$ 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).