ABSTRACT

A crystal is an anisotropic medium, so that its equation of motion in the linear approximation must be expressed in the general form (I.11). The stress σjk can be expressed in the same approximation in terms of the strain with the help of relation (I.13c) : σik=ciklj∊lj, https://s3-euw1-ap-pe-df-pch-content-public-u.s3.eu-west-1.amazonaws.com/9780429332227/64e5e3df-c95f-4a2a-a02e-98ef4c2d440f/content/equ11_1.tif"/>