Question:

A disc of mass M and radius R is rolling with angular speed to on a horizontal plane as shown. The magnitude of angular momentum of the disc about the origin O is

Updated On: Jun 14, 2022
  • $\bigg( \frac{1}{2} \bigg) MR^2 \omega $
  • $MR^2 \omega $
  • $\bigg( \frac{3}{2} \bigg) MR^2 \omega $
  • $ 2MR^2 \omega $
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The Correct Option is C

Solution and Explanation

$ L_0 = L_{CM} +M (r \times v)$ $\hspace27mm$ ..........(i)
We may write
Angular momentum about O = Angular momentum about
CM + Angular momentum o f CM about origin
$\therefore \, \, \, \, \, \, L_0 = I \omega +MRv $
'
$ \, \, \, \, \, \, \, \, \, \, \, = \frac{1}{2} MR^2 \omega +MR (R \omega ) = \frac{3}{2} MR^2 \omega $
NOTE that in this case [ Figure (a) ] both the terms in E (i)
i.e $ L_{CM} \, \, and \, \, (r \times v ) $have the same direction A. That is why we haveused $ L_0 = /L \omega + MR v$ . We will use $L_0 = l \omega - MRv $ =/o)~MRv if they are in opposite direction as shown in figure (b).
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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.