“…In order to introduce the displacement kinematic assumptions, in this work the generalized Galerkin method is employed, as well described in the book of Washizu, 30 and the three-dimensional mechanical displacements u=(u,v,w) are expressed as: where the three-dimensional displacements can be approximated by a proper choice of the functions in the shell reference surface bold-italicud(α,β), for the shell reference system see Figure 1, and of the functions along the thickness bold-italicgd(z), moreover the accuracy depends also on the number of terms N. In this work the attention is focused on advanced shell kinematic models well-known in literature as Layer-Wise models (LW). In order to easily implement this modeling, the Legendre polynomial are used and, in particular, an higher-order cubic expansion LW 3 has taken into account: in which the used polynomials are function of ζ , locally defined: −1≤ζ≤1, for more details refers to the work of Valvano et al., 24 and the superscript k indicates the kth layer, it means that the polynomial is defined layer-by-layer. To consider a lower kinematic model LW ith , the higher-order terms bold-italicujth, with j>i, are set to zero.…”