[Kinetics] Add class BulkKinetics
This class serves as a common base for GasKinetics and AqueousKinetics, eliminating most of the redundancy between the two classes.
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6 changed files with 262 additions and 662 deletions
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@ -1,6 +1,5 @@
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/**
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* @file AqueousKinetics.h
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*
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* @ingroup chemkinetics
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*/
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@ -9,44 +8,23 @@
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#ifndef CT_AQUEOUSKINETICS_H
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#define CT_AQUEOUSKINETICS_H
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#include "Kinetics.h"
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#include "ReactionStoichMgr.h"
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#include "RateCoeffMgr.h"
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#include "cantera/base/utilities.h"
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#include "BulkKinetics.h"
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namespace Cantera
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{
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// forward references
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class ReactionData;
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/**
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* Kinetics manager for elementary aqueous-phase chemistry. This
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* kinetics manager implements standard mass-action reaction rate
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* expressions for liquids
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*
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*
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* Concentration
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* Kinetics manager for elementary aqueous-phase chemistry. This kinetics
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* manager implements standard mass-action reaction rate expressions for liquids
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*
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* @ingroup kinetics
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* @deprecated Not actually implemented
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*/
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class AqueousKinetics : public Kinetics
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class AqueousKinetics : public BulkKinetics
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{
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public:
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//! @name Constructors
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//! @{
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/// Constructor. Creates an empty reaction mechanism.
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AqueousKinetics(thermo_t* thermo = 0);
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AqueousKinetics(const AqueousKinetics& right);
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AqueousKinetics& operator=(const AqueousKinetics& right);
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//! Duplication routine for objects which inherit from Kinetics
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/*!
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* This virtual routine can be used to duplicate %Kinetics objects
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@ -59,117 +37,25 @@ public:
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* m_thermo vector within this object
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*/
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virtual Kinetics* duplMyselfAsKinetics(const std::vector<thermo_t*> & tpVector) const;
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//@}
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virtual int type() const {
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return cAqueousKinetics;
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}
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virtual doublereal reactantStoichCoeff(size_t k, size_t i) const {
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return getValue(m_rrxn[k], i, 0.0);
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}
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virtual doublereal productStoichCoeff(size_t k, size_t i) const {
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return getValue(m_prxn[k], i, 0.0);
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}
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//! @name Reaction Rates Of Progress
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//@{
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virtual void getEquilibriumConstants(doublereal* kc);
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virtual void getDeltaGibbs(doublereal* deltaG);
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virtual void getDeltaEnthalpy(doublereal* deltaH);
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virtual void getDeltaEntropy(doublereal* deltaS);
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virtual void getDeltaSSGibbs(doublereal* deltaG);
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virtual void getDeltaSSEnthalpy(doublereal* deltaH);
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virtual void getDeltaSSEntropy(doublereal* deltaS);
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//! @}
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//! @name Reaction Mechanism Informational Query Routines
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//! @{
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virtual bool isReversible(size_t i) {
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if (std::find(m_revindex.begin(), m_revindex.end(), i)
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< m_revindex.end()) {
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return true;
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} else {
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return false;
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}
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}
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virtual void getFwdRateConstants(doublereal* kfwd);
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virtual void getRevRateConstants(doublereal* krev,
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bool doIrreversible = false);
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//! @}
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//! @name Reaction Mechanism Setup Routines
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//! @{
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virtual void init();
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virtual void addReaction(ReactionData& r);
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virtual void finalize();
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virtual bool ready() const;
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virtual void update_T();
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virtual void update_C();
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void updateROP();
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/*!
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* Update temperature-dependent portions of reaction rates and
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* falloff functions.
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*/
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//! Update temperature-dependent portions of reaction rates
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void _update_rates_T();
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/*!
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* Update properties that depend on concentrations. Currently only
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* the enhanced collision partner concentrations are updated here.
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*/
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//! Update properties that depend on concentrations.
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void _update_rates_C();
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//@}
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protected:
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size_t m_nfall;
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Rate1<Arrhenius> m_rates;
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std::vector<size_t> m_irrev;
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size_t m_nirrev;
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size_t m_nrev;
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/**
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* Difference between the input global reactants order
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* and the input global products order. Changed to a double
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* to account for the fact that we can have real-valued
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* stoichiometries.
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*/
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vector_fp m_dn;
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std::vector<size_t> m_revindex;
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vector_fp m_conc;
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vector_fp m_grt;
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//! @name Aqueous kinetics data
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//!@{
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bool m_ROP_ok;
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doublereal m_temp;
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//!@}
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private:
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void addElementaryReaction(ReactionData& r);
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/**
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* Update the equilibrium constants in molar units.
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*/
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//! Update the equilibrium constants in molar units.
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void updateKc();
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bool m_finalized;
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virtual void addReaction(ReactionData& r);
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};
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}
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63
include/cantera/kinetics/BulkKinetics.h
Normal file
63
include/cantera/kinetics/BulkKinetics.h
Normal file
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@ -0,0 +1,63 @@
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/**
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* @file BulkKinetics.h
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* @ingroup chemkinetics
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*/
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#ifndef CT_BULKKINETICS_H
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#define CT_BULKKINETICS_H
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#include "Kinetics.h"
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#include "RateCoeffMgr.h"
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namespace Cantera
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{
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//! Partial specialization of Kinetics for chemistry in a single bulk phase
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class BulkKinetics : public Kinetics
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{
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public:
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BulkKinetics(thermo_t* thermo = 0);
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virtual Kinetics* duplMyselfAsKinetics(const std::vector<thermo_t*> & tpVector) const;
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virtual bool isReversible(size_t i);
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virtual void getDeltaGibbs(doublereal* deltaG);
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virtual void getDeltaEnthalpy(doublereal* deltaH);
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virtual void getDeltaEntropy(doublereal* deltaS);
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virtual void getDeltaSSGibbs(doublereal* deltaG);
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virtual void getDeltaSSEnthalpy(doublereal* deltaH);
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virtual void getDeltaSSEntropy(doublereal* deltaS);
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virtual void getRevRateConstants(doublereal* krev,
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bool doIrreversible = false);
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virtual void addReaction(ReactionData& r);
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virtual void init();
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virtual void finalize();
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virtual bool ready() const;
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protected:
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virtual void addElementaryReaction(ReactionData& r);
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Rate1<Arrhenius> m_rates;
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std::vector<size_t> m_revindex; //!< Indices of reversible reactions
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std::vector<size_t> m_irrev; //!< Indices of irreversible reactions
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//! Difference between the global reactants order and the global products
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//! order. Of type "double" to account for the fact that we can have real-
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//! valued stoichiometries.
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vector_fp m_dn;
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vector_fp m_conc;
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vector_fp m_grt;
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bool m_ROP_ok;
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doublereal m_temp;
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bool m_finalized;
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};
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}
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#endif
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@ -9,26 +9,20 @@
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#ifndef CT_GASKINETICS_H
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#define CT_GASKINETICS_H
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#include "Kinetics.h"
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#include "ReactionStoichMgr.h"
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#include "BulkKinetics.h"
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#include "ThirdBodyMgr.h"
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#include "FalloffMgr.h"
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#include "RateCoeffMgr.h"
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namespace Cantera
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{
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// forward references
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class Enhanced3BConc;
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class ReactionData;
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/**
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* Kinetics manager for elementary gas-phase chemistry. This
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* kinetics manager implements standard mass-action reaction rate
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* expressions for low-density gases.
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* @ingroup kinetics
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*/
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class GasKinetics : public Kinetics
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class GasKinetics : public BulkKinetics
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{
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public:
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//! @name Constructors and General Information
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*/
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GasKinetics(thermo_t* thermo = 0);
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//! Copy Constructor
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GasKinetics(const GasKinetics& right);
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//! Assignment operator
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GasKinetics& operator=(const GasKinetics& right);
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virtual Kinetics* duplMyselfAsKinetics(const std::vector<thermo_t*> & tpVector) const;
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virtual int type() const {
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//! @{
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virtual void getEquilibriumConstants(doublereal* kc);
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virtual void getDeltaGibbs(doublereal* deltaG);
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virtual void getDeltaEnthalpy(doublereal* deltaH);
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virtual void getDeltaEntropy(doublereal* deltaS);
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virtual void getDeltaSSGibbs(doublereal* deltaG);
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virtual void getDeltaSSEnthalpy(doublereal* deltaH);
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virtual void getDeltaSSEntropy(doublereal* deltaS);
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//! @}
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//! @name Reaction Mechanism Informational Query Routines
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//! @{
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virtual bool isReversible(size_t i) {
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if (std::find(m_revindex.begin(), m_revindex.end(), i)
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< m_revindex.end()) {
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return true;
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} else {
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return false;
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}
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}
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virtual void getFwdRateConstants(doublereal* kfwd);
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virtual void getRevRateConstants(doublereal* krev,
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bool doIrreversible = false);
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//! @}
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//! @name Reaction Mechanism Setup Routines
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//! @{
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@ -111,30 +75,15 @@ protected:
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Rate1<Arrhenius> m_falloff_low_rates;
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Rate1<Arrhenius> m_falloff_high_rates;
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Rate1<Arrhenius> m_rates;
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FalloffMgr m_falloffn;
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ThirdBodyMgr<Enhanced3BConc> m_3b_concm;
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ThirdBodyMgr<Enhanced3BConc> m_falloff_concm;
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std::vector<size_t> m_irrev;
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Rate1<Plog> m_plog_rates;
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Rate1<ChebyshevRate> m_cheb_rates;
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size_t m_nirrev;
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size_t m_nrev;
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/**
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* Difference between the input global reactants order
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* and the input global products order. Changed to a double
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* to account for the fact that we can have real-valued
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* stoichiometries.
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*/
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vector_fp m_dn;
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std::vector<size_t> m_revindex;
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//! @name Reaction rate data
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//!@{
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doublereal m_logp_ref;
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doublereal m_logStandConc;
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vector_fp m_rfn_low;
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vector_fp m_rfn_high;
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bool m_ROP_ok;
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doublereal m_temp;
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doublereal m_pres; //!< Last pressure at which rates were evaluated
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vector_fp falloff_work;
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vector_fp concm_3b_values;
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vector_fp concm_falloff_values;
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//!@}
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vector_fp m_conc;
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void processFalloffReactions();
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vector_fp m_grt;
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private:
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void addElementaryReaction(ReactionData& r);
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void addThreeBodyReaction(ReactionData& r);
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void addFalloffReaction(ReactionData& r);
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void addPlogReaction(ReactionData& r);
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*
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* Homogeneous kinetics in an aqueous phase, either condensed
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* or dilute in salts
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*
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*/
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/*
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* Copyright (2006) Sandia Corporation. Under the terms of
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{
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AqueousKinetics::AqueousKinetics(thermo_t* thermo) :
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m_nfall(0),
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m_nirrev(0),
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m_nrev(0),
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m_ROP_ok(false),
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m_temp(0.0),
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m_finalized(false)
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BulkKinetics(thermo)
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{
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if (thermo != 0) {
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addPhase(*thermo);
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}
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}
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AqueousKinetics::AqueousKinetics(const AqueousKinetics& right) :
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m_nfall(0),
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m_nirrev(0),
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m_nrev(0),
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m_ROP_ok(false),
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m_temp(0.0),
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m_finalized(false)
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{
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*this = right;
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}
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AqueousKinetics& AqueousKinetics::operator=(const AqueousKinetics& right)
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{
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if (this == &right) {
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return *this;
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}
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Kinetics::operator=(right);
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m_nfall = right.m_nfall;
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m_rates = right.m_rates;
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m_irrev = right.m_irrev;
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m_nirrev = right.m_nirrev;
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m_nrev = right.m_nrev;
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m_rxntype = right.m_rxntype;
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m_dn = right.m_dn;
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m_revindex = right.m_revindex;
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m_ROP_ok = right.m_ROP_ok;
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m_temp = right.m_temp;
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m_conc = right.m_conc;
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m_grt = right.m_grt;
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m_finalized = right.m_finalized;
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throw CanteraError("GasKinetics::operator=()",
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"Unfinished implementation");
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return *this;
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}
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Kinetics* AqueousKinetics::duplMyselfAsKinetics(const std::vector<thermo_t*> & tpVector) const
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@ -81,19 +30,10 @@ Kinetics* AqueousKinetics::duplMyselfAsKinetics(const std::vector<thermo_t*> & t
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return gK;
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}
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void AqueousKinetics::update_T()
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{
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}
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void AqueousKinetics::update_C()
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{
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}
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void AqueousKinetics::_update_rates_T()
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{
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doublereal T = thermo().temperature();
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doublereal logT = log(T);
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m_rates.update(T, logT, &m_rfn[0]);
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m_rates.update(T, log(T), &m_rfn[0]);
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m_temp = T;
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updateKc();
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void AqueousKinetics::_update_rates_C()
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{
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thermo().getActivityConcentrations(&m_conc[0]);
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m_ROP_ok = false;
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}
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@ -122,12 +61,12 @@ void AqueousKinetics::updateKc()
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m_rxnstoich.getRevReactionDelta(m_ii, &m_grt[0], &m_rkcn[0]);
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doublereal rrt = 1.0/(GasConstant * thermo().temperature());
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for (size_t i = 0; i < m_nrev; i++) {
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for (size_t i = 0; i < m_revindex.size(); i++) {
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size_t irxn = m_revindex[i];
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m_rkcn[irxn] = exp(m_rkcn[irxn]*rrt);
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}
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for (size_t i = 0; i != m_nirrev; ++i) {
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for (size_t i = 0; i != m_irrev.size(); ++i) {
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m_rkcn[ m_irrev[i] ] = 0.0;
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}
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}
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@ -157,103 +96,6 @@ void AqueousKinetics::getEquilibriumConstants(doublereal* kc)
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m_temp = 0.0;
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}
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void AqueousKinetics::getDeltaGibbs(doublereal* deltaG)
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{
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/*
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* Get the chemical potentials of the species in the
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* ideal gas solution.
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*/
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thermo().getChemPotentials(&m_grt[0]);
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/*
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* Use the stoichiometric manager to find deltaG for each
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* reaction.
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*/
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m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaG);
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}
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void AqueousKinetics::getDeltaEnthalpy(doublereal* deltaH)
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{
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/*
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* Get the partial molar enthalpy of all species in the
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* ideal gas.
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*/
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thermo().getPartialMolarEnthalpies(&m_grt[0]);
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/*
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* Use the stoichiometric manager to find deltaG for each
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* reaction.
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*/
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m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaH);
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}
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||||
|
||||
void AqueousKinetics::getDeltaEntropy(doublereal* deltaS)
|
||||
{
|
||||
/*
|
||||
* Get the partial molar entropy of all species in the
|
||||
* solid solution.
|
||||
*/
|
||||
thermo().getPartialMolarEntropies(&m_grt[0]);
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaS for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaS);
|
||||
}
|
||||
|
||||
void AqueousKinetics::getDeltaSSGibbs(doublereal* deltaG)
|
||||
{
|
||||
/*
|
||||
* Get the standard state chemical potentials of the species.
|
||||
* This is the array of chemical potentials at unit activity
|
||||
* We define these here as the chemical potentials of the pure
|
||||
* species at the temperature and pressure of the solution.
|
||||
*/
|
||||
thermo().getStandardChemPotentials(&m_grt[0]);
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaG for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaG);
|
||||
}
|
||||
|
||||
void AqueousKinetics::getDeltaSSEnthalpy(doublereal* deltaH)
|
||||
{
|
||||
/*
|
||||
* Get the standard state enthalpies of the species.
|
||||
* This is the array of chemical potentials at unit activity
|
||||
* We define these here as the enthalpies of the pure
|
||||
* species at the temperature and pressure of the solution.
|
||||
*/
|
||||
thermo().getEnthalpy_RT(&m_grt[0]);
|
||||
doublereal RT = thermo().temperature() * GasConstant;
|
||||
for (size_t k = 0; k < m_kk; k++) {
|
||||
m_grt[k] *= RT;
|
||||
}
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaG for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaH);
|
||||
}
|
||||
|
||||
void AqueousKinetics::getDeltaSSEntropy(doublereal* deltaS)
|
||||
{
|
||||
/*
|
||||
* Get the standard state entropy of the species.
|
||||
* We define these here as the entropies of the pure
|
||||
* species at the temperature and pressure of the solution.
|
||||
*/
|
||||
thermo().getEntropy_R(&m_grt[0]);
|
||||
doublereal R = GasConstant;
|
||||
for (size_t k = 0; k < m_kk; k++) {
|
||||
m_grt[k] *= R;
|
||||
}
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaS for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaS);
|
||||
}
|
||||
|
||||
void AqueousKinetics::updateROP()
|
||||
{
|
||||
_update_rates_T();
|
||||
|
|
@ -272,19 +114,15 @@ void AqueousKinetics::updateROP()
|
|||
// copy the forward rates to the reverse rates
|
||||
copy(m_ropf.begin(), m_ropf.end(), m_ropr.begin());
|
||||
|
||||
// for reverse rates computed from thermochemistry, multiply
|
||||
// the forward rates copied into m_ropr by the reciprocals of
|
||||
// the equilibrium constants
|
||||
// for reverse rates computed from thermochemistry, multiply the forward
|
||||
// rates copied into m_ropr by the reciprocals of the equilibrium constants
|
||||
multiply_each(m_ropr.begin(), m_ropr.end(), m_rkcn.begin());
|
||||
|
||||
// multiply ropf by concentration products
|
||||
m_rxnstoich.multiplyReactants(&m_conc[0], &m_ropf[0]);
|
||||
//m_reactantStoich.multiply(m_conc.begin(), ropf.begin());
|
||||
|
||||
// for reversible reactions, multiply ropr by concentration
|
||||
// products
|
||||
// for reversible reactions, multiply ropr by concentration products
|
||||
m_rxnstoich.multiplyRevProducts(&m_conc[0], &m_ropr[0]);
|
||||
//m_revProductStoich.multiply(m_conc.begin(), ropr.begin());
|
||||
|
||||
for (size_t j = 0; j != m_ii; ++j) {
|
||||
m_ropnet[j] = m_ropf[j] - m_ropr[j];
|
||||
|
|
@ -309,84 +147,13 @@ void AqueousKinetics::getFwdRateConstants(doublereal* kfwd)
|
|||
}
|
||||
}
|
||||
|
||||
void AqueousKinetics::getRevRateConstants(doublereal* krev,
|
||||
bool doIrreversible)
|
||||
{
|
||||
/*
|
||||
* go get the forward rate constants. -> note, we don't
|
||||
* really care about speed or redundancy in these
|
||||
* informational routines.
|
||||
*/
|
||||
getFwdRateConstants(krev);
|
||||
|
||||
if (doIrreversible) {
|
||||
getEquilibriumConstants(&m_ropnet[0]);
|
||||
for (size_t i = 0; i < m_ii; i++) {
|
||||
krev[i] /= m_ropnet[i];
|
||||
}
|
||||
} else {
|
||||
/*
|
||||
* m_rkcn[] is zero for irreversible reactions
|
||||
*/
|
||||
for (size_t i = 0; i < m_ii; i++) {
|
||||
krev[i] *= m_rkcn[i];
|
||||
}
|
||||
}
|
||||
}
|
||||
|
||||
void AqueousKinetics::addReaction(ReactionData& r)
|
||||
{
|
||||
if (r.reactionType == ELEMENTARY_RXN) {
|
||||
addElementaryReaction(r);
|
||||
}
|
||||
|
||||
m_dn.push_back(accumulate(r.pstoich.begin(), r.pstoich.end(), 0.0) -
|
||||
accumulate(r.rstoich.begin(), r.rstoich.end(), 0.0));
|
||||
if (r.reversible) {
|
||||
m_revindex.push_back(nReactions());
|
||||
m_nrev++;
|
||||
} else {
|
||||
m_irrev.push_back(nReactions());
|
||||
m_nirrev++;
|
||||
}
|
||||
Kinetics::addReaction(r);
|
||||
}
|
||||
|
||||
void AqueousKinetics::addElementaryReaction(ReactionData& r)
|
||||
{
|
||||
// install rate coeff calculator
|
||||
m_rates.install(nReactions(), r);
|
||||
}
|
||||
|
||||
void AqueousKinetics::init()
|
||||
{
|
||||
m_kk = thermo().nSpecies();
|
||||
m_rrxn.resize(m_kk);
|
||||
m_prxn.resize(m_kk);
|
||||
m_conc.resize(m_kk);
|
||||
m_grt.resize(m_kk);
|
||||
}
|
||||
|
||||
void AqueousKinetics::finalize()
|
||||
{
|
||||
if (!m_finalized) {
|
||||
m_finalized = true;
|
||||
|
||||
// Guarantee that these arrays can be converted to double* even in the
|
||||
// special case where there are no reactions defined.
|
||||
if (!m_ii) {
|
||||
m_perturb.resize(1, 1.0);
|
||||
m_ropf.resize(1, 0.0);
|
||||
m_ropr.resize(1, 0.0);
|
||||
m_ropnet.resize(1, 0.0);
|
||||
m_rkcn.resize(1, 0.0);
|
||||
}
|
||||
}
|
||||
}
|
||||
|
||||
bool AqueousKinetics::ready() const
|
||||
{
|
||||
return m_finalized;
|
||||
BulkKinetics::addReaction(r);
|
||||
}
|
||||
|
||||
}
|
||||
|
|
|
|||
164
src/kinetics/BulkKinetics.cpp
Normal file
164
src/kinetics/BulkKinetics.cpp
Normal file
|
|
@ -0,0 +1,164 @@
|
|||
#include "cantera/kinetics/BulkKinetics.h"
|
||||
|
||||
namespace Cantera
|
||||
{
|
||||
|
||||
BulkKinetics::BulkKinetics(thermo_t* thermo) :
|
||||
m_ROP_ok(false),
|
||||
m_temp(0.0),
|
||||
m_finalized(false)
|
||||
{
|
||||
if (thermo) {
|
||||
addPhase(*thermo);
|
||||
}
|
||||
}
|
||||
|
||||
|
||||
Kinetics* BulkKinetics::duplMyselfAsKinetics(const std::vector<thermo_t*> & tpVector) const
|
||||
{
|
||||
BulkKinetics* kin = new BulkKinetics(*this);
|
||||
kin->assignShallowPointers(tpVector);
|
||||
return kin;
|
||||
}
|
||||
|
||||
bool BulkKinetics::isReversible(size_t i) {
|
||||
if (std::find(m_revindex.begin(), m_revindex.end(), i)
|
||||
< m_revindex.end()) {
|
||||
return true;
|
||||
} else {
|
||||
return false;
|
||||
}
|
||||
}
|
||||
|
||||
|
||||
void BulkKinetics::getDeltaGibbs(doublereal* deltaG)
|
||||
{
|
||||
// Get the chemical potentials of the species in the ideal gas solution.
|
||||
thermo().getChemPotentials(&m_grt[0]);
|
||||
// Use the stoichiometric manager to find deltaG for each reaction.
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaG);
|
||||
}
|
||||
|
||||
void BulkKinetics::getDeltaEnthalpy(doublereal* deltaH)
|
||||
{
|
||||
// Get the partial molar enthalpy of all species in the ideal gas.
|
||||
thermo().getPartialMolarEnthalpies(&m_grt[0]);
|
||||
// Use the stoichiometric manager to find deltaH for each reaction.
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaH);
|
||||
}
|
||||
|
||||
void BulkKinetics::getDeltaEntropy(doublereal* deltaS)
|
||||
{
|
||||
// Get the partial molar entropy of all species in the solid solution.
|
||||
thermo().getPartialMolarEntropies(&m_grt[0]);
|
||||
// Use the stoichiometric manager to find deltaS for each reaction.
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaS);
|
||||
}
|
||||
|
||||
void BulkKinetics::getDeltaSSGibbs(doublereal* deltaG)
|
||||
{
|
||||
// Get the standard state chemical potentials of the species. This is the
|
||||
// array of chemical potentials at unit activity. We define these here as
|
||||
// the chemical potentials of the pure species at the temperature and
|
||||
// pressure of the solution.
|
||||
thermo().getStandardChemPotentials(&m_grt[0]);
|
||||
// Use the stoichiometric manager to find deltaG for each reaction.
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaG);
|
||||
}
|
||||
|
||||
void BulkKinetics::getDeltaSSEnthalpy(doublereal* deltaH)
|
||||
{
|
||||
// Get the standard state enthalpies of the species.
|
||||
thermo().getEnthalpy_RT(&m_grt[0]);
|
||||
doublereal RT = thermo().temperature() * GasConstant;
|
||||
for (size_t k = 0; k < m_kk; k++) {
|
||||
m_grt[k] *= RT;
|
||||
}
|
||||
// Use the stoichiometric manager to find deltaH for each reaction.
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaH);
|
||||
}
|
||||
|
||||
void BulkKinetics::getDeltaSSEntropy(doublereal* deltaS)
|
||||
{
|
||||
// Get the standard state entropy of the species. We define these here as
|
||||
// the entropies of the pure species at the temperature and pressure of the
|
||||
// solution.
|
||||
thermo().getEntropy_R(&m_grt[0]);
|
||||
doublereal R = GasConstant;
|
||||
for (size_t k = 0; k < m_kk; k++) {
|
||||
m_grt[k] *= R;
|
||||
}
|
||||
// Use the stoichiometric manager to find deltaS for each reaction.
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaS);
|
||||
}
|
||||
|
||||
void BulkKinetics::getRevRateConstants(doublereal* krev, bool doIrreversible)
|
||||
{
|
||||
/*
|
||||
* go get the forward rate constants. -> note, we don't
|
||||
* really care about speed or redundancy in these
|
||||
* informational routines.
|
||||
*/
|
||||
getFwdRateConstants(krev);
|
||||
|
||||
if (doIrreversible) {
|
||||
getEquilibriumConstants(&m_ropnet[0]);
|
||||
for (size_t i = 0; i < m_ii; i++) {
|
||||
krev[i] /= m_ropnet[i];
|
||||
}
|
||||
} else {
|
||||
// m_rkcn[] is zero for irreversible reactions
|
||||
for (size_t i = 0; i < m_ii; i++) {
|
||||
krev[i] *= m_rkcn[i];
|
||||
}
|
||||
}
|
||||
}
|
||||
|
||||
void BulkKinetics::addReaction(ReactionData& r)
|
||||
{
|
||||
m_dn.push_back(accumulate(r.pstoich.begin(), r.pstoich.end(), 0.0) -
|
||||
accumulate(r.rstoich.begin(), r.rstoich.end(), 0.0));
|
||||
|
||||
if (r.reversible) {
|
||||
m_revindex.push_back(nReactions());
|
||||
} else {
|
||||
m_irrev.push_back(nReactions());
|
||||
}
|
||||
Kinetics::addReaction(r);
|
||||
}
|
||||
|
||||
void BulkKinetics::addElementaryReaction(ReactionData& r)
|
||||
{
|
||||
m_rates.install(nReactions(), r);
|
||||
}
|
||||
|
||||
void BulkKinetics::init()
|
||||
{
|
||||
m_kk = thermo().nSpecies();
|
||||
m_rrxn.resize(m_kk);
|
||||
m_prxn.resize(m_kk);
|
||||
m_conc.resize(m_kk);
|
||||
m_grt.resize(m_kk);
|
||||
}
|
||||
|
||||
void BulkKinetics::finalize()
|
||||
{
|
||||
m_finalized = true;
|
||||
|
||||
// Guarantee that these arrays can be converted to double* even in the
|
||||
// special case where there are no reactions defined.
|
||||
if (!m_ii) {
|
||||
m_perturb.resize(1, 1.0);
|
||||
m_ropf.resize(1, 0.0);
|
||||
m_ropr.resize(1, 0.0);
|
||||
m_ropnet.resize(1, 0.0);
|
||||
m_rkcn.resize(1, 0.0);
|
||||
}
|
||||
}
|
||||
|
||||
bool BulkKinetics::ready() const
|
||||
{
|
||||
return m_finalized;
|
||||
}
|
||||
|
||||
}
|
||||
|
|
@ -13,73 +13,13 @@ using namespace std;
|
|||
namespace Cantera
|
||||
{
|
||||
GasKinetics::GasKinetics(thermo_t* thermo) :
|
||||
BulkKinetics(thermo),
|
||||
m_nfall(0),
|
||||
m_nirrev(0),
|
||||
m_nrev(0),
|
||||
m_logp_ref(0.0),
|
||||
m_logc_ref(0.0),
|
||||
m_logStandConc(0.0),
|
||||
m_ROP_ok(false),
|
||||
m_temp(0.0),
|
||||
m_pres(0.0),
|
||||
m_finalized(false)
|
||||
m_pres(0.0)
|
||||
{
|
||||
if (thermo != 0) {
|
||||
addPhase(*thermo);
|
||||
}
|
||||
}
|
||||
|
||||
GasKinetics::GasKinetics(const GasKinetics& right)
|
||||
{
|
||||
*this = right;
|
||||
}
|
||||
|
||||
GasKinetics& GasKinetics::operator=(const GasKinetics& right)
|
||||
{
|
||||
if (this == &right) {
|
||||
return *this;
|
||||
}
|
||||
|
||||
Kinetics::operator=(right);
|
||||
|
||||
m_nfall = right.m_nfall;
|
||||
m_fallindx = right.m_fallindx;
|
||||
m_falloff_low_rates = right.m_falloff_low_rates;
|
||||
m_falloff_high_rates = right.m_falloff_high_rates;
|
||||
m_rates = right.m_rates;
|
||||
m_falloffn = right.m_falloffn;
|
||||
m_3b_concm = right.m_3b_concm;
|
||||
m_falloff_concm = right.m_falloff_concm;
|
||||
m_irrev = right.m_irrev;
|
||||
m_plog_rates = right.m_plog_rates;
|
||||
m_cheb_rates = right.m_cheb_rates;
|
||||
|
||||
m_nirrev = right.m_nirrev;
|
||||
m_nrev = right.m_nrev;
|
||||
m_rrxn = right.m_rrxn;
|
||||
m_prxn = right.m_prxn;
|
||||
m_dn = right.m_dn;
|
||||
m_revindex = right.m_revindex;
|
||||
|
||||
m_logp_ref = right.m_logp_ref;
|
||||
m_logc_ref = right.m_logc_ref;
|
||||
m_logStandConc = right.m_logStandConc;
|
||||
m_rfn_low = right.m_rfn_low;
|
||||
m_rfn_high = right.m_rfn_high;
|
||||
m_ROP_ok = right.m_ROP_ok;
|
||||
m_temp = right.m_temp;
|
||||
falloff_work = right.falloff_work;
|
||||
concm_3b_values = right.concm_3b_values;
|
||||
concm_falloff_values = right.concm_falloff_values;
|
||||
|
||||
m_conc = right.m_conc;
|
||||
m_grt = right.m_grt;
|
||||
m_finalized = right.m_finalized;
|
||||
|
||||
throw CanteraError("GasKinetics::operator=()",
|
||||
"Unfinished implementation");
|
||||
|
||||
return *this;
|
||||
}
|
||||
|
||||
Kinetics* GasKinetics::duplMyselfAsKinetics(const std::vector<thermo_t*> & tpVector) const
|
||||
|
|
@ -166,13 +106,13 @@ void GasKinetics::updateKc()
|
|||
m_rxnstoich.getRevReactionDelta(m_ii, &m_grt[0], &m_rkcn[0]);
|
||||
|
||||
doublereal rrt = 1.0/(GasConstant * thermo().temperature());
|
||||
for (size_t i = 0; i < m_nrev; i++) {
|
||||
for (size_t i = 0; i < m_revindex.size(); i++) {
|
||||
size_t irxn = m_revindex[i];
|
||||
m_rkcn[irxn] = std::min(exp(m_rkcn[irxn]*rrt - m_dn[irxn]*m_logStandConc),
|
||||
BigNumber);
|
||||
}
|
||||
|
||||
for (size_t i = 0; i != m_nirrev; ++i) {
|
||||
for (size_t i = 0; i != m_irrev.size(); ++i) {
|
||||
m_rkcn[ m_irrev[i] ] = 0.0;
|
||||
}
|
||||
}
|
||||
|
|
@ -196,103 +136,6 @@ void GasKinetics::getEquilibriumConstants(doublereal* kc)
|
|||
m_temp = 0.0;
|
||||
}
|
||||
|
||||
void GasKinetics::getDeltaGibbs(doublereal* deltaG)
|
||||
{
|
||||
/*
|
||||
* Get the chemical potentials of the species in the
|
||||
* ideal gas solution.
|
||||
*/
|
||||
thermo().getChemPotentials(&m_grt[0]);
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaG for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaG);
|
||||
}
|
||||
|
||||
void GasKinetics::getDeltaEnthalpy(doublereal* deltaH)
|
||||
{
|
||||
/*
|
||||
* Get the partial molar enthalpy of all species in the
|
||||
* ideal gas.
|
||||
*/
|
||||
thermo().getPartialMolarEnthalpies(&m_grt[0]);
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaG for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaH);
|
||||
}
|
||||
|
||||
void GasKinetics::getDeltaEntropy(doublereal* deltaS)
|
||||
{
|
||||
/*
|
||||
* Get the partial molar entropy of all species in the
|
||||
* solid solution.
|
||||
*/
|
||||
thermo().getPartialMolarEntropies(&m_grt[0]);
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaS for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaS);
|
||||
}
|
||||
|
||||
void GasKinetics::getDeltaSSGibbs(doublereal* deltaG)
|
||||
{
|
||||
/*
|
||||
* Get the standard state chemical potentials of the species.
|
||||
* This is the array of chemical potentials at unit activity
|
||||
* We define these here as the chemical potentials of the pure
|
||||
* species at the temperature and pressure of the solution.
|
||||
*/
|
||||
thermo().getStandardChemPotentials(&m_grt[0]);
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaG for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaG);
|
||||
}
|
||||
|
||||
void GasKinetics::getDeltaSSEnthalpy(doublereal* deltaH)
|
||||
{
|
||||
/*
|
||||
* Get the standard state enthalpies of the species.
|
||||
* This is the array of chemical potentials at unit activity
|
||||
* We define these here as the enthalpies of the pure
|
||||
* species at the temperature and pressure of the solution.
|
||||
*/
|
||||
thermo().getEnthalpy_RT(&m_grt[0]);
|
||||
doublereal RT = thermo().temperature() * GasConstant;
|
||||
for (size_t k = 0; k < m_kk; k++) {
|
||||
m_grt[k] *= RT;
|
||||
}
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaG for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaH);
|
||||
}
|
||||
|
||||
void GasKinetics::getDeltaSSEntropy(doublereal* deltaS)
|
||||
{
|
||||
/*
|
||||
* Get the standard state entropy of the species.
|
||||
* We define these here as the entropies of the pure
|
||||
* species at the temperature and pressure of the solution.
|
||||
*/
|
||||
thermo().getEntropy_R(&m_grt[0]);
|
||||
doublereal R = GasConstant;
|
||||
for (size_t k = 0; k < m_kk; k++) {
|
||||
m_grt[k] *= R;
|
||||
}
|
||||
/*
|
||||
* Use the stoichiometric manager to find deltaS for each
|
||||
* reaction.
|
||||
*/
|
||||
m_rxnstoich.getReactionDelta(m_ii, &m_grt[0], deltaS);
|
||||
}
|
||||
|
||||
void GasKinetics::processFalloffReactions()
|
||||
{
|
||||
// use m_ropr for temporary storage of reduced pressure
|
||||
|
|
@ -346,19 +189,15 @@ void GasKinetics::updateROP()
|
|||
// copy the forward rates to the reverse rates
|
||||
copy(m_ropf.begin(), m_ropf.end(), m_ropr.begin());
|
||||
|
||||
// for reverse rates computed from thermochemistry, multiply
|
||||
// the forward rates copied into m_ropr by the reciprocals of
|
||||
// the equilibrium constants
|
||||
// for reverse rates computed from thermochemistry, multiply the forward
|
||||
// rates copied into m_ropr by the reciprocals of the equilibrium constants
|
||||
multiply_each(m_ropr.begin(), m_ropr.end(), m_rkcn.begin());
|
||||
|
||||
// multiply ropf by concentration products
|
||||
m_rxnstoich.multiplyReactants(&m_conc[0], &m_ropf[0]);
|
||||
//m_reactantStoich.multiply(m_conc.begin(), ropf.begin());
|
||||
|
||||
// for reversible reactions, multiply ropr by concentration
|
||||
// products
|
||||
// for reversible reactions, multiply ropr by concentration products
|
||||
m_rxnstoich.multiplyRevProducts(&m_conc[0], &m_ropr[0]);
|
||||
//m_revProductStoich.multiply(m_conc.begin(), ropr.begin());
|
||||
|
||||
for (size_t j = 0; j != m_ii; ++j) {
|
||||
m_ropnet[j] = m_ropf[j] - m_ropr[j];
|
||||
|
|
@ -389,10 +228,6 @@ void GasKinetics::getFwdRateConstants(doublereal* kfwd)
|
|||
m_3b_concm.multiply(&m_ropf[0], &concm_3b_values[0]);
|
||||
}
|
||||
|
||||
/*
|
||||
* This routine is hardcoded to replace some of the values
|
||||
* of the ropf vector.
|
||||
*/
|
||||
if (m_nfall) {
|
||||
processFalloffReactions();
|
||||
}
|
||||
|
|
@ -405,28 +240,6 @@ void GasKinetics::getFwdRateConstants(doublereal* kfwd)
|
|||
}
|
||||
}
|
||||
|
||||
void GasKinetics::getRevRateConstants(doublereal* krev, bool doIrreversible)
|
||||
{
|
||||
/*
|
||||
* go get the forward rate constants. -> note, we don't
|
||||
* really care about speed or redundancy in these
|
||||
* informational routines.
|
||||
*/
|
||||
getFwdRateConstants(krev);
|
||||
|
||||
if (doIrreversible) {
|
||||
getEquilibriumConstants(&m_ropnet[0]);
|
||||
for (size_t i = 0; i < m_ii; i++) {
|
||||
krev[i] /= m_ropnet[i];
|
||||
}
|
||||
} else {
|
||||
// m_rkcn[] is zero for irreversible reactions
|
||||
for (size_t i = 0; i < m_ii; i++) {
|
||||
krev[i] *= m_rkcn[i];
|
||||
}
|
||||
}
|
||||
}
|
||||
|
||||
void GasKinetics::addReaction(ReactionData& r)
|
||||
{
|
||||
switch (r.reactionType) {
|
||||
|
|
@ -451,17 +264,7 @@ void GasKinetics::addReaction(ReactionData& r)
|
|||
}
|
||||
|
||||
// operations common to all reaction types
|
||||
m_dn.push_back(accumulate(r.pstoich.begin(), r.pstoich.end(), 0.0) -
|
||||
accumulate(r.rstoich.begin(), r.rstoich.end(), 0.0));
|
||||
|
||||
if (r.reversible) {
|
||||
m_revindex.push_back(nReactions());
|
||||
m_nrev++;
|
||||
} else {
|
||||
m_irrev.push_back(nReactions());
|
||||
m_nirrev++;
|
||||
}
|
||||
Kinetics::addReaction(r);
|
||||
BulkKinetics::addReaction(r);
|
||||
}
|
||||
|
||||
void GasKinetics::addFalloffReaction(ReactionData& r)
|
||||
|
|
@ -474,17 +277,15 @@ void GasKinetics::addFalloffReaction(ReactionData& r)
|
|||
m_falloff_low_rates.install(m_nfall, r);
|
||||
m_rfn_low.push_back(r.rateCoeffParameters[0]);
|
||||
|
||||
// add this reaction number to the list of
|
||||
// falloff reactions
|
||||
// add this reaction number to the list of falloff reactions
|
||||
m_fallindx.push_back(nReactions());
|
||||
|
||||
// install the enhanced third-body concentration
|
||||
// calculator for this reaction
|
||||
// install the enhanced third-body concentration calculator for this
|
||||
// reaction
|
||||
m_falloff_concm.install(m_nfall, r.thirdBodyEfficiencies,
|
||||
r.default_3b_eff);
|
||||
|
||||
// install the falloff function calculator for
|
||||
// this reaction
|
||||
// install the falloff function calculator for this reaction
|
||||
m_falloffn.install(m_nfall, r.falloffType, r.reactionType,
|
||||
r.falloffParameters);
|
||||
|
||||
|
|
@ -492,14 +293,8 @@ void GasKinetics::addFalloffReaction(ReactionData& r)
|
|||
++m_nfall;
|
||||
}
|
||||
|
||||
void GasKinetics::addElementaryReaction(ReactionData& r)
|
||||
{
|
||||
m_rates.install(nReactions(), r);
|
||||
}
|
||||
|
||||
void GasKinetics::addThreeBodyReaction(ReactionData& r)
|
||||
{
|
||||
// install rate coeff calculator
|
||||
m_rates.install(nReactions(), r);
|
||||
m_3b_concm.install(nReactions(), r.thirdBodyEfficiencies,
|
||||
r.default_3b_eff);
|
||||
|
|
@ -507,44 +302,26 @@ void GasKinetics::addThreeBodyReaction(ReactionData& r)
|
|||
|
||||
void GasKinetics::addPlogReaction(ReactionData& r)
|
||||
{
|
||||
// install rate coefficient calculator
|
||||
m_plog_rates.install(nReactions(), r);
|
||||
}
|
||||
|
||||
void GasKinetics::addChebyshevReaction(ReactionData& r)
|
||||
{
|
||||
// install rate coefficient calculator
|
||||
m_cheb_rates.install(nReactions(), r);
|
||||
}
|
||||
|
||||
void GasKinetics::init()
|
||||
{
|
||||
m_kk = thermo().nSpecies();
|
||||
m_rrxn.resize(m_kk);
|
||||
m_prxn.resize(m_kk);
|
||||
m_conc.resize(m_kk);
|
||||
m_grt.resize(m_kk);
|
||||
BulkKinetics::init();
|
||||
m_logp_ref = log(thermo().refPressure()) - log(GasConstant);
|
||||
}
|
||||
|
||||
void GasKinetics::finalize()
|
||||
{
|
||||
if (!m_finalized) {
|
||||
falloff_work.resize(m_falloffn.workSize());
|
||||
concm_3b_values.resize(m_3b_concm.workSize());
|
||||
concm_falloff_values.resize(m_falloff_concm.workSize());
|
||||
m_finalized = true;
|
||||
|
||||
// Guarantee that these arrays can be converted to double* even in the
|
||||
// special case where there are no reactions defined.
|
||||
if (!m_ii) {
|
||||
m_perturb.resize(1, 1.0);
|
||||
m_ropf.resize(1, 0.0);
|
||||
m_ropr.resize(1, 0.0);
|
||||
m_ropnet.resize(1, 0.0);
|
||||
m_rkcn.resize(1, 0.0);
|
||||
}
|
||||
}
|
||||
BulkKinetics::finalize();
|
||||
falloff_work.resize(m_falloffn.workSize());
|
||||
concm_3b_values.resize(m_3b_concm.workSize());
|
||||
concm_falloff_values.resize(m_falloff_concm.workSize());
|
||||
}
|
||||
|
||||
bool GasKinetics::ready() const
|
||||
|
|
|
|||
Loading…
Add table
Reference in a new issue