Conservation of momentum/kinetic energy in inelastic collisions.

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Discussion Overview

The discussion revolves around the conservation of momentum and kinetic energy in inelastic collisions. Participants explore the principles governing these concepts, addressing the apparent contradiction between the conservation of momentum and the non-conservation of kinetic energy during such events.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about how momentum can be conserved in inelastic collisions while kinetic energy is not, noting that energy is lost as sound and heat.
  • Another participant points out that inelastic collisions are characterized by the non-conservation of kinetic energy, questioning if the original poster's inquiry is about why kinetic energy is conserved in some collisions but not others.
  • A participant reiterates the conservation of momentum, emphasizing that the velocity of the center of mass remains constant, while also noting that the total kinetic energy changes, leading to a contradiction that they do not understand.
  • Another participant elaborates on the definitions of mass and velocity in the context of momentum and energy, explaining that the total kinetic energy cannot be calculated using the average velocity of the system's center of mass, using an analogy involving building blocks to illustrate the point about averages.
  • A later reply expresses satisfaction with the explanation provided, indicating that it helped clarify their understanding.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the original poster's confusion, but there is a general agreement on the definitions and principles of momentum and kinetic energy in inelastic collisions. The discussion includes multiple viewpoints and clarifications without resolving the initial confusion.

Contextual Notes

The discussion highlights the complexity of averaging in physical equations, particularly in the context of kinetic energy and momentum, without resolving the underlying assumptions or mathematical steps involved.

Sweeney
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I'm finding it difficult to understand how momentum is conserved in an inelastic collision, but kinetic energy isn't. I understand some energy leaves the system in the form of sound and heat.

If we look at the momentum of the system before and after the collision, P=mV, they are equal, due to CoM. Assuming a constant mass we can also say that the velocity of the system is constant.

Now looking at kinetic energy, E=(1/2)mv^2 we know that it changes. Again assuming a constant mass we can say that v^2 changes and thus v changes. Obviously these two statements contradict each other, but I don't understand where I went wrong.
 
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I'll try and think of a good way to put it... but in response to your first line, inelastic collisions are defined by a non-conservation of kinetic energy. That being said, is your question really, "why is kinetic energy conserved in some, but not all, collisions?"
 
Sweeney said:
If we look at the momentum of the system before and after the collision, P=mV, they are equal, due to CoM. Assuming a constant mass we can also say that the velocity of the system is constant.
The velocity of the system's center of mass remains constant.

Now looking at kinetic energy, E=(1/2)mv^2 we know that it changes. Again assuming a constant mass we can say that v^2 changes and thus v changes. Obviously these two statements contradict each other, but I don't understand where I went wrong.
The total kinetic energy of the system = Ʃ(1/2)mv^2 for each mass element. v is not the velocity of the center of mass.
 
Sweeney said:
I'm finding it difficult to understand how momentum is conserved in an inelastic collision, but kinetic energy isn't. I understand some energy leaves the system in the form of sound and heat.

If we look at the momentum of the system before and after the collision, P=mV, they are equal, due to CoM. Assuming a constant mass we can also say that the velocity of the system is constant.

If there is a collision then there are at least three quantities that can be meant by "m" and at least three quantities that can be meant by "V".

It would seem that you are taking m to denote the sum of the masses of the colliding objects and V to denote the velocity of the center-of-mass of the colliding objects.

For momentum, that works out because P(total) = m(total) * V(average)

For energy, this does not work because E(total) != 1/2 m(total) * V(average)^2

Let's take an more familiar example... Suppose that you have a pile of building blocks. They are all shaped like cubes. Some are big and some are little. If you pile all the blocks on top of one another you can determine the height of the tower by multiplying the average size of each block by the number of blocks. But you cannot correctly determine the total volume of the blocks by taking the average size the blocks, cubing that and multiplying by the number of blocks.

The average of the cubes is not equal to the cube of the average.
The average of the squares is not equal to the square of the average.
The average of the inverse is not equal to the inverse of the average.

Averages don't commute in general.

That's why there are things like the "harmonic mean" or the "root mean square".
 
Absolutely perfect answer! I finally can understand it.
 

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