$A$ uniform rod of mass $m$ and length $\ell$ hinged at end $A$ is released from the horizontal position shown in the figure. Just after the rod is released:
Column $I$Column $II$
$(A)$ Angular acceleration of $C$$(P)$ $\frac{3g}{2}$
$(B)$ Angular acceleration of $B$$(Q)$ $\frac{3g}{2\ell}$
$(C)$ Acceleration of $C$$(R)$ $\frac{3g}{4}$
$(D)$ Acceleration of $B$$(S)$ $\frac{3g}{\ell}$

  • A
    $A \rightarrow S, B \rightarrow S, C \rightarrow R, D \rightarrow P$
  • B
    $A \rightarrow Q, B \rightarrow Q, C \rightarrow R, D \rightarrow P$
  • C
    $A \rightarrow Q, B \rightarrow S, C \rightarrow P, D \rightarrow R$
  • D
    $A \rightarrow S, B \rightarrow Q, C \rightarrow P, D \rightarrow R$

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Two discs $A$ and $B$ are mounted coaxially on a vertical axle. The discs have moments of inertia $I$ and $2I$ respectively about the common axis. Disc $A$ is imparted an initial angular velocity $2\omega$ using the entire potential energy of a spring compressed by a distance $x_1$. Disc $B$ is imparted an angular velocity $\omega$ by a spring having the same spring constant and compressed by a distance $x_2$. Both the discs rotate in the clockwise direction.
$1.$ The ratio of $x_1/x_2$ is
$(A)$ $2$ $(B)$ $1/2$ $(C)$ $\sqrt{2}$ $(D)$ $1/\sqrt{2}$
$2.$ When disc $B$ is brought in contact with disc $A$,they acquire a common angular velocity in time $t$. The average frictional torque on one disc by the other during this period is
$(A)$ $\frac{2I\omega}{3t}$ $(B)$ $\frac{9I\omega}{2t}$ $(C)$ $\frac{9I\omega}{4t}$ $(D)$ $\frac{3I\omega}{2t}$
$3.$ The loss of kinetic energy during the above process is
$(A)$ $\frac{I\omega^2}{2}$ $(B)$ $\frac{I\omega^2}{3}$ $(C)$ $\frac{I\omega^2}{4}$ $(D)$ $\frac{I\omega^2}{6}$

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