Vapor Entropy

Entropy is a state function, that is, its value does not depend on the past history of the system. The entropy change for an infinitesimal reversible process is given by:

 

  image\THRM06.gif

 

where: dS = change in entropy 

image\THRM07.gif = heat absorbed from surroundings in a reversible process

T = system temperature 

 

Most processes are not truly reversible and there is a net change in entropy when going from one state to the next. Entropy can be visualized as a measure of the disorder of a system. At equilibrium, the entropy of a system is at its minimum value.

 

Entropies for both liquids and vapors in PRO/II are computed as functions of the enthalpies using an equation of state or generalized correlation. They are used for isentropic calculations involving compressors and expanders and for free energy minimization reactors.

 

Available methods for calculating vapor entropy are listed below. Refer "Entropy" under "Basic Principles" in Volume 1, Chapter 2 of  the PRO/II Reference Manual for more information on entropies.

 

Curl-Pitzer

PR-Panag.-Reid

Lee-Kesler

PR-Modified Panag.-Reid

Soave-Redlich-Kwong

BWRS

SRK-Kabadi-Danner

Lee-Kesler-Plocker

SRK-Huron-Vidal

UNIWAALS

SRK-Panag.-Reid

Glycol

SRK-Modified Panag.-Reid

Hayden O'Connell

SRK-SimSci

Truncated Virial

SRK-Hexamer

User-added Methods

Peng Robinson

SAFT

PR-Huron-Vidal

PHSC

Predictive Peng-Robinson78