This note is concerned with extremals for the integral
J(
u) =
W(
ux)
dx
with W a given smooth function of
ux =
and with u prescribed at
x = 0 and
x = 1; say
u(0) = 0 , u(1) = p0.
In applications to one dimensional elasticity, W is the stored energy function.
We call
u0(x) = p0 x the
trivial solution.
Our examples point out the care needed in choosing function space when discussing the existence and stability of equilibrium solutions in elasticity, and they are indicative of difficulties for realistic models of nonlinear elastic materials in one and higher dimensions.