Energy conservation in superball collision

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Homework Help Overview

The discussion revolves around the conservation of energy and momentum in a collision involving two elastic "superballs" of different masses. The original poster presents a scenario where the balls are released from a height and questions the resulting velocities after the collision, particularly focusing on the top ball's velocity.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of energy and momentum conservation, questioning the correctness of the derived velocities for both balls after the collision. There is a focus on the calculations involving the zero momentum frame and the potential loss of speed for the larger ball during the collision.

Discussion Status

Several participants are engaged in checking calculations and discussing the application of conservation laws. There is an acknowledgment of potential errors in reasoning, particularly regarding the velocities of the balls post-collision. Some participants suggest that using momentum conservation might yield the correct results, while others express uncertainty about their calculations.

Contextual Notes

Participants note discrepancies in the calculations and the need to verify assumptions regarding the velocities before and after the collision. The discussion highlights the complexity of the problem and the importance of careful reasoning in applying conservation principles.

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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Perhaps the big ball loses some speed when colliding with the smaller ball ? How did you find this ##u## for the bottom ball ?
 
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:
Alettix said:
Oh wait, I really messed it up! The speed of the big ball should be ## u - 2v_{ZMF}##, shouldn't it?
Yes, and with that I think you will find the energy is conserved in the lab frame.
 
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  • #10
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! :)
 
  • #11
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:
 
  • #12
Buffu said:
That is not going to get conserved
Are you sure, or are you just guessing?
 
  • #13
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 ?
 
  • #14
Buffu said:
I checked if it is going to conserve in post number 4.
Can you please check my calculations ?
You have some signs wrong in the second equation.
 

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