.ThermofluidStream.Media.additionalMedia.SingleGasAndIncompressible.PartialSingleGasAndIncompressible

SingleGases medium combined with Incompressible medium

Information

Gas medium combined with incompressible medium. Only the parameters to PartialMedium  and selection of SingleGases and Incompressible are incomplete. 

Observe that this implementation only works for Incompressible with one substance .

It is assumed that the gas and the liquid do not interact. This is a simplification since many substances mix , e. g. water and air where there is air molecules mixed into the liquid water and water steam mixed in the air.

To calculate the media properties a linear interpolation based on the mass-fractions between the gas and liquid is performed. Depending on the chosen property this may be more or less meaningful. Whenever possible,

one shall therefore use the properties of gas and liquid directly. Compare e.g. with a typical refrigerant, where many of the properties are only defined in the one-phase regions.

The intended use for this media is in systems where the properties of the mix of the media is not very important to get absolutely correct, but where both of the substances of the mix can occur at any physical location

in the system, but then mostly in pure or nearly pure form.

Contents

Name Description
 SingleGas SingleGas choice
 Incompressible Incompressible choice
 ThermodynamicState
 BaseProperties Base properties (p, d, T, h, u, R_s, MM, and X of Incompressible mixed with SingleGases
 setState_pTX set the thermodynamic state record from p, T, X
 setState_phX
 T_hX
 h_TX
 pressure Return the pressure from the thermodynamic state
 isentropicExponent Return the isentropic exponent
 temperature Return the temperature from the thermodynamicstate
 massFraction Return the massfraction from the thermodynamic state
 density Return the density from the thermodynamic state
 d_pT_Incompressible
 specificEnthalpy Return the specific enthalpy from the thermodynamic state
 specificEntropy Return the specific entropy from the thermodynamic state, total mixing assumed
 specificInternalEnergy Return the specific internal energy from the thermodynamic state
 specificGibbsEnergy Return specific Gibbs energy from the thermodynamic state
 specificHelmholtzEnergy Return specific Helmholtz energy from thermodynamic state
 specificHeatCapacityCp Return specific heat capacity at constant pressure
 specificHeatCapacityCv Return specific heat capacity at constant volume
 dynamicViscosity Return dynamic viscosity from the thermodynamic state
 thermalConductivity Return thermal conductivity from thermodynamic state
 molarMass Return molar mass from the thermodynamic state

Revisions

Author: Ingela Lind, M Sc, Ph D, Technical Fellow, Simulation and Thermal Analysis, Vehicle Systems, SAAB Aerosystems, 2024


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