Like a plate, a shell has bending stiffness, but it has additional stiffness because of its curvature. If you hold a sheet of paper by the edge, it will hang down because it has no stiffness. However, if you curve it even slightly, it will support small objects such as a
pencil. The dynamic shell wave equations
[9] are obtained by adding an axial inertia term to the static shell equations
[8]. We shall simplify our analysis by assuming that the shell is
shallow, or the radius of curvature
R is large, so that we can ignore radial and tangential components of the displacement
. This is a reasonable assumption for height/radius ratios up to around 0.25. The following ...