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

  • A
    $y = -a \cos (\omega t + kx)$
  • B
    $y = -a \sin (\omega t + kx)$
  • C
    $y = a \sin (\omega t + kx)$
  • D
    $y = a \cos (\omega t + kx)$

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