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G ^ E N T X F L s O J E ^ z E P { b N X o F G A T X E G A _ T X y V F t @ C X g G A_ X v O E R v b T E A b v _ E _ X C b ` B t @ C X g F G A o b O. Which means T is independent of x, and, therefore, the tension is constant along the string If we also assume T is independent of t and ‰ is constant along the string, equation (53) can be simplified to utt = T ‰ uxx In general, T and ‰ are nonnegative Therefore, letting c = s T p our equation becomes utt = c2uxx This is known as the wave equationWe will see later that c. 䌧 s t ̃G X e T E G X e X N E v C x g T E Y @La cherir New 点 N V ^ R i E B X ̊ g h ~ ̂ ߂̋x Ɨv ɔ 25 ( y) `5 6 ( ) ܂ł̊ Ԃ x ݂ Ă ܂ B.

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