Local action principles on a manifold \M are invariant (if at all) only
under diffeomorphisms that preserve the boundary of \M. Suppose, however,
that we wish to study only part of a system described by such a principle;
namely, the part that lies in a bounded region R of spacetime where R is
specified in some diffeomorphism invariant manner. In this case, a description
of the physics within R should be invariant under {\it all} diffeomorphisms
regardless of whether they preserve the boundary of this region. The following
letter shows that physics in such a region can be described by an action
principle that i) is invariant under both diffeomorphisms which preserve the
boundary of R and those that do not, ii) leaves the dynamics of the part of
the system {\it outside} the region R completely undetermined, and iii) can
be constructed without first solving the original equations of motion.Comment: 5 pages (10 preprint pages) ReVTe