$A$ uniform rod of mass $m$ and length $l$ rotates in a horizontal plane with an angular velocity $\omega$ about a vertical axis passing through one end. The tension in the rod at a distance $x$ from the axis is

  • A
    $\frac{1}{2} m \omega^2 x$
  • B
    $\frac{1}{2} m \omega^2 \frac{x^2}{l}$
  • C
    $\frac{1}{2} m \omega^2 l \left( 1 - \frac{x}{l} \right)$
  • D
    $\frac{1}{2} \frac{m \omega^2}{l} \left( l^2 - x^2 \right)$

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