作者: A.J. Easteal , L.A. Woolf
DOI: 10.1016/0378-4363(84)90073-1
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摘要: Abstract Examination of shear viscosity (η) and self-diffusion coefficient ( D ) data for liquid methane, together with equivalent hard sphere diameters (σ ϱ derived from densities along the solid-liquid coexistence curve, is used to show that Stokes-Einstein equation in hydrodynamic slip limit obeyed only at very high densities. The product ησ / kT differs significantly both low values obtained molecular dynamics (MD) simulations a fluid. Values η/η E (η = Enskog dense fluid viscosity) place those MD simulations, gave expected A η (translational-rotational coupling factor) nitrogen > 1), (within uncertainty experimental on which calculation based) liquefied rare gases 1) temperatures within 20–25% critical temperatures. Apparent departures smooth behaviour, approaching triple points, are accounted by assumption less packing liquids transition than