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Thermodynamic functions as correlation-function integrals.

K Koga1, B Widom

  • 1Department of Chemistry, Faculty of Science, Okayama University, Okayama 700-8530, Japan. koga@okayama-u.ac.jp

The Journal of Chemical Physics
|March 29, 2013
PubMed
Summary
This summary is machine-generated.

Thermodynamic functions can be expressed using correlation-function integrals. The choice of molecular centers is arbitrary, but these integrals remain independent of the choice, as shown for hard spheres and propane.

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Area of Science:

  • Thermodynamics
  • Statistical Mechanics
  • Physical Chemistry

Background:

  • Thermodynamic functions are often expressed as correlation-function integrals.
  • Key integrals include Ornstein-Zernike, Kirkwood-Buff, and virial coefficient formulas.
  • The choice of molecular centers for distance measurement is arbitrary.

Purpose of the Study:

  • To recall expressions of thermodynamic functions as correlation-function integrals.
  • To highlight the independence of these integrals from the arbitrary choice of molecular centers.
  • To illustrate this principle with specific examples.

Main Methods:

  • Recalling established integral expressions for thermodynamic functions.
  • Analyzing the impact of arbitrary molecular center choices on correlation functions.
  • Illustrating with calculations for hard spheres and propane.
  • Utilizing computer simulations for pair correlations in water and aqueous solutions.

Main Results:

  • Correlation-function integrals for thermodynamic properties are independent of the chosen molecular centers.
  • This independence was demonstrated for hard spheres in 1D, 2D, and 3D.
  • The principle was also shown for gaseous propane and simulated water systems.

Conclusions:

  • The arbitrariness of molecular center selection does not affect the resulting thermodynamic integrals.
  • This confirms the robustness of correlation-function integral methods in thermodynamics.
  • The findings are validated across different dimensions and molecular systems.