“…Extensions of the kinematics of the Di Sciuva's First-order zigzag theory (linear zigzag model) include, among other: (i) extension to the linear [41] and nonlinear [48] multilayered shell theory; (ii) general lamination lay-up [42,47,49]; (iii) satisfaction of the shear stress-free boundary conditions on the top and bottom surfaces [44,46,50]; (iv) polynomial expansion of the global part to any degree [47,49]; (v) extension to the dynamics, buckling [16,47,49,48]; (vi) thermal effects [68], [69]; (vii) sublaminates approach [68,69,70,71,72,73,74]; (viii) inclusion of von Kármán geometrically nonlinear effects [16,48,49]; (ix) extension to the nonlinear theory of laminated composites with damaged interfaces [49,68,69,74,75,76]; (x) inclusion of the transverse normal strain and stress [74,77,78]; (xi) visco-elastic effects [79]; (xii) active control of beams, plates and shells [80].…”