Cantera
3.0.0
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Class ChemEquil implements a chemical equilibrium solver for single-phase solutions. More...
#include <ChemEquil.h>
Class ChemEquil implements a chemical equilibrium solver for single-phase solutions.
It is a "non-stoichiometric" solver in the terminology of Smith and Missen [40], meaning that every intermediate state is a valid chemical equilibrium state, but does not necessarily satisfy the element constraints. In contrast, the solver implemented in class MultiPhaseEquil uses a "stoichiometric" algorithm, in which each intermediate state satisfies the element constraints but is not a state of chemical equilibrium. Non- stoichiometric methods are faster when they converge, but stoichiometric ones tend to be more robust and can be used also for problems with multiple condensed phases. As expected, the ChemEquil solver is faster than MultiPhaseEquil for many single-phase equilibrium problems (particularly if there are only a few elements but very many species), but can be less stable. Problem situations include low temperatures where only a few species have non-zero mole fractions, precisely stoichiometric compositions (for example, 2 H2 + O2). In general, if speed is important, this solver should be tried first, and if it fails then use MultiPhaseEquil.
Definition at line 78 of file ChemEquil.h.
Public Member Functions | |
ChemEquil (ThermoPhase &s) | |
Constructor combined with the initialization function. | |
int | equilibrate (ThermoPhase &s, const char *XY, int loglevel=0) |
Equilibrate a phase, holding the elemental composition fixed at the initial value found within the ThermoPhase object s. | |
int | equilibrate (ThermoPhase &s, const char *XY, vector< double > &elMoles, int loglevel=0) |
Compute the equilibrium composition for two specified properties and the specified element moles. | |
Public Attributes | |
EquilOpt | options |
Options controlling how the calculation is carried out. | |
Protected Member Functions | |
double | nAtoms (size_t k, size_t m) const |
number of atoms of element m in species k. | |
void | initialize (ThermoPhase &s) |
Prepare for equilibrium calculations. | |
void | setToEquilState (ThermoPhase &s, const vector< double > &x, double t) |
Set mixture to an equilibrium state consistent with specified element potentials and temperature. | |
int | setInitialMoles (ThermoPhase &s, vector< double > &elMoleGoal, int loglevel=0) |
Estimate the initial mole numbers. | |
int | estimateElementPotentials (ThermoPhase &s, vector< double > &lambda, vector< double > &elMolesGoal, int loglevel=0) |
Generate a starting estimate for the element potentials. | |
int | estimateEP_Brinkley (ThermoPhase &s, vector< double > &lambda, vector< double > &elMoles) |
Do a calculation of the element potentials using the Brinkley method, p. | |
int | dampStep (ThermoPhase &s, vector< double > &oldx, double oldf, vector< double > &grad, vector< double > &step, vector< double > &x, double &f, vector< double > &elmols, double xval, double yval) |
Find an acceptable step size and take it. | |
void | equilResidual (ThermoPhase &s, const vector< double > &x, const vector< double > &elmtotal, vector< double > &resid, double xval, double yval, int loglevel=0) |
Evaluates the residual vector F, of length m_mm. | |
void | equilJacobian (ThermoPhase &s, vector< double > &x, const vector< double > &elmols, DenseMatrix &jac, double xval, double yval, int loglevel=0) |
void | adjustEloc (ThermoPhase &s, vector< double > &elMolesGoal) |
void | update (const ThermoPhase &s) |
Update internally stored state information. | |
double | calcEmoles (ThermoPhase &s, vector< double > &x, const double &n_t, const vector< double > &Xmol_i_calc, vector< double > &eMolesCalc, vector< double > &n_i_calc, double pressureConst) |
Given a vector of dimensionless element abundances, this routine calculates the moles of the elements and the moles of the species. | |
Protected Attributes | |
ThermoPhase * | m_phase |
Pointer to the ThermoPhase object used to initialize this object. | |
size_t | m_mm |
number of elements in the phase | |
size_t | m_kk |
number of species in the phase | |
size_t | m_skip = npos |
size_t | m_nComponents |
This is equal to the rank of the stoichiometric coefficient matrix when it is computed. | |
function< double(ThermoPhase &)> | m_p1 |
function< double(ThermoPhase &)> | m_p2 |
vector< double > | m_molefractions |
Current value of the mole fractions in the single phase. length = m_kk. | |
double | m_elementTotalSum = 1.0 |
Current value of the sum of the element abundances given the current element potentials. | |
vector< double > | m_elementmolefracs |
Current value of the element mole fractions. | |
vector< double > | m_reswork |
vector< double > | m_jwork1 |
vector< double > | m_jwork2 |
vector< double > | m_comp |
Storage of the element compositions. natom(k,m) = m_comp[k*m_mm+ m];. | |
double | m_temp |
double | m_dens |
double | m_p0 = OneAtm |
size_t | m_eloc = npos |
Index of the element id corresponding to the electric charge of each species. | |
vector< double > | m_startSoln |
vector< double > | m_grt |
vector< double > | m_mu_RT |
vector< double > | m_muSS_RT |
Dimensionless values of the Gibbs free energy for the standard state of each species, at the temperature and pressure of the solution (the star standard state). | |
vector< size_t > | m_component |
double | m_elemFracCutoff = 1e-100 |
element fractional cutoff, below which the element will be zeroed. | |
bool | m_doResPerturb = false |
vector< size_t > | m_orderVectorElements |
vector< size_t > | m_orderVectorSpecies |
int | m_loglevel |
Verbosity of printed output. | |
ChemEquil | ( | ThermoPhase & | s | ) |
Constructor combined with the initialization function.
This constructor initializes the ChemEquil object with everything it needs to start solving equilibrium problems.
s | ThermoPhase object that will be used in the equilibrium calls. |
Definition at line 43 of file ChemEquil.cpp.
int equilibrate | ( | ThermoPhase & | s, |
const char * | XY, | ||
int | loglevel = 0 |
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Equilibrate a phase, holding the elemental composition fixed at the initial value found within the ThermoPhase object s.
The value of two specified properties are obtained by querying the ThermoPhase object. The properties must be already contained within the current thermodynamic state of the system.
Definition at line 293 of file ChemEquil.cpp.
int equilibrate | ( | ThermoPhase & | s, |
const char * | XY, | ||
vector< double > & | elMoles, | ||
int | loglevel = 0 |
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Compute the equilibrium composition for two specified properties and the specified element moles.
The two specified properties are obtained by querying the ThermoPhase object. The properties must be already contained within the current thermodynamic state of the system.
s | phase object to be equilibrated |
XY | property pair to hold constant |
elMoles | specified vector of element abundances. |
loglevel | Specify amount of debug logging (0 to disable) |
Definition at line 301 of file ChemEquil.cpp.
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number of atoms of element m in species k.
Definition at line 139 of file ChemEquil.h.
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Prepare for equilibrium calculations.
s | object representing the solution phase. |
Definition at line 48 of file ChemEquil.cpp.
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Set mixture to an equilibrium state consistent with specified element potentials and temperature.
s | mixture to be updated |
x | vector of non-dimensional element potentials \[ \lambda_m/RT \] . |
t | temperature in K. |
Definition at line 116 of file ChemEquil.cpp.
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Estimate the initial mole numbers.
This version borrows from the MultiPhaseEquil solver.
Definition at line 166 of file ChemEquil.cpp.
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Generate a starting estimate for the element potentials.
Definition at line 201 of file ChemEquil.cpp.
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Do a calculation of the element potentials using the Brinkley method, p.
129 Smith and Missen [40].
We have found that the previous estimate may not be good enough to avoid drastic numerical issues associated with the use of a numerically generated Jacobian used in the main algorithm.
The Brinkley algorithm, here, assumes a constant T, P system and uses a linearized analytical Jacobian that turns out to be very stable even given bad initial guesses.
The pressure and temperature to be used are in the ThermoPhase object input into the routine.
The initial guess for the element potentials used by this routine is taken from the input vector, x.
elMoles is the input element abundance vector to be matched.
Nonideal phases are handled in principle. This is done by calculating the activity coefficients and adding them into the formula in the correct position. However, these are treated as a RHS contribution only. Therefore, convergence might be a problem. This has not been tested. Also molality based unit systems aren't handled.
On return, int return value contains the success code:
NOTE: update for activity coefficients.
Definition at line 828 of file ChemEquil.cpp.
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Find an acceptable step size and take it.
The original implementation employed a line search technique that enforced a reduction in the norm of the residual at every successful step. Unfortunately, this method created false convergence errors near the end of a significant number of steps, usually special conditions where there were stoichiometric constraints.
This new method just does a delta damping approach, based on limiting the jump in the dimensionless element potentials. Mole fractions are limited to a factor of 2 jump in the values from this method. Near convergence, the delta damping gets out of the way.
Definition at line 674 of file ChemEquil.cpp.
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Evaluates the residual vector F, of length m_mm.
Definition at line 713 of file ChemEquil.cpp.
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Definition at line 759 of file ChemEquil.cpp.
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Definition at line 1297 of file ChemEquil.cpp.
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Update internally stored state information.
Definition at line 137 of file ChemEquil.cpp.
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Given a vector of dimensionless element abundances, this routine calculates the moles of the elements and the moles of the species.
s | ThermoPhase object | |
[in] | x | current dimensionless element potentials |
[in] | Xmol_i_calc | Mole fractions of the species |
[in] | pressureConst | Pressure |
Definition at line 792 of file ChemEquil.cpp.
EquilOpt options |
Options controlling how the calculation is carried out.
Definition at line 127 of file ChemEquil.h.
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Pointer to the ThermoPhase object used to initialize this object.
This ThermoPhase object must be compatible with the ThermoPhase objects input from the equilibrate function. Currently, this means that the 2 ThermoPhases have to have consist of the same species and elements.
Definition at line 136 of file ChemEquil.h.
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number of elements in the phase
Definition at line 251 of file ChemEquil.h.
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number of species in the phase
Definition at line 252 of file ChemEquil.h.
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Definition at line 253 of file ChemEquil.h.
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This is equal to the rank of the stoichiometric coefficient matrix when it is computed.
It's initialized to m_mm.
Definition at line 257 of file ChemEquil.h.
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Definition at line 259 of file ChemEquil.h.
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Definition at line 259 of file ChemEquil.h.
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Current value of the mole fractions in the single phase. length = m_kk.
Definition at line 262 of file ChemEquil.h.
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Current value of the sum of the element abundances given the current element potentials.
Definition at line 266 of file ChemEquil.h.
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Current value of the element mole fractions.
Note these aren't the goal element mole fractions.
Definition at line 270 of file ChemEquil.h.
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Definition at line 271 of file ChemEquil.h.
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Definition at line 272 of file ChemEquil.h.
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Definition at line 273 of file ChemEquil.h.
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Storage of the element compositions. natom(k,m) = m_comp[k*m_mm+ m];.
Definition at line 276 of file ChemEquil.h.
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Definition at line 277 of file ChemEquil.h.
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Definition at line 277 of file ChemEquil.h.
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Definition at line 278 of file ChemEquil.h.
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Index of the element id corresponding to the electric charge of each species.
Equal to -1 if there is no such element id.
Definition at line 282 of file ChemEquil.h.
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Definition at line 284 of file ChemEquil.h.
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Definition at line 286 of file ChemEquil.h.
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Definition at line 287 of file ChemEquil.h.
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Dimensionless values of the Gibbs free energy for the standard state of each species, at the temperature and pressure of the solution (the star standard state).
Definition at line 292 of file ChemEquil.h.
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Definition at line 293 of file ChemEquil.h.
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element fractional cutoff, below which the element will be zeroed.
Definition at line 296 of file ChemEquil.h.
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Definition at line 297 of file ChemEquil.h.
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Definition at line 299 of file ChemEquil.h.
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Definition at line 300 of file ChemEquil.h.
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Verbosity of printed output.
No messages when m_loglevel == 0. More output as level increases.
Definition at line 304 of file ChemEquil.h.