The free energy of a (1 x 1)-surface, with no relaxation and no adsorp
tion, is calculated using a bond-breaking mode in which the potential
energy of the crystal is treated as the sum of the energy of the bonds
connecting pair-wise atoms. Based on a purely geometrical model, the
number of broken bonds or dangling bonds per atom is calculated on the
surface of the crystal when an atomically flat plane h(hkl) is create
d. The results provide a general expression of the surface free energy
in terms of Miller indices hkl. The anisotropy of the surface free en
ergy is completely described in the expression. Considering nearest-ne
ighboring bonding only, the orientation dependence of the surface free
energy is discussed for simple cubic (sc) and cubic tetrahedral (cth)
crystals, respectively. Wulff plots and the equilibrium forms for the
sc and the cth crystals are obtained on the basis of their expression
s of the surface free energy, implying the cube and the octahedron are
the equilibrium forms for the sc and the cth crystals, respectively.
Furthermore a predicted anisotropy of fee metals is discussed. (C) 199
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