Bilinear Mindlin Plate Element

Most of the following explanation concerns four node plate elements, Figure 1. 3-Node Shell Elements explains the three node plate element, shown in Figure 2.

Plate theory assumes that one dimension (the thickness, z) of the structure is small compared to the other dimensions. Hence, the 3D continuum theory is reduced to a 2D theory. Nodal unknowns are the velocities $(v_{x^{\prime }}{v}_{y^{\prime }}{v}_z)$ of the midplane and the nodal rotation rates $\left({\omega }_{x^{\prime }}{\omega }_y\right)$ as a consequence of the suppressed z direction. The thickness of elements can be kept constant, or allowed to be variable. This is user-defined. The elements are always in a state of plane stress, that is ${\sigma }_{zz}=0$ , or there is no stress acting perpendicular to the plane of the element. A plane orthogonal to the midplane remains a plane, but not necessarily orthogonal as in Kirchhoff theory, (where ${\epsilon }_{xz}={\epsilon }_{yz}=0$ ) leading to the rotations rates ${\omega }_x=-\frac{\partial v_z}{\partial y}$ and ${\omega }_y=\frac{\partial v_z}{\partial x}$ . In Mindlin plate theory, the rotations are independent variables.