Highly Influential

with Dirichlet boundary conditions. Here Ω represents the frequency of the solution. The method I used to find the periodic solutions u(Ω) for large Ω originates in the work of Craig and Wayne [2] where they constructed solutions for free vibrations, i.e., for f = 0. No smallness assumption is imposed on f and solutions are smooth. Previous works on (1… (More)

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