“…The boundary condition u (1) = 0, u (1) = g(u(1)) means that the right end of the beam is attached to a bearing device, given by the function g. Fourth-order two-point boundary value problems are useful for mechanics of materials because the problems usually characterize the deformations of an elastic beam. The existence and multiplicity of positive solutions for the elastic beam equations have been studied extensively, see for example [3,7,18,28,29,35,37,40] and references therein. But in the existing literature, there are few papers concerned with the uniqueness of positive solutions.…”