(a) whan the disc slides down and comes onto the plank, then
`mgh=1/2mv^(2)`
`:. v=sqrt((2gh))`
Let `v_(1)` be the common velocity of both, the disc and plank when they move together. From law of conservation of linear momentum,
`mv=(M + m)v_(1)`
`:. v_(1)=(mv)/((M + m))`
Now, change in `KE=(K)_f-(K)_i=("work done")_("friction")`
`:. 1/2(M + m)v_(1)^(2)-(1)/(2)mv^(2)= ("work done" )_("friction")`
or `W_("fr")=1/2(M = m)[(mv)/(M + m]]^(2)-1/2m v^(2)`
`=1/2mv^(2)[m/(M + m)-1]`
as`(1)/(2)mv^(2)=mgh`
`W_(f r)=-mgh[M/(M+m)]`
(b) In part (a), we have calculated work done from the ground frame of reference. Now let us take plank as the reference frame.
.
Accleration of plank `a_(0)=f/m =(mu mg)/M`
Free body diagram of disc with respect to plank is shown in figure.
Here, `ma_(0)="pseudo force"`.
Retardation of disc `w.r.t.` plank.
`a_r=(f+ma_(0))/(m)=(mumg+(mum^(2)g)/(M))/(m)=mumg+(mumg)/(M)`
`=((M+m)/(M))mug`
The disc will stop after travalling a distance `S_(r)` relative to plank, where
`S_(r)=(v_(r)^(2))/(2a_(r))(Mgh)/((M + m)mug), (0=v_(r)^(2)-2a_(r)S_(r))`
`:.` Work done by friction in this frame of reference
`W_(f r)=-fS_(r)-(mumg)[(Mgh)/((M+m)mug)]`
`=-(Mmgh)/((M + m))`
which is same as part (a).