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AVEVA™ Process Simulation

Equations for the SRKH method

  • Last UpdatedAug 21, 2025
  • 2 minute read

The general equation relating excess Gibbs free energy to fugacity coefficients is given by:

SRKH - Equation for the Excess Gibbs Free Energy

where

gE is the excess Gibbs free energy per mole

f is the fugacity coefficient of the mixture

fi is the fugacity coefficient of component i

We calculate the excess Gibbs free energy at infinite pressure by using the Redlich-Kwong equation of state (EOS) and the linear mixing rules for the parameter b from the general cubic EOS. At infinite pressure, the preceding equation becomes:

SRKH - Equation for the Excess Gibbs Free Energy at Infinite Dilution

where

gE is the excess Gibbs free energy at infinite pressure

We can rewrite this equation to produce a new mixing rule for parameter a from the general cubic EOS:

SRKH - Mixing Rule for Parameter a Based on Excess Gibbs Free Energy at Infinite Dilution

We can then use any liquid activity coefficient (LACT) method to calculate the excess Gibbs free energy. Huron and Vidal chose to use the NRTL method to calculate the excess Gibbs free energy.

SRKH - NRTL Equation for the Excess Gibbs Free Energy at Infinite Dilution

SRKH - NRTL Equation for c-sub(ij) at Infinite Dilution

SRKH - NRTL Equation for G-sub(ji) at Infinite Dilution

where

gji and gii are experimentally determined parameters taken from the SRKH data bank

The only difference between the classical Non-Random Two-Liquid (NRTL) equation and the preceding equation is the definition of the local composition as corrected volume fractions, which leads to the introduction of the volume parameter bj in the calculation of Gji. Substituting for the excess Gibbs free energy in the preceding equation yields:

SRKH - Equation for Parameter a with Substituted NRTL Excess Gibbs Free Energy at Infinite Dilution

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