4984 lines
158 KiB
C++
4984 lines
158 KiB
C++
/*!
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* @file vcs_solve_TP.cpp Implementation file that contains the
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* main algorithm for finding an equilibrium
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*/
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/*
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* $Id$
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*/
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/*
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* Copywrite (2005) Sandia Corporation. Under the terms of
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* Contract DE-AC04-94AL85000 with Sandia Corporation, the
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* U.S. Government retains certain rights in this software.
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*/
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#include <cstdio>
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#include <cstdlib>
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#include <cmath>
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#include "vcs_solve.h"
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#include "vcs_internal.h"
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#include "vcs_VolPhase.h"
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#include "vcs_species_thermo.h"
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namespace VCSnonideal {
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/*****************************************************************************/
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/************ Prototypes for static functions ********************************/
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static void print_space(int num);
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#ifdef DEBUG
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//static double minor_alt_calc(int, int, int *, char *);
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#else
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//static double minor_alt_calc(int, int, int *);
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#endif
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#ifdef DEBUG
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# ifdef DEBUG_MORE
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static void prneav(void);
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static int prnfm(void);
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# endif
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#endif
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/*****************************************************************************/
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/*****************************************************************************/
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/*****************************************************************************/
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#ifdef DEBUG
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void VCS_SOLVE::checkDelta1(double * const ds,
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double * const delTPhMoles, int kspec) {
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std::vector<double> dchange(NPhase, 0.0);
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for (int k = 0; k < kspec; k++) {
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if (SpeciesUnknownType[k] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
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int iph = PhaseID[k];
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dchange[iph] += ds[k];
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}
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}
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for (int iphase = 0; iphase < NPhase; iphase++) {
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double denom = MAX(TMoles, 1.0E-4);
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if (!vcs_doubleEqual(dchange[iphase]/denom, delTPhMoles[iphase]/denom)) {
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plogf("checkDelta1: we have found a problem\n");
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exit(-1);
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}
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}
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}
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#endif
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/*****************************************************************************/
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/*****************************************************************************/
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/*****************************************************************************/
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int VCS_SOLVE::vcs_solve_TP(int print_lvl, int printDetails, int maxit)
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/**************************************************************************
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*
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* NONIDEAL SYSTEM STOICHIOMETRIC EQUILBRIUM ALGORITHM USING VCS METHOD
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* ----------------------------------------------------------------------
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*
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* Any number of single-species phases and two multi-species phases
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* can be handled by the present version (the latter is readily
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* modified). Phase 1 is nominally a gas, since alog(P) is added to the
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* standard chemical potential data. This can be overridden by
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* setting p = 1. Phase 2 is nominally a liquid, or any phase for
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* which the standard chemical potential data is independent of P.
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* Multi-species phases is deemed to be absent if nt .lt. 1.0E-10.
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* If multi-species phase is absent at equilibrium, dgRT value refers
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* to 1 - sigma(x(I)), where x(I) are virtual mole fractions at the
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* current equilibrium.
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* A linear programming routine must be provided for the initial
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* estimate of the equilibrium composition
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*
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* Input
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* print_lvl = 1 -> Print results to standard output
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* 0 -> don't report on anything
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* printDetails = 1 -> Print intermediate results.
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* MAXIT -> Maximum number of iterations for the algorithm
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*
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* Return Value
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*
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* solveFail = TRUE -> Failure to solve the current problem
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* FALSE -> Normal successful return.
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*
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* Some definitions of variables
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*
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* NL = Number of species in multiphase non-gaseous phases
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* M = Number of species
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* NC = Number of components.
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* NE = Number of elements
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*
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* E(J) = Char*2 name for the Jth element in the mechanism
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*
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* IT = Running count on the number of iterations of the algorithm.
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* ITL = Controls whether the FORCER subroutine is called. TRUE means
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* that FORCER is not called.
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* MajorSpeciesHaveConverged = Indicates convergence amongst
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* major species.
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* -> Also controls whether a new reaction adjustment is requested.
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* IM = IM is true if all noncomponent species are minor or nonexistent
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* NRUNS = number of problems to run
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* M = Number of species
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* NE = Number of elements
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* NS1 = number of single-species phases
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* NL1 = Number of phase2 species
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* IF = Type of chemical potential data: -1 kcal/mol
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* 0 MU/RT
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* 1 kJ/mol
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* IEST = Initial estimate: 0 user estimate
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* -1 machine estimate
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* For each Species:
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* SP = Species name
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* BM = formula vector
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* SI = Type of phase, 0 single-species
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* 1 multi-species gas
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* 2 multi-species liquid
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* FF = Input standard chemical potential
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*
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* E(J) = Char*2 name for the Jth element in the mechanism
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*
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* Return Codes
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* ------------------
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* 0 = Equilibrium Achieved
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* 1 = Range space error encountered. The element abundance criteria are
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* only partially satisfied. Specifically, the first NC= (number of
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* components) conditions are satisfied. However, the full NE
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* (number of elements) conditions are not satisfied. The equilibrirum
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* condition is returned.
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* -1 = Maximum number of iterations is exceeded. Convergence was not
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* found.
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*
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*************************************************************************/
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{
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int conv = FALSE, retn = VCS_SUCCESS;
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double test, RT;
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int j, k, l, solveFail, l1, kspec, irxn, im, forced, iph;
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// double *ss, *sm, *sa, *aw, *wx,
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double dx, xx, par, tsecond;
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int liqphase = FALSE, numSpecliquid = 0;
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int dofast, soldel, ll, it1;
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int lec, npb, iti, i, lnospec;
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int rangeErrorFound = 0;
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bool giveUpOnElemAbund = false;
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int finalElemAbundAttempts = 0;
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bool MajorSpeciesHaveConverged = false;
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int uptodate_minors = TRUE;
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bool justDeletedMultiPhase = FALSE;
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int usedZeroedSpecies; /* return flag from basopt indicating that
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one of the components had a zero concentration */
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vcs_VolPhase *Vphase;
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double *sc_irxn = NULL; /* Stoichiometric coefficients for cur rxn */
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double *dnPhase_irxn;
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#ifdef DEBUG
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char ANOTE[128];
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/*
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* Set the debug print lvl to the same as the print lvl.
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*/
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vcs_debug_print_lvl = printDetails;
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#endif
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if (printDetails > 0 && print_lvl == 0) {
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print_lvl = 1;
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}
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/*
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* Initialize and set up all counters
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*/
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vcs_counters_init(0);
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tsecond = vcs_second();
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/*
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* Malloc temporary space for usage in this routine and in
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* subroutines
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* sm[ne*ne]
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* ss[ne]
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* sa[ne]
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* aw[m]
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* wx[ne]
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* xy[m]
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*/
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std::vector<double> sm(m_numElemConstraints*m_numElemConstraints, 0.0);
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std::vector<double> ss(m_numElemConstraints, 0.0);
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std::vector<double> sa(m_numElemConstraints, 0.0);
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std::vector<double> aw(m_numSpeciesTot, 0.0);
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std::vector<double> wx(m_numElemConstraints, 0.0);
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solveFail = FALSE;
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im = FALSE;
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/* ****************************************************** */
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/* **** Evaluate the elemental composition ****** */
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/* ****************************************************** */
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vcs_elab();
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/* ******************************************************* */
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/* **** Printout the initial conditions for problem ****** */
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/* ******************************************************* */
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if (NPhase > 1) {
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if (! VPhaseList[1]->SingleSpecies) {
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liqphase = TRUE;
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numSpecliquid = VPhaseList[1]->NVolSpecies;
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}
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}
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if (print_lvl != 0) {
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plogf("VCS CALCULATION METHOD\n\n ");
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plogf("%s\n", Title.c_str());
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plogf("\n\n%5d SPECIES%8d ELEMENTS", m_numSpeciesTot, m_numElemConstraints);
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plogf("%16d COMPONENTS\n%5d PHASE1 SPECIES", m_numComponents,
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((VPhaseList[0])->NVolSpecies));
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plogf("%10d PHASE2 SPECIES%8d SINGLE SPECIES PHASES\n\n",
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numSpecliquid,
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m_numSpeciesTot - (VPhaseList[0])->NVolSpecies - numSpecliquid);
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plogf(" PRESSURE%22.3f ATM\n TEMPERATURE%19.3f K\n",
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Pres, T);
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Vphase = VPhaseList[0];
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if (Vphase->NVolSpecies > 0) {
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plogf(" PHASE1 INERTS%17.3f\n", TPhInertMoles[0]);
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}
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if (liqphase) {
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plogf(" PHASE2 INERTS%17.3f\n", TPhInertMoles[1]);
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}
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plogf("\n ELEMENTAL ABUNDANCES CORRECT");
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plogf(" FROM ESTIMATE Type\n\n");
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for (i = 0; i < m_numElemConstraints; ++i) {
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print_space(26); plogf("%-2.2s", (ElName[i]).c_str());
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plogf("%20.12E%20.12E %3d\n", gai[i], ga[i], m_elType[i]);
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}
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if (iest < 0) {
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plogf("\n MODIFIED LINEAR PROGRAMMING ESTIMATE OF EQUILIBRIUM\n");
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}
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if (iest >= 0) {
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plogf("\n USER ESTIMATE OF EQUILIBRIUM\n");
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}
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if (m_VCS_UnitsFormat == VCS_UNITS_KCALMOL) {
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plogf(" Stan. Chem. Pot. in kcal/mole\n");
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}
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if (m_VCS_UnitsFormat == VCS_UNITS_UNITLESS) {
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plogf(" Stan. Chem. Pot. is MU/RT\n");
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}
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if (m_VCS_UnitsFormat == VCS_UNITS_KJMOL) {
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plogf(" Stan. Chem. Pot. in KJ/mole\n");
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}
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if (m_VCS_UnitsFormat == VCS_UNITS_KELVIN) {
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plogf(" Stan. Chem. Pot. in Kelvin\n");
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}
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if (m_VCS_UnitsFormat == VCS_UNITS_MKS) {
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plogf(" Stan. Chem. Pot. in J/kmol\n");
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}
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plogf("\n SPECIES FORMULA VECTOR");
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print_space(29);
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plogf(" STAN_CHEM_POT EQUILIBRIUM_EST. Species_Type\n\n");
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print_space(14);
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for (i = 0; i < m_numElemConstraints; ++i) plogf(" %-2.2s", ElName[i].c_str());
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plogf(" SI(I)\n");
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RT = vcs_nondimMult_TP(m_VCS_UnitsFormat, T);
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for (i = 0; i < m_numSpeciesTot; ++i) {
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plogf(" %-12s", SpName[i].c_str());
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for (j = 0; j < m_numElemConstraints; ++j) {
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plogf("%3g", FormulaMatrix[j][i]);
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}
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if (PhaseID[i] == 0) {
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plogf(" 1");
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} else if (PhaseID[i] == 1) {
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if (liqphase) plogf(" 2");
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else plogf(" 0");
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} else {
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plogf(" 0");
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}
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print_space(47-m_numElemConstraints*3);
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plogf("%12.5E %12.5E", RT * ff[i], soln[i]);
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if (SpeciesUnknownType[i] == VCS_SPECIES_TYPE_MOLNUM) {
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plogf(" Mol_Num");
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} else if (SpeciesUnknownType[i] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
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plogf(" Voltage");
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} else {
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plogf(" Unknown");
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}
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plogf(" \n");
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}
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}
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for (i = 0; i < m_numSpeciesTot; ++i) {
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if (soln[i] < 0.0) {
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plogf("On Input species %-12s has a "
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"negative MF, setting it small\n",
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SpName[i].c_str());
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soln[i] = VCS_DELETE_SPECIES_CUTOFF;
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}
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}
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/* *********************************************** */
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/* **** EVALUATE TOTAL MOLES, GAS AND LIQUID ***** */
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/* *********************************************** */
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/* - Evaluate the total moles of gas and liquid */
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/* - These quantities are storred in the global variables */
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vcs_tmoles();
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/* ******************************************* */
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/* **** EVALUATE ALL CHEMICAL POTENTIALS ***** */
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/* ******************************************* */
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vcs_dfe(VCS_DATA_PTR(soln), 0, 0, 0, m_numSpeciesRdc);
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/*
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* HKM -> If there was a machine estimate, we used to branch
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* to the code segment which determined whether we needed a
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* new component basis. If we did, we would go to L429.
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* If we didn't, we would go to a point below basopt() below.
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* I have taken this section out of the code for simplicity's
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* sake. It's not need for speed, since in any recursive
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* call to this subroutine we would have an initial estimate
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* of the solution. And, we don't need to optimize the
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* startup of nonrecursive calls to this subroutine.
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*/
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/* *********************************************************** */
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/* **** DETERMINE BASIS SPECIES, EVALUATE STOICHIOMETRY ****** */
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/* *********************************************************** */
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/*
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* This is an entry point for later in the calculation
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*/
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L_COMPONENT_CALC: ;
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test = -1.0e-10;
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retn = vcs_basopt(FALSE, VCS_DATA_PTR(aw), VCS_DATA_PTR(sa),
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VCS_DATA_PTR(sm), VCS_DATA_PTR(ss),
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test, &usedZeroedSpecies);
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if (retn != VCS_SUCCESS) return retn;
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if (conv) {
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goto L_RETURN_BLOCK;
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}
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it1 = 1;
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MajorSpeciesHaveConverged = false;
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/*************************************************************************/
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/************** EVALUATE INITIAL MAJOR-MINOR VECTOR **********************/
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/*************************************************************************/
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m_numRxnMinorZeroed = 0;
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for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
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kspec = ir[irxn];
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spStatus[irxn] = vcs_species_type(kspec);
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if (spStatus[irxn] == VCS_SPECIES_MINOR) {
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spStatus[irxn] = VCS_SPECIES_MAJOR;
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#ifdef DEBUG
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if (vcs_debug_print_lvl >= 2) {
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plogf(" --- Minor species changed to major: ");
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plogf("%-12s\n", SpName[kspec].c_str());
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}
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#endif
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}
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if (spStatus[irxn] != VCS_SPECIES_MAJOR) {
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++m_numRxnMinorZeroed;
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}
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}
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im = (m_numRxnMinorZeroed == m_numRxnRdc);
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lec = FALSE;
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if (! vcs_elabcheck(0)) {
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#ifdef DEBUG
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if (vcs_debug_print_lvl >= 2) {
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plogf(" --- Element Abundance check failed\n");
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}
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#endif
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vcs_elcorr(VCS_DATA_PTR(sm), VCS_DATA_PTR(wx));
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vcs_dfe(VCS_DATA_PTR(soln), 0, 0, 0, m_numSpeciesRdc);
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}
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#ifdef DEBUG
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else {
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if (vcs_debug_print_lvl >= 2) {
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plogf(" --- Element Abundance check passed\n");
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}
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}
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#endif
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// Update the phase objects with the contents of the soln vector
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vcs_updateVP(0);
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vcs_deltag(0, false);
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iti = 0;
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goto L_MAINLOOP_ALL_SPECIES;
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/* ********************************************************* */
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/* **** SET INITIAL VALUES FOR ITERATION ******************* */
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/* **** EVALUATE REACTION ADJUSTMENTS ******************* */
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/* ********************************************************* */
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/*
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* This is the top of the loop ----------------------------------------
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* Every 4th iteration ITI = 0. Else, It's equal to a negative number
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*/
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L_MAINLOOP_MM4_SPECIES: ;
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iti = ((it1/4) *4) - it1;
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/*
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* Entry point when the code wants to force an ITI=0 calculation
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*/
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L_MAINLOOP_ALL_SPECIES: ;
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if (iti == 0) {
|
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/*
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* Evaluate the minor non-componenent species chemical
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* potentials and delta G for their formation reactions
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* We have already evaluated the major non-components
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*/
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if (uptodate_minors == FALSE) {
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vcs_dfe(VCS_DATA_PTR(soln), 0, 1, 0, m_numSpeciesRdc);
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vcs_deltag(1, false);
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}
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uptodate_minors = TRUE;
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} else {
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uptodate_minors = FALSE;
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}
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|
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if (printDetails) {
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plogf("\n"); vcs_print_line("=", 110);
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plogf(" Iteration = %3d, Iterations since last evaluation of "
|
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"optimal basis = %3d",
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m_VCount->Its, it1 - 1);
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if (iti == 0) {
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plogf(" (all species)\n");
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} else {
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plogf(" (only major species)\n");
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}
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}
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|
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vcs_dcopy(VCS_DATA_PTR(fel), VCS_DATA_PTR(m_gibbsSpecies), m_numSpeciesRdc);
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vcs_dcopy(VCS_DATA_PTR(feTrial), VCS_DATA_PTR(m_gibbsSpecies), m_numSpeciesRdc);
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vcs_dcopy(VCS_DATA_PTR(ActCoeff0), VCS_DATA_PTR(ActCoeff), m_numSpeciesRdc);
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vcs_dcopy(VCS_DATA_PTR(dgl), VCS_DATA_PTR(dg), m_numRxnRdc);
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|
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/* Go find a new reaction adjustment ->
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* i.e., change in extent of reaction for each reaction.
|
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*
|
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* Zero out the entire vector of updates. We sometimes would
|
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* query these values below, and we want to be sure that no
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* information is left from previous iterations.
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*/
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vcs_dzero(VCS_DATA_PTR(ds), m_numSpeciesTot);
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/*
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* Figure out whether we will calculate new reaction step sizes
|
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* for the major species.
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* -> We won't if all species are minors (im), OR
|
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* all major species have already converged
|
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*/
|
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if (!(MajorSpeciesHaveConverged) && ! im) {
|
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soldel = vcs_RxnStepSizes();
|
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/* - If SOLDEL is true then we encountered a reaction between */
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/* - single-species-phase species, only, and have adjusted */
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|
/* - the mole number vector, W(), directly. In this case, */
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/* - we should immediately go back and recompute a new */
|
|
/* - component basis, if the species that was zeroed was */
|
|
/* - a component. SOLDEL is true when this is so. */
|
|
if (soldel > 0) {
|
|
/* - We have changed the base mole number amongst single- */
|
|
/* - species-phase species. However, we don't need to */
|
|
/* - recaculate their chemical potentials because they */
|
|
/* - are constant, anyway! */
|
|
if (soldel == 2) {
|
|
goto L_COMPONENT_CALC;
|
|
}
|
|
/* - We have not changed the actual DG values for */
|
|
/* - any species, even the one we deleted. Thus, */
|
|
/* - we don't need to start over. */
|
|
}
|
|
} else {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
if (im) {
|
|
plogf(" --- vcs_RxnStepSizes not called because all"
|
|
"species are minors\n");
|
|
} else {
|
|
plogf(" --- vcs_RxnStepSizes not called because "
|
|
"all majors have converged\n");
|
|
}
|
|
}
|
|
#endif
|
|
}
|
|
|
|
lec = FALSE;
|
|
/*
|
|
* Zero out the net change in moles of multispecies phases
|
|
*/
|
|
vcs_dzero(VCS_DATA_PTR(DelTPhMoles), NPhase);
|
|
/* **************************************************************** */
|
|
/* ***************** MAIN LOOP IN CALCULATION ******************** */
|
|
/* **************************************************************** */
|
|
/*
|
|
* Loop through all of the reactions, irxn, pertaining to the
|
|
* formation reaction for species kspec in canonical form.
|
|
*
|
|
* At the end of this loop, we will have a new estimate for the
|
|
* mole numbers wt[kspec] for all species consistent with an extent
|
|
* of reaction, ds[kspec] for all noncomponent species formation
|
|
* reactions. We will have also ensured that all predicted
|
|
* non-component mole numbers are greater than zero.
|
|
*/
|
|
if (m_VCount->Its > maxit) {
|
|
solveFail = -1;
|
|
/*
|
|
* Clean up and exit code even though we haven't
|
|
* converged. -> we have run out of iterations!
|
|
*/
|
|
goto L_RETURN_BLOCK;
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Main Loop Treatment of each non-component species ");
|
|
if (iti == 0) plogf("- Full Calculation:\n");
|
|
else plogf("- Major Components Calculation:\n");
|
|
plogf(" --- Species IC ");
|
|
plogf(" Moles Tent_Moles Rxn_Adj | Comment \n");
|
|
}
|
|
#endif
|
|
|
|
for (irxn = 0; irxn < m_numRxnRdc; irxn++) {
|
|
kspec = ir[irxn];
|
|
sc_irxn = sc[irxn];
|
|
iph = PhaseID[kspec];
|
|
Vphase = VPhaseList[iph];
|
|
#ifdef DEBUG
|
|
ANOTE[0] = '\0';
|
|
#endif
|
|
/********************************************************************/
|
|
/********************** VOLTAGE SPECIES **************************/
|
|
/********************************************************************/
|
|
if (spStatus[irxn] == VCS_SPECIES_INTERFACIALVOLTAGE) {
|
|
#ifdef DEBUG
|
|
dx = minor_alt_calc(kspec, irxn, &soldel, ANOTE);
|
|
#else
|
|
dx = minor_alt_calc(kspec, irxn, &soldel);
|
|
#endif
|
|
ds[kspec] = dx;
|
|
}
|
|
else if (spStatus[irxn] < VCS_SPECIES_MINOR) {
|
|
|
|
/********************************************************************/
|
|
/********************** ZEROED OUT SPECIES **************************/
|
|
/********************************************************************/
|
|
bool resurrect = true;
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 3) {
|
|
plogf(" --- %s currently zeroed (SpStatus=%-2d):",
|
|
SpName[kspec].c_str(), spStatus[irxn]);
|
|
plogf("%3d DG = %11.4E WT = %11.4E W = %11.4E DS = %11.4E\n",
|
|
irxn, dg[irxn], wt[kspec], soln[kspec], ds[kspec]);
|
|
}
|
|
#endif
|
|
// HKM Alternative is to not allow ds[] = 0.0 phases
|
|
// to pop back into existence. For esthetics, I'm allowing this.
|
|
// so that dg < 0.0 phases with zero mole numbers become components.
|
|
// This is also better, because that component will be the first
|
|
// one to pop into existence if there is a minute quantity of the element.
|
|
// This could change in the future.
|
|
//if (dg[irxn] >= 0.0 || ds[kspec] <= 0.0) {
|
|
if (dg[irxn] >= 0.0 ) {
|
|
wt[kspec] = soln[kspec];
|
|
ds[kspec] = 0.0;
|
|
resurrect = false;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "Species stays zeroed: DG = %11.4E",
|
|
dg[irxn]);
|
|
if (dg[irxn] < 0.0) {
|
|
sprintf(ANOTE, "Species stays zeroed even though dg neg:DG = %11.4E, ds zeroed ",
|
|
dg[irxn]);
|
|
}
|
|
//if (vcs_debug_print_lvl >= 2) {
|
|
//plogf(" --- "); plogf("%-12s", SpName[kspec]);
|
|
//plogf("%3d%11.4E%11.4E%11.4E | %s\n",
|
|
// spStatus[irxn], w[kspec], wt[kspec],
|
|
// ds[kspec], ANOTE);
|
|
//}
|
|
#endif
|
|
} else {
|
|
for (int j = 0; j < m_numElemConstraints; ++j) {
|
|
int elType = m_elType[j];
|
|
if (elType == VCS_ELEM_TYPE_ABSPOS) {
|
|
double atomComp = FormulaMatrix[j][kspec];
|
|
if (atomComp > 0.0) {
|
|
double maxPermissible = gai[j] / atomComp;
|
|
if (maxPermissible < VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "Species stays zeroed even though dG neg, because of %s elemAbund",
|
|
ElName[j].c_str());
|
|
#endif
|
|
resurrect = false;
|
|
break;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* Resurrect the species
|
|
*/
|
|
if (resurrect) {
|
|
if (Vphase->Existence == 0) Vphase->Existence = 1;
|
|
--m_numRxnMinorZeroed;
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Zeroed species changed to major: ");
|
|
plogf("%-12s\n", SpName[kspec].c_str());
|
|
}
|
|
#endif
|
|
spStatus[irxn] = VCS_SPECIES_MAJOR;
|
|
im = FALSE;
|
|
MajorSpeciesHaveConverged = false;
|
|
if (ds[kspec] > 0.0) {
|
|
dx = ds[kspec] * 0.01;
|
|
|
|
wt[kspec] = soln[kspec] + dx;
|
|
} else {
|
|
wt[kspec] = TMoles * VCS_DELETE_PHASE_CUTOFF * 10.;
|
|
dx = wt[kspec] - soln[kspec];
|
|
}
|
|
ds[kspec] = dx;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "Born:IC=-1 to IC=1:DG=%11.4E", dg[irxn]);
|
|
#endif
|
|
} else {
|
|
wt[kspec] = soln[kspec];
|
|
ds[kspec] = 0.0;
|
|
dx = 0.0;
|
|
}
|
|
} else if (spStatus[irxn] == VCS_SPECIES_MINOR) {
|
|
/********************************************************************/
|
|
/***************************** MINOR SPECIES ************************/
|
|
/********************************************************************/
|
|
/*
|
|
* Unless ITI isn't equal to zero we zero out changes
|
|
* to minor species.
|
|
*/
|
|
if (iti != 0) {
|
|
wt[kspec] = soln[kspec];
|
|
ds[kspec] = 0.0;
|
|
dx = 0.0;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,"minor species not considered");
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- "); plogf("%-12s", SpName[kspec].c_str());
|
|
plogf("%3d%11.4E%11.4E%11.4E | %s\n",
|
|
spStatus[irxn], soln[kspec], wt[kspec],
|
|
ds[kspec], ANOTE);
|
|
}
|
|
#endif
|
|
continue;
|
|
}
|
|
/*
|
|
* Minor species alternative calculation
|
|
* ---------------------------------------
|
|
* This is based upon the following approximation:
|
|
* The mole fraction changes due to these reactions don't affect
|
|
* the mole numbers of the component species. Therefore the
|
|
* following approximation is valid for an ideal solution
|
|
* 0 = DG(I) + log(WT(I)/W(I))
|
|
* (DG contains the contribution from FF(I) + log(W(I)/TL) )
|
|
* Thus,
|
|
* WT(I) = W(I) EXP(-DG(I))
|
|
* If soldel is true on return, then we branch to the section
|
|
* that deletes a species from the current set of active species.
|
|
*/
|
|
#ifdef DEBUG
|
|
dx = minor_alt_calc(kspec, irxn, &soldel, ANOTE);
|
|
#else
|
|
dx = minor_alt_calc(kspec, irxn, &soldel);
|
|
#endif
|
|
ds[kspec] = dx;
|
|
if (soldel) {
|
|
/*******************************************************************/
|
|
/***** DELETE MINOR SPECIES LESS THAN VCS_DELETE_SPECIES_CUTOFF */
|
|
/***** MOLE NUMBER */
|
|
/*******************************************************************/
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Delete minor species in multispec phase: %-12s\n",
|
|
SpName[kspec].c_str());
|
|
}
|
|
#endif
|
|
ds[kspec] = 0.0;
|
|
/*
|
|
* Delete species, kspec. The alternate return is for the case
|
|
* where all species become deleted. Then, we need to
|
|
* branch to the code where we reevaluate the deletion
|
|
* of all species.
|
|
*/
|
|
lnospec = delete_species(kspec);
|
|
if (lnospec) goto L_RECHECK_DELETED;
|
|
/*
|
|
* Go back to consider the next species in the list.
|
|
* Note, however, that the next species in the list is now
|
|
* in slot l. In deleting the previous species L, We have
|
|
* exchanged slot MR with slot l, and then have
|
|
* decremented MR.
|
|
* Therefore, we will decrement the species counter, here.
|
|
*/
|
|
--irxn;
|
|
#ifdef DEBUG
|
|
goto L_MAIN_LOOP_END_NO_PRINT;
|
|
#else
|
|
goto L_MAIN_LOOP_END;
|
|
#endif
|
|
}
|
|
} else {
|
|
/********************************************************************/
|
|
/*********************** MAJOR SPECIES ******************************/
|
|
/********************************************************************/
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "Normal Major Calc");
|
|
#endif
|
|
/*
|
|
* Check for superconvergence of the formation reaction. Do
|
|
* nothing if it is superconverged. Skip to the end of the
|
|
* irxn loop if it is superconverged.
|
|
*/
|
|
if (fabs(dg[irxn]) <= tolmaj2) {
|
|
wt[kspec] = soln[kspec];
|
|
ds[kspec] = 0.0;
|
|
dx = 0.0;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "major species is converged");
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- "); plogf("%-12s", SpName[kspec].c_str());
|
|
plogf("%3d%11.4E%11.4E%11.4E | %s\n",
|
|
spStatus[irxn], soln[kspec], wt[kspec],
|
|
ds[kspec], ANOTE);
|
|
}
|
|
#endif
|
|
continue;
|
|
}
|
|
/*
|
|
* Set the initial step size, dx, equal to the value produced
|
|
* by the routine, vcs_RxnStepSize().
|
|
*
|
|
* Note the multiplition logic is to make sure that
|
|
* dg[] didn't change sign due to w[] changing in the
|
|
* middle of the iteration. (it can if a single species
|
|
* phase goes out of existence).
|
|
*/
|
|
if ((dg[irxn] * ds[kspec]) <= 0.0) {
|
|
dx = ds[kspec];
|
|
} else {
|
|
dx = 0.0;
|
|
ds[kspec] = 0.0;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "dx set to 0, DG flipped sign due to "
|
|
"changed initial point");
|
|
#endif
|
|
}
|
|
/*
|
|
* Form a tentative value of the new species moles
|
|
*/
|
|
wt[kspec] = soln[kspec] + dx;
|
|
/*
|
|
* Check for non-positive mole fraction of major species.
|
|
* If we find one, we branch to a section below. Then,
|
|
* depending upon the outcome, we branch to sections below,
|
|
* or we restart the entire iteration.
|
|
*/
|
|
if (wt[kspec] <= 0.0) {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "initial nonpos moles= %11.3E",
|
|
wt[kspec]);
|
|
#endif
|
|
/* ************************************************* */
|
|
/* *** NON-POSITIVE MOLES OF MAJOR SPECIES ********* */
|
|
/* ************************************************* */
|
|
/*
|
|
* We are here when a tentative value of a mole fraction
|
|
* created by a tentative value of DS(*) is negative.
|
|
* We branch from here depending upon whether this
|
|
* species is in a single species phase or in
|
|
* a multispecies phase.
|
|
*/
|
|
if (! (SSPhase[kspec])) {
|
|
/*
|
|
* Section for multispecies phases:
|
|
* - Cut reaction adjustment for positive moles of
|
|
* major species in multispecies phases.
|
|
* Decrease its concentration by a factor of 10.
|
|
*/
|
|
dx = -0.9 * soln[kspec];
|
|
ds[kspec] = dx;
|
|
wt[kspec] = soln[kspec] + dx;
|
|
/*
|
|
* Change major to minor if the current species
|
|
* has a mole number that is less than 1/100 of the
|
|
* total moles in the problem.
|
|
* However, it also has to be a small species within its
|
|
* own phase as well.
|
|
* we can't call vcs_species_type() because the phase moles
|
|
* would be wrong.
|
|
*/
|
|
if (wt[kspec] < 0.005 * TMoles) {
|
|
iph = PhaseID[kspec];
|
|
if (wt[kspec] < (TPhMoles[iph] * 0.01)) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Major species changed to minor: ");
|
|
plogf("%-12s\n", SpName[kspec].c_str());
|
|
}
|
|
#endif
|
|
spStatus[irxn] = VCS_SPECIES_MINOR;
|
|
++m_numRxnMinorZeroed;
|
|
im = (m_numRxnMinorZeroed == m_numRxnRdc);
|
|
}
|
|
}
|
|
} else {
|
|
/*
|
|
* Section for single species phases:
|
|
* Calculate a dx that will wipe out the
|
|
* moles in the phase.
|
|
*/
|
|
dx = -soln[kspec];
|
|
/*
|
|
* Calculate an update that doesn't create a negative mole
|
|
* number for a component species. Actually, restrict this
|
|
* a little more so that the component values can only be
|
|
* reduced by two 99%,
|
|
*/
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
if (sc_irxn[j] != 0.0) {
|
|
wx[j] = soln[j] + sc_irxn[j] * dx;
|
|
if (wx[j] <= soln[j] * 0.01 - 1.0E-150) {
|
|
dx = MAX(dx, soln[j] * -0.99 / sc_irxn[j]);
|
|
}
|
|
} else {
|
|
wx[j] = soln[j];
|
|
}
|
|
}
|
|
wt[kspec] = soln[kspec] + dx;
|
|
if (wt[kspec] > 0.0) {
|
|
ds[kspec] = dx;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,
|
|
"zeroing SS phase created a neg component species "
|
|
"-> reducing step size instead");
|
|
#endif
|
|
} else {
|
|
/*
|
|
* We are going to zero the single species phase.
|
|
* Set the existence flag
|
|
*/
|
|
iph = PhaseID[kspec];
|
|
Vphase = VPhaseList[iph];
|
|
Vphase->Existence = 0;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "zero SS phase: moles went neg");
|
|
#endif
|
|
/*
|
|
* Change the base mole numbers for the iteration.
|
|
* We need to do this here, because we have decided
|
|
* to eliminate the phase in this special section
|
|
* outside the main loop.
|
|
*/
|
|
soln[kspec] = 0.0;
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
soln[j] = wx[j];
|
|
}
|
|
/*
|
|
* Change the total number of moles in all phases due to
|
|
* the reaction that wil be zeroing out the pure species
|
|
* phase. Make sure the moles in the current ss phase is
|
|
* identically zero.
|
|
*/
|
|
dnPhase_irxn = DnPhase[irxn];
|
|
for (int iphase = 0; iphase < NPhase; iphase++) {
|
|
TPhMoles[iphase] += dnPhase_irxn[iphase] * dx;
|
|
}
|
|
TPhMoles[iph] = 0.0;
|
|
vcs_updateVP(0);
|
|
/*
|
|
* Recalcuate the chemical potentials, FE(), and the
|
|
* reaction free energy changes, DG(), for the current
|
|
* set of reactions being considered. The set of reactions
|
|
* is determined by the value of iti.
|
|
*/
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, iti, 0, m_numSpeciesRdc);
|
|
vcs_deltag(iti, false);
|
|
/*
|
|
* Redefine the starting conditions for noncomponents
|
|
* which have yet to be processed in the main loop
|
|
*/
|
|
for (ll = kspec+1; ll < m_numSpeciesRdc; ++ll) {
|
|
fel[ll] = m_gibbsSpecies[ll];
|
|
}
|
|
for (ll = irxn+1; ll < m_numRxnRdc; ++ll) {
|
|
dgl[ll] = dg[ll];
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
if (spStatus[irxn] >= 0) {
|
|
plogf(" --- SS species changed to zeroedss: ");
|
|
plogf("%-12s\n", SpName[kspec].c_str());
|
|
}
|
|
}
|
|
#endif
|
|
spStatus[irxn] = VCS_SPECIES_ZEROEDSS;
|
|
++m_numRxnMinorZeroed;
|
|
im = (m_numRxnMinorZeroed == m_numRxnRdc);
|
|
if (im && iti != 0) {
|
|
goto L_EQUILIB_CHECK;
|
|
}
|
|
wt[kspec] = soln[kspec];
|
|
ds[kspec] = 0.0;
|
|
dx = 0.0;
|
|
}
|
|
}
|
|
}
|
|
/*********************************************************************/
|
|
/*** LINE SEARCH ALGORITHM FOR MAJOR SPECIES IN NON-IDEAL PHASES *****/
|
|
/*********************************************************************/
|
|
/*
|
|
* Skip the line search if we are birthing a species
|
|
*/
|
|
if (dx != 0.0 && (soln[kspec] > 0.0) &&
|
|
(SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE)) {
|
|
double dx_old = dx;
|
|
#ifdef DEBUG
|
|
dx = vcs_line_search(irxn, dx_old, ANOTE);
|
|
#else
|
|
dx = vcs_line_search(irxn, dx_old);
|
|
#endif
|
|
}
|
|
ds[kspec] = dx;
|
|
|
|
} /* End of Loop on ic[irxn] -> the type of species */
|
|
/***********************************************************************/
|
|
/****** CALCULATE MOLE NUMBER CHANGE FOR THE COMPONENT BASIS ***********/
|
|
/***********************************************************************/
|
|
if (dx != 0.0 && (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE)) {
|
|
/*
|
|
* Change the amount of the component compounds according
|
|
* to the reaction delta that we just computed.
|
|
* This should keep the amount of material constant.
|
|
*/
|
|
#ifdef DEBUG
|
|
if (ds[kspec] != dx) {
|
|
plogf("we have a problem!\n");
|
|
exit(-1);
|
|
}
|
|
#endif
|
|
for (k = 0; k < m_numComponents; ++k) {
|
|
ds[k] += sc_irxn[k] * dx;
|
|
}
|
|
/*
|
|
* Calculate the tentative change in the total number of
|
|
* moles in all of the phases
|
|
*/
|
|
|
|
dnPhase_irxn = DnPhase[irxn];
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
DelTPhMoles[iph] += dx * dnPhase_irxn[iph];
|
|
}
|
|
}
|
|
#ifdef DEBUG
|
|
checkDelta1(VCS_DATA_PTR(ds), VCS_DATA_PTR(DelTPhMoles), kspec+1);
|
|
#endif
|
|
/*
|
|
* Branch point for returning -
|
|
*/
|
|
#ifndef DEBUG
|
|
L_MAIN_LOOP_END: ;
|
|
#endif
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
wt[kspec] = soln[kspec] + ds[kspec];
|
|
plogf(" --- "); plogf("%-12.12s", SpName[kspec].c_str());
|
|
plogf("%3d%11.4E%11.4E%11.4E | %s\n",
|
|
spStatus[irxn], soln[kspec], wt[kspec],
|
|
ds[kspec], ANOTE);
|
|
}
|
|
L_MAIN_LOOP_END_NO_PRINT: ;
|
|
#endif
|
|
/**************** END OF MAIN LOOP OVER FORMATION REACTIONS ************/
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
for (k = 0; k < m_numComponents; k++) {
|
|
plogf(" --- "); plogf("%-12.12s", SpName[k].c_str());
|
|
plogf(" c%11.4E%11.4E%11.4E |\n",
|
|
soln[k], soln[k]+ds[k], ds[k]);
|
|
}
|
|
plogf(" "); vcs_print_line("-", 80);
|
|
plogf(" --- Finished Main Loop\n");
|
|
}
|
|
#endif
|
|
/*************************************************************************/
|
|
/*********** LIMIT REDUCTION OF BASIS SPECIES TO 99% *********************/
|
|
/*************************************************************************/
|
|
/*
|
|
* We have a tentative DS(L=1,MR). Now apply other criteria
|
|
* to limit it's magnitude.
|
|
*/
|
|
par = 0.5;
|
|
for (k = 0; k < m_numComponents; ++k) {
|
|
if (soln[k] > 0.0) {
|
|
xx = -ds[k] / soln[k];
|
|
if (par < xx) {
|
|
par = xx;
|
|
#ifdef DEBUG
|
|
ll = k;
|
|
#endif
|
|
}
|
|
} else {
|
|
if (ds[k] < 0.0) {
|
|
/*
|
|
* If we are here, we then do a step which violates element
|
|
* conservation.
|
|
*/
|
|
iph = PhaseID[k];
|
|
DelTPhMoles[iph] -= ds[k];
|
|
ds[k] = 0.0;
|
|
}
|
|
}
|
|
}
|
|
par = 1.0 / par;
|
|
if (par <= 1.01 && par > 0.0) {
|
|
/* Reduce the size of the step by the multiplicative factor, par */
|
|
par *= 0.99;
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Reduction in step size due to component ");
|
|
plogf("%s", SpName[ll].c_str());
|
|
plogf(" going negative = %11.3E\n", par);
|
|
}
|
|
#endif
|
|
for (i = 0; i < m_numSpeciesTot; ++i) {
|
|
ds[i] *= par;
|
|
}
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
DelTPhMoles[iph] *= par;
|
|
}
|
|
} else {
|
|
par = 1.0;
|
|
}
|
|
#ifdef DEBUG
|
|
checkDelta1(VCS_DATA_PTR(ds), VCS_DATA_PTR(DelTPhMoles), m_numSpeciesTot);
|
|
#endif
|
|
|
|
/*
|
|
* Now adjust the wt[kspec]'s so that the reflect the decrease in
|
|
* the overall length of ds[kspec] just calculated. At the end
|
|
* of this section wt[], ds[], tPhMoles, and tPhMoles1 should all be
|
|
* consistent with a new estimate of the state of the system.
|
|
*/
|
|
for (kspec = 0; kspec < m_numSpeciesTot; ++kspec) {
|
|
wt[kspec] = soln[kspec] + ds[kspec];
|
|
if (wt[kspec] < 0.0 && (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE)) {
|
|
plogf("vcs_solve_TP: ERROR on step change wt[%d:%s]: %g < 0.0\n",
|
|
kspec, SpName[kspec].c_str(), wt[kspec]);
|
|
exit(-1);
|
|
}
|
|
}
|
|
|
|
/*
|
|
* Calculate the tentative total mole numbers for each phase
|
|
*/
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
TPhMoles1[iph] = TPhMoles[iph] + DelTPhMoles[iph];
|
|
}
|
|
/*
|
|
* Calculate the new chemical potentials using the tentative
|
|
* solution values. We only calculate a subset of these, because
|
|
* we have only updated a subset of the W().
|
|
*/
|
|
vcs_updateVP(1);
|
|
vcs_dfe(VCS_DATA_PTR(wt), 1, iti, 0, m_numSpeciesTot);
|
|
/*
|
|
* Evaluate DeltaG for all components if ITI=0, and for
|
|
* major components only if ITI NE 0
|
|
*/
|
|
if (iti == 0) vcs_deltag(0, false);
|
|
else vcs_deltag(-1, false);
|
|
|
|
/*
|
|
* Print Intermediate results
|
|
*/
|
|
// HKM Actually always need to calculate this
|
|
// or else nonprintouts get different results and sometimes
|
|
// fail in the line search algorithm -> Why is this?
|
|
vcs_dfe(VCS_DATA_PTR(wt), 1, 1, 0, m_numSpeciesRdc);
|
|
if (printDetails) {
|
|
if (iti != 0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" *** vcs_dfe for printout only:");
|
|
}
|
|
#endif
|
|
vcs_dfe(VCS_DATA_PTR(wt), 1, 1, 0, m_numSpeciesRdc);
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" *** vcs_deltag for printout only:");
|
|
}
|
|
#endif
|
|
vcs_deltag(1, false);
|
|
}
|
|
|
|
plogf(" "); vcs_print_line("-", 103);
|
|
plogf(" --- Summary of the Update ");
|
|
if (iti == 0) {
|
|
plogf(" (all species):\n");
|
|
} else {
|
|
plogf(" (only major species):\n");
|
|
}
|
|
plogf(" --- Species Status Initial_Moles Final_Moles Initial_Mu/RT");
|
|
plogf(" Mu/RT Init_Del_G/RT Delta_G/RT\n");
|
|
for (i = 0; i < m_numComponents; ++i) {
|
|
plogf(" --- %-12.12s", SpName[i].c_str()); plogf(" ");
|
|
plogf("%14.6E%14.6E%14.6E%14.6E\n", soln[i],
|
|
wt[i], fel[i], m_gibbsSpecies[i]);
|
|
}
|
|
for (i = m_numComponents; i < m_numSpeciesRdc; ++i) {
|
|
l1 = i - m_numComponents;
|
|
plogf(" --- %-12.12s", SpName[i].c_str());
|
|
plogf(" %2d %14.6E%14.6E%14.6E%14.6E%14.6E%14.6E\n",
|
|
spStatus[l1], soln[i],
|
|
wt[i], fel[i], m_gibbsSpecies[i],
|
|
dgl[l1], dg[l1]);
|
|
}
|
|
for (kspec = m_numSpeciesRdc; kspec < m_numSpeciesTot; ++kspec) {
|
|
l1 = kspec - m_numComponents;
|
|
plogf(" --- %-12.12s", SpName[kspec].c_str());
|
|
plogf(" %2d %14.6E%14.6E%14.6E%14.6E%14.6E%14.6E\n",
|
|
spStatus[l1], soln[kspec],
|
|
wt[kspec], fel[kspec], m_gibbsSpecies[kspec],
|
|
dgl[l1], dg[l1]);
|
|
}
|
|
plogf(" ---"); print_space(56);
|
|
plogf("Norms of Delta G():%14.6E%14.6E\n",
|
|
l2normdg(VCS_DATA_PTR(dgl)),
|
|
l2normdg(VCS_DATA_PTR(dg)));
|
|
|
|
plogf(" --- Phase_Name Moles(after update)\n");
|
|
plogf(" --- "); vcs_print_line("-", 50);
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
Vphase = VPhaseList[iph];
|
|
plogf(" --- %18s = %15.7E\n", Vphase->PhaseName.c_str(), TPhMoles1[iph]);
|
|
}
|
|
plogf(" "); vcs_print_line("-", 103);
|
|
plogf(" --- Total Dimensionless Gibbs Free Energy = %15.7E\n",
|
|
vcs_Total_Gibbs(VCS_DATA_PTR(wt), VCS_DATA_PTR(m_gibbsSpecies),
|
|
VCS_DATA_PTR(TPhMoles1)));
|
|
if (m_VCount->Its > 150) {
|
|
plogf(" --- Troublesome solve\n");
|
|
}
|
|
#ifdef DEBUG
|
|
#ifdef DEBUG_MORE
|
|
if (vcs_debug_print_lvl >= 3) {
|
|
prneav();
|
|
}
|
|
#endif
|
|
#endif
|
|
}
|
|
/* *************************************************************** */
|
|
/* **** CONVERGENCE FORCER SECTION ******************************* */
|
|
/* *************************************************************** */
|
|
/*
|
|
* Save the previous delta G in the old vector for
|
|
* printout purposes
|
|
*/
|
|
if (printDetails) {
|
|
vcs_dcopy(VCS_DATA_PTR(dgl), VCS_DATA_PTR(dg), m_numRxnRdc);
|
|
}
|
|
forced = FALSE;
|
|
// if (! im && ! MajorSpeciesHaveConverged) {
|
|
forced = force(iti);
|
|
//}
|
|
/*
|
|
* Print out the changes to the solution that FORCER produced
|
|
*/
|
|
if (printDetails && forced) {
|
|
|
|
if (iti != 0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 3) {
|
|
plogf(" *** vcs_dfe for printout only:");
|
|
}
|
|
#endif
|
|
vcs_updateVP(0);
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 1, 0, m_numSpeciesRdc);
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 3) {
|
|
plogf(" *** vcs_deltag call for printouts only;");
|
|
}
|
|
#endif
|
|
vcs_deltag(1, false);
|
|
}
|
|
plogf(" -----------------------------------------------------\n");
|
|
plogf(" --- FORCER SUBROUTINE changed the solution:\n");
|
|
plogf(" --- SPECIES Status TENT MOLES");
|
|
plogf(" FINAL MOLES TENT_DEL_G/RT FINAL_DELTA_G/RT\n");
|
|
for (i = 0; i < m_numComponents; ++i) {
|
|
plogf(" --- %-12.12s", SpName[i].c_str());
|
|
plogf(" %14.6E%14.6E\n", wt[i], soln[i]);
|
|
}
|
|
for (kspec = m_numComponents; kspec < m_numSpeciesRdc; ++kspec) {
|
|
irxn = kspec - m_numComponents;
|
|
plogf(" --- %-12.12s", SpName[kspec].c_str());
|
|
plogf(" %2d %14.6E%14.6E%14.6E%14.6E\n", spStatus[irxn],
|
|
wt[kspec], soln[kspec], dgl[irxn], dg[irxn]);
|
|
}
|
|
print_space(26);
|
|
plogf("Norms of Delta G():%14.6E%14.6E\n",
|
|
l2normdg(VCS_DATA_PTR(dgl)),
|
|
l2normdg(VCS_DATA_PTR(dg)));
|
|
plogf(" Total moles of gas = %15.7E\n", TPhMoles[0]);
|
|
if ((NPhase > 1) && (! (VPhaseList[1])->SingleSpecies)) {
|
|
plogf(" Total moles of liquid = %15.7E\n", TPhMoles[1]);
|
|
} else {
|
|
plogf(" Total moles of liquid = %15.7E\n", 0.0);
|
|
}
|
|
plogf(" Total Dimensionless Gibbs Free Energy = %15.7E\n",
|
|
vcs_Total_Gibbs(VCS_DATA_PTR(soln), VCS_DATA_PTR(m_gibbsSpecies),
|
|
VCS_DATA_PTR(TPhMoles)));
|
|
plogf(" -----------------------------------------------------\n");
|
|
}
|
|
/*************************************************************************/
|
|
/******************* RESET VALUES AT END OF ITERATION ********************/
|
|
/******************* UPDATE MOLE NUMBERS *********************************/
|
|
/*************************************************************************/
|
|
/*
|
|
* If the solution wasn't changed in the forcer routine,
|
|
* then copy the tentative mole numbers and Phase moles
|
|
* into the actual mole numbers and phase moles.
|
|
* We will consider this current step to be completed.
|
|
*
|
|
* Accept the step. -> the tentative solution now becomes
|
|
* the real solution. If FORCED is true, then
|
|
* we have already done this inside the FORCED
|
|
* loop.
|
|
*/
|
|
if (! forced) {
|
|
vcs_dcopy(VCS_DATA_PTR(TPhMoles), VCS_DATA_PTR(TPhMoles1), NPhase);
|
|
vcs_dcopy(VCS_DATA_PTR(soln), VCS_DATA_PTR(wt), m_numSpeciesRdc);
|
|
}
|
|
vcs_updateVP(0);
|
|
/*
|
|
* Increment the iteration counters
|
|
*/
|
|
++(m_VCount->Its);
|
|
++it1;
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Increment counter increased, step is accepted: %4d\n",
|
|
m_VCount->Its);
|
|
}
|
|
#endif
|
|
/*************************************************************************/
|
|
/******************* HANDLE DELETION OF MULTISPECIES PHASES **************/
|
|
/*************************************************************************/
|
|
/*
|
|
* We delete multiphases, when the total moles in the multiphase
|
|
* is reduced below a relative threshold.
|
|
* Set microscopic multispecies phases with total relative
|
|
* number of moles less than VCS_DELETE_PHASE_CUTOFF to
|
|
* absolute zero.
|
|
*/
|
|
justDeletedMultiPhase = FALSE;
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
Vphase = VPhaseList[iph];
|
|
if (!(Vphase->SingleSpecies)) {
|
|
if (TPhMoles[iph] != 0.0 &&
|
|
TPhMoles[iph]/TMoles <= VCS_DELETE_PHASE_CUTOFF) {
|
|
soldel = 1;
|
|
for (kspec = 0; kspec < m_numSpeciesRdc; kspec++) {
|
|
if (PhaseID[kspec] == iph && soln[kspec] > 0.0) {
|
|
irxn = kspec - m_numComponents;
|
|
if (kspec < m_numComponents) {
|
|
if (soln[kspec] > VCS_DELETE_SPECIES_CUTOFF) {
|
|
soldel = 0;
|
|
break;
|
|
}
|
|
} else {
|
|
for (k = 0; k < m_numComponents; k++) {
|
|
if (sc[irxn][k] != 0.0) {
|
|
if (soln[kspec]/soln[k] > VCS_DELETE_PHASE_CUTOFF) {
|
|
soldel = 0;
|
|
break;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
if (soldel) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 1) {
|
|
plogf(" --- Setting microscopic phase %d to zero\n", iph);
|
|
}
|
|
#endif
|
|
justDeletedMultiPhase = TRUE;
|
|
delete_multiphase(iph);
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* If we have deleted a multispecies phase because the
|
|
* equilibrium moles decreased, then we will update all
|
|
* the component basis calculation, and therefore all
|
|
* of the thermo functions just to be safe.
|
|
*/
|
|
if (justDeletedMultiPhase) {
|
|
justDeletedMultiPhase = FALSE;
|
|
retn = vcs_basopt(FALSE, VCS_DATA_PTR(aw), VCS_DATA_PTR(sa),
|
|
VCS_DATA_PTR(sm), VCS_DATA_PTR(ss), test,
|
|
&usedZeroedSpecies);
|
|
if (retn != VCS_SUCCESS) return retn;
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 0, 0, m_numSpeciesRdc);
|
|
vcs_deltag(0, true);
|
|
uptodate_minors = TRUE;
|
|
if (conv) {
|
|
/*
|
|
* HKM -> I don't understand why the code would just give
|
|
* up here in some cases.
|
|
* This should probably be taken out
|
|
*/
|
|
plogf(" DELETION OF MULTISPECIES PHASE. ");
|
|
plogf("Convergence to number of positive n(i) less than C.\n");
|
|
plogf("Check results to follow carefully. \n\n");
|
|
goto L_RETURN_BLOCK;
|
|
}
|
|
}
|
|
/*************************************************************************/
|
|
/***************** CHECK FOR ELEMENT ABUNDANCE****************************/
|
|
/*************************************************************************/
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Normal element abundance check");
|
|
}
|
|
#endif
|
|
vcs_elab();
|
|
if (! vcs_elabcheck(0)) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" - failed -> redoing element abundances.\n");
|
|
}
|
|
#endif
|
|
vcs_elcorr(VCS_DATA_PTR(sm), VCS_DATA_PTR(wx));
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 0, 0, m_numSpeciesRdc);
|
|
vcs_deltag(0, true);
|
|
uptodate_minors = TRUE;
|
|
}
|
|
#ifdef DEBUG
|
|
else {
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" - passed\n");
|
|
}
|
|
}
|
|
#endif
|
|
/*************************************************************************/
|
|
/***************** CHECK FOR OPTIMUM BASIS *******************************/
|
|
/*************************************************************************/
|
|
/*
|
|
* HKM -> We first evaluate whether the components species are
|
|
* ordered according to their mole numbers. If they are,
|
|
* then we can essential do an order(NR) operation instead
|
|
* of an order(NR*NC) operation to determine whether
|
|
* a new basis is needed.
|
|
*
|
|
* HKM -> This section used to be branched to initially if
|
|
* there was a machine estimate. I took it out to simplify
|
|
* the code logic.
|
|
*/
|
|
dofast = (m_numComponents != 1);
|
|
for (i = 1; i < m_numComponents; ++i) {
|
|
if (soln[i - 1] < soln[i]) {
|
|
dofast = FALSE;
|
|
break;
|
|
}
|
|
}
|
|
dofast = false;
|
|
if (dofast) {
|
|
for (i = 0; i < m_numRxnRdc; ++i) {
|
|
l = ir[i];
|
|
for (j = m_numComponents - 1; j >= 0; j--) {
|
|
if (soln[l] > soln[j]) {
|
|
if (sc[i][j] != 0.0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Get a new basis because %s", SpName[l].c_str());
|
|
plogf(" is larger than comp %s", SpName[j].c_str());
|
|
plogf(" and share nonzero stoic: %-9.1f\n",
|
|
sc[i][j]);
|
|
}
|
|
#endif
|
|
goto L_COMPONENT_CALC;
|
|
}
|
|
} else {
|
|
break;
|
|
}
|
|
#ifdef DEBUG_HKM
|
|
if (spStatus[i] == VCS_SPECIES_ZEROEDMS) {
|
|
if (soln[j] == 0.0) {
|
|
if (sc[i][j] != 0.0) {
|
|
if (dg[i] < 0.0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Get a new basis because %s", SpName[l].c_str());
|
|
plogf(" has dg < 0.0 and comp %s has zero mole num", SpName[j].c_str());
|
|
plogf(" and share nonzero stoic: %-9.1f\n",
|
|
sc[i][j]);
|
|
}
|
|
#endif
|
|
goto L_COMPONENT_CALC;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
#endif
|
|
}
|
|
}
|
|
} else {
|
|
for (i = 0; i < m_numRxnRdc; ++i) {
|
|
l = ir[i];
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
if (soln[l] > soln[j]) {
|
|
if (sc[i][j] != 0.0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Get a new basis because ");
|
|
plogf("%s", SpName[l].c_str());
|
|
plogf(" is larger than comp ");
|
|
plogf("%s", SpName[j].c_str());
|
|
plogf(" and share nonzero stoic: %-9.1f\n",
|
|
sc[i][j]);
|
|
}
|
|
#endif
|
|
goto L_COMPONENT_CALC;
|
|
}
|
|
}
|
|
#ifdef DEBUG_HKM
|
|
if (spStatus[i] == VCS_SPECIES_ZEROEDMS) {
|
|
if (soln[j] == 0.0) {
|
|
if (sc[i][j] != 0.0) {
|
|
if (dg[i] < 0.0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Get a new basis because %s", SpName[l].c_str());
|
|
plogf(" has dg < 0.0 and comp %s has zero mole num", SpName[j].c_str());
|
|
plogf(" and share nonzero stoic: %-9.1f\n",
|
|
sc[i][j]);
|
|
}
|
|
#endif
|
|
goto L_COMPONENT_CALC;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
#endif
|
|
}
|
|
}
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Check for an optimum basis passed\n");
|
|
}
|
|
#endif
|
|
/*************************************************************************/
|
|
/********************** RE-EVALUATE MAJOR-MINOR VECTOR IF NECESSARY ******/
|
|
/*************************************************************************/
|
|
/*
|
|
* Skip this section if we haven't done a full calculation.
|
|
* Go right to the check equilibrium section
|
|
*/
|
|
if (iti == 0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Reevaluate major-minor status of noncomponents:\n");
|
|
}
|
|
#endif
|
|
m_numRxnMinorZeroed = 0;
|
|
for (irxn = 0; irxn < m_numRxnRdc; irxn++) {
|
|
kspec = ir[irxn];
|
|
|
|
int speciesType = vcs_species_type(kspec);
|
|
if (speciesType < VCS_SPECIES_MINOR) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
if (spStatus[irxn] >= VCS_SPECIES_MINOR) {
|
|
plogf(" --- major/minor species is now zeroed out: %s\n",
|
|
SpName[kspec].c_str());
|
|
}
|
|
}
|
|
#endif
|
|
++m_numRxnMinorZeroed;
|
|
} else if (speciesType == VCS_SPECIES_MINOR) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
if (spStatus[irxn] != VCS_SPECIES_MINOR) {
|
|
if (spStatus[irxn] == VCS_SPECIES_MAJOR) {
|
|
plogf(" --- Noncomponent turned from major to minor: ");
|
|
} else if (spStatus[irxn] == VCS_SPECIES_COMPONENT) {
|
|
plogf(" --- Component turned into a minor species: ");
|
|
} else {
|
|
plogf(" --- Zeroed Species turned into a "
|
|
"minor species: ");
|
|
}
|
|
plogf("%s\n", SpName[kspec].c_str());
|
|
}
|
|
}
|
|
#endif
|
|
++m_numRxnMinorZeroed;
|
|
} else if (speciesType == VCS_SPECIES_MAJOR) {
|
|
if (spStatus[irxn] != VCS_SPECIES_MAJOR) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
if (spStatus[irxn] == VCS_SPECIES_MINOR) {
|
|
plogf(" --- Noncomponent turned from minor to major: ");
|
|
} else if (spStatus[irxn] == VCS_SPECIES_COMPONENT) {
|
|
plogf(" --- Component turned into a major: ");
|
|
} else {
|
|
plogf(" --- Noncomponent turned from zeroed to major: ");
|
|
}
|
|
plogf("%s\n", SpName[kspec].c_str());
|
|
}
|
|
#endif
|
|
spStatus[irxn] = VCS_SPECIES_MAJOR;
|
|
/*
|
|
* For this special case, we must reevaluate thermo functions
|
|
*/
|
|
if (iti != 0) {
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 0, kspec, kspec+1);
|
|
vcs_deltag(0, false);
|
|
}
|
|
}
|
|
}
|
|
spStatus[irxn] = speciesType;
|
|
}
|
|
/*
|
|
* This logical variable indicates whether all current
|
|
* non-component species are minor or nonexistent
|
|
*/
|
|
im = (m_numRxnMinorZeroed == m_numRxnRdc);
|
|
}
|
|
/*************************************************************************/
|
|
/***************** EQUILIBRIUM CHECK FOR MAJOR SPECIES *******************/
|
|
/*************************************************************************/
|
|
L_EQUILIB_CHECK: ;
|
|
if (! im) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Equilibrium check for major species: ");
|
|
}
|
|
#endif
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
if (spStatus[irxn] == VCS_SPECIES_MAJOR && (fabs(dg[irxn]) > tolmaj)) {
|
|
if (m_VCount->Its >= maxit) {
|
|
solveFail = -1;
|
|
/*
|
|
* Clean up and exit code even though we haven't
|
|
* converged. -> we have run out of iterations!
|
|
*/
|
|
goto L_RETURN_BLOCK;
|
|
} else {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf("%s failed\n", SpName[ir[irxn]].c_str());
|
|
}
|
|
#endif
|
|
/*
|
|
* Set MajorSpeciesHaveConverged to false to indicate that
|
|
* convergence amongst
|
|
* major species has not been achieved
|
|
*/
|
|
MajorSpeciesHaveConverged = false;
|
|
/*
|
|
* Go back and do another iteration with variable ITI
|
|
*/
|
|
goto L_MAINLOOP_MM4_SPECIES;
|
|
}
|
|
}
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" MAJOR SPECIES CONVERGENCE achieved\n");
|
|
}
|
|
#endif
|
|
}
|
|
#ifdef DEBUG
|
|
else {
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" MAJOR SPECIES CONVERGENCE achieved "
|
|
"(because there are no major species)\n");
|
|
}
|
|
}
|
|
#endif
|
|
/*
|
|
* Set MajorSpeciesHaveConverged to true to indicate
|
|
* that convergence amongst major species has been achieved
|
|
*/
|
|
MajorSpeciesHaveConverged = true;
|
|
/*************************************************************************/
|
|
/*************** EQUILIBRIUM CHECK FOR MINOR SPECIES *********************/
|
|
/*************************************************************************/
|
|
if (m_numRxnMinorZeroed != 0) {
|
|
/*
|
|
* Calculate the chemical potential and reaction DeltaG
|
|
* for minor species, if needed.
|
|
*/
|
|
if (iti != 0) {
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 1, 0, m_numSpeciesRdc);
|
|
vcs_deltag(1, false);
|
|
uptodate_minors = TRUE;
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Equilibrium check for minor species: ");
|
|
}
|
|
#endif
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
if (spStatus[irxn] == VCS_SPECIES_MINOR && (fabs(dg[irxn]) > tolmin)) {
|
|
if (m_VCount->Its >= maxit) {
|
|
solveFail = -1;
|
|
/*
|
|
* Clean up and exit code. -> Even though we have not
|
|
* converged, we have run out of iterations !
|
|
*/
|
|
goto L_RETURN_BLOCK;
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf("%s failed\n", SpName[ir[irxn]].c_str());
|
|
}
|
|
#endif
|
|
/*
|
|
* Set iti to zero to force a full calculation, and go back
|
|
* to the main loop to do another iteration.
|
|
*/
|
|
iti = 0;
|
|
goto L_MAINLOOP_ALL_SPECIES;
|
|
}
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" CONVERGENCE achieved\n");
|
|
}
|
|
#endif
|
|
}
|
|
/*************************************************************************/
|
|
/*********************** FINAL ELEMENTAL ABUNDANCE CHECK *****************/
|
|
/*************************************************************************/
|
|
/*
|
|
* Recalculate the element abundance vector again
|
|
*/
|
|
vcs_updateVP(0);
|
|
vcs_elab();
|
|
|
|
/* LEC is only true when we are near the end game */
|
|
if (lec) {
|
|
if (!giveUpOnElemAbund) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Check the Full Element Abundances: ");
|
|
}
|
|
#endif
|
|
/*
|
|
* Final element abundance check:
|
|
* If we fail then we need to go back and correct
|
|
* the element abundances, and then go do a major step
|
|
*/
|
|
if (! vcs_elabcheck(1) ) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
if (! vcs_elabcheck(0)) {
|
|
plogf(" failed\n");
|
|
} else {
|
|
plogf(" passed for NC but failed for NE: RANGE ERROR\n");
|
|
}
|
|
}
|
|
#endif
|
|
// delete?
|
|
goto L_ELEM_ABUND_CHECK;
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" passed\n");
|
|
}
|
|
#endif
|
|
}
|
|
/*
|
|
* If we have deleted a species then we need to recheck the
|
|
* the deleted species, before exiting
|
|
*/
|
|
if (m_numSpeciesRdc != m_numSpeciesTot) {
|
|
goto L_RECHECK_DELETED;
|
|
}
|
|
/* - Final checks are passed -> go check out */
|
|
goto L_RETURN_BLOCK;
|
|
}
|
|
lec = TRUE;
|
|
/* *************************************************** */
|
|
/* **** CORRECT ELEMENTAL ABUNDANCES ***************** */
|
|
/* *************************************************** */
|
|
L_ELEM_ABUND_CHECK: ;
|
|
/*
|
|
* HKM - Put in an element abundance check. The element abundances
|
|
* were being corrected even if they were perfectly OK to
|
|
* start with. This is actually an expensive operation, so
|
|
* I took it out. Also vcs_dfe() doesn't need to be called if
|
|
* no changes were made.
|
|
*/
|
|
rangeErrorFound = 0;
|
|
if (! vcs_elabcheck(1)) {
|
|
int ncBefore = vcs_elabcheck(0);
|
|
vcs_elcorr(VCS_DATA_PTR(sm), VCS_DATA_PTR(wx));
|
|
int ncAfter = vcs_elabcheck(0);
|
|
int neAfter = vcs_elabcheck(1);
|
|
/*
|
|
* Go back to evaluate the total moles of gas and liquid.
|
|
*/
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 0, 0, m_numSpeciesRdc);
|
|
vcs_deltag(0, false);
|
|
/*
|
|
*
|
|
*/
|
|
if (!ncBefore) {
|
|
if (ncAfter) {
|
|
/*
|
|
* We have breathed new life into the old problem. Now the
|
|
* element abundances up to NC agree. Go back and
|
|
* restart the main loop calculation, resetting the
|
|
* end conditions.
|
|
*/
|
|
lec = FALSE;
|
|
iti = 0;
|
|
goto L_MAINLOOP_ALL_SPECIES;
|
|
} else {
|
|
/*
|
|
* We are still hosed
|
|
*/
|
|
if (finalElemAbundAttempts >= 3) {
|
|
giveUpOnElemAbund = true;
|
|
goto L_EQUILIB_CHECK;
|
|
} else {
|
|
finalElemAbundAttempts++;
|
|
lec = FALSE;
|
|
iti = 0;
|
|
goto L_MAINLOOP_ALL_SPECIES;
|
|
}
|
|
}
|
|
} else {
|
|
if (ncAfter) {
|
|
if (neAfter) {
|
|
/*
|
|
* Recovery of end element abundances
|
|
* -> go do equilibrium check again and then
|
|
* check out.
|
|
*/
|
|
goto L_EQUILIB_CHECK;
|
|
} else {
|
|
/*
|
|
* Probably an unrecoverable range error
|
|
*/
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- vcs_solve_tp: RANGE SPACE ERROR ENCOUNTERED\n");
|
|
plogf(" --- vcs_solve_tp: - Giving up on NE Element Abundance satisfaction \n");
|
|
plogf(" --- vcs_solve_tp: - However, NC Element Abundance criteria is satisfied \n");
|
|
plogf(" --- vcs_solve_tp: - Returning the calculated equilibrium condition \n");
|
|
}
|
|
#endif
|
|
rangeErrorFound = 1;
|
|
giveUpOnElemAbund = true;
|
|
goto L_EQUILIB_CHECK;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
// Calculate delta g's
|
|
vcs_deltag(0, false);
|
|
// Go back to equilibrium check as a prep to eventually checking out
|
|
goto L_EQUILIB_CHECK;
|
|
|
|
/* *************************************************** */
|
|
/* **** RECHECK DELETED SPECIES ********************** */
|
|
/* *************************************************** */
|
|
/*
|
|
* We are here for two reasons. One is if we have
|
|
* achieved convergence, but some species have been eliminated
|
|
* from the problem because they were in multispecies phases
|
|
* and their mole fractions drifted less than
|
|
* VCS_DELETE_SPECIES_CUTOFF .
|
|
* The other reason why we are here is because all of the
|
|
* non-component species in the problem have been eliminated
|
|
* for one reason or another.
|
|
*/
|
|
L_RECHECK_DELETED: ;
|
|
npb = recheck_deleted();
|
|
/*
|
|
* If we haven't found any species that needed adding we are done.
|
|
*/
|
|
if (npb <= 0) {
|
|
goto L_RETURN_BLOCK_B;
|
|
}
|
|
/*
|
|
* If we have found something to add, recalculate everything
|
|
* for minor species and go back to do a full iteration
|
|
*/
|
|
MajorSpeciesHaveConverged = true;
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 1, 0, m_numSpeciesRdc);
|
|
vcs_deltag(0, false);
|
|
iti = 0;
|
|
goto L_MAINLOOP_ALL_SPECIES;
|
|
/*************************************************************************/
|
|
/******************** CLEANUP AND RETURN BLOCK ***************************/
|
|
/*************************************************************************/
|
|
L_RETURN_BLOCK: ;
|
|
|
|
npb = recheck_deleted();
|
|
/*
|
|
* If we haven't found any species that needed adding we are done.
|
|
*/
|
|
if (npb > 0) {
|
|
/*
|
|
* If we have found something to add, recalculate everything
|
|
* for minor species and go back to do a full iteration
|
|
*/
|
|
MajorSpeciesHaveConverged = true;
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 1, 0, m_numSpeciesRdc);
|
|
vcs_deltag(0, false);
|
|
iti = 0;
|
|
goto L_MAINLOOP_ALL_SPECIES;
|
|
}
|
|
|
|
L_RETURN_BLOCK_B: ;
|
|
|
|
/*
|
|
* Add back deleted species in non-zeroed phases. Estimate their
|
|
* mole numbers.
|
|
*/
|
|
add_deleted();
|
|
/*
|
|
* Make sure the volume phase objects hold the same state and
|
|
* information as the vcs object. This also update the Cantera objects
|
|
* with this information.
|
|
*/
|
|
vcs_updateVP(0);
|
|
/*
|
|
* Store the final Delta G values for each non-component species
|
|
* in the species slot rather than the reaction slot
|
|
*/
|
|
kspec = m_numSpeciesTot;
|
|
i = m_numRxnTot;
|
|
for (irxn = 0; irxn < m_numRxnTot; ++irxn) {
|
|
--kspec;
|
|
--i;
|
|
dg[kspec] = dg[i];
|
|
}
|
|
vcs_dzero(VCS_DATA_PTR(dg), m_numComponents);
|
|
/*
|
|
* Evaluate the final mole fractions
|
|
* storring them in wt[]
|
|
*/
|
|
vcs_vdzero(wt, m_numSpeciesTot);
|
|
for (kspec = 0; kspec < m_numSpeciesTot; ++kspec) {
|
|
if (SSPhase[kspec]) {
|
|
wt[kspec] = 1.0;
|
|
} else {
|
|
iph = PhaseID[kspec];
|
|
if (TPhMoles[iph] != 0.0) {
|
|
wt[kspec] = soln[kspec] / TPhMoles[iph];
|
|
} else {
|
|
/*
|
|
* For MultiSpecies phases that are zeroed out,
|
|
* return the mole fraction vector from the VolPhase object.
|
|
* This contains the mole fraction that would be true if
|
|
* the phase just pops into existence.
|
|
*/
|
|
i = indPhSp[kspec];
|
|
Vphase = VPhaseList[iph];
|
|
wt[kspec] = Vphase->molefraction(i);
|
|
}
|
|
}
|
|
}
|
|
// Return an error code if a Range Space Error is thought to have occurred.
|
|
if (rangeErrorFound) {
|
|
solveFail = 1;
|
|
}
|
|
/*
|
|
* Free temporary storage used in this routine
|
|
* and increment counters
|
|
*/
|
|
/*
|
|
* Calculate counters
|
|
*/
|
|
tsecond = vcs_second() - tsecond;
|
|
m_VCount->Time_vcs_TP = tsecond;
|
|
m_VCount->T_Time_vcs_TP += m_VCount->Time_vcs_TP;
|
|
(m_VCount->T_Calls_vcs_TP)++;
|
|
m_VCount->T_Its += m_VCount->Its;
|
|
m_VCount->T_Basis_Opts += m_VCount->Basis_Opts;
|
|
m_VCount->T_Time_basopt += m_VCount->Time_basopt;
|
|
/*
|
|
* Return a Flag indicating whether convergence occurred
|
|
*/
|
|
return solveFail;
|
|
} /* vcs_solve_TP() **********************************************************/
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
double VCS_SOLVE::minor_alt_calc(int kspec, int irxn, int *do_delete
|
|
#ifdef DEBUG
|
|
, char *ANOTE
|
|
#endif
|
|
)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* minor_alt_calc:
|
|
*
|
|
* Minor species alternative calculation
|
|
* ---------------------------------------
|
|
*
|
|
* This is based upon the following approximation:
|
|
* The mole fraction changes due to these reactions don't affect
|
|
* the mole numbers of the component species. Therefore the following
|
|
* approximation is valid for an ideal solution phase:
|
|
* 0 = DG(I) + log(WT(I)/W(I))
|
|
*
|
|
* W(i) = Old mole number of species i in the phase
|
|
* WT(i) = Trial new mole number of species i in the pahse
|
|
*
|
|
* (DG contains the contribution from
|
|
* FF(I) + log(ActCoeff[i] * W(I)/Total_Moles) )
|
|
* Thus,
|
|
* WT(I) = W(I) EXP(-DG(I))
|
|
*
|
|
* Most of this section is mainly restricting the update to reasonable
|
|
* values.
|
|
*
|
|
*
|
|
* Note: This routine was generalized to incorporate
|
|
* nonideal phases.
|
|
*
|
|
* Input:
|
|
* ------
|
|
* kspec, irxn = the current species and corresponding formation
|
|
* reaction number.
|
|
* Output:
|
|
* ---------
|
|
* return value: dx = the change in mole number
|
|
* do_delete: BOOLEAN which if true on return, then we branch
|
|
* to the section that deletes a species from the
|
|
* current set of active species.
|
|
*************************************************************************/
|
|
{
|
|
double dx;
|
|
double w_kspec = soln[kspec];
|
|
double *wt_kspec = VCS_DATA_PTR(wt) + kspec;
|
|
double wTrial;
|
|
double *ds_kspec = VCS_DATA_PTR(ds) + kspec;
|
|
double dg_irxn = dg[irxn];
|
|
int iphase = PhaseID[kspec];
|
|
vcs_VolPhase *Vphase = VPhaseList[iphase];
|
|
*do_delete = FALSE;
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
if (w_kspec <= 0.0) {
|
|
w_kspec = VCS_DELETE_MINORSPECIES_CUTOFF;
|
|
}
|
|
if (dg_irxn < -20.) {
|
|
dg_irxn = -20.;
|
|
}
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,"minor species alternative calc");
|
|
#endif
|
|
if (dg_irxn >= 82.0) {
|
|
(*wt_kspec) = w_kspec * 1.0e-6;
|
|
if (w_kspec < VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
goto L_ZERO_SPECIES;
|
|
}
|
|
} else {
|
|
if (fabs(dg_irxn) <= tolmin2) {
|
|
(*wt_kspec) = w_kspec;
|
|
(*ds_kspec) = 0.0;
|
|
return 0.0;
|
|
}
|
|
// c = log(ActCoeff[kspec] * w_kspec) - dg_irxn;
|
|
|
|
|
|
|
|
}
|
|
|
|
if (dg_irxn > 10.0) {
|
|
(*wt_kspec) = w_kspec * 1.0e-5;
|
|
if (w_kspec < VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
goto L_ZERO_SPECIES;
|
|
}
|
|
} else {
|
|
double ac0 = ActCoeff[kspec];
|
|
double ac = ac0;
|
|
double w0 = w_kspec;
|
|
double dd = exp(-dg_irxn);
|
|
|
|
wTrial = w0 * ac0 / ac * dd;
|
|
*wt_kspec = wTrial;
|
|
Vphase->setMolesFromVCS(VCS_DATA_PTR(wt));
|
|
Vphase->sendToVCSActCoeff(VCS_DATA_PTR(ActCoeff));
|
|
double ac1 = ActCoeff[kspec];
|
|
double acprime = 0.0;
|
|
if (fabs(wTrial - w0) > 1.0E-8 * w0) {
|
|
acprime = (ac1 - ac0) / (wTrial - w0);
|
|
}
|
|
double jac = acprime * wTrial + ac1;
|
|
double fTrial = ac1 * wTrial - ac0*w0*dd;
|
|
double w2 = wTrial - fTrial / jac;
|
|
if (w2 > 100.*w0) {
|
|
*wt_kspec = 100.0 * w0;
|
|
} else if (100. * w2 < w0) {
|
|
*wt_kspec = 0.01 * w0;
|
|
} else {
|
|
*wt_kspec = w2;
|
|
}
|
|
}
|
|
|
|
if ((*wt_kspec) < VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
goto L_ZERO_SPECIES;
|
|
}
|
|
dx = (*wt_kspec) - w_kspec;
|
|
(*ds_kspec) = dx;
|
|
return dx;
|
|
/*
|
|
*
|
|
* Alternate return based for cases where we need to delete the species
|
|
* from the current list of active species, because its concentration
|
|
* has gotten too small.
|
|
*/
|
|
L_ZERO_SPECIES: ;
|
|
*do_delete = TRUE;
|
|
dx = - w_kspec;
|
|
(*ds_kspec) = dx;
|
|
return dx;
|
|
}
|
|
else {
|
|
/*
|
|
* Voltage calculation
|
|
* HKM -> Need to check the sign
|
|
*/
|
|
dx = dg[irxn]/ Faraday_dim;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,"voltage species alternative calc");
|
|
#endif
|
|
}
|
|
return dx;
|
|
}
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
int VCS_SOLVE::delta_species(int kspec, double *delta_ptr)
|
|
|
|
/************************************************************************
|
|
*
|
|
* delta_species():
|
|
*
|
|
* Change the concentration of a species by delta moles.
|
|
* Make sure to conserve
|
|
* elements and keep track of the total moles in all phases.
|
|
*
|
|
* return:
|
|
* 1: succeeded
|
|
* 0: failed.
|
|
************************************************************************/
|
|
{
|
|
int irxn = kspec - m_numComponents;
|
|
int retn = 1;
|
|
int j;
|
|
double tmp;
|
|
double delta = *delta_ptr;
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
/*
|
|
* Attempt the given dx. If it doesn't work, try to see if a smaller
|
|
* one would work,
|
|
*/
|
|
double dx = delta;
|
|
double *sc_irxn = sc[irxn];
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
if (soln[j] > 0.0) {
|
|
tmp = sc_irxn[j] * dx;
|
|
if (-tmp > soln[j]) {
|
|
retn = 0;
|
|
dx = MIN(dx, - soln[j] / sc_irxn[j]);
|
|
}
|
|
}
|
|
/*
|
|
* If the component has a zero concentration and is a reactant
|
|
* in the formation reaction, then dx == 0.0, and we just return.
|
|
*/
|
|
if (soln[j] <= 0.0) {
|
|
if (sc_irxn[j] < 0.0) {
|
|
*delta_ptr = 0.0;
|
|
return 0;
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* ok, we found a positive dx. implement it.
|
|
*/
|
|
*delta_ptr = dx;
|
|
soln[kspec] += dx;
|
|
int iph = PhaseID[kspec];
|
|
TPhMoles[iph] += dx;
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
iph = PhaseID[j];
|
|
tmp = sc_irxn[j] * dx;
|
|
soln[j] += tmp;
|
|
TPhMoles[iph] += tmp;
|
|
if (soln[j] < 0.0) {
|
|
soln[j] = 0.0;
|
|
}
|
|
}
|
|
}
|
|
return retn;
|
|
}
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
int VCS_SOLVE::zero_species(int kspec)
|
|
|
|
/************************************************************************
|
|
*
|
|
* zero_species:
|
|
*
|
|
* Zero out the concentration of a species. Make sure to conserve
|
|
* elements and keep track of the total moles in all phases.
|
|
* w[]
|
|
* TPhMoles[]
|
|
*
|
|
* return:
|
|
* 1: succeeded
|
|
* 0: failed.
|
|
************************************************************************/
|
|
{
|
|
int retn = 1;
|
|
/*
|
|
* Calculate a delta that will eliminate the species.
|
|
*/
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
double dx = -(soln[kspec]);
|
|
if (dx != 0.0) {
|
|
retn = delta_species(kspec, &dx);
|
|
if (!retn) {
|
|
plogf("zero_species: Couldn't zero the species %d, "
|
|
"did delta of %g. orig conc of %g\n",
|
|
kspec, dx, soln[kspec] + dx);
|
|
}
|
|
}
|
|
}
|
|
return retn;
|
|
}
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
int VCS_SOLVE::delete_species(int kspec)
|
|
|
|
/************************************************************************
|
|
*
|
|
* delete_species:
|
|
*
|
|
* Rearrange data when species is added or removed. The Lth species is
|
|
* moved to the back of the species vector. The back of the species
|
|
* vector is indicated by the value of MR, the current number of
|
|
* active species in the mechanism.
|
|
*
|
|
* Input
|
|
* kspec = species number
|
|
* Return value
|
|
* The return is true when the current number of
|
|
* noncomponent species is equal to zero. A recheck of deleted species
|
|
* is carried out in the main code.
|
|
*************************************************************************/
|
|
{
|
|
int klast = m_numSpeciesRdc - 1;
|
|
int iph = PhaseID[kspec];
|
|
vcs_VolPhase *Vphase = VPhaseList[iph];
|
|
int irxn = kspec - m_numComponents; /* This is the noncomponent rxn index */
|
|
/*
|
|
* Zero the concentration of the species.
|
|
* -> This zeroes w[kspec] and modifies TPhMoles[]
|
|
*/
|
|
int retn = zero_species(kspec);
|
|
if (! retn) {
|
|
plogf("Failed to delete a species!\n");
|
|
exit(-1);
|
|
}
|
|
/*
|
|
* Decrement the minor species counter if the current species is
|
|
* a minor species
|
|
*/
|
|
if (spStatus[irxn] != VCS_SPECIES_MAJOR) --(m_numRxnMinorZeroed);
|
|
spStatus[irxn] = VCS_SPECIES_DELETED;
|
|
dg[irxn] = 0.0;
|
|
dgl[irxn] = 0.0;
|
|
m_gibbsSpecies[kspec] = 0.0;
|
|
fel[kspec] = 0.0;
|
|
wt[kspec] = 0.0;
|
|
/*
|
|
* Rearrange the data if the current species isn't the last active
|
|
* species.
|
|
*/
|
|
if (kspec != klast) {
|
|
vcs_switch_pos(TRUE, klast, kspec);
|
|
}
|
|
/*
|
|
* Adjust the total moles in a phase downwards.
|
|
*/
|
|
Vphase->setMolesFromVCSCheck(VCS_DATA_PTR(soln), VCS_DATA_PTR(TPhMoles));
|
|
|
|
/*
|
|
* Adjust the current number of active species and reactions counters
|
|
*/
|
|
--(m_numRxnRdc);
|
|
--(m_numSpeciesRdc);
|
|
|
|
/*
|
|
* Check to see whether we have just annihilated a multispecies phase.
|
|
* If it is extinct, call the delete_multiphase() function.
|
|
*/
|
|
if (! SSPhase[klast]) {
|
|
if (Vphase->Existence != 2) {
|
|
Vphase->Existence = 0;
|
|
for (kspec = 0; kspec < m_numSpeciesRdc; kspec++) {
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
if (PhaseID[kspec] == iph) {
|
|
if (soln[kspec] > 0.0) {
|
|
Vphase->Existence = 1;
|
|
break;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
if (Vphase->Existence == 0) {
|
|
delete_multiphase(iph);
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* When the total number of noncomponent species is zero, we
|
|
* have to signal the calling code
|
|
*/
|
|
return (m_numRxnRdc == 0);
|
|
} /* delete_species() ********************************************************/
|
|
|
|
/****************************************************************************
|
|
*
|
|
* reinsert_deleted():
|
|
*
|
|
* irxn = id of the noncomponent species formation reaction for the
|
|
* species to be added in.
|
|
*
|
|
* We make decisions on the initial mole number, and major-minor status
|
|
* here. We also fix up the total moles in a phase.
|
|
*
|
|
* The algorithm proceeds to implement these decisions in the previous
|
|
* position of the species. Then, vcs_switch_pos is called to move the
|
|
* species into the last active species slot, incrementing the number
|
|
* of active species at the same time.
|
|
*
|
|
* This routine is responsible for the global data manipulation only.
|
|
*/
|
|
void VCS_SOLVE::vcs_reinsert_deleted(int kspec) {
|
|
int i, k, irxn = kspec - m_numComponents;
|
|
int *phaseID = VCS_DATA_PTR(PhaseID);
|
|
double dx;
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Add back a deleted species: %-12s\n", SpName[kspec].c_str());
|
|
}
|
|
#endif
|
|
/*
|
|
* Set the species back to minor species status
|
|
* this adjusts soln[] and TPhMoles[]
|
|
* HKM -> make this a relative mole number!
|
|
*/
|
|
dx = VCS_DELETE_SPECIES_CUTOFF * 10.;
|
|
delta_species(kspec, &dx);
|
|
spStatus[irxn] = VCS_SPECIES_MINOR;
|
|
|
|
if (SSPhase[kspec]) {
|
|
spStatus[irxn] = VCS_SPECIES_MAJOR;
|
|
--(m_numRxnMinorZeroed);
|
|
}
|
|
int iph = PhaseID[kspec];
|
|
vcs_VolPhase *Vphase = VPhaseList[iph];
|
|
Vphase->setMolesFromVCSCheck(VCS_DATA_PTR(soln), VCS_DATA_PTR(TPhMoles));
|
|
/*
|
|
* We may have popped a multispecies phase back
|
|
* into existence. If we did, we have to check
|
|
* the other species in that phase.
|
|
* Take care of the spStatus[] flag.
|
|
* The value of spStatus[] must change from
|
|
* VCS_SPECIES_ZEROEDPHASE to VCS_SPECIES_ZEROEDMS
|
|
* for those other species.
|
|
*/
|
|
if (! SSPhase[kspec]) {
|
|
if (Vphase->Existence == 0) {
|
|
Vphase->Existence = 1;
|
|
for (k = 0; k < m_numSpeciesTot; k++) {
|
|
if (phaseID[k] == iph) {
|
|
i = k - m_numComponents;
|
|
if (spStatus[i] == VCS_SPECIES_ZEROEDPHASE)
|
|
spStatus[i] = VCS_SPECIES_ZEROEDMS;
|
|
}
|
|
}
|
|
}
|
|
} else {
|
|
Vphase->Existence = 1;
|
|
}
|
|
|
|
++(m_numRxnRdc);
|
|
++(m_numSpeciesRdc);
|
|
++(m_numRxnMinorZeroed);
|
|
|
|
if (kspec != (m_numSpeciesRdc - 1)) {
|
|
/*
|
|
* Rearrange both the species and the non-component global data
|
|
*/
|
|
vcs_switch_pos(TRUE, (m_numSpeciesRdc - 1), kspec);
|
|
}
|
|
} /* vcs_reinsert_deleted() */
|
|
|
|
/****************************************************************************
|
|
*
|
|
* delete_multiphase():
|
|
*
|
|
* This routine handles the bookkeepking involved with the
|
|
* deletion of multiphase phases from the
|
|
* problem. When they are deleted, all of their species become active
|
|
* species, even though their mole numbers are set to zero.
|
|
* The routine does not make the decision to eliminate multiphases.
|
|
*
|
|
* Note, species in phases with zero mole numbers are still
|
|
* considered active. Whether the phase pops back into
|
|
* existence or not is checked as part of the main iteration
|
|
* loop.
|
|
*/
|
|
void VCS_SOLVE::delete_multiphase(int iph) {
|
|
int kspec, j, irxn;
|
|
double dx;
|
|
vcs_VolPhase *Vphase = VPhaseList[iph];
|
|
/*
|
|
* set the phase existence flag to dead
|
|
*/
|
|
Vphase->Existence = 0;
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- delete_multiphase %d, %s\n", iph, Vphase->PhaseName.c_str());
|
|
}
|
|
#endif
|
|
/*
|
|
* Zero out the total moles counters for the phase
|
|
*/
|
|
TPhMoles[iph] = 0.0;
|
|
TPhMoles1[iph] = 0.0;
|
|
DelTPhMoles[iph] = 0.0;
|
|
|
|
/*
|
|
* Loop over all of the active species in the phase.
|
|
*/
|
|
for (kspec = 0; kspec < m_numSpeciesRdc; ++kspec) {
|
|
if (PhaseID[kspec] == iph) {
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
irxn = kspec - m_numComponents;
|
|
/*
|
|
* calculate an extent of rxn, dx, that zeroes out the species.
|
|
*/
|
|
dx = - (soln[kspec]);
|
|
/*
|
|
* Set the mole numbers of that species to zero.
|
|
*/
|
|
soln[kspec] = 0.0;
|
|
wt[kspec] = 0.0;
|
|
ds[kspec] = 0.0;
|
|
/*
|
|
* Change the status flag of the species to that of an
|
|
* zeroed phase
|
|
*/
|
|
spStatus[irxn] = VCS_SPECIES_ZEROEDPHASE;
|
|
/*
|
|
* changed the component mole numbers to account for the
|
|
* final extent of reaction. Make sure to keep component
|
|
* mole numbers constant.
|
|
* HKM -> note, this will cause a loss of moles!
|
|
*/
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
soln[j] += sc[irxn][j] * dx;
|
|
if (soln[j] < 0.0) {
|
|
soln[j] = 0.0;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* Loop over all of the inactive species in the phase:
|
|
* Right now we reinstate all species in a deleted multiphase.
|
|
* We may only want to reinstate the "major ones" in the future.
|
|
* Note, species in phases with zero mole numbers are still
|
|
* considered active. Whether the phase pops back into
|
|
* existence or not is checked as part of the main iteration
|
|
* loop.
|
|
*/
|
|
for (kspec = m_numSpeciesRdc; kspec < m_numSpeciesTot; ++kspec) {
|
|
if (PhaseID[kspec] == iph) {
|
|
irxn = kspec - m_numComponents;
|
|
soln[kspec] = 0.0;
|
|
wt[kspec] = 0.0;
|
|
ds[kspec] = 0.0;
|
|
spStatus[irxn] = VCS_SPECIES_ZEROEDPHASE;
|
|
|
|
++(m_numRxnRdc);
|
|
++(m_numSpeciesRdc);
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Make %s", SpName[kspec].c_str());
|
|
plogf(" an active but zeroed species because its phase "
|
|
"was zeroed\n");
|
|
}
|
|
#endif
|
|
if (kspec != (m_numSpeciesRdc - 1)) {
|
|
/*
|
|
* Rearrange both the species and the non-component global data
|
|
*/
|
|
vcs_switch_pos(TRUE, (m_numSpeciesRdc - 1), kspec);
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* Upload the state to the VP object
|
|
*/
|
|
Vphase->setMolesFromVCSCheck(VCS_DATA_PTR(soln), VCS_DATA_PTR(TPhMoles), iph);
|
|
|
|
} /* delete_multiphase() *****************************************************/
|
|
|
|
/*****************************************************************************
|
|
*
|
|
* recheck_deleted:
|
|
*
|
|
* Recheck deleted species in multispecies phases.
|
|
*
|
|
* HKM -> This algorithm needs to be updated for activity coefficients
|
|
*/
|
|
int VCS_SOLVE::recheck_deleted(void)
|
|
{
|
|
int iph, kspec, irxn, npb;
|
|
double *xtcutoff = VCS_DATA_PTR(TmpPhase);
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Start rechecking deleted species in multispec phases\n");
|
|
}
|
|
#endif
|
|
if (m_numSpeciesRdc == m_numSpeciesTot) return 0;
|
|
/*
|
|
* Use the standard chemical potentials for the chemical potentials
|
|
* of deleted species. Then, calculate Delta G for
|
|
* for formation reactions
|
|
*/
|
|
for (kspec = m_numSpeciesRdc; kspec < m_numSpeciesTot; ++kspec) {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
}
|
|
/*
|
|
* Recalculate the DeltaG's of the formation reactions for the
|
|
* deleted species in the mechanism
|
|
*/
|
|
vcs_deltag(0, true);
|
|
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
if (TPhMoles[iph] > 0.0)
|
|
xtcutoff[iph] = log (TPhMoles[iph] / VCS_DELETE_SPECIES_CUTOFF);
|
|
else
|
|
xtcutoff[iph] = 0.0;
|
|
}
|
|
/*
|
|
*
|
|
* We are checking the equation:
|
|
*
|
|
* sum_u = sum_j_comp [ sigma_i_j * u_j ]
|
|
* = u_i_O + log((AC_i * W_i)/TPhMoles)
|
|
*
|
|
* by first evaluating:
|
|
*
|
|
* DG_i_O = u_i_O - sum_u.
|
|
*
|
|
* Then, if TL is zero, the phase pops into existence if DG_i_O < 0.
|
|
* Also, if the phase exists, then we check to see if the species
|
|
* can have a mole number larger than VCS_DELETE_SPECIES_CUTOFF
|
|
* (default value = 1.0E-32).
|
|
*
|
|
* HKM:
|
|
* This seems to be an inconsistency in the algorithm here that needs
|
|
* correcting. The requirement above may bypass some multiphases which
|
|
* should exist. The real requirement for the phase to exist is:
|
|
*
|
|
* sum_i_in_phase [ exp(-DG_i_O) ] >= 1.0
|
|
*
|
|
* Thus, we need to amend th code. Also nonideal solutions will tend to
|
|
* complicate matters severely also.
|
|
*/
|
|
npb = 0;
|
|
for (irxn = m_numRxnRdc; irxn < m_numRxnTot; ++irxn) {
|
|
kspec = ir[irxn];
|
|
iph = PhaseID[kspec];
|
|
if (TPhMoles[iph] == 0.0) {
|
|
if (dg[irxn] < 0.0) {
|
|
vcs_reinsert_deleted(kspec);
|
|
npb++;
|
|
} else {
|
|
soln[kspec] = 0.0;
|
|
}
|
|
} else if (TPhMoles[iph] > 0.0) {
|
|
if (dg[irxn] < xtcutoff[iph]) {
|
|
vcs_reinsert_deleted(kspec);
|
|
npb++;
|
|
}
|
|
}
|
|
}
|
|
return npb;
|
|
} /* recheck_deleted() *******************************************************/
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void VCS_SOLVE::add_deleted(void)
|
|
|
|
/*************************************************************************
|
|
*
|
|
* Provide an estimate for the deleted species in phases that
|
|
* are not zeroed out
|
|
*
|
|
*************************************************************************/
|
|
{
|
|
int iph, kspec, retn;
|
|
if (m_numSpeciesRdc == m_numSpeciesTot) return;
|
|
/*
|
|
* Use the standard chemical potentials for the chemical potentials
|
|
* of deleted species. Then, calculate Delta G for
|
|
* for formation reactions
|
|
*
|
|
* HKM Note: We need to update this step for nonunity activity
|
|
* coefficients.
|
|
* The formula will be fe = ff + RT * ln(actCoeff)
|
|
* where the activity coefficient is evaluated at
|
|
* ~ infinite dilution.
|
|
*/
|
|
for (kspec = m_numSpeciesRdc; kspec < m_numSpeciesTot; ++kspec) {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
}
|
|
/*
|
|
* Recalculate the DeltaG's of the formation reactions for the
|
|
* deleted species in the mechanism
|
|
*/
|
|
vcs_deltag(0, true);
|
|
|
|
|
|
for (int irxn = m_numRxnRdc; irxn < m_numRxnTot; ++irxn) {
|
|
kspec = ir[irxn];
|
|
iph = PhaseID[kspec];
|
|
if (TPhMoles[iph] > 0.0) {
|
|
double maxDG = MIN(dg[irxn], 300);
|
|
double dx = TPhMoles[iph] * exp(- maxDG);
|
|
retn = delta_species(kspec, &dx);
|
|
}
|
|
}
|
|
|
|
vcs_dfe(VCS_DATA_PTR(soln), 0, 0, 0, m_numSpeciesTot);
|
|
vcs_deltag(0, true);
|
|
}
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
int VCS_SOLVE::force(int iti)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* force:
|
|
*
|
|
* Convergence Forcer:
|
|
*
|
|
* This routine optimizes the minimization of the total gibbs free
|
|
* energy:
|
|
* Gibbs = sum_k( fe_k * w_k )
|
|
* along the current direction ds[], by choosing a value, al: (0<al<1)
|
|
* such that the a parabola approximation to Gibbs(al) fit to the
|
|
* end points al = 0 and al = 1 is minimizied.
|
|
* s1 = slope of Gibbs function at al = 0, which is the previous
|
|
* solution = d(Gibbs)/d(al).
|
|
* s2 = slope of Gibbs function at al = 1, which is the current
|
|
* solution = d(Gibbs)/d(al).
|
|
* Only if there has been an inflection point (i.e., s1 < 0 and s2 > 0),
|
|
* does this code section kick in. It finds the point on the parabola
|
|
* where the slope is equal to zero.
|
|
*
|
|
* NOTE: The algorithm used to find the slope is not quite accurate.
|
|
* The term, sum_k( (fe_k_n - fe_k_n-1) * w_k_n-1 )
|
|
* is dropped from s1, and, the term,
|
|
* sum_k( (fe_k_n - fe_k_n-1) * w_k_n ), is dropped from s2
|
|
*************************************************************************/
|
|
{
|
|
double s1, s2, al;
|
|
int i, iph;
|
|
double *dptr = VCS_DATA_PTR(m_gibbsSpecies);
|
|
//int numSpeciesRdc = m_numSpeciesRdc;
|
|
|
|
/* *************************************************** */
|
|
/* **** CALCULATE SLOPE AT END OF THE STEP ********** */
|
|
/* *************************************************** */
|
|
s2 = 0.0;
|
|
for (i = 0; i < m_numSpeciesRdc; ++i) {
|
|
s2 += dptr[i] * ds[i];
|
|
}
|
|
#ifdef DEBUG_NOT
|
|
if (s2 <= 0.0) {
|
|
#ifdef DEBUG_NOT
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- subroutine FORCE produced no adjustments,");
|
|
plogf(" failed s2 test\n");
|
|
}
|
|
#endif
|
|
return FALSE;
|
|
}
|
|
#endif
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- subroutine FORCE: End Slope = %g\n", s2);
|
|
}
|
|
#endif
|
|
/* *************************************************** */
|
|
/* **** CALCULATE ORIGINAL SLOPE ********************* */
|
|
/* ************************************************** */
|
|
s1 = 0.0;
|
|
dptr = VCS_DATA_PTR(fel);
|
|
for (i = 0; i < m_numSpeciesRdc; ++i) {
|
|
s1 += dptr[i] * ds[i];
|
|
}
|
|
#ifdef DEBUG_NOT
|
|
if (s1 >= 0.0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- subroutine FORCE produced no adjustments,");
|
|
plogf(" failed s1 test -PROBLEM!!\n");
|
|
}
|
|
#endif
|
|
return FALSE;
|
|
}
|
|
#endif
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- subroutine FORCE: Beginning Slope = %g\n", s1);
|
|
}
|
|
#endif
|
|
/* *************************************************** */
|
|
/* **** FIT PARABOLA ********************************* */
|
|
/* *************************************************** */
|
|
al = 1.0;
|
|
if (fabs(s1 -s2) > 1.0E-200) {
|
|
al = s1 / (s1 - s2);
|
|
}
|
|
if (al >= 0.95 || al < 0.0) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- subroutine FORCE produced no adjustments (al = %g)\n", al);
|
|
}
|
|
#endif
|
|
return FALSE;
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- subroutine FORCE produced a damping factor = %g\n", al);
|
|
}
|
|
#endif
|
|
/* *************************************************** */
|
|
/* **** ADJUST MOLE NUMBERS, CHEM. POT *************** */
|
|
/* *************************************************** */
|
|
dptr = VCS_DATA_PTR(soln);
|
|
for (i = 0; i < m_numSpeciesRdc; ++i) {
|
|
dptr[i] += al * ds[i];
|
|
}
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
TPhMoles[iph] += al * DelTPhMoles[iph];
|
|
}
|
|
vcs_updateVP(0);
|
|
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- subroutine FORCE adjusted the mole "
|
|
"numbers, AL = %10.3f\n", al);
|
|
}
|
|
#endif
|
|
/*
|
|
* Because we changed the mole numbers, we need to
|
|
* calculate the chemical potentials again. If a major-
|
|
* only step is being carried out, then we don't need to
|
|
* update the minor noncomponents.
|
|
*/
|
|
vcs_dfe(dptr, 0, iti, 0, m_numSpeciesRdc);
|
|
/*
|
|
* Evaluate DeltaG for all components if ITI=0, and for
|
|
* major components only if ITI NE 0
|
|
*/
|
|
vcs_deltag(iti, false);
|
|
return TRUE;
|
|
} /* force() *****************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*
|
|
* vcs_RxnStepSizes():
|
|
*
|
|
* Calculates formation reaction step sizes.
|
|
* This is equation 6.4-16, p. 143 in Smith and Missen.
|
|
*
|
|
* Output
|
|
* -------
|
|
* ds(I) : reaction adjustments, where I refers to the Ith species
|
|
* formation reaction. This is adjustment is for species
|
|
* i + M, where M is the number of components.
|
|
* Special branching occurs sometimes. This causes the component basis
|
|
* to be reevaluated
|
|
* return = 0 : normal return
|
|
* 1 : A single species phase species has been zeroed out
|
|
* in this routine. The species is a noncomponent
|
|
* 2 : Same as one but, the zeroed species is a component.
|
|
*/
|
|
int VCS_SOLVE::vcs_RxnStepSizes() {
|
|
int j, k, irxn, kspec, soldel = 0, iph;
|
|
double s, xx, dss;
|
|
vcs_VolPhase *Vphase = 0;
|
|
double *dnPhase_irxn;
|
|
#ifdef DEBUG
|
|
char ANOTE[128];
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" "); for (j = 0; j < 82; j++) plogf("-"); plogf("\n");
|
|
plogf(" --- Subroutine vcs_RxnStepSizes called - Details:\n");
|
|
plogf(" "); for (j = 0; j < 82; j++) plogf("-"); plogf("\n");
|
|
plogf(" --- Species Moles Rxn_Adjustment DeltaG"
|
|
" | Comment\n");
|
|
}
|
|
#endif
|
|
/*
|
|
* We update the matrix dlnActCoeffdmolNumber[][] at the
|
|
* top of the loop, when necessary
|
|
*/
|
|
if (UseActCoeffJac) {
|
|
vcs_CalcLnActCoeffJac(VCS_DATA_PTR(soln));
|
|
}
|
|
/************************************************************************
|
|
******** LOOP OVER THE FORMATION REACTIONS *****************************
|
|
************************************************************************/
|
|
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,"Normal Calc");
|
|
#endif
|
|
|
|
kspec = ir[irxn];
|
|
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
|
|
dnPhase_irxn = DnPhase[irxn];
|
|
|
|
if (soln[kspec] == 0.0 && (! SSPhase[kspec])) {
|
|
/********************************************************************/
|
|
/******* MULTISPECIES PHASE WITH total moles equal to zero *********/
|
|
/*******************************************************************/
|
|
/*
|
|
* If dg[irxn] is negative, then the multispecies phase should
|
|
* come alive again. Add a small positive step size to
|
|
* make it come alive.
|
|
*/
|
|
if (dg[irxn] < -1.0e-4) {
|
|
/*
|
|
* First decide if this species is part of a multiphase that
|
|
* is nontrivial in size.
|
|
*/
|
|
iph = PhaseID[kspec];
|
|
double tphmoles = TPhMoles[iph];
|
|
double trphmoles = tphmoles / TMoles;
|
|
if (trphmoles > VCS_DELETE_PHASE_CUTOFF) {
|
|
ds[kspec] = TMoles * VCS_SMALL_MULTIPHASE_SPECIES;
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,
|
|
"MultSpec: small species born again DG = %11.3E",
|
|
dg[irxn]);
|
|
#endif
|
|
} else {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "MultSpec: phase come alive DG = %11.3E", dg[irxn]);
|
|
#endif
|
|
Vphase = VPhaseList[iph];
|
|
int numSpPhase = Vphase->NVolSpecies;
|
|
ds[kspec] = TMoles * 10.0 * VCS_DELETE_PHASE_CUTOFF / numSpPhase;
|
|
}
|
|
--(m_numRxnMinorZeroed);
|
|
} else {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "MultSpec: still dead DG = %11.3E", dg[irxn]);
|
|
#endif
|
|
ds[kspec] = 0.0;
|
|
}
|
|
} else {
|
|
/********************************************************************/
|
|
/************************* REGULAR PROCESSING ************/
|
|
/********************************************************************/
|
|
/*
|
|
* First take care of cases where we want to bail out
|
|
*
|
|
*
|
|
* Don't bother if superconvergence has already been achieved
|
|
* in this mode.
|
|
*/
|
|
if (fabs(dg[irxn]) <= tolmaj2) {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,"Skipped: superconverged DG = %11.3E", dg[irxn]);
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- %-12.12s", SpName[kspec].c_str());
|
|
plogf(" %12.4E %12.4E %12.4E | %s\n",
|
|
soln[kspec], ds[kspec], dg[irxn], ANOTE);
|
|
}
|
|
#endif
|
|
continue;
|
|
}
|
|
/*
|
|
* Don't calculate for minor or nonexistent species if
|
|
* their values are to be decreasing anyway.
|
|
*/
|
|
if ((spStatus[irxn] != VCS_SPECIES_MAJOR) && (dg[irxn] >= 0.0)) {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE,"Skipped: IC = %3d and DG >0: %11.3E",
|
|
spStatus[irxn], dg[irxn]);
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- %-12.12s", SpName[kspec].c_str());
|
|
plogf(" %12.4E %12.4E %12.4E | %s\n",
|
|
soln[kspec], ds[kspec], dg[irxn], ANOTE);
|
|
}
|
|
#endif
|
|
continue;
|
|
}
|
|
/*
|
|
* Start of the regular processing
|
|
*/
|
|
if (SSPhase[kspec]) {
|
|
s = 0.0;
|
|
} else {
|
|
s = 1.0 / soln[kspec] ;
|
|
}
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
if (!SSPhase[j]) {
|
|
if (soln[j] > 0.0) {
|
|
s += SQUARE(sc[irxn][j]) / soln[j];
|
|
}
|
|
}
|
|
}
|
|
for (j = 0; j < NPhase; j++) {
|
|
Vphase = VPhaseList[j];
|
|
if (! Vphase->SingleSpecies) {
|
|
if (TPhMoles[j] > 0.0)
|
|
s -= SQUARE(dnPhase_irxn[j]) / TPhMoles[j];
|
|
}
|
|
}
|
|
if (s != 0.0) {
|
|
/*
|
|
* Take into account of the
|
|
* derivatives of the activity coefficients with respect to the
|
|
* mole numbers, even in our diagonal approximation.
|
|
*/
|
|
if (UseActCoeffJac) {
|
|
double s_old = s;
|
|
s = vcs_Hessian_diag_adj(irxn, s_old);
|
|
#ifdef DEBUG
|
|
if (s_old != s) {
|
|
sprintf(ANOTE, "Normal calc: diag adjusted from %g "
|
|
"to %g due to act coeff", s_old, s);
|
|
}
|
|
#endif
|
|
}
|
|
|
|
ds[kspec] = -dg[irxn] / s;
|
|
// New section to do damping of the ds[]
|
|
/*
|
|
*
|
|
*/
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
double stoicC = sc[irxn][j];
|
|
if (stoicC != 0.0) {
|
|
double negChangeComp = - stoicC * ds[kspec];
|
|
if (negChangeComp > soln[j]) {
|
|
if (soln[j] > 0.0) {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "Delta damped from %g "
|
|
"to %g due to component %d (%10s) going neg", ds[kspec],
|
|
-soln[j]/stoicC, j, SpName[j].c_str());
|
|
#endif
|
|
ds[kspec] = - soln[j] / stoicC;
|
|
} else {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "Delta damped from %g "
|
|
"to %g due to component %d (%10s) zero", ds[kspec],
|
|
-soln[j]/stoicC, j, SpName[j].c_str());
|
|
#endif
|
|
ds[kspec] = 0.0;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
// Implement a damping term that limits ds to the size of the mole number
|
|
if (-ds[kspec] > soln[kspec]) {
|
|
#ifdef DEBUG
|
|
sprintf(ANOTE, "Delta damped from %g "
|
|
"to %g due to %s going negative", ds[kspec],
|
|
-soln[kspec], SpName[kspec].c_str());
|
|
#endif
|
|
ds[kspec] = -soln[kspec];
|
|
}
|
|
|
|
} else {
|
|
/* ************************************************************ */
|
|
/* **** REACTION IS ENTIRELY AMONGST SINGLE SPECIES PHASES **** */
|
|
/* **** DELETE ONE OF THE PHASES AND RECOMPUTE BASIS ********* */
|
|
/* ************************************************************ */
|
|
/*
|
|
* Either the species L will disappear or one of the
|
|
* component single species phases will disappear. The sign
|
|
* of DG(I) will indicate which way the reaction will go.
|
|
* Then, we need to follow the reaction to see which species
|
|
* will zero out first.
|
|
* -> The species to be zeroed out will be "k".
|
|
*/
|
|
if (dg[irxn] > 0.0) {
|
|
dss = soln[kspec];
|
|
k = kspec;
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
if (sc[irxn][j] > 0.0) {
|
|
xx = soln[j] / sc[irxn][j];
|
|
if (xx < dss) {
|
|
dss = xx;
|
|
k = j;
|
|
}
|
|
}
|
|
}
|
|
dss = -dss;
|
|
} else {
|
|
dss = 1.0e10;
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
if (sc[irxn][j] < 0.0) {
|
|
xx = -soln[j] / sc[irxn][j];
|
|
if (xx < dss) {
|
|
dss = xx;
|
|
k = j;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* Here we adjust the mole fractions
|
|
* according to DSS and the stoichiometric array
|
|
* to take into account that we are eliminating
|
|
* the kth species. DSS contains the amount
|
|
* of moles of the kth species that needs to be
|
|
* added back into the component species.
|
|
*/
|
|
if (dss != 0.0) {
|
|
soln[kspec] += dss;
|
|
TPhMoles[PhaseID[kspec]] += dss;
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
soln[j] += dss * sc[irxn][j];
|
|
TPhMoles[PhaseID[j]] += dss * sc[irxn][j];
|
|
}
|
|
soln[k] = 0.0;
|
|
iph = PhaseID[k];
|
|
Vphase = VPhaseList[iph];
|
|
Vphase->Existence = 0;
|
|
TPhMoles[iph] = 0.0;
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- vcs_RxnStepSizes Special section to delete %s\n",
|
|
SpName[k].c_str());
|
|
plogf(" --- Immediate return - Restart iteration\n");
|
|
}
|
|
#endif
|
|
/*
|
|
* We need to immediately recompute the
|
|
* component basis, because we just zeroed
|
|
* it out.
|
|
*/
|
|
if (k != kspec) soldel = 2;
|
|
else soldel = 1;
|
|
return soldel;
|
|
}
|
|
}
|
|
} /* End of regular processing */
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- %-12.12s", SpName[kspec].c_str());
|
|
plogf(" %12.4E %12.4E %12.4E | %s\n",
|
|
soln[kspec], ds[kspec], dg[irxn], ANOTE);
|
|
}
|
|
#endif
|
|
} /* End of loop over SpeciesUnknownType */
|
|
} /* End of loop over non-component stoichiometric formation reactions */
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" "); vcs_print_line("-", 82);
|
|
}
|
|
#endif
|
|
return soldel;
|
|
}
|
|
/*****************************************************************************/
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_deltag:
|
|
*
|
|
* This subroutine calculates reaction free energy changes for
|
|
* all noncomponent formation reactions. Formation reactions are
|
|
* reactions which create each noncomponent species from the component
|
|
* species. SC(J,I) are the stoichiometric coefficients for these
|
|
* reactions. A stoichiometric coefficient of one is assumed for
|
|
* species I in this reaction.
|
|
*
|
|
* INPUT
|
|
* L = < 0 : Calculate reactions corresponding to
|
|
* major noncomponent and zeroed species only
|
|
* L = 0 : Do all noncomponent reactions, i, between
|
|
* 0 <= i < irxnl
|
|
* L > 0 : Calculate reactions corresponding to
|
|
* minor noncomponent and zeroed species only
|
|
* irxnl : used with L = 0 to indicate upper limit.
|
|
*
|
|
* Note we special case one important issue.
|
|
* If the component has zero moles, then we do not
|
|
* allow deltaG < 0.0 for formation reactions which
|
|
* would lead to the loss of more of the component.
|
|
* This dG < 0.0 feeds back into the algorithm in several
|
|
* places, and leads to a infinite loop in at least one case.
|
|
*/
|
|
void VCS_SOLVE::vcs_deltag(int l, bool doDeleted) {
|
|
int iph;
|
|
int lneed, irxn, kspec;
|
|
double *dtmp_ptr;
|
|
int icase = 0;
|
|
int irxnl = m_numRxnRdc;
|
|
if (doDeleted) {
|
|
irxnl = m_numRxnTot;
|
|
}
|
|
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Subroutine vcs_deltag called for ");
|
|
if (l < 0) {
|
|
plogf("major noncomponents\n");
|
|
} else if (l == 0) {
|
|
plogf("all noncomponents\n");
|
|
} else {
|
|
plogf("minor noncomponents\n");
|
|
}
|
|
}
|
|
#endif
|
|
/* ************************************************* */
|
|
/* **** MAJORS and ZEREOD SPECIES ONLY ************* */
|
|
/* ************************************************* */
|
|
if (l < 0) {
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
if (spStatus[irxn] != VCS_SPECIES_MINOR) {
|
|
icase = 0;
|
|
dg[irxn] = m_gibbsSpecies[ir[irxn]];
|
|
dtmp_ptr = sc[irxn];
|
|
for (kspec = 0; kspec < m_numComponents; ++kspec) {
|
|
dg[irxn] += dtmp_ptr[kspec] * m_gibbsSpecies[kspec];
|
|
if (soln[kspec] < VCS_DELETE_MINORSPECIES_CUTOFF && dtmp_ptr[kspec] < 0.0) {
|
|
icase = 1;
|
|
}
|
|
}
|
|
if (icase) {
|
|
dg[irxn] = MAX(0.0, dg[irxn]);
|
|
}
|
|
}
|
|
}
|
|
} else if (l == 0) {
|
|
/* ************************************************* */
|
|
/* **** ALL REACTIONS ****************************** */
|
|
/* ************************************************* */
|
|
for (irxn = 0; irxn < irxnl; ++irxn) {
|
|
icase = 0;
|
|
dg[irxn] = m_gibbsSpecies[ir[irxn]];
|
|
dtmp_ptr = sc[irxn];
|
|
for (kspec = 0; kspec < m_numComponents; ++kspec) {
|
|
dg[irxn] += dtmp_ptr[kspec] * m_gibbsSpecies[kspec];
|
|
if (soln[kspec] < VCS_DELETE_MINORSPECIES_CUTOFF && dtmp_ptr[kspec] < 0.0) {
|
|
icase = 1;
|
|
}
|
|
}
|
|
if (icase) {
|
|
dg[irxn] = MAX(0.0, dg[irxn]);
|
|
}
|
|
}
|
|
} else {
|
|
/* ************************************************* */
|
|
/* **** MINORS AND ZEROED SPECIES ****************** */
|
|
/* ************************************************* */
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
if (spStatus[irxn] <= VCS_SPECIES_MINOR) {
|
|
icase = 0;
|
|
dg[irxn] = m_gibbsSpecies[ir[irxn]];
|
|
dtmp_ptr = sc[irxn];
|
|
for (kspec = 0; kspec < m_numComponents; ++kspec) {
|
|
dg[irxn] += dtmp_ptr[kspec] * m_gibbsSpecies[kspec];
|
|
if (soln[kspec] < VCS_DELETE_MINORSPECIES_CUTOFF && dtmp_ptr[kspec] < 0.0) {
|
|
icase = 1;
|
|
}
|
|
}
|
|
if (icase) {
|
|
dg[irxn] = MAX(0.0, dg[irxn]);
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/* ************************************************* */
|
|
/* **** MULTISPECIES PHASES WITH ZERO MOLES************ */
|
|
/* ************************************************* */
|
|
/*
|
|
* Massage the free energies for species with zero mole fractions
|
|
* in multispecies phases. This section implements the
|
|
* Equation 3.8-5 in Smith and Missen, p.59.
|
|
* A multispecies phase will exist iff
|
|
* 1 < sum_i(exp(-dg_i)/AC_i)
|
|
* If DG is negative then that species wants to be reintroduced into
|
|
* the calculation.
|
|
* For small dg_i, the expression below becomes:
|
|
* 1 - sum_i(exp(-dg_i)/AC_i) ~ sum_i((dg_i-1)/AC_i) + 1
|
|
*
|
|
* So, what we are doing here is equalizing all DG's in a multispecies
|
|
* phase whose total mole number has already been zeroed out.
|
|
* It must have to do with the case where a complete multispecies
|
|
* phase is currently zeroed out. In that case, when one species
|
|
* in that phase has a negative DG, then the phase should kick in.
|
|
* This code section will cause that to happen, because a negative
|
|
* DG will dominate the calculation of SDEL. Then, DG(I) for all
|
|
* species in that phase will be forced to be equal and negative.
|
|
* Thus, all species in that phase will come into being at the
|
|
* same time.
|
|
*
|
|
* HKM -> The ratio of mole fractions at the reinstatement
|
|
* time should be equal to the normalized weighting
|
|
* of exp(-dg_i) / AC_i. This should be implemented.
|
|
*
|
|
* HKM -> There is circular logic here. ActCoeff depends on the
|
|
* mole fractions of a phase that does not exist. In actuality
|
|
* the proto-mole fractions should be selected from the
|
|
* solution of a nonlinear problem with NsPhase unknowns
|
|
*
|
|
* X_i = exp(-dg[irxn]) / ActCoeff_i / denom
|
|
*
|
|
* where
|
|
* denom = sum_i[ exp(-dg[irxn]) / ActCoeff_i ]
|
|
*
|
|
* This can probably be solved by successive iteration.
|
|
* This should be implemented.
|
|
*/
|
|
int k;
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
lneed = FALSE;
|
|
vcs_VolPhase *Vphase = VPhaseList[iph];
|
|
if (! Vphase->SingleSpecies) {
|
|
double sum = 0.0;
|
|
for (k = 0; k < Vphase->NVolSpecies; k++) {
|
|
kspec = Vphase->IndSpecies[k];
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
sum += soln[kspec];
|
|
}
|
|
if (sum > 0.0) break;
|
|
}
|
|
if (sum == 0.0) {
|
|
lneed = TRUE;
|
|
}
|
|
}
|
|
|
|
if (lneed) {
|
|
double poly = 0.0;
|
|
for (k = 0; k < Vphase->NVolSpecies; k++) {
|
|
kspec = Vphase->IndSpecies[k];
|
|
irxn = kspec - m_numComponents;
|
|
if (dg[irxn] > 50.0) dg[irxn] = 50.0;
|
|
if (dg[irxn] < -50.0) dg[irxn] = -50.0;
|
|
poly += exp(-dg[irxn])/ActCoeff[kspec];
|
|
}
|
|
/*
|
|
* Calculate dg[] for each species in a zeroed multispecies phase.
|
|
* All of the dg[]'s will be equal. If dg[] is negative, then
|
|
* the phase will come back into existence.
|
|
*/
|
|
for (k = 0; k < Vphase->NVolSpecies; k++) {
|
|
kspec = Vphase->IndSpecies[k];
|
|
irxn = kspec - m_numComponents;
|
|
dg[irxn] = 1.0 - poly;
|
|
}
|
|
|
|
}
|
|
}
|
|
|
|
|
|
#ifdef DEBUG_NOT
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
checkFinite(dg[irxn]);
|
|
}
|
|
#endif
|
|
} /* vcs_deltag() ************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
int VCS_SOLVE::vcs_basopt(int ifirst, double aw[], double sa[], double sm[],
|
|
double ss[], double test, int *usedZeroedSpecies)
|
|
|
|
/**************************************************************************
|
|
* Choose the optimum basis for the calculations. This is done by
|
|
* choosing the species with the largest mole fraction
|
|
* not currently a linear combination of the previous components.
|
|
* Then, calculate the stoichiometric coefficient matrix for that
|
|
* basis.
|
|
*
|
|
* Calculates the identity of the component species in the mechanism.
|
|
* Rearranges the solution data to put the component data at the
|
|
* front of the species list.
|
|
*
|
|
* Then, calculates SC(J,I) the formation reactions for all noncomponent
|
|
*
|
|
* species in the mechanism.
|
|
* Also calculates DNG(I) and DNL(I), the net mole change for each
|
|
* formation reaction.
|
|
* Also, initializes IR(I) to the default state.
|
|
*
|
|
* Input
|
|
* ---------
|
|
* IFIRST = If true, the SC, DNG, and DNL are not calculated.
|
|
* TEST = This is a small negative number dependent upon whether
|
|
* an estimate is supplied or not.
|
|
* W(I) = Mole fractions which will be used to construct an
|
|
* optimal basis from.
|
|
*
|
|
* Output
|
|
* ---------
|
|
* usedZeroedSpecies = If true, then a species with a zero concentration
|
|
* was used as a component. The problem may be
|
|
* converged.
|
|
*
|
|
* Other Variables
|
|
* aw[i] = Mole fraction work space (# species in length)
|
|
* sa[j] = Gramm-Schmidt orthog work space (nc in length)
|
|
* ss[j] = Gramm-Schmidt orthog work space (nc in length)
|
|
* sm[i+j*ne] = QR matrix work space (nc*ne in length)
|
|
*
|
|
*************************************************************************/
|
|
{
|
|
int j, k, l, i, jl, ml, jr, lindep, irxn, kspec;
|
|
int ncTrial;
|
|
int juse = -1;
|
|
int jlose = -1;
|
|
double *dptr, *scrxn_ptr;
|
|
double tsecond = vcs_second();
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" "); for(i=0; i<77; i++) plogf("-"); plogf("\n");
|
|
plogf(" --- Subroutine BASOPT called to ");
|
|
if (ifirst) plogf("calculate the number of components\n");
|
|
else plogf("reevaluate the components\n");
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf("\n");
|
|
plogf(" --- Formula Matrix used in BASOPT calculation\n");
|
|
plogf(" --- Active | ");
|
|
for (j = 0; j < m_numElemConstraints; j++) {
|
|
plogf(" %1d ", ElActive[j]);
|
|
}
|
|
plogf("\n");
|
|
plogf(" --- Species | ");
|
|
for (j = 0; j < m_numElemConstraints; j++) {
|
|
plogf(" ");
|
|
vcs_print_stringTrunc(ElName[j].c_str(), 4, 1);
|
|
}
|
|
plogf("\n");
|
|
for (k = 0; k < m_numSpeciesTot; k++) {
|
|
plogf(" --- ");
|
|
vcs_print_stringTrunc(SpName[k].c_str(), 11, 1);
|
|
plogf(" | ");
|
|
for (j = 0; j < m_numElemConstraints; j++) {
|
|
plogf("%5.1g", FormulaMatrix[j][k]);
|
|
}
|
|
plogf("\n");
|
|
}
|
|
plogf("\n");
|
|
}
|
|
}
|
|
#endif
|
|
|
|
/*
|
|
* Calculate the maximum value of the number of components possible
|
|
* It's equal to the minimum of the number of elements and the
|
|
* number of total species.
|
|
*/
|
|
ncTrial = MIN(m_numElemConstraints, m_numSpeciesTot);
|
|
m_numComponents = ncTrial;
|
|
*usedZeroedSpecies = FALSE;
|
|
|
|
/*
|
|
* Use a temporary work array for the mole numbers, aw[]
|
|
*/
|
|
vcs_dcopy(aw, VCS_DATA_PTR(soln), m_numSpeciesTot);
|
|
/*
|
|
* Take out the Voltage unknowns from consideration
|
|
*/
|
|
for (k = 0; k < m_numSpeciesTot; k++) {
|
|
if (SpeciesUnknownType[k] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
aw[k] = test;
|
|
}
|
|
}
|
|
|
|
jr = -1;
|
|
/*
|
|
* Top of a loop of some sort based on the index JR. JR is the
|
|
* current number of component species found.
|
|
*/
|
|
do {
|
|
++jr;
|
|
/* - Top of another loop point based on finding a linearly */
|
|
/* - independent species */
|
|
do {
|
|
/*
|
|
* Search the remaining part of the mole fraction vector, AW,
|
|
* for the largest remaining species. Return its identity in K.
|
|
* The first search criteria is always the largest positive
|
|
* magnitude of the mole number.
|
|
*/
|
|
k = vcs_amax(aw, jr, m_numSpeciesTot);
|
|
/*
|
|
* The fun really starts when you have run out of species that have a significant
|
|
* concentration. It becomes extremely important to make a good choice of which
|
|
* species you want to pick to fill out the basis. Basically, you don't want to
|
|
* use species with elements abundances which aren't pegged to zero. This means
|
|
* that those modes will never be allowed to grow. You want to have the
|
|
* best chance that the component will grow positively.
|
|
*
|
|
* Suppose you start with CH4, N2, as the only species with nonzero compositions.
|
|
* You have the following abundances:
|
|
*
|
|
* Abundances:
|
|
* ----------------
|
|
* C 2.0
|
|
* N 2.0
|
|
* H 4.0
|
|
* O 0.0
|
|
*
|
|
* For example, Make the following choice:
|
|
*
|
|
* CH4 N2 O choose -> OH
|
|
* or
|
|
* CH4 N2 O choose -> H2
|
|
*
|
|
* OH and H2 both fill out the basis. They will pass the algorithm. However,
|
|
* choosing OH as the next species will create a situation where H2 can not
|
|
* grow in concentration. This happened in practice, btw. The reason is that
|
|
* the formation reaction for H2 will cause one of the component species
|
|
* to go negative.
|
|
*
|
|
* The basic idea here is to pick a simple species whose mole number
|
|
* can grow according to the element compositions. Candidates are still
|
|
* filtered according to their linear independence.
|
|
*
|
|
* Note, if there is electronic charge and the electron species,
|
|
* you should probably pick the electron as a component, if it
|
|
* linearly independent. The algorithm below will do this automagically.
|
|
*
|
|
*/
|
|
if ((aw[k] != test) && aw[k] < VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
*usedZeroedSpecies = TRUE;
|
|
|
|
double maxConcPossKspec = 0.0;
|
|
double maxConcPoss = 0.0;
|
|
int kfound = -1;
|
|
int minNonZeroes = 100000;
|
|
int nonZeroesKspec = 0;
|
|
for (kspec = ncTrial; kspec < m_numSpeciesTot; kspec++) {
|
|
if (aw[kspec] >= 0.0) {
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
maxConcPossKspec = 1.0E10;
|
|
nonZeroesKspec = 0;
|
|
for (int j = 0; j < m_numElemConstraints; ++j) {
|
|
if (ElActive[j]) {
|
|
if (m_elType[j] == VCS_ELEM_TYPE_ABSPOS) {
|
|
double nu = FormulaMatrix[j][kspec];
|
|
if (nu != 0.0) {
|
|
nonZeroesKspec++;
|
|
maxConcPossKspec = MIN(gai[j] / nu, maxConcPossKspec);
|
|
}
|
|
}
|
|
}
|
|
}
|
|
if ((maxConcPossKspec >= maxConcPoss) || (maxConcPossKspec > 1.0E-5)) {
|
|
if (nonZeroesKspec <= minNonZeroes) {
|
|
if (kfound < 0 || nonZeroesKspec < minNonZeroes) {
|
|
kfound = kspec;
|
|
} else {
|
|
// ok we are sitting pretty equal here decide on the raw ss Gibbs energy
|
|
if (ff[kspec] <= ff[kfound]) {
|
|
kfound = kspec;
|
|
}
|
|
}
|
|
}
|
|
if (nonZeroesKspec < minNonZeroes) {
|
|
minNonZeroes = nonZeroesKspec;
|
|
}
|
|
if (maxConcPossKspec > maxConcPoss) {
|
|
maxConcPoss = maxConcPossKspec;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
if (kfound == -1) {
|
|
double gmin = 0.0;
|
|
kfound = k;
|
|
for (kspec = ncTrial; kspec < m_numSpeciesTot; kspec++) {
|
|
if (aw[kspec] >= 0.0) {
|
|
irxn = kspec - ncTrial;
|
|
if (dg[irxn] < gmin) {
|
|
gmin = dg[irxn];
|
|
kfound = kspec;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
k = kfound;
|
|
}
|
|
|
|
|
|
if (aw[k] == test) {
|
|
m_numComponents = jr;
|
|
ncTrial = m_numComponents;
|
|
int numPreDeleted = m_numRxnTot - m_numRxnRdc;
|
|
if (numPreDeleted != (m_numSpeciesTot - m_numSpeciesRdc)) {
|
|
plogf("we shouldn't be here\n");
|
|
exit(-1);
|
|
}
|
|
m_numRxnTot = m_numSpeciesTot - ncTrial;
|
|
m_numRxnRdc = m_numRxnTot - numPreDeleted;
|
|
m_numSpeciesRdc = m_numSpeciesTot - numPreDeleted;
|
|
for (i = 0; i < m_numSpeciesTot; ++i) {
|
|
ir[i] = ncTrial + i;
|
|
}
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Total number of components found = %3d (ne = %d)\n ",
|
|
ncTrial, m_numElemConstraints);
|
|
}
|
|
#endif
|
|
goto L_END_LOOP;
|
|
}
|
|
/*
|
|
* Assign a small negative number to the component that we have
|
|
* just found, in order to take it out of further consideration.
|
|
*/
|
|
aw[k] = test;
|
|
/* *********************************************************** */
|
|
/* **** CHECK LINEAR INDEPENDENCE WITH PREVIOUS SPECIES ****** */
|
|
/* *********************************************************** */
|
|
/*
|
|
* Modified Gram-Schmidt Method, p. 202 Dalquist
|
|
* QR factorization of a matrix without row pivoting.
|
|
*/
|
|
jl = jr;
|
|
for (j = 0; j < m_numElemConstraints; ++j) {
|
|
sm[j + jr*m_numElemConstraints] = FormulaMatrix[j][k];
|
|
}
|
|
if (jl > 0) {
|
|
/*
|
|
* Compute the coefficients of JA column of the
|
|
* the upper triangular R matrix, SS(J) = R_J_JR
|
|
* (this is slightly different than Dalquist)
|
|
* R_JA_JA = 1
|
|
*/
|
|
for (j = 0; j < jl; ++j) {
|
|
ss[j] = 0.0;
|
|
for (i = 0; i < m_numElemConstraints; ++i) {
|
|
ss[j] += sm[i + jr*m_numElemConstraints] * sm[i + j*m_numElemConstraints];
|
|
}
|
|
ss[j] /= sa[j];
|
|
}
|
|
/*
|
|
* Now make the new column, (*,JR), orthogonal to the
|
|
* previous columns
|
|
*/
|
|
for (j = 0; j < jl; ++j) {
|
|
for (l = 0; l < m_numElemConstraints; ++l) {
|
|
sm[l + jr*m_numElemConstraints] -= ss[j] * sm[l + j*m_numElemConstraints];
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* Find the new length of the new column in Q.
|
|
* It will be used in the denominator in future row calcs.
|
|
*/
|
|
sa[jr] = 0.0;
|
|
for (ml = 0; ml < m_numElemConstraints; ++ml) {
|
|
sa[jr] += SQUARE(sm[ml + jr*m_numElemConstraints]);
|
|
}
|
|
/* **************************************************** */
|
|
/* **** IF NORM OF NEW ROW .LT. 1E-3 REJECT ********** */
|
|
/* **************************************************** */
|
|
if (sa[jr] < 1.0e-6) lindep = TRUE;
|
|
else lindep = FALSE;
|
|
} while(lindep);
|
|
/* ****************************************** */
|
|
/* **** REARRANGE THE DATA ****************** */
|
|
/* ****************************************** */
|
|
if (jr != k) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- %-12.12s", (SpName[k]).c_str());
|
|
plogf("(%9.2g) replaces %-12.12s", soln[k], SpName[jr].c_str());
|
|
plogf("(%9.2g) as component %3d\n", soln[jr], jr);
|
|
}
|
|
#endif
|
|
vcs_switch_pos(FALSE, jr, k);
|
|
vcsUtil_dsw(aw, jr, k);
|
|
}
|
|
#ifdef DEBUG
|
|
else {
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- %-12.12s", SpName[k].c_str());
|
|
plogf("(%9.2g) remains ", soln[k]);
|
|
plogf(" as component %3d\n", jr);
|
|
}
|
|
}
|
|
#endif
|
|
/* - entry point from up above */
|
|
L_END_LOOP: ;
|
|
/*
|
|
* If we haven't found enough components, go back
|
|
* and find some more. (nc -1 is used below, because
|
|
* jr is counted from 0, via the C convention.
|
|
*/
|
|
} while (jr < (ncTrial-1));
|
|
|
|
if (ifirst) goto L_CLEANUP;
|
|
/* ****************************************************** */
|
|
/* **** EVALUATE THE STOICHIOMETRY ********************** */
|
|
/* ****************************************************** */
|
|
/*
|
|
* Formulate the matrix problem for the stoichiometric
|
|
* coefficients. CX + B = 0
|
|
* C will be an nc x nc matrix made up of the formula
|
|
* vectors for the components.
|
|
* n rhs's will be solved for. Thus, B is an nc x n
|
|
* matrix.
|
|
*
|
|
* BIG PROBLEM 1/21/99:
|
|
*
|
|
* This algorithm makes the assumption that the
|
|
* first nc rows of the formula matrix aren't rank deficient.
|
|
* However, this might not be the case. For example, assume
|
|
* that the first element in FormulaMatrix[] is argon. Assume that
|
|
* no species in the matrix problem actually includes argon.
|
|
* Then, the first row in sm[], below will be indentically
|
|
* zero. bleh.
|
|
* What needs to be done is to perform a rearrangement
|
|
* of the ELEMENTS -> i.e. rearrange, FormulaMatrix, sp, and gai, such
|
|
* that the first nc elements form in combination with the
|
|
* nc components create an invertible sm[]. not a small
|
|
* project, but very doable.
|
|
* An alternative would be to turn the matrix problem
|
|
* below into an ne x nc problem, and do QR elimination instead
|
|
* of Gauss-Jordon elimination.
|
|
* Note the rearrangement of elements need only be done once
|
|
* in the problem. It's actually very similar to the top of
|
|
* this program with ne being the species and nc being the
|
|
* elements!!
|
|
*/
|
|
for (j = 0; j < ncTrial; ++j) {
|
|
for (i = 0; i < ncTrial; ++i) {
|
|
sm[i + j*m_numElemConstraints] = FormulaMatrix[i][j];
|
|
}
|
|
}
|
|
for (i = 0; i < m_numRxnTot; ++i) {
|
|
k = ir[i];
|
|
for (j = 0; j < ncTrial; ++j) {
|
|
sc[i][j] = FormulaMatrix[j][k];
|
|
}
|
|
}
|
|
/*
|
|
* Use Gauss-Jordon block elimination to calculate
|
|
* the reaction matrix, sc[][].
|
|
*/
|
|
j = vcsUtil_mlequ(sm, m_numElemConstraints, ncTrial, sc[0], m_numRxnTot);
|
|
if (j == 1) {
|
|
plogf("vcs_solve_TP ERROR: mlequ returned an error condition\n");
|
|
return VCS_FAILED_CONVERGENCE;
|
|
}
|
|
|
|
/*
|
|
* NOW, if we have interfacial voltage unknowns, what we did
|
|
* was just wrong -> hopefully it didn't blow up. Redo the problem.
|
|
* Search for inactive E
|
|
*/
|
|
juse = -1;
|
|
jlose = -1;
|
|
for (j = 0; j < m_numElemConstraints; j++) {
|
|
if (! (ElActive[j])) {
|
|
if (!strcmp((ElName[j]).c_str(), "E")) {
|
|
juse = j;
|
|
}
|
|
}
|
|
}
|
|
for (j = 0; j < m_numElemConstraints; j++) {
|
|
if (ElActive[j]) {
|
|
if (!strncmp((ElName[j]).c_str(), "cn_", 3)) {
|
|
jlose = j;
|
|
}
|
|
}
|
|
}
|
|
for (k = 0; k < m_numSpeciesTot; k++) {
|
|
if (SpeciesUnknownType[k] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
|
|
for (j = 0; j < ncTrial; ++j) {
|
|
for (i = 0; i < ncTrial; ++i) {
|
|
if (i == jlose) {
|
|
sm[i + j*m_numElemConstraints] = FormulaMatrix[juse][j];
|
|
} else {
|
|
sm[i + j*m_numElemConstraints] = FormulaMatrix[i][j];
|
|
}
|
|
}
|
|
}
|
|
for (i = 0; i < m_numRxnTot; ++i) {
|
|
k = ir[i];
|
|
for (j = 0; j < ncTrial; ++j) {
|
|
if (j == jlose) {
|
|
aw[j] = FormulaMatrix[juse][k];
|
|
} else {
|
|
aw[j] = FormulaMatrix[j][k];
|
|
}
|
|
}
|
|
}
|
|
j = vcsUtil_mlequ(sm, m_numElemConstraints, ncTrial, aw, 1);
|
|
if (j == 1) {
|
|
plogf("vcs_solve_TP ERROR: mlequ returned an error condition\n");
|
|
return VCS_FAILED_CONVERGENCE;
|
|
}
|
|
i = k - ncTrial;
|
|
for (j = 0; j < ncTrial; j++) {
|
|
sc[i][j] = aw[j];
|
|
}
|
|
}
|
|
}
|
|
|
|
|
|
/*
|
|
* Calculate the szTmp array for each formation reaction
|
|
*/
|
|
for (i = 0; i < m_numRxnTot; i++) {
|
|
double szTmp = 0.0;
|
|
for (j = 0; j < ncTrial; j++) {
|
|
szTmp += fabs(sc[i][j]);
|
|
}
|
|
scSize[i] = szTmp;
|
|
}
|
|
|
|
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Components:");
|
|
for (j = 0; j < ncTrial; j++) {
|
|
plogf(" %3d ", j);
|
|
}
|
|
plogf("\n --- Components Moles:");
|
|
for (j = 0; j < ncTrial; j++) {
|
|
plogf("%10.3g", soln[j]);
|
|
}
|
|
plogf("\n --- NonComponent| Moles | ");
|
|
for (j = 0; j < ncTrial; j++) {
|
|
plogf("%-10.10s", SpName[j].c_str());
|
|
}
|
|
//plogf("| scSize");
|
|
plogf("\n");
|
|
for (i = 0; i < m_numRxnTot; i++) {
|
|
plogf(" --- %3d ", ir[i]);
|
|
plogf("%-10.10s", SpName[ir[i]].c_str());
|
|
plogf("|%10.3g|", soln[ir[i]]);
|
|
for (j = 0; j < ncTrial; j++) {
|
|
plogf(" %6.2f", sc[i][j]);
|
|
}
|
|
//plogf(" | %6.2f", scSize[i]);
|
|
plogf("\n");
|
|
}
|
|
plogf(" "); for(i=0; i<77; i++) plogf("-"); plogf("\n");
|
|
}
|
|
#endif
|
|
/* **************************************************** */
|
|
/* **** EVALUATE DELTA N VALUES *********************** */
|
|
/* **************************************************** */
|
|
/*
|
|
* Evaluate the change in gas and liquid total moles
|
|
* due to reaction vectors, DNG and DNL.
|
|
*/
|
|
|
|
/*
|
|
* Zero out the change of Phase Moles array
|
|
*/
|
|
vcs_dzero(DnPhase[0], (NSPECIES0)*(NPHASE0));
|
|
vcs_izero(PhaseParticipation[0], (NSPECIES0)*(NPHASE0));
|
|
/*
|
|
* Loop over each reaction, creating the change in Phase Moles
|
|
* array, DnPhase[irxn][iphase],
|
|
* and the phase participation array, PhaseParticipation[irxn][iphase]
|
|
*/
|
|
for (irxn = 0; irxn < m_numRxnTot; ++irxn) {
|
|
scrxn_ptr = sc[irxn];
|
|
dptr = DnPhase[irxn];
|
|
kspec = ir[irxn];
|
|
int iph = PhaseID[kspec];
|
|
int *pp_ptr = PhaseParticipation[irxn];
|
|
dptr[iph] = 1.0;
|
|
pp_ptr[iph]++;
|
|
for (j = 0; j < ncTrial; ++j) {
|
|
iph = PhaseID[j];
|
|
if (fabs(scrxn_ptr[j]) <= 1.0e-6) {
|
|
scrxn_ptr[j] = 0.0;
|
|
} else {
|
|
dptr[iph] += scrxn_ptr[j];
|
|
pp_ptr[iph]++;
|
|
}
|
|
}
|
|
}
|
|
|
|
L_CLEANUP: ;
|
|
tsecond = vcs_second() - tsecond;
|
|
m_VCount->Time_basopt += tsecond;
|
|
(m_VCount->Basis_Opts)++;
|
|
return VCS_SUCCESS;
|
|
} /* vcs_basopt() ************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
int VCS_SOLVE::vcs_species_type(int kspec)
|
|
|
|
/*************************************************************************
|
|
*
|
|
* vcs_species_type:
|
|
*
|
|
* Evaluate the species category for the input species
|
|
* return the type in the return variable
|
|
*************************************************************************/
|
|
{
|
|
int irxn = kspec - m_numComponents;
|
|
int iph, k;
|
|
|
|
if (kspec < m_numComponents) return VCS_SPECIES_COMPONENT;
|
|
if (SpeciesUnknownType[kspec] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
return VCS_SPECIES_INTERFACIALVOLTAGE;
|
|
}
|
|
iph = PhaseID[kspec];
|
|
if (soln[kspec] <= 0.0) {
|
|
if (dg[irxn] >= 0.0) {
|
|
/*
|
|
* We are here when the species is or should be zeroed out
|
|
*/
|
|
if (SSPhase[kspec]) {
|
|
return VCS_SPECIES_ZEROEDSS;
|
|
} else {
|
|
if (TPhMoles[iph] == 0.0) return VCS_SPECIES_ZEROEDPHASE;
|
|
else return VCS_SPECIES_ZEROEDMS;
|
|
}
|
|
}
|
|
/*
|
|
* The Gibbs free energy for this species is such that
|
|
* it will pop back into existence.
|
|
* -> Set it to a major species in anticipation.
|
|
* -> One exception to this is if a needed component
|
|
* is also zeroed out. Then, don't pop the phase back into
|
|
* existence.
|
|
* -> Another exception to this is if a needed regular element
|
|
* is also zeroed out. Then, don't pop the phase or the species back into
|
|
* existence.
|
|
*/
|
|
for (int j = 0; j < m_numComponents; ++j) {
|
|
double stoicC = sc[irxn][j];
|
|
if (stoicC != 0.0) {
|
|
double negChangeComp = - stoicC;
|
|
if (negChangeComp > 0.0) {
|
|
if (soln[j] < 1.0E-60) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- %s would have popped back into existance but"
|
|
" needed component %s is zero\n",
|
|
SpName[kspec].c_str(), SpName[j].c_str());
|
|
}
|
|
#endif
|
|
if (SSPhase[kspec]) {
|
|
return VCS_SPECIES_ZEROEDSS;
|
|
} else {
|
|
return VCS_SPECIES_ZEROEDMS;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
for (int j = 0; j < m_numElemConstraints; ++j) {
|
|
int elType = m_elType[j];
|
|
if (elType == VCS_ELEM_TYPE_ABSPOS) {
|
|
double atomComp = FormulaMatrix[j][kspec];
|
|
if (atomComp > 0.0) {
|
|
double maxPermissible = gai[j] / atomComp;
|
|
if (maxPermissible < VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- %s would have popped back into existance but"
|
|
" needed element %s is zero\n",
|
|
SpName[kspec].c_str(), (ElName[j]).c_str());
|
|
}
|
|
#endif
|
|
if (SSPhase[kspec]) {
|
|
return VCS_SPECIES_ZEROEDSS;
|
|
} else {
|
|
return VCS_SPECIES_ZEROEDMS;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
return VCS_SPECIES_MAJOR;
|
|
}
|
|
/*
|
|
* Always treat species in single species phases as majors
|
|
*/
|
|
if (SSPhase[kspec]) return VCS_SPECIES_MAJOR;
|
|
/*
|
|
* Check to see whether the current species is a major component
|
|
* of its phase. If it is, it is a major component
|
|
*/
|
|
if (soln[kspec] > (TPhMoles[iph] * 0.1)) return VCS_SPECIES_MAJOR;
|
|
/*
|
|
* Main check in the loop:
|
|
* Check to see if there is a component with a mole number that is
|
|
* within a factor of 100 of the current species.
|
|
* If there is and that component is not part of a single species
|
|
* phase and shares a non-zero stoichiometric coefficient, then
|
|
* the current species is a major species.
|
|
*/
|
|
double szAdj = scSize[irxn] * sqrt(m_numRxnTot);
|
|
for (k = 0; k < m_numComponents; ++k) {
|
|
if (!(SSPhase[k])) {
|
|
if (sc[irxn][k] != 0.0) {
|
|
if (soln[kspec] * szAdj >= soln[k] * 0.01) {
|
|
return VCS_SPECIES_MAJOR;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
return VCS_SPECIES_MINOR;
|
|
}
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void VCS_SOLVE::vcs_chemPotPhase(int iph, const double *const molNum,
|
|
double * const ac, double * const mu_i,
|
|
bool do_deleted)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_chemPotPhase:
|
|
*
|
|
* We calculate the dimensionless chemical potentials of all species
|
|
* in a single phase.
|
|
*
|
|
* Formula:
|
|
* ---------------
|
|
*
|
|
* Ideal Mixtures:
|
|
*
|
|
* fe(I) = ff(I) + ln(z(I)) - ln(tPhMoles_ptr[iph])
|
|
*
|
|
* ( This is equivalent to the adding the log of the
|
|
* mole fraction onto the standard chemical
|
|
* potential. )
|
|
*
|
|
* Non-Ideal Mixtures:
|
|
* ActivityConvention = 0:
|
|
* fe(I) = ff(I) + ln(ActCoeff[i]z(I)) - ln(tPhMoles_ptr[iph])
|
|
*
|
|
* ( This is equivalent to the adding the log of the
|
|
* mole fraction multiplied by the activity coefficient
|
|
* onto the standard chemical potential. )
|
|
*
|
|
* ActivityConvention = 1: -> molality activity formulation
|
|
* fe(I) = ff(I) + ln(ActCoeff[i]z(I)) - ln(tPhMoles_ptr[iph])
|
|
* - ln(Mnaught * m_units)
|
|
*
|
|
* note: z(I)/tPhMoles_ptr[iph] = Xmol[i] is the mole fraction
|
|
* of i in the phase.
|
|
*
|
|
* NOTE:
|
|
* As per the discussion in vcs_dfe(), for small species where the mole
|
|
* fraction
|
|
* z(i) < VCS_DELETE_MINORSPECIES_CUTOFF
|
|
* The chemical potential is calculated as:
|
|
* fe(I) = ff(I) + ln(ActCoeff[i](VCS_DELETE_MINORSPECIES_CUTOFF))
|
|
*
|
|
* Input
|
|
* --------
|
|
* iph : Phase to be calculated
|
|
* molNum(i) : Number of moles of species i
|
|
* (VCS species order)
|
|
* ff : standard state chemical potentials. These are the
|
|
* chemical potentials of the standard states at
|
|
* the same T and P as the solution.
|
|
* (VCS species order)
|
|
* Output
|
|
* -------
|
|
* ac[] : Activity coefficients for species in phase
|
|
* (VCS species order)
|
|
* mu_i[] : Dimensionless chemical potentials for phase species
|
|
* (VCS species order)
|
|
*
|
|
*************************************************************************/
|
|
{
|
|
vcs_VolPhase *Vphase = VPhaseList[iph];
|
|
int nkk = Vphase->NVolSpecies;
|
|
int k, kspec;
|
|
|
|
#ifdef DEBUG
|
|
//if (vcs_debug_print_lvl >= 2) {
|
|
// plogf(" --- Subroutine vcs_chemPotPhase called for phase %d\n",
|
|
// iph);
|
|
//}
|
|
#endif
|
|
double tMoles = TPhInertMoles[iph];
|
|
for (k = 0; k < nkk; k++) {
|
|
kspec = Vphase->IndSpecies[k];
|
|
tMoles += molNum[kspec];
|
|
}
|
|
double tlogMoles = 0.0;
|
|
if (tMoles > 0.0) {
|
|
tlogMoles = log(tMoles);
|
|
}
|
|
|
|
Vphase->setMolesFromVCS(molNum);
|
|
Vphase->sendToVCSActCoeff(ac);
|
|
|
|
double phi = Vphase->electricPotential();
|
|
double Faraday_phi = Faraday_dim * phi;
|
|
|
|
for (k = 0; k < nkk; k++) {
|
|
kspec = Vphase->IndSpecies[k];
|
|
if (kspec >= m_numComponents) {
|
|
int irxn = kspec - m_numComponents;
|
|
if (!do_deleted &&
|
|
(spStatus[irxn] == VCS_SPECIES_DELETED)) {
|
|
continue;
|
|
}
|
|
}
|
|
if (SpeciesUnknownType[kspec] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
#ifdef DEBUG
|
|
if (molNum[kspec] != phi) {
|
|
plogf("We have an inconsistency!\n");
|
|
exit(-1);
|
|
}
|
|
if (Charge[kspec] != -1.0) {
|
|
plogf("We have an unexpected situation!\n");
|
|
exit(-1);
|
|
}
|
|
#endif
|
|
mu_i[kspec] = ff[kspec] + Charge[kspec] * Faraday_phi;
|
|
} else {
|
|
if (SSPhase[kspec]) {
|
|
mu_i[kspec] = ff[kspec] + Charge[kspec] * Faraday_phi;
|
|
} else if (molNum[kspec] <= VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
mu_i[kspec] = ff[kspec] + log(ac[kspec] * VCS_DELETE_MINORSPECIES_CUTOFF)
|
|
- tlogMoles - SpecLnMnaught[kspec] + Charge[kspec] * Faraday_phi;
|
|
} else {
|
|
mu_i[kspec] = ff[kspec] + log(ac[kspec] * molNum[kspec])
|
|
- tlogMoles - SpecLnMnaught[kspec] + Charge[kspec] * Faraday_phi;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void VCS_SOLVE::vcs_dfe(double *z, int kk, int ll, int lbot, int ltop)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_dfe:
|
|
*
|
|
* We calculate the dimensionless chemical potentials of all species
|
|
* or certain groups of species here, at a fixed temperature and pressure,
|
|
* for the input mole vector z[] in the parameter list.
|
|
* Nondimensionalization is achieved by division by RT.
|
|
*
|
|
* Note, for multispecies phases which are currently zeroed out,
|
|
* the chemical potential is filled out with the standard chemical
|
|
* potential.
|
|
*
|
|
* For species in multispecies phases whose concentration is zero,
|
|
* we need to set the mole fraction to a very low value.
|
|
* It's chemical potential
|
|
* is then calculated using the VCS_DELETE_MINORSPECIES_CUTOFF concentration
|
|
* to keep numbers positive.
|
|
*
|
|
*
|
|
* Formula:
|
|
* ---------------
|
|
*
|
|
* Ideal Mixtures:
|
|
*
|
|
* fe(I) = ff(I) + ln(z(I)) - ln(tPhMoles_ptr[iph])
|
|
*
|
|
* ( This is equivalent to the adding the log of the
|
|
* mole fraction onto the standard chemical
|
|
* potential. )
|
|
*
|
|
* Non-Ideal Mixtures:
|
|
* ActivityConvention = 0:
|
|
* fe(I) = ff(I) + ln(ActCoeff[i]z(I)) - ln(tPhMoles_ptr[iph])
|
|
*
|
|
* ( This is equivalent to the adding the log of the
|
|
* mole fraction multiplied by the activity coefficient
|
|
* onto the standard chemical potential. )
|
|
*
|
|
* ActivityConvention = 1: -> molality activity formulation
|
|
* fe(I) = ff(I) + ln(ActCoeff[i]z(I)) - ln(tPhMoles_ptr[iph])
|
|
* - ln(Mnaught * m_units)
|
|
*
|
|
* note: z(I)/tPhMoles_ptr[iph] = Xmol[i] is the mole fraction
|
|
* of i in the phase.
|
|
*
|
|
* NOTE:
|
|
* As per the discussion above, for small species where the mole
|
|
* fraction
|
|
* z(i) < VCS_DELETE_MINORSPECIES_CUTOFF
|
|
* The chemical potential is calculated as:
|
|
* fe(I) = ff(I) + ln(ActCoeff[i](VCS_DELETE_MINORSPECIES_CUTOFF))
|
|
*
|
|
* VCS_SPECIES_TYPE_INTERFACIALVOLTAGE
|
|
*
|
|
* These chemical potentials refer to electrons in
|
|
* metal electrodes. They have the following formula
|
|
*
|
|
* fe(I) = ff(I) - F V / RT
|
|
*
|
|
* F is Faraday's constant.
|
|
* R = gas constant
|
|
* T = temperature
|
|
* V = potential of the interface = phi_electrode - phi_solution
|
|
*
|
|
* For these species, the solution vector is V in volts.
|
|
*
|
|
* Input
|
|
* --------
|
|
* ll = 0: Calculate for all species
|
|
* -1: calculate for components and for major non-components
|
|
* 1: calculate for components and for minor non-components
|
|
* lbot : restricts the calculation of the chemical potential
|
|
* ltop to the species between LBOT <= i < LTOP. Usually
|
|
* LBOT and LTOP will be equal to 0 and MR, respectively.
|
|
* z(i) : Number of moles of species i
|
|
* -> This can either be the current solution vector WT()
|
|
* or the actual solution vector W()
|
|
* kk 1: Use the tentative values for the total number of
|
|
* moles in the phases, i.e., use TG1 instead of TG etc.
|
|
* 0: Use the base values of the total number of
|
|
* moles in each system.
|
|
* ff : standard state chemical potentials. These are the
|
|
* chemical potentials of the standard states at
|
|
* the same T and P as the solution.
|
|
* tg : Total Number of moles in the phase.
|
|
*
|
|
*
|
|
*************************************************************************/
|
|
{
|
|
int l1, l2, iph, kspec, irxn;
|
|
int iphase;
|
|
double *tPhMoles_ptr;
|
|
double *tlogMoles;
|
|
vcs_VolPhase *Vphase;
|
|
VCS_SPECIES_THERMO *st_ptr;
|
|
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
if (ll == 0) {
|
|
if (lbot != 0) {
|
|
plogf(" --- Subroutine vcs_dfe called for one species: ");
|
|
plogf("%-12.12s", SpName[lbot].c_str());
|
|
} else {
|
|
plogf(" --- Subroutine vcs_dfe called for all species");
|
|
}
|
|
} else if (ll > 0) {
|
|
plogf(" --- Subroutine vcs_dfe called for components and minors");
|
|
} else {
|
|
plogf(" --- Subroutine vcs_dfe called for components and majors");
|
|
}
|
|
if (kk == 1) plogf(" using tentative solution\n");
|
|
else plogf("\n");
|
|
}
|
|
#endif
|
|
if (kk <= 0) {
|
|
tPhMoles_ptr = VCS_DATA_PTR(TPhMoles);
|
|
} else {
|
|
tPhMoles_ptr = VCS_DATA_PTR(TPhMoles1);
|
|
}
|
|
tlogMoles = VCS_DATA_PTR(TmpPhase);
|
|
/*
|
|
* Might as well recalculate the phase mole vector
|
|
* and compare to the storred one. They should be correct.
|
|
*/
|
|
double *tPhInertMoles = VCS_DATA_PTR(TPhInertMoles);
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
tlogMoles[iph] = tPhInertMoles[iph];
|
|
|
|
}
|
|
for (kspec = 0; kspec < m_numSpeciesTot; kspec++) {
|
|
if(SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
iph = PhaseID[kspec];
|
|
tlogMoles[iph] += z[kspec];
|
|
}
|
|
}
|
|
#ifdef DEBUG
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
if (! vcs_doubleEqual(tlogMoles[iph], tPhMoles_ptr[iph])) {
|
|
plogf("phase Moles may be off, iph = %d, %20.14g %20.14g \n",
|
|
iph, tlogMoles[iph], tPhMoles_ptr[iph]);
|
|
exit(0);
|
|
}
|
|
}
|
|
#endif
|
|
vcs_dzero(tlogMoles, NPhase);
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
if (tPhMoles_ptr[iph] > 0.0) {
|
|
tlogMoles[iph] = log(tPhMoles_ptr[iph]);
|
|
}
|
|
}
|
|
/*
|
|
* Zero the indicator that that tells us the activity coefficients
|
|
* are current
|
|
*/
|
|
vcs_izero(VCS_DATA_PTR(CurrPhAC), NPhase);
|
|
|
|
if (ll != 0) {
|
|
l1 = lbot;
|
|
l2 = m_numComponents;
|
|
} else {
|
|
l1 = lbot;
|
|
l2 = ltop;
|
|
}
|
|
|
|
/*
|
|
* Calculate activity coefficients for all phases that are
|
|
* not current
|
|
*/
|
|
for (iphase = 0; iphase < NPhase; iphase++) {
|
|
if (!CurrPhAC[iphase]) {
|
|
Vphase = VPhaseList[iphase];
|
|
if (!Vphase->SingleSpecies) {
|
|
Vphase->setMolesFromVCS(z);
|
|
Vphase->sendToVCSActCoeff(VCS_DATA_PTR(ActCoeff));
|
|
}
|
|
phasePhi[iphase] = Vphase->electricPotential();
|
|
CurrPhAC[iphase] = 1;
|
|
}
|
|
}
|
|
/* ************************************************************** */
|
|
/* **** ALL SPECIES, OR COMPONENTS ****************************** */
|
|
/* ************************************************************** */
|
|
/*
|
|
* Do all of the species when LL = 0. Then we are done for the routine
|
|
* When LL ne 0., just do the initial components. We will then
|
|
* finish up below with loops over either the major noncomponent
|
|
* species or the minor noncomponent species.
|
|
*/
|
|
for (kspec = l1; kspec < l2; ++kspec) {
|
|
iphase = PhaseID[kspec];
|
|
if (SpeciesUnknownType[kspec] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
#ifdef DEBUG
|
|
if (z[kspec] != phasePhi[iphase]) {
|
|
plogf("We have an inconsistency!\n");
|
|
exit(-1);
|
|
}
|
|
if (Charge[kspec] != -1.0) {
|
|
plogf("We have an unexpected situation!\n");
|
|
exit(-1);
|
|
}
|
|
#endif
|
|
m_gibbsSpecies[kspec] = ff[kspec] + Charge[kspec] * Faraday_dim * phasePhi[iphase];
|
|
} else {
|
|
if (SSPhase[kspec]) {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
} else {
|
|
if (z[kspec] <= VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
iph = PhaseID[kspec];
|
|
if (tPhMoles_ptr[iph] > 0.0) {
|
|
m_gibbsSpecies[kspec] = ff[kspec]
|
|
+ log(ActCoeff[kspec] * VCS_DELETE_MINORSPECIES_CUTOFF)
|
|
- tlogMoles[PhaseID[kspec]] - SpecLnMnaught[kspec]
|
|
+ Charge[kspec] * Faraday_dim * phasePhi[iphase];
|
|
} else {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
}
|
|
} else {
|
|
m_gibbsSpecies[kspec] = ff[kspec] + log(ActCoeff[kspec] * z[kspec])
|
|
- tlogMoles[PhaseID[kspec]] - SpecLnMnaught[kspec]
|
|
+ Charge[kspec] * Faraday_dim * phasePhi[iphase];
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/* ************************************************ */
|
|
/* **** MAJORS ONLY ******************************* */
|
|
/* ************************************************ */
|
|
if (ll < 0) {
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
if (spStatus[irxn] != VCS_SPECIES_MINOR) {
|
|
kspec = ir[irxn];
|
|
iphase = PhaseID[kspec];
|
|
if (SpeciesUnknownType[kspec] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
#ifdef DEBUG
|
|
if (z[kspec] != phasePhi[iphase]) {
|
|
plogf("We have an inconsistency!\n");
|
|
exit(-1);
|
|
}
|
|
if (Charge[kspec] != -1.0) {
|
|
plogf("We have an unexpected situation!\n");
|
|
exit(-1);
|
|
}
|
|
#endif
|
|
m_gibbsSpecies[kspec] = ff[kspec] + Charge[kspec] * Faraday_dim * phasePhi[iphase];
|
|
} else {
|
|
if (SSPhase[kspec]) {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
} else {
|
|
if (z[kspec] <= VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
iph = PhaseID[kspec];
|
|
if (tPhMoles_ptr[iph] > 0.0) {
|
|
m_gibbsSpecies[kspec] = ff[kspec]
|
|
+ log(ActCoeff[kspec] * VCS_DELETE_MINORSPECIES_CUTOFF)
|
|
- tlogMoles[PhaseID[kspec]] - SpecLnMnaught[kspec]
|
|
+ Charge[kspec] * Faraday_dim * phasePhi[iphase]; ;
|
|
} else {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
}
|
|
} else {
|
|
m_gibbsSpecies[kspec] = ff[kspec] + log(ActCoeff[kspec] * z[kspec])
|
|
- tlogMoles[PhaseID[kspec]] - SpecLnMnaught[kspec]
|
|
+ Charge[kspec] * Faraday_dim * phasePhi[iphase];
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
/* ************************************************ */
|
|
/* **** MINORS ONLY ******************************* */
|
|
/* ************************************************ */
|
|
} else if (ll > 0) {
|
|
for (irxn = 0; irxn < m_numRxnRdc; ++irxn) {
|
|
if (spStatus[irxn] == VCS_SPECIES_MINOR) {
|
|
kspec = ir[irxn];
|
|
iphase = PhaseID[kspec];
|
|
if (SpeciesUnknownType[kspec] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
#ifdef DEBUG
|
|
if (z[kspec] != phasePhi[iphase]) {
|
|
plogf("We have an inconsistency!\n");
|
|
exit(-1);
|
|
}
|
|
if (Charge[kspec] != -1.0) {
|
|
plogf("We have an unexpected situation!\n");
|
|
exit(-1);
|
|
}
|
|
#endif
|
|
m_gibbsSpecies[kspec] = ff[kspec] + Charge[kspec] * Faraday_dim * phasePhi[iphase]; ;
|
|
} else {
|
|
if (SSPhase[kspec]) {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
} else {
|
|
if (z[kspec] <= VCS_DELETE_MINORSPECIES_CUTOFF) {
|
|
iph = PhaseID[kspec];
|
|
if (tPhMoles_ptr[iph] > 0.0) {
|
|
m_gibbsSpecies[kspec] = ff[kspec]
|
|
+ log(ActCoeff[kspec] * VCS_DELETE_MINORSPECIES_CUTOFF)
|
|
- tlogMoles[PhaseID[kspec]] - SpecLnMnaught[kspec];
|
|
} else {
|
|
m_gibbsSpecies[kspec] = ff[kspec];
|
|
}
|
|
} else {
|
|
st_ptr = SpeciesThermo[kspec];
|
|
m_gibbsSpecies[kspec] = ff[kspec] + log(ActCoeff[kspec] * z[kspec])
|
|
- tlogMoles[PhaseID[kspec]] - SpecLnMnaught[kspec];
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
#ifdef DEBUG_NOT
|
|
for (kspec = 0; kspec < m_numSpeciesRdc; kspec++) {
|
|
checkFinite(fe[kspec]);
|
|
}
|
|
#endif
|
|
} /* vcs_dfe() ***************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
int vcsUtil_mlequ(double *c, int idem, int n, double *b, int m)
|
|
|
|
/*************************************************************************
|
|
*
|
|
* vcs_mlequ:
|
|
*
|
|
* Invert an nxn matrix and solve m rhs's
|
|
*
|
|
* Solve C X + B = 0;
|
|
*
|
|
* This routine uses Gauss elimination and is optimized for the solution
|
|
* of lots of rhs's.
|
|
* A crude form of row pivoting is used here.
|
|
*
|
|
*
|
|
* c[i+j*idem] = c_i_j = Matrix to be inverted: i = row number
|
|
* j = column number
|
|
* b[i+j*idem] = b_i_j = vectors of rhs's: i = row number
|
|
* j = column number
|
|
* (each column is a new rhs)
|
|
* n = number of rows and columns in the matrix
|
|
* m = number of rhs to be solved for
|
|
* idem = first dimension in the fortran calling routine
|
|
* idem >= n must be true
|
|
*
|
|
* Return Value
|
|
* 1 : Matrix is singluar
|
|
* 0 : solution is OK
|
|
*
|
|
* The solution is returned in the matrix b.
|
|
*************************************************************************/
|
|
{
|
|
int i, j, k, l;
|
|
double R;
|
|
|
|
/*
|
|
* Loop over the rows
|
|
* -> At the end of each loop, the only nonzero entry in the column
|
|
* will be on the diagonal. We can therfore just invert the
|
|
* diagonal at the end of the program to solve the equation system.
|
|
*/
|
|
for (i = 0; i < n; ++i) {
|
|
if (c[i + i * idem] == 0.0) {
|
|
/*
|
|
* Do a simple form of row pivoting to find a non-zero pivot
|
|
*/
|
|
for (k = i + 1; k < n; ++k) {
|
|
if (c[k + i * idem] != 0.0) goto FOUND_PIVOT;
|
|
}
|
|
plogf("vcs_mlequ ERROR: Encountered a zero column: %d\n", i);
|
|
return 1;
|
|
FOUND_PIVOT: ;
|
|
for (j = 0; j < n; ++j) c[i + j * idem] += c[k + j * idem];
|
|
for (j = 0; j < m; ++j) b[i + j * idem] += b[k + j * idem];
|
|
}
|
|
|
|
for (l = 0; l < n; ++l) {
|
|
if (l != i && c[l + i * idem] != 0.0) {
|
|
R = c[l + i * idem] / c[i + i * idem];
|
|
c[l + i * idem] = 0.0;
|
|
for (j = i+1; j < n; ++j) c[l + j * idem] -= c[i + j * idem] * R;
|
|
for (j = 0; j < m; ++j) b[l + j * idem] -= b[i + j * idem] * R;
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* The negative in the last expression is due to the form of B upon
|
|
* input
|
|
*/
|
|
for (i = 0; i < n; ++i) {
|
|
for (j = 0; j < m; ++j)
|
|
b[i + j * idem] = -b[i + j * idem] / c[i + i*idem];
|
|
}
|
|
return VCS_SUCCESS;
|
|
} /* vcs_mlequ() *************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void vcsUtil_isw(int x[], int i1, int i2)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_isw:
|
|
*
|
|
* Switches the value of X(i1) with X(i2)
|
|
*************************************************************************/
|
|
{
|
|
int t;
|
|
t = x[i1];
|
|
x[i1] = x[i2];
|
|
x[i2] = t;
|
|
} /* vcs_isw() ***************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void vcsUtil_dsw(double *x, int i1, int i2)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_dsw:
|
|
*
|
|
* Switches the value of X(i1) with X(i2)
|
|
*************************************************************************/
|
|
{
|
|
double t;
|
|
t = x[i1];
|
|
x[i1] = x[i2];
|
|
x[i2] = t;
|
|
} /* vcs_dsw() ***************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void vcsUtil_ssw(char **vstr, int i1, int i2)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_ssw:
|
|
*
|
|
* Switches the place of two strings in an array of strings.
|
|
* (Limited to strings of length less than 24 characters).
|
|
*************************************************************************/
|
|
{
|
|
char tmp[24];
|
|
(void) strncpy(tmp, vstr[i2], (size_t) 24);
|
|
(void) strncpy(vstr[i2], vstr[i1], (size_t) 24);
|
|
(void) strncpy(vstr[i1], tmp, (size_t) 24);
|
|
}
|
|
|
|
/*
|
|
*
|
|
* vcs_stsw:
|
|
*
|
|
* Switches the place of two strings in a vector of strings.
|
|
*/
|
|
void vcsUtil_stsw(std::vector<std::string> & vstr, int i1, int i2)
|
|
{
|
|
std::string tmp(vstr[i2]);
|
|
vstr[i2] = vstr[i1];
|
|
vstr[i1] = tmp;
|
|
}
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
#ifdef DEBUG
|
|
|
|
void VCS_SOLVE::prneav(void)
|
|
|
|
/*************************************************************************
|
|
*
|
|
* Print out and check the elemental abundance vector
|
|
*
|
|
*************************************************************************/
|
|
{
|
|
int kerr, i, j;
|
|
std::vector<double> eav(m_numElemConstraints, 0.0);
|
|
|
|
for (j = 0; j < m_numElemConstraints; ++j) {
|
|
for (i = 0; i < m_numSpeciesTot; ++i) {
|
|
if (SpeciesUnknownType[i] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
eav[j] += FormulaMatrix[j][i] * soln[i];
|
|
}
|
|
}
|
|
}
|
|
kerr = FALSE;
|
|
plogf( "--------------------------------------------------");
|
|
plogf("ELEMENT ABUNDANCE VECTOR:\n");
|
|
plogf(" Element Now Orignal Deviation Type\n");
|
|
for (j = 0; j < m_numElemConstraints; ++j) {
|
|
plogf(" "); plogf("%-2.2s", (ElName[j]).c_str());
|
|
plogf(" = %15.6E %15.6E %15.6E %3d\n",
|
|
eav[j], gai[j], eav[j] - gai[j], m_elType[j]);
|
|
if (gai[j] != 0.) {
|
|
if (fabs(eav[j] - gai[j]) > gai[j] * 5.0e-9)
|
|
kerr = TRUE;
|
|
} else {
|
|
if (fabs(eav[j]) > 1.0e-10) kerr = TRUE;
|
|
}
|
|
}
|
|
if (kerr) {
|
|
plogf("Element abundance check failure\n");
|
|
}
|
|
plogf("--------------------------------------------------\n");
|
|
}
|
|
#endif
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
double VCS_SOLVE::l2normdg(double dg[])
|
|
|
|
/*************************************************************************
|
|
*
|
|
* l2normdg:
|
|
*
|
|
* Calculate the norm of the DG vector.
|
|
* Positive DG for species which don't exist are ignored.
|
|
************************************************************************/
|
|
{
|
|
double tmp;
|
|
int irxn;
|
|
if (m_numRxnRdc <= 0) return 0.0;
|
|
for (irxn = 0, tmp = 0.0; irxn < m_numRxnRdc; ++irxn) {
|
|
if (spStatus[irxn] == VCS_SPECIES_MAJOR || spStatus[irxn] == VCS_SPECIES_MINOR ||
|
|
dg[irxn] < 0.0) {
|
|
if (spStatus[irxn] != VCS_SPECIES_ZEROEDMS) {
|
|
tmp += dg[irxn] * dg[irxn];
|
|
}
|
|
}
|
|
}
|
|
return (sqrt(tmp / m_numRxnRdc));
|
|
}
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void VCS_SOLVE::vcs_tmoles(void)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_tmoles:
|
|
*
|
|
* Calculates the total number of moles of species in all phases.
|
|
* Calculates the total number of moles in all phases.
|
|
* Reconciles Phase existence flags with total moles in each phase.
|
|
*************************************************************************/
|
|
{
|
|
int i;
|
|
double sum;
|
|
vcs_VolPhase *Vphase;
|
|
for (i = 0; i < NPhase; i++) {
|
|
TPhMoles[i] = TPhInertMoles[i];
|
|
}
|
|
for (i = 0; i < m_numSpeciesTot; i++) {
|
|
if (SpeciesUnknownType[i] == VCS_SPECIES_TYPE_MOLNUM) {
|
|
TPhMoles[PhaseID[i]] += soln[i];
|
|
}
|
|
}
|
|
sum = 0.0;
|
|
for (i = 0; i < NPhase; i++) {
|
|
sum += TPhMoles[i];
|
|
Vphase = VPhaseList[i];
|
|
// Took out because we aren't updating mole fractions in Vphase
|
|
// Vphase->TMoles = TPhMoles[i];
|
|
if (TPhMoles[i] == 0.0) {
|
|
Vphase->Existence = 0;
|
|
} else {
|
|
if (TPhInertMoles[i] > 0.0) {
|
|
Vphase->Existence = 2;
|
|
} else {
|
|
Vphase->Existence = 1;
|
|
}
|
|
}
|
|
}
|
|
TMoles = sum;
|
|
} /* vcs_tmoles() ************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void VCS_SOLVE::vcs_updateVP (int place)
|
|
|
|
/*************************************************************************
|
|
* vcs_updateVP()
|
|
*
|
|
* This routine uploads the state of the system into all of the
|
|
* VolumePhase objects in the current problem.
|
|
* place
|
|
* 0 -> from soln
|
|
* 1 -> from wt
|
|
*************************************************************************/
|
|
{
|
|
vcs_VolPhase *Vphase;
|
|
for (int i = 0; i < NPhase; i++) {
|
|
Vphase = VPhaseList[i];
|
|
if (place == 0) {
|
|
Vphase->setMolesFromVCSCheck(VCS_DATA_PTR(soln),
|
|
VCS_DATA_PTR(TPhMoles), i);
|
|
} else if (place == 1) {
|
|
Vphase->setMolesFromVCSCheck(VCS_DATA_PTR(wt),
|
|
VCS_DATA_PTR(TPhMoles1), i);
|
|
} else {
|
|
plogf("we shouldn't be here\n");
|
|
exit(-1);
|
|
}
|
|
}
|
|
}
|
|
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void VCS_SOLVE::vcs_switch2D(double * const * const Jac, int k1, int k2)
|
|
|
|
/**************************************************************************
|
|
* vcs_switch2D:
|
|
*
|
|
* Switch rows and columns of a square matrix
|
|
*************************************************************************/
|
|
{
|
|
int i;
|
|
register double dtmp;
|
|
for (i = 0; i < m_numSpeciesTot; i++) {
|
|
SWAP(Jac[k1][i], Jac[k2][i], dtmp);
|
|
}
|
|
for (i = 0; i < m_numSpeciesTot; i++) {
|
|
SWAP(Jac[i][k1], Jac[i][k2], dtmp);
|
|
}
|
|
}
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
|
|
void VCS_SOLVE::vcs_switch_pos(int ifunc, int k1, int k2)
|
|
|
|
/**************************************************************************
|
|
*
|
|
* vcs_switch_pos:
|
|
*
|
|
* Swaps the indecises for all of the global data for two species, k1
|
|
* and k2.
|
|
*
|
|
* ifunc: If true, switch the species data and the noncomponent reaction
|
|
* data. This must be called for a non-component species only.
|
|
*
|
|
* If false, switch the species data only. Typically, we use this
|
|
* option when determining the component species and at the
|
|
* end of the calculation, when we want to return unscrambled
|
|
* results.
|
|
*************************************************************************/
|
|
{
|
|
register int j;
|
|
register double t1 = 0.0;
|
|
int i1, i2, iph, kp1, kp2;
|
|
vcs_VolPhase *pv1, *pv2;
|
|
VCS_SPECIES_THERMO *st_tmp;
|
|
if (k1 == k2) return;
|
|
#ifdef DEBUG
|
|
if (k1 < 0 || k1 > (m_numSpeciesTot - 1) ||
|
|
k2 < 0 || k2 > (m_numSpeciesTot - 1) ) {
|
|
plogf("vcs_switch_pos: ifunc = 0: inappropriate args: %d %d\n",
|
|
k1, k2);
|
|
}
|
|
#endif
|
|
/*
|
|
* Handle the index pointer in the phase structures first
|
|
*/
|
|
pv1 = VPhaseList[PhaseID[k1]];
|
|
pv2 = VPhaseList[PhaseID[k2]];
|
|
|
|
kp1 = indPhSp[k1];
|
|
kp2 = indPhSp[k2];
|
|
#ifdef DEBUG
|
|
if (pv1->IndSpecies[kp1] != k1) {
|
|
plogf("Indexing error in program\n");
|
|
exit(-1);
|
|
}
|
|
if (pv2->IndSpecies[kp2] != k2) {
|
|
plogf("Indexing error in program\n");
|
|
exit(-1);
|
|
}
|
|
#endif
|
|
pv1->IndSpecies[kp1] = k2;
|
|
pv2->IndSpecies[kp2] = k1;
|
|
|
|
vcsUtil_stsw(SpName, k1, k2);
|
|
SWAP(soln[k1], soln[k2], t1);
|
|
SWAP(SpeciesUnknownType[k1], SpeciesUnknownType[k2], j);
|
|
SWAP(wt[k1], wt[k2], t1);
|
|
SWAP(ff[k1], ff[k2], t1);
|
|
SWAP(m_gibbsSpecies[k1], m_gibbsSpecies[k2], t1);
|
|
SWAP(ds[k1], ds[k2], t1);
|
|
SWAP(fel[k1], fel[k2], t1);
|
|
SWAP(feTrial[k1], feTrial[k2], t1);
|
|
SWAP(SSPhase[k1], SSPhase[k2], j);
|
|
SWAP(PhaseID[k1], PhaseID[k2], j);
|
|
SWAP(ind[k1], ind[k2], j);
|
|
SWAP(indPhSp[k1], indPhSp[k2], j);
|
|
SWAP(SpecActConvention[k1], SpecActConvention[k2], j);
|
|
SWAP(SpecLnMnaught[k1], SpecLnMnaught[k2], t1);
|
|
SWAP(ActCoeff[k1], ActCoeff[k2], t1);
|
|
SWAP(ActCoeff0[k1], ActCoeff0[k2], t1);
|
|
SWAP(WtSpecies[k1], WtSpecies[k2], t1);
|
|
SWAP(Charge[k1], Charge[k2], t1);
|
|
SWAP(SpeciesThermo[k1], SpeciesThermo[k2], st_tmp);
|
|
SWAP(VolPM[k1], VolPM[k2], t1);
|
|
|
|
for (j = 0; j < m_numElemConstraints; ++j) {
|
|
SWAP(FormulaMatrix[j][k1], FormulaMatrix[j][k2], t1);
|
|
}
|
|
if (UseActCoeffJac) {
|
|
vcs_switch2D(dLnActCoeffdMolNum.baseDataAddr(), k1, k2);
|
|
}
|
|
|
|
/*
|
|
* Handle the index pointer in the phase structures
|
|
*/
|
|
|
|
|
|
if (ifunc) {
|
|
/*
|
|
* Find the noncomponent indecises for the two species
|
|
*/
|
|
i1 = k1 - m_numComponents;
|
|
i2 = k2 - m_numComponents;
|
|
#ifdef DEBUG
|
|
if (i1 < 0 || i1 > (m_numRxnTot - 1) ||
|
|
i2 < 0 || i2 > (m_numRxnTot - 1) ) {
|
|
plogf("switch_pos: ifunc = 1: inappropriate noncomp values: %d %d\n",
|
|
i1 , i2);
|
|
}
|
|
#endif
|
|
for (j = 0; j < m_numComponents; ++j) {
|
|
SWAP(sc[i1][j], sc[i2][j], t1);
|
|
}
|
|
SWAP(scSize[i1], scSize[i2], t1);
|
|
for (iph = 0; iph < NPhase; iph++) {
|
|
SWAP(DnPhase[i1][iph], DnPhase[i2][iph], t1);
|
|
SWAP(PhaseParticipation[i1][iph],
|
|
PhaseParticipation[i2][iph], j);
|
|
}
|
|
SWAP(dg[i1], dg[i2], t1);
|
|
SWAP(dgl[i1], dgl[i2], t1);
|
|
SWAP(spStatus[i1], spStatus[i2], j);
|
|
|
|
/*
|
|
* We don't want to swap ir[], because the values of ir should
|
|
* stay the same after the swap
|
|
*
|
|
* vcs_isw(ir, i1, i2);
|
|
*/
|
|
}
|
|
} /* vcs_switch_pos() ********************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
/*****************************************************************************/
|
|
static void print_space(int num)
|
|
{
|
|
int j;
|
|
for (j = 0; j < num; j++) plogf(" ");
|
|
}
|
|
|
|
/****************************************************************************
|
|
*
|
|
* vcs_deltag_Phase():
|
|
*
|
|
* Calculate deltag of formation for all species in a single
|
|
* phase. It is assumed that the fe[] is up to date for all species.
|
|
* Howevever, if the phase is currently zereoed out, a subproblem
|
|
* is calculated to solve for AC[i] and pseudo-X[i] for that
|
|
* phase.
|
|
*/
|
|
void VCS_SOLVE::vcs_deltag_Phase(int iphase, bool doDeleted) {
|
|
int iph;
|
|
int irxn, kspec, kcomp;
|
|
double *dtmp_ptr;
|
|
int irxnl = m_numRxnRdc;
|
|
if (doDeleted) irxnl = m_numRxnTot;
|
|
vcs_VolPhase *vPhase = VPhaseList[iphase];
|
|
|
|
#ifdef DEBUG
|
|
if (vcs_debug_print_lvl >= 2) {
|
|
plogf(" --- Subroutine vcs_deltag_Phase called for phase %d\n",
|
|
iphase);
|
|
}
|
|
#endif
|
|
|
|
/*
|
|
* Single species Phase
|
|
*/
|
|
if (vPhase->SingleSpecies) {
|
|
kspec = vPhase->IndSpecies[0];
|
|
#ifdef DEBUG
|
|
if (iphase != PhaseID[kspec]) {
|
|
plogf("vcs_deltag_Phase index error\n");
|
|
exit(-1);
|
|
}
|
|
#endif
|
|
if (kspec >= m_numComponents) {
|
|
irxn = kspec - m_numComponents;
|
|
dg[irxn] = m_gibbsSpecies[kspec];
|
|
dtmp_ptr = sc[irxn];
|
|
for (kcomp = 0; kcomp < m_numComponents; ++kcomp) {
|
|
dg[irxn] += dtmp_ptr[kcomp] * m_gibbsSpecies[kcomp];
|
|
}
|
|
}
|
|
}
|
|
/*
|
|
* Multispecies Phase
|
|
*/
|
|
else {
|
|
bool zeroedPhase = TRUE;
|
|
|
|
for (irxn = 0; irxn < irxnl; ++irxn) {
|
|
kspec = ir[irxn];
|
|
if (SpeciesUnknownType[kspec] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
iph = PhaseID[kspec];
|
|
if (iph == iphase ) {
|
|
if (soln[kspec] > 0.0) zeroedPhase = FALSE;
|
|
dg[irxn] = m_gibbsSpecies[kspec];
|
|
dtmp_ptr = sc[irxn];
|
|
for (kcomp = 0; kcomp < m_numComponents; ++kcomp) {
|
|
dg[irxn] += dtmp_ptr[kcomp] * m_gibbsSpecies[kcomp];
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
/*
|
|
* special section for zeroed phases
|
|
*/
|
|
/* ************************************************* */
|
|
/* **** MULTISPECIES PHASES WITH ZERO MOLES************ */
|
|
/* ************************************************* */
|
|
/*
|
|
* Massage the free energies for species with zero mole fractions
|
|
* in multispecies phases. This section implements the
|
|
* Equation 3.8-5 in Smith and Missen, p.59.
|
|
* A multispecies phase will exist iff
|
|
* 1 < sum_i(exp(-dg_i)/AC_i)
|
|
* If DG is negative then that species wants to be reintroduced into
|
|
* the calculation.
|
|
* For small dg_i, the expression below becomes:
|
|
* 1 - sum_i(exp(-dg_i)/AC_i) ~ sum_i((dg_i-1)/AC_i) + 1
|
|
*
|
|
*
|
|
* HKM -> The ratio of mole fractions at the reinstatement
|
|
* time should be equal to the normalized weighting
|
|
* of exp(-dg_i) / AC_i. This should be implemented.
|
|
*
|
|
* HKM -> There is circular logic here. ActCoeff depends on the
|
|
* mole fractions of a phase that does not exist. In actuality
|
|
* the proto-mole fractions should be selected from the
|
|
* solution of a nonlinear problem with NsPhase unknowns
|
|
*
|
|
* X_i = exp(-dg[irxn]) / ActCoeff_i / denom
|
|
*
|
|
* where
|
|
* denom = sum_i[ exp(-dg[irxn]) / ActCoeff_i ]
|
|
*
|
|
* This can probably be solved by successive iteration.
|
|
* This should be implemented.
|
|
*/
|
|
/*
|
|
* Calculate dg[] for each species in a zeroed multispecies phase.
|
|
* All of the dg[]'s will be equal. If dg[] is negative, then
|
|
* the phase will come back into existence.
|
|
*/
|
|
if (zeroedPhase) {
|
|
double phaseDG = 1.0;
|
|
for (irxn = 0; irxn < irxnl; ++irxn) {
|
|
kspec = ir[irxn];
|
|
iph = PhaseID[kspec];
|
|
if (iph == iphase) {
|
|
if (dg[irxn] > 50.0) dg[irxn] = 50.0;
|
|
if (dg[irxn] < -50.0) dg[irxn] = -50.0;
|
|
phaseDG -= exp(-dg[irxn])/ActCoeff[kspec];
|
|
}
|
|
}
|
|
/*
|
|
* Overwrite the individual dg's with the phase DG.
|
|
*/
|
|
for (irxn = 0; irxn < irxnl; ++irxn) {
|
|
kspec = ir[irxn];
|
|
iph = PhaseID[kspec];
|
|
if (iph == iphase) {
|
|
dg[irxn] = 1.0 - phaseDG;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
}
|
|
|
|
/****************************************************************************
|
|
*
|
|
* vcs_birthGuess
|
|
*
|
|
* Birth guess returns the number of moles of a species
|
|
* that is coming back to life. or -> whose concentration has
|
|
* been forced to zero by a constraint for some reason, and needs
|
|
* to be reinitialized.
|
|
*/
|
|
double VCS_SOLVE::vcs_birthGuess(int kspec) {
|
|
int irxn = kspec - m_numComponents;
|
|
int soldel = false;
|
|
double dx = 0.0;
|
|
if (SpeciesUnknownType[kspec] == VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
return dx;
|
|
}
|
|
double w_kspec = VCS_DELETE_SPECIES_CUTOFF;
|
|
// Check to make sure that species is zero in the solution vector
|
|
// If it isn't, we don't know what's happening
|
|
if (soln[kspec] != 0.0) {
|
|
w_kspec = 0.0;
|
|
plogf("we shouldn't be here\n");
|
|
exit(-1);
|
|
}
|
|
int ss = SSPhase[kspec];
|
|
if (!ss) {
|
|
/*
|
|
* Logic to handle species in multiple species phases
|
|
*/
|
|
#ifdef DEBUG
|
|
char ANOTE[32];
|
|
double dxm = minor_alt_calc(kspec, irxn, &soldel, ANOTE);
|
|
#else
|
|
double dxm = minor_alt_calc(kspec, irxn, &soldel);
|
|
#endif
|
|
dx = w_kspec + dxm;
|
|
if (dx > 1.0E-15) {
|
|
dx = 1.0E-15;
|
|
}
|
|
} else {
|
|
/*
|
|
* Logic to handle single species phases
|
|
*/
|
|
dx = VCS_DELETE_SPECIES_CUTOFF * 100.;
|
|
}
|
|
|
|
/*
|
|
* Check to see if the current value of the components
|
|
* allow the dx.
|
|
* If we are in danger of zeroing a component,
|
|
* only go 1/3 the way to zeroing the component with
|
|
* this dx. Note, this may mean that dx= 0 coming
|
|
* back from this routine. This evaluation should
|
|
* be respected.
|
|
*/
|
|
double *sc_irxn = sc[irxn];
|
|
for (int j = 0; j < m_numComponents; ++j) {
|
|
// Only loop over element contraints that involve positive def. constraints
|
|
if (SpeciesUnknownType[j] != VCS_SPECIES_TYPE_INTERFACIALVOLTAGE) {
|
|
if (soln[j] > 0.0) {
|
|
double tmp = sc_irxn[j] * dx;
|
|
if (3.0*(-tmp) > soln[j]) {
|
|
dx = MIN(dx, - 0.3333* soln[j] / sc_irxn[j]);
|
|
}
|
|
}
|
|
if (soln[j] <= 0.0) {
|
|
if (sc_irxn[j] < 0.0) {
|
|
dx = 0.0;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
return dx;
|
|
}
|
|
/*****************************************************************/
|
|
}
|
|
|