The Johnson–Kendall–Roberts and the Maugis models have been used to model the adhesion of spherical elastic bodies (represented by paraboloids). Recent work has investigated adhesion of higher-order monomial shapes. These results differ significantly from those of paraboloids. Given that any practical shape will not be “exactly” either a paraboloid or a higher-order monomial, the question arises as to the ranges of validity of these models and what is the requirement, if any, for a transition model. In this investigation the ranges of validity of these models are established by considering a two-term transition model. Furthermore the need for using this transition model is shown to depend not only on the geometry of the bodies but also on material properties.