Kinematics describes how the plate's displacements and strains relate:
where u, v, and w are the displacements in the x, y, and z directions, respectively.
|Kinematics for Classical Plates|
The above equations are too general to be useful. A few assumptions on how a plate's cross section rotates and twists need to be made in order to simplify the problem. For classical plate, the assumptions were given by Kirchoff and dictate how the 'normals' behave (normals are lines perpendicular to the plate's middle plane and are thus embedded in the plate's cross section).
Based on these assumptions, the displacement fields can be expressed in terms of the distances by which the plate's middle plane moves from its resting (unloaded) position u0, v0, and w0 and the rotations of the plate's middle plane , , and .
With the normals straight and unstretched, we can safely assume that the shear strain in the z direction is negligible:
Using the assumption that the normals remain normal to the midplane, we can make the x and y dependancy in u(x, y,z) and v(x,y,z) explicit via a simple geometric expression,
The kinematics equations therefore become
where the strains of the middle plane are
and the curvatures (changes of slope) of the middle plane are
Combine the above equations, the strain fields can be written in terms of the mid-plane strains and curvatures.