The resonance frequency spectrum is first derived for an m-layered Goupillaud-type elastic medium that is subjected to a discrete sinusoidal forcing function that varies harmonically with time at one end and held fixed at the other end. Analytical stress solutions are obtained from a coupled first-order system of difference equations using z-transform methods, where the determinant of the resulting global system matrix in the z-space |Am| is a palindromic polynomial with real coefficients. The zeros of the palindromic polynomial are distinct and are proven to lie on the unit circle for 1≤m≤5 and for certain classes of multilayered designs identified by tridiagonal Toeplitz matrices. An important result is the physical interpretation that all the positive angles, coterminal with the angles corresponding to the zeros of |Am| on the unit circle, represent the resonance frequency spectrum for the discrete model. A sequence of resonance frequencies for the discrete model appears to be universal for all multilayered designs with an odd number of layers, as it is independent of any design parameters.The resonance frequency results for the discrete model are then extended to describe the resonance frequency spectrum for the continuous model, where the forcing function applied at one end of the strip is continuous and varies harmonically with time while the other end is held fixed. The proposed natural frequency spectrum for a free-fixed m-layered Goupillaud-type strip is confirmed by independently solving a simplified form of the frequency equation, obtained after applying a transformation of the spatial variable. Our results suggest that the natural frequency spectrum depends on the layer impedance ratios and it is inversely proportional to the equal wave travel time for each layer.The results are used to identify layered designs with a common frequency spectrum and modify an existing design to obtain a desired frequency spectrum. Other connections are made with previous stress optimization results, the Chebyshev polynomials of the first and second kind, as well as the natural frequencies of a free-fixed non-Goupillaud-type layered strip.
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