Relativity & Conservation of Momentum: A vs B Collision

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Discussion Overview

The discussion revolves around the conservation of momentum in the context of a collision between two objects, A and B, moving toward each other. Participants explore the implications of different reference frames on momentum calculations and the nature of momentum as a conserved quantity. The conversation touches on theoretical aspects of collisions and energy transfer, including considerations of object rigidity and structure.

Discussion Character

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

Main Points Raised

  • One participant asserts that the combined object C's velocity after the collision should be the total of the velocities of A and B, raising a question about the outcome of the collision.
  • Another participant clarifies that momentum is defined as mass times velocity, emphasizing the need to consider the masses of A and B and their directions in different reference frames.
  • A further contribution distinguishes between conservation and frame-invariance, explaining that while momentum is conserved, it is not invariant across reference frames, leading to different momentum values depending on the observer's frame.
  • One participant speculates on the nature of the collision's energy transfer, suggesting that the outcome may vary based on the objects' rigidity and structure, proposing various potential reactions such as crumpling or bouncing.

Areas of Agreement / Disagreement

Participants express differing views on the implications of reference frames for momentum calculations, indicating that multiple competing perspectives remain. There is no consensus on the specific outcomes of the collision or the nature of momentum across frames.

Contextual Notes

Participants assume equal masses for A and B and small velocities relative to the speed of light, which may limit the applicability of their arguments. The discussion does not resolve the complexities introduced by different reference frames or the specifics of energy transfer in collisions.

hprog
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Suppose A and B are in uniform motion toward each other, coming from the right and left respectively.
A claims B to move 100 mph to the left and B claims that A moves 100 mph to the right.
Now let us assume that A and B collide together and they crumple up into a combined object C, and let assume that friction and other factors were low, then according to the conservation of momentum the velocity has now to be the total of the velocities.
Will C now move to the left or the right?
If A was at rest, then the total velocity will be 100 to the left, and if B was at rest then the total should be 100 to the right.
So what is wrong here?
 
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Conservation of momentum doesn't say that "the velocity has to be the total of the velocities". Momentum is mass times velocity. So first of all we need to know the masses of A and B.

Let's assume that those masses are equal (which is probably what you meant). Let's also assume that the velocities are small compared to the speed of light, so we don't have to worry about any relativistic complications. Then we can write:

[tex]mv_{A} + mv_{B} = 2mv_{C}[/tex]

where m is the common mass of A and B (so C, which is the two put together, has mass 2m). Note that each of the v's is a vector, so we have to know, not just their magnitudes, but their directions in order to evaluate the above equation. But, as you noted, the directions depend on whose reference frame we use. In A's frame, we have [itex]v_{A} = 0[/itex] and [itex]v_{B} = -100[/itex], whereas in B's frame, we have [itex]v_{A} = 100[/itex] and [itex]v_{B} = 0[/itex] (we're assuming that positive velocities are to the right and negative velocities are to the left). Plugging those numbers into the above equation will give you what [itex]v_{C}[/itex] must be in each frame.

It is true that the two answers, the one for A's frame and the one for B's frame, will be different. Is that what's bothering you?
 
hprog said:
So what is wrong here?
You need to distinguish between conservation and frame-invariance. Momentum is a conserved quantity, but it is not frame-invariant.

A frame-invariant quantity is one which is the same in all reference frames. Different frames disagree on v so they disagree on momentum. Momentum is not frame-invariant, or in other words momentum is relative to the reference frame.

A conserved quantity is one which does not change as a function of time in a given reference frame. Momentum is a conserved quantity. In other words, in a given reference frame its value before a collision is the same as its value after a collision.
 
The way in which the energy is transferred would depend on the makeup of the objects, would it not? If the objects were completely rigid and hit each other at an angle exactly parallel to their trajectory, they would bounce back in exactly opposite trajectories, correct? If the objects were made of smaller particles, the objects would react in accordance to their constituent particles and their structure withing the objects. My guess is that the objects would either crumple and bounce, shatter and bounce, or react and emit radiation. But I'm not a physicist.
 

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