Gibbs ensemble Monte Carlo simulations have been used to calculate vapour-liquid equilibria of diatomic and dipolar diatomic fluids. Dipolar two-centre Lennard-Jones diatomics with elongations L* = L/σ between 0·33 and 1·00 have been studied for various values of dipole moments μ*d = μd/(εσ3)1/2. The results for phase equilibrium are in good agreement with recent theoretical predictions based on cluster-expansion perturbation theory.
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Dubey et al. (1993) studied this question.
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