m_time->end()).c_str(),
                 m_time->run_length().c_str(), m_time->calendar().c_str());
}
void IBIceModel::time_setup() {…}
 
void IBIceModel::misc_setup() {
  super::misc_setup();
 
 
  // ------ Initialize MassEnth structures: base, cur, rate
  for (auto &ii : cur.all_vecs) {
    ii.vec.set(0);
  }
  compute_enth2(cur.total.enth, cur.total.mass);
  cur.set_epsilon();
 
  // base = cur
  auto base_ii(base.all_vecs.begin());
  auto cur_ii(cur.all_vecs.begin());
  for (; base_ii != base.all_vecs.end(); ++base_ii, ++cur_ii) {
    base_ii->vec.copy_from(cur_ii->vec);
  }
}
void IBIceModel::misc_setup() {…}
 
/** Sums over columns to compute enthalpy on 2D m_grid.
This is used to track conservation of energy.
 
NOTE: Unfortunately so far PISM does not keep track of enthalpy in
"partially-filled" cells, so Enth2(i,j) is not valid at locations like
this one. We need to address this, but so far, it seems to me, the
best thing we can do is estimate Enth2(i,j) at partially-filled cells
by computing the average over icy neighbors. I think you can re-use
the idea from IceModel::get_threshold_thickness(...) (iMpartm_grid->cc).  */
 
void IBIceModel::compute_enth2(pism::array::Scalar &enth2, pism::array::Scalar &mass2) {
  //   getInternalColumn() is allocated already
  double ice_density = m_config->get_number("constants.ice.density", "kg m-3");
 
  const auto &ice_enthalpy = m_energy_model->enthalpy();
  const auto &ice_thickness = m_geometry.ice_thickness;
 
 
  array::AccessScope access{ &ice_thickness, &ice_enthalpy, // Inputs
                             &enth2, &mass2 };              // Outputs
  for (auto p = m_grid->points(); p; p.next()) {
    const int i = p.i(), j = p.j();
 
    enth2(i, j) = 0;
    mass2(i, j) = 0;
 
    // count all ice, including cells that have so little they
    // are considered "ice-free"
    if (ice_thickness(i, j) > 0) {
      int ks = (int)m_grid->kBelowHeight(ice_thickness(i, j));
      const auto *Enth = ice_enthalpy.get_column(i, j);
 
      for (int k = 0; k < ks; ++k) {
        double dz = (m_grid->z(k + 1) - m_grid->z(k));
        enth2(i, j) += Enth[k] * dz; // [m J kg-1]
      }
 
      // Last layer is (potentially) partial
      double dz = (ice_thickness(i, j) - m_grid->z(ks));
      enth2(i, j) += Enth[ks] * dz; // [m J kg-1]
 
      // Finish off after all layers processed
      enth2(i, j) *= ice_density;                      // --> [J m-2]
      mass2(i, j) = ice_thickness(i, j) * ice_density; // --> [kg m-2]
    }
  }
}
void IBIceModel::compute_enth2(pism::array::Scalar &enth2, pism::array::Scalar &mass2) {…}
 
 
/** Merges surface temperature derived from m_ice_enthalpy into any NaN values
in the vector provided.
@param deltah IN: Input from Icebin (change in enthalpy of each m_grid
    cell over the timestep) [W m-2].
@param default_val: The value that deltah(i,j) will have if no value
    is listed for that m_grid cell
@param timestep_s: Length of the current coupling timestep [s]
@param surface_temp OUT: Resulting surface temperature to use as the Dirichlet B.C.
*/
void IBIceModel::construct_surface_temp(
    pism::array::Scalar &deltah, // IN: Input from Icebin
    double default_val,
    double timestep_s,                 // Length of this coupling interval [s]
    pism::array::Scalar &surface_temp) // OUT: Temperature @ top of ice sheet (to use for Dirichlet B.C.)
 
{
  printf("BEGIN IBIceModel::merge_surface_temp default_val=%g\n", default_val);
  EnthalpyConverter::Ptr EC = ctx()->enthalpy_converter();
 
  double ice_density = m_config->get_number("constants.ice.density");
  const auto &ice_enthalpy = m_energy_model->enthalpy();
  const auto &ice_thickness = m_geometry.ice_thickness;
 
  {
    array::AccessScope access{ &ice_enthalpy, &deltah, &ice_thickness, &surface_temp };
 
    // First time around, set effective_surface_temp to top temperature
    for (int i = m_grid->xs(); i < m_grid->xs() + m_grid->xm(); ++i) {
      for (int j = m_grid->ys(); j < m_grid->ys() + m_grid->ym(); ++j) {
        double &surface_temp_ij(surface_temp(i, j));
        double const &deltah_ij(deltah(i, j));
 
        const auto *Enth = ice_enthalpy.get_column(i, j);
 
        // Enthalpy at top of ice sheet
        const int ks      = m_grid->kBelowHeight(ice_thickness(i, j));
        double spec_enth3 = Enth[ks]; // Specific enthalpy [J kg-1]
 
        if (deltah_ij != default_val) {
          // Adjust enthalpy @top by deltah
          double toplayer_dz = ice_thickness(i, j) - m_grid->z(ks); // [m]
 
          // [J kg-1] = [J kg-1]
          //     + [J m-2 s-1] * [m^2 m-3] * [m^3 kg-1] * [s]
          spec_enth3 = spec_enth3 + deltah_ij / (toplayer_dz * ice_density) * timestep_s;
        }
 
 
        // Convert specific enthalpy value to surface temperature
        const double p  = 0.0;                            // Pressure at top of ice sheet
        surface_temp_ij = EC->temperature(spec_enth3, p); // [K]
      }
    }
  }
 
  printf("END IBIceModel::merge_surface_temp\n");
}
void IBIceModel::construct_surface_temp( {…}
} // namespace icebin
namespace icebin {…}
} // namespace pism