The modeling of a Reissner-type plate theory for elastic, monoclinic material is presented. The basic theory is derived using the a-priori-assumption free uniform-approximation approach, which is based upon series expansions of the displacement field and a structured truncation of the elastic potential that gives rise to a hierarchy of approximating theories. An a-priori estimate for the approximation error shows that higher-order theories have indeed a higher rate of convergence with respect to the relative slenderness of the plate. Using a pseudo-reduction approach, the number of PDEs to be solved is reduced significantly. The resulting first-order theory is the classical monoclinic plate theory, whereas, the second order theory is not determined uniquely by the approach. Uniqueness is achieved by introduction of an orthogonal decomposition of higherorder gradients of the in-plane displacements. The final second-order theory coincides with the Reissner-Mindlin theory for the special case of isotropic material.
The uniform approximation techniqueA monoclinic plate theory covering anisotropic edge effects is presented. For the special case of a linear elastic, isotropic material it equals the well established plate theory of Reissner [1,2] and could therefore be regarded as an anisotropic extension of this theory. All details of the modeling of the presented theory can be found in [3].The modeling is based on the so-called uniform-approximation technique, a modeling approach for consistent plate and shell theories that came up in the middle of the last century [4]. More recently, it was applied in [5,6] for the derivation of higher-order isotropic plate theories and the approach was extended towards monoclinic material in [7].The key idea of the uniform-approximation technique is to derive plate theories from the three-dimensional theory of linear elasticity, by the use of dimensionless coordinates and series expansions in thickness direction of the plate. Here, we use abstract Fourier-series expansions for the unknown quantities. To this end, a L 2 -basis of orthogonal polynomials is used that are scaled Legendre polynomials, firstly introduced in [7]. An advantage of the approach is that, on the one hand, the associated, generalized stress-resultants of the lowest order coincide with the classical shear forces and moments, while on the other hand, the stress-resultants in general turn out to be the Fourier coefficients of the stress field. This gives higher-order stress resultants a direct physical meaning and, moreover, it allows for a three-dimensional stress field reconstruction from the solution of the plate theory, which is a major advantage in comparison to other series expansions.It can be shown [7] that varying the first variation of the elastic potential with respect to the virtual displacement coefficients leads to an exact two-dimensional form of the three-dimensional equilibrium equations formulated in the generalized stress resultants. However, the arising infinite system of equations is intractabl...