Abstract
The elastic field around a dislocation piercing obliquely an anisotropic thin crystal is obtained by combining the classical solution applicable to an infinite anisotropic crystal with an analysis using the concept of continuous dislocation density. Numerical applications are presented for inclined dislocations in Ni3Al and Ni.
Acknowledgements
We would like to thank Professor D.H. Warrington for his pertinent comments on the manuscript.
Disclosure statement
No potential conflict of interest was reported by the authors.