“…The equation of motion takes the form of (1) where W mn (r, φ) is the mode shape of the mode (m, n); r [0, a] is the radial variable; a is the plate radius; φ [0, 2π] is the angular variable; m = 0, 1, 2, ... , ∞ and n = 1, 2, 3, ... , ∞ are the numbers of nodal diameters and nodal circles, respectively; A mn , C mn are unknown constants [10,11]. The orthogonality condition [10] is (4) where δ mp and δ nq are the Kronecker deltas, and the following integral has been used to obtain (5) (6) where λ mn = k mn a is the eigenvalue.…”