Detailed Description
The mother of all state classes.
This class provides the basic properties based on interrelations of the properties, their derivatives and the Helmholtz energy terms. It does not provide the mechanism to update the values. This has to be implemented in a subclass. Most functions are defined as virtual functions allowing us redefine them later, for example to implement the TTSE technique. The functions defined here are always used as a fall-back.
This base class does not perform any checks on the two-phase conditions and alike. Most of the functions defined here only apply to compressible single state substances. Make sure you are aware of all the assumptions we made when using this class.
Add build table function to Abstract State Interpolator inherit AS implemented by TTSE BICUBIC
Definition at line 78 of file AbstractState.h.
#include <AbstractState.h>
Public Member Functions | |
| AbstractState () | |
| virtual | ~AbstractState () |
| void | set_T (CoolPropDbl T) |
| Set the internal variable T without a flash call (expert use only!) More... | |
| virtual std::string | backend_name (void)=0 |
| virtual bool | using_mole_fractions (void)=0 |
| virtual bool | using_mass_fractions (void)=0 |
| virtual bool | using_volu_fractions (void)=0 |
| virtual void | set_mole_fractions (const std::vector< CoolPropDbl > &mole_fractions)=0 |
| virtual void | set_mass_fractions (const std::vector< CoolPropDbl > &mass_fractions)=0 |
| virtual void | set_volu_fractions (const std::vector< CoolPropDbl > &mass_fractions) |
| virtual void | set_reference_stateS (const std::string &reference_state) |
| Set the reference state based on a string representation. More... | |
| virtual void | set_reference_stateD (double T, double rhomolar, double hmolar0, double smolar0) |
| std::vector< CoolPropDbl > | mole_fractions_liquid (void) |
| Get the mole fractions of the equilibrium liquid phase. More... | |
| std::vector< double > | mole_fractions_liquid_double (void) |
| Get the mole fractions of the equilibrium liquid phase (but as a double for use in SWIG wrapper) More... | |
| std::vector< CoolPropDbl > | mole_fractions_vapor (void) |
| Get the mole fractions of the equilibrium vapor phase. More... | |
| std::vector< double > | mole_fractions_vapor_double (void) |
| Get the mole fractions of the equilibrium vapor phase (but as a double for use in SWIG wrapper) More... | |
| virtual const std::vector< CoolPropDbl > & | get_mole_fractions (void)=0 |
| Get the mole fractions of the fluid. More... | |
| virtual const std::vector< CoolPropDbl > | get_mass_fractions (void) |
| Get the mass fractions of the fluid. More... | |
| virtual void | update (CoolProp::input_pairs input_pair, double Value1, double Value2)=0 |
| Update the state using two state variables. More... | |
| virtual void | update_with_guesses (CoolProp::input_pairs input_pair, double Value1, double Value2, const GuessesStructure &guesses) |
| virtual bool | available_in_high_level (void) |
| virtual std::string | fluid_param_string (const std::string &) |
| Return a string from the backend for the mixture/fluid - backend dependent - could be CAS #, name, etc. More... | |
| std::vector< std::string > | fluid_names (void) |
| Return a vector of strings of the fluid names that are in use. More... | |
| virtual const double | get_fluid_constant (std::size_t i, parameters param) const |
| virtual void | set_binary_interaction_double (const std::string &CAS1, const std::string &CAS2, const std::string ¶meter, const double value) |
| Set binary mixture floating point parameter (EXPERT USE ONLY!!!) More... | |
| virtual void | set_binary_interaction_double (const std::size_t i, const std::size_t j, const std::string ¶meter, const double value) |
| Set binary mixture floating point parameter (EXPERT USE ONLY!!!) More... | |
| virtual void | set_binary_interaction_string (const std::string &CAS1, const std::string &CAS2, const std::string ¶meter, const std::string &value) |
| Set binary mixture string parameter (EXPERT USE ONLY!!!) More... | |
| virtual void | set_binary_interaction_string (const std::size_t i, const std::size_t j, const std::string ¶meter, const std::string &value) |
| Set binary mixture string parameter (EXPERT USE ONLY!!!) More... | |
| virtual double | get_binary_interaction_double (const std::string &CAS1, const std::string &CAS2, const std::string ¶meter) |
| Get binary mixture double value (EXPERT USE ONLY!!!) More... | |
| virtual double | get_binary_interaction_double (const std::size_t i, const std::size_t j, const std::string ¶meter) |
| Get binary mixture double value (EXPERT USE ONLY!!!) More... | |
| virtual std::string | get_binary_interaction_string (const std::string &CAS1, const std::string &CAS2, const std::string ¶meter) |
| Get binary mixture string value (EXPERT USE ONLY!!!) More... | |
| virtual void | apply_simple_mixing_rule (std::size_t i, std::size_t j, const std::string &model) |
| Apply a simple mixing rule (EXPERT USE ONLY!!!) More... | |
| virtual void | set_cubic_alpha_C (const size_t i, const std::string ¶meter, const double c1, const double c2, const double c3) |
| Set the cubic alpha function's constants: More... | |
| virtual void | set_fluid_parameter_double (const size_t i, const std::string ¶meter, const double value) |
| Set fluid parameter (currently the volume translation parameter for cubic) More... | |
| virtual double | get_fluid_parameter_double (const size_t i, const std::string ¶meter) |
| Double fluid parameter (currently the volume translation parameter for cubic) More... | |
| virtual bool | clear () |
| Clear all the cached values. More... | |
| virtual bool | clear_comp_change () |
| When the composition changes, clear all cached values that are only dependent on composition, but not the thermodynamic state. More... | |
| virtual const CoolProp::SimpleState & | get_reducing_state () |
| const CoolProp::SimpleState & | get_state (const std::string &state) |
| Get a desired state point - backend dependent. More... | |
| double | Tmin (void) |
| Get the minimum temperature in K. More... | |
| double | Tmax (void) |
| Get the maximum temperature in K. More... | |
| double | pmax (void) |
| Get the maximum pressure in Pa. More... | |
| double | Ttriple (void) |
| Get the triple point temperature in K. More... | |
| phases | phase (void) |
| Get the phase of the state. More... | |
| void | specify_phase (phases phase) |
| Specify the phase for all further calculations with this state class. More... | |
| void | unspecify_phase (void) |
| Unspecify the phase and go back to calculating it based on the inputs. More... | |
| double | T_critical (void) |
| Return the critical temperature in K. More... | |
| double | p_critical (void) |
| Return the critical pressure in Pa. More... | |
| double | rhomolar_critical (void) |
| Return the critical molar density in mol/m^3. More... | |
| double | rhomass_critical (void) |
| Return the critical mass density in kg/m^3. More... | |
| std::vector< CriticalState > | all_critical_points (void) |
| Return the vector of critical points, including points that are unstable or correspond to negative pressure. More... | |
| void | build_spinodal () |
| Construct the spinodal curve for the mixture (or pure fluid) More... | |
| SpinodalData | get_spinodal_data () |
| Get the data from the spinodal curve constructed in the call to build_spinodal() More... | |
| void | criticality_contour_values (double &L1star, double &M1star) |
| Calculate the criticality contour values \(\mathcal{L}_1^*\) and \(\mathcal{M}_1^*\). More... | |
| double | tangent_plane_distance (const double T, const double p, const std::vector< double > &w, const double rhomolar_guess=-1) |
| double | T_reducing (void) |
| Return the reducing point temperature in K. More... | |
| double | rhomolar_reducing (void) |
| Return the molar density at the reducing point in mol/m^3. More... | |
| double | rhomass_reducing (void) |
| Return the mass density at the reducing point in kg/m^3. More... | |
| double | p_triple (void) |
| Return the triple point pressure in Pa. More... | |
| std::string | name () |
| Return the name - backend dependent. More... | |
| std::string | description () |
| Return the description - backend dependent. More... | |
| double | dipole_moment () |
| Return the dipole moment in C-m (1 D = 3.33564e-30 C-m) More... | |
| double | keyed_output (parameters key) |
| Retrieve a value by key. More... | |
| double | trivial_keyed_output (parameters key) |
| A trivial keyed output like molar mass that does not depend on the state. More... | |
| double | saturated_liquid_keyed_output (parameters key) |
| Get an output from the saturated liquid state by key. More... | |
| double | saturated_vapor_keyed_output (parameters key) |
| Get an output from the saturated vapor state by key. More... | |
| double | T (void) |
| Return the temperature in K. More... | |
| double | rhomolar (void) |
| Return the molar density in mol/m^3. More... | |
| double | rhomass (void) |
| Return the mass density in kg/m^3. More... | |
| double | p (void) |
| Return the pressure in Pa. More... | |
| double | Q (void) |
| Return the vapor quality (mol/mol); Q = 0 for saturated liquid. More... | |
| double | tau (void) |
| Return the reciprocal of the reduced temperature ( \(\tau = T_c/T\)) More... | |
| double | delta (void) |
| Return the reduced density ( \(\delta = \rho/\rho_c\)) More... | |
| double | molar_mass (void) |
| Return the molar mass in kg/mol. More... | |
| double | acentric_factor (void) |
| Return the acentric factor. More... | |
| double | gas_constant (void) |
| Return the mole-fraction weighted gas constant in J/mol/K. More... | |
| double | Bvirial (void) |
| Return the B virial coefficient. More... | |
| double | dBvirial_dT (void) |
| Return the derivative of the B virial coefficient with respect to temperature. More... | |
| double | Cvirial (void) |
| Return the C virial coefficient. More... | |
| double | dCvirial_dT (void) |
| Return the derivative of the C virial coefficient with respect to temperature. More... | |
| double | compressibility_factor (void) |
| Return the compressibility factor \( Z = p/(rho R T) \). More... | |
| double | hmolar (void) |
| Return the molar enthalpy in J/mol. More... | |
| double | hmolar_residual (void) |
| Return the residual molar enthalpy in J/mol. More... | |
| double | hmass (void) |
| Return the mass enthalpy in J/kg. More... | |
| double | hmolar_excess (void) |
| Return the excess molar enthalpy in J/mol. More... | |
| double | hmass_excess (void) |
| Return the excess mass enthalpy in J/kg. More... | |
| double | smolar (void) |
| Return the molar entropy in J/mol/K. More... | |
| double | smolar_residual (void) |
| Return the residual molar entropy (as a function of temperature and density) in J/mol/K. More... | |
| double | smass (void) |
| Return the molar entropy in J/kg/K. More... | |
| double | smolar_excess (void) |
| Return the molar entropy in J/mol/K. More... | |
| double | smass_excess (void) |
| Return the molar entropy in J/kg/K. More... | |
| double | umolar (void) |
| Return the molar internal energy in J/mol. More... | |
| double | umass (void) |
| Return the mass internal energy in J/kg. More... | |
| double | umolar_excess (void) |
| Return the excess internal energy in J/mol. More... | |
| double | umass_excess (void) |
| Return the excess internal energy in J/kg. More... | |
| double | cpmolar (void) |
| Return the molar constant pressure specific heat in J/mol/K. More... | |
| double | cpmass (void) |
| Return the mass constant pressure specific heat in J/kg/K. More... | |
| double | cp0molar (void) |
| Return the molar constant pressure specific heat for ideal gas part only in J/mol/K. More... | |
| double | cp0mass (void) |
| Return the mass constant pressure specific heat for ideal gas part only in J/kg/K. More... | |
| double | cvmolar (void) |
| Return the molar constant volume specific heat in J/mol/K. More... | |
| double | cvmass (void) |
| Return the mass constant volume specific heat in J/kg/K. More... | |
| double | gibbsmolar (void) |
| Return the Gibbs energy in J/mol. More... | |
| double | gibbsmolar_residual (void) |
| Return the residual Gibbs energy in J/mol. More... | |
| double | gibbsmass (void) |
| Return the Gibbs energy in J/kg. More... | |
| double | gibbsmolar_excess (void) |
| Return the excess Gibbs energy in J/mol. More... | |
| double | gibbsmass_excess (void) |
| Return the excess Gibbs energy in J/kg. More... | |
| double | helmholtzmolar (void) |
| Return the Helmholtz energy in J/mol. More... | |
| double | helmholtzmass (void) |
| Return the Helmholtz energy in J/kg. More... | |
| double | helmholtzmolar_excess (void) |
| Return the excess Helmholtz energy in J/mol. More... | |
| double | helmholtzmass_excess (void) |
| Return the excess Helmholtz energy in J/kg. More... | |
| double | volumemolar_excess (void) |
| Return the excess volume in m^3/mol. More... | |
| double | volumemass_excess (void) |
| Return the excess volume in m^3/kg. More... | |
| double | speed_sound (void) |
| Return the speed of sound in m/s. More... | |
| double | isothermal_compressibility (void) |
| Return the isothermal compressibility \( \kappa = -\frac{1}{v}\left.\frac{\partial v}{\partial p}\right|_T=\frac{1}{\rho}\left.\frac{\partial \rho}{\partial p}\right|_T\) in 1/Pa. More... | |
| double | isobaric_expansion_coefficient (void) |
| Return the isobaric expansion coefficient \( \beta = \frac{1}{v}\left.\frac{\partial v}{\partial T}\right|_p = -\frac{1}{\rho}\left.\frac{\partial \rho}{\partial T}\right|_p\) in 1/K. More... | |
| double | isentropic_expansion_coefficient (void) |
| Return the isentropic expansion coefficient \( \kappa_s = -\frac{c_p}{c_v}\frac{v}{p}\left.\frac{\partial p}{\partial v}\right|_T = \frac{\rho}{p}\left.\frac{\partial p}{\partial \rho}\right|_s\). More... | |
| double | fugacity_coefficient (std::size_t i) |
| Return the fugacity coefficient of the i-th component of the mixture. More... | |
| std::vector< double > | fugacity_coefficients () |
| Return a vector of the fugacity coefficients for all components in the mixture. More... | |
| double | fugacity (std::size_t i) |
| Return the fugacity of the i-th component of the mixture. More... | |
| double | chemical_potential (std::size_t i) |
| Return the chemical potential of the i-th component of the mixture. More... | |
| double | fundamental_derivative_of_gas_dynamics (void) |
| Return the fundamental derivative of gas dynamics \( \Gamma \). More... | |
| double | PIP () |
| Return the phase identification parameter (PIP) of G. Venkatarathnam and L.R. Oellrich, "Identification of the phase of a fluid using partial derivatives of pressure, volume, and temperature without reference to saturation properties: Applications in phase equilibria calculations". More... | |
| void | true_critical_point (double &T, double &rho) |
| Calculate the "true" critical point for pure fluids where dpdrho|T and d2p/drho2|T are equal to zero. More... | |
| void | ideal_curve (const std::string &type, std::vector< double > &T, std::vector< double > &p) |
| Calculate an ideal curve for a pure fluid. More... | |
| CoolPropDbl | first_partial_deriv (parameters Of, parameters Wrt, parameters Constant) |
| The first partial derivative in homogeneous phases. More... | |
| CoolPropDbl | second_partial_deriv (parameters Of1, parameters Wrt1, parameters Constant1, parameters Wrt2, parameters Constant2) |
| The second partial derivative in homogeneous phases. More... | |
| CoolPropDbl | first_saturation_deriv (parameters Of1, parameters Wrt1) |
| The first partial derivative along the saturation curve. More... | |
| CoolPropDbl | second_saturation_deriv (parameters Of1, parameters Wrt1, parameters Wrt2) |
| The second partial derivative along the saturation curve. More... | |
| double | first_two_phase_deriv (parameters Of, parameters Wrt, parameters Constant) |
| Calculate the first "two-phase" derivative as described by Thorade and Sadaat, EAS, 2013. More... | |
| double | second_two_phase_deriv (parameters Of, parameters Wrt1, parameters Constant1, parameters Wrt2, parameters Constant2) |
| Calculate the second "two-phase" derivative as described by Thorade and Sadaat, EAS, 2013. More... | |
| double | first_two_phase_deriv_splined (parameters Of, parameters Wrt, parameters Constant, double x_end) |
| Calculate the first "two-phase" derivative as described by Thorade and Sadaat, EAS, 2013. More... | |
| void | build_phase_envelope (const std::string &type="") |
| Construct the phase envelope for a mixture. More... | |
| const CoolProp::PhaseEnvelopeData & | get_phase_envelope_data () |
| After having calculated the phase envelope, return the phase envelope data. More... | |
| virtual bool | has_melting_line (void) |
| Return true if the fluid has a melting line - default is false, but can be re-implemented by derived class. More... | |
| double | melting_line (int param, int given, double value) |
| double | saturation_ancillary (parameters param, int Q, parameters given, double value) |
| double | viscosity (void) |
| Return the viscosity in Pa-s. More... | |
| void | viscosity_contributions (CoolPropDbl &dilute, CoolPropDbl &initial_density, CoolPropDbl &residual, CoolPropDbl &critical) |
| Return the viscosity contributions, each in Pa-s. More... | |
| double | conductivity (void) |
| Return the thermal conductivity in W/m/K. More... | |
| void | conductivity_contributions (CoolPropDbl &dilute, CoolPropDbl &initial_density, CoolPropDbl &residual, CoolPropDbl &critical) |
| Return the thermal conductivity contributions, each in W/m/K. More... | |
| double | surface_tension (void) |
| Return the surface tension in N/m. More... | |
| double | Prandtl (void) |
| Return the Prandtl number (dimensionless) More... | |
| void | conformal_state (const std::string &reference_fluid, CoolPropDbl &T, CoolPropDbl &rhomolar) |
| Find the conformal state needed for ECS. More... | |
| void | change_EOS (const std::size_t i, const std::string &EOS_name) |
| Change the equation of state for a given component to a specified EOS. More... | |
| CoolPropDbl | alpha0 (void) |
| Return the term \( \alpha^0 \). More... | |
| CoolPropDbl | dalpha0_dDelta (void) |
| Return the term \( \alpha^0_{\delta} \). More... | |
| CoolPropDbl | dalpha0_dTau (void) |
| Return the term \( \alpha^0_{\tau} \). More... | |
| CoolPropDbl | d2alpha0_dDelta2 (void) |
| Return the term \( \alpha^0_{\delta\delta} \). More... | |
| CoolPropDbl | d2alpha0_dDelta_dTau (void) |
| Return the term \( \alpha^0_{\delta\tau} \). More... | |
| CoolPropDbl | d2alpha0_dTau2 (void) |
| Return the term \( \alpha^0_{\tau\tau} \). More... | |
| CoolPropDbl | d3alpha0_dTau3 (void) |
| Return the term \( \alpha^0_{\tau\tau\tau} \). More... | |
| CoolPropDbl | d3alpha0_dDelta_dTau2 (void) |
| Return the term \( \alpha^0_{\delta\tau\tau} \). More... | |
| CoolPropDbl | d3alpha0_dDelta2_dTau (void) |
| Return the term \( \alpha^0_{\delta\delta\tau} \). More... | |
| CoolPropDbl | d3alpha0_dDelta3 (void) |
| Return the term \( \alpha^0_{\delta\delta\delta} \). More... | |
| CoolPropDbl | alphar (void) |
| Return the term \( \alpha^r \). More... | |
| CoolPropDbl | dalphar_dDelta (void) |
| Return the term \( \alpha^r_{\delta} \). More... | |
| CoolPropDbl | dalphar_dTau (void) |
| Return the term \( \alpha^r_{\tau} \). More... | |
| CoolPropDbl | d2alphar_dDelta2 (void) |
| Return the term \( \alpha^r_{\delta\delta} \). More... | |
| CoolPropDbl | d2alphar_dDelta_dTau (void) |
| Return the term \( \alpha^r_{\delta\tau} \). More... | |
| CoolPropDbl | d2alphar_dTau2 (void) |
| Return the term \( \alpha^r_{\tau\tau} \). More... | |
| CoolPropDbl | d3alphar_dDelta3 (void) |
| Return the term \( \alpha^r_{\delta\delta\delta} \). More... | |
| CoolPropDbl | d3alphar_dDelta2_dTau (void) |
| Return the term \( \alpha^r_{\delta\delta\tau} \). More... | |
| CoolPropDbl | d3alphar_dDelta_dTau2 (void) |
| Return the term \( \alpha^r_{\delta\tau\tau} \). More... | |
| CoolPropDbl | d3alphar_dTau3 (void) |
| Return the term \( \alpha^r_{\tau\tau\tau} \). More... | |
| CoolPropDbl | d4alphar_dDelta4 (void) |
| Return the term \( \alpha^r_{\delta\delta\delta\delta} \). More... | |
| CoolPropDbl | d4alphar_dDelta3_dTau (void) |
| Return the term \( \alpha^r_{\delta\delta\delta\tau} \). More... | |
| CoolPropDbl | d4alphar_dDelta2_dTau2 (void) |
| Return the term \( \alpha^r_{\delta\delta\tau\tau} \). More... | |
| CoolPropDbl | d4alphar_dDelta_dTau3 (void) |
| Return the term \( \alpha^r_{\delta\tau\tau\tau} \). More... | |
| CoolPropDbl | d4alphar_dTau4 (void) |
| Return the term \( \alpha^r_{\tau\tau\tau\tau} \). More... | |
Static Public Member Functions | |
| static AbstractState * | factory (const std::string &backend, const std::string &fluid_names) |
| A factory function to return a pointer to a new-allocated instance of one of the backends. More... | |
| static AbstractState * | factory (const std::string &backend, const std::vector< std::string > &fluid_names) |
| A factory function to return a pointer to a new-allocated instance of one of the backends. More... | |
Protected Member Functions | |
| bool | isSupercriticalPhase (void) |
| bool | isHomogeneousPhase (void) |
| bool | isTwoPhase (void) |
| virtual CoolPropDbl | calc_hmolar (void) |
| Using this backend, calculate the molar enthalpy in J/mol. More... | |
| virtual CoolPropDbl | calc_hmolar_residual (void) |
| Using this backend, calculate the residual molar enthalpy in J/mol. More... | |
| virtual CoolPropDbl | calc_smolar (void) |
| Using this backend, calculate the molar entropy in J/mol/K. More... | |
| virtual CoolPropDbl | calc_smolar_residual (void) |
| Using this backend, calculate the residual molar entropy in J/mol/K. More... | |
| virtual CoolPropDbl | calc_umolar (void) |
| Using this backend, calculate the molar internal energy in J/mol. More... | |
| virtual CoolPropDbl | calc_cpmolar (void) |
| Using this backend, calculate the molar constant-pressure specific heat in J/mol/K. More... | |
| virtual CoolPropDbl | calc_cpmolar_idealgas (void) |
| Using this backend, calculate the ideal gas molar constant-pressure specific heat in J/mol/K. More... | |
| virtual CoolPropDbl | calc_cvmolar (void) |
| Using this backend, calculate the molar constant-volume specific heat in J/mol/K. More... | |
| virtual CoolPropDbl | calc_gibbsmolar (void) |
| Using this backend, calculate the molar Gibbs function in J/mol. More... | |
| virtual CoolPropDbl | calc_gibbsmolar_residual (void) |
| Using this backend, calculate the residual molar Gibbs function in J/mol. More... | |
| virtual CoolPropDbl | calc_helmholtzmolar (void) |
| Using this backend, calculate the molar Helmholtz energy in J/mol. More... | |
| virtual CoolPropDbl | calc_speed_sound (void) |
| Using this backend, calculate the speed of sound in m/s. More... | |
| virtual CoolPropDbl | calc_isothermal_compressibility (void) |
| Using this backend, calculate the isothermal compressibility \( \kappa = -\frac{1}{v}\left.\frac{\partial v}{\partial p}\right|_T=\frac{1}{\rho}\left.\frac{\partial \rho}{\partial p}\right|_T\) in 1/Pa. More... | |
| virtual CoolPropDbl | calc_isobaric_expansion_coefficient (void) |
| Using this backend, calculate the isobaric expansion coefficient \( \beta = \frac{1}{v}\left.\frac{\partial v}{\partial T}\right|_p = -\frac{1}{\rho}\left.\frac{\partial \rho}{\partial T}\right|_p\) in 1/K. More... | |
| virtual CoolPropDbl | calc_isentropic_expansion_coefficient (void) |
| Using this backend, calculate the isentropic expansion coefficient \( \kappa_s = -\frac{c_p}{c_v}\frac{v}{p}\left.\frac{\partial p}{\partial v}\right|_T = \frac{\rho}{p}\left.\frac{\partial p}{\partial \rho}\right|_s\). More... | |
| virtual CoolPropDbl | calc_viscosity (void) |
| Using this backend, calculate the viscosity in Pa-s. More... | |
| virtual CoolPropDbl | calc_conductivity (void) |
| Using this backend, calculate the thermal conductivity in W/m/K. More... | |
| virtual CoolPropDbl | calc_surface_tension (void) |
| Using this backend, calculate the surface tension in N/m. More... | |
| virtual CoolPropDbl | calc_molar_mass (void) |
| Using this backend, calculate the molar mass in kg/mol. More... | |
| virtual CoolPropDbl | calc_acentric_factor (void) |
| Using this backend, calculate the acentric factor. More... | |
| virtual CoolPropDbl | calc_pressure (void) |
| Using this backend, calculate the pressure in Pa. More... | |
| virtual CoolPropDbl | calc_gas_constant (void) |
| Using this backend, calculate the universal gas constant \(R_u\) in J/mol/K. More... | |
| virtual CoolPropDbl | calc_fugacity_coefficient (std::size_t i) |
| Using this backend, calculate the fugacity coefficient (dimensionless) More... | |
| virtual std::vector< CoolPropDbl > | calc_fugacity_coefficients () |
| Using this backend, calculate the fugacity in Pa. More... | |
| virtual CoolPropDbl | calc_fugacity (std::size_t i) |
| Using this backend, calculate the fugacity in Pa. More... | |
| virtual CoolPropDbl | calc_chemical_potential (std::size_t i) |
| Using this backend, calculate the chemical potential in J/mol. More... | |
| virtual CoolPropDbl | calc_PIP (void) |
| Using this backend, calculate the phase identification parameter (PIP) More... | |
| virtual void | calc_excess_properties (void) |
| Using this backend, calculate and cache the excess properties. More... | |
| virtual CoolPropDbl | calc_alphar (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_dalphar_dDelta (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_dalphar_dTau (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d2alphar_dDelta2 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d2alphar_dDelta_dTau (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d2alphar_dTau2 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alphar_dDelta3 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\delta}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alphar_dDelta2_dTau (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alphar_dDelta_dTau2 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alphar_dTau3 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d4alphar_dDelta4 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\delta\delta}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d4alphar_dDelta3_dTau (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\delta\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d4alphar_dDelta2_dTau2 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d4alphar_dDelta_dTau3 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\tau\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d4alphar_dTau4 (void) |
| Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau\tau\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_alpha0 (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_dalpha0_dDelta (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_dalpha0_dTau (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d2alpha0_dDelta_dTau (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\delta}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d2alpha0_dDelta2 (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d2alpha0_dTau2 (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alpha0_dDelta3 (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\delta\delta}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alpha0_dDelta2_dTau (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\delta\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alpha0_dDelta_dTau2 (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\tau\tau}\) (dimensionless) More... | |
| virtual CoolPropDbl | calc_d3alpha0_dTau3 (void) |
| Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\tau\tau\tau}\) (dimensionless) More... | |
| virtual void | calc_reducing_state (void) |
| virtual CoolPropDbl | calc_Tmax (void) |
| Using this backend, calculate the maximum temperature in K. More... | |
| virtual CoolPropDbl | calc_Tmin (void) |
| Using this backend, calculate the minimum temperature in K. More... | |
| virtual CoolPropDbl | calc_pmax (void) |
| Using this backend, calculate the maximum pressure in Pa. More... | |
| virtual CoolPropDbl | calc_GWP20 (void) |
| Using this backend, calculate the 20-year global warming potential (GWP) More... | |
| virtual CoolPropDbl | calc_GWP100 (void) |
| Using this backend, calculate the 100-year global warming potential (GWP) More... | |
| virtual CoolPropDbl | calc_GWP500 (void) |
| Using this backend, calculate the 500-year global warming potential (GWP) More... | |
| virtual CoolPropDbl | calc_ODP (void) |
| Using this backend, calculate the ozone depletion potential (ODP) More... | |
| virtual CoolPropDbl | calc_flame_hazard (void) |
| Using this backend, calculate the flame hazard. More... | |
| virtual CoolPropDbl | calc_health_hazard (void) |
| Using this backend, calculate the health hazard. More... | |
| virtual CoolPropDbl | calc_physical_hazard (void) |
| Using this backend, calculate the physical hazard. More... | |
| virtual CoolPropDbl | calc_dipole_moment (void) |
| Using this backend, calculate the dipole moment in C-m (1 D = 3.33564e-30 C-m) More... | |
| virtual CoolPropDbl | calc_first_partial_deriv (parameters Of, parameters Wrt, parameters Constant) |
| Calculate the first partial derivative for the desired derivative. More... | |
| virtual CoolPropDbl | calc_second_partial_deriv (parameters Of1, parameters Wrt1, parameters Constant1, parameters Wrt2, parameters Constant2) |
| Calculate the second partial derivative using the given backend. More... | |
| virtual CoolPropDbl | calc_reduced_density (void) |
| Using this backend, calculate the reduced density (rho/rhoc) More... | |
| virtual CoolPropDbl | calc_reciprocal_reduced_temperature (void) |
| Using this backend, calculate the reciprocal reduced temperature (Tc/T) More... | |
| virtual CoolPropDbl | calc_Bvirial (void) |
| Using this backend, calculate the second virial coefficient. More... | |
| virtual CoolPropDbl | calc_Cvirial (void) |
| Using this backend, calculate the third virial coefficient. More... | |
| virtual CoolPropDbl | calc_dBvirial_dT (void) |
| Using this backend, calculate the derivative dB/dT. More... | |
| virtual CoolPropDbl | calc_dCvirial_dT (void) |
| Using this backend, calculate the derivative dC/dT. More... | |
| virtual CoolPropDbl | calc_compressibility_factor (void) |
| Using this backend, calculate the compressibility factor Z \( Z = p/(\rho R T) \). More... | |
| virtual std::string | calc_name (void) |
| Using this backend, get the name of the fluid. More... | |
| virtual std::string | calc_description (void) |
| Using this backend, get the description of the fluid. More... | |
| virtual CoolPropDbl | calc_Ttriple (void) |
| Using this backend, get the triple point temperature in K. More... | |
| virtual CoolPropDbl | calc_p_triple (void) |
| Using this backend, get the triple point pressure in Pa. More... | |
| virtual CoolPropDbl | calc_T_critical (void) |
| Using this backend, get the critical point temperature in K. More... | |
| virtual CoolPropDbl | calc_T_reducing (void) |
| Using this backend, get the reducing point temperature in K. More... | |
| virtual CoolPropDbl | calc_p_critical (void) |
| Using this backend, get the critical point pressure in Pa. More... | |
| virtual CoolPropDbl | calc_p_reducing (void) |
| Using this backend, get the reducing point pressure in Pa. More... | |
| virtual CoolPropDbl | calc_rhomolar_critical (void) |
| Using this backend, get the critical point molar density in mol/m^3. More... | |
| virtual CoolPropDbl | calc_rhomass_critical (void) |
| Using this backend, get the critical point mass density in kg/m^3 - Added for IF97Backend which is mass based. More... | |
| virtual CoolPropDbl | calc_rhomolar_reducing (void) |
| Using this backend, get the reducing point molar density in mol/m^3. More... | |
| virtual void | calc_phase_envelope (const std::string &type) |
| Using this backend, construct the phase envelope, the variable type describes the type of phase envelope to be built. More... | |
| virtual CoolPropDbl | calc_rhomass (void) |
| virtual CoolPropDbl | calc_hmass (void) |
| virtual CoolPropDbl | calc_hmass_excess (void) |
| virtual CoolPropDbl | calc_smass (void) |
| virtual CoolPropDbl | calc_smass_excess (void) |
| virtual CoolPropDbl | calc_cpmass (void) |
| virtual CoolPropDbl | calc_cp0mass (void) |
| virtual CoolPropDbl | calc_cvmass (void) |
| virtual CoolPropDbl | calc_umass (void) |
| virtual CoolPropDbl | calc_umass_excess (void) |
| virtual CoolPropDbl | calc_gibbsmass (void) |
| virtual CoolPropDbl | calc_gibbsmass_excess (void) |
| virtual CoolPropDbl | calc_helmholtzmass (void) |
| virtual CoolPropDbl | calc_helmholtzmass_excess (void) |
| virtual CoolPropDbl | calc_volumemass_excess (void) |
| virtual void | update_states (void) |
| Update the states after having changed the reference state for enthalpy and entropy. More... | |
| virtual CoolPropDbl | calc_melting_line (int param, int given, CoolPropDbl value) |
| virtual CoolPropDbl | calc_saturation_ancillary (parameters param, int Q, parameters given, double value) |
| virtual phases | calc_phase (void) |
| Using this backend, calculate the phase. More... | |
| virtual void | calc_specify_phase (phases phase) |
| Using this backend, specify the phase to be used for all further calculations. More... | |
| virtual void | calc_unspecify_phase (void) |
| Using this backend, unspecify the phase. More... | |
| virtual std::vector< std::string > | calc_fluid_names (void) |
| Using this backend, get a vector of fluid names. More... | |
| virtual const CoolProp::SimpleState & | calc_state (const std::string &state) |
| virtual const CoolProp::PhaseEnvelopeData & | calc_phase_envelope_data (void) |
| virtual std::vector< CoolPropDbl > | calc_mole_fractions_liquid (void) |
| virtual std::vector< CoolPropDbl > | calc_mole_fractions_vapor (void) |
| virtual const std::vector< CoolPropDbl > | calc_mass_fractions (void) |
| virtual CoolPropDbl | calc_fraction_min (void) |
| Get the minimum fraction (mole, mass, volume) for incompressible fluid. More... | |
| virtual CoolPropDbl | calc_fraction_max (void) |
| Get the maximum fraction (mole, mass, volume) for incompressible fluid. More... | |
| virtual CoolPropDbl | calc_T_freeze (void) |
| virtual CoolPropDbl | calc_first_saturation_deriv (parameters Of1, parameters Wrt1) |
| virtual CoolPropDbl | calc_second_saturation_deriv (parameters Of1, parameters Wrt1, parameters Wrt2) |
| virtual CoolPropDbl | calc_first_two_phase_deriv (parameters Of, parameters Wrt, parameters Constant) |
| virtual CoolPropDbl | calc_second_two_phase_deriv (parameters Of, parameters Wrt, parameters Constant, parameters Wrt2, parameters Constant2) |
| virtual CoolPropDbl | calc_first_two_phase_deriv_splined (parameters Of, parameters Wrt, parameters Constant, CoolPropDbl x_end) |
| virtual CoolPropDbl | calc_saturated_liquid_keyed_output (parameters key) |
| virtual CoolPropDbl | calc_saturated_vapor_keyed_output (parameters key) |
| virtual void | calc_ideal_curve (const std::string &type, std::vector< double > &T, std::vector< double > &p) |
| virtual CoolPropDbl | calc_T (void) |
| Using this backend, get the temperature. More... | |
| virtual CoolPropDbl | calc_rhomolar (void) |
| Using this backend, get the molar density in mol/m^3. More... | |
| virtual double | calc_tangent_plane_distance (const double T, const double p, const std::vector< double > &w, const double rhomolar_guess) |
| Using this backend, calculate the tangent plane distance for a given trial composition. More... | |
| virtual void | calc_true_critical_point (double &T, double &rho) |
| Using this backend, return true critical point where dp/drho|T = 0 and d2p/drho^2|T = 0. More... | |
| virtual void | calc_conformal_state (const std::string &reference_fluid, CoolPropDbl &T, CoolPropDbl &rhomolar) |
| virtual void | calc_viscosity_contributions (CoolPropDbl &dilute, CoolPropDbl &initial_density, CoolPropDbl &residual, CoolPropDbl &critical) |
| virtual void | calc_conductivity_contributions (CoolPropDbl &dilute, CoolPropDbl &initial_density, CoolPropDbl &residual, CoolPropDbl &critical) |
| virtual std::vector< CriticalState > | calc_all_critical_points (void) |
| virtual void | calc_build_spinodal () |
| virtual SpinodalData | calc_get_spinodal_data () |
| virtual void | calc_criticality_contour_values (double &L1star, double &M1star) |
| virtual void | mass_to_molar_inputs (CoolProp::input_pairs &input_pair, CoolPropDbl &value1, CoolPropDbl &value2) |
| Convert mass-based input pair to molar-based input pair; If molar-based, do nothing. More... | |
| virtual void | calc_change_EOS (const std::size_t i, const std::string &EOS_name) |
| Change the equation of state for a given component to a specified EOS. More... | |
Constructor & Destructor Documentation
◆ AbstractState()
|
inline |
Definition at line 690 of file AbstractState.h.
◆ ~AbstractState()
|
inlinevirtual |
Definition at line 693 of file AbstractState.h.
Member Function Documentation
◆ acentric_factor()
| double CoolProp::AbstractState::acentric_factor | ( | void | ) |
Return the acentric factor.
Definition at line 677 of file AbstractState.cpp.
◆ all_critical_points()
|
inline |
Return the vector of critical points, including points that are unstable or correspond to negative pressure.
Definition at line 960 of file AbstractState.h.
◆ alpha0()
|
inline |
Return the term \( \alpha^0 \).
Definition at line 1455 of file AbstractState.h.
◆ alphar()
|
inline |
Return the term \( \alpha^r \).
Definition at line 1506 of file AbstractState.h.
◆ apply_simple_mixing_rule()
|
inlinevirtual |
Apply a simple mixing rule (EXPERT USE ONLY!!!)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 895 of file AbstractState.h.
◆ available_in_high_level()
|
inlinevirtual |
A function that says whether the backend instance can be instantiated in the high-level interface In general this should be true, except for some other backends (especially the tabular backends) To disable use in high-level interface, implement this function and return false
Reimplemented in CoolProp::TabularBackend.
Definition at line 844 of file AbstractState.h.
◆ backend_name()
|
pure virtual |
Get a string representation of the backend - for instance "HelmholtzEOSMixtureBackend" for the core mixture model in CoolProp
Must be overloaded by the backend to provide the backend's name
Implemented in CoolProp::TTSEBackend, CoolProp::BicubicBackend, CoolProp::REFPROPMixtureBackend, CoolProp::REFPROPBackend, CoolProp::PCSAFTBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, CoolProp::HelmholtzEOSBackend, CoolProp::VTPRBackend, CoolProp::PengRobinsonBackend, and CoolProp::SRKBackend.
◆ build_phase_envelope()
| void CoolProp::AbstractState::build_phase_envelope | ( | const std::string & | type = "" | ) |
Construct the phase envelope for a mixture.
- Parameters
-
type currently a dummy variable that is not used
Definition at line 711 of file AbstractState.cpp.
◆ build_spinodal()
|
inline |
Construct the spinodal curve for the mixture (or pure fluid)
Definition at line 965 of file AbstractState.h.
◆ Bvirial()
| double CoolProp::AbstractState::Bvirial | ( | void | ) |
Return the B virial coefficient.
Definition at line 723 of file AbstractState.cpp.
◆ calc_acentric_factor()
|
inlineprotectedvirtual |
Using this backend, calculate the acentric factor.
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 223 of file AbstractState.h.
◆ calc_all_critical_points()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 668 of file AbstractState.h.
◆ calc_alpha0()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 326 of file AbstractState.h.
◆ calc_alphar()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::PCSAFTBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 263 of file AbstractState.h.
◆ calc_build_spinodal()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 671 of file AbstractState.h.
◆ calc_Bvirial()
|
inlineprotectedvirtual |
Using this backend, calculate the second virial coefficient.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 431 of file AbstractState.h.
◆ calc_change_EOS()
|
inlineprotectedvirtual |
Change the equation of state for a given component to a specified EOS.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 685 of file AbstractState.h.
◆ calc_chemical_potential()
|
inlineprotectedvirtual |
Using this backend, calculate the chemical potential in J/mol.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 247 of file AbstractState.h.
◆ calc_compressibility_factor()
|
inlineprotectedvirtual |
Using this backend, calculate the compressibility factor Z \( Z = p/(\rho R T) \).
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::PCSAFTBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 447 of file AbstractState.h.
◆ calc_conductivity()
|
inlineprotectedvirtual |
Using this backend, calculate the thermal conductivity in W/m/K.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 211 of file AbstractState.h.
◆ calc_conductivity_contributions()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 665 of file AbstractState.h.
◆ calc_conformal_state()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 658 of file AbstractState.h.
◆ calc_cp0mass()
|
inlineprotectedvirtual |
Definition at line 520 of file AbstractState.h.
◆ calc_cpmass()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::IncompressibleBackend, and CoolProp::IF97Backend.
Definition at line 517 of file AbstractState.h.
◆ calc_cpmolar()
|
inlineprotectedvirtual |
Using this backend, calculate the molar constant-pressure specific heat in J/mol/K.
Reimplemented in CoolProp::TabularBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 167 of file AbstractState.h.
◆ calc_cpmolar_idealgas()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal gas molar constant-pressure specific heat in J/mol/K.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 171 of file AbstractState.h.
◆ calc_criticality_contour_values()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 677 of file AbstractState.h.
◆ calc_Cvirial()
|
inlineprotectedvirtual |
Using this backend, calculate the third virial coefficient.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 435 of file AbstractState.h.
◆ calc_cvmass()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::IncompressibleBackend, and CoolProp::IF97Backend.
Definition at line 523 of file AbstractState.h.
◆ calc_cvmolar()
|
inlineprotectedvirtual |
Using this backend, calculate the molar constant-volume specific heat in J/mol/K.
Reimplemented in CoolProp::TabularBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 175 of file AbstractState.h.
◆ calc_d2alpha0_dDelta2()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 342 of file AbstractState.h.
◆ calc_d2alpha0_dDelta_dTau()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\delta}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 338 of file AbstractState.h.
◆ calc_d2alpha0_dTau2()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 346 of file AbstractState.h.
◆ calc_d2alphar_dDelta2()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 275 of file AbstractState.h.
◆ calc_d2alphar_dDelta_dTau()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 279 of file AbstractState.h.
◆ calc_d2alphar_dTau2()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 283 of file AbstractState.h.
◆ calc_d3alpha0_dDelta2_dTau()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\delta\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 354 of file AbstractState.h.
◆ calc_d3alpha0_dDelta3()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\delta\delta}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 350 of file AbstractState.h.
◆ calc_d3alpha0_dDelta_dTau2()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 358 of file AbstractState.h.
◆ calc_d3alpha0_dTau3()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\tau\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 362 of file AbstractState.h.
◆ calc_d3alphar_dDelta2_dTau()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 291 of file AbstractState.h.
◆ calc_d3alphar_dDelta3()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\delta}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 287 of file AbstractState.h.
◆ calc_d3alphar_dDelta_dTau2()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 295 of file AbstractState.h.
◆ calc_d3alphar_dTau3()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 299 of file AbstractState.h.
◆ calc_d4alphar_dDelta2_dTau2()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 312 of file AbstractState.h.
◆ calc_d4alphar_dDelta3_dTau()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\delta\tau}\) (dimensionless)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 308 of file AbstractState.h.
◆ calc_d4alphar_dDelta4()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\delta\delta\delta}\) (dimensionless)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 304 of file AbstractState.h.
◆ calc_d4alphar_dDelta_dTau3()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta\tau\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 316 of file AbstractState.h.
◆ calc_d4alphar_dTau4()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau\tau\tau\tau}\) (dimensionless)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 320 of file AbstractState.h.
◆ calc_dalpha0_dDelta()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\delta}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 330 of file AbstractState.h.
◆ calc_dalpha0_dTau()
|
inlineprotectedvirtual |
Using this backend, calculate the ideal-gas Helmholtz energy term \(\alpha^0_{\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 334 of file AbstractState.h.
◆ calc_dalphar_dDelta()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\delta}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 267 of file AbstractState.h.
◆ calc_dalphar_dTau()
|
inlineprotectedvirtual |
Using this backend, calculate the residual Helmholtz energy term \(\alpha^r_{\tau}\) (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 271 of file AbstractState.h.
◆ calc_dBvirial_dT()
|
inlineprotectedvirtual |
Using this backend, calculate the derivative dB/dT.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 439 of file AbstractState.h.
◆ calc_dCvirial_dT()
|
inlineprotectedvirtual |
Using this backend, calculate the derivative dC/dT.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 443 of file AbstractState.h.
◆ calc_description()
|
inlineprotectedvirtual |
Using this backend, get the description of the fluid.
Reimplemented in CoolProp::IncompressibleBackend.
Definition at line 456 of file AbstractState.h.
◆ calc_dipole_moment()
|
inlineprotectedvirtual |
Using this backend, calculate the dipole moment in C-m (1 D = 3.33564e-30 C-m)
Reimplemented in CoolProp::REFPROPMixtureBackend.
Definition at line 412 of file AbstractState.h.
◆ calc_excess_properties()
|
inlineprotectedvirtual |
Using this backend, calculate and cache the excess properties.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 257 of file AbstractState.h.
◆ calc_first_partial_deriv()
|
protectedvirtual |
Calculate the first partial derivative for the desired derivative.
Reimplemented in CoolProp::TabularBackend, and CoolProp::IncompressibleBackend.
Definition at line 1002 of file AbstractState.cpp.
◆ calc_first_saturation_deriv()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::TabularBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 613 of file AbstractState.h.
◆ calc_first_two_phase_deriv()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::TabularBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 619 of file AbstractState.h.
◆ calc_first_two_phase_deriv_splined()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::TabularBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 625 of file AbstractState.h.
◆ calc_flame_hazard()
|
inlineprotectedvirtual |
Using this backend, calculate the flame hazard.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 400 of file AbstractState.h.
◆ calc_fluid_names()
|
inlineprotectedvirtual |
Using this backend, get a vector of fluid names.
Reimplemented in CoolProp::TabularBackend, CoolProp::HelmholtzEOSMixtureBackend, CoolProp::VTPRBackend, CoolProp::AbstractCubicBackend, and CoolProp::REFPROPMixtureBackend.
Definition at line 578 of file AbstractState.h.
◆ calc_fraction_max()
|
inlineprotectedvirtual |
Get the maximum fraction (mole, mass, volume) for incompressible fluid.
Reimplemented in CoolProp::IncompressibleBackend.
Definition at line 606 of file AbstractState.h.
◆ calc_fraction_min()
|
inlineprotectedvirtual |
Get the minimum fraction (mole, mass, volume) for incompressible fluid.
Reimplemented in CoolProp::IncompressibleBackend.
Definition at line 602 of file AbstractState.h.
◆ calc_fugacity()
|
inlineprotectedvirtual |
Using this backend, calculate the fugacity in Pa.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 243 of file AbstractState.h.
◆ calc_fugacity_coefficient()
|
inlineprotectedvirtual |
Using this backend, calculate the fugacity coefficient (dimensionless)
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::VTPRBackend.
Definition at line 235 of file AbstractState.h.
◆ calc_fugacity_coefficients()
|
inlineprotectedvirtual |
Using this backend, calculate the fugacity in Pa.
Reimplemented in CoolProp::PCSAFTBackend.
Definition at line 239 of file AbstractState.h.
◆ calc_gas_constant()
|
inlineprotectedvirtual |
Using this backend, calculate the universal gas constant \(R_u\) in J/mol/K.
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 231 of file AbstractState.h.
◆ calc_get_spinodal_data()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 674 of file AbstractState.h.
◆ calc_gibbsmass()
|
inlineprotectedvirtual |
Definition at line 532 of file AbstractState.h.
◆ calc_gibbsmass_excess()
|
inlineprotectedvirtual |
Definition at line 535 of file AbstractState.h.
◆ calc_gibbsmolar()
|
inlineprotectedvirtual |
Using this backend, calculate the molar Gibbs function in J/mol.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 179 of file AbstractState.h.
◆ calc_gibbsmolar_residual()
|
inlineprotectedvirtual |
Using this backend, calculate the residual molar Gibbs function in J/mol.
Reimplemented in CoolProp::PCSAFTBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 183 of file AbstractState.h.
◆ calc_GWP100()
|
inlineprotectedvirtual |
Using this backend, calculate the 100-year global warming potential (GWP)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 388 of file AbstractState.h.
◆ calc_GWP20()
|
inlineprotectedvirtual |
Using this backend, calculate the 20-year global warming potential (GWP)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 384 of file AbstractState.h.
◆ calc_GWP500()
|
inlineprotectedvirtual |
Using this backend, calculate the 500-year global warming potential (GWP)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 392 of file AbstractState.h.
◆ calc_health_hazard()
|
inlineprotectedvirtual |
Using this backend, calculate the health hazard.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 404 of file AbstractState.h.
◆ calc_helmholtzmass()
|
inlineprotectedvirtual |
Definition at line 538 of file AbstractState.h.
◆ calc_helmholtzmass_excess()
|
inlineprotectedvirtual |
Definition at line 541 of file AbstractState.h.
◆ calc_helmholtzmolar()
|
inlineprotectedvirtual |
Using this backend, calculate the molar Helmholtz energy in J/mol.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 187 of file AbstractState.h.
◆ calc_hmass()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::IncompressibleBackend, and CoolProp::IF97Backend.
Definition at line 505 of file AbstractState.h.
◆ calc_hmass_excess()
|
inlineprotectedvirtual |
Definition at line 508 of file AbstractState.h.
◆ calc_hmolar()
|
inlineprotectedvirtual |
Using this backend, calculate the molar enthalpy in J/mol.
Reimplemented in CoolProp::TabularBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 147 of file AbstractState.h.
◆ calc_hmolar_residual()
|
inlineprotectedvirtual |
Using this backend, calculate the residual molar enthalpy in J/mol.
Reimplemented in CoolProp::PCSAFTBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 151 of file AbstractState.h.
◆ calc_ideal_curve()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 635 of file AbstractState.h.
◆ calc_isentropic_expansion_coefficient()
|
inlineprotectedvirtual |
Using this backend, calculate the isentropic expansion coefficient \( \kappa_s = -\frac{c_p}{c_v}\frac{v}{p}\left.\frac{\partial p}{\partial v}\right|_T = \frac{\rho}{p}\left.\frac{\partial p}{\partial \rho}\right|_s\).
Definition at line 203 of file AbstractState.h.
◆ calc_isobaric_expansion_coefficient()
|
inlineprotectedvirtual |
Using this backend, calculate the isobaric expansion coefficient \( \beta = \frac{1}{v}\left.\frac{\partial v}{\partial T}\right|_p = -\frac{1}{\rho}\left.\frac{\partial \rho}{\partial T}\right|_p\) in 1/K.
Definition at line 199 of file AbstractState.h.
◆ calc_isothermal_compressibility()
|
inlineprotectedvirtual |
Using this backend, calculate the isothermal compressibility \( \kappa = -\frac{1}{v}\left.\frac{\partial v}{\partial p}\right|_T=\frac{1}{\rho}\left.\frac{\partial \rho}{\partial p}\right|_T\) in 1/Pa.
Definition at line 195 of file AbstractState.h.
◆ calc_mass_fractions()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::TabularBackend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::REFPROPMixtureBackend.
Definition at line 597 of file AbstractState.h.
◆ calc_melting_line()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::IncompressibleBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 553 of file AbstractState.h.
◆ calc_molar_mass()
|
inlineprotectedvirtual |
Using this backend, calculate the molar mass in kg/mol.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::PCSAFTBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, CoolProp::VTPRBackend, and CoolProp::AbstractCubicBackend.
Definition at line 219 of file AbstractState.h.
◆ calc_mole_fractions_liquid()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 591 of file AbstractState.h.
◆ calc_mole_fractions_vapor()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 594 of file AbstractState.h.
◆ calc_name()
|
inlineprotectedvirtual |
Using this backend, get the name of the fluid.
Reimplemented in CoolProp::TabularBackend, CoolProp::IncompressibleBackend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::REFPROPMixtureBackend.
Definition at line 452 of file AbstractState.h.
◆ calc_ODP()
|
inlineprotectedvirtual |
Using this backend, calculate the ozone depletion potential (ODP)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 396 of file AbstractState.h.
◆ calc_p_critical()
|
inlineprotectedvirtual |
Using this backend, get the critical point pressure in Pa.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 478 of file AbstractState.h.
◆ calc_p_reducing()
|
inlineprotectedvirtual |
Using this backend, get the reducing point pressure in Pa.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 482 of file AbstractState.h.
◆ calc_p_triple()
|
inlineprotectedvirtual |
Using this backend, get the triple point pressure in Pa.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 465 of file AbstractState.h.
◆ calc_phase()
|
inlineprotectedvirtual |
Using this backend, calculate the phase.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::PCSAFTBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 566 of file AbstractState.h.
◆ calc_phase_envelope()
|
inlineprotectedvirtual |
Using this backend, construct the phase envelope, the variable type describes the type of phase envelope to be built.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 498 of file AbstractState.h.
◆ calc_phase_envelope_data()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 587 of file AbstractState.h.
◆ calc_physical_hazard()
|
inlineprotectedvirtual |
Using this backend, calculate the physical hazard.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 408 of file AbstractState.h.
◆ calc_PIP()
|
inlineprotectedvirtual |
Using this backend, calculate the phase identification parameter (PIP)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 251 of file AbstractState.h.
◆ calc_pmax()
|
inlineprotectedvirtual |
Using this backend, calculate the maximum pressure in Pa.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 379 of file AbstractState.h.
◆ calc_pressure()
|
inlineprotectedvirtual |
Using this backend, calculate the pressure in Pa.
Reimplemented in CoolProp::PCSAFTBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 227 of file AbstractState.h.
◆ calc_reciprocal_reduced_temperature()
|
inlineprotectedvirtual |
Using this backend, calculate the reciprocal reduced temperature (Tc/T)
Reimplemented in CoolProp::AbstractCubicBackend.
Definition at line 426 of file AbstractState.h.
◆ calc_reduced_density()
|
inlineprotectedvirtual |
Using this backend, calculate the reduced density (rho/rhoc)
Reimplemented in CoolProp::AbstractCubicBackend.
Definition at line 422 of file AbstractState.h.
◆ calc_reducing_state()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 366 of file AbstractState.h.
◆ calc_rhomass()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::IncompressibleBackend, and CoolProp::IF97Backend.
Definition at line 502 of file AbstractState.h.
◆ calc_rhomass_critical()
|
inlineprotectedvirtual |
Using this backend, get the critical point mass density in kg/m^3 - Added for IF97Backend which is mass based.
Reimplemented in CoolProp::IF97Backend.
Definition at line 490 of file AbstractState.h.
◆ calc_rhomolar()
|
inlineprotectedvirtual |
Using this backend, get the molar density in mol/m^3.
Reimplemented in CoolProp::TabularBackend, and CoolProp::IF97Backend.
Definition at line 644 of file AbstractState.h.
◆ calc_rhomolar_critical()
|
inlineprotectedvirtual |
Using this backend, get the critical point molar density in mol/m^3.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 486 of file AbstractState.h.
◆ calc_rhomolar_reducing()
|
inlineprotectedvirtual |
Using this backend, get the reducing point molar density in mol/m^3.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 494 of file AbstractState.h.
◆ calc_saturated_liquid_keyed_output()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 629 of file AbstractState.h.
◆ calc_saturated_vapor_keyed_output()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 632 of file AbstractState.h.
◆ calc_saturation_ancillary()
|
inlineprotectedvirtual |
- Parameters
-
param The key for the parameter to be returned Q The quality for the parameter that is given (0 = saturated liquid, 1 = saturated vapor) given The key for the parameter that is given value The value for the parameter that is given
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 561 of file AbstractState.h.
◆ calc_second_partial_deriv()
|
protectedvirtual |
Calculate the second partial derivative using the given backend.
Definition at line 1011 of file AbstractState.cpp.
◆ calc_second_saturation_deriv()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 616 of file AbstractState.h.
◆ calc_second_two_phase_deriv()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 622 of file AbstractState.h.
◆ calc_smass()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::IncompressibleBackend, and CoolProp::IF97Backend.
Definition at line 511 of file AbstractState.h.
◆ calc_smass_excess()
|
inlineprotectedvirtual |
Definition at line 514 of file AbstractState.h.
◆ calc_smolar()
|
inlineprotectedvirtual |
Using this backend, calculate the molar entropy in J/mol/K.
Reimplemented in CoolProp::TabularBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 155 of file AbstractState.h.
◆ calc_smolar_residual()
|
inlineprotectedvirtual |
Using this backend, calculate the residual molar entropy in J/mol/K.
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::PCSAFTBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 159 of file AbstractState.h.
◆ calc_specify_phase()
|
inlineprotectedvirtual |
Using this backend, specify the phase to be used for all further calculations.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::PCSAFTBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 570 of file AbstractState.h.
◆ calc_speed_sound()
|
inlineprotectedvirtual |
Using this backend, calculate the speed of sound in m/s.
Reimplemented in CoolProp::TabularBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 191 of file AbstractState.h.
◆ calc_state()
|
inlineprotectedvirtual |
Using this backend, calculate a phase given by the state string
- Parameters
-
state A string that describes the state desired, one of "hs_anchor", "critical"/"crit", "reducing"
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 583 of file AbstractState.h.
◆ calc_surface_tension()
|
inlineprotectedvirtual |
Using this backend, calculate the surface tension in N/m.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 215 of file AbstractState.h.
◆ calc_T()
|
inlineprotectedvirtual |
Using this backend, get the temperature.
Reimplemented in CoolProp::TabularBackend.
Definition at line 640 of file AbstractState.h.
◆ calc_T_critical()
|
inlineprotectedvirtual |
Using this backend, get the critical point temperature in K.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 470 of file AbstractState.h.
◆ calc_T_freeze()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::IncompressibleBackend.
Definition at line 609 of file AbstractState.h.
◆ calc_T_reducing()
|
inlineprotectedvirtual |
Using this backend, get the reducing point temperature in K.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 474 of file AbstractState.h.
◆ calc_tangent_plane_distance()
|
inlineprotectedvirtual |
Using this backend, calculate the tangent plane distance for a given trial composition.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 649 of file AbstractState.h.
◆ calc_Tmax()
|
inlineprotectedvirtual |
Using this backend, calculate the maximum temperature in K.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 371 of file AbstractState.h.
◆ calc_Tmin()
|
inlineprotectedvirtual |
Using this backend, calculate the minimum temperature in K.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 375 of file AbstractState.h.
◆ calc_true_critical_point()
|
inlineprotectedvirtual |
Using this backend, return true critical point where dp/drho|T = 0 and d2p/drho^2|T = 0.
Reimplemented in CoolProp::REFPROPMixtureBackend.
Definition at line 654 of file AbstractState.h.
◆ calc_Ttriple()
|
inlineprotectedvirtual |
Using this backend, get the triple point temperature in K.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 461 of file AbstractState.h.
◆ calc_umass()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::IncompressibleBackend, and CoolProp::IF97Backend.
Definition at line 526 of file AbstractState.h.
◆ calc_umass_excess()
|
inlineprotectedvirtual |
Definition at line 529 of file AbstractState.h.
◆ calc_umolar()
|
inlineprotectedvirtual |
Using this backend, calculate the molar internal energy in J/mol.
Reimplemented in CoolProp::TabularBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 163 of file AbstractState.h.
◆ calc_unspecify_phase()
|
inlineprotectedvirtual |
Using this backend, unspecify the phase.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::PCSAFTBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 574 of file AbstractState.h.
◆ calc_viscosity()
|
inlineprotectedvirtual |
Using this backend, calculate the viscosity in Pa-s.
Reimplemented in CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 207 of file AbstractState.h.
◆ calc_viscosity_contributions()
|
inlineprotectedvirtual |
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 662 of file AbstractState.h.
◆ calc_volumemass_excess()
|
inlineprotectedvirtual |
Definition at line 544 of file AbstractState.h.
◆ change_EOS()
|
inline |
Change the equation of state for a given component to a specified EOS.
- Parameters
-
i Index of the component to change (if a pure fluid, i=0) EOS_name Name of the EOS to use (something like "SRK", "PR", "XiangDeiters", but backend-specific)
- Note
- Calls the calc_change_EOS function of the implementation
Definition at line 1447 of file AbstractState.h.
◆ chemical_potential()
| double CoolProp::AbstractState::chemical_potential | ( | std::size_t | i | ) |
Return the chemical potential of the i-th component of the mixture.
Definition at line 707 of file AbstractState.cpp.
◆ clear()
|
virtual |
Clear all the cached values.
Ancillary curve values
Bulk values
Smoothing values
Cached low-level elements for in-place calculation of other properties
Two-Phase variables
Transport properties
Reimplemented in CoolProp::IncompressibleBackend, CoolProp::IF97Backend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 186 of file AbstractState.cpp.
◆ clear_comp_change()
|
virtual |
When the composition changes, clear all cached values that are only dependent on composition, but not the thermodynamic state.
Definition at line 176 of file AbstractState.cpp.
◆ compressibility_factor()
| double CoolProp::AbstractState::compressibility_factor | ( | void | ) |
Return the compressibility factor \( Z = p/(rho R T) \).
Definition at line 735 of file AbstractState.cpp.
◆ conductivity()
| double CoolProp::AbstractState::conductivity | ( | void | ) |
Return the thermal conductivity in W/m/K.
Definition at line 670 of file AbstractState.cpp.
◆ conductivity_contributions()
|
inline |
Return the thermal conductivity contributions, each in W/m/K.
Definition at line 1424 of file AbstractState.h.
◆ conformal_state()
|
inline |
Find the conformal state needed for ECS.
- Parameters
-
reference_fluid The reference fluid for which the conformal state will be calculated T Temperature (initial guess must be provided, or < 0 to start with unity shape factors) rhomolar Molar density (initial guess must be provided, or < 0 to start with unity shape factors)
Definition at line 1439 of file AbstractState.h.
◆ cp0mass()
|
inline |
Return the mass constant pressure specific heat for ideal gas part only in J/kg/K.
Definition at line 1136 of file AbstractState.h.
◆ cp0molar()
| double CoolProp::AbstractState::cp0molar | ( | void | ) |
Return the molar constant pressure specific heat for ideal gas part only in J/mol/K.
Definition at line 655 of file AbstractState.cpp.
◆ cpmass()
|
inline |
Return the mass constant pressure specific heat in J/kg/K.
Definition at line 1130 of file AbstractState.h.
◆ cpmolar()
| double CoolProp::AbstractState::cpmolar | ( | void | ) |
Return the molar constant pressure specific heat in J/mol/K.
Definition at line 651 of file AbstractState.cpp.
◆ criticality_contour_values()
|
inline |
Calculate the criticality contour values \(\mathcal{L}_1^*\) and \(\mathcal{M}_1^*\).
Definition at line 975 of file AbstractState.h.
◆ Cvirial()
| double CoolProp::AbstractState::Cvirial | ( | void | ) |
Return the C virial coefficient.
Definition at line 726 of file AbstractState.cpp.
◆ cvmass()
|
inline |
Return the mass constant volume specific heat in J/kg/K.
Definition at line 1142 of file AbstractState.h.
◆ cvmolar()
| double CoolProp::AbstractState::cvmolar | ( | void | ) |
Return the molar constant volume specific heat in J/mol/K.
Definition at line 658 of file AbstractState.cpp.
◆ d2alpha0_dDelta2()
|
inline |
Return the term \( \alpha^0_{\delta\delta} \).
Definition at line 1470 of file AbstractState.h.
◆ d2alpha0_dDelta_dTau()
|
inline |
Return the term \( \alpha^0_{\delta\tau} \).
Definition at line 1475 of file AbstractState.h.
◆ d2alpha0_dTau2()
|
inline |
Return the term \( \alpha^0_{\tau\tau} \).
Definition at line 1480 of file AbstractState.h.
◆ d2alphar_dDelta2()
|
inline |
Return the term \( \alpha^r_{\delta\delta} \).
Definition at line 1521 of file AbstractState.h.
◆ d2alphar_dDelta_dTau()
|
inline |
Return the term \( \alpha^r_{\delta\tau} \).
Definition at line 1526 of file AbstractState.h.
◆ d2alphar_dTau2()
|
inline |
Return the term \( \alpha^r_{\tau\tau} \).
Definition at line 1531 of file AbstractState.h.
◆ d3alpha0_dDelta2_dTau()
|
inline |
Return the term \( \alpha^0_{\delta\delta\tau} \).
Definition at line 1495 of file AbstractState.h.
◆ d3alpha0_dDelta3()
|
inline |
Return the term \( \alpha^0_{\delta\delta\delta} \).
Definition at line 1500 of file AbstractState.h.
◆ d3alpha0_dDelta_dTau2()
|
inline |
Return the term \( \alpha^0_{\delta\tau\tau} \).
Definition at line 1490 of file AbstractState.h.
◆ d3alpha0_dTau3()
|
inline |
Return the term \( \alpha^0_{\tau\tau\tau} \).
Definition at line 1485 of file AbstractState.h.
◆ d3alphar_dDelta2_dTau()
|
inline |
Return the term \( \alpha^r_{\delta\delta\tau} \).
Definition at line 1541 of file AbstractState.h.
◆ d3alphar_dDelta3()
|
inline |
Return the term \( \alpha^r_{\delta\delta\delta} \).
Definition at line 1536 of file AbstractState.h.
◆ d3alphar_dDelta_dTau2()
|
inline |
Return the term \( \alpha^r_{\delta\tau\tau} \).
Definition at line 1546 of file AbstractState.h.
◆ d3alphar_dTau3()
|
inline |
Return the term \( \alpha^r_{\tau\tau\tau} \).
Definition at line 1551 of file AbstractState.h.
◆ d4alphar_dDelta2_dTau2()
|
inline |
Return the term \( \alpha^r_{\delta\delta\tau\tau} \).
Definition at line 1566 of file AbstractState.h.
◆ d4alphar_dDelta3_dTau()
|
inline |
Return the term \( \alpha^r_{\delta\delta\delta\tau} \).
Definition at line 1561 of file AbstractState.h.
◆ d4alphar_dDelta4()
|
inline |
Return the term \( \alpha^r_{\delta\delta\delta\delta} \).
Definition at line 1556 of file AbstractState.h.
◆ d4alphar_dDelta_dTau3()
|
inline |
Return the term \( \alpha^r_{\delta\tau\tau\tau} \).
Definition at line 1571 of file AbstractState.h.
◆ d4alphar_dTau4()
|
inline |
Return the term \( \alpha^r_{\tau\tau\tau\tau} \).
Definition at line 1576 of file AbstractState.h.
◆ dalpha0_dDelta()
|
inline |
Return the term \( \alpha^0_{\delta} \).
Definition at line 1460 of file AbstractState.h.
◆ dalpha0_dTau()
|
inline |
Return the term \( \alpha^0_{\tau} \).
Definition at line 1465 of file AbstractState.h.
◆ dalphar_dDelta()
|
inline |
Return the term \( \alpha^r_{\delta} \).
Definition at line 1511 of file AbstractState.h.
◆ dalphar_dTau()
|
inline |
Return the term \( \alpha^r_{\tau} \).
Definition at line 1516 of file AbstractState.h.
◆ dBvirial_dT()
| double CoolProp::AbstractState::dBvirial_dT | ( | void | ) |
Return the derivative of the B virial coefficient with respect to temperature.
Definition at line 729 of file AbstractState.cpp.
◆ dCvirial_dT()
| double CoolProp::AbstractState::dCvirial_dT | ( | void | ) |
Return the derivative of the C virial coefficient with respect to temperature.
Definition at line 732 of file AbstractState.cpp.
◆ delta()
| double CoolProp::AbstractState::delta | ( | void | ) |
Return the reduced density ( \(\delta = \rho/\rho_c\))
Definition at line 549 of file AbstractState.cpp.
◆ description()
|
inline |
Return the description - backend dependent.
Definition at line 1021 of file AbstractState.h.
◆ dipole_moment()
|
inline |
Return the dipole moment in C-m (1 D = 3.33564e-30 C-m)
Definition at line 1026 of file AbstractState.h.
◆ factory() [1/2]
|
inlinestatic |
A factory function to return a pointer to a new-allocated instance of one of the backends.
This is a convenience function to allow for the use of '&' delimited fluid names. Slightly less computationally efficient than the
- Parameters
-
backend The backend in use, one of "HEOS", "REFPROP", etc. fluid_names Fluid names as a '&' delimited string
- Returns
Definition at line 702 of file AbstractState.h.
◆ factory() [2/2]
|
static |
A factory function to return a pointer to a new-allocated instance of one of the backends.
- Parameters
-
backend The backend in use, "HEOS", "REFPROP", etc. fluid_names A vector of strings of the fluid names
- Returns
- A pointer to the instance generated
Several backends are possible:
- "?" : The backend is unknown, we will parse the fluid string to determine the backend to be used. Probably will use HEOS backend (see below)
- "HEOS" : The Helmholtz Equation of State backend for use with pure and pseudo-pure fluids, and mixtures, all of which are based on multi-parameter Helmholtz Energy equations of state. The fluid part of the string should then either be
- A pure or pseudo-pure fluid name (eg. "PROPANE" or "R410A"), yielding a HelmholtzEOSBackend instance.
- A string that encodes the components of the mixture with a "&" between them (e.g. "R32&R125"), yielding a HelmholtzEOSMixtureBackend instance.
- "REFPROP" : The REFPROP backend will be used. The fluid part of the string should then either be
- A pure or pseudo-pure fluid name (eg. "PROPANE" or "R410A"), yielding a REFPROPBackend instance.
- A string that encodes the components of the mixture with a "&" between them (e.g. "R32&R125"), yielding a REFPROPMixtureBackend instance.
- "INCOMP": The incompressible backend will be used
- "TTSE&XXXX": The TTSE backend will be used, and the tables will be generated using the XXXX backend where XXXX is one of the base backends("HEOS", "REFPROP", etc. )
- "BICUBIC&XXXX": The Bicubic backend will be used, and the tables will be generated using the XXXX backend where XXXX is one of the base backends("HEOS", "REFPROP", etc. )
Very Important!! : Use a smart pointer to manage the pointer returned. In older versions of C++, you can use std::tr1::smart_ptr. In C++2011 you can use std::shared_ptr
Definition at line 126 of file AbstractState.cpp.
◆ first_partial_deriv()
|
inline |
The first partial derivative in homogeneous phases.
\[ \left(\frac{\partial A}{\partial B}\right)_C = \frac{\left(\frac{\partial A}{\partial \tau}\right)_\delta\left(\frac{\partial C}{\partial \delta}\right)_\tau-\left(\frac{\partial A}{\partial \delta}\right)_\tau\left(\frac{\partial C}{\partial \tau}\right)_\delta}{\left(\frac{\partial B}{\partial \tau}\right)_\delta\left(\frac{\partial C}{\partial \delta}\right)_\tau-\left(\frac{\partial B}{\partial \delta}\right)_\tau\left(\frac{\partial C}{\partial \tau}\right)_\delta} = \frac{N}{D}\]
Definition at line 1231 of file AbstractState.h.
◆ first_saturation_deriv()
|
inline |
The first partial derivative along the saturation curve.
Implementing the algorithms and ideas of: Matthis Thorade, Ali Saadat, "Partial derivatives of thermodynamic state properties for dynamic simulation", Environmental Earth Sciences, December 2013, Volume 70, Issue 8, pp 3497-3503
Basically the idea is that the p-T derivative is given by Clapeyron relations:
\[ \left(\frac{\partial T}{\partial p}\right)_{\sigma} = T\left(\frac{v'' - v'}{h'' - h'}\right)_{\sigma} \]
and then other derivatives can be obtained along the saturation curve from
\[ \left(\frac{\partial y}{\partial p}\right)_{\sigma} = \left(\frac{\partial y}{\partial p}\right)+\left(\frac{\partial y}{\partial T}\right)\left(\frac{\partial T}{\partial p}\right)_{\sigma} \]
\[ \left(\frac{\partial y}{\partial T}\right)_{\sigma} = \left(\frac{\partial y}{\partial T}\right)+\left(\frac{\partial y}{\partial p}\right)\left(\frac{\partial p}{\partial T}\right)_{\sigma} \]
where derivatives without the \( \sigma \) are homogeneous (conventional) derivatives.
- Parameters
-
Of1 The parameter that the derivative is taken of Wrt1 The parameter that the derivative is taken with respect to
Definition at line 1283 of file AbstractState.h.
◆ first_two_phase_deriv()
|
inline |
Calculate the first "two-phase" derivative as described by Thorade and Sadaat, EAS, 2013.
Implementing the algorithms and ideas of: Matthis Thorade, Ali Saadat, "Partial derivatives of thermodynamic state properties for dynamic simulation", Environmental Earth Sciences, December 2013, Volume 70, Issue 8, pp 3497-3503
Spline evaluation is as described in: S Quoilin, I Bell, A Desideri, P Dewallef, V Lemort, "Methods to increase the robustness of finite-volume flow models in thermodynamic systems", Energies 7 (3), 1621-1640
- Note
- Not all derivatives are supported!
- Parameters
-
Of The parameter to be derived Wrt The parameter that the derivative is taken with respect to Constant The parameter that is held constant
- Returns
Definition at line 1327 of file AbstractState.h.
◆ first_two_phase_deriv_splined()
|
inline |
Calculate the first "two-phase" derivative as described by Thorade and Sadaat, EAS, 2013.
Implementing the algorithms and ideas of: Matthis Thorade, Ali Saadat, "Partial derivatives of thermodynamic state properties for dynamic simulation", Environmental Earth Sciences, December 2013, Volume 70, Issue 8, pp 3497-3503
Spline evaluation is as described in: S Quoilin, I Bell, A Desideri, P Dewallef, V Lemort, "Methods to increase the robustness of finite-volume flow models in thermodynamic systems", Energies 7 (3), 1621-1640
- Note
- Not all derivatives are supported! If you need all three currently supported values (drho_dh__p, drho_dp__h and rho_spline), you should calculate drho_dp__h first to avoid duplicate calculations.
- Parameters
-
Of The parameter to be derived Wrt The parameter that the derivative is taken with respect to Constant The parameter that is held constant x_end The end vapor quality at which the spline is defined (spline is active in [0, x_end])
- Returns
Definition at line 1371 of file AbstractState.h.
◆ fluid_names()
| std::vector< std::string > CoolProp::AbstractState::fluid_names | ( | void | ) |
Return a vector of strings of the fluid names that are in use.
Definition at line 173 of file AbstractState.cpp.
◆ fluid_param_string()
|
inlinevirtual |
Return a string from the backend for the mixture/fluid - backend dependent - could be CAS #, name, etc.
Reimplemented in CoolProp::REFPROPMixtureBackend, CoolProp::IncompressibleBackend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 849 of file AbstractState.h.
◆ fugacity()
| double CoolProp::AbstractState::fugacity | ( | std::size_t | i | ) |
Return the fugacity of the i-th component of the mixture.
Definition at line 703 of file AbstractState.cpp.
◆ fugacity_coefficient()
| double CoolProp::AbstractState::fugacity_coefficient | ( | std::size_t | i | ) |
Return the fugacity coefficient of the i-th component of the mixture.
Definition at line 695 of file AbstractState.cpp.
◆ fugacity_coefficients()
| std::vector< double > CoolProp::AbstractState::fugacity_coefficients | ( | ) |
Return a vector of the fugacity coefficients for all components in the mixture.
Definition at line 699 of file AbstractState.cpp.
◆ fundamental_derivative_of_gas_dynamics()
| double CoolProp::AbstractState::fundamental_derivative_of_gas_dynamics | ( | void | ) |
Return the fundamental derivative of gas dynamics \( \Gamma \).
see also Colonna et al, FPE, 2010
\[ \Gamma = 1+\frac{\rho}{c}\left(\frac{\partial c}{\partial \rho}\right)_{s} = 1+\frac{\rho}{2c^2}\left(\frac{\partial^2 p}{\partial \rho^2}\right)_{s} = \frac{v^3}{2c^2}\left(\frac{\partial^2 p}{\partial v^2}\right)_{s}\]
Note: densities are mass-based densities, not mole-based densities
Definition at line 739 of file AbstractState.cpp.
◆ gas_constant()
| double CoolProp::AbstractState::gas_constant | ( | void | ) |
Return the mole-fraction weighted gas constant in J/mol/K.
Definition at line 691 of file AbstractState.cpp.
◆ get_binary_interaction_double() [1/2]
|
inlinevirtual |
Get binary mixture double value (EXPERT USE ONLY!!!)
Reimplemented in CoolProp::AbstractCubicBackend, CoolProp::REFPROPMixtureBackend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::VTPRBackend.
Definition at line 887 of file AbstractState.h.
◆ get_binary_interaction_double() [2/2]
|
inlinevirtual |
Get binary mixture double value (EXPERT USE ONLY!!!)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 883 of file AbstractState.h.
◆ get_binary_interaction_string()
|
inlinevirtual |
Get binary mixture string value (EXPERT USE ONLY!!!)
Reimplemented in CoolProp::REFPROPMixtureBackend.
Definition at line 891 of file AbstractState.h.
◆ get_fluid_constant()
|
inlinevirtual |
Get a constant for one of the fluids forming this mixture
- Parameters
-
i Index (0-based) of the fluid param parameter you want to obtain (probably one that is a trivial parameter)
Reimplemented in CoolProp::PCSAFTBackend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 860 of file AbstractState.h.
◆ get_fluid_parameter_double()
|
inlinevirtual |
Double fluid parameter (currently the volume translation parameter for cubic)
Reimplemented in CoolProp::AbstractCubicBackend.
Definition at line 907 of file AbstractState.h.
◆ get_mass_fractions()
|
inlinevirtual |
Get the mass fractions of the fluid.
Definition at line 828 of file AbstractState.h.
◆ get_mole_fractions()
|
pure virtual |
Get the mole fractions of the fluid.
Implemented in CoolProp::PCSAFTBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, CoolProp::AbstractCubicBackend, CoolProp::TabularBackend, CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
◆ get_phase_envelope_data()
|
inline |
After having calculated the phase envelope, return the phase envelope data.
Definition at line 1388 of file AbstractState.h.
◆ get_reducing_state()
|
inlinevirtual |
Get the state that is used in the equation of state or mixture model to reduce the state. For pure fluids this is usually, but not always, the critical point. For mixture models, it is usually composition dependent
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 919 of file AbstractState.h.
◆ get_spinodal_data()
|
inline |
Get the data from the spinodal curve constructed in the call to build_spinodal()
Definition at line 970 of file AbstractState.h.
◆ get_state()
|
inline |
Get a desired state point - backend dependent.
Definition at line 924 of file AbstractState.h.
◆ gibbsmass()
|
inline |
Return the Gibbs energy in J/kg.
Definition at line 1150 of file AbstractState.h.
◆ gibbsmass_excess()
|
inline |
Return the excess Gibbs energy in J/kg.
Definition at line 1156 of file AbstractState.h.
◆ gibbsmolar()
| double CoolProp::AbstractState::gibbsmolar | ( | void | ) |
Return the Gibbs energy in J/mol.
Definition at line 627 of file AbstractState.cpp.
◆ gibbsmolar_excess()
| double CoolProp::AbstractState::gibbsmolar_excess | ( | void | ) |
Return the excess Gibbs energy in J/mol.
Definition at line 635 of file AbstractState.cpp.
◆ gibbsmolar_residual()
| double CoolProp::AbstractState::gibbsmolar_residual | ( | void | ) |
Return the residual Gibbs energy in J/mol.
Definition at line 631 of file AbstractState.cpp.
◆ has_melting_line()
|
inlinevirtual |
Return true if the fluid has a melting line - default is false, but can be re-implemented by derived class.
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 1397 of file AbstractState.h.
◆ helmholtzmass()
|
inline |
Return the Helmholtz energy in J/kg.
Definition at line 1162 of file AbstractState.h.
◆ helmholtzmass_excess()
|
inline |
Return the excess Helmholtz energy in J/kg.
Definition at line 1168 of file AbstractState.h.
◆ helmholtzmolar()
| double CoolProp::AbstractState::helmholtzmolar | ( | void | ) |
Return the Helmholtz energy in J/mol.
Definition at line 639 of file AbstractState.cpp.
◆ helmholtzmolar_excess()
| double CoolProp::AbstractState::helmholtzmolar_excess | ( | void | ) |
Return the excess Helmholtz energy in J/mol.
Definition at line 643 of file AbstractState.cpp.
◆ hmass()
|
inline |
Return the mass enthalpy in J/kg.
Definition at line 1092 of file AbstractState.h.
◆ hmass_excess()
|
inline |
Return the excess mass enthalpy in J/kg.
Definition at line 1098 of file AbstractState.h.
◆ hmolar()
| double CoolProp::AbstractState::hmolar | ( | void | ) |
Return the molar enthalpy in J/mol.
Definition at line 595 of file AbstractState.cpp.
◆ hmolar_excess()
| double CoolProp::AbstractState::hmolar_excess | ( | void | ) |
Return the excess molar enthalpy in J/mol.
Definition at line 603 of file AbstractState.cpp.
◆ hmolar_residual()
| double CoolProp::AbstractState::hmolar_residual | ( | void | ) |
Return the residual molar enthalpy in J/mol.
Definition at line 599 of file AbstractState.cpp.
◆ ideal_curve()
|
inline |
Calculate an ideal curve for a pure fluid.
- Parameters
-
type The type of ideal curve you would like to calculate - "Ideal", "Boyle", "Joule-Thomson", "Joule Inversion", etc. T The temperatures along the curve in K p The pressures along the curve in Pa
Definition at line 1219 of file AbstractState.h.
◆ isentropic_expansion_coefficient()
| double CoolProp::AbstractState::isentropic_expansion_coefficient | ( | void | ) |
Return the isentropic expansion coefficient \( \kappa_s = -\frac{c_p}{c_v}\frac{v}{p}\left.\frac{\partial p}{\partial v}\right|_T = \frac{\rho}{p}\left.\frac{\partial p}{\partial \rho}\right|_s\).
Definition at line 720 of file AbstractState.cpp.
◆ isHomogeneousPhase()
|
inlineprotected |
Definition at line 90 of file AbstractState.h.
◆ isobaric_expansion_coefficient()
| double CoolProp::AbstractState::isobaric_expansion_coefficient | ( | void | ) |
Return the isobaric expansion coefficient \( \beta = \frac{1}{v}\left.\frac{\partial v}{\partial T}\right|_p = -\frac{1}{\rho}\left.\frac{\partial \rho}{\partial T}\right|_p\) in 1/K.
Definition at line 717 of file AbstractState.cpp.
◆ isothermal_compressibility()
| double CoolProp::AbstractState::isothermal_compressibility | ( | void | ) |
Return the isothermal compressibility \( \kappa = -\frac{1}{v}\left.\frac{\partial v}{\partial p}\right|_T=\frac{1}{\rho}\left.\frac{\partial \rho}{\partial p}\right|_T\) in 1/Pa.
Definition at line 714 of file AbstractState.cpp.
◆ isSupercriticalPhase()
|
inlineprotected |
Definition at line 86 of file AbstractState.h.
◆ isTwoPhase()
|
inlineprotected |
Definition at line 94 of file AbstractState.h.
◆ keyed_output()
| double CoolProp::AbstractState::keyed_output | ( | parameters | key | ) |
Retrieve a value by key.
Definition at line 430 of file AbstractState.cpp.
◆ mass_to_molar_inputs()
|
protectedvirtual |
Convert mass-based input pair to molar-based input pair; If molar-based, do nothing.
< Mass density in kg/m^3, Temperature in K
< Entropy in J/kg/K, Temperature in K
< Mass density in kg/m^3, Pressure in Pa
< Mass density in kg/m^3, molar quality
< Enthalpy in J/kg, Pressure in Pa
< Pressure in Pa, Entropy in J/kg/K
< Pressure in Pa, Internal energy in J/kg
< Enthalpy in J/kg, Entropy in J/kg/K
< Entropy in J/kg/K, Internal energy in J/kg
< Mass density in kg/m^3, Enthalpy in J/kg
< Mass density in kg/m^3, Entropy in J/kg/K
< Mass density in kg/m^3, Internal energy in J/kg
Definition at line 278 of file AbstractState.cpp.
◆ melting_line()
| double CoolProp::AbstractState::melting_line | ( | int | param, |
| int | given, | ||
| double | value | ||
| ) |
Return a value from the melting line
- Parameters
-
param The key for the parameter to be returned given The key for the parameter that is given value The value for the parameter that is given
Definition at line 674 of file AbstractState.cpp.
◆ molar_mass()
| double CoolProp::AbstractState::molar_mass | ( | void | ) |
Return the molar mass in kg/mol.
Definition at line 687 of file AbstractState.cpp.
◆ mole_fractions_liquid()
|
inline |
Get the mole fractions of the equilibrium liquid phase.
Definition at line 806 of file AbstractState.h.
◆ mole_fractions_liquid_double()
|
inline |
Get the mole fractions of the equilibrium liquid phase (but as a double for use in SWIG wrapper)
Definition at line 810 of file AbstractState.h.
◆ mole_fractions_vapor()
|
inline |
Get the mole fractions of the equilibrium vapor phase.
Definition at line 816 of file AbstractState.h.
◆ mole_fractions_vapor_double()
|
inline |
Get the mole fractions of the equilibrium vapor phase (but as a double for use in SWIG wrapper)
Definition at line 820 of file AbstractState.h.
◆ name()
|
inline |
Return the name - backend dependent.
Definition at line 1017 of file AbstractState.h.
◆ p()
|
inline |
Return the pressure in Pa.
Definition at line 1060 of file AbstractState.h.
◆ p_critical()
| double CoolProp::AbstractState::p_critical | ( | void | ) |
Return the critical pressure in Pa.
Definition at line 574 of file AbstractState.cpp.
◆ p_triple()
| double CoolProp::AbstractState::p_triple | ( | void | ) |
Return the triple point pressure in Pa.
Definition at line 577 of file AbstractState.cpp.
◆ phase()
|
inline |
Get the phase of the state.
Definition at line 938 of file AbstractState.h.
◆ PIP()
|
inline |
Return the phase identification parameter (PIP) of G. Venkatarathnam and L.R. Oellrich, "Identification of the phase of a fluid using partial derivatives of pressure, volume, and temperature without reference to saturation properties: Applications in phase equilibria calculations".
Definition at line 1203 of file AbstractState.h.
◆ pmax()
| double CoolProp::AbstractState::pmax | ( | void | ) |
Get the maximum pressure in Pa.
Definition at line 562 of file AbstractState.cpp.
◆ Prandtl()
|
inline |
Return the Prandtl number (dimensionless)
Definition at line 1430 of file AbstractState.h.
◆ Q()
|
inline |
Return the vapor quality (mol/mol); Q = 0 for saturated liquid.
Definition at line 1064 of file AbstractState.h.
◆ rhomass()
|
inline |
Return the mass density in kg/m^3.
Definition at line 1056 of file AbstractState.h.
◆ rhomass_critical()
| double CoolProp::AbstractState::rhomass_critical | ( | void | ) |
Return the critical mass density in kg/m^3.
Definition at line 583 of file AbstractState.cpp.
◆ rhomass_reducing()
| double CoolProp::AbstractState::rhomass_reducing | ( | void | ) |
Return the mass density at the reducing point in kg/m^3.
Definition at line 592 of file AbstractState.cpp.
◆ rhomolar()
|
inline |
Return the molar density in mol/m^3.
Definition at line 1052 of file AbstractState.h.
◆ rhomolar_critical()
| double CoolProp::AbstractState::rhomolar_critical | ( | void | ) |
Return the critical molar density in mol/m^3.
Definition at line 580 of file AbstractState.cpp.
◆ rhomolar_reducing()
| double CoolProp::AbstractState::rhomolar_reducing | ( | void | ) |
Return the molar density at the reducing point in mol/m^3.
Definition at line 586 of file AbstractState.cpp.
◆ saturated_liquid_keyed_output()
|
inline |
Get an output from the saturated liquid state by key.
Definition at line 1039 of file AbstractState.h.
◆ saturated_vapor_keyed_output()
|
inline |
Get an output from the saturated vapor state by key.
Definition at line 1043 of file AbstractState.h.
◆ saturation_ancillary()
| double CoolProp::AbstractState::saturation_ancillary | ( | parameters | param, |
| int | Q, | ||
| parameters | given, | ||
| double | value | ||
| ) |
Return the value from a saturation ancillary curve (if the backend implements it)
- Parameters
-
param The key for the parameter to be returned Q The quality for the parameter that is given (0 = saturated liquid, 1 = saturated vapor) given The key for the parameter that is given value The value for the parameter that is given
Definition at line 680 of file AbstractState.cpp.
◆ second_partial_deriv()
|
inline |
The second partial derivative in homogeneous phases.
The first partial derivative (CoolProp::AbstractState::first_partial_deriv) can be expressed as
\[ \left(\frac{\partial A}{\partial B}\right)_C = \frac{\left(\frac{\partial A}{\partial T}\right)_\rho\left(\frac{\partial C}{\partial \rho}\right)_T-\left(\frac{\partial A}{\partial \rho}\right)_T\left(\frac{\partial C}{\partial T}\right)_\rho}{\left(\frac{\partial B}{\partial T}\right)_\rho\left(\frac{\partial C}{\partial \rho}\right)_T-\left(\frac{\partial B}{\partial \rho}\right)_T\left(\frac{\partial C}{\partial T}\right)_\rho} = \frac{N}{D}\]
and the second derivative can be expressed as
\[ \frac{\partial}{\partial D}\left(\left(\frac{\partial A}{\partial B}\right)_C\right)_E = \frac{\frac{\partial}{\partial T}\left( \left(\frac{\partial A}{\partial B}\right)_C \right)_\rho\left(\frac{\partial E}{\partial \rho}\right)_T-\frac{\partial}{\partial \rho}\left(\left(\frac{\partial A}{\partial B}\right)_C\right)_T\left(\frac{\partial E}{\partial T}\right)_\rho}{\left(\frac{\partial D}{\partial T}\right)_\rho\left(\frac{\partial E}{\partial \rho}\right)_T-\left(\frac{\partial D}{\partial \rho}\right)_T\left(\frac{\partial E}{\partial T}\right)_\rho} \]
which can be expressed in parts as
\[\left(\frac{\partial N}{\partial \rho}\right)_{T} = \left(\frac{\partial A}{\partial T}\right)_\rho\left(\frac{\partial^2 C}{\partial \rho^2}\right)_{T}+\left(\frac{\partial^2 A}{\partial T\partial\rho}\right)\left(\frac{\partial C}{\partial \rho}\right)_{T}-\left(\frac{\partial A}{\partial \rho}\right)_T\left(\frac{\partial^2 C}{\partial T\partial\rho}\right)-\left(\frac{\partial^2 A}{\partial \rho^2}\right)_{T}\left(\frac{\partial C}{\partial T}\right)_\rho\]
\[\left(\frac{\partial D}{\partial \rho}\right)_{T} = \left(\frac{\partial B}{\partial T}\right)_\rho\left(\frac{\partial^2 C}{\partial \rho^2}\right)_{T}+\left(\frac{\partial^2 B}{\partial T\partial\rho}\right)\left(\frac{\partial C}{\partial \rho}\right)_{T}-\left(\frac{\partial B}{\partial \rho}\right)_T\left(\frac{\partial^2 C}{\partial T\partial\rho}\right)-\left(\frac{\partial^2 B}{\partial \rho^2}\right)_{T}\left(\frac{\partial C}{\partial T}\right)_\rho\]
\[\left(\frac{\partial N}{\partial T}\right)_{\rho} = \left(\frac{\partial A}{\partial T}\right)_\rho\left(\frac{\partial^2 C}{\partial \rho\partial T}\right)+\left(\frac{\partial^2 A}{\partial T^2}\right)_\rho\left(\frac{\partial C}{\partial \rho}\right)_{T}-\left(\frac{\partial A}{\partial \rho}\right)_T\left(\frac{\partial^2 C}{\partial T^2}\right)_\rho-\left(\frac{\partial^2 A}{\partial \rho\partial T}\right)\left(\frac{\partial C}{\partial T}\right)_\rho\]
\[\left(\frac{\partial D}{\partial T}\right)_{\rho} = \left(\frac{\partial B}{\partial T}\right)_\rho\left(\frac{\partial^2 C}{\partial \rho\partial T}\right)+\left(\frac{\partial^2 B}{\partial T^2}\right)_\rho\left(\frac{\partial C}{\partial \rho}\right)_{T}-\left(\frac{\partial B}{\partial \rho}\right)_T\left(\frac{\partial^2 C}{\partial T^2}\right)_\rho-\left(\frac{\partial^2 B}{\partial \rho\partial T}\right)\left(\frac{\partial C}{\partial T}\right)_\rho\]
\[\frac{\partial}{\partial \rho}\left( \left(\frac{\partial A}{\partial B}\right)_C \right)_T = \frac{D\left(\frac{\partial N}{\partial \rho}\right)_{T}-N\left(\frac{\partial D}{\partial \rho}\right)_{\tau}}{D^2}\]
\[\frac{\partial}{\partial T}\left( \left(\frac{\partial A}{\partial B}\right)_C \right)_\rho = \frac{D\left(\frac{\partial N}{\partial T}\right)_{\rho}-N\left(\frac{\partial D}{\partial T}\right)_{\rho}}{D^2}\]
The terms \( N \) and \( D \) are the numerator and denominator from CoolProp::AbstractState::first_partial_deriv respectively
Definition at line 1258 of file AbstractState.h.
◆ second_saturation_deriv()
|
inline |
The second partial derivative along the saturation curve.
Implementing the algorithms and ideas of: Matthis Thorade, Ali Saadat, "Partial derivatives of thermodynamic state properties for dynamic simulation", Environmental Earth Sciences, December 2013, Volume 70, Issue 8, pp 3497-3503
Like with first_saturation_deriv, we can express the derivative as
\[ \left(\frac{\partial y}{\partial T}\right)_{\sigma} = \left(\frac{\partial y}{\partial T}\right)+\left(\frac{\partial y}{\partial p}\right)\left(\frac{\partial p}{\partial T}\right)_{\sigma} \]
where \( y \) is already a saturation derivative. So you might end up with something like
\[ \left(\frac{\partial \left(\frac{\partial T}{\partial p}\right)_{\sigma}}{\partial T}\right)_{\sigma} = \left(\frac{\partial \left(\frac{\partial T}{\partial p}\right)_{\sigma}}{\partial T}\right)+\left(\frac{\partial \left(\frac{\partial T}{\partial p}\right)_{\sigma}}{\partial p}\right)\left(\frac{\partial p}{\partial T}\right)_{\sigma} \]
- Parameters
-
Of1 The parameter that the first derivative is taken of Wrt1 The parameter that the first derivative is taken with respect to Wrt2 The parameter that the second derivative is taken with respect to
Definition at line 1304 of file AbstractState.h.
◆ second_two_phase_deriv()
|
inline |
Calculate the second "two-phase" derivative as described by Thorade and Sadaat, EAS, 2013.
Implementing the algorithms and ideas of: Matthis Thorade, Ali Saadat, "Partial derivatives of thermodynamic state properties for dynamic simulation", Environmental Earth Sciences, December 2013, Volume 70, Issue 8, pp 3497-3503
- Note
- Not all derivatives are supported!
- Parameters
-
Of The parameter to be derived Wrt1 The parameter that the derivative is taken with respect to in the first derivative Constant1 The parameter that is held constant in the first derivative Wrt2 The parameter that the derivative is taken with respect to in the second derivative Constant2 The parameter that is held constant in the second derivative
- Returns
Definition at line 1347 of file AbstractState.h.
◆ set_binary_interaction_double() [1/2]
|
inlinevirtual |
Set binary mixture floating point parameter (EXPERT USE ONLY!!!)
Reimplemented in CoolProp::AbstractCubicBackend, CoolProp::REFPROPMixtureBackend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::VTPRBackend.
Definition at line 870 of file AbstractState.h.
◆ set_binary_interaction_double() [2/2]
|
inlinevirtual |
Set binary mixture floating point parameter (EXPERT USE ONLY!!!)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 866 of file AbstractState.h.
◆ set_binary_interaction_string() [1/2]
|
inlinevirtual |
Set binary mixture string parameter (EXPERT USE ONLY!!!)
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 879 of file AbstractState.h.
◆ set_binary_interaction_string() [2/2]
|
inlinevirtual |
Set binary mixture string parameter (EXPERT USE ONLY!!!)
Definition at line 874 of file AbstractState.h.
◆ set_cubic_alpha_C()
|
inlinevirtual |
Set the cubic alpha function's constants:
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 899 of file AbstractState.h.
◆ set_fluid_parameter_double()
|
inlinevirtual |
Set fluid parameter (currently the volume translation parameter for cubic)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
Definition at line 903 of file AbstractState.h.
◆ set_mass_fractions()
|
pure virtual |
◆ set_mole_fractions()
|
pure virtual |
◆ set_reference_stateD()
|
inlinevirtual |
Set the reference state based on a thermodynamic state point specified by temperature and molar density
- Parameters
-
T Temperature at reference state [K] rhomolar Molar density at reference state [mol/m^3] hmolar0 Molar enthalpy at reference state [J/mol] smolar0 Molar entropy at reference state [J/mol/K]
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 782 of file AbstractState.h.
◆ set_reference_stateS()
|
inlinevirtual |
Set the reference state based on a string representation.
- Parameters
-
reference_state The reference state to use, one of
| Reference State | Description |
|---|---|
| "IIR" | h = 200 kJ/kg, s=1 kJ/kg/K at 0C saturated liquid |
| "ASHRAE" | h = 0, s = 0 @ -40C saturated liquid |
| "NBP" | h = 0, s = 0 @ 1.0 bar saturated liquid |
| "DEF" | Reset to the default reference state for the fluid |
| "RESET" | Remove the offset |
The offset in the ideal gas Helmholtz energy can be obtained from
\[ \displaystyle\frac{\Delta s}{R_u/M}+\frac{\Delta h}{(R_u/M)T}\tau \]
where \( \Delta s = s-s_{spec} \) and \( \Delta h = h-h_{spec} \)
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 772 of file AbstractState.h.
◆ set_T()
|
inline |
Set the internal variable T without a flash call (expert use only!)
Definition at line 732 of file AbstractState.h.
◆ set_volu_fractions()
|
inlinevirtual |
Reimplemented in CoolProp::PCSAFTBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, and CoolProp::AbstractCubicBackend.
Definition at line 749 of file AbstractState.h.
◆ smass()
|
inline |
Return the molar entropy in J/kg/K.
Definition at line 1106 of file AbstractState.h.
◆ smass_excess()
|
inline |
Return the molar entropy in J/kg/K.
Definition at line 1112 of file AbstractState.h.
◆ smolar()
| double CoolProp::AbstractState::smolar | ( | void | ) |
Return the molar entropy in J/mol/K.
Definition at line 607 of file AbstractState.cpp.
◆ smolar_excess()
| double CoolProp::AbstractState::smolar_excess | ( | void | ) |
Return the molar entropy in J/mol/K.
Definition at line 615 of file AbstractState.cpp.
◆ smolar_residual()
| double CoolProp::AbstractState::smolar_residual | ( | void | ) |
Return the residual molar entropy (as a function of temperature and density) in J/mol/K.
Definition at line 611 of file AbstractState.cpp.
◆ specify_phase()
|
inline |
Specify the phase for all further calculations with this state class.
Definition at line 942 of file AbstractState.h.
◆ speed_sound()
| double CoolProp::AbstractState::speed_sound | ( | void | ) |
Return the speed of sound in m/s.
Definition at line 662 of file AbstractState.cpp.
◆ surface_tension()
| double CoolProp::AbstractState::surface_tension | ( | void | ) |
Return the surface tension in N/m.
Definition at line 683 of file AbstractState.cpp.
◆ T()
|
inline |
Return the temperature in K.
Definition at line 1048 of file AbstractState.h.
◆ T_critical()
| double CoolProp::AbstractState::T_critical | ( | void | ) |
Return the critical temperature in K.
Definition at line 565 of file AbstractState.cpp.
◆ T_reducing()
| double CoolProp::AbstractState::T_reducing | ( | void | ) |
Return the reducing point temperature in K.
Definition at line 568 of file AbstractState.cpp.
◆ tangent_plane_distance()
|
inline |
Return the tangent plane distance for a given trial composition w
- Parameters
-
T Temperature (K) p Pressure (Pa) w The trial composition rhomolar_guess (mol/m^3) The molar density guess value (if <0 (default), not used; if >0, guess value will be used in flash evaluation)
\[ tpd(w) = \sum_i w_i(\ln w_i + \ln \phi_i(w) - d_i) \]
with
\[ d_i = \ln z_i + \ln \phi_i(z) \]
Or you can express the \( tpd \) in terms of fugacity (See Table 7.3 from GERG 2004 monograph) since \( \ln \phi_i = \ln f_i - \ln p -\ln z_i\) thus
\[ d_i = \ln f_i(z) - \ln p\]
and
\[ tpd(w) = \sum_i w_i(\ln f_i(w) - \ln p - d_i) \]
and the \( \ln p \) cancel, leaving
\[ tpd(w) = \sum_i w_i(\ln f_i(w) - \ln f_i(z)) \]
Definition at line 1002 of file AbstractState.h.
◆ tau()
| double CoolProp::AbstractState::tau | ( | void | ) |
Return the reciprocal of the reduced temperature ( \(\tau = T_c/T\))
Definition at line 545 of file AbstractState.cpp.
◆ Tmax()
| double CoolProp::AbstractState::Tmax | ( | void | ) |
Get the maximum temperature in K.
Definition at line 556 of file AbstractState.cpp.
◆ Tmin()
| double CoolProp::AbstractState::Tmin | ( | void | ) |
Get the minimum temperature in K.
Definition at line 553 of file AbstractState.cpp.
◆ trivial_keyed_output()
| double CoolProp::AbstractState::trivial_keyed_output | ( | parameters | key | ) |
A trivial keyed output like molar mass that does not depend on the state.
Definition at line 368 of file AbstractState.cpp.
◆ true_critical_point()
|
inline |
Calculate the "true" critical point for pure fluids where dpdrho|T and d2p/drho2|T are equal to zero.
Definition at line 1208 of file AbstractState.h.
◆ Ttriple()
| double CoolProp::AbstractState::Ttriple | ( | void | ) |
Get the triple point temperature in K.
Definition at line 559 of file AbstractState.cpp.
◆ umass()
|
inline |
Return the mass internal energy in J/kg.
Definition at line 1118 of file AbstractState.h.
◆ umass_excess()
|
inline |
Return the excess internal energy in J/kg.
Definition at line 1124 of file AbstractState.h.
◆ umolar()
| double CoolProp::AbstractState::umolar | ( | void | ) |
Return the molar internal energy in J/mol.
Definition at line 619 of file AbstractState.cpp.
◆ umolar_excess()
| double CoolProp::AbstractState::umolar_excess | ( | void | ) |
Return the excess internal energy in J/mol.
Definition at line 623 of file AbstractState.cpp.
◆ unspecify_phase()
|
inline |
Unspecify the phase and go back to calculating it based on the inputs.
Definition at line 946 of file AbstractState.h.
◆ update()
|
pure virtual |
Update the state using two state variables.
Implemented in CoolProp::REFPROPMixtureBackend, CoolProp::TabularBackend, CoolProp::PCSAFTBackend, CoolProp::IncompressibleBackend, CoolProp::IF97Backend, CoolProp::HelmholtzEOSMixtureBackend, and CoolProp::AbstractCubicBackend.
◆ update_states()
|
inlineprotectedvirtual |
Update the states after having changed the reference state for enthalpy and entropy.
Reimplemented in CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 549 of file AbstractState.h.
◆ update_with_guesses()
|
inlinevirtual |
Update the state using two state variables and providing guess values Some or all of the guesses will be used - this is backend dependent
Reimplemented in CoolProp::REFPROPMixtureBackend, and CoolProp::HelmholtzEOSMixtureBackend.
Definition at line 837 of file AbstractState.h.
◆ using_mass_fractions()
|
pure virtual |
◆ using_mole_fractions()
|
pure virtual |
◆ using_volu_fractions()
|
pure virtual |
◆ viscosity()
| double CoolProp::AbstractState::viscosity | ( | void | ) |
Return the viscosity in Pa-s.
Definition at line 666 of file AbstractState.cpp.
◆ viscosity_contributions()
|
inline |
Return the viscosity contributions, each in Pa-s.
Definition at line 1418 of file AbstractState.h.
◆ volumemass_excess()
|
inline |
Return the excess volume in m^3/kg.
Definition at line 1174 of file AbstractState.h.
◆ volumemolar_excess()
| double CoolProp::AbstractState::volumemolar_excess | ( | void | ) |
Return the excess volume in m^3/mol.
Definition at line 647 of file AbstractState.cpp.
Member Data Documentation
◆ _alpha0
|
protected |
Cached low-level elements for in-place calculation of other properties.
Definition at line 132 of file AbstractState.h.
◆ _alphar
|
protected |
Definition at line 133 of file AbstractState.h.
◆ _conductivity
|
protected |
Definition at line 113 of file AbstractState.h.
◆ _cp0molar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _cpmolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _critical
|
protected |
Two important points.
Definition at line 99 of file AbstractState.h.
◆ _cvmolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _d2alpha0_dDelta2
|
protected |
Definition at line 132 of file AbstractState.h.
◆ _d2alpha0_dDelta_dTau
|
protected |
Definition at line 132 of file AbstractState.h.
◆ _d2alpha0_dTau2
|
protected |
Definition at line 132 of file AbstractState.h.
◆ _d2alphar_dDelta2
|
protected |
Definition at line 134 of file AbstractState.h.
◆ _d2alphar_dDelta2_lim
|
protected |
Definition at line 137 of file AbstractState.h.
◆ _d2alphar_dDelta_dTau
|
protected |
Definition at line 134 of file AbstractState.h.
◆ _d2alphar_dDelta_dTau_lim
|
protected |
Definition at line 137 of file AbstractState.h.
◆ _d2alphar_dTau2
|
protected |
Definition at line 133 of file AbstractState.h.
◆ _d3alpha0_dDelta2_dTau
|
protected |
Definition at line 133 of file AbstractState.h.
◆ _d3alpha0_dDelta3
|
protected |
Definition at line 133 of file AbstractState.h.
◆ _d3alpha0_dDelta_dTau2
|
protected |
Definition at line 133 of file AbstractState.h.
◆ _d3alpha0_dTau3
|
protected |
Definition at line 132 of file AbstractState.h.
◆ _d3alphar_dDelta2_dTau
|
protected |
Definition at line 134 of file AbstractState.h.
◆ _d3alphar_dDelta2_dTau_lim
|
protected |
Definition at line 137 of file AbstractState.h.
◆ _d3alphar_dDelta3
|
protected |
Definition at line 134 of file AbstractState.h.
◆ _d3alphar_dDelta_dTau2
|
protected |
Definition at line 134 of file AbstractState.h.
◆ _d3alphar_dTau3
|
protected |
Definition at line 134 of file AbstractState.h.
◆ _d4alphar_dDelta2_dTau2
|
protected |
Definition at line 135 of file AbstractState.h.
◆ _d4alphar_dDelta3_dTau
|
protected |
Definition at line 135 of file AbstractState.h.
◆ _d4alphar_dDelta4
|
protected |
Definition at line 135 of file AbstractState.h.
◆ _d4alphar_dDelta_dTau3
|
protected |
Definition at line 135 of file AbstractState.h.
◆ _d4alphar_dTau4
|
protected |
Definition at line 134 of file AbstractState.h.
◆ _dalpha0_dDelta
|
protected |
Definition at line 132 of file AbstractState.h.
◆ _dalpha0_dTau
|
protected |
Definition at line 132 of file AbstractState.h.
◆ _dalphar_dDelta
|
protected |
Definition at line 133 of file AbstractState.h.
◆ _dalphar_dDelta_lim
|
protected |
Definition at line 137 of file AbstractState.h.
◆ _dalphar_dTau
|
protected |
Definition at line 133 of file AbstractState.h.
◆ _delta
|
protected |
Definition at line 110 of file AbstractState.h.
◆ _drho_spline_dh__constp
|
protected |
Definition at line 129 of file AbstractState.h.
◆ _drho_spline_dp__consth
|
protected |
Definition at line 129 of file AbstractState.h.
◆ _fluid_type
|
protected |
Some administrative variables.
Definition at line 82 of file AbstractState.h.
◆ _fugacity_coefficient
|
protected |
Definition at line 126 of file AbstractState.h.
◆ _gas_constant
|
protected |
Universal gas constant [J/mol/K].
Definition at line 105 of file AbstractState.h.
◆ _gibbsmolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _gibbsmolar_excess
|
protected |
Definition at line 121 of file AbstractState.h.
◆ _gibbsmolar_residual
|
protected |
Definition at line 118 of file AbstractState.h.
◆ _helmholtzmolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _helmholtzmolar_excess
|
protected |
Definition at line 121 of file AbstractState.h.
◆ _hmolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _hmolar_excess
|
protected |
Excess properties.
Definition at line 121 of file AbstractState.h.
◆ _hmolar_residual
|
protected |
Residual properties.
Definition at line 118 of file AbstractState.h.
◆ _logp
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _logrhomolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _molar_mass
|
protected |
Molar mass [mol/kg].
Definition at line 102 of file AbstractState.h.
◆ _p
|
protected |
Definition at line 108 of file AbstractState.h.
◆ _phase
|
protected |
The key for the phase from CoolProp::phases enum.
Definition at line 83 of file AbstractState.h.
◆ _pLanc
|
protected |
Definition at line 124 of file AbstractState.h.
◆ _pVanc
|
protected |
Definition at line 124 of file AbstractState.h.
◆ _Q
|
protected |
Definition at line 108 of file AbstractState.h.
◆ _R
|
protected |
Definition at line 108 of file AbstractState.h.
◆ _reducing
|
protected |
Definition at line 99 of file AbstractState.h.
◆ _rho_spline
|
protected |
Smoothing values.
Definition at line 129 of file AbstractState.h.
◆ _rhoLanc
|
protected |
Ancillary values.
Definition at line 124 of file AbstractState.h.
◆ _rhoLmolar
|
protected |
Two-Phase variables.
Definition at line 140 of file AbstractState.h.
◆ _rhomolar
|
protected |
Bulk values.
Definition at line 108 of file AbstractState.h.
◆ _rhoVanc
|
protected |
Definition at line 124 of file AbstractState.h.
◆ _rhoVmolar
|
protected |
Definition at line 140 of file AbstractState.h.
◆ _smolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _smolar_excess
|
protected |
Definition at line 121 of file AbstractState.h.
◆ _smolar_residual
|
protected |
Definition at line 118 of file AbstractState.h.
◆ _speed_sound
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _surface_tension
|
protected |
Definition at line 113 of file AbstractState.h.
◆ _T
|
protected |
Definition at line 108 of file AbstractState.h.
◆ _tau
|
protected |
Definition at line 110 of file AbstractState.h.
◆ _TLanc
|
protected |
Definition at line 124 of file AbstractState.h.
◆ _TVanc
|
protected |
Definition at line 124 of file AbstractState.h.
◆ _umolar
|
protected |
Definition at line 115 of file AbstractState.h.
◆ _umolar_excess
|
protected |
Definition at line 121 of file AbstractState.h.
◆ _viscosity
|
protected |
Transport properties.
Definition at line 113 of file AbstractState.h.
◆ _volumemolar_excess
|
protected |
Definition at line 121 of file AbstractState.h.
◆ imposed_phase_index
|
protected |
If the phase is imposed, the imposed phase index.
Definition at line 84 of file AbstractState.h.
The documentation for this class was generated from the following files:
- include/AbstractState.h
- src/AbstractState.cpp
