Abstract
Basing on linear elasticity, the displacement field $u_z =B\vartheta \ln r$ (in cylindrical coordinates $r, \vartheta, z$) was derived. This displacement has a jump on the half-plane $\vartheta = 0$. Stresses orthogonal to this discontinuity plane are continuous.References
1. J. FRIEDEL, Dislocations, Pergamon Press, Oxford 1964.
2. J.P. HIRTH, Theory of dislocations [in Russian], Atomizdat, Moskva 1972.
3. Z. WESOŁOWSKI, E. KROENER, A. SEEGER, Nonlinear theory of the interaction between two screw dislocations, CMDS Conference, Paderborn 1992.
2. J.P. HIRTH, Theory of dislocations [in Russian], Atomizdat, Moskva 1972.
3. Z. WESOŁOWSKI, E. KROENER, A. SEEGER, Nonlinear theory of the interaction between two screw dislocations, CMDS Conference, Paderborn 1992.
