Redlich-Kwong equation of state: Difference between revisions

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A modification of the the Redlich-Kwong equation of state was presented by Giorgio Soave in order to allow better representation of non-spherical molecules<ref>[http://dx.doi.org/10.1016/0009-2509(72)80096-4  Giorgio Soave "Equilibrium constants from a modified Redlich-Kwong equation of state", Chemical Engineering Science  '''27''' pp. 1197-1203 (1972)]</ref>.  In order to do this, the square root temperature dependence was replaced with a temperature dependent acentricity factor:
A modification of the the Redlich-Kwong equation of state was presented by Giorgio Soave in order to allow better representation of non-spherical molecules<ref>[http://dx.doi.org/10.1016/0009-2509(72)80096-4  Giorgio Soave "Equilibrium constants from a modified Redlich-Kwong equation of state", Chemical Engineering Science  '''27''' pp. 1197-1203 (1972)]</ref>.  In order to do this, the square root temperature dependence was replaced with a temperature dependent acentricity factor:


:<math>\alpha=\left(1+\left(0.48508+1.55171\omega-0.15613\omega^2\right)\left(1-\sqrt\frac{T}{T_c}\right)\right)^2 </math>
:<math>\alpha(T)=\left(1+\left(0.48508+1.55171\omega-0.15613\omega^2\right)\left(1-\sqrt\frac{T}{T_c}\right)\right)^2 </math>


where <math>T_c</math> is the critical temperature and <math>\omega</math> is the acentric factor for the gas.  This leads to an equation of state of the form:
where <math>T_c</math> is the critical temperature and <math>\omega</math> is the acentric factor for the gas.  This leads to an equation of state of the form:


:<math> \left[p+\frac{a\alpha}{v(v+b)}\right]\left(v-b\right)=RT</math>
:<math> \left[p+\frac{a\alpha(T)}{v(v+b)}\right]\left(v-b\right)=RT</math>


or equivalently:
or equivalently:


:<math> p=\frac{RT}{v-b}-\frac{a\alpha}{v(v+b)}</math>
:<math> p=\frac{RT}{v-b}-\frac{a\alpha(T)}{v(v+b)}</math>





Revision as of 02:59, 7 November 2011

The Redlich-Kwong equation of state is[1]:

[p+aT1/2v(v+b)](v−b)=RT

where

a=0.4278R2Tc2.5Pc

and

b=0.0867RTcPc

where p is the pressure, T is the temperature and R is the molar gas constant. Tc is the critical temperature and Pc is the pressure at the critical point.

Soave Modification

A modification of the the Redlich-Kwong equation of state was presented by Giorgio Soave in order to allow better representation of non-spherical molecules[2]. In order to do this, the square root temperature dependence was replaced with a temperature dependent acentricity factor:

α(T)=(1+(0.48508+1.55171ω−0.15613ω2)(1−TTc))2

where Tc is the critical temperature and ω is the acentric factor for the gas. This leads to an equation of state of the form:

[p+aα(T)v(v+b)](v−b)=RT

or equivalently:

p=RTv−b−aα(T)v(v+b)


References