.AixLib.Media.AirIncompressible

Information

This medium package models moist air using a gas law in which pressure and temperature are independent, which often leads to significantly faster and more robust computations. Additionally, the density is constant to improve the simulation stability and speed.

This medium uses the gas law

ρ = ρstp,

where pstd is a constant reference density.


The medium model can be used for air duct simulations, where the pressures and temperatures are close to the reference values.


Note that models in this package implement the equation for the internal energy as

u = h - pstp ⁄ ρstp,

where u is the internal energy per unit mass, h is the enthalpy per unit mass, pstp is the static pressure and ρstp is the mass density at standard pressure and temperature. The reason for this implementation is that in general,

h = u + p v,

from which follows that

u = h - p v = h - p ⁄ ρ = h - pstp ⁄ ρstd,

because p ⁄ ρ = pstp ⁄ ρstp in this medium model.

The enthalpy is computed using the convention that h=0 if T=0 °C and no water vapor is present.

Contents

NameDescription
 ThermodynamicStateThermodynamicState record for moist air
 BasePropertiesBase properties
 densityGas density
 dynamicViscosityReturn the dynamic viscosity of dry air
 enthalpyOfCondensingGasEnthalpy of steam per unit mass of steam
 enthalpyOfGasEnthalpy of gas mixture per unit mass of gas mixture
 enthalpyOfLiquidEnthalpy of liquid (per unit mass of liquid) which is linear in the temperature
 enthalpyOfNonCondensingGasEnthalpy of non-condensing gas per unit mass of steam
 enthalpyOfVaporizationEnthalpy of vaporization of water
 gasConstantReturn ideal gas constant as a function from thermodynamic state, only valid for phi<1
 pressureReturns pressure of ideal gas as a function of the thermodynamic state record
 isobaricExpansionCoefficientIsobaric expansion coefficient beta
 isothermalCompressibilityIsothermal compressibility factor
 saturationPressureSaturation curve valid for 223.16 <= T <= 373.16 (and slightly outside with less accuracy)
 specificEntropyReturn the specific entropy, only valid for phi<1
 density_derp_TReturn the partial derivative of density with respect to pressure at constant temperature
 density_derT_pReturn the partial derivative of density with respect to temperature at constant pressure
 density_derXReturn the partial derivative of density with respect to mass fractions at constant pressure and temperature
 specificHeatCapacityCpSpecific heat capacity of gas mixture at constant pressure
 specificHeatCapacityCvSpecific heat capacity of gas mixture at constant volume
 setState_dTXReturn thermodynamic state as function of density d, temperature T and composition X
 setState_phXReturn thermodynamic state as function of pressure p, specific enthalpy h and composition X
 setState_pTXReturn thermodynamic state as function of p, T and composition X or Xi
 setState_psXReturn the thermodynamic state as function of p, s and composition X or Xi
 specificEnthalpyCompute specific enthalpy from pressure, temperature and mass fraction
 specificEnthalpy_pTXSpecific enthalpy
 specificGibbsEnergySpecific Gibbs energy
 specificHelmholtzEnergySpecific Helmholtz energy
 isentropicEnthalpyReturn the isentropic enthalpy
 specificInternalEnergySpecific internal energy
 temperatureReturn temperature of ideal gas as a function of the thermodynamic state record
 molarMassReturn the molar mass
 temperature_phXCompute temperature from specific enthalpy and mass fraction
 thermalConductivityThermal conductivity of dry air as a polynomial in the temperature

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