Two energy approaches to electroelastic fracture yielding path-indepen
dent integrals already proposed in the literature are analysed in this
paper. A particular problem concerning the propagation of an electric
ally conducting crack in a dielectric is formulated and the near-tip s
olution is obtained. This is used to show that one of the above-mentio
ned energy balances for the fractured body contains a diverging integr
al, becoming inadequate for the description of such a real situation.
The controversy concerning the path-independent integrals is identifie
d as being a controversy between two basic different formulations of e
lectroelasticity equations. In the present context, the obtained resul
ts actually represents an argument in favour of the theory that views
the action of electromagnetic fields via contact forces rather than at
-a-distance forces.