| Name | Description |
|---|---|
| liqViscPcorLucas | Lucas liquid viscosity pressure correction. |
| liqThCondLatini | |
| liqSurfTensSastriRao | |
| BaseProperties | |
| ThermodynamicState | |
| setState_pTX | Return ThermodynamicState record as function of p,T and composition X or Xi |
| setState_dTX | Return ThermodynamicState record as function of T,d and composition X or Xi |
| setState_phX | Return ThermodynamicState record as function of p,H and composition X or Xi |
| setState_psX | Return thermodynamic state as function of p, s and composition X or Xi |
| pressure | Return pressure |
| temperature | Return temperature |
| density | Return density |
| density_derp_T | Return density derivative w.r.t. pressure at const temperature. OK |
| density_derT_p | Return density derivative w.r.t. temperature at constant pressure. OK |
| density_derp_h | Return density derivative w.r.t. pressure at const specific enthalpy. Numerical derivative in two phases differs from HelmholtzMedia, but is similar to ExternalMedia |
| density_derh_p | Return density derivative w.r.t. specific enthalpy at constant pressure. OK |
| specificEnthalpy | Return specific enthalpy |
| specificInternalEnergy | Return specific internal energy |
| specificEntropy | Return specific entropy |
| specificGibbsEnergy | Return specific Gibbs energy |
| specificHelmholtzEnergy | Return specific Helmholtz energy |
| specificHeatCapacityCp | Return specific heat capacity at constant pressure. OK |
| specificHeatCapacityCv | Return heat capacity at constant volume |
| isentropicExponent | Return isentropic exponent |
| isobaricExpansionCoefficient | Returns the approximate isobaric expansion coefficient beta=dV_dT/V |
| isothermalCompressibility | Returns overall the isothermal compressibility factor |
| velocityOfSound | Return velocity of sound |
| jouleThomsonCoefficient | |
| dynamicViscosity | Return dynamic viscosity |
| thermalConductivity | Return thermal conductivity |
| molarMass | Return the molar mass of the medium |
| surfaceTension | Return surface tension |
| setSmoothState | Return thermodynamic state so that it smoothly approximates: if x > 0 then state_a else state_b |
| density_pT | |
| density_pT_state | |
| specificEnthalpy_pT | |
| specificEnthalpy_pT_state | |
| density_pT_der | |
| specificEnthalpy_pT_der | |
| density_ph | |
| density_ph_state | |
| temperature_ph | |
| temperature_ph_state | |
| density_ph_der | |
| temperature_ph_der | |
| pressure_dT | |
| pressure_dT_state | |
| specificEnthalpy_dT | |
| specificEnthalpy_dT_state | |
| pressure_dT_der | |
| pressure_derd_T | pressure derivative w.r.t. density at constant T. OK |
| pressure_derT_d | pressure derivative w.r.t. T at constant density. OK |
| specifiEnthalpy_dT_der | |
| specificEnthalpy_derd_T | pressure derivative w.r.t. density at constant T. OK, but it seems clear that beta and kappa are bad calculated for the gas |
| specificEnthalpy_derT_d | pressure derivative w.r.t. density at constant T. To be finished analyticaly for two phases |