packageAir_Base
Extends from Modelica.Media.Interfaces.PartialPureSubstance (Base class for pure substances of one chemical substance).
Information
This model calculates medium properties for air in the liquid, gas and two phase regions. Three variable pairs can be the independent variables of the model:
- Pressure p and specific enthalpy h are the most natural choice for general applications. This is the recommended choice for most general purpose applications.
- Pressure p and temperature T are the most natural choice for applications where air is always in the same phase (liquid or gas).
- Density d and temperature T are explicit variables of the Helmholtz function in the near-critical region and can be the best choice for applications with super-critical or near-critical states.
The following quantities are always computed:
| Variable | Unit | Description |
| T | K | temperature |
| u | J/kg | specific internal energy |
| d | kg/m^3 | density |
| p | Pa | pressure |
| h | J/kg | specific enthalpy |
In some cases additional medium properties are needed. A component that needs these optional properties has to call one of the functions listed in Modelica.Media.UsersGuide.MediumUsage.OptionalProperties and in Modelica.Media.UsersGuide.MediumUsage.TwoPhase.
Many further properties can be computed. Using the well-known Bridgman's Tables, all first partial derivatives of the standard thermodynamic variables can be computed easily.
Parameters
| Type | Name | Default | Description |
|---|---|---|---|
| Modelica.Media.Interfaces.Choices.IndependentVariables | ThermoStates (from PartialMedium) | Enumeration type for independent variables | |
| String | mediumName (from PartialMedium) | "unusablePartialMedium" | Name of the medium |
| String[:] | substanceNames (from PartialMedium) | {mediumName} | Names of the mixture substances. Set substanceNames={mediumName} if only one substance. |
| String[:] | extraPropertiesNames (from PartialMedium) | fill("", 0) | Names of the additional (extra) transported properties. Set extraPropertiesNames=fill("",0) if unused |
| Boolean | singleState (from PartialMedium) | = true, if u and d are not a function of pressure | |
| Boolean | reducedX (from PartialMedium) | true | = true, if medium contains the equation sum(X) = 1.0; set reducedX=true, if only one substance (see docu for details) |
| Boolean | fixedX (from PartialMedium) | false | = true, if medium contains the equation X = reference_X |
| AbsolutePressure | reference_p (from PartialMedium) | 101325 | Reference pressure of Medium: default 1 atmosphere |
| Temperature | reference_T (from PartialMedium) | 298.15 | Reference temperature of Medium: default 25 deg Celsius |
| MassFraction[nX] | reference_X (from PartialMedium) | fill(1/nX, nX) | Default mass fractions of medium |
| AbsolutePressure | p_default (from PartialMedium) | 101325 | Default value for pressure of medium (for initialization) |
| Temperature | T_default (from PartialMedium) | Modelica.Units.Conversions.from_degC(20) | Default value for temperature of medium (for initialization) |
| SpecificEnthalpy | h_default (from PartialMedium) | specificEnthalpy_pTX(p_default, T_default, X_default) | Default value for specific enthalpy of medium (for initialization) |
| MassFraction[nX] | X_default (from PartialMedium) | reference_X | Default value for mass fractions of medium (for initialization) |
| ExtraProperty[nC] | C_default (from PartialMedium) | fill(0, nC) | Default value for trace substances of medium (for initialization) |
| Integer | nS (from PartialMedium) | size(substanceNames, 1) | Number of substances |
| Integer | nX (from PartialMedium) | nS | Number of mass fractions |
| Integer | nXi (from PartialMedium) | if fixedX then 0 else if reducedX then nS - 1 else nS | Number of structurally independent mass fractions (see docu for details) |
| Integer | nC (from PartialMedium) | size(extraPropertiesNames, 1) | Number of extra (outside of standard mass-balance) transported properties |
| Real[nC] | C_nominal (from PartialMedium) | 1.0e-6*ones(nC) | Default for the nominal values for the extra properties |
| Boolean | ph_explicit | True if explicit in pressure and specific enthalpy | |
| Boolean | dT_explicit | True if explicit in density and temperature | |
| Boolean | pT_explicit | True if explicit in pressure and temperature |
Contents
| Name | Description |
|---|---|
| Thermodynamic state | |
| Base properties of air | |
| Computes density as a function of pressure and specific enthalpy | |
| Computes temperature as a function of pressure and specific enthalpy | |
| Compute temperature from pressure and specific enthalpy | |
| Computes density as a function of pressure and specific enthalpy | |
| Computes pressure as a function of density and temperature | |
| Computes specific enthalpy as a function of density and temperature | |
| Computes specific enthalpy as a function of pressure and temperature | |
| Computes specific enthalpy as a function of pressure and temperature | |
| Computes density as a function of pressure and temperature | |
| Return dynamic viscosity as a function of the thermodynamic state record | |
| Thermal conductivity of air | |
| Return pressure of ideal gas | |
| Return temperature of ideal gas | |
| Return density of ideal gas | |
| Return specific enthalpy | |
| Return specific internal energy | |
| Return specific Gibbs energy | |
| Return specific Helmholtz energy | |
| Specific entropy of air | |
| Specific heat capacity at constant pressure of air | |
| Specific heat capacity at constant volume of air | |
| Return isentropic exponent | |
| Isothermal compressibility of air | |
| Isobaric expansion coefficient of air | |
| Return velocity of sound as a function of the thermodynamic state record | |
| Density derivative by specific enthalpy | |
| Density derivative by pressure | |
| Return thermodynamic state of air as function of d and T | |
| Return thermodynamic state of air as function of p and h | |
| Return thermodynamic state of air as function of p and s | |
| Return thermodynamic state of air as function of p and T | |
| Return thermodynamic state so that it smoothly approximates: if x > 0 then state_a else state_b | |
| Return the molar mass of the medium |