539.3On the basis of two refined theories of multilayer shells [3,4], a comparative analysis is given of anisotropy in cross-reinforced shells. As is known, investigating anisotropy in problems of axisymmetric deformation of anisotropic shells reduces to integrating a system of ordinary differential equations of eighth order in classical Kirchhoff--Love theory [6,7, 9], of tenth order in Timoshenko-type theory [3, 8, ii], and of twelfth-order in the generalized Timoshenko theory [4].i. Consider a thin multilayer shell of constant thickness h, consisting of N anisotropic layers. The initial surface adopted is the internal surface of any k-th layer or contact surface of layers, which is referred to the curvilinear orthogonal coordinates ~:, ~2. The transverse coordinate z runs in the direction of increase in the external normal to the initial surface.Suppose that 6k is the distance from the initial surface to the upper boundary surface of the k-th layer; Ai are Lame parameters; ki are the curvatures of the coordinate lines; ui, w are the tangential and normal displacements of points of the initial surface; ui(k) are the tangential displacements of points of the k-th layer. Here and below, i = i, 2; k = i, 2, ..., N.In analyzing the stress--strain state of multilayer reinforced shells, nonclassical theory is used [3,4], with the following basic hypotheses.i. The transverse tangential stress varies over the shell thickness according to the lawwhere f(z) is a continuous function, which is specified a priori and satisfies the condition f(6o) = f(6N) = O.2. The normal stress acting on areas parallel to the initial surface area is negligibly small in comparison with the other components of the stress tensor. The first three hypotheses are common to both theories. The kinematic hypothesis of Timoshenko type in Eq. (1.2) is traditional and has been used repeatedly in problems of calculating shells with finite shear rigidity.The general kinematic hypothesis in Eqo (1.3) is less widespread.In contrast to Eq. (1.2), it allows the nonlinear dependence of the tangential stress-and strain-tensor components on the transverse coordinate z to be described.