A two-dimensional formulation of the problem of lateral cantilever buc
kling, within the frame work of the theory of sheardeformable thin ela
stic anisotropic plates, is used as the basis of the derivation of a o
ne-dimensional system of differential equations and boundary condition
s for generalized versions of the lateral buckling problems associated
with the names of Euler, Michell, Prandtl, and Timoshenko. It is show
n that, in general, the one-dimensional formulation is governed by a t
enth-older boundary value problem, which reduces to an eighth-order pr
oblem upon assuming absent crosswise transverse shear deformability. T
he remaining problem becomes one of the sixth-order, in the spirit of
classical beam theory, upon an assumption of negligible negligible war
ping stiffness effects. It is further shown that for the problem of a
plate which is end loaded in shear only, the use of first integrals al
lows the derivation of a fourth-aider problem and of a second order pr
oblem, respectively, with the latter being consistent with the classic
al Michell-Prandtl problem.