Momentum conservation inelastic collection

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Discussion Overview

The discussion centers on the conservation of momentum in inelastic collisions, specifically examining scenarios such as a car crashing into a stationary tree and coming to a stop. Participants explore the implications of momentum conservation when kinetic energy is transformed into heat and the roles of external forces and systems in these interactions.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that momentum is conserved in an isolated system, such as the car and the tree, despite the car coming to a stop.
  • Others argue that external forces, such as the Earth, must be considered, as they influence the overall momentum of the system.
  • A participant questions how momentum can be conserved if the car's kinetic energy is transformed into thermal energy, suggesting a potential discrepancy in the conservation laws.
  • There is a discussion about the transformation of macroscopic momentum into microscopic motions of particles, with some participants asserting that momentum remains conserved at the particle level.
  • Some participants highlight that while kinetic energy can be transformed into heat, momentum must still account for the directionality of motion, leading to different conservation implications.
  • A participant raises the scenario of a car skidding to a stop, questioning whether momentum is conserved in that case and where the momentum would be transferred.

Areas of Agreement / Disagreement

Participants express differing views on the conservation of momentum in inelastic collisions, with no consensus reached on the implications of external forces or the relationship between kinetic energy and momentum in these scenarios.

Contextual Notes

Participants note the significance of defining the system boundaries and the effects of external forces, which complicate the discussion of momentum conservation. There are also unresolved questions regarding the measurable impact of the Earth's mass on momentum changes.

Who May Find This Useful

This discussion may be of interest to those studying physics, particularly in the areas of mechanics and conservation laws, as well as individuals exploring the nuances of inelastic collisions and energy transformations.

UMath1
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If a car crashes with a stationary tree and comes to stop, we could say that the kinetic energy of the car was converted to heat and that the collision was inelastic. However, conservation of momentum dictates that momentum is still conserved. How would that be possible given that neither the tree nor the car possesses any velocity after the collision?
 
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UMath1 said:
conservation of momentum dictates that momentum is still conserved.
In an isolated system as seen from an inertial frame of reference.
 
wouldn't this meet both those criteria
 
The logical conclusion is that momentum is not conserved ! Something exercises a force that changes the momentum... the car deforms and that requires a lot of work.
 
UMath1 said:
wouldn't this meet both those criteria
What is your isolated system?
 
The car and the tree
 
Plus the Earth underneath - or else the tree would fall over
 
Right. The car, tree, and Earth underneath.
 
So how is momentum conserved?
 
  • #10
mearth >> mcar but in principle you change the (angular) momentum of the Earth a little bit :smile:
(just as much as when you accelerate from standstill for this unhealthy experiment, only in the opposite direction)
 
  • #11
That doesn't quite make sense to me. If kinetic energy is transformed into thermal energy, how come the linear momentum is transformed into angular momentum of the earth. Why is it not that the macroscopic momentum of the car is transformed into the microscopic momenta of the particles that make up the car?
 
  • #12
Ok, linear. We can safely assume the Earth is flat.

The parts of the car are welded, screwed, glued etc. together. The sum of their momenta before IS the momentum of the car.
 
  • #13
Right, but before the net motion of all the parts of the car is in the same direction. So we treat the car as one big particle with momentum in a given direction.

After the collision, the change is that motion of the parts of the car are in random directions and there is no net motion in any given direction, so the car has no velocity and has all its kinetic energy transformed into heat, the random motion of the microscopic particles making up the car.

My question is that why is momentum not transferred from the macroscopic motion of the car to the random microscopic motions of the particles making up the car like kinetic energy is?
 
  • #14
UMath1 said:
My question is that why is momentum not transferred from the macroscopic motion of the car to the random microscopic motions of the particles making up the car like kinetic energy is?
Because momentum is conserved. The Earth moves as a result of the collision.

In every single interaction among all the bazillions of particles that constitute the car and the earth, momentum is conserved in that interaction. Momentum is an additive property -- the momentum of the whole is the sum of the momenta of the parts. If the momentum of all of the particles is otherwise randomized, the law of conservation of momentum assures us that there is still a bias in the direction of the original bulk momentum so that total momentum is conserved. ∑mv is conserved.

Kinetic energy is also conserved in every tiny interaction. But there is no direction to kinetic energy. The law of conservation of energy only assures us that Σ½mv2 is conserved. It is silent on whether the component velocities are or are not aligned.
 
  • #15
UMath1 said:
My question is that why is momentum not transferred from the macroscopic motion of the car to the random microscopic motions of the particles making up the car like kinetic energy is?

The energy is independent of the direction of motion (no matter what direction a particle is moving, its kinetic energy will be ##mv^2/2##) but momentum is not (a particle moving to the left will have momentum ##-mv## while a particle moving to the right will have momentum ##mv## - the net momentum of the two particles is zero).

Momentum and energy must both be conserved in the collision. Thus, after the collision all the collision fragments will collectively have the same net momentum as the original projectile. Even if the collision were to completely vaporize both objects so all that all that is left is a cloud hot gas, on average a few more particles will be moving more in one direction than the other so there will be some net momentum and the cloud as a whole will be moving. (You can see this in online videos of high-speed projectiles penetrating armor plate - a flare of fast-moving incandescently hot gas bursts out the back side, obviously carrying substantial momentum).
 
  • #16
UMath1 said:
The car and the tree
The car and the tree do not form an isolated system. There is a very large external force exerted on the car-tree system.

UMath1 said:
Right. The car, tree, and Earth underneath.
What is the mass of the earth? How much would you expect the Earth's velocity to change? Do you think this is measurable?
 
  • #17
No its very insignificant owing to the large mass of the earth.
 
  • #18
What about if you had a car that skids to a stop. That would not exactly be a collision, but wouldn't momentum still be conserved if you considered the closed system to be the Earth and the car? Where would the momentum of the car be transferred to then?
 
  • #19
UMath1 said:
wouldn't momentum still be conserved if you considered the closed system to be the Earth and the car?
Yes

UMath1 said:
Where would the momentum of the car be transferred to then?
Based on the answers you have received so far, what do you think? Can you justify your answer using Newtons 3rd law?
 

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