Lorene::Eos Class Reference
[Equations of state]

Equation of state base class. More...

#include <eos.h>

Inheritance diagram for Lorene::Eos:
Lorene::Eos_Fermi Lorene::Eos_fitting Lorene::Eos_incomp Lorene::Eos_mag Lorene::Eos_multi_poly Lorene::Eos_poly Lorene::Eos_strange Lorene::Eos_strange_cr Lorene::Eos_tabul Lorene::MEos

List of all members.

Public Member Functions

virtual ~Eos ()
 Destructor.
const char * get_name () const
 Returns the EOS name.
void set_name (const char *name_i)
 Sets the EOS name.
virtual bool operator== (const Eos &) const =0
 Comparison operator (egality).
virtual bool operator!= (const Eos &) const =0
 Comparison operator (difference).
virtual int identify () const =0
 Returns a number to identify the sub-classe of Eos the object belongs to.
virtual void sauve (FILE *) const
 Save in a file.
virtual double nbar_ent_p (double ent, const Param *par=0x0) const =0
 Computes the baryon density from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).
Cmp nbar_ent (const Cmp &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the baryon density field from the log-enthalpy field and extra parameters.
Scalar nbar_ent (const Scalar &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the baryon density field from the log-enthalpy field and extra parameters.
virtual double ener_ent_p (double ent, const Param *par=0x0) const =0
 Computes the total energy density from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).
Cmp ener_ent (const Cmp &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the total energy density from the log-enthalpy and extra parameters.
Scalar ener_ent (const Scalar &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the total energy density from the log-enthalpy and extra parameters.
virtual double press_ent_p (double ent, const Param *par=0x0) const =0
 Computes the pressure from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).
Cmp press_ent (const Cmp &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the pressure from the log-enthalpy and extra parameters.
Scalar press_ent (const Scalar &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the pressure from the log-enthalpy and extra parameters.
virtual double der_nbar_ent_p (double ent, const Param *par=0x0) const =0
 Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).
Cmp der_nbar_ent (const Cmp &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy and extra parameters.
Scalar der_nbar_ent (const Scalar &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy and extra parameters.
virtual double der_ener_ent_p (double ent, const Param *par=0x0) const =0
 Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy with extra parameters (virtual function implemented in the derived classes).
Cmp der_ener_ent (const Cmp &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy and extra parameters.
Scalar der_ener_ent (const Scalar &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy and extra parameters.
virtual double der_press_ent_p (double ent, const Param *par=0x0) const =0
 Computes the logarithmic derivative $d\ln p/d\ln H$ from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).
Cmp der_press_ent (const Cmp &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the logarithmic derivative $d\ln p/d\ln H$ from the log-enthalpy and extra parameters.
Scalar der_press_ent (const Scalar &ent, int nzet, int l_min=0, Param *par=0x0) const
 Computes the logarithmic derivative $d\ln p/d\ln H$ from the log-enthalpy and extra parameters.

Static Public Member Functions

static Eoseos_from_file (FILE *)
 Construction of an EOS from a binary file.
static Eoseos_from_file (ifstream &)
 Construction of an EOS from a formatted file.

Protected Member Functions

 Eos ()
 Standard constructor.
 Eos (const char *name_i)
 Standard constructor with name.
 Eos (const Eos &)
 Copy constructor.
 Eos (FILE *)
 Constructor from a binary file (created by the function sauve(FILE*) ).
 Eos (ifstream &)
 Constructor from a formatted file.
virtual ostream & operator>> (ostream &) const =0
 Operator >>.
void calcule (const Cmp &thermo, int nzet, int l_min, double(Eos::*fait)(double, const Param *) const, Param *par, Cmp &resu) const
 General computational method for Cmp 's.
void calcule (const Scalar &thermo, int nzet, int l_min, double(Eos::*fait)(double, const Param *) const, Param *par, Scalar &resu) const
 General computational method for Scalar 's.

Protected Attributes

char name [100]
 EOS name.

Friends

ostream & operator<< (ostream &, const Eos &)
 Display.

Detailed Description

Equation of state base class.

()

Definition at line 193 of file eos.h.


Constructor & Destructor Documentation

Lorene::Eos::Eos (  )  [protected]

Standard constructor.

Definition at line 115 of file eos.C.

References set_name().

Lorene::Eos::Eos ( const char *  name_i  )  [explicit, protected]

Standard constructor with name.

Definition at line 123 of file eos.C.

References set_name().

Lorene::Eos::Eos ( const Eos eos_i  )  [protected]

Copy constructor.

Definition at line 131 of file eos.C.

References name, and set_name().

Lorene::Eos::Eos ( FILE *  fich  )  [protected]

Constructor from a binary file (created by the function sauve(FILE*) ).

This constructor is protected because any EOS construction from a binary file must be done via the function Eos::eos_from_file(FILE*) .

Definition at line 139 of file eos.C.

References name.

Lorene::Eos::Eos ( ifstream &  fich  )  [protected]

Constructor from a formatted file.

This constructor is protected because any EOS construction from a formatted file must be done via the function Eos::eos_from_file(ifstream&) .

Definition at line 147 of file eos.C.

References name.

Lorene::Eos::~Eos (  )  [virtual]

Destructor.

Definition at line 159 of file eos.C.


Member Function Documentation

void Lorene::Eos::calcule ( const Scalar thermo,
int  nzet,
int  l_min,
double(Eos::*)(double, const Param *) const   fait,
Param par,
Scalar resu 
) const [protected]

General computational method for Scalar 's.

Parameters:
thermo [input] thermodynamical quantity (for instance the enthalpy field)from which the thermodynamical quantity resu is to be computed.
nzet [input] number of domains where resu is to be computed.
l_min [input] index of the innermost domain is which resu is to be computed [default value: 0]; resu is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
fait [input] pointer on the member function of class Eos which performs the pointwise calculation.
par possible extra parameters of the EOS
resu [output] result of the computation.

Definition at line 282 of file eos.C.

References Lorene::Param::add_int_mod(), Lorene::Scalar::annule(), Lorene::Valeur::c, Lorene::Valeur::coef_i(), Lorene::Tbl::get_etat(), Lorene::Scalar::get_etat(), Lorene::Tensor::get_mp(), Lorene::Mg3d::get_nzone(), Lorene::Scalar::get_spectral_va(), Lorene::Tbl::get_taille(), Lorene::Valeur::set_etat_c_qcq(), Lorene::Tbl::set_etat_qcq(), Lorene::Mtbl::set_etat_qcq(), Lorene::Scalar::set_etat_qcq(), Lorene::Tbl::set_etat_zero(), Lorene::Scalar::set_etat_zero(), Lorene::Scalar::set_spectral_va(), Lorene::Tbl::t, and Lorene::Mtbl::t.

void Lorene::Eos::calcule ( const Cmp thermo,
int  nzet,
int  l_min,
double(Eos::*)(double, const Param *) const   fait,
Param par,
Cmp resu 
) const [protected]

General computational method for Cmp 's.

Parameters:
thermo [input] thermodynamical quantity (for instance the enthalpy field)from which the thermodynamical quantity resu is to be computed.
nzet [input] number of domains where resu is to be computed.
l_min [input] index of the innermost domain is which resu is to be computed [default value: 0]; resu is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
fait [input] pointer on the member function of class Eos which performs the pointwise calculation.
par possible extra parameters of the EOS
resu [output] result of the computation.

Definition at line 210 of file eos.C.

References Lorene::Param::add_int_mod(), Lorene::Cmp::annule(), Lorene::Valeur::c, Lorene::Valeur::coef_i(), Lorene::Tbl::get_etat(), Lorene::Cmp::get_etat(), Lorene::Cmp::get_mp(), Lorene::Mg3d::get_nzone(), Lorene::Tbl::get_taille(), Lorene::Valeur::set_etat_c_qcq(), Lorene::Tbl::set_etat_qcq(), Lorene::Mtbl::set_etat_qcq(), Lorene::Cmp::set_etat_qcq(), Lorene::Tbl::set_etat_zero(), Lorene::Cmp::set_etat_zero(), Lorene::Tbl::t, Lorene::Mtbl::t, and Lorene::Cmp::va.

Scalar Lorene::Eos::der_ener_ent ( const Scalar ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the derivative dln(e)/dln(H) is to be computed.
l_min index of the innermost domain is which the coefficient dln(n)/dln(H) is to be computed [default value: 0]; the derivative dln(e)/dln(H) is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
dln(e)/dln(H)

Definition at line 461 of file eos.C.

References calcule(), der_ener_ent_p(), and Lorene::Tensor::get_mp().

Cmp Lorene::Eos::der_ener_ent ( const Cmp ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the derivative dln(e)/dln(H) is to be computed.
l_min index of the innermost domain is which the coefficient dln(n)/dln(H) is to be computed [default value: 0]; the derivative dln(e)/dln(H) is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
dln(e)/dln(H)

Definition at line 451 of file eos.C.

References calcule(), der_ener_ent_p(), and Lorene::Cmp::get_mp().

virtual double Lorene::Eos::der_ener_ent_p ( double  ent,
const Param par = 0x0 
) const [pure virtual]

Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy with extra parameters (virtual function implemented in the derived classes).

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
par possible extra parameters of the EOS
Returns:
dln(e)/dln(H)

Implemented in Lorene::Eos_poly, Lorene::Eos_poly_newt, Lorene::Eos_incomp, Lorene::Eos_incomp_newt, Lorene::Eos_strange, Lorene::Eos_strange_cr, Lorene::Eos_Fermi, Lorene::MEos, Lorene::Eos_fitting, Lorene::Eos_mag, Lorene::Eos_multi_poly, and Lorene::Eos_tabul.

Scalar Lorene::Eos::der_nbar_ent ( const Scalar ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the derivative dln(n)/dln(H) is to be computed.
l_min index of the innermost domain is which the coefficient dln(n)/dln(H) is to be computed [default value: 0]; the derivative dln(n)/dln(H) is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
dln(n)/dln(H)

Definition at line 438 of file eos.C.

References calcule(), der_nbar_ent_p(), and Lorene::Tensor::get_mp().

Cmp Lorene::Eos::der_nbar_ent ( const Cmp ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the derivative dln(n)/dln(H) is to be computed.
l_min index of the innermost domain is which the coefficient dln(n)/dln(H) is to be computed [default value: 0]; the derivative dln(n)/dln(H) is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
dln(n)/dln(H)

Definition at line 428 of file eos.C.

References calcule(), der_nbar_ent_p(), and Lorene::Cmp::get_mp().

virtual double Lorene::Eos::der_nbar_ent_p ( double  ent,
const Param par = 0x0 
) const [pure virtual]

Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
par possible extra parameters of the EOS
Returns:
dln(n)/dln(H)

Implemented in Lorene::Eos_poly, Lorene::Eos_poly_newt, Lorene::Eos_incomp, Lorene::Eos_incomp_newt, Lorene::Eos_strange, Lorene::Eos_strange_cr, Lorene::Eos_Fermi, Lorene::MEos, Lorene::Eos_fitting, Lorene::Eos_mag, Lorene::Eos_multi_poly, and Lorene::Eos_tabul.

Scalar Lorene::Eos::der_press_ent ( const Scalar ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the logarithmic derivative $d\ln p/d\ln H$ from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the derivative dln(p)/dln(H) is to be computed.
par possible extra parameters of the EOS
l_min index of the innermost domain is which the coefficient dln(n)/dln(H) is to be computed [default value: 0]; the derivative dln(p)/dln(H) is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
Returns:
dln(p)/dln(H)

Definition at line 483 of file eos.C.

References calcule(), der_press_ent_p(), and Lorene::Tensor::get_mp().

Cmp Lorene::Eos::der_press_ent ( const Cmp ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the logarithmic derivative $d\ln p/d\ln H$ from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the derivative dln(p)/dln(H) is to be computed.
par possible extra parameters of the EOS
l_min index of the innermost domain is which the coefficient dln(n)/dln(H) is to be computed [default value: 0]; the derivative dln(p)/dln(H) is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
Returns:
dln(p)/dln(H)

Definition at line 473 of file eos.C.

References calcule(), der_press_ent_p(), and Lorene::Cmp::get_mp().

virtual double Lorene::Eos::der_press_ent_p ( double  ent,
const Param par = 0x0 
) const [pure virtual]

Computes the logarithmic derivative $d\ln p/d\ln H$ from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
par possible extra parameters of the EOS
Returns:
dln(p)/dln(H)

Implemented in Lorene::Eos_poly, Lorene::Eos_poly_newt, Lorene::Eos_incomp, Lorene::Eos_incomp_newt, Lorene::Eos_strange, Lorene::Eos_strange_cr, Lorene::Eos_Fermi, Lorene::MEos, Lorene::Eos_fitting, Lorene::Eos_mag, Lorene::Eos_multi_poly, and Lorene::Eos_tabul.

Scalar Lorene::Eos::ener_ent ( const Scalar ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the total energy density from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the energy density is to be computed.
l_min index of the innermost domain is which the energy density is to be computed [default value: 0]; the energy density is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
energy density [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Definition at line 394 of file eos.C.

References calcule(), ener_ent_p(), and Lorene::Tensor::get_mp().

Cmp Lorene::Eos::ener_ent ( const Cmp ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the total energy density from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the energy density is to be computed.
l_min index of the innermost domain is which the energy density is to be computed [default value: 0]; the energy density is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
energy density [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Definition at line 384 of file eos.C.

References calcule(), ener_ent_p(), and Lorene::Cmp::get_mp().

virtual double Lorene::Eos::ener_ent_p ( double  ent,
const Param par = 0x0 
) const [pure virtual]

Computes the total energy density from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
par possible extra parameters of the EOS
Returns:
energy density e [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Implemented in Lorene::Eos_poly, Lorene::Eos_poly_newt, Lorene::Eos_incomp, Lorene::Eos_incomp_newt, Lorene::Eos_strange, Lorene::Eos_strange_cr, Lorene::Eos_Fermi, Lorene::MEos, Lorene::Eos_consistent, Lorene::Eos_fitting, Lorene::Eos_mag, Lorene::Eos_multi_poly, and Lorene::Eos_tabul.

Eos * Lorene::Eos::eos_from_file ( ifstream &  fich  )  [static]

Construction of an EOS from a formatted file.

The fist line of the file must start by the EOS number, according to the following conventions:

  • 1 = relativistic polytropic EOS (class Eos_poly ).
  • 2 = Newtonian polytropic EOS (class Eos_poly_newt ).
  • 3 = Relativistic incompressible EOS (class Eos_incomp ).
  • 4 = Newtonian incompressible EOS (class Eos_incomp_newt ).
  • 5 = Strange matter (MIT Bag model)
  • 6 = Strange matter (MIT Bag model) with crust
  • 10 = SLy4 (Douchin & Haensel 2001)
  • 11 = FPS (Friedman-Pandharipande + Skyrme)
  • 12 = BPAL12 (Bombaci et al. 1995)
  • 13 = AkmalPR (Akmal, Pandharipande & Ravenhall 1998)
  • 14 = BBB2 (Baldo, Bombaci & Burgio 1997)
  • 15 = BalbN1H1 (Balberg 2000)
  • 16 = GlendNH3 (Glendenning 1985, case 3)
  • 17 = Compstar (Tabulated EOS for 2010 CompStar school)
  • 18 = magnetized (tabulated) equation of state
  • 19 = relativistic ideal Fermi gas at zero temperature (class Eos_Fermi)
  • 100 = Multi-domain EOS (class MEos )
  • 110 = Multi-polytropic EOS (class Eos_multi_poly )
  • 120 = Fitted SLy4 (Shibata 2004)
  • 121 = Fitted FPS (Shibata 2004)
  • 122 = Fitted AkmalPR (Taniguchi 2005)

The second line in the file should contain a name given by the user to the EOS. The following lines should contain the EOS parameters (one parameter per line), in the same order than in the class declaration.

Definition at line 317 of file eos_from_file.C.

Eos * Lorene::Eos::eos_from_file ( FILE *  fich  )  [static]

Construction of an EOS from a binary file.

The file must have been created by the function sauve(FILE*) .

Definition at line 180 of file eos_from_file.C.

References Lorene::fread_be().

const char * Lorene::Eos::get_name (  )  const

Returns the EOS name.

Definition at line 176 of file eos.C.

References name.

virtual int Lorene::Eos::identify (  )  const [pure virtual]
Scalar Lorene::Eos::nbar_ent ( const Scalar ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the baryon density field from the log-enthalpy field and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the baryon density is to be computed.
l_min index of the innermost domain is which the baryon density is to be computed [default value: 0]; the baryon density is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
baryon density [unit: $n_{\rm nuc} := 0.1 \ {\rm fm}^{-3}$]

Definition at line 369 of file eos.C.

References calcule(), Lorene::Tensor::get_mp(), and nbar_ent_p().

Cmp Lorene::Eos::nbar_ent ( const Cmp ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the baryon density field from the log-enthalpy field and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the baryon density is to be computed.
l_min index of the innermost domain is which the baryon density is to be computed [default value: 0]; the baryon density is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
baryon density [unit: $n_{\rm nuc} := 0.1 \ {\rm fm}^{-3}$]

Definition at line 359 of file eos.C.

References calcule(), Lorene::Cmp::get_mp(), and nbar_ent_p().

virtual double Lorene::Eos::nbar_ent_p ( double  ent,
const Param par = 0x0 
) const [pure virtual]

Computes the baryon density from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
par possible extra parameters of the EOS
Returns:
baryon density [unit: $n_{\rm nuc} := 0.1 \ {\rm fm}^{-3}$]

Implemented in Lorene::Eos_poly, Lorene::Eos_poly_newt, Lorene::Eos_incomp, Lorene::Eos_incomp_newt, Lorene::Eos_strange, Lorene::Eos_strange_cr, Lorene::Eos_Fermi, Lorene::MEos, Lorene::Eos_consistent, Lorene::Eos_fitting, Lorene::Eos_mag, Lorene::Eos_multi_poly, and Lorene::Eos_tabul.

virtual bool Lorene::Eos::operator!= ( const Eos  )  const [pure virtual]

Comparison operator (difference).

virtual bool Lorene::Eos::operator== ( const Eos  )  const [pure virtual]

Comparison operator (egality).

virtual ostream& Lorene::Eos::operator>> ( ostream &   )  const [protected, pure virtual]
Scalar Lorene::Eos::press_ent ( const Scalar ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the pressure from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the pressure is to be computed.
l_min index of the innermost domain is which the pressure is to be computed [default value: 0]; the pressure is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
pressure [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Definition at line 416 of file eos.C.

References calcule(), Lorene::Tensor::get_mp(), and press_ent_p().

Cmp Lorene::Eos::press_ent ( const Cmp ent,
int  nzet,
int  l_min = 0,
Param par = 0x0 
) const

Computes the pressure from the log-enthalpy and extra parameters.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
nzet number of domains where the pressure is to be computed.
l_min index of the innermost domain is which the pressure is to be computed [default value: 0]; the pressure is computed only in domains whose indices are in [l_min,l_min+nzet-1] . In the other domains, it is set to zero.
par possible extra parameters of the EOS
Returns:
pressure [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Definition at line 406 of file eos.C.

References calcule(), Lorene::Cmp::get_mp(), and press_ent_p().

virtual double Lorene::Eos::press_ent_p ( double  ent,
const Param par = 0x0 
) const [pure virtual]

Computes the pressure from the log-enthalpy and extra parameters (virtual function implemented in the derived classes).

Parameters:
ent [input, unit: $c^2$] log-enthalpy H defined by $H = c^2 \ln\left( {e+p \over m_B c^2 n} \right) $, where e is the (total) energy density, p the pressure, n the baryon density, and $m_B$ the baryon mass
par possible extra parameters of the EOS
Returns:
pressure p [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Implemented in Lorene::Eos_poly, Lorene::Eos_poly_newt, Lorene::Eos_incomp, Lorene::Eos_incomp_newt, Lorene::Eos_strange, Lorene::Eos_strange_cr, Lorene::Eos_Fermi, Lorene::MEos, Lorene::Eos_consistent, Lorene::Eos_fitting, Lorene::Eos_mag, Lorene::Eos_multi_poly, and Lorene::Eos_tabul.

void Lorene::Eos::sauve ( FILE *  fich  )  const [virtual]
void Lorene::Eos::set_name ( const char *  name_i  ) 

Sets the EOS name.

Definition at line 170 of file eos.C.

References name.


Friends And Related Function Documentation

ostream& operator<< ( ostream &  ,
const Eos  
) [friend]

Display.


Member Data Documentation

char Lorene::Eos::name[100] [protected]

EOS name.

Definition at line 199 of file eos.h.


The documentation for this class was generated from the following files:

Generated on 7 Dec 2019 for LORENE by  doxygen 1.6.1