cantera/Cantera/src/StoichSubstance.h

425 lines
12 KiB
C++

/**
*
* @file StoichSubstance.h
*
* This file contains the class declarations for the StoichSubstance
* ThermoPhase class.
*/
/* $Author$
* $Date$
* $Revision$
*
* Copyright 2001 California Institute of Technology
*
*/
#ifndef CT_STOICHSUBSTANCE_H
#define CT_STOICHSUBSTANCE_H
#include "mix_defs.h"
#include "ThermoPhase.h"
#include "SpeciesThermo.h"
namespace Cantera {
/**
* @ingroup thermoprops
*
* Class StoichSubstance represents a stoichiometric (fixed composition)
* incompressible substance.
* \nosubgrouping
*
*/
class StoichSubstance : public ThermoPhase {
public:
StoichSubstance():
m_kk(0),
m_tmin(0.0),
m_tmax(0.0),
m_press(OneAtm),
m_p0(OneAtm),
m_tlast(-1.0) {}
virtual ~StoichSubstance() {}
/**
*
* @name Utilities
* @{
*/
/**
* Equation of state flag. Returns the value cStoichSubstance,
* defined in mix_defs.h.
*/
virtual int eosType() const { return cStoichSubstance; }
/**
* @}
* @name Molar Thermodynamic Properties of the Solution ---------
* @{
*/
/**
* Molar enthalpy. Units: J/kmol. For an incompressible,
* stoichiometric substance, the internal energy is
* independent of pressure, and therefore the molar enthalpy
* is \f[ \hat h(T, P) = \hat u(T) + P \hat v \f], where the
* molar specific volume is constant.
*/
virtual doublereal enthalpy_mole() const {
double hh = intEnergy_mole() + m_press / molarDensity();
return hh;
}
/**
* Molar internal energy. J/kmol. For an incompressible,
* stoichiometric substance, the molar internal energy is
* independent of pressure. Since the thermodynamic properties
* are specified by giving the standard-state enthalpy, the
* term \f$ P_0 \hat v\f$ is subtracted from the specified molar
* enthalpy to compute the molar internal energy.
*/
virtual doublereal intEnergy_mole() const {
_updateThermo();
return GasConstant * temperature() * m_h0_RT[0]
- m_p0 / molarDensity();
}
/**
* Molar entropy. Units: J/kmol/K. For an incompressible,
* stoichiometric substance, the molar entropy depends only on
* the temperature.
*/
virtual doublereal entropy_mole() const {
_updateThermo();
return GasConstant * m_s0_R[0];
}
/**
* Molar gibbs Function. Units: J/kmol. This is determined
* from the molar enthalpy and entropy functions.
*/
virtual doublereal gibbs_mole() const {
return enthalpy_mole() - temperature() * entropy_mole();
}
/**
* Molar heat capacity at constant pressure. Units: J/kmol/K.
* For an incompressible substance, \f$ \hat c_p = \hat c_v\f$.
*/
virtual doublereal cp_mole() const {
_updateThermo();
return GasConstant * m_cp0_R[0];
}
/**
* Molar heat capacity at constant volume. Units: J/kmol/K.
* For an incompressible substance, \f$ \hat c_p = \hat c_v\f$.
*/
virtual doublereal cv_mole() const {
return cp_mole();
}
//@}
/**
* @name Mechanical Equation of State
* @{
*/
/**
* Pressure. Units: Pa.
* For an incompressible substance, the density is independent
* of pressure. This method simply returns the stored
* pressure value.
*/
virtual doublereal pressure() const {
return m_press;
}
/**
* Set the pressure at constant temperature. Units: Pa.
* For an incompressible substance, the density is
* independent of pressure. Therefore, this method only
* stores the specified pressure value. It does not
* modify the density.
*/
virtual void setPressure(doublereal p) {
m_press = p;
}
//@}
/**
* @name Chemical Potentials and Activities
*@{
*/
/**
* This method returns the array of generalized
* concentrations. For a stoichiometric substance, there is
* only one species, and the generalized concentration is 1.0.
*/
virtual void getActivityConcentrations(doublereal* c) const {
c[0] = 1.0;
}
/**
* The standard concentration. This is defined as the concentration
* by which the generalized concentration is normalized to produce
* the activity.
*/
virtual doublereal standardConcentration(int k=0) const {
return 1.0;
}
/**
* Returns the natural logarithm of the standard
* concentration of the kth species
*/
virtual doublereal logStandardConc(int k=0) const {
return 0.0;
}
/**
* Get the array of chemical potentials at unit activity
* \f$ \mu^0_k \f$.
*
* For a stoichiometric substance, there is no activity term in
* the chemical potential expression, and therefore the
* standard chemical potential and the chemical potential
* are both equal to the molar Gibbs function.
*/
virtual void getStandardChemPotentials(doublereal* mu0) const {
mu0[0] = gibbs_mole();
}
/**
* Returns the units of the standard and generalized
* concentrations Note they have the same units, as their
* ratio is defined to be equal to the activity of the kth
* species in the solution, which is unitless.
*
* This routine is used in print out applications where the
* units are needed. Usually, MKS units are assumed throughout
* the program and in the XML input files.
*
* uA[0] = kmol units - default = 0
* uA[1] = m units - default = 0
* uA[2] = kg units - default = 0;
* uA[3] = Pa(pressure) units - default = 0;
* uA[4] = Temperature units - default = 0;
* uA[5] = time units - default = 0
*/
virtual void getUnitsStandardConc(double *uA, int k = 0,
int sizeUA = 6);
//@}
/// @name Partial Molar Properties of the Solution ----------------------------------
//@{
/**
* Get the array of non-dimensional chemical potentials
* \f$ \mu_k / \hat R T \f$.
*/
virtual void getChemPotentials_RT(doublereal* mu) const {
mu[0] = gibbs_mole() / (GasConstant * temperature());
}
/**
* For a stoichiometric substance, there is only one species.
* This method returns the molar gibbs function in the
* first element of array \c mu.
*/
virtual void getChemPotentials(doublereal* mu) const {
mu[0] = gibbs_mole();
}
/**
* Get the species electrochemical potentials. Units: J/kmol.
* This method adds a term \f$ Fz_k \phi_k \f$ to the
* to each chemical potential.
*/
void getElectrochemPotentials(doublereal* mu) const {
getChemPotentials(mu);
}
/**
* Returns an array of partial molar enthalpies for the species
* in the mixture.
* Units (J/kmol)
*/
virtual void getPartialMolarEnthalpies(doublereal* hbar) const {
hbar[0] = enthalpy_mole();
}
/**
* Returns an array of partial molar entropies of the species in the
* solution. Units: J/kmol/K.
*/
virtual void getPartialMolarEntropies(doublereal* sbar) const {
sbar[0] = entropy_mole();
}
/**
* returns an array of partial molar volumes of the species
* in the solution. Units: m^3 kmol-1.
*/
virtual void getPartialMolarVolumes(doublereal* vbar) const {
vbar[0] = 1.0 / molarDensity();
}
//@}
/// @name Properties of the Standard State of the Species in the Solution -------------------------------------
//@{
/**
* Get the nondimensional Enthalpy functions for the species
* at their standard states at the current
* <I>T</I> and <I>P</I> of the solution.
*/
virtual void getEnthalpy_RT(doublereal* hrt) const {
hrt[0] = enthalpy_mole() / (GasConstant * temperature());
}
/**
* Get the array of nondimensional Enthalpy functions for the
* standard state species
* at the current <I>T</I> and <I>P</I> of the solution.
*/
virtual void getEntropy_R(doublereal* sr) const {
sr[0] = entropy_mole() / GasConstant;
}
/**
* Get the nondimensional Gibbs functions for the species
* at their standard states of solution at the current T and P
* of the solution.
*/
virtual void getGibbs_RT(doublereal* grt) const {
grt[0] = gibbs_mole() / (GasConstant * temperature());
}
/**
* Get the nondimensional Heat Capacities at constant
* pressure for the standard state of the species
* at the current T and P.
*/
virtual void getCp_R(doublereal* cpr) const {
cpr[0] = cp_mole() / GasConstant;
}
/**
* Get the standard volumes for the standard state of the species
* at the current T and P
*/
virtual void getStandardVolumes(doublereal*vol) const {
vol[0] = 1.0 / molarDensity();
}
//@}
/// @name Thermodynamic Values for the Species Reference States --------------------
//@{
/**
* Returns the vector of nondimensional
* enthalpies of the reference state at the current temperature
* of the solution and the reference pressure for the species.
*
* This function fills in its one entry in hrt[] by calling
* the underlying species thermo function for the
* dimensionless enthalpy.
*/
virtual void getEnthalpy_RT_ref(doublereal *hrt) const {
_updateThermo();
hrt[0] = m_h0_RT[0];
}
/**
* Returns the vector of nondimensional
* enthalpies of the reference state at the current temperature
* of the solution and the reference pressure for the species.
*
* This function fills in its one entry in hrt[] by calling
* the underlying species thermo function for the
* dimensionless gibbs free energy, calculated from the
* dimensionless enthalpy and entropy.
*/
virtual void getGibbs_RT_ref(doublereal *grt) const {
_updateThermo();
grt[0] = m_h0_RT[0] - m_s0_R[0];
}
/**
* Returns the vector of the
* gibbs function of the reference state at the current temperature
* of the solution and the reference pressure for the species.
* units = J/kmol
*
* This function fills in its one entry in g[] by calling
* the underlying species thermo functions for the
* gibbs free energy, calculated from enthalpy and the
* entropy, and the multiplying by RT.
*/
virtual void getGibbs_ref(doublereal *g) const {
getGibbs_RT_ref(g);
g[0] *= GasConstant * temperature();
}
/**
* Returns the vector of nondimensional
* entropies of the reference state at the current temperature
* of the solution and the reference pressure for the species.
*
* This function fills in its one entry in hrt[] by calling
* the underlying species thermo function for the
* dimensionless entropy.
*/
virtual void getEntropy_R_ref(doublereal *er) const {
_updateThermo();
er[0] = m_s0_R[0];
}
virtual void initThermo();
virtual void setParameters(int n, double *c);
virtual void getParameters(int &n, double * const c);
virtual void setParametersFromXML(const XML_Node& eosdata);
protected:
int m_kk;
doublereal m_tmin, m_tmax, m_press, m_p0;
mutable doublereal m_tlast;
mutable array_fp m_h0_RT;
mutable array_fp m_cp0_R;
mutable array_fp m_s0_R;
private:
void _updateThermo() const;
};
}
#endif