ملخص
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.
اللغة الأصلية | English |
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الصفحات (من إلى) | 227-231 |
عدد الصفحات | 5 |
دورية | Journal of Non-Crystalline Solids |
مستوى الصوت | 312-314 |
المعرِّفات الرقمية للأشياء | |
حالة النشر | Published - أكتوبر 2002 |
ASJC Scopus subject areas
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