Energy conservation in superball collision

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Alettix
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Homework Statement


There are two elastic "superballs" of mass M and m placed on top of each other with a smal distance. The lighter ball of mass m is on top of the bigger ball of mass M. The balls are released from a height h and have velocity u when they hit the ground. Prove that the top ball will have velocity ## v = \frac{3M-m}{M+m} \cdot u ## when it leaves the bigger ball.

Homework Equations


momentum conservation ## p_{before} = p_{after} ##
energy conservation ##E_{before} = E_{after} ##
zero momentum frame velocity: ##v_{ZMF} = \frac{p_{tot}}{m_tot} ##

The Attempt at a Solution


I didn't find it problematic to prove the requried result (see attached solution). What I find problematic is the result itself. I must have made some very silly misstake in my reasoning, but the end result I get is that the speed of the top ball after all collisions is ## u + 2v_{ZMF}## and of the bottom ball ##u##. However, before the two balls collide, they both had velocity ##u##. Clearly, energy conservation cannot be satisfied!

Can somebody please point out my probably very stupid misstake to me? Thank you! :)
 

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BvU said:
Perhaps the big ball loses some speed when colliding with the smaller ball ? How did you find this ##u## for the bottom ball ?
Oh wait, I really messed it up! The speed of the big ball should be ## u - 2v_{ZMF}##, shouldn't it?
 
Alettix said:
Oh wait, I really messed it up! The speed of the big ball should be ## u - 2v_{ZMF}##, shouldn't it?
##E_{ki} = 1/2mu^2 + 1/2Mu^2##
##E_{kf} = 1/2m(u^2 + 2(2v_{ZMF})u + (2v_{ZMF})^2) \\+ 1/2M(u^2 + 2(2v_{ZMF})u - (2v_{ZMF})^2)##
##E_{kf} = (1/2M+1/2m)u^2 + m(2v_{ZMF})u + 2m(v_{ZMF})^2 + M(2v_{ZMF})u - 2M(v_{ZMF})^2##
##E_{kf} = (1/2M+1/2m)u^2 + 2(v_{ZMF})^2(m - M) + (M + m)(2v_{ZMF})u##
##E_{ki} \ne E_{kf}##
I think I did this correctly.
 
Buffu said:
##E_{ki} = 1/2mu^2 + 1/2Mu^2##
##E_{kf} = 1/2m(u^2 + 2(2v_{ZMF})u + (2v_{ZMF})^2) \\+ 1/2M(u^2 + 2(2v_{ZMF})u - (2v_{ZMF})^2)##
##E_{kf} = (1/2M+1/2m)u^2 + m(2v_{ZMF})u + 2m(v_{ZMF})^2 + M(2v_{ZMF})u - 2M(v_{ZMF})^2##
##E_{kf} = (1/2M+1/2m)u^2 + 2(v_{ZMF})^2(m - M) + (M + m)(2v_{ZMF})u##
##E_{ki} \ne E_{kf}##
I think I did this correctly.
Sooo, ##u - 2v_{ZMF}## is not right either?
 
I think using momentum conservation will give right answer.
Alettix said:
Sooo, ##u - 2v_{ZMF}## is not right either?
 
Buffu said:
I think using momentum conservation will give right answer.
As far as I am concerned ZMF is meant to make it quicker and easier, so I would like to use that method. But yes, momentum conservation should always give the right answer.
 
Alettix said:
As far as I am concerned ZMF is meant to make it quicker and easier, so I would like to use that method. But yes, momentum conservation should always give the right answer.
No that's not what I meant.
I mean that we can get right velocity for big ball after collision using momentum conservation.

##mu + Mu = m(u + 2v_{ZMF}) + M\color{red}{V}##
 
Last edited:
haruspex said:
Yes, and with that I think you will find the energy is conserved in the lab frame.
Yes. Thank you for helping me get it right! :)
 
haruspex said:
Yes, and with that I think you will find the energy is conserved in the lab frame.
That looks correct but I did not get it.

Initial velocity in lab frame :-
Big mass - u
Small mass - u

Final velocity in lab frame :-
Big mass - ##u - 2v_{ZMF}##
Small mass - ##u + 2v_{ZMF}##
As per OP,

That is not going to get conserved. Either I am getting final velocity of small mass wrong or the big mass.
Can you help me please ? :oldconfused::oldconfused:
 
haruspex said:
Are you sure, or are you just guessing?
I checked if it is going to conserve in post number 4.
Can you please check my calculations ?