When does a PDE solve a variational problem?

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I understand that for a functional $J[f]$ on the space of differentiable functions $f$ on some domain, setting $\delta J[f]|_{f=f_0} = 0$ yields a (possibly nonlinear) partial differential equation in $f_0$, the $f$ that minimizes $J$. Solutions are non-degenerate if extrema of $J$ are locally unique, and the uniqueness of the PDE is related to the number of extrema of $J$.

My question is if, given a known (nonlinear) partial differential equation with solutions $u$, there is a general method to construct a functional that the $u$ will minimize?

I am not interested in functionals of the form $(f-u)^2$ and other functionals that contain the explicit form of the solutions $u$, and would like to know if there is a method to find $J$ given the terms in the PDE. I'm aware that this can be done for all linear equations such as $Lu=v$ in a straightforward way; namely, for $L\cdot u=v$, $J[u] = \langle u\cdot L\cdot u \rangle - \langle v \cdot u \rangle - \langle u \cdot v \rangle$; but don't know of any extensions to nonlinear PDEs.

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The problem of determining a Lagrangian (and so the action functional) such that the corresponding Euler-Lagrange equation equal a given PDE is known as the inverse problem of variational calculus. See wikipedia (http://en.wikipedia.org/wiki/Inverse_problem_for_Lagrangian_mechanics) for an introduction and nlab (http://ncatlab.org/nlab/show/variational+bicomplex) for a mathematical generalization of this idea (especially the references in the later are useful: Takens/Zuckermann/...).

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When I've tried this in the past, I've just sat down and stared at the problem for a long time. But frequently the opposite happens, and a physics PDE is derived from some conservation law (such as the Maxwell-Vlasov equation or more generally the BBGKY hierarchy) or are actually derived from some action principle that itself is derived from some symmetry considerations. Why would you go the other direction?