Abstract
Different ways are proposed to find the expression of the material inhomogeneity forces (so-called configuration forces) in the nonlinear elasticity of electromagnetic solids. This expression involves both the Eshelby material stress tensor and the pseudomomentum of which the interest has been shown by Peierls. It distinguishes automatically the essentially material quantities from those attached to pure fields. In the case of brittle fracture, it yields the electromagnetoelastic generalization of the J-integral (e.g., in piezoelectric ceramics or in magnetostrictive ferromagnets)
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