Editing Fully anisotropic rigid molecules

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The fivefold dependence of the pair functions, <math>\Phi(12)=\Phi(r_{12},\theta_1, \theta_2, \phi_{12}, \chi_1, \chi_2)</math>, for liquids of rigid, fully anisotropic molecules makes these equations excessively complex for numerical work <ref>[http://dx.doi.org/10.1063/1.469615 F. Lado, E. Lomba and M. Lombardero "Integral equation algorithm for fluids of fully anisotropic molecules", Journal of Chemical Physics '''103''' pp. 481-484 (1995)]</ref>.
The fivefold dependence of the pair functions, <math>\Phi(12)=\Phi(r_{12},\theta_1, \theta_2, \phi_{12}, \chi_1, \chi_2)</math>, for liquids of rigid, fully anisotropic molecules makes these equations excessively complex for numerical work (see  Ref. 1).
The first and essential ingredient for their reduction is a spherical harmonic
The first and essential ingredient for their reduction is a spherical harmonic
expansion of the correlation functions,  
expansion of the correlation functions,  
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<math>\Phi_{l_1 l_2 m}^{00}(r_{12})</math> for linear molecules.
<math>\Phi_{l_1 l_2 m}^{00}(r_{12})</math> for linear molecules.
==References==
==References==
<references/>
#[http://dx.doi.org/10.1063/1.469615 F. Lado, E. Lomba and M. Lombardero "Integral equation algorithm for fluids of fully anisotropic molecules", Journal of Chemical Physics '''103''' pp. 481-484 (1995)]
;Related reading
*[http://dx.doi.org/10.1063/1.3693623 R. Ishizuka and N. Yoshida "Application of efficient algorithm for solving six-dimensional molecular Ornstein-Zernike equation", Journal of Chemical Physics '''136''' 114106 (2012)]
[[category: integral equations]]
[[category: integral equations]]
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