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• W1782394874 abstract "We show that for any liquid or solid with strong correlation between its NVT virial and potential-energy equilibrium fluctuations, the temperature is a product of a function of excess entropy per particle and a function of density, T = f(s)h(ρ). This implies that (1) the system's isomorphs (curves in the phase diagram of invariant structure and dynamics) are described by h(ρ)/T = Const., (2) the density-scaling exponent is a function of density only, and (3) a Grüneisen-type equation of state applies for the configurational degrees of freedom. For strongly correlating atomic systems one has h(ρ) = ∑(n)C(n)ρ(n/3) in which the only non-zero terms are those appearing in the pair potential expanded as ν(r) = ∑(n)ν(n)r(-n). Molecular dynamics simulations of Lennard-Jones type systems confirm the theory." @default.
• W1782394874 created "2016-06-24" @default.
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• W1782394874 date "2012-02-14" @default.
• W1782394874 modified "2023-10-18" @default.
• W1782394874 title "Communication: Thermodynamics of condensed matter with strong pressure-energy correlations" @default.
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• W1782394874 doi "https://doi.org/10.1063/1.3685804" @default.
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