For the melting transition, the solid is represented by an anharmonic model and the liquid is described by the Percusndash;Yevick approximation. The behavior of the liquid at high densities is studied on the isothermskTthinsp;sol;thinsp;egr;thinsp;equals;thinsp;1.3, 1.8,and2.0, wherekis the Boltzmann's constant,Tis the temperature, andegr;is the well depth of the Lennardhyphen;Jones 12ndash;6 pair potential. No solutions of the Percusndash;Yevick equation were found forrgr;sgr;3above 1.3, wherergr;1is the particle density andsgr;is the radial parameter of the Lennardhyphen;Jones potential. The liquid structure is found to be very different from the solid structure near the melting line. The liquid pressures are about 50percnt; low for experimental melting densities of argon. This discrepancy gives rise to melting pressures up to twice the experimental values.
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