Concentration fluctuations of monomer-dimer mixture

N. Sulaiman; S. M. Osman; I. Ali; R. N. Singh

doi:10.1016/S0022-3093(02)01668-X

Concentration fluctuations of monomer-dimer mixture

N. Sulaiman, S. M. Osman, I. Ali, R. N. Singh^*

^*Corresponding author for this work

Physics

Research output: Contribution to journal › Article › peer-review

1 Citation (Scopus)

Abstract

The recently proposed scaling theory of a fused hard-sphere mixture is extended to a fluid mixture of monomers and dimers. The contribution from the attractive force is introduced within the Barker-Henderson perturbation theory via the double Yukawa potential with the parameters fitted to the Lennard-Jones potential. The results suggest that the non-spherical shape of the dimer bond and the non-additivity of the potential play a dominant role to induce phase separation or compound formation in the mixture.

Original language	English
Pages (from-to)	227-231
Number of pages	5
Journal	Journal of Non-Crystalline Solids
Volume	312-314
DOIs	https://doi.org/10.1016/S0022-3093(02)01668-X
Publication status	Published - Oct 2002

ASJC Scopus subject areas

Ceramics and Composites
Electronic, Optical and Magnetic Materials

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title = "Concentration fluctuations of monomer-dimer mixture",

abstract = "The recently proposed scaling theory of a fused hard-sphere mixture is extended to a fluid mixture of monomers and dimers. The contribution from the attractive force is introduced within the Barker-Henderson perturbation theory via the double Yukawa potential with the parameters fitted to the Lennard-Jones potential. The results suggest that the non-spherical shape of the dimer bond and the non-additivity of the potential play a dominant role to induce phase separation or compound formation in the mixture.",

author = "N. Sulaiman and Osman, {S. M.} and I. Ali and Singh, {R. N.}",

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AU - Ali, I.

AU - Singh, R. N.

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AB - The recently proposed scaling theory of a fused hard-sphere mixture is extended to a fluid mixture of monomers and dimers. The contribution from the attractive force is introduced within the Barker-Henderson perturbation theory via the double Yukawa potential with the parameters fitted to the Lennard-Jones potential. The results suggest that the non-spherical shape of the dimer bond and the non-additivity of the potential play a dominant role to induce phase separation or compound formation in the mixture.

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