An open organ pipe of length $l$ is sounded together with another open organ pipe of length $(l+l_1)$ in their fundamental modes. Speed of sound in air is $V$. The beat frequency heard will be $(l_1 \ll l)$

  • A
    $\frac{V l_1^2}{2 l}$
  • B
    $\frac{V l_1}{2 l^2}$
  • C
    $\frac{V l_1}{4 l^2}$
  • D
    $\frac{V l^2}{2 l_1}$

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