In general, both the naming and the abbreviations follow the guidelines presented in the media package of the Modelica standard library. However, adaptions are made for functions and variables related to the Helmholtz equation of state. These adaptions are presented below.
The naming of the models follows the guideline presented below:
Refrigerant _ Reference Point _ Range of validity for pressure _ Range of validity for temperature _ Approach of calculating fitted formulas
Some special abbreviations are introduced for functions and variables related to the Helmholtz energy equation of state. Some examples are given below:
Expression |
Abbreviation |
Comment |
alpha_0 |
f_Idg |
Helmholtz energy of ideal gas |
alpha_r |
f_Res |
Helmholtz energy of residual gas |
tau * d(alpha_0)/(dtau)_delta=const. |
t_fIdg_t |
Partial derivative of f_Idg with respect to tau |
tau*tau * dd(alpha_0)/(dtau*dtau)_delta=const. |
tt_fIdg_tt |
Partial derivative of f_Idg with respect to tau*tau |
tau*delta * dd(alpha_r)/(dtau*ddelta) |
td_fRes_td |
Partial derivative of f_Res with respect to tau*delta |
Some special abbreviations are introduced for partial derivatives. Some examples are given below:
Expression |
Abbreviation |
Comment |
d(d)/(dp)_h=const. |
ddph |
Partial derivative of density with respect to pressure at constant specific enthalpy |
d(T)/(ds)_p=const. |
dTsp |
Partial derivative of temperature with respect to specific entropy and constant pressure |
d(Tsat)/(dp) |
dTp |
Partial derivative of saturation temperature with respect to pressure |
d(dl)/(dp) |
ddldp |
Partial derivative of bubble density with respect to pressure |
d(dv)/(dp) |
ddvdp |
Partial derivative of dew density with respect to pressure |