Surface energies of Au͑100͒ p͑1 ϫ 1͒ and Au͑100͒-hex as modeled by a p͑1 ϫ 5͒ unit cell have been calculated as a function of surface charge by the density functional method. When the surface is neutral, the surface energy of Au͑100͒-hex is lower than that of Au͑100͒, consistent with the experimental observation that a Au͑100͒ surface has a hexagonal, instead of a square top layer. Calculations show that the surface energies of both systems increase when the surfaces are positively charged and there is a crossover with increasing charge so that the Au͑100͒-square becomes the ground state. This suggests that the surface-to-hexagonal reconstruction observed in this material can be reversed by an external field or surface charging. The required electric field is quite large, but is achievable at metal/electrolyte interfaces. In this paper, we analyze metal/ electrolyte interfacial energies and metal surface energies, discuss the possible role of specific adsorption, and compare our results to experiments by converting the calculated surface energies from surface-charge-density dependent to electrode-potential dependent, based on the relationship of the work function and potential of zero charge. Experimental results can be explained to some extent.