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Solutions of linear wave equations for forced oscillations in a finite region become infinite or large at and near resonant frequencies. For certain one-dimensional forced oscillation problems for the non-linear wave equations from which the linear ones are derived solutions appear to exist at all frequencies. A perturbation procedure for obtaining these solutions at and near the linear resonant frequencies and at other frequencies when the amplitudes of the oscillations are small is given.
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William D. Collins (1971) studied this question.
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