$A$ travelling wave represented by $y = A \sin (\omega t - kx)$ is superimposed on another wave represented by $y = A \sin (\omega t + kx)$. The resultant is

  • A
    $A$ standing wave having nodes at $x = (n + 1/2) \lambda/2, n = 0, 1, 2$
  • B
    $A$ wave travelling along $+x$ direction
  • C
    $A$ wave travelling along $-x$ direction
  • D
    $A$ standing wave having nodes at $x = n \lambda/2, n = 0, 1, 2$

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