Abstract
We apply second order Andersen–Weeks–Chandler perturbation theory to the one-component sticky-hard-spheres fluid. We compare the results with the mean spherical approximation, the Percus–Yevick approximation, two generalized Percus–Yevick approximations, and the Monte Carlo simulations.
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Appendix A: Correction to Approximation (45)
Appendix A: Correction to Approximation (45)
One can understand that Eq. (45) is not an exact relation by comparing the small density expansion of the left and right hand side. For the left hand side we have [9]
where in the Mayer graphs the filled circles are field points of weight 1 and connecting bonds are Mayer functions of the reference system \(f_0\). And using
in the right hand side one finds,
So that the correction term is of order \(\rho \), namely,
The correct small density expansion for the density derivative of the two body correlation function is
where the first term neglected in KSA is \(\rho ^2\alpha _1^\prime =O(\rho ^3)\).
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Fantoni, R. Andersen–Weeks–Chandler Perturbation Theory and One-Component Sticky-Hard-Spheres. J Stat Phys 168, 652–665 (2017). https://doi.org/10.1007/s10955-017-1810-2
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DOI: https://doi.org/10.1007/s10955-017-1810-2