/** * @file GasKinetics.cpp * * Homogeneous kinetics in ideal gases * */ // Copyright 2001 California Institute of Technology #include "GasKinetics.h" #include "ReactionData.h" #include "Enhanced3BConc.h" #include "ThirdBodyMgr.h" #include "RateCoeffMgr.h" //#include "../user/grirxnstoich.h" #include using namespace std; namespace Cantera { /** * Construct an empty reaction mechanism. */ GasKinetics:: GasKinetics(thermo_t* thermo) : Kinetics(), m_kk(0), m_nfall(0), m_nirrev(0), m_nrev(0), m_finalized(false) { if (thermo != 0) addPhase(*thermo); m_kdata = new GasKineticsData; m_kdata->m_temp = 0.0; m_rxnstoich = new ReactionStoichMgr; } GasKinetics:: ~GasKinetics() {delete m_kdata; delete m_rxnstoich;} /** * Update temperature-dependent portions of reaction rates and * falloff functions. */ void GasKinetics:: update_T() {} void GasKinetics:: update_C() {} void GasKinetics:: _update_rates_T() { doublereal T = thermo().temperature(); m_kdata->m_logStandConc = log(thermo().standardConcentration()); doublereal logT = log(T); if (!m_kdata->m_rfn.empty()) { m_rates.update(T, logT, &m_kdata->m_rfn[0]); } if (!m_kdata->m_rfn_low.empty()) { m_falloff_low_rates.update(T, logT, &m_kdata->m_rfn_low[0]); m_falloff_high_rates.update(T, logT, &m_kdata->m_rfn_high[0]); } if (!m_kdata->falloff_work.empty()) { m_falloffn.updateTemp(T, &m_kdata->falloff_work[0]); } m_kdata->m_temp = T; updateKc(); m_kdata->m_ROP_ok = false; } /** * Update properties that depend on concentrations. Currently only * the enhanced collision partner concentrations are updated here. */ void GasKinetics:: _update_rates_C() { thermo().getActivityConcentrations(&m_conc[0]); doublereal ctot = thermo().molarDensity(); if (!m_kdata->concm_3b_values.empty()) { m_3b_concm.update(m_conc, ctot, &m_kdata->concm_3b_values[0]); } if (!m_kdata->concm_falloff_values.empty()) { m_falloff_concm.update(m_conc, ctot, &m_kdata->concm_falloff_values[0]); } m_kdata->m_ROP_ok = false; } /** * Update the equilibrium constants in molar units. */ void GasKinetics::updateKc() { int i, irxn; vector_fp& m_rkc = m_kdata->m_rkcn; thermo().getStandardChemPotentials(&m_grt[0]); fill(m_rkc.begin(), m_rkc.end(), 0.0); // compute Delta G^0 for all reversible reactions m_rxnstoich->getRevReactionDelta(m_ii, &m_grt[0], &m_rkc[0]); doublereal logStandConc = m_kdata->m_logStandConc; doublereal rrt = 1.0/(GasConstant * thermo().temperature()); for (i = 0; i < m_nrev; i++) { irxn = m_revindex[i]; m_rkc[irxn] = exp(m_rkc[irxn]*rrt - m_dn[irxn]*logStandConc); } for(i = 0; i != m_nirrev; ++i) { m_rkc[ m_irrev[i] ] = 0.0; } } /** * Get the equilibrium constants of all reactions, whether * reversible or not. */ void GasKinetics::getEquilibriumConstants(doublereal* kc) { int i; _update_rates_T(); vector_fp& rkc = m_kdata->m_rkcn; //thermo().getGibbs_RT(m_grt.begin()); thermo().getStandardChemPotentials(&m_grt[0]); fill(rkc.begin(), rkc.end(), 0.0); // compute Delta G^0 for all reactions m_rxnstoich->getReactionDelta(m_ii, &m_grt[0], &rkc[0]); doublereal logStandConc = m_kdata->m_logStandConc; doublereal rrt = 1.0/(GasConstant * thermo().temperature()); for (i = 0; i < m_ii; i++) { kc[i] = exp(-rkc[i]*rrt + m_dn[i]*logStandConc); } // force an update of T-dependent properties, so that m_rkcn will // be updated before it is used next. m_kdata->m_temp = 0.0; } /** * * getDeltaGibbs(): * * Return the vector of values for the reaction gibbs free energy * change * These values depend upon the concentration * of the ideal gas. * * units = J kmol-1 */ 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); } /** * * getDeltaEnthalpy(): * * Return the vector of values for the reactions change in * enthalpy. * These values depend upon the concentration * of the solution. * * units = J kmol-1 */ 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); } /************************************************************************ * * getDeltaEntropy(): * * Return the vector of values for the reactions change in * entropy. * These values depend upon the concentration * of the solution. * * units = J kmol-1 Kelvin-1 */ 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); } /** * * getDeltaSSGibbs(): * * Return the vector of values for the reaction * standard state gibbs free energy change. * These values don't depend upon the concentration * of the solution. * * units = J kmol-1 */ 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); } /** * * getDeltaSSEnthalpy(): * * Return the vector of values for the change in the * standard state enthalpies of reaction. * These values don't depend upon the concentration * of the solution. * * units = J kmol-1 */ 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 (int 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); } /********************************************************************* * * getDeltaSSEntropy(): * * Return the vector of values for the change in the * standard state entropies for each reaction. * These values don't depend upon the concentration * of the solution. * * units = J kmol-1 Kelvin-1 */ 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 (int 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() { int i; const vector_fp& fc = m_kdata->concm_falloff_values; const array_fp& m_rf_low = m_kdata->m_rfn_low; const array_fp& m_rf_high = m_kdata->m_rfn_high; // use m_ropr for temporary storage of reduced pressure array_fp& pr = m_kdata->m_ropr; array_fp& ropf = m_kdata->m_ropf; for (i = 0; i < m_nfall; i++) { pr[i] = fc[i] * m_rf_low[i] / m_rf_high[i]; } double* falloff_work = (m_kdata->falloff_work.empty()) ? 0 : &m_kdata->falloff_work[0]; m_falloffn.pr_to_falloff(&pr[0], falloff_work); for (i = 0; i < m_nfall; i++) { pr[i] *= m_rf_high[i]; } scatter_copy(pr.begin(), pr.begin() + m_nfall, ropf.begin(), m_fallindx.begin()); } void GasKinetics::updateROP() { _update_rates_T(); _update_rates_C(); if (m_kdata->m_ROP_ok) return; const vector_fp& rf = m_kdata->m_rfn; const vector_fp& m_rkc = m_kdata->m_rkcn; array_fp& ropf = m_kdata->m_ropf; array_fp& ropr = m_kdata->m_ropr; array_fp& ropnet = m_kdata->m_ropnet; // copy rate coefficients into ropf copy(rf.begin(), rf.end(), ropf.begin()); // multiply ropf by enhanced 3b conc for all 3b rxns if (!m_kdata->concm_3b_values.empty()) { m_3b_concm.multiply( &ropf[0], &m_kdata->concm_3b_values[0] ); } if (m_nfall) { processFalloffReactions(); } // multiply by perturbation factor multiply_each(ropf.begin(), ropf.end(), m_perturb.begin()); // copy the forward rates to the reverse rates copy(ropf.begin(), ropf.end(), ropr.begin()); // for reverse rates computed from thermochemistry, multiply // the forward rates copied into m_ropr by the reciprocals of // the equilibrium constants multiply_each(ropr.begin(), ropr.end(), m_rkc.begin()); // multiply ropf by concentration products m_rxnstoich->multiplyReactants(&m_conc[0], &ropf[0]); //m_reactantStoich.multiply(m_conc.begin(), ropf.begin()); // for reversible reactions, multiply ropr by concentration // products m_rxnstoich->multiplyRevProducts(&m_conc[0], &ropr[0]); //m_revProductStoich.multiply(m_conc.begin(), ropr.begin()); for (int j = 0; j != m_ii; ++j) { ropnet[j] = ropf[j] - ropr[j]; } m_kdata->m_ROP_ok = true; } /** * * getFwdRateConstants(): * * Update the rate of progress for the reactions. * This key routine makes sure that the rate of progress vectors * located in the solid kinetics data class are up to date. */ void GasKinetics:: getFwdRateConstants(doublereal *kfwd) { _update_rates_T(); _update_rates_C(); // copy rate coefficients into ropf const vector_fp& rf = m_kdata->m_rfn; array_fp& ropf = m_kdata->m_ropf; copy(rf.begin(), rf.end(), ropf.begin()); // multiply ropf by enhanced 3b conc for all 3b rxns if (!m_kdata->concm_3b_values.empty()) { m_3b_concm.multiply(&ropf[0], &m_kdata->concm_3b_values[0] ); } /* * This routine is hardcoded to replace some of the values * of the ropf vector. */ if (m_nfall) { processFalloffReactions(); } // multiply by perturbation factor multiply_each(ropf.begin(), ropf.end(), m_perturb.begin()); for (int i = 0; i < m_ii; i++) { kfwd[i] = ropf[i]; } } /** * * getRevRateConstants(): * * Return a vector of the reverse reaction rate constants * * Length is the number of reactions. units depends * on many issues. Note, this routine will return rate constants * for irreversible reactions if the default for * doIrreversible is overridden. */ 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) { doublereal *tmpKc = &m_kdata->m_ropnet[0]; getEquilibriumConstants(tmpKc); for (int i = 0; i < m_ii; i++) { krev[i] /= tmpKc[i]; } } else { /* * m_rkc[] is zero for irreversibly reactions */ const vector_fp& m_rkc = m_kdata->m_rkcn; for (int i = 0; i < m_ii; i++) { krev[i] *= m_rkc[i]; } } } void GasKinetics:: addReaction(const ReactionData& r) { if (r.reactionType == ELEMENTARY_RXN) addElementaryReaction(r); else if (r.reactionType == THREE_BODY_RXN) addThreeBodyReaction(r); else if (r.reactionType == FALLOFF_RXN) addFalloffReaction(r); // operations common to all reaction types installReagents( r ); installGroups(reactionNumber(), r.rgroups, r.pgroups); incrementRxnCount(); m_rxneqn.push_back(r.equation); } void GasKinetics:: addFalloffReaction(const ReactionData& r) { // install high and low rate coeff calculators size_t iloc = m_falloff_high_rates.install(m_nfall, r.rateCoeffType, r.rateCoeffParameters.size(), &r.rateCoeffParameters[0] ); m_falloff_low_rates.install( m_nfall, r.rateCoeffType, r.auxRateCoeffParameters.size(), DATA_PTR(r.auxRateCoeffParameters) ); // add constant terms to high and low rate // coeff value vectors m_kdata->m_rfn_high.push_back(r.rateCoeffParameters[0]); m_kdata->m_rfn_low.push_back(r.auxRateCoeffParameters[0]); // add a dummy entry in m_rf, where computed falloff // rate coeff will be put m_kdata->m_rfn.push_back(0.0); // add this reaction number to the list of // falloff reactions m_fallindx.push_back( reactionNumber() ); // 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 m_falloffn.install( m_nfall, r.falloffType, r.falloffParameters ); // forward rxn order equals number of reactants, since rate // coeff is defined in terms of the high-pressure limit m_fwdOrder.push_back(r.reactants.size()); // increment the falloff reaction counter ++m_nfall; registerReaction( reactionNumber(), FALLOFF_RXN, iloc); } void GasKinetics:: addElementaryReaction(const ReactionData& r) { size_t iloc; // install rate coeff calculator iloc = m_rates.install( reactionNumber(), r.rateCoeffType, r.rateCoeffParameters.size(), DATA_PTR(r.rateCoeffParameters) ); // add constant term to rate coeff value vector m_kdata->m_rfn.push_back(r.rateCoeffParameters[0]); // forward rxn order equals number of reactants m_fwdOrder.push_back(r.reactants.size()); registerReaction( reactionNumber(), ELEMENTARY_RXN, iloc); } void GasKinetics:: addThreeBodyReaction(const ReactionData& r) { size_t iloc; // install rate coeff calculator iloc = m_rates.install( reactionNumber(), r.rateCoeffType, r.rateCoeffParameters.size(), DATA_PTR(r.rateCoeffParameters) ); // add constant term to rate coeff value vector m_kdata->m_rfn.push_back(r.rateCoeffParameters[0]); // forward rxn order equals number of reactants + 1 m_fwdOrder.push_back(r.reactants.size() + 1); m_3b_concm.install( reactionNumber(), r.thirdBodyEfficiencies, r.default_3b_eff ); registerReaction( reactionNumber(), THREE_BODY_RXN, iloc); } void GasKinetics::installReagents(const ReactionData& r) { m_kdata->m_ropf.push_back(0.0); // extend by one for new rxn m_kdata->m_ropr.push_back(0.0); m_kdata->m_ropnet.push_back(0.0); size_t n, ns, m; doublereal nsFlt; doublereal reactantGlobalOrder = 0.0; doublereal productGlobalOrder = 0.0; size_t rnum = reactionNumber(); std::vector rk; size_t nr = r.reactants.size(); for (n = 0; n < nr; n++) { nsFlt = r.rstoich[n]; reactantGlobalOrder += nsFlt; ns = (size_t) nsFlt; if ((doublereal) ns != nsFlt) { if (ns < 1) { ns = 1; } } if (r.rstoich[n] != 0.0) m_rrxn[r.reactants[n]][rnum] += r.rstoich[n]; for (m = 0; m < ns; m++) { rk.push_back(r.reactants[n]); } } m_reactants.push_back(rk); std::vector pk; size_t np = r.products.size(); for (n = 0; n < np; n++) { nsFlt = r.pstoich[n]; productGlobalOrder += nsFlt; ns = (size_t) nsFlt; if ((double) ns != nsFlt) { if (ns < 1) { ns = 1; } } if (r.pstoich[n] != 0.0) m_prxn[r.products[n]][rnum] += r.pstoich[n]; for (m = 0; m < ns; m++) { pk.push_back(r.products[n]); } } m_products.push_back(pk); m_kdata->m_rkcn.push_back(0.0); m_rxnstoich->add(reactionNumber(), r); if (r.reversible) { m_dn.push_back(productGlobalOrder - reactantGlobalOrder); m_revindex.push_back(reactionNumber()); m_nrev++; } else { m_dn.push_back(productGlobalOrder - reactantGlobalOrder); m_irrev.push_back( reactionNumber() ); m_nirrev++; } } void GasKinetics::installGroups(int irxn, const vector& r, const vector& p) { if (!r.empty()) { writelog("installing groups for reaction "+int2str(reactionNumber())); m_rgroups[reactionNumber()] = r; m_pgroups[reactionNumber()] = p; } } 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); m_kdata->m_logp_ref = log(thermo().refPressure()) - log(GasConstant); } void GasKinetics::finalize() { if (!m_finalized) { // int i, j, nr, np; m_kdata->falloff_work.resize( static_cast(m_falloffn.workSize())); m_kdata->concm_3b_values.resize( static_cast(m_3b_concm.workSize())); m_kdata->concm_falloff_values.resize( static_cast(m_falloff_concm.workSize())); // for (i = 0; i < m_ii; i++) { // nr = m_reactants[i].size(); // for (j = 0; j < nr; j++) { // m_rstoich[i][m_reactants[i][j]]++; // } // np = m_products[i].size(); // for (j = 0; j < np; j++) { // m_pstoich[i][m_products[i][j]]++; // } // } //m_rxnstoich->write("c.cpp"); m_finalized = true; } } bool GasKinetics::ready() const { return (m_finalized); } }