Line data    Source code

       1           0 : // Distributed under the MIT License.
       2             : // See LICENSE.txt for details.
       3             : 
       4             : #pragma once
       5             : 
       6             : #include <boost/preprocessor/arithmetic/dec.hpp>
       7             : #include <boost/preprocessor/arithmetic/inc.hpp>
       8             : #include <boost/preprocessor/control/expr_iif.hpp>
       9             : #include <boost/preprocessor/list/adt.hpp>
      10             : #include <boost/preprocessor/repetition/for.hpp>
      11             : #include <boost/preprocessor/repetition/repeat.hpp>
      12             : #include <boost/preprocessor/tuple/to_list.hpp>
      13             : #include <limits>
      14             : #include <pup.h>
      15             : 
      16             : #include "DataStructures/Tensor/TypeAliases.hpp"
      17             : #include "Options/String.hpp"
      18             : #include "PointwiseFunctions/Hydro/EquationsOfState/EquationOfState.hpp"
      19             : #include "PointwiseFunctions/Hydro/Units.hpp"
      20             : #include "Utilities/Serialization/CharmPupable.hpp"
      21             : #include "Utilities/TMPL.hpp"
      22             : 
      23             : /// \cond
      24             : class DataVector;
      25             : /// \endcond
      26             : 
      27             : namespace EquationsOfState {
      28             : /*!
      29             :  * \ingroup EquationsOfStateGroup
      30             :  * \brief Equation of state for a piecewise polytropic fluid
      31             :  *
      32             :  * A piecewise polytropic equation of state \f$p=K_i\rho^{\Gamma_i}\f$ where
      33             :  *  \f$K_i\f$ is the polytropic constant and \f$\Gamma_i\f$ is the polytropic
      34             :  * exponent. Here the subscript \f$i\f$ indicates two pairs of constants and
      35             :  *  exponents which characterize `the stiffness' of the matter at low and high
      36             :  *  densities.  For a given density, the polytropic exponent is related to the
      37             :  *  polytropic index \f$N_p\f$ by \f$N_p=1/(\Gamma-1)\f$.  For posterity,
      38             :  *  this two piece polytrope has been used in toy models of CCSNe (e.g.,
      39             :  *  \cite Dimmelmeier2001 ) and could be extended to a general "M" number of
      40             :  * parts for simplified equations of state for neutron stars (e.g.,
      41             :  *  \cite OBoyle2020 ). For a reference to a general piecewise polytrope, see
      42             :  * Section 2.4.7 of \cite RezzollaBook.
      43             :  */
      44             : template <bool IsRelativistic>
      45           1 : class PiecewisePolytropicFluid : public EquationOfState<IsRelativistic, 1> {
      46             :  public:
      47           0 :   static constexpr size_t thermodynamic_dim = 1;
      48           0 :   static constexpr bool is_relativistic = IsRelativistic;
      49             : 
      50             :   /// The density demarcating the high and low density descriptions of the
      51             :   /// fluid.
      52           1 :   struct PiecewisePolytropicTransitionDensity {
      53           0 :     using type = double;
      54           0 :     static constexpr Options::String help = {
      55             :         "Density below (above) which, the matter is described by a low (high) "
      56             :         "density polytropic fluid."};
      57           0 :     static double lower_bound() { return 0.0; }
      58             :   };
      59             : 
      60             :   /// The constant \f$K\f$ scaling the low density material
      61             :   /// \f$p=K\rho^{\Gamma}\f$.
      62             :   ///
      63             :   /// Note, by enforcing pressure continuity at the transition density
      64             :   /// \f$\bar{\rho}\f$, the high density constant \f$K_{high}\f$ is given
      65             :   /// as \f$K_{high} = K_{low} (\bar{\rho})^{\Gamma_{low} - \Gamma_{high}}\f$.
      66           1 :   struct PolytropicConstantLow {
      67           0 :     using type = double;
      68           0 :     static constexpr Options::String help = {
      69             :         "Polytropic constant K for lower"
      70             :         " density material"};
      71           0 :     static double lower_bound() { return 0.0; }
      72             :   };
      73             : 
      74             :   /// The exponent \f$\Gamma\f$, scaling the low density material
      75             :   /// \f$p=K\rho^{\Gamma}\f$.
      76           1 :   struct PolytropicExponentLow {
      77           0 :     using type = double;
      78           0 :     static constexpr Options::String help = {
      79             :         "Polytropic exponent for lower"
      80             :         " density material."};
      81           0 :     static double lower_bound() { return 1.0; }
      82             :   };
      83             : 
      84             :   /// The exponent \f$\Gamma\f$, scaling the high density material
      85             :   /// \f$p=K\rho^{\Gamma}\f$.
      86           1 :   struct PolytropicExponentHigh {
      87           0 :     using type = double;
      88           0 :     static constexpr Options::String help = {
      89             :         "Polytropic exponent for higher"
      90             :         " density material."};
      91           0 :     static double lower_bound() { return 1.0; }
      92             :   };
      93             : 
      94           0 :   static constexpr Options::String help = {
      95             :       "A piecewise polytropic fluid equation of state.\n"
      96             :       "The pressure is related to the rest mass density by p = K_i rho ^ "
      97             :       "Gamma_i, "
      98             :       "where p is the pressure, rho is the rest mass density, K_i is the "
      99             :       "polytropic constant either describing the low or high density material, "
     100             :       "and Gamma_i is the polytropic exponent for the low or high density "
     101             :       "material. The polytropic index N_i is defined as Gamma_i = 1 + 1 / N_i."
     102             :       "  The subscript `i' refers to different pairs of Gamma and K that can"
     103             :       " describe either low or high density material."};
     104             : 
     105           0 :   using options =
     106             :       tmpl::list<PiecewisePolytropicTransitionDensity, PolytropicConstantLow,
     107             :                  PolytropicExponentLow, PolytropicExponentHigh>;
     108             : 
     109           0 :   PiecewisePolytropicFluid() = default;
     110           0 :   PiecewisePolytropicFluid(const PiecewisePolytropicFluid&) = default;
     111           0 :   PiecewisePolytropicFluid& operator=(const PiecewisePolytropicFluid&) =
     112             :       default;
     113           0 :   PiecewisePolytropicFluid(PiecewisePolytropicFluid&&) = default;
     114           0 :   PiecewisePolytropicFluid& operator=(PiecewisePolytropicFluid&&) = default;
     115           0 :   ~PiecewisePolytropicFluid() override = default;
     116             : 
     117           0 :   PiecewisePolytropicFluid(double transition_density,
     118             :                            double polytropic_constant_lo,
     119             :                            double polytropic_exponent_lo,
     120             :                            double polytropic_exponent_hi);
     121             : 
     122           0 :   std::unique_ptr<EquationOfState<IsRelativistic, 1>> get_clone()
     123             :       const override;
     124             : 
     125           1 :   std::unique_ptr<EquationOfState<IsRelativistic, 3>> promote_to_3d_eos()
     126             :       const override;
     127             : 
     128           1 :   std::unique_ptr<EquationOfState<IsRelativistic, 2>> promote_to_2d_eos()
     129             :       const override;
     130             : 
     131           0 :   bool is_equal(const EquationOfState<IsRelativistic, 1>& rhs) const override;
     132             : 
     133           0 :   bool operator==(const PiecewisePolytropicFluid<IsRelativistic>& rhs) const;
     134             : 
     135           0 :   bool operator!=(const PiecewisePolytropicFluid<IsRelativistic>& rhs) const;
     136             : 
     137             :   EQUATION_OF_STATE_FORWARD_DECLARE_MEMBERS(PiecewisePolytropicFluid, 1)
     138             : 
     139           0 :   WRAPPED_PUPable_decl_base_template(  // NOLINT
     140             :       SINGLE_ARG(EquationOfState<IsRelativistic, 1>), PiecewisePolytropicFluid);
     141             : 
     142             :   /// The lower bound of the rest mass density that is valid for this EOS
     143           1 :   double rest_mass_density_lower_bound() const override { return 0.0; }
     144             : 
     145             :   /// The upper bound of the rest mass density that is valid for this EOS
     146           1 :   double rest_mass_density_upper_bound() const override;
     147             : 
     148             :   /// The lower bound of the specific enthalpy that is valid for this EOS
     149           1 :   double specific_enthalpy_lower_bound() const override {
     150             :     return IsRelativistic ? 1.0 : 0.0;
     151             :   }
     152             : 
     153             :   /// The lower bound of the specific internal energy that is valid for this EOS
     154           1 :   double specific_internal_energy_lower_bound() const override { return 0.0; }
     155             : 
     156             :   /// The upper bound of the specific internal energy that is valid for this EOS
     157           1 :   double specific_internal_energy_upper_bound() const override;
     158             : 
     159             :   /// The vacuum baryon mass for this EoS
     160           1 :   double baryon_mass() const override {
     161             :     return hydro::units::geometric::default_baryon_mass;
     162             :   }
     163             : 
     164             :  private:
     165             :   EQUATION_OF_STATE_FORWARD_DECLARE_MEMBER_IMPLS(1)
     166             : 
     167           0 :   double transition_density_ = std::numeric_limits<double>::signaling_NaN();
     168           0 :   double transition_pressure_ = std::numeric_limits<double>::signaling_NaN();
     169           0 :   double transition_spec_eint_ = std::numeric_limits<double>::signaling_NaN();
     170           0 :   double polytropic_constant_lo_ = std::numeric_limits<double>::signaling_NaN();
     171           0 :   double polytropic_exponent_lo_ = std::numeric_limits<double>::signaling_NaN();
     172           0 :   double polytropic_constant_hi_ = std::numeric_limits<double>::signaling_NaN();
     173           0 :   double polytropic_exponent_hi_ = std::numeric_limits<double>::signaling_NaN();
     174             : };
     175             : 
     176             : /// \cond
     177             : template <bool IsRelativistic>
     178             : PUP::able::PUP_ID
     179             :     EquationsOfState::PiecewisePolytropicFluid<IsRelativistic>::my_PUP_ID = 0;
     180             : /// \endcond
     181             : }  // namespace EquationsOfState