Same as SimpleNaturalGas but with fixed composition
Extends from SimpleNaturalGas (Simple natural gas mix with 6 components).
Name | Description |
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Inherited | |
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Thermodynamic state variables |
data={Common.SingleGasesData.CH4,Common.SingleGasesData.C2H6,Common.SingleGasesData.C3H8,Common.SingleGasesData.C4H10_n_butane,Common.SingleGasesData.N2,Common.SingleGasesData.CO2} | Data records of ideal gas substances |
excludeEnthalpyOfFormation=true | If true, enthalpy of formation Hf is not included in specific enthalpy h |
referenceChoice=ReferenceEnthalpy.ZeroAt0K | Choice of reference enthalpy |
h_offset=0.0 | User defined offset for reference enthalpy, if referenceChoice = UserDefined |
MMX=data[:].MM | Molar masses of components |
methodForThermalConductivity=1 | |
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Base properties (p, d, T, h, u, R_s, MM, X, and Xi of NASA mixture gas |
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Return thermodynamic state as function of p, T and composition X |
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Return thermodynamic state as function of p, h and composition X |
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Return thermodynamic state as function of p, s and composition X |
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Return thermodynamic state as function of d, T and composition X |
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Return thermodynamic state so that it smoothly approximates: if x > 0 then state_a else state_b |
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Return pressure of ideal gas |
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Return temperature of ideal gas |
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Return density of ideal gas |
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Return specific enthalpy |
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Return specific internal energy |
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Return specific entropy |
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Return specific Gibbs energy |
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Return specific Helmholtz energy |
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Return specific enthalpy |
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Return specific enthalpy derivative |
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Return gasConstant |
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Return specific heat capacity at constant pressure |
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Return specific heat capacity at constant volume from temperature and gas data |
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Return mixing entropy of ideal gases / R |
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Return temperature dependent part of the entropy, expects full entropy vector |
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Return isentropic exponent |
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Return velocity of sound |
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Approximate method of calculating h_is from upstream properties and downstream pressure |
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Return isentropic enthalpy |
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Return viscosities of gas mixtures at low pressures (Wilke method) |
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Return mixture dynamic viscosity |
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Return the viscosity of gas mixtures without access to component viscosities (Chung, et. al. rules) |
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Return thermal conductivities of low-pressure gas mixtures (Mason and Saxena Modification) |
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Return thermal conductivity for low pressure gas mixtures |
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Return isobaric expansion coefficient beta |
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Return isothermal compressibility factor |
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Return density derivative by pressure at constant temperature |
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Return density derivative by temperature at constant pressure |
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Return density derivative by mass fraction |
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Return molar mass of mixture |
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Return temperature from specific enthalpy and mass fraction |
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Return temperature from pressure, specific entropy and mass fraction |
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Return specific entropy from pressure, temperature and mass fractions |
fluidConstants={Common.FluidData.CH4,Common.FluidData.C2H6,Common.FluidData.C3H8,Common.FluidData.C4H10_n_butane,Common.FluidData.N2,Common.FluidData.CO2} | Constant data for the fluid |
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Return mass fractions X from mole fractions |
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Return mole fractions from mass fractions X |
ThermoStates=Modelica.Media.Interfaces.Choices.IndependentVariables.pTX | Enumeration type for independent variables |
mediumName="SimpleNaturalGas" | Name of the medium |
substanceNames={"Methane","Ethane","Propane","N-Butane,","Nitrogen","Carbondioxide"} | Names of the mixture substances. Set substanceNames={mediumName} if only one substance. |
extraPropertiesNames=fill("", 0) | Names of the additional (extra) transported properties. Set extraPropertiesNames=fill("",0) if unused |
singleState=false | = true, if u and d are not a function of pressure |
reducedX=false | = true if medium contains the equation sum(X) = 1.0; set reducedX=true if only one substance (see docu for details) |
fixedX=true | = true if medium contains the equation X = reference_X |
reference_p=101325 | Reference pressure of Medium: default 1 atmosphere |
reference_T=298.15 | Reference temperature of Medium: default 25 deg Celsius |
reference_X={0.92,0.048,0.005,0.002,0.015,0.01} | Default mass fractions of medium |
p_default=101325 | Default value for pressure of medium (for initialization) |
T_default=Modelica.Units.Conversions.from_degC(20) | Default value for temperature of medium (for initialization) |
h_default=specificEnthalpy_pTX(p_default, T_default, X_default) | Default value for specific enthalpy of medium (for initialization) |
X_default=reference_X | Default value for mass fractions of medium (for initialization) |
C_default=fill(0, nC) | Default value for trace substances of medium (for initialization) |
nS=size(substanceNames, 1) | Number of substances |
nX=nS | Number of mass fractions |
nXi=if fixedX then 0 else if reducedX then nS - 1 else nS | Number of structurally independent mass fractions (see docu for details) |
nC=size(extraPropertiesNames, 1) | Number of extra (outside of standard mass-balance) transported properties |
C_nominal=1.0e-6*ones(nC) | Default for the nominal values for the extra properties |
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Critical, triple, molecular and other standard data of fluid |
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Return the Prandtl number |
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Alias for deprecated name |
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Alias for deprecated name |
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Alias for isobaricExpansionCoefficient for user convenience |
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Alias of isothermalCompressibility for user convenience |
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Return density derivative w.r.t. pressure at const specific enthalpy |
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Return density derivative w.r.t. specific enthalpy at constant pressure |
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Return specific enthalpy from p, T, and X or Xi |
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Return specific enthalpy from p, T, and X or Xi |
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Return density from p, T, and X or Xi |
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Return temperature from p, h, and X or Xi |
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Return density from p, h, and X or Xi |
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Return temperature from p,s, and X or Xi |
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Return density from p, s, and X or Xi |
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Return specific enthalpy from p, s, and X or Xi |
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Type for mass flow rate with medium specific attributes |
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Type for absolute pressure with medium specific attributes |
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Type for density with medium specific attributes |
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Type for dynamic viscosity with medium specific attributes |
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Type for enthalpy flow rate with medium specific attributes |
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Type for mass fraction with medium specific attributes |
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Type for mole fraction with medium specific attributes |
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Type for molar mass with medium specific attributes |
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Type for molar volume with medium specific attributes |
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Type for isentropic exponent with medium specific attributes |
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Type for specific energy with medium specific attributes |
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Type for specific internal energy with medium specific attributes |
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Type for specific enthalpy with medium specific attributes |
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Type for specific entropy with medium specific attributes |
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Type for specific heat capacity with medium specific attributes |
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Type for surface tension with medium specific attributes |
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Type for temperature with medium specific attributes |
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Type for thermal conductivity with medium specific attributes |
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Type for Prandtl number with medium specific attributes |
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Type for velocity of sound with medium specific attributes |
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Type for unspecified, mass-specific property transported by flow |
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Type for conserved integral of unspecified, mass specific property |
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Type for flow rate of unspecified, mass-specific property |
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Type for isobaric expansion coefficient with medium specific attributes |
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Type for dipole moment with medium specific attributes |
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Type for partial derivative of density with respect to pressure with medium specific attributes |
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Type for partial derivative of density with respect to enthalpy with medium specific attributes |
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Type for partial derivative of enthalpy with respect to pressure with medium specific attributes |
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Type for partial derivative of density with respect to temperature with medium specific attributes |
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Type for partial derivative of temperature with respect to pressure with medium specific attributes |
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Saturation properties of two phase medium |
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Validity limits for fluid model |
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Phase of the fluid: 1 for 1-phase, 2 for two-phase, 0 for not known, e.g., interactive use |
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The most basic version of a record used in several degrees of detail |
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The ideal gas version of a record used in several degrees of detail |
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The two phase fluid version of a record used in several degrees of detail |