In plane elasticity the solutions of the stress field of rigid inclusi
on problems yield the solutions of cavity problems loaded by uniform s
hear tractions sigma = 2mu(OMEGA - omega0)\kappa = -1, where OMEGA is
the rotation of the inclusion and omega0 the rotation of the material
(evaluated at kappa = -1, kappa being the Kolosov constant). It is pro
ved that if the limit of the stress field for the inclusion problem ex
ists at kappa = -1, then it corresponds to a constant rotation field.