Moment of inertia of a uniform annular disc of internal radius $r$ and external radius $R$ and mass $M$ about an axis through its centre and perpendicular to its plane is
$\frac{1}{2}M\left( {{R^2} - {r^2}} \right)$
$\frac{1}{2}M\left( {{R^2} + {r^2}} \right)$
$\frac{{M\left( {{R^4} + {r^4}} \right)}}{{2\left( {{R^2} + {r^2}} \right)}}$
$\frac{1}{2}\frac{{M\left( {{R^4} + {r^4}} \right)}}{{\left( {{R^2} - {r^2}} \right)}}$
A thin circular ring of mass $M$ and radius $R$ is rotating about its axis with a constant angular velocity $\omega $. Two objects, each of mass $m$, are attached gently to the opposite ends of a diameter of the ring. The ring rotates now with an angular velocity
Radius of gyration of a body depends on
A solid cylinder of mass $M$ and radius $R$ rolls without slipping down an inclined plane making an angle $\theta $ with the horizontal. then its acceleration is
If the equation for the displacement of a particle moving on a circular path is given by:
$\theta = 2t^3 + 0.5$
Where $\theta $ is in radian and $t$ in second, then the angular velocity of the particle at $t = 2\,sec$ is $t=$ ....... $rad/sec$