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(ii) Rigorous Solution: By expanding the second term in (1.2), we have Acoswt+B(coswtcosf 0 sinwtsinf 0)=0; Fawwaz T. Ulaby, Eric Michielssen, and Umberto Ravaioli, Fundamentals of Applied Electromagnetics c 2010 Prentice Hall

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The solution to this di erential equation is a cosine (or a sine), of frequency. k m. That is called the resonant frequency - also called natural frequency or q fundamental frequency - of an undamped spring-like oscillator. Let us call such frequency ! 0. Hence,! 2 0 = k m, and we can solve for k, yielding k= m! 2 0. The displacement is given ...

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