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The difficulty in solving the equations of elasticity is also due to three-dimensional character of the problem. The one-dimensional problem, which is relevant to experiments where the only excited mode is the longitudinal, has an analytic solution derived by Thomson (see Ref.). To our knowledge, the only treatment of the three-dimensional problem is the one proposed by Pezeril (Refs.). However, these are for different geometries and boundary conditions than the free-standing film
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