Editing Reference hyper-netted chain

The '''reference hyper-netted chain''' (RHNC) is sometimes referred to as the modified-HNC (MHNC) (Ref. 1)
Rosenfeld and Ashcroft (1979) (Ref. 1) proposed the `anzatz of universality':
 "...the bridge functions.. ..constitute the same family of curves, irrespective of the assumed pair potential"
The basis of the method is to solve the modified [[HNC]] equation
(with inclusion of the one-parameter [[bridge function]]s
appropriate to [[hard sphere model | hard spheres]]), and determine the only free parameter <math>\eta</math>
(related to the hard-sphere diameter) by requiring [[thermodynamic consistency]].
Fred Lado  (Ref. 2) and Rosenfeld and Ashcroft (1979) (Ref. 3)
noticed that the [[Ornstein-Zernike relation]]  can always be written in the form
:<math>\gamma_{12} =  \rho \int_V (h_{13} - \gamma_{13}) h_{23} ~{\rm d}(3)</math>
In view of this a hybrid solution between the [[HNC| hyper-netted chain]]
approximation and the Malijevsky-Labik formula for hard spheres (Ref. 4 and 5)
was proposed. The philosophy of this method is that the  bridge functional of the
liquid is fairly similar to that of the hard sphere fluid.
(See also Ref.s 6 and 7)
The RHNC closure is given by (Eq. 17 Ref. 7)
:<math> c\left(r\right) = h(r) - \ln [g(r) e^{\beta \Phi(r)}] + B_0(r) </math>
along with the constraint (Eq. 18 Ref. 7)
:<math>\rho \int [g(r) - g_0(r)] \delta B_0(r) dr_3 = 0 </math>
where <math>\Phi(r)</math> is the [[intermolecular pair potential]].
Incorporating a reference potential <math>\Phi_0(r)= \Phi_0(r;\sigma,\epsilon)</math>
this equation becomes  (Eqs. 19a and 19b in Ref. 7)
:<math>\rho \int [g(r) - g_0(r)] \sigma \frac{\partial B_0(r)}{\partial \sigma}dr_3 = 0 </math>
and 
:<math>\rho \int [g(r) - g_0(r)] \epsilon \frac{\partial B_0(r)}{\partial \epsilon} dr_3 = 0 </math>
These are the conditions that will determine the optimum values of <math>\sigma</math> and <math>\epsilon</math>
that minimise the free energy. 
The RHNC satisfies the 'Hiroike' termodynamic relation test Ref. 7 and 9, i.e.
:<math>\left.\frac{\partial U}{\partial V}\right\vert_{T} = T \left.\frac{\partial p}{\partial T}\right\vert_{V} -p</math>
For highly asymmetric mixtures see Ref. 9.

==References==
#[http://dx.doi.org/10.1103/PhysRevA.20.1208 Yaakov Rosenfeld and N. W. Ashcroft "Theory of simple classical fluids: Universality in the short-range structure", Physical Review A '''20''' pp. 1208 - 1235 (1979)]
#[http://dx.doi.org/10.1103/PhysRevA.8.2548  F. Lado "Perturbation Correction for the Free Energy and Structure of Simple Fluids", Physical Review A    '''8''' 2548 - 2552 (1973)]
#[http://dx.doi.org/10.1080/00268978700100441 Anatol Malijevský and Stanislav Labík "The bridge function for hard spheres", Molecular Physics, '''60''' pp. 663-669 (1987)]
#[http://dx.doi.org/10.1080/00268978900101181 Stanislav Labík and Anatol Malijevský "Bridge function for hard spheres in high density and overlap regions", Molecular Physics, '''67''' pp. 431-438 (1989)]
#[http://dx.doi.org/ PLA_1982_89_0196]
#[http://dx.doi.org/10.1103/PhysRevA.28.2374  F. Lado, S. M. Foiles and N. W. Ashcroft, "Solutions of the reference-hypernetted-chain equation with minimized free energy", Physical Review A '''28''' 2374 - 2379 (1983)]
#[http://dx.doi.org/10.1143/JPSJ.12.326 Kazuo Hiroike "Radial Distribution Function of Fluids I", Journal of the Physical Society of Japan '''12''' pp. 326-334 (1957)]
#[http://dx.doi.org/10.1143/JPSJ.12.864 Kazuo Hiroike "Radial Distribution Function of Fluids II", Journal of the Physical Society of Japan '''12''' pp. pp. 864-873 (1957)]
#[http://dx.doi.org/10.1063/1.2102891     S. Amokrane, A. Ayadim, and J. G. Malherbe "Structure of highly asymmetric hard-sphere mixtures: An efficient closure of the Ornstein-Zernike equations", Journal of Chemical Physics, '''123''' 174508 (2005)]



[[Category: Integral equations]]