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(URL: http://xxx.lanl.gov). Note that the terminology in this paper is different to that here. There as here, I take the (Formula presented) limit to obtain the (Formula presented) model, but in this reference I describe the (Formula presented) model as sticky spheres. This does not mean that in this reference I am considering the model defined by Baxter 21
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R. P. Sear, Mol. Phys. (to be published) (e-print cond-mat/9805201) (URL: http://xxx.lanl.gov). Note that the terminology in this paper is different to that here. There as here, I take the (Formula presented) limit to obtain the (Formula presented) model, but in this reference I describe the (Formula presented) model as sticky spheres. This does not mean that in this reference I am considering the model defined by Baxter 21.
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Sear, R.P.1
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36849140039
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27
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85037250633
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The temperature range when (Formula presented) is zero 5 9. For finite but short-ranged potentials it is small, as can be seen in the computer simulation results of Hagen and Frenkel 33, and in the theoretical results of Baus and co-workers 34 35 36. Even as the range of the potential increases toward the value at which a liquid phase becomes stable, the temperature range over which the coexisting fluid density decreases from rather high values, volume fractions above 40%, to very low values is narrow. This is enforced by the approach from below the metastable vapor-liquid critical point, to the fluid–solid-coexistence curve. Isotherms are very flat near a critical point and so the approaching critical point forces the curve of the coexisting fluid density (plotted against temperature) to be very flat
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The temperature range when (Formula presented) is zero 59. For finite but short-ranged potentials it is small, as can be seen in the computer simulation results of Hagen and Frenkel 33, and in the theoretical results of Baus and co-workers 343536. Even as the range of the potential increases toward the value at which a liquid phase becomes stable, the temperature range over which the coexisting fluid density decreases from rather high values, volume fractions above 40%, to very low values is narrow. This is enforced by the approach from below the metastable vapor-liquid critical point, to the fluid–solid-coexistence curve. Isotherms are very flat near a critical point and so the approaching critical point forces the curve of the coexisting fluid density (plotted against temperature) to be very flat.
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35
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33646973798
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Tejero, C.F.1
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