$A$ thin uniform metal rod of mass $M$ and length $L$ is swinging about a horizontal axis passing through its end. Its maximum angular velocity is $\omega$. Its centre of mass rises to a maximum height of (where $g$ is the acceleration due to gravity):

  • A
    $\frac{L^2 \omega^2}{3g}$
  • B
    $\frac{L^2 \omega^2}{2g}$
  • C
    $\frac{L^2 \omega^2}{6g}$
  • D
    $\frac{L^2 \omega^2}{4g}$

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