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É n g h ~ i Z ^ É s 揺 a 63 _ C G r 3F ( n } / I t B X ̎ʐ^ j. 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) After we do this, let's also identify the wave. P X g @ V R E p X g ̔̔ N J j R E X s ` A c A @ I W i p X g n C ̐ ( N J j R) ŏƃp h ܂ B Ζ{ ̎ ͂ ɍ ߂ A A p X g ̔̔.
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