From 85d9d360c77444e27f67bb5975bd0d9e922361d5 Mon Sep 17 00:00:00 2001 From: Ray Speth Date: Fri, 17 Aug 2012 16:43:34 +0000 Subject: [PATCH] Fixed a bunch of spelling issues --- include/cantera/base/ctml.h | 12 +++---- include/cantera/equil/MultiPhase.h | 2 +- include/cantera/equil/vcs_defs.h | 6 ++-- include/cantera/equil/vcs_solve.h | 22 ++++++------ include/cantera/kinetics/ReactionData.h | 2 +- include/cantera/kinetics/ReactionStoichMgr.h | 2 +- include/cantera/numerics/NonlinearSolver.h | 2 +- include/cantera/thermo/IdealGasPhase.h | 2 +- include/cantera/thermo/IdealSolidSolnPhase.h | 2 +- include/cantera/thermo/LatticePhase.h | 2 +- include/cantera/thermo/LatticeSolidPhase.h | 4 +-- include/cantera/thermo/RedlichKwongMFTP.h | 4 +-- include/cantera/thermo/ThermoPhase.h | 2 +- include/cantera/transport/LiquidTransport.h | 4 +-- include/cantera/transport/SimpleTransport.h | 2 +- src/apps/csvdiff.cpp | 5 ++- src/base/ctml.cpp | 18 +++++----- src/equil/BasisOptimize.cpp | 6 ++-- src/equil/ChemEquil.cpp | 2 +- src/equil/vcs_MultiPhaseEquil.cpp | 4 +-- src/equil/vcs_elem.cpp | 4 +-- src/equil/vcs_phaseStability.cpp | 2 +- src/equil/vcs_solve_TP.cpp | 34 +++++++++---------- src/kinetics/Kinetics.cpp | 2 +- src/kinetics/KineticsFactory.cpp | 2 +- src/kinetics/importKinetics.cpp | 4 +-- src/numerics/NonlinearSolver.cpp | 2 +- src/oneD/OneDim.cpp | 2 +- src/thermo/DebyeHuckel.cpp | 4 +-- src/thermo/HMWSoln.cpp | 6 ++-- src/thermo/HMWSoln_input.cpp | 2 +- src/thermo/IdealSolidSolnPhase.cpp | 10 +++--- src/thermo/LatticeSolidPhase.cpp | 2 +- src/thermo/MineralEQ3.cpp | 2 +- src/thermo/PDSS_HKFT.cpp | 4 +-- src/thermo/RedlichKwongMFTP.cpp | 2 +- src/thermo/SpeciesThermoFactory.cpp | 16 ++++----- src/thermo/ThermoPhase.cpp | 2 +- src/thermo/VPSSMgrFactory.cpp | 4 +-- src/transport/LiquidTransport.cpp | 6 ++-- .../VCSnonideal/NaCl_equil/HMW_NaCl.xml | 18 +++++----- .../HMW_dupl_test/HMW_NaCl_sp1977_alt.xml | 12 +++---- .../HMW_graph_CpvT/HMW_NaCl_sp1977_alt.xml | 12 +++---- .../cathermo/HMW_graph_GvI/HMW_NaCl.xml | 18 +++++----- .../HMW_graph_GvT/HMW_NaCl_sp1977_alt.xml | 12 +++---- .../HMW_graph_HvT/HMW_NaCl_sp1977_alt.xml | 12 +++---- .../HMW_graph_VvT/HMW_NaCl_sp1977_alt.xml | 12 +++---- 47 files changed, 156 insertions(+), 157 deletions(-) diff --git a/include/cantera/base/ctml.h b/include/cantera/base/ctml.h index e2e4b1377..c8e18ac5b 100644 --- a/include/cantera/base/ctml.h +++ b/include/cantera/base/ctml.h @@ -316,7 +316,7 @@ void getMap(const Cantera::XML_Node& node, std::map& m //! This function interprets the value portion of an XML element //! as a series of "Pairs" separated by white space. /*! - * Each pair consists of nonwhite-space characters. + * Each pair consists of non-whitespace characters. * The first ":" found in the pair string is used to separate * the string into two parts. The first part is called the "key" * The second part is called the "val". @@ -351,7 +351,7 @@ int getPairs(const Cantera::XML_Node& node, std::vector& key, //! This function interprets the value portion of an XML element //! as a series of "Matrix ids and entries" separated by white space. /*! - * Each pair consists of nonwhite-space characters. + * Each pair consists of non-whitespace characters. * The first two ":" found in the pair string is used to separate * the string into three parts. The first part is called the first * key. The second part is the second key. Both parts must match @@ -384,7 +384,7 @@ int getPairs(const Cantera::XML_Node& node, std::vector& key, * @param keyStringCol Key string for the column entries * @param returnValues Return Matrix. * @param convert If this is true, and if the node has a units - * attribute, then conversion to si units is carried + * attribute, then conversion to SI units is carried * out. Default is true. * @param matrixSymmetric If true entries are made so that the matrix * is always symmetric. Default is false. @@ -755,7 +755,7 @@ void getNamedStringValue(const Cantera::XML_Node& node, const std::string& nameS * Code snippet: * @verbatim const XML_Node &parent; - string nameString = "vacency_species"; + string nameString = "vacancy_species"; string valueString = getChildValue(parent, nameString std::string typeString); @endverbatim @@ -765,9 +765,9 @@ void getNamedStringValue(const Cantera::XML_Node& node, const std::string& nameS * from the following the snippet in the XML file: * * @verbatim - + O(V) - <\vancencySpecies> + <\vacancySpecies> @endverbatim * * @param parent parent reference to the XML_Node object of the parent XML element diff --git a/include/cantera/equil/MultiPhase.h b/include/cantera/equil/MultiPhase.h index 792b11c67..f221e013b 100644 --- a/include/cantera/equil/MultiPhase.h +++ b/include/cantera/equil/MultiPhase.h @@ -419,7 +419,7 @@ public: /// Volume [m^3]. /*! - * Returns the cummulative sum of the volumes of all the + * Returns the cumulative sum of the volumes of all the * phases in the %MultiPhase. */ doublereal volume() const; diff --git a/include/cantera/equil/vcs_defs.h b/include/cantera/equil/vcs_defs.h index c83743fc8..74c00e148 100644 --- a/include/cantera/equil/vcs_defs.h +++ b/include/cantera/equil/vcs_defs.h @@ -168,7 +168,7 @@ namespace VCSnonideal //! Species is a SS phase, that is currently zeroed out. /*! * The species lies in a single-species phase which - * is currently zereod out. + * is currently zeroed out. */ #define VCS_SPECIES_ZEROEDSS -3 @@ -185,7 +185,7 @@ namespace VCSnonideal /*! * The unknown is equal to the interfacial voltage * drop across the interface on the SHE (standard - * hyrdogen electrode) scale (volts). + * hydrogen electrode) scale (volts). */ #define VCS_SPECIES_INTERFACIALVOLTAGE -5 @@ -363,7 +363,7 @@ namespace VCSnonideal /*! * Typically, these species are electrons in metals. There is an * infinite supply of them. However, their electrical potential - * is ddefined by the interface voltage. + * is defined by the interface voltage. */ #define VCS_SPECIES_TYPE_INTERFACIALVOLTAGE -5 //@} diff --git a/include/cantera/equil/vcs_solve.h b/include/cantera/equil/vcs_solve.h index 494707b2f..9bbeb1def 100644 --- a/include/cantera/equil/vcs_solve.h +++ b/include/cantera/equil/vcs_solve.h @@ -120,7 +120,7 @@ public: //! Main routine that solves for equilibrium at constant T and P //! using a variant of the VCS method /*! - * This is the main routine taht solves for equilibrium at constant T and P + * This is the main routine that solves for equilibrium at constant T and P * using a variant of the VCS method. Nonideal phases can be accommodated * as well. * @@ -232,7 +232,7 @@ public: * * @param molNum Mole number vector * @param j index into molNum[] that indicates where the search will start from - * Previous successful components are swapped into the fronto of + * Previous successful components are swapped into the front of * molNum[]. * @param n Length of molNum[] */ @@ -633,7 +633,7 @@ public: /*! * 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 + * However, if the phase is currently zeroed out, a subproblem * is calculated to solve for AC[i] and pseudo-X[i] for that * phase. * @@ -1151,7 +1151,7 @@ private: */ int vcs_delete_species(const size_t kspec); - //! This routine handles the bookkeepking involved with the + //! This routine handles the bookkeeping involved with the //! deletion of multiphase phases from the problem. /*! * When they are deleted, all of their species become active @@ -1314,7 +1314,7 @@ private: * * along the current direction m_deltaMolNumSpecies[], by choosing a value, al: (0 Species lies in a single-species phase which - * is currently zereod out. - * - VCS_SPECIES_ZEREODSS + * is currently zeroed out. + * - VCS_SPECIES_ZEROEDSS * -4 -> Species has such a small mole fraction it is * deleted even though its phase may possibly exist. * The species is believed to have such a small @@ -1826,7 +1826,7 @@ public: * -5 -> Species refers to an electron in the metal * The unknown is equal to the interfacial voltage * drop across the interface on the SHE (standard - * hydroogen electrode) scale (volts). + * hydrogen electrode) scale (volts). * - VCS_SPECIES_INTERFACIALVOLTAGE * -6 -> Species lies in a multicomponent phase that * is zeroed atm and will stay deleted due to a diff --git a/include/cantera/kinetics/ReactionData.h b/include/cantera/kinetics/ReactionData.h index ddcf48dc4..fb07624f8 100644 --- a/include/cantera/kinetics/ReactionData.h +++ b/include/cantera/kinetics/ReactionData.h @@ -68,7 +68,7 @@ public: //! Vector of rate coefficient parameters vector_fp rateCoeffParameters; - //! Vector of auxillary rate coefficient parameters + //! Vector of auxiliary rate coefficient parameters vector_fp auxRateCoeffParameters; int falloffType; diff --git a/include/cantera/kinetics/ReactionStoichMgr.h b/include/cantera/kinetics/ReactionStoichMgr.h index b1f782f87..0d6d11c43 100644 --- a/include/cantera/kinetics/ReactionStoichMgr.h +++ b/include/cantera/kinetics/ReactionStoichMgr.h @@ -188,7 +188,7 @@ public: * only computes 'dg' for the reversible reactions, and the * entries of 'dg' for the irreversible reactions are * unaltered. This is primarily designed for use in - * calculating reveerse rate coefficients from thermochemistry + * calculating reverse rate coefficients from thermochemistry * for reversible reactions. */ virtual void getRevReactionDelta(size_t nr, const doublereal* g, doublereal* dg); diff --git a/include/cantera/numerics/NonlinearSolver.h b/include/cantera/numerics/NonlinearSolver.h index 911d05581..fc3234905 100644 --- a/include/cantera/numerics/NonlinearSolver.h +++ b/include/cantera/numerics/NonlinearSolver.h @@ -557,7 +557,7 @@ public: * effect of ensuring that all delta variables will have the same order of magnitude at convergence * end. * - * The second way is the explicity set the column factors in the second argument of this function call. + * The second way is the explicitly set the column factors in the second argument of this function call. * * The final way to input the scales is to override the ResidJacEval member function call, * diff --git a/include/cantera/thermo/IdealGasPhase.h b/include/cantera/thermo/IdealGasPhase.h index 00af64dc2..4a2b7d160 100644 --- a/include/cantera/thermo/IdealGasPhase.h +++ b/include/cantera/thermo/IdealGasPhase.h @@ -917,7 +917,7 @@ protected: //! Number of Elements in the phase /*! - * This member is defined here, from a call to the Elements ojbect, for speed. + * This member is defined here, from a call to the Elements object, for speed. */ size_t m_mm; diff --git a/include/cantera/thermo/IdealSolidSolnPhase.h b/include/cantera/thermo/IdealSolidSolnPhase.h index 50e8d23fa..8d73b84ed 100644 --- a/include/cantera/thermo/IdealSolidSolnPhase.h +++ b/include/cantera/thermo/IdealSolidSolnPhase.h @@ -424,7 +424,7 @@ public: * concentration divided by the standard concentration is also * equal to the activity of species. * - * For this implentation the activity is defined to be the + * For this implementation the activity is defined to be the * mole fraction of the species. The generalized concentration * is defined to be equal to the mole fraction divided by * the partial molar volume. The generalized concentrations diff --git a/include/cantera/thermo/LatticePhase.h b/include/cantera/thermo/LatticePhase.h index 36918be3c..f2e7f206f 100644 --- a/include/cantera/thermo/LatticePhase.h +++ b/include/cantera/thermo/LatticePhase.h @@ -974,7 +974,7 @@ protected: mutable vector_fp m_s0_R; - //! String name for the species which represents a vacency + //! String name for the species which represents a vacancy //! in the lattice /*! * This string is currently unused diff --git a/include/cantera/thermo/LatticeSolidPhase.h b/include/cantera/thermo/LatticeSolidPhase.h index a9caed11c..754046bc3 100644 --- a/include/cantera/thermo/LatticeSolidPhase.h +++ b/include/cantera/thermo/LatticeSolidPhase.h @@ -638,7 +638,7 @@ public: /*! * * @param n Integer value of the lattice whose mole fractions are being set - * @param x string comtaining Name:value pairs that will specify the mole fractions + * @param x string containing Name:value pairs that will specify the mole fractions * of species on a particular lattice */ void setLatticeMoleFractionsByName(int n, std::string x); @@ -648,7 +648,7 @@ public: /*! * This routine returns the calculation manager for the sublattice * - * @param k Speices id. The default is -1, meaning return the default + * @param k Species id. The default is -1, meaning return the default * * @internal */ diff --git a/include/cantera/thermo/RedlichKwongMFTP.h b/include/cantera/thermo/RedlichKwongMFTP.h index 445fb4c51..bcf77edf3 100644 --- a/include/cantera/thermo/RedlichKwongMFTP.h +++ b/include/cantera/thermo/RedlichKwongMFTP.h @@ -642,7 +642,7 @@ public: * * * @return We return the density of the fluid at the requested phase. If we have not found any - * acceptable density we return a -1. If we have found an accectable density at a + * acceptable density we return a -1. If we have found an acceptable density at a * different phase, we return a -2. */ virtual doublereal densityCalc(doublereal TKelvin, doublereal pressure, int phase, doublereal rhoguess); @@ -743,7 +743,7 @@ protected: //! boolean indicating whether standard mixing rules are applied /*! * - 1 = Yes, there are standard cross terms in the a coefficient matrices. - * - 0 = No, there are nonstaandard cross terms in the a coefficient matrices. + * - 0 = No, there are nonstandard cross terms in the a coefficient matrices. */ int m_standardMixingRules; diff --git a/include/cantera/thermo/ThermoPhase.h b/include/cantera/thermo/ThermoPhase.h index 2dce1fb11..464e0cb33 100644 --- a/include/cantera/thermo/ThermoPhase.h +++ b/include/cantera/thermo/ThermoPhase.h @@ -1355,7 +1355,7 @@ public: //! for species reference-state thermodynamic properties /*! * - * @param k Speices id. The default is -1, meaning return the default + * @param k Species id. The default is -1, meaning return the default * * @internal */ diff --git a/include/cantera/transport/LiquidTransport.h b/include/cantera/transport/LiquidTransport.h index e43b50442..7fe6a2453 100644 --- a/include/cantera/transport/LiquidTransport.h +++ b/include/cantera/transport/LiquidTransport.h @@ -323,7 +323,7 @@ public: //! Return the thermal diffusion coefficients /*! - * These are all zero for this simple implementaion + * These are all zero for this simple implementation * * @param dt thermal diffusion coefficients */ @@ -334,7 +334,7 @@ public: * The thermal conductivity calculation is handled by subclasses of * LiquidTranInteraction as specified in the input file. * These in turn employ subclasses of LTPspecies to - * determine the individual species thermal condictivities. + * determine the individual species thermal conductivities. */ virtual doublereal thermalConductivity(); diff --git a/include/cantera/transport/SimpleTransport.h b/include/cantera/transport/SimpleTransport.h index 971782541..eb2012af7 100644 --- a/include/cantera/transport/SimpleTransport.h +++ b/include/cantera/transport/SimpleTransport.h @@ -317,7 +317,7 @@ public: //! Return the thermal diffusion coefficients /*! - * These are all zero for this simple implementaion + * These are all zero for this simple implementation * * @param dt thermal diffusion coefficients */ diff --git a/src/apps/csvdiff.cpp b/src/apps/csvdiff.cpp index 3d9edd3a9..b086cbcf8 100644 --- a/src/apps/csvdiff.cpp +++ b/src/apps/csvdiff.cpp @@ -189,8 +189,7 @@ static double calc_rdiff(double d1, double d2, double rtol, double atol) * characters. * * Argument: - * str => original string. On exit, this string will have beent - * altered. + * str => original string. On exit, this string will have been altered. * strlets -> Vector of pointers to char *. The vector has a size * larger than or equal to maxPieces. * maxPieces -> largest number of pieces to divide the string into. @@ -243,7 +242,7 @@ static int breakStrCommas(char* str, char** strlets, int maxPieces) * nTitleLines = Number of title lines * nColTitleLines = Number of column title lines * nCol = Number of columns -> basically equal to the - * number of variabless + * number of variables * nDataRows = Number of rows of data in the file * */ diff --git a/src/base/ctml.cpp b/src/base/ctml.cpp index e16232193..d234d8b7a 100644 --- a/src/base/ctml.cpp +++ b/src/base/ctml.cpp @@ -307,7 +307,7 @@ XML_Node* getByTitle(const Cantera::XML_Node& node, const std::string& title) * Code snippet: * @verbatim const XML_Node &parent; - string name = "vacency_species"; + string name = "vacancy_species"; string valueString = getChildValue(parent, name std::string typeString); @endverbatim @@ -317,9 +317,9 @@ XML_Node* getByTitle(const Cantera::XML_Node& node, const std::string& title) * from the following the snippet in the XML file: * * @verbatim - + O(V) - <\vancencySpecies> + <\vacancySpecies> @endverbatim * * @param parent parent reference to the XML_Node object of the parent XML element @@ -579,7 +579,7 @@ doublereal getFloatCurrent(const Cantera::XML_Node& node, +vmax+".\n"); } } - // Note, most type's of converters default to toSI() type atm. + // Note, most types of converters default to toSI() type atm. // This may change and become more specific in the future. if (type == "actEnergy" && units != "") { fctr = actEnergyToSI(units); @@ -595,7 +595,7 @@ doublereal getFloatCurrent(const Cantera::XML_Node& node, fctr = toSI(units); #ifdef DEBUG_MODE writelog("\nWarning: conversion toSI() was done on node value " + node.name() + - "but wasn't explicity requested. Type was \"" + type + "\"\n"); + "but wasn't explicitly requested. Type was \"" + type + "\"\n"); #endif } // Note, below currently produces a lot of output due to transport blocks. @@ -911,7 +911,7 @@ size_t getFloatArray(const Cantera::XML_Node& node, std::vector & v, * item in the value text. This was allowed in * previous versions of Cantera, even though it * would appear to be odd. So, we keep the - * possibilty in for backwards compatibility. + * possibility in for backwards compatibility. */ if (!val.empty()) { dtmp = atofCheck(val.c_str()); @@ -978,7 +978,7 @@ void getMap(const Cantera::XML_Node& node, std::map& m // This function interprets the value portion of an XML element // as a series of "Pairs" separated by white space. /* - * Each pair consists of nonwhite-space characters. + * Each pair consists of non-whitespace characters. * The first ":" found in the pair string is used to separate * the string into two parts. The first part is called the "key" * The second part is called the "val". @@ -1029,7 +1029,7 @@ int getPairs(const Cantera::XML_Node& node, std::vector& key, // This function interprets the value portion of an XML element // as a series of "Matrix ids and entries" separated by white space. /* - * Each pair consists of nonwhite-space characters. + * Each pair consists of non-whitespace characters. * The first two ":" found in the pair string is used to separate * the string into three parts. The first part is called the first * key. The second part is the second key. Both parts must match @@ -1060,7 +1060,7 @@ int getPairs(const Cantera::XML_Node& node, std::vector& key, * @param keyStringCol Key string for the column entries * @param returnValues Return Matrix. * @param convert If this is true, and if the node has a units - * attribute, then conversion to si units is carried + * attribute, then conversion to SI units is carried * out. Default is true. * @param matrixSymmetric If true entries are made so that the matrix * is always symmetric. Default is false. diff --git a/src/equil/BasisOptimize.cpp b/src/equil/BasisOptimize.cpp index 68f288283..5c1662133 100644 --- a/src/equil/BasisOptimize.cpp +++ b/src/equil/BasisOptimize.cpp @@ -388,7 +388,7 @@ L_END_LOOP: * 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 + * Then, the first row in sm[], below will be identically * zero. bleh. * What needs to be done is to perform a rearrangement * of the ELEMENTS -> i.e. rearrange, FormulaMatrix, sp, and gai, such @@ -397,7 +397,7 @@ L_END_LOOP: * 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. + * of Gauss-Jordan 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 @@ -420,7 +420,7 @@ L_END_LOOP: } } /* - * Use Gauss-Jordon block elimination to calculate + * Use Gauss-Jordan block elimination to calculate * the reaction matrix */ int ierr = mlequ(DATA_PTR(sm), ne, nComponents, DATA_PTR(formRxnMatrix), nNonComponents); diff --git a/src/equil/ChemEquil.cpp b/src/equil/ChemEquil.cpp index b9016acbb..f5a5a493b 100644 --- a/src/equil/ChemEquil.cpp +++ b/src/equil/ChemEquil.cpp @@ -1568,7 +1568,7 @@ int ChemEquil::estimateEP_Brinkley(thermo_t& s, vector_fp& x, * its stability properties, i.e., it heads in the right direction, * albeit with lousy convergence rates. * - * NOTE: This probably should be extended to a full blown Gauss-Jordon + * NOTE: This probably should be extended to a full blown Gauss-Jordan * factorization scheme in the future. For Example * the scheme below would fail for the set: HCl NH4Cl, NH3. * Hopefully, it's caught by the equal rows logic below. diff --git a/src/equil/vcs_MultiPhaseEquil.cpp b/src/equil/vcs_MultiPhaseEquil.cpp index e266d84c1..aa9b7bc9e 100644 --- a/src/equil/vcs_MultiPhaseEquil.cpp +++ b/src/equil/vcs_MultiPhaseEquil.cpp @@ -656,7 +656,7 @@ int vcs_MultiPhaseEquil::equilibrate_TP(int estimateEquil, * Transfer the information back to the MultiPhase object. * Note we don't just call setMoles, because some multispecies * solution phases may be zeroed out, and that would cause a problem - * for that routine. Also, the mole fractions of such zereod out + * for that routine. Also, the mole fractions of such zeroed out * phases actually contain information about likely reemergent * states. */ @@ -1586,7 +1586,7 @@ int vcs_MultiPhaseEquil::determine_PhaseStability(int iph, double& funcStab, int * Transfer the information back to the MultiPhase object. * Note we don't just call setMoles, because some multispecies * solution phases may be zeroed out, and that would cause a problem - * for that routine. Also, the mole fractions of such zereod out + * for that routine. Also, the mole fractions of such zeroed out * phases actually contain information about likely reemergent * states. */ diff --git a/src/equil/vcs_elem.cpp b/src/equil/vcs_elem.cpp index 2ea7d84ed..2d8646bc0 100644 --- a/src/equil/vcs_elem.cpp +++ b/src/equil/vcs_elem.cpp @@ -115,7 +115,7 @@ bool VCS_SOLVE::vcs_elabcheck(int ibound) } else { /* * For normal element balances, we require absolute compliance - * even for rediculously small numbers. + * even for ridiculously small numbers. */ if (m_elType[i] == VCS_ELEM_TYPE_ABSPOS) { return false; @@ -168,7 +168,7 @@ int VCS_SOLVE::vcs_elcorr(double aa[], double x[]) * vcs_elcorr: * * This subroutine corrects for element abundances. At the end of the - * surbroutine, the total moles in all phases are recalculated again, + * subroutine, the total moles in all phases are recalculated again, * because we have changed the number of moles in this routine. * * Input diff --git a/src/equil/vcs_phaseStability.cpp b/src/equil/vcs_phaseStability.cpp index 68ee59885..3298f30ca 100644 --- a/src/equil/vcs_phaseStability.cpp +++ b/src/equil/vcs_phaseStability.cpp @@ -192,7 +192,7 @@ int VCS_SOLVE::vcs_phasePopDeterminePossibleList() } /* * This is a vector over each zeroed phase - * For zeroed phases, it lists the components, which are currently zereoed, + * For zeroed phases, it lists the components, which are currently zeroed, * which have a species with a negative stoichiometric value wrt one or more species in the phase. * Cut out components which have a pos stoichiometric value with another species in the phase. */ diff --git a/src/equil/vcs_solve_TP.cpp b/src/equil/vcs_solve_TP.cpp index 4943d4cfe..8dc2432fd 100644 --- a/src/equil/vcs_solve_TP.cpp +++ b/src/equil/vcs_solve_TP.cpp @@ -75,7 +75,7 @@ void VCS_SOLVE::checkDelta1(double* const dsLocal, // Main routine that solves for equilibrium at constant T and P // using a variant of the VCS method /* - * This is the main routine taht solves for equilibrium at constant T and P + * This is the main routine that solves for equilibrium at constant T and P * using a variant of the VCS method. Nonideal phases can be accommodated * as well. * @@ -360,7 +360,7 @@ L_MAINLOOP_ALL_SPECIES: ; if (iti == 0) { /* - * Evaluate the minor non-componenent species chemical + * Evaluate the minor non-component species chemical * potentials and delta G for their formation reactions * We have already evaluated the major non-components */ @@ -811,7 +811,7 @@ L_MAINLOOP_ALL_SPECIES: * 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 + * Note the multiplication 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). @@ -2449,7 +2449,7 @@ void VCS_SOLVE::vcs_reinsert_deleted(size_t kspec) } /****************************************************************************/ -// This routine handles the bookkeepking involved with the +// This routine handles the bookkeeping involved with the // deletion of multiphase phases from the problem. /* * When they are deleted, all of their species become active @@ -2905,7 +2905,7 @@ size_t VCS_SOLVE::vcs_add_all_deleted() * * along the current direction m_deltaMolNumSpecies[], by choosing a value, al: (0 i.e. rearrange, m_formulaMatrix, sp, @@ -3391,7 +3391,7 @@ L_END_LOOP: * 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. + * of Gauss-Jordan 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 @@ -3409,7 +3409,7 @@ L_END_LOOP: } } /* - * Use Gauss-Jordon block elimination to calculate + * Use Gauss-Jordan block elimination to calculate * the reaction matrix, m_stoichCoeffRxnMatrix[][]. */ @@ -3636,11 +3636,11 @@ L_CLEANUP: * * Mole numbers are frequently equal to each other in equilibrium problems * due to constraints. Swaps are only done if there are a 1% difference in the - * mole numbers. Of course this logic isn't fullproof. + * mole numbers. Of course this logic isn't foolproof. * * @param molNum Mole number vector * @param j index into molNum[] that indicates where the search will start from - * Previous successful components are swapped into the fronto of + * Previous successful components are swapped into the front of * molNum[]. * @param n Length of molNum[] */ @@ -4697,8 +4697,8 @@ void VCS_SOLVE::vcs_updateVP(const int vcsState) * Its concentration is currently zero. * - VCS_SPECIES_ZEROEDMS * -3 -> Species lies in a single-species phase which - * is currently zereod out. - * - VCS_SPECIES_ZEREODSS + * is currently zeroed out. + * - VCS_SPECIES_ZEROEDSS * -4 -> Species has such a small mole fraction it is * deleted even though its phase may possibly exist. * The species is believed to have such a small @@ -4709,7 +4709,7 @@ void VCS_SOLVE::vcs_updateVP(const int vcsState) * -5 -> Species refers to an electron in the metal * The unknown is equal to the interfacial voltage * drop across the interface on the SHE (standard - * hydroogen electrode) scale (volts). + * hydrogen electrode) scale (volts). * - VCS_SPECIES_INTERFACIALVOLTAGE * -6 -> Species lies in a multicomponent phase that * is zeroed atm and will stay deleted due to a @@ -4817,7 +4817,7 @@ bool VCS_SOLVE::vcs_evaluate_speciesType() } /*****************************************************************************/ -// Switch rows and columns of a sqare matrix +// Switch rows and columns of a square matrix /* * Switches the row and column of a matrix. * So that after @@ -4825,7 +4825,7 @@ bool VCS_SOLVE::vcs_evaluate_speciesType() * J[k1][j] = J_old[k2][j] and J[j][k1] = J_old[j][k2] * J[k2][j] = J_old[k1][j] and J[j][k2] = J_old[j][k1] * - * @param Jac Double pointer to the jacobiam + * @param Jac Double pointer to the Jacobian * @param k1 first row/column value to be switched * @param k2 second row/column value to be switched */ @@ -4928,7 +4928,7 @@ void VCS_SOLVE::vcs_deltag(const int l, const bool doDeleted, } #endif /* ************************************************* */ - /* **** MAJORS and ZEREOD SPECIES ONLY ************* */ + /* **** MAJORS and ZEROED SPECIES ONLY ************* */ /* ************************************************* */ if (l < 0) { for (irxn = 0; irxn < m_numRxnRdc; ++irxn) { @@ -5221,7 +5221,7 @@ void VCS_SOLVE::vcs_printDeltaG(const int stateCalc) /* * 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 + * However, if the phase is currently zeroed out, a subproblem * is calculated to solve for AC[i] and pseudo-X[i] for that * phase. * diff --git a/src/kinetics/Kinetics.cpp b/src/kinetics/Kinetics.cpp index 851a22cdf..700be60f7 100644 --- a/src/kinetics/Kinetics.cpp +++ b/src/kinetics/Kinetics.cpp @@ -201,7 +201,7 @@ void Kinetics::assignShallowPointers(const std::vector & tpVector) //==================================================================================================================== /** * Takes as input an array of properties for all species in the - * mechanism and copies those values beloning to a particular + * mechanism and copies those values belonging to a particular * phase to the output array. * @param data Input data array. * @param phase Pointer to one of the phase objects participating diff --git a/src/kinetics/KineticsFactory.cpp b/src/kinetics/KineticsFactory.cpp index 7a921f562..4d2755364 100644 --- a/src/kinetics/KineticsFactory.cpp +++ b/src/kinetics/KineticsFactory.cpp @@ -40,7 +40,7 @@ static int _itypes[] = {0, cGasKinetics, cGRI30, cInterfaceKinetics, cEdgeKine * The element has one attribute called "model", * with a string value. The value of this string * is used to decide which kinetics manager is used - * to calculate the reacton mechanism. + * to calculate the reaction mechanism. * * Return * --------- diff --git a/src/kinetics/importKinetics.cpp b/src/kinetics/importKinetics.cpp index 97d5f14a1..2ec6056ed 100644 --- a/src/kinetics/importKinetics.cpp +++ b/src/kinetics/importKinetics.cpp @@ -442,7 +442,7 @@ static void getFalloff(const XML_Node& f, ReactionData& rdata) } else if (np == 3) { rdata.falloffType = TROE3_FALLOFF; } else { - throw CanteraError("getFalloff()", "Troe parameterization is specified by number of pararameters, " + throw CanteraError("getFalloff()", "Troe parameterization is specified by number of parameters, " + int2str(np) + ", is not equal to 3 or 4"); } } else if (type == "SRI") { @@ -460,7 +460,7 @@ static void getFalloff(const XML_Node& f, ReactionData& rdata) throw CanteraError("getFalloff()", "SRI3 m_c parameter is less than zero: " + fp2str(c[2])); } } else { - throw CanteraError("getFalloff()", "SRI parameterization is specified by number of pararameters, " + throw CanteraError("getFalloff()", "SRI parameterization is specified by number of parameters, " + int2str(np) + ", is not equal to 3 or 5"); } } diff --git a/src/numerics/NonlinearSolver.cpp b/src/numerics/NonlinearSolver.cpp index 6060cac98..9a2824a65 100644 --- a/src/numerics/NonlinearSolver.cpp +++ b/src/numerics/NonlinearSolver.cpp @@ -653,7 +653,7 @@ doublereal NonlinearSolver::residErrorNorm(const doublereal* const resid, const * effect of ensuring that all delta variables will have the same order of magnitude at convergence * end. * - * The second way is the explicity set the column factors in the second argument of this function call. + * The second way is the explicitly set the column factors in the second argument of this function call. * * The final way to input the scales is to override the ResidJacEval member function call, * diff --git a/src/oneD/OneDim.cpp b/src/oneD/OneDim.cpp index a87385573..3c034bfda 100644 --- a/src/oneD/OneDim.cpp +++ b/src/oneD/OneDim.cpp @@ -136,7 +136,7 @@ void OneDim::writeStats(int printTime) //============================================================================================================== /** - * Save statistics on function and Jacobiab evaulation, and reset + * Save statistics on function and Jacobian evaluation, and reset * the counters. Statistics are saved only if the number of * Jacobian evaluations is greater than zero. The statistics saved * are diff --git a/src/thermo/DebyeHuckel.cpp b/src/thermo/DebyeHuckel.cpp index c060774c8..59b677737 100644 --- a/src/thermo/DebyeHuckel.cpp +++ b/src/thermo/DebyeHuckel.cpp @@ -1392,7 +1392,7 @@ initThermoXML(XML_Node& phaseNode, std::string id) * Fill in the vector specifying the electrolyte species * type * - * First fill in default values. Everthing is either + * First fill in default values. Everything is either * a charge species, a nonpolar neutral, or the solvent. */ for (size_t k = 0; k < m_kk; k++) { @@ -1845,7 +1845,7 @@ void DebyeHuckel::s_update_lnMolalityActCoeff() const * Debye-Huckel parameter A_Debye * This parameter appears on the top of the activity * coefficient expression. - * It depends on T (and P), as it depends explicity + * It depends on T (and P), as it depends explicitly * on the temperature. Also, the dielectric constant * is usually a fairly strong function of T, also. */ diff --git a/src/thermo/HMWSoln.cpp b/src/thermo/HMWSoln.cpp index 541984549..ea1cb986f 100644 --- a/src/thermo/HMWSoln.cpp +++ b/src/thermo/HMWSoln.cpp @@ -1439,7 +1439,7 @@ doublereal HMWSoln::satPressure(doublereal t) const * * where epsilon = e_rel * e_naught * - * Note, this is si units. Frequently, gaussian units are + * Note, this is SI units. Frequently, gaussian units are * used in Pitzer's papers where D is used, D = epsilon/(4 Pi) * units = A_Debye has units of sqrt(gmol kg-1). */ @@ -1543,7 +1543,7 @@ double HMWSoln::dA_DebyedP_TP(double tempArg, double presArg) const /* - * Calculate the DH Parameter used for the Enthalpy calcalations + * Calculate the DH Parameter used for the Enthalpy calculations * * ADebye_L = 4 R T**2 d(Aphi) / dT * @@ -1565,7 +1565,7 @@ double HMWSoln::ADebye_L(double tempArg, double presArg) const } /* - * Calculate the DH Parameter used for the Volume calcalations + * Calculate the DH Parameter used for the Volume calculations * * ADebye_V = - 4 R T d(Aphi) / dP * diff --git a/src/thermo/HMWSoln_input.cpp b/src/thermo/HMWSoln_input.cpp index 87c080efa..23c86f733 100644 --- a/src/thermo/HMWSoln_input.cpp +++ b/src/thermo/HMWSoln_input.cpp @@ -1473,7 +1473,7 @@ initThermoXML(XML_Node& phaseNode, std::string id) * Fill in the vector specifying the electrolyte species * type * - * First fill in default values. Everthing is either + * First fill in default values. Everything is either * a charge species, a nonpolar neutral, or the solvent. */ for (size_t k = 0; k < m_kk; k++) { diff --git a/src/thermo/IdealSolidSolnPhase.cpp b/src/thermo/IdealSolidSolnPhase.cpp index 15078c83b..a6c652ddc 100644 --- a/src/thermo/IdealSolidSolnPhase.cpp +++ b/src/thermo/IdealSolidSolnPhase.cpp @@ -427,10 +427,10 @@ void IdealSolidSolnPhase::setConcentrations(const doublereal* const c) * concentrations. The generalized concentrations are used * in the evaluation of the rates of progress for reactions * involving species in this phase. The generalized - * concentration dividied by the standard concentration is also + * concentration divided by the standard concentration is also * equal to the activity of species. * - * For this implentation the activity is defined to be the + * For this implementation the activity is defined to be the * mole fraction of the species. The generalized concentration * is defined to be equal to the mole fraction divided by * the partial molar volume. The generalized concentrations @@ -462,7 +462,7 @@ void IdealSolidSolnPhase::setConcentrations(const doublereal* const c) * state into the thermodynamics functions. Therefore the * standard state on which the activities are based depend * on both temperature and pressure. If we hadn't, it would have - * appeared in this function in a very awkwards exp[] format. + * appeared in this function in a very awkward exp[] format. * * @param c[] Pointer to array of doubles of length m_kk, which on exit * will contain the generalized concentrations. @@ -1067,7 +1067,7 @@ const vector_fp& IdealSolidSolnPhase::entropy_R_ref() const /* * initThermo() function initializes the object for use. * - * Before its invokation, the class isn't ready for calculation. + * Before its invocation, the class isn't ready for calculation. */ void IdealSolidSolnPhase::initThermo() { @@ -1203,7 +1203,7 @@ initLengths() /* * Obtain the reference pressure by calling the ThermoPhase - * function refPressure, which in turm calls the + * function refPressure, which in turn calls the * species thermo reference pressure function of the * same name. */ diff --git a/src/thermo/LatticeSolidPhase.cpp b/src/thermo/LatticeSolidPhase.cpp index f951a4be6..6473b767c 100644 --- a/src/thermo/LatticeSolidPhase.cpp +++ b/src/thermo/LatticeSolidPhase.cpp @@ -672,7 +672,7 @@ void LatticeSolidPhase::setParametersFromXML(const XML_Node& eosdata) // for species reference-state thermodynamic properties /* * - * @param k Speices id. The default is -1, meaning return the default + * @param k Species id. The default is -1, meaning return the default * * @internal */ diff --git a/src/thermo/MineralEQ3.cpp b/src/thermo/MineralEQ3.cpp index 794609cd3..09fad0a3e 100644 --- a/src/thermo/MineralEQ3.cpp +++ b/src/thermo/MineralEQ3.cpp @@ -561,7 +561,7 @@ doublereal MineralEQ3::LookupGe(const std::string& elemName) doublereal geValue = entropyElement298(iE); if (geValue == ENTROPY298_UNKNOWN) { throw CanteraError("PDSS_HKFT::LookupGe", - "element " + elemName + " doesn not have a supplied entropy298"); + "element " + elemName + " does not have a supplied entropy298"); } geValue *= (-298.15); return geValue; diff --git a/src/thermo/PDSS_HKFT.cpp b/src/thermo/PDSS_HKFT.cpp index 0166d9cd4..4afcff6f9 100644 --- a/src/thermo/PDSS_HKFT.cpp +++ b/src/thermo/PDSS_HKFT.cpp @@ -598,7 +598,7 @@ void PDSS_HKFT::initThermo() doublereal DHjmol = m_deltaH_formation_tr_pr * 1.0E3 * 4.184; - // If the discrepency is greater than 100 cal gmol-1, print + // If the discrepancy is greater than 100 cal gmol-1, print // an error and exit. if (fabs(Hcalc -DHjmol) > 100.* 1.0E3 * 4.184) { throw CanteraError(" PDSS_HKFT::initThermo()", @@ -1218,7 +1218,7 @@ doublereal PDSS_HKFT::LookupGe(const std::string& elemName) doublereal geValue = m_tp->entropyElement298(iE); if (geValue == ENTROPY298_UNKNOWN) { throw CanteraError("PDSS_HKFT::LookupGe", - "element " + elemName + " doesn not have a supplied entropy298"); + "element " + elemName + " does not have a supplied entropy298"); } geValue *= (-298.15); return geValue; diff --git a/src/thermo/RedlichKwongMFTP.cpp b/src/thermo/RedlichKwongMFTP.cpp index 7434fe0bd..f83c8fa16 100644 --- a/src/thermo/RedlichKwongMFTP.cpp +++ b/src/thermo/RedlichKwongMFTP.cpp @@ -1305,7 +1305,7 @@ doublereal RedlichKwongMFTP::liquidVolEst(doublereal TKelvin, doublereal& presGu * * * @return We return the density of the fluid at the requested phase. If we have not found any - * acceptable density we return a -1. If we have found an accectable density at a + * acceptable density we return a -1. If we have found an acceptable density at a * different phase, we return a -2. */ doublereal RedlichKwongMFTP::densityCalc(doublereal TKelvin, doublereal presPa, int phaseRequested, doublereal rhoguess) diff --git a/src/thermo/SpeciesThermoFactory.cpp b/src/thermo/SpeciesThermoFactory.cpp index 12ddececa..1a3f125a2 100644 --- a/src/thermo/SpeciesThermoFactory.cpp +++ b/src/thermo/SpeciesThermoFactory.cpp @@ -271,7 +271,7 @@ void NasaThermo::checkContinuity(std::string name, double tmid, const doublereal * This is called by method installThermoForSpecies if a NASA block is found in the XML input. * * @param speciesName String name of the species - * @param sp SpeciesThermo object that will receive the nasa polynomial object + * @param sp SpeciesThermo object that will receive the NASA polynomial object * @param k Species index within the phase * @param f0ptr Ptr to the first XML_Node for the first NASA polynomial * @param f1ptr Ptr to the first XML_Node for the first NASA polynomial @@ -366,7 +366,7 @@ static doublereal LookupGe(const std::string& elemName, ThermoPhase* th_ptr) doublereal geValue = th_ptr->entropyElement298(iE); if (geValue == ENTROPY298_UNKNOWN) { throw CanteraError("PDSS_HKFT::LookupGe", - "element " + elemName + " doesn not have a supplied entropy298"); + "element " + elemName + " does not have a supplied entropy298"); } geValue *= (-298.15); return geValue; @@ -408,7 +408,7 @@ static doublereal convertDGFormation(size_t k, ThermoPhase* th_ptr) * * @param speciesName String name of the species * @param th_ptr Pointer to the %ThermoPhase object - * @param sp SpeciesThermo object that will receive the nasa polynomial object + * @param sp SpeciesThermo object that will receive the NASA polynomial object * @param k Species index within the phase * @param MinEQ3node Ptr to the first XML_Node for the first MinEQ3 parameterization */ @@ -441,7 +441,7 @@ static void installMinEQ3asShomateThermoFromXML(std::string speciesName, doublereal Hcalc = Mu0_tr_pr + 298.15 * e; doublereal DHjmol = deltaH_formation_pr_tr * 1.0E3 * 4.184; - // If the discrepency is greater than 100 cal gmol-1, print + // If the discrepancy is greater than 100 cal gmol-1, print // an error and exit. if (fabs(Hcalc -DHjmol) > 10.* 1.0E6 * 4.184) { throw CanteraError("installMinEQ3asShomateThermoFromXML()", @@ -494,7 +494,7 @@ static void installMinEQ3asShomateThermoFromXML(std::string speciesName, * This is called by method installThermoForSpecies if a Shomate block is found in the XML input. * * @param speciesName String name of the species - * @param sp SpeciesThermo object that will receive the nasa polynomial object + * @param sp SpeciesThermo object that will receive the NASA polynomial object * @param k Species index within the phase * @param f0ptr Ptr to the first XML_Node for the first NASA polynomial * @param f1ptr Ptr to the first XML_Node for the first NASA polynomial @@ -561,7 +561,7 @@ static void installShomateThermoFromXML(std::string speciesName, SpeciesThermo& * This is called by method installThermoForSpecies if a SimpleThermo block is found * * @param speciesName String name of the species - * @param sp SpeciesThermo object that will receive the nasa polynomial object + * @param sp SpeciesThermo object that will receive the NASA polynomial object * @param k Species index within the phase * @param f XML_Node for the SimpleThermo block */ @@ -591,7 +591,7 @@ static void installSimpleThermoFromXML(std::string speciesName, * This is called by method installThermoForSpecies if a NASA9 block is found in the XML input. * * @param speciesName String name of the species - * @param sp SpeciesThermo object that will receive the nasa polynomial object + * @param sp SpeciesThermo object that will receive the NASA polynomial object * @param k Species index within the phase * @param tp Vector of XML Nodes that make up the parameterization */ @@ -698,7 +698,7 @@ static void installStatMechThermoFromXML(std::string speciesName, * This is called by method installThermoForSpecies if a Adsorbate block is found in the XML input. * * @param speciesName String name of the species - * @param sp SpeciesThermo object that will receive the nasa polynomial object + * @param sp SpeciesThermo object that will receive the NASA polynomial object * @param k Species index within the phase * @param f XML Node that contains the parameterization */ diff --git a/src/thermo/ThermoPhase.cpp b/src/thermo/ThermoPhase.cpp index c5defa7a3..5426e5b93 100644 --- a/src/thermo/ThermoPhase.cpp +++ b/src/thermo/ThermoPhase.cpp @@ -898,7 +898,7 @@ void ThermoPhase::setSpeciesThermo(SpeciesThermo* spthermo) // for species reference-state thermodynamic properties /* * - * @param k Speices id. The default is -1, meaning return the default + * @param k Species id. The default is -1, meaning return the default * * @internal */ diff --git a/src/thermo/VPSSMgrFactory.cpp b/src/thermo/VPSSMgrFactory.cpp index 7fb206572..d3ff83a6c 100644 --- a/src/thermo/VPSSMgrFactory.cpp +++ b/src/thermo/VPSSMgrFactory.cpp @@ -52,8 +52,8 @@ mutex_t VPSSMgrFactory::vpss_species_thermo_mutex; * * @param spDataNodeList Species Data XML node. This node contains a list * of species XML nodes underneath it. - * @param has_nasa_idealGas Boolean indicating that one species has a nasa ideal gas standard state - * @param has_nasa_constVol Boolean indicating that one species has a nasa ideal solution standard state + * @param has_nasa_idealGas Boolean indicating that one species has a NASA ideal gas standard state + * @param has_nasa_constVol Boolean indicating that one species has a NASA ideal solution standard state * @param has_shomate_idealGas Boolean indicating that one species has a shomate ideal gas standard state * @param has_shomate_constVol Boolean indicating that one species has a shomate ideal solution standard state * @param has_simple_idealGas Boolean indicating that one species has a simple ideal gas standard state diff --git a/src/transport/LiquidTransport.cpp b/src/transport/LiquidTransport.cpp index 15bec42c5..efa7464b7 100644 --- a/src/transport/LiquidTransport.cpp +++ b/src/transport/LiquidTransport.cpp @@ -704,7 +704,7 @@ void LiquidTransport::getSpeciesHydrodynamicRadius(doublereal* const radius) * The thermal conductivity calculation is handled by subclasses of * LiquidTranInteraction as specified in the input file. * These in turn employ subclasses of LTPspecies to - * determine the individual species thermal condictivities. + * determine the individual species thermal conductivities. */ doublereal LiquidTransport::thermalConductivity() { @@ -725,7 +725,7 @@ doublereal LiquidTransport::thermalConductivity() // Return the thermal diffusion coefficients /* - * These are all zero for this simple implementaion + * These are all zero for this simple implementation * * @param dt thermal diffusion coefficients */ @@ -1642,7 +1642,7 @@ void LiquidTransport::stefan_maxwell_solve() * the molar based values. This may change. * * Note, we have broken the symmetry of the matrix here, due to - * consideratins involving species concentrations going to zero. + * considerations involving species concentrations going to zero. * */ for (size_t i = 0; i < m_nsp; i++) { diff --git a/test_problems/VCSnonideal/NaCl_equil/HMW_NaCl.xml b/test_problems/VCSnonideal/NaCl_equil/HMW_NaCl.xml index b8ab726fb..42a499ff3 100644 --- a/test_problems/VCSnonideal/NaCl_equil/HMW_NaCl.xml +++ b/test_problems/VCSnonideal/NaCl_equil/HMW_NaCl.xml @@ -117,11 +117,11 @@ @@ -150,11 +150,11 @@ @@ -207,11 +207,11 @@ diff --git a/test_problems/cathermo/HMW_dupl_test/HMW_NaCl_sp1977_alt.xml b/test_problems/cathermo/HMW_dupl_test/HMW_NaCl_sp1977_alt.xml index df6f5fa23..212af8691 100644 --- a/test_problems/cathermo/HMW_dupl_test/HMW_NaCl_sp1977_alt.xml +++ b/test_problems/cathermo/HMW_dupl_test/HMW_NaCl_sp1977_alt.xml @@ -150,11 +150,11 @@ @@ -207,11 +207,11 @@ diff --git a/test_problems/cathermo/HMW_graph_CpvT/HMW_NaCl_sp1977_alt.xml b/test_problems/cathermo/HMW_graph_CpvT/HMW_NaCl_sp1977_alt.xml index df6f5fa23..212af8691 100644 --- a/test_problems/cathermo/HMW_graph_CpvT/HMW_NaCl_sp1977_alt.xml +++ b/test_problems/cathermo/HMW_graph_CpvT/HMW_NaCl_sp1977_alt.xml @@ -150,11 +150,11 @@ @@ -207,11 +207,11 @@ diff --git a/test_problems/cathermo/HMW_graph_GvI/HMW_NaCl.xml b/test_problems/cathermo/HMW_graph_GvI/HMW_NaCl.xml index d6a66e35c..e62868aa3 100644 --- a/test_problems/cathermo/HMW_graph_GvI/HMW_NaCl.xml +++ b/test_problems/cathermo/HMW_graph_GvI/HMW_NaCl.xml @@ -117,11 +117,11 @@ @@ -150,11 +150,11 @@ @@ -207,11 +207,11 @@ diff --git a/test_problems/cathermo/HMW_graph_GvT/HMW_NaCl_sp1977_alt.xml b/test_problems/cathermo/HMW_graph_GvT/HMW_NaCl_sp1977_alt.xml index df6f5fa23..212af8691 100644 --- a/test_problems/cathermo/HMW_graph_GvT/HMW_NaCl_sp1977_alt.xml +++ b/test_problems/cathermo/HMW_graph_GvT/HMW_NaCl_sp1977_alt.xml @@ -150,11 +150,11 @@ @@ -207,11 +207,11 @@ diff --git a/test_problems/cathermo/HMW_graph_HvT/HMW_NaCl_sp1977_alt.xml b/test_problems/cathermo/HMW_graph_HvT/HMW_NaCl_sp1977_alt.xml index df6f5fa23..212af8691 100644 --- a/test_problems/cathermo/HMW_graph_HvT/HMW_NaCl_sp1977_alt.xml +++ b/test_problems/cathermo/HMW_graph_HvT/HMW_NaCl_sp1977_alt.xml @@ -150,11 +150,11 @@ @@ -207,11 +207,11 @@ diff --git a/test_problems/cathermo/HMW_graph_VvT/HMW_NaCl_sp1977_alt.xml b/test_problems/cathermo/HMW_graph_VvT/HMW_NaCl_sp1977_alt.xml index df6f5fa23..212af8691 100644 --- a/test_problems/cathermo/HMW_graph_VvT/HMW_NaCl_sp1977_alt.xml +++ b/test_problems/cathermo/HMW_graph_VvT/HMW_NaCl_sp1977_alt.xml @@ -150,11 +150,11 @@ @@ -207,11 +207,11 @@