$A$ thin rod of mass $m$ and length $l$ is oscillating about a horizontal axis through its one end. Its maximum angular speed is $\omega$. Its centre of mass will rise up to a maximum height of:

  • A
    $\frac{1}{6} \frac{l \omega}{g}$
  • B
    $\frac{1}{2} \frac{l^2 \omega^2}{g}$
  • C
    $\frac{1}{6} \frac{l^2 \omega^2}{g}$
  • D
    $\frac{1}{3} \frac{l^2 \omega^2}{g}$

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