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 |