Abstract
In the cases where misfit in f.c.c. epitaxial films is accommodated by partial dislocations bounding stacking faults, it would appear from the work of Jesser (1970) that a measurement of the residual elastic strain in a thick crystal would yield a value for the stacking-fault energy of the epitaxial film. It is shown, however, that because of necessary incorporation of stair-rod dislocations where the stacking faults cross, such a value can only be an upper limit, and that in practice this is not likely to be a very useful upper limit. A numerical example is worked out for the case of cobalt on (100) copper.