Question:

A cord is wound around the circumference of wheel of radius $r$, the axis of wheel is horizontal and moment of inertia about it is $I$. A weight mg is attached to the cord at the end. The weight falls from rest. After falling through a distance $h$, the angular velocity of wheel will be

Updated On: Jul 5, 2022
  • $\sqrt{\frac{2gh}{1+mr}}$
  • $\sqrt {2gh}$
  • $\left[\frac{2 mgh }{1+ mr ^{2}}\right]^{1 / 2}$
  • $\sqrt {\frac {2mgh}{1+2mr^2}}$
Hide Solution
collegedunia
Verified By Collegedunia

The Correct Option is C

Solution and Explanation

Applying energy conservation, we have $$ U _{ i }+ K _{ i }= U _{ f }+ K _{ f } $$ Where, $U _{ i }=$ initial potential energy of the (block + pulley) system $U _{ f }=$ final potential energy of the (block+pulley) system $K _{ i }=$ initial kinetic energy of the system $K _{ f }=$ final kinetic energy of the system Here, initial situation corresponds to rest position of the system and final situation correspond to position after falling through height $h$. Eg. (i) gives $0+0=- mgh +\frac{1}{2} mv ^{2}+\frac{1}{2} 1 \omega^{2}$ $$ \begin{aligned} \Rightarrow mgh &=\frac{1}{2} m (\omega r )^{2}+\frac{1}{2} l \omega^{2} \\ &=\frac{1}{2} m \omega^{2} r ^{2}+\frac{1}{2} l \omega^{2} \end{aligned} $$ $\Rightarrow 2 mgh =\omega^{2}\left[ mr ^{2}+1\right]$ $\Rightarrow \omega^{2}=\frac{2 mgh }{1+ mr ^{2}}$ $\Rightarrow \omega=\left[\frac{2 mgh }{1+ mr ^{2}}\right]^{1 / 2}$
Was this answer helpful?
0
0

Top Questions on System of Particles & Rotational Motion

View More Questions

Concepts Used:

System of Particles and Rotational Motion

  1. The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
  2. The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.