Q. A circular platform is free to rotate in a horizontal plane about a vertical axis passing through its centre. A tortoise is sitting at the edge of the platform. Now the platform is given an angular velocity $\omega_{0}$. When the tortoise moves along a chord of the platform with a constant velocity (w.r.t. the platform), the angular velocity of the platform will vary with the time $t$ as

A) [image:7_image38.emf]
B) [image:7_image39.emf]
C) [image:7_image40.emf]
D) [image:7_image41.emf]
Explanation

(c) As there is no external torque, angular momentum will remain constant. When the tortoise moves from $A$ to $C$, figure, moment of inertia of the platform and tortoise decreases. Therefore, angular velocity of the system increases. When the tortoise moves from $C$ to $B$, moment of inertia increases. Therefore, angular velocity decreases
[image:7_image130.emf]
If, $M$=mass of platform
$R =$radius of platform
$m =$mass of tortoise moving along the chord $AB$
$a =$perpendicular distance of $O$ from $AB$
Initial angular momentum, $I_{1} = mR^{2} + \frac{MR^{2}}{2}$
At any time $t$, let the tortoise reach $D$ moving with velocity $v$
$\therefore\ AD = vt$
$AC = \sqrt{R^{2} - a^{2}}$
As $DC = AC - AD = (\sqrt{R^{2} - a^{2}} - vt)$
$\therefore\ \ OD = r = a^{2} + \left\lbrack \sqrt{R^{2} - a^{2}} - vt \right\rbrack^{2}$
Angular momentum at time $t$
$I_{2} = mr^{2} + \frac{MR^{2}}{2}$
As angular momentum is conserved
$\therefore\ \ I_{1}\omega_{0} = I_{2}\omega(t)$
This shows that variation of $\omega(t)$ with time is nonlinear. Choice (c) is correct

Dr. Abubacker
Reviewed by Dr. Abubacker

Physics Educator & NEET/JEE Specialist

Ph.D. in Physics with 19+ years of teaching experience.