How is momentum conserved if you lose kinetic energy?

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SUMMARY

The discussion centers on the conservation of momentum and kinetic energy during inelastic collisions. Participants clarify that while kinetic energy (KE) is lost due to heat and other forms of energy dissipation, momentum remains conserved. This is mathematically supported by the equations governing momentum (mv) and kinetic energy (1/2 mv²). The conversation highlights the importance of understanding momentum as a vector quantity, which can cancel out, unlike kinetic energy, which is a scalar and always positive.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with the concepts of momentum and kinetic energy
  • Basic knowledge of vector and scalar quantities
  • Mathematical proficiency in handling equations involving mass and velocity
NEXT STEPS
  • Study the principles of inelastic collisions in physics
  • Learn about the vector nature of momentum and its implications
  • Explore the concept of energy dissipation in mechanical systems
  • Investigate the role of friction in momentum transfer during collisions
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Physics students, educators, and anyone interested in understanding the principles of momentum conservation and energy transformation in collisions.

Minki
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The energy component of KE is the velocity. Momentum is mass x velocity so, in a collision containing in-elasticity, if KE is lost to heat then that heat energy must have been supplied by the velocity of the object. And since velocity has been lost to supply the heat then the overall momentum after the collision must be less than before the collision. The only way I can think that you could say that momentum is conserved is if you are including heat vibration in the overall momentum, including heat that has been dissipated to the environment. Thanks for any help on this.
 
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Have you taken into account the fact that momentum is a vector not a scalar?
 
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Yes. As far as I can see, the speed component of velocity is lost therefore the resultant vector must be smaller.
 
Momentum goes as mv and kinetic energy goes as mv^2, so, mathematically, it is possible for momentum to be conserved while kinetic energy is lost. Take as an example the totally inelastic collision of a moving mass m with an initially stationary mass, also of mass m. Initially the momentum is mv and afterwards both masses are moving with half the original velocity of the initially moving mass, so the momentum is still mv. But, what do you calculate for the initial and final kinetic energy of the system?
 
Minki said:
As far as I can see...
Do the math.

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Minki said:
The energy component of KE is the velocity.
I can't make sense of this statement. Energy is energy. Velocity is not energy. When I look at the kinetic energy equation I see more than just velocity and when I look at the animation @A.T. provided I see that other thing isn't constant.
 
Thanks to both.
Chestermiller: Yes I've done the math and it does show that KE is lost and momentum is conserved. But from a practical viewpoint, I can't see how this can be the case - for the reason that I gave about the transfer of velocity being needed to dissipate energy.

russ_watters: Velocity is not energy? Well that's turned my whole understanding of physics on its head! Where is the energy then in half m v squared?
 
Minki said:
Yes I've done the math and it does show that KE is lost and momentum is conserved. But from a practical viewpoint, I can't see how this can be the case
Your view is not really practical if it disagrees with basic math.
 
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A.T: Not so much a view - more a need to understand what is happening in a demonstrable way, and to show how the math model works.
 
  • #10
Minki said:
russ_watters: Velocity is not energy? Well that's turned my whole understanding of physics on its head! Where is the energy then in half m v squared?
The entire expression is energy. That's what the equals sign means!

Is a wheel a car or just part of a car?

To me it also seems like you are not paying attention to what the math says/means. Clearly if KE=V then [kinetic] energy is velocity. But you are clearly aware that that isn't the equation for kinetic energy. So I don't understand why you keep saying it.
 
  • #11
Hi @Minki:

I am surprised that you have not asked the question,
"What happened to the missing energy?"​
The total mechanical energy of the system before the collision is
E = (1/2) mv2.​
After the collision, it is
E = (1/4) mv2.​

Regards,
Buzz
 
  • #12
Ok I think I get it. I see energy as mass under motion. If m or v is increased, then the energy is increased, but increasing the velocity is more significant than increasing the mass, hence the v squared. In a 100% inelastic condition, if a mass m with velocity v collides with an equal mass, then the mass doubles and the velocity halves. Halving the velocity is not fully compensated for by the doubling of the mass because the velocity is more significant than the mass when it comes to energy. But momentum is unaffected because that measurement gives mass and velocity equal significance.

Buzz: Does the missing energy becomes vibration in the masses?
 
  • #13
Minki said:
Thanks to both.
Chestermiller: Yes I've done the math and it does show that KE is lost and momentum is conserved. But from a practical viewpoint, I can't see how this can be the case - for the reason that I gave about the transfer of velocity being needed to dissipate energy.

russ_watters: Velocity is not energy? Well that's turned my whole understanding of physics on its head! Where is the energy then in half m v squared?

Its in the combination of mass and velocity.

You shouldn't assume mass is always a constant. With inelastic collisions two masses can become merged into one. Rockets loose mass as fuel is consumed or stages dropped. So both m and v can change.
 
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  • #14
Minki said:
Does the missing energy becomes vibration in the masses?
Hi Minki:

Well, the missing energy has to go somewhere. One possibility is (internal mechanical) vibrations, as you suggest. Another is a different kind of vibration (at the molecular level) which is an increase in temperature. I can imagine that there are more alternative ways depending on the physical/chemical structure of the masses, but I do not have the knowledge to be more specific.

Regards,
Buzz
 
  • #15
Yes, that's what I thought Buzz.

Well I'm glad I got that sorted out, and thanks to everyone for your help.
 
  • #16
Minki said:
if a mass m with velocity v collides with an equal mass, then the mass doubles and the velocity halves
Or if a mass m with velocity v/2 collides with an equal mass and velocity -v/2, the mass doubles and the velocity goes away.

By no coincidence, the reduction in kinetic energy is the same as when one mass had velocity v and the other had velocity 0.
 
  • #17
phinds said:
Have you taken into account the fact that momentum is a vector not a scalar?
Minki said:
Yes. As far as I can see, the speed component of velocity is lost therefore the resultant vector must be smaller.
No, I don’t think that you have taken into account the vector nature of momentum.

Say you have two objects with identical masses and equal and opposite velocity. No matter what the magnitude velocity is, the momentum is zero. However, the KE can be annywhere between zero and infinity. The vector nature of momentum is the key. Once you truly do grasp that the conclusion is clear: two momenta can cancel each other, two KEs cannot
 
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  • #18
Dale said:
No, I don’t think that you have taken into account the vector nature of momentum.

Say you have two objects with identical masses and equal and opposite velocity. No matter what the magnitude velocity is, the momentum is zero. However, the KE can be annywhere between zero and infinity. The vector nature of momentum is the key. Once you truly do grasp that the conclusion is clear: two momenta can cancel each other, two KEs cannot
Hopefully this is not a derail, but I'm not sure I see how this distinction helps the OP. I recognize I myself tripped over this distinction in a recent thread (and it might have been you or @jbriggs who pointed it out), but in common everyday use, they don't seem to act much different in terms of vector vs scalar nature, particularly when looked at in 1D: 1+1=2 (or 1-1=0) regardless of if those numbers are vectors or scalars. What is the difference/value of one vs the other? Or maybe another way: is a purely 1D momentum problem necessarily a vector problem? The direction seems to me to be little more than a placeholder.

Or perhaps more concisely: what is the difference between a 1D vector and a scalar?

To me what seems like the relevant difference between energy and momentum for the OP is that energy is universally conserved whereas momentum is conserved for the objects. The objects have the same combined momentum before and after the collision, but the excess energy has been released into the universe. This explains to me why two different equations can produce two different answers yet both are "conserved" in their own way.

And as for why kinetic energy is a scalar and not a vector, I know we don't generally like sources from places like quora, but their answer makes a lot of sense: because we choose to define it that way - it could have been a vector if it proved useful. Being a scalar makes it easier to use conservation of energy because you don't have to worry about directions when converting between different forms of energy, particularly for forms of energy that don't have an inherrent directionality.

Am I off base on anything here?
 
  • #19
Minki said:
The energy component of KE is the velocity.
I don't think that is a good way to think about it.
It's true that KE deals with the speed of a macroscopic object...
but it might be good to see some details of what is going on.

Here's a way to think about it,
which I learned from teaching mechanics from Tom Moore's Six Ideas That Shaped Physics Unit C.

Total Momentum conservation comes from Newton's Third Law.
So, that holds in any interaction of particles.

Now for kinetic energy...
If, in that interaction,
the transfer of momentum to an object (i.e. the impulse) changes the magnitude of the velocity vector of the object,
then nonzero work is done on the object. Essentially, look at the dot product of d\vec p and \vec v.
The change in kinetic energy is then \int\vec v \cdot d\vec p
 
  • #20
Not sure if this will offer additional insight to the OP, but thought I'd mention it:

For elastic collisions (consider 1D for simplicity) the relative velocity between two colliding objects is the same before and after the collision. If the collision is inelastic the relative velocity differs before and after the collision (the ratio of relative velocities is known as the coefficient of restitution).

If you know the how the relative velocities before and after the collision will differ then you can still solve the system of equations for an inelastic collision in which momentum is conserved and kinetic energy has changed.
 
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  • #21
russ_watters said:
To me what seems like the relevant difference between energy and momentum for the OP is that energy is universally conserved whereas momentum is conserved for the objects. The objects have the same combined momentum before and after the collision, but the excess energy has been released into the universe. This explains to me why two different equations can produce two different answers yet both are "conserved" in their own way.
...
Am I off base on anything here?
I don’t think that you are off base, but I don’t think that is the issue that bothered the OP. He seemed to recognize that KE was not conserved and that it could go out as you say into other forms of energy. My understanding of the issue is that he sees an inevitable coupling between KE and momentum since they are both functions of v.

Regarding the 1D approach. In 1D the distinction would be that energy is non negative while momentum is signed.
 
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  • #22
Ok, thanks for those extra insights. Something else I'd like to get cleared up: I've read that momentum is always conserved, for both elastic and inelastic collisions. But is it still said to be conserved if there is friction? Momentum will be transferred to the particles making up the material which is causing the friction, and I would have thought that the momentum would then be said to have been dissipated?
 
  • #23
Minki said:
Ok, thanks for those extra insights. Something else I'd like to get cleared up: I've read that momentum is always conserved, for both elastic and inelastic collisions. But is it still said to be conserved if there is friction? Momentum will be transferred to the particles making up the material which is causing the friction, and I would have thought that the momentum would then be said to have been dissipated?
If there is friction, there is something you are rubbing against. If you transfer momentum to that something, that something transfers equal and opposite momentum to you. Newton's third law in action.

If you skate across a rink and do a stop in front of the goalie, the momentum you lost is transferred to the rink. The rink gains exactly as much momentum as you lost.
 
  • #24
So it's still conserved in the original mass because whatever you transfer it to will have transferred it straight back? Even if that transfer ends up as heat?
 
  • #25
Minki said:
So it's still conserved in the original mass because whatever you transfer it to will have transferred it straight back? Even if that transfer ends up as heat?
Momentum is transferred to something else. It does not come back. It goes to the something else. The total for the closed system consisting of you plus the something else remains unchanged.

Kinetic energy can end up as heat. Momentum is forever.
 
  • #26
Ok, so it can only be said to be conserved if you consider the original mass and the environment which the momentum was transferred to.
 
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  • #27
Ok thanks.
 
  • #28
Minki said:
Ok, so it can only be said to be conserved if you consider the original mass and the environment which the momentum was transferred to.
Specifically it is my understanding that every time you start or stop moving (or accelerate) on Earth, you change the Earth's rotation rate.
 
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  • #29
Yes, when you start moving the Earth's state is changed, but when you stop the Earth is returned to its original state.
 
  • #30
Minki said:
Ok, so it can only be said to be conserved if you consider the original mass and the environment which the momentum was transferred to.
The environment is not different than the second mass in a collision. The total momentum is conserved, not the individual momenta of each mass.
 

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