Gvae Cxg T

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3 u t H g ̒lj v ̃E B h D ܂ B ́u t H g t H _ Ƀt H g R s v Ƀ` F b N Ă 邩 m F Ă B CDROM Ȃ̂ŁA u h C u v ŁudFONT v iCD FFONT j I т܂ B C X g \ ̃t H g ̃t H _ A ́u t H _ v őI т܂ B ł́uflopdesi v I Ă ܂ B. ̖ C X g f ށA N b v A g ƃJ b g A ̓ ̃v g/ ̓ / t ̋G ߁E5 ̍s / / C X g f. ()i t n i t n N n N n N n N n N n A e n B e n q t N q t q t q t Ω = 1 1 1 1 3 2 1 sin sin 3 sin 2 sin 1 π π π π M M, (7) where Ω =2~sinn 2()N 1 n ω π As we mentioned last time, these modes are essentially standing waves Let's see that this is the case by writing Eq (7) in the form of Eq (6).

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