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 |
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Pages (from-to) | 227-231 |
Number of pages | 5 |
Journal | Journal of Non-Crystalline Solids |
Volume | 312-314 |
DOIs | |
Publication status | Published - Oct 2002 |
ASJC Scopus subject areas
- Ceramics and Composites
- Electronic, Optical and Magnetic Materials