Wertheim's first order thermodynamic perturbation theory (TPT1): Difference between revisions

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Wertheim's first order thermodynamic perturbation theory (TPT1) <ref>[http://dx.doi.org/10.1007/BF01017362 M. S. Wertheim "Fluids with highly directional attractive forces. I. Statistical thermodynamics" Journal of Statistical Physics '''35''' pp. 19-34 (1984)]</ref>
<ref>[http://dx.doi.org/10.1007/BF01017363 M. S. Wertheim "Fluids with highly directional attractive forces. II. Thermodynamic perturbation theory and integral equations" Journal of Statistical Physics '''35''' pp. 35-47 (1984)]</ref>
<ref>[http://dx.doi.org/10.1007/BF01127721 M. S. Wertheim "Fluids with highly directional attractive forces. III. Multiple attraction sites" Journal of Statistical Physics '''42''' pp. 459-476 (1986)]</ref>
<ref>[http://dx.doi.org/10.1007/BF01127722 M. S. Wertheim "Fluids with highly directional attractive forces. IV. Equilibrium polymerization" Journal of Statistical Physics '''42''' pp. 477-492 (1986)]</ref>
<ref>[http://dx.doi.org/10.1063/1.453326  M. S. Wertheim "Thermodynamic perturbation theory of polymerization", Journal of Chemical Physics '''87''' pp. 7323-7331 (1987)]</ref>
can be expressed as:
:<math>Z_{\rm TPT1} = \frac{p}{\rho k_BT}= mZ_{\rm monomer}- (m-1)\left( 1 + \rho_{\rm monomer}\frac{\partial \ln {\rm g}(\sigma)}{\partial \rho_{\rm monomer}}\right)</math>
where <math>Z_{\rm monomer}</math> is the [[equations of state | equation of state]] of the monomer system and ''m'' is the number of monomers in the chains.
For example, in the study of the [[Flexible hard sphere chains | flexible hard sphere chain]] model one can use the
[[Carnahan-Starling equation of state]] for <math>Z_{\rm monomer}</math>, leading to
:<math>
Z_{\rm FHSC} = m \frac{ 1 + \eta + \eta^2 - \eta^3 }{(1-\eta)^3 } - (m-1) \frac{1+\eta-( \eta^2/2)}{(1-\eta)(1-\eta/2)}= 1+ m \frac{ 4\eta -2 \eta^2 }{(1-\eta)^3 } - (m-1) \frac{5\eta-2 \eta^2}{(1-\eta)(2-\eta)}
</math>
==See also==
*[[SAFT]]
==References==
==References==
#[http://dx.doi.org/10.1007/BF01017362 M. S. Wertheim "Fluids with highly directional attractive forces. I. Statistical thermodynamics" Journal of Statistical Physics '''35''' pp. 19-34 (1984)]
<references/>
#[http://dx.doi.org/10.1007/BF01017363 M. S. Wertheim "Fluids with highly directional attractive forces. II. Thermodynamic perturbation theory and integral equations" Journal of Statistical Physics '''35''' pp. 35-47 (1984)]
;Related reading
#[http://dx.doi.org/10.1007/BF01127721 M. S. Wertheim "Fluids with highly directional attractive forces. III. Multiple attraction sites" Journal of Statistical Physics '''42''' pp. 459-476 (1986)]
*[http://dx.doi.org/10.1063/1.4947023 Bennett D. Marshall "Dual chain perturbation theory: A new equation of state for polyatomic molecules", Journal of Chemical Physics '''144''' 164104 (2016)]
#[http://dx.doi.org/10.1007/BF01127722 M. S. Wertheim "Fluids with highly directional attractive forces. IV. Equilibrium polymerization" Journal of Statistical Physics '''42''' pp. 477-492 (1986)]
 
#[http://dx.doi.org/10.1063/1.453326 M. S. Wertheim "Thermodynamic perturbation theory of polymerization", Journal of Chemical Physics '''87''' pp. 7323-7331 (1987)]


[[category:perturbation theory]]
[[category:perturbation theory]]

Latest revision as of 23:15, 20 July 2016

Wertheim's first order thermodynamic perturbation theory (TPT1) [1] [2] [3] [4] [5] can be expressed as:

where is the equation of state of the monomer system and m is the number of monomers in the chains.

For example, in the study of the flexible hard sphere chain model one can use the Carnahan-Starling equation of state for , leading to

See also[edit]

References[edit]

  1. ↑ M. S. Wertheim "Fluids with highly directional attractive forces. I. Statistical thermodynamics" Journal of Statistical Physics 35 pp. 19-34 (1984)
  2. ↑ M. S. Wertheim "Fluids with highly directional attractive forces. II. Thermodynamic perturbation theory and integral equations" Journal of Statistical Physics 35 pp. 35-47 (1984)
  3. ↑ M. S. Wertheim "Fluids with highly directional attractive forces. III. Multiple attraction sites" Journal of Statistical Physics 42 pp. 459-476 (1986)
  4. ↑ M. S. Wertheim "Fluids with highly directional attractive forces. IV. Equilibrium polymerization" Journal of Statistical Physics 42 pp. 477-492 (1986)
  5. ↑ M. S. Wertheim "Thermodynamic perturbation theory of polymerization", Journal of Chemical Physics 87 pp. 7323-7331 (1987)
Related reading
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