The goal of the present study was to develop a general strategy for interpolating the perturbation contributions between simulations of individual state points in order to facilitate usage of molecular simulation results in engineering applications. We find that the athermal entropy of mixing deviates significantly from ideality, but still follows the van der Waals mixing formula. This leads to an accurate characterization of the entropic contribution for mixtures of all sizes and shapes. A general rule is developed for predicting the athermal entropy of mixing based on knowledge of the volume ratios of the constituent molecules. The simulations are compared to several theories, including the MCSL theory for hard spheres,[2] the SAFT model,[3] and the Guggenheim-Staverman theory.[4]
Keywords: Thermodynamic properties, molecular simulation, polymers, entropy, mixtures, phase equilibria.
Reference:
1. Gray, N. H.; Elliott, J. R. In Quadratic Mixing in Perturbation Theory, AIChE Fall National Meeting, Austin, TX, 2004; Austin, TX, 2004; p 160e.
2. Mansoori, G. A.; Carnahan, N. F.; Starling, K. E.; Leland, T. W., Equilibrium Thermodynamic Properties of the Mixture of Hard Spheres. J. Chem. Phys 1971, 54, 1523-1525.
3. Chapman, W. G.; Gubbins, K. E.; Jackson, G.; Radosz, M., SAFT: Equation of State Solution Model for Associating Fluids. Fluid Phase Equilib. 1989, 52, 31.
4. Abrams, D. S.; Prausnitz, J. M., Statistical Thermodynamics of Liquid Mixtures: A New Expression for the Excess Gibbs Energy of Partly or Completely Miscible Systems. AIChE J. 1975, 21, 116.