ABSTRACT

This chapter is devoted to the axisymmetric problem of the theory of elasticity that can be also reduced to the biharmonic equation. Consider a transversely isotropic cylinder referred to cylindrical coordinates ρ, θ, z as in Figure 6.1 with coordinates ρ and z normalized to the cylinder half-length L. Cylindrical coordinates https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780429332081/46add4fd-c5a6-449f-94be-67b35b0d4c26/content/fig6_1.tif"/>