The correct option is
A h=45RWe first use the conservation of linear momentum
ΔP=FΔt
Thus we get
mvo−0=FΔt
Also using the conservation of angular momentum we have
ΔL=τΔt
Icωo−0=FhΔt
ωo=mvohIc
Here we see that ω≠vR. Thus this is a condition of rolling with slipping.
The kinetic frictional force is the only force which acts in horizontal direction and increases the velocity of the ball to 97vo where pure rolling starts.
Now far the translational motion we have(refer the FBD)
Fx=max
μN=mac=μmg
ac=μg
Also for rotational motion
τ=Icα
−μNR=Icα
−μmgR=Icα
α=−μmgRIc(negative sign means anticlockwise direction)
Now when the ball starts rolling at time , we get the linear velocity of the ball as
v=vo+act
97vo=vo+μgt
t=2vo7μg
Also the angular velocity of the ball is given as
ω=ωo+αt
ω=ωo−(μmgRIc)t=mvohIc−27mRvoIc
ω=mvoIc(h−27R)
Now when the pure rolling starts we have
v=Rω
97vo=mvoIc(h−27R)R
97=52mmR2(h−27R)R
97=52R(h−27R)=52hR−57
h=45R