ABSTRACT

In this chapter, the author writes the dimensionless equations of the antiplane boundary layer. This problem coincides with the antiplane problem of elasticity theory within constant factors. The author assumes that the faces and the edge do not have electrodes. In this case, the simultaneous equations of the antiplane electroelastic problem for the edge have the form. The author assumes that the shell’s faces are covered with electrodes. She shows that the antiplane boundary layer at a rigidly fixed edge (with preliminary polarization being directed along the edge) has a much greater intensity than the inner electroelastic state and is decisive in defining the greatest stresses.