Name | Description |
---|---|
Lucas liquid viscosity pressure correction. | |
Return ThermodynamicState record as function of p,T and composition X or Xi | |
Return ThermodynamicState record as function of T,d and composition X or Xi | |
Return ThermodynamicState record as function of p,H and composition X or Xi | |
Return thermodynamic state as function of p, s and composition X or Xi | |
Return pressure | |
Return temperature | |
Return density | |
Return density derivative w.r.t. pressure at const temperature. OK | |
Return density derivative w.r.t. temperature at constant pressure. OK | |
Return density derivative w.r.t. pressure at const specific enthalpy. Numerical derivative in two phases differs from HelmholtzMedia, but is similar to ExternalMedia | |
Return density derivative w.r.t. specific enthalpy at constant pressure. OK | |
Return specific enthalpy | |
Return specific internal energy | |
Return specific entropy | |
Return specific Gibbs energy | |
Return specific Helmholtz energy | |
Return specific heat capacity at constant pressure. OK | |
Return heat capacity at constant volume | |
Return isentropic exponent | |
Returns the approximate isobaric expansion coefficient beta=dV_dT/V | |
Returns overall the isothermal compressibility factor | |
Return velocity of sound | |
Return dynamic viscosity | |
Return thermal conductivity | |
Return the molar mass of the medium | |
Return surface tension | |
Return thermodynamic state so that it smoothly approximates: if x > 0 then state_a else state_b | |
pressure derivative w.r.t. density at constant T. OK | |
pressure derivative w.r.t. T at constant density. OK | |
pressure derivative w.r.t. density at constant T. OK, but it seems clear that beta and kappa are bad calculated for the gas | |
pressure derivative w.r.t. density at constant T. To be finished analyticaly for two phases |