Question
Question: A Stick of length L and mass M lies on a frictionless horizontal surface on which it is free to move...
A Stick of length L and mass M lies on a frictionless horizontal surface on which it is free to move in any way. A ball of mass m moving with speed v collides elastically with the stick as shown in figure, If after the collision ball comes to rest, then what should be the mass of the ball?
a.) m = 2M
b.) m = M
c.) m=2M
d.) m=4M
Solution
In this question,given that the stick is at rest and the ball hits the stick and after the Collision ball comes to rest this means that he whole momentum of ball is transferred to the stick and it is also given that the Collision is elastic this means there is no energy loss in the Collison
Complete answer:
Since it is given in the question that the stick is free to move in any direction, so this means that stick will have to follow both conservation of angular momentum as well as conservation of linear momentum
Let’s first start by applying conservation of Linear momentum
So according to conservation of linear momentum
MV = mv
Or V=Vmv ……….. (1)
Where “M” is the mass of the stick and “V” is the velocity if the stick
“m” is the mass of the ball and “v” is the velocity of the ball
Now apply law of conservation of angular momentum
mv(2L)=(12ML2)ω
On solving we get,
ω=ML6mv ………. (2)
Now since it is given that the Collision is elastic and we know that initially the kinetic energy of stick was zero as it is given that initially the stick was at rest so this means we will have only kinetic energy of ball at initial stage, so we can write as
0+21mv2=21MV2+21Iω2
Now putting the values of from equation (1) and (2) we get
m=4M
This means that the mass of stick is four times at that of mass of ball
So, we can say that option (d) is the correct answer .
Note:
In the above question we have to find the mass of the ball and since the stick was at rest then this means that the conservation of momentum will be followed. We need to make sure that we remember the equation for conservation of momentum as this is used very widely in physics.