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Using our cleaving-wall method developed previously for the study of crystal−melt interfaces ( J. Phys. Chem. B 2005, 109, 17802), we compute with high precision the interfacial free energies of the hard-sphere fluid (γ wf ) and crystal (γ wc ) in contact with a structureless hard wall. The interfacial free energies are determined as functions of density and, for γ wc, as functions of crystal/wall orientation [(111), (100), and (110)]. Using the current calculations, along with our previously calculated value for the hard-sphere (111) crystal−fluid interfacial free energy,, we show that, at the crystal−fluid coexistence conditions, γ wf − [ + ] > 0. This inequality demonstrates that a (111) hard-sphere crystal will completely wet a hard-sphere fluid/structureless hard wall. This conclusion from thermodynamics is consistent with recent structural evidence by Dijkstra ( Phys. Rev. Lett . 2004, 93, 108303) of wall-induced prefreezing of a hard-sphere fluid in contact with a structureless hard wall. We also find evidence that a (111) crystal will wet a (110) crystal/wall interface.
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Laird et al. (2007) studied this question.
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