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CGP EDU Academic Team
Published on: September 12, 2026
The stationary wave $y = 2a \sin kx \cos \omega t$ in a closed organ pipe is the result of the superposition of $y = a \sin(\omega t - kx)$ and
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B
In closed organ pipe. If $y_{\text{incident}} = a \sin(\omega t - kx)$
then $y_{\text{reflected}} = a \sin(\omega t + kx + \pi) = -a \sin(\omega t + kx)$
Superimposition of these two waves give the required stationary wave.
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