cantera/src/thermo/IdealGasPhase.cpp

648 lines
16 KiB
C++

/**
* @file IdealGasPhase.cpp
* ThermoPhase object for the ideal gas equation of
* state - workhorse for %Cantera (see \ref thermoprops
* and class \link Cantera::IdealGasPhase IdealGasPhase\endlink).
*/
#include "cantera/base/ct_defs.h"
#include "cantera/thermo/mix_defs.h"
#include "cantera/thermo/IdealGasPhase.h"
#include "cantera/thermo/SpeciesThermo.h"
using namespace std;
namespace Cantera
{
// Default empty Constructor
IdealGasPhase::IdealGasPhase():
m_mm(0),
m_tmin(0.0),
m_tmax(0.0),
m_p0(-1.0),
m_tlast(0.0),
m_logc0(0.0)
{
}
// Copy Constructor
IdealGasPhase::IdealGasPhase(const IdealGasPhase& right):
m_mm(right.m_mm),
m_tmin(right.m_tmin),
m_tmax(right.m_tmax),
m_p0(right.m_p0),
m_tlast(right.m_tlast),
m_logc0(right.m_logc0)
{
/*
* Use the assignment operator to do the brunt
* of the work for the copy constructor.
*/
*this = right;
}
// Assignment operator
/*
* Assignment operator for the object. Constructed
* object will be a clone of this object, but will
* also own all of its data.
*
* @param right Object to be copied.
*/
IdealGasPhase& IdealGasPhase::
operator=(const IdealGasPhase& right)
{
if (&right != this) {
ThermoPhase::operator=(right);
m_mm = right.m_mm;
m_tmin = right.m_tmin;
m_tmax = right.m_tmax;
m_p0 = right.m_p0;
m_tlast = right.m_tlast;
m_logc0 = right.m_logc0;
m_h0_RT = right.m_h0_RT;
m_cp0_R = right.m_cp0_R;
m_g0_RT = right.m_g0_RT;
m_s0_R = right.m_s0_R;
m_expg0_RT= right.m_expg0_RT;
m_pp = right.m_pp;
}
return *this;
}
// Duplicator from the %ThermoPhase parent class
/*
* Given a pointer to a %ThermoPhase object, this function will
* duplicate the %ThermoPhase object and all underlying structures.
* This is basically a wrapper around the copy constructor.
*
* @return returns a pointer to a %ThermoPhase
*/
ThermoPhase* IdealGasPhase::duplMyselfAsThermoPhase() const
{
return new IdealGasPhase(*this);
}
// Molar Thermodynamic Properties of the Solution ------------------
/*
* Molar internal energy. J/kmol. For an ideal gas mixture,
* \f[
* \hat u(T) = \sum_k X_k \hat h^0_k(T) - \hat R T,
* \f]
* and is a function only of temperature.
* The reference-state pure-species enthalpies
* \f$ \hat h^0_k(T) \f$ are computed by the species thermodynamic
* property manager.
* @see SpeciesThermo
*/
doublereal IdealGasPhase::intEnergy_mole() const
{
return GasConstant * temperature()
* (mean_X(&enthalpy_RT_ref()[0]) - 1.0);
}
/*
* Molar entropy. Units: J/kmol/K.
* For an ideal gas mixture,
* \f[
* \hat s(T, P) = \sum_k X_k \hat s^0_k(T) - \hat R \log (P/P^0).
* \f]
* The reference-state pure-species entropies
* \f$ \hat s^0_k(T) \f$ are computed by the species thermodynamic
* property manager.
* @see SpeciesThermo
*/
doublereal IdealGasPhase::entropy_mole() const
{
return GasConstant * (mean_X(&entropy_R_ref()[0]) -
sum_xlogx() - std::log(pressure()/m_spthermo->refPressure()));
}
/*
* Molar Gibbs free Energy for an ideal gas.
* Units = J/kmol.
*/
doublereal IdealGasPhase::gibbs_mole() const
{
return enthalpy_mole() - temperature() * entropy_mole();
}
/*
* Molar heat capacity at constant pressure. Units: J/kmol/K.
* For an ideal gas mixture,
* \f[
* \hat c_p(t) = \sum_k \hat c^0_{p,k}(T).
* \f]
* The reference-state pure-species heat capacities
* \f$ \hat c^0_{p,k}(T) \f$ are computed by the species thermodynamic
* property manager.
* @see SpeciesThermo
*/
doublereal IdealGasPhase::cp_mole() const
{
return GasConstant * mean_X(&cp_R_ref()[0]);
}
/*
* Molar heat capacity at constant volume. Units: J/kmol/K.
* For an ideal gas mixture,
* \f[ \hat c_v = \hat c_p - \hat R. \f]
*/
doublereal IdealGasPhase::cv_mole() const
{
return cp_mole() - GasConstant;
}
/**
* @returns species translational/rotational specific heat at
* constant volume.
*
* Either: $5/2 R_s$ or $3/2 R_s$ for molecules/atoms.
*
*/
doublereal IdealGasPhase::cv_tr(doublereal atomicity) const
{
// k is the species number
int dum = 0;
int type = 0;
doublereal c[12];
doublereal minTemp;
doublereal maxTemp;
doublereal refPressure;
m_spthermo->reportParams(dum,type,c,minTemp,maxTemp,refPressure);
if (type != 111) {
throw CanteraError("Error in IdealGasPhase.cpp",
"cv_tr only supported for StatMech!. \n\n");
}
// see reportParameters for specific details
return c[3];
}
/**
* @returns species translational specific heat at constant volume.
*/
doublereal IdealGasPhase::cv_trans() const
{
return 1.5*GasConstant;
}
/**
* @returns species rotational specific heat at constant volume.
*
*/
doublereal IdealGasPhase::cv_rot(double atom) const
{
return std::max(cv_tr(atom) - cv_trans(), 0.);
}
/**
* @returns species vibrational specific heat at
* constant volume.
*
* C^{vib}_{v,s} = \frac{\partial e^{vib}_{v,s} }{\partial T}
*
* The species vibration energy ($e^{vib}_{v,s}$) is:
*
* 0: atom
*
* Diatomic:
* \f[
* \frac{R_s \theta_{v,s}}{e^{\theta_{v,s}/T}-1}
* \f]
*
* General Molecules:
* \f[
* \sum_i \frac{R_s \theta_{v,s,i}}{e^{\theta_{v,s,i}/T}-1}
* \f]
*
*/
doublereal IdealGasPhase::cv_vib(const int k, const doublereal T) const
{
// k is the species number
int dum = 0;
int type = 0;
doublereal c[12];
doublereal minTemp;
doublereal maxTemp;
doublereal refPressure;
c[0] = temperature();
m_spthermo->reportParams(dum,type,c,minTemp,maxTemp,refPressure);
// basic sanity check
if (type != 111) {
throw CanteraError("Error in IdealGasPhase.cpp",
"cv_vib only supported for StatMech!. \n\n");
}
// see reportParameters for specific details
return c[4];
}
// Mechanical Equation of State ----------------------------
// Chemical Potentials and Activities ----------------------
/*
* Returns the standard concentration \f$ C^0_k \f$, which is used to normalize
* the generalized concentration.
*/
doublereal IdealGasPhase::standardConcentration(size_t k) const
{
double p = pressure();
return p/(GasConstant * temperature());
}
/*
* Returns the natural logarithm of the standard
* concentration of the kth species
*/
doublereal IdealGasPhase::logStandardConc(size_t k) const
{
_updateThermo();
double p = pressure();
double lc = std::log(p / (GasConstant * temperature()));
return lc;
}
/*
* Get the array of non-dimensional activity coefficients
*/
void IdealGasPhase::getActivityCoefficients(doublereal* ac) const
{
for (size_t k = 0; k < m_kk; k++) {
ac[k] = 1.0;
}
}
/*
* Get the array of chemical potentials at unit activity \f$
* \mu^0_k(T,P) \f$.
*/
void IdealGasPhase::getStandardChemPotentials(doublereal* muStar) const
{
const vector_fp& gibbsrt = gibbs_RT_ref();
scale(gibbsrt.begin(), gibbsrt.end(), muStar, _RT());
double tmp = log(pressure() /m_spthermo->refPressure());
tmp *= GasConstant * temperature();
for (size_t k = 0; k < m_kk; k++) {
muStar[k] += tmp; // add RT*ln(P/P_0)
}
}
// Partial Molar Properties of the Solution --------------
void IdealGasPhase::getChemPotentials(doublereal* mu) const
{
getStandardChemPotentials(mu);
//doublereal logp = log(pressure()/m_spthermo->refPressure());
doublereal xx;
doublereal rt = temperature() * GasConstant;
//const vector_fp& g_RT = gibbs_RT_ref();
for (size_t k = 0; k < m_kk; k++) {
xx = std::max(SmallNumber, moleFraction(k));
mu[k] += rt*(log(xx));
}
}
/*
* Get the array of partial molar enthalpies of the species
* units = J / kmol
*/
void IdealGasPhase::getPartialMolarEnthalpies(doublereal* hbar) const
{
const vector_fp& _h = enthalpy_RT_ref();
doublereal rt = GasConstant * temperature();
scale(_h.begin(), _h.end(), hbar, rt);
}
/*
* Get the array of partial molar entropies of the species
* units = J / kmol / K
*/
void IdealGasPhase::getPartialMolarEntropies(doublereal* sbar) const
{
const vector_fp& _s = entropy_R_ref();
doublereal r = GasConstant;
scale(_s.begin(), _s.end(), sbar, r);
doublereal logp = log(pressure()/m_spthermo->refPressure());
for (size_t k = 0; k < m_kk; k++) {
doublereal xx = std::max(SmallNumber, moleFraction(k));
sbar[k] += r * (- logp - log(xx));
}
}
/*
* Get the array of partial molar internal energies of the species
* units = J / kmol
*/
void IdealGasPhase::getPartialMolarIntEnergies(doublereal* ubar) const
{
const vector_fp& _h = enthalpy_RT_ref();
doublereal rt = GasConstant * temperature();
for (size_t k = 0; k < m_kk; k++) {
ubar[k] = rt * (_h[k] - 1.0);
}
}
/*
* Get the array of partial molar heat capacities
*/
void IdealGasPhase::getPartialMolarCp(doublereal* cpbar) const
{
const vector_fp& _cp = cp_R_ref();
scale(_cp.begin(), _cp.end(), cpbar, GasConstant);
}
/*
* Get the array of partial molar volumes
* units = m^3 / kmol
*/
void IdealGasPhase::getPartialMolarVolumes(doublereal* vbar) const
{
double vol = 1.0 / molarDensity();
for (size_t k = 0; k < m_kk; k++) {
vbar[k] = vol;
}
}
// 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 T and P of the
* solution
*/
void IdealGasPhase::getEnthalpy_RT(doublereal* hrt) const
{
const vector_fp& _h = enthalpy_RT_ref();
copy(_h.begin(), _h.end(), hrt);
}
/*
* Get the array of nondimensional entropy functions for the
* standard state species
* at the current <I>T</I> and <I>P</I> of the solution.
*/
void IdealGasPhase::getEntropy_R(doublereal* sr) const
{
const vector_fp& _s = entropy_R_ref();
copy(_s.begin(), _s.end(), sr);
double tmp = log(pressure() /m_spthermo->refPressure());
for (size_t k = 0; k < m_kk; k++) {
sr[k] -= tmp;
}
}
/*
* Get the nondimensional gibbs function for the species
* standard states at the current T and P of the solution.
*/
void IdealGasPhase::getGibbs_RT(doublereal* grt) const
{
const vector_fp& gibbsrt = gibbs_RT_ref();
copy(gibbsrt.begin(), gibbsrt.end(), grt);
double tmp = log(pressure() /m_spthermo->refPressure());
for (size_t k = 0; k < m_kk; k++) {
grt[k] += tmp;
}
}
/*
* get the pure Gibbs free energies of each species assuming
* it is in its standard state. This is the same as
* getStandardChemPotentials().
*/
void IdealGasPhase::getPureGibbs(doublereal* gpure) const
{
const vector_fp& gibbsrt = gibbs_RT_ref();
scale(gibbsrt.begin(), gibbsrt.end(), gpure, _RT());
double tmp = log(pressure() /m_spthermo->refPressure());
tmp *= _RT();
for (size_t k = 0; k < m_kk; k++) {
gpure[k] += tmp;
}
}
/*
* Returns the vector of nondimensional
* internal Energies of the standard state at the current temperature
* and pressure of the solution for each species.
*/
void IdealGasPhase::getIntEnergy_RT(doublereal* urt) const
{
const vector_fp& _h = enthalpy_RT_ref();
for (size_t k = 0; k < m_kk; k++) {
urt[k] = _h[k] - 1.0;
}
}
/*
* Get the nondimensional heat capacity at constant pressure
* function for the species
* standard states at the current T and P of the solution.
*/
void IdealGasPhase::getCp_R(doublereal* cpr) const
{
const vector_fp& _cpr = cp_R_ref();
copy(_cpr.begin(), _cpr.end(), cpr);
}
/*
* Get the molar volumes of the species standard states at the current
* <I>T</I> and <I>P</I> of the solution.
* units = m^3 / kmol
*
* @param vol Output vector containing the standard state volumes.
* Length: m_kk.
*/
void IdealGasPhase::getStandardVolumes(doublereal* vol) const
{
double tmp = 1.0 / molarDensity();
for (size_t k = 0; k < m_kk; k++) {
vol[k] = tmp;
}
}
// Thermodynamic Values for the Species Reference States ---------
/*
* Returns the vector of nondimensional
* enthalpies of the reference state at the current temperature
* and reference pressure.
*/
void IdealGasPhase::getEnthalpy_RT_ref(doublereal* hrt) const
{
const vector_fp& _h = enthalpy_RT_ref();
copy(_h.begin(), _h.end(), hrt);
}
/*
* Returns the vector of nondimensional
* enthalpies of the reference state at the current temperature
* and reference pressure.
*/
void IdealGasPhase::getGibbs_RT_ref(doublereal* grt) const
{
const vector_fp& gibbsrt = gibbs_RT_ref();
copy(gibbsrt.begin(), gibbsrt.end(), grt);
}
/*
* Returns the vector of the
* gibbs function of the reference state at the current temperature
* and reference pressure.
* units = J/kmol
*/
void IdealGasPhase::getGibbs_ref(doublereal* g) const
{
const vector_fp& gibbsrt = gibbs_RT_ref();
scale(gibbsrt.begin(), gibbsrt.end(), g, _RT());
}
/*
* Returns the vector of nondimensional
* entropies of the reference state at the current temperature
* and reference pressure.
*/
void IdealGasPhase::getEntropy_R_ref(doublereal* er) const
{
const vector_fp& _s = entropy_R_ref();
copy(_s.begin(), _s.end(), er);
}
/*
* Returns the vector of nondimensional
* internal Energies of the reference state at the current temperature
* of the solution and the reference pressure for each species.
*/
void IdealGasPhase::getIntEnergy_RT_ref(doublereal* urt) const
{
const vector_fp& _h = enthalpy_RT_ref();
for (size_t k = 0; k < m_kk; k++) {
urt[k] = _h[k] - 1.0;
}
}
/*
* Returns the vector of nondimensional
* constant pressure heat capacities of the reference state
* at the current temperature and reference pressure.
*/
void IdealGasPhase::getCp_R_ref(doublereal* cprt) const
{
const vector_fp& _cpr = cp_R_ref();
copy(_cpr.begin(), _cpr.end(), cprt);
}
void IdealGasPhase::getStandardVolumes_ref(doublereal* vol) const
{
doublereal tmp = _RT() / m_p0;
for (size_t k = 0; k < m_kk; k++) {
vol[k] = tmp;
}
}
// new methods defined here -------------------------------
void IdealGasPhase::initThermo()
{
m_mm = nElements();
doublereal tmin = m_spthermo->minTemp();
doublereal tmax = m_spthermo->maxTemp();
if (tmin > 0.0) {
m_tmin = tmin;
}
if (tmax > 0.0) {
m_tmax = tmax;
}
m_p0 = refPressure();
m_h0_RT.resize(m_kk);
m_g0_RT.resize(m_kk);
m_expg0_RT.resize(m_kk);
m_cp0_R.resize(m_kk);
m_s0_R.resize(m_kk);
m_pp.resize(m_kk);
}
/*
* Set mixture to an equilibrium state consistent with specified
* chemical potentials and temperature. This method is needed by
* the ChemEquil equilibrium solver.
*/
void IdealGasPhase::setToEquilState(const doublereal* mu_RT)
{
double tmp, tmp2;
const vector_fp& grt = gibbs_RT_ref();
/*
* Within the method, we protect against inf results if the
* exponent is too high.
*
* If it is too low, we set
* the partial pressure to zero. This capability is needed
* by the elemental potential method.
*/
doublereal pres = 0.0;
for (size_t k = 0; k < m_kk; k++) {
tmp = -grt[k] + mu_RT[k];
if (tmp < -600.) {
m_pp[k] = 0.0;
} else if (tmp > 500.0) {
tmp2 = tmp / 500.;
tmp2 *= tmp2;
m_pp[k] = m_p0 * exp(500.) * tmp2;
} else {
m_pp[k] = m_p0 * exp(tmp);
}
pres += m_pp[k];
}
// set state
setState_PX(pres, &m_pp[0]);
}
/// This method is called each time a thermodynamic property is
/// requested, to check whether the internal species properties
/// within the object need to be updated.
/// Currently, this updates the species thermo polynomial values
/// for the current value of the temperature. A check is made
/// to see if the temperature has changed since the last
/// evaluation. This object does not contain any persistent
/// data that depends on the concentration, that needs to be
/// updated. The state object modifies its concentration
/// dependent information at the time the setMoleFractions()
/// (or equivalent) call is made.
void IdealGasPhase::_updateThermo() const
{
doublereal tnow = temperature();
// If the temperature has changed since the last time these
// properties were computed, recompute them.
if (m_tlast != tnow) {
m_spthermo->update(tnow, &m_cp0_R[0], &m_h0_RT[0],
&m_s0_R[0]);
m_tlast = tnow;
// update the species Gibbs functions
for (size_t k = 0; k < m_kk; k++) {
m_g0_RT[k] = m_h0_RT[k] - m_s0_R[k];
}
m_logc0 = log(m_p0/(GasConstant * tnow));
m_tlast = tnow;
}
}
}