Eos_Fermi Class Reference
[Equations of state]

Degenerate ideal Fermi gas. More...

#include <eos.h>

Inheritance diagram for Eos_Fermi:
Eos

List of all members.

Public Member Functions

 Eos_Fermi (double mass)
 Standard constructor (sets g_s to 2).
 Eos_Fermi (double mass, int g_degen)
 Standard constructor.
 Eos_Fermi (const Eos_Fermi &)
 Copy constructor.
virtual ~Eos_Fermi ()
 Destructor.
void operator= (const Eos_Fermi &)
 Assignment to another Eos_Fermi.
virtual bool operator== (const Eos &) const
 Comparison operator (egality).
virtual bool operator!= (const Eos &) const
 Comparison operator (difference).
virtual int identify () const
 Returns a number to identify the sub-classe of Eos the object belongs to.
double get_m () const
 Returns the fermion mass in eV/c2.
int get_g_degen () const
 Returns the degeneracy factor.
virtual void sauve (FILE *) const
 Save in a file.
virtual double nbar_ent_p (double ent, const Param *par=0x0) const
 Computes the baryon density from the log-enthalpy.
virtual double ener_ent_p (double ent, const Param *par=0x0) const
 Computes the total energy density from the log-enthalpy.
virtual double press_ent_p (double ent, const Param *par=0x0) const
 Computes the pressure from the log-enthalpy.
virtual double der_nbar_ent_p (double ent, const Param *par=0x0) const
 Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy.
virtual double der_ener_ent_p (double ent, const Param *par=0x0) const
 Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy.
virtual double der_press_ent_p (double ent, const Param *par=0x0) const
 Computes the logarithmic derivative $d\ln p/d\ln H$ from the log-enthalpy.
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).
Cmp nbar_ent (const Cmp &ent, int nzet, int l_min=0, const 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, const Param *par=0x0) const
 Computes the baryon density field from the log-enthalpy field and extra parameters.
Cmp ener_ent (const Cmp &ent, int nzet, int l_min=0, const 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, const Param *par=0x0) const
 Computes the total energy density from the log-enthalpy and extra parameters.
Cmp press_ent (const Cmp &ent, int nzet, int l_min=0, const 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, const Param *par=0x0) const
 Computes the pressure from the log-enthalpy and extra parameters.
Cmp der_nbar_ent (const Cmp &ent, int nzet, int l_min=0, const 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, const Param *par=0x0) const
 Computes the logarithmic derivative $d\ln n/d\ln H$ from the log-enthalpy and extra parameters.
Cmp der_ener_ent (const Cmp &ent, int nzet, int l_min=0, const 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, const Param *par=0x0) const
 Computes the logarithmic derivative $d\ln e/d\ln H$ from the log-enthalpy and extra parameters.
Cmp der_press_ent (const Cmp &ent, int nzet, int l_min=0, const 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, const 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 Eos * eos_from_file (FILE *)
 Construction of an EOS from a binary file.
static Eos * eos_from_file (ifstream &)
 Construction of an EOS from a formatted file.

Protected Member Functions

 Eos_Fermi (FILE *)
 Constructor from a binary file (created by the function sauve(FILE*) ).
 Eos_Fermi (ifstream &)
 Constructor from a formatted file.
void set_auxiliary ()
 Computes the auxiliary quantities n_0 , ener_0.
virtual ostream & operator>> (ostream &) const
 Operator >>.
void calcule (const Cmp &thermo, int nzet, int l_min, double(Eos::*fait)(double, const Param *) const, 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, const Param *par, Scalar &resu) const
 General computational method for Scalar 's.

Protected Attributes

double m_0
 Individual particule mass $m_0$ [unit: eV/c2].
int g_s
 Degeneracy parameter.
double n_0
 Number density scale [unit: $n_{\rm nuc} := 0.1 \ {\rm fm}^{-3}$].
double ener_0
 Energy density scale [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$].
double p_0
 Pressure scale [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$].
char name [100]
 EOS name.

Friends

Eos * Eos::eos_from_file (FILE *)
 The construction functions from a file.
Eos * Eos::eos_from_file (ifstream &)
ostream & operator<< (ostream &, const Eos &)
 Display.

Detailed Description

Degenerate ideal Fermi gas.

This equation of state describes an ideal gas of relativistic fermions at zero temperature. It has two parameters : the fermion mass $m$ and the degeneracy $g_s$ of each momentum state (for electrons or neutrons : $g_s = 2$).

*** NB: This class is _under construction_ and not fully tested yet ! ***

()

Definition at line 2080 of file eos.h.

Constructor & Destructor Documentation

Eos_Fermi::Eos_Fermi ( double  mass  ) 

Standard constructor (sets g_s to 2).

Parameters:
mass mass of each fermion in eV/c2

Definition at line 58 of file eos_fermi.C.

References set_auxiliary().

Eos_Fermi::Eos_Fermi ( double  mass,
int  g_degen 
)

Standard constructor.

Parameters:
mass mass of each fermion in eV/c2
g_degen degeneracy factor (value for electrons or neutrons: 2)

Definition at line 69 of file eos_fermi.C.

References set_auxiliary().

Eos_Fermi::Eos_Fermi ( const Eos_Fermi &  eosi  ) 

Copy constructor.

Definition at line 80 of file eos_fermi.C.

References set_auxiliary().

Eos_Fermi::Eos_Fermi ( 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 91 of file eos_fermi.C.

References fread_be(), g_s, m_0, and set_auxiliary().

Eos_Fermi::Eos_Fermi ( 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 104 of file eos_fermi.C.

References g_s, m_0, and set_auxiliary().

Eos_Fermi::~Eos_Fermi (  )  [virtual]

Destructor.

Definition at line 119 of file eos_fermi.C.

Member Function Documentation

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

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 264 of file eos.C.

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

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

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 199 of file eos.C.

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

Scalar Eos::der_ener_ent ( const Scalar &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 436 of file eos.C.

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

Cmp Eos::der_ener_ent ( const Cmp &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 426 of file eos.C.

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

double Eos_Fermi::der_ener_ent_p ( double  ent,
const Param *  par = 0x0 
) const [virtual]

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

Parameters:
ent [input, unit: $c^2$] log-enthalpy H
par possible extra parameters of the EOS (not used here)
Returns:
dln(e)/dln(H)

Implements Eos.

Definition at line 307 of file eos_fermi.C.

Scalar Eos::der_nbar_ent ( const Scalar &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 413 of file eos.C.

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

Cmp Eos::der_nbar_ent ( const Cmp &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 403 of file eos.C.

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

double Eos_Fermi::der_nbar_ent_p ( double  ent,
const Param *  par = 0x0 
) const [virtual]

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

Parameters:
ent [input, unit: $c^2$] log-enthalpy H
par possible extra parameters of the EOS (not used here)
Returns:
dln(n)/dln(H)

Implements Eos.

Definition at line 297 of file eos_fermi.C.

Scalar Eos::der_press_ent ( const Scalar &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 458 of file eos.C.

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

Cmp Eos::der_press_ent ( const Cmp &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 448 of file eos.C.

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

double Eos_Fermi::der_press_ent_p ( double  ent,
const Param *  par = 0x0 
) const [virtual]

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

Parameters:
ent [input, unit: $c^2$] log-enthalpy H
par possible extra parameters of the EOS
Returns:
dln(p)/dln(H)

Implements Eos.

Definition at line 317 of file eos_fermi.C.

Scalar Eos::ener_ent ( const Scalar &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 369 of file eos.C.

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

Cmp Eos::ener_ent ( const Cmp &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 359 of file eos.C.

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

double Eos_Fermi::ener_ent_p ( double  ent,
const Param *  par = 0x0 
) const [virtual]

Computes the total energy density from the log-enthalpy.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H
par possible extra parameters of the EOS (not used here)
Returns:
energy density e [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Implements Eos.

Definition at line 260 of file eos_fermi.C.

References ener_0, exp(), log(), and sqrt().

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

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 297 of file eos_from_file.C.

Eos * Eos::eos_from_file ( FILE *  fich  )  [static, inherited]

Construction of an EOS from a binary file.

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

Definition at line 165 of file eos_from_file.C.

References fread_be().

int Eos_Fermi::get_g_degen (  )  const

Returns the degeneracy factor.

Definition at line 162 of file eos_fermi.C.

References g_s.

double Eos_Fermi::get_m (  )  const

Returns the fermion mass in eV/c2.

Definition at line 158 of file eos_fermi.C.

References m_0.

const char * Eos::get_name (  )  const [inherited]

Returns the EOS name.

Definition at line 165 of file eos.C.

References Eos::name.

int Eos_Fermi::identify (  )  const [virtual]

Returns a number to identify the sub-classe of Eos the object belongs to.

Implements Eos.

Definition at line 149 of file eos_from_file.C.

Scalar Eos::nbar_ent ( const Scalar &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 344 of file eos.C.

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

Cmp Eos::nbar_ent ( const Cmp &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 334 of file eos.C.

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

double Eos_Fermi::nbar_ent_p ( double  ent,
const Param *  par = 0x0 
) const [virtual]

Computes the baryon density from the log-enthalpy.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H
par possible extra parameters of the EOS (not used here)
Returns:
baryon density n [unit: $n_{\rm nuc} := 0.1 \ {\rm fm}^{-3}$]

Implements Eos.

Definition at line 244 of file eos_fermi.C.

References exp(), n_0, and sqrt().

virtual bool Eos::operator!= ( const Eos &   )  const [pure virtual, inherited]

Comparison operator (difference).

bool Eos_Fermi::operator!= ( const Eos &  eos_i  )  const [virtual]

Comparison operator (difference).

Definition at line 206 of file eos_fermi.C.

References operator==().

void Eos_Fermi::operator= ( const Eos_Fermi &  eosi  ) 

Assignment to another Eos_Fermi.

Definition at line 128 of file eos_fermi.C.

References g_s, m_0, Eos::name, set_auxiliary(), and Eos::set_name().

virtual bool Eos::operator== ( const Eos &   )  const [pure virtual, inherited]

Comparison operator (egality).

bool Eos_Fermi::operator== ( const Eos &  eos_i  )  const [virtual]

Comparison operator (egality).

Definition at line 173 of file eos_fermi.C.

References g_s, identify(), Eos::identify(), and m_0.

ostream & Eos_Fermi::operator>> ( ostream &  ost  )  const [protected, virtual]

Operator >>.

Implements Eos.

Definition at line 226 of file eos_fermi.C.

References g_s, and m_0.

Scalar Eos::press_ent ( const Scalar &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 391 of file eos.C.

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

Cmp Eos::press_ent ( const Cmp &  ent,
int  nzet,
int  l_min = 0,
const Param *  par = 0x0 
) const [inherited]

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 381 of file eos.C.

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

double Eos_Fermi::press_ent_p ( double  ent,
const Param *  par = 0x0 
) const [virtual]

Computes the pressure from the log-enthalpy.

Parameters:
ent [input, unit: $c^2$] log-enthalpy H
par possible extra parameters of the EOS (not used here)
Returns:
pressure p [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$

Implements Eos.

Definition at line 278 of file eos_fermi.C.

References exp(), log(), p_0, and sqrt().

void Eos_Fermi::sauve ( FILE *  fich  )  const [virtual]

Save in a file.

Reimplemented from Eos.

Definition at line 217 of file eos_fermi.C.

References fwrite_be(), g_s, and m_0.

void Eos_Fermi::set_auxiliary (  )  [protected]

Computes the auxiliary quantities n_0 , ener_0.

Definition at line 144 of file eos_fermi.C.

References ener_0, g_s, m_0, n_0, and p_0.

void Eos::set_name ( const char *  name_i  )  [inherited]

Sets the EOS name.

Definition at line 159 of file eos.C.

References Eos::name.

Friends And Related Function Documentation

Eos* Eos::eos_from_file ( FILE *   )  [friend]

The construction functions from a file.

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

Display.

Member Data Documentation

double Eos_Fermi::ener_0 [protected]

Energy density scale [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$].

Definition at line 2102 of file eos.h.

int Eos_Fermi::g_s [protected]

Degeneracy parameter.

Definition at line 2093 of file eos.h.

double Eos_Fermi::m_0 [protected]

Individual particule mass $m_0$ [unit: eV/c2].

Definition at line 2089 of file eos.h.

double Eos_Fermi::n_0 [protected]

Number density scale [unit: $n_{\rm nuc} := 0.1 \ {\rm fm}^{-3}$].

Definition at line 2097 of file eos.h.

char Eos::name[100] [protected, inherited]

EOS name.

Definition at line 186 of file eos.h.

double Eos_Fermi::p_0 [protected]

Pressure scale [unit: $\rho_{\rm nuc} c^2$], where $\rho_{\rm nuc} := 1.66\ 10^{17} \ {\rm kg/m}^3$].

Definition at line 2108 of file eos.h.

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