$A$ 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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The mass of the pulley is $m$ and its radius is $R$. Assume the pulley to be a uniform disc. The pulley is free to rotate about an axis passing through its centre and perpendicular to its plane. The string is massless and inextensible,and it is wrapped on the pulley. There is no slipping between the string and the pulley. The length of the string which is not wrapped on the pulley is $2R$. $A$ block of mass $m$ is released from the position as shown in the figure. The impulse exerted by the string on the pulley at the moment the string becomes taut is $J$. The value of $\frac{2m \sqrt{gR}}{J}$ is equal to:

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