Many physics problems have , source , fields , satisfying differential constraints, symbolized by $E\in\cal EJ\in\cal J\cal E\cal JL(x)$ takes values in certain nonlinear manifolds , and coercivity, boundedness hold, then the Green’s function satisfies exact identities. We also link Green’s functions of different problems. The analysis, based on the theory of exact relations for composites, does not assume microscale variations in , and allows for other equations, such as for waves in lossy media. For bodies , in which , the Dirichlet-to-Neumann map satisfies boundary field equalities. These generalize the notion of conservation laws: the constraints on the fields inside give identities satisfied by the boundary fields, and provide extra constraints on the interior fields. A consequence is this: if a matrix valued field with takes values in a set (independent of ) that lies on a nonlinear manifold, we find conditions on the manifold, and on $\cal Bq(x)=n(x)\cdot Q(x)n(x)\partial\OmegaQ(x)\Omega\cal Dq(x)$ to take values in . We find there are additional divergence free fields inside that in turn generate additional boundary field equalities. There exist partial Null-Lagrangians, functionals of a vector potential and its gradient, that act as null-Lagrangians when is constrained for to take values in certain sets $\cal Aw$ satisfies appropriate boundary conditions. The extension to certain non-linear minimization problems is also sketched.

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