Short version: Does anyone know of good references for using functional derivatives to obtain equilibrium (or dynamic) equations in elastic theories?
More background:
I've frequently encountered complex elastic problems that might involve strain gradients, nonlinearities, etc. As a physicist, the approach that seems natural to me when I want to find the equilibrium positions $\mathbf{r}$ of bits of matter initially at $\mathbf{R}$ is to take the functional derivative of the energy functional with respect to $\mathbf{r}(\mathbf{R})$ and set it equal to zero. This works out pretty well because the nature of elasticity is that the energy density is semilocal and invariant under rotations and translations, so you get some nice simplifications even for complex solids.
I'm confident this is correct but I don't want to claim it as a new technique and I've found only passing references to it. Does anyone know anything of the history of using functional derivatives in elasticity (or solid mechanics more generally)?