“…We now analyse a particular 3D case of more relevance to the turbine blade of Fig 3, which consists of cylindrical double walls [34] with sufficient length and constant external radius of curvature, π
. By updating the kinematic equations (Eqs (1a-b)) to account for the Poisson's ratio, π, effect and by postulating zero total bending curvatures, the theoretical 2D solution (Eqs (1)) for flat walls, based on classical beam theory, can be extended into an approximate 3D solution for cylindrical walls, based on flat plate theory; the solution is provided in Appendix D [34]. The solution is exact for flat systems (and cylindrical systems of π
/π‘ β β) and remains an accurate approximation for cylindrical systems of low curvature, i.e.…”