Inelastic collisions -- how is momentum conserved but not energy?

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Homework Help Overview

The discussion revolves around inelastic collisions, specifically addressing the conservation of momentum versus the loss of kinetic energy. Participants explore the implications of these principles in the context of collisions involving different masses and velocities.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants examine the conditions under which momentum is conserved while kinetic energy is not, questioning the nature of energy loss during inelastic collisions. There are discussions about maximum energy loss and the factors influencing it, including the impact parameter and the coefficient of restitution.

Discussion Status

The conversation is active, with various interpretations of inelastic collisions being explored. Some participants provide insights into the relationship between momentum and energy, while others clarify definitions and conditions for different types of collisions. There is no explicit consensus, but productive avenues for understanding are being pursued.

Contextual Notes

Participants note that the term "inelastic" can encompass a range of collision types, not just perfectly inelastic ones. The discussion also touches on the complexities of energy transformations during collisions, including sound and deformation, which are relevant to the understanding of energy conservation.

richengle
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Homework Statement
in an INELASTIC collision, how is momentum conserved, but not energy?
Relevant Equations
Cons of Momentum
m1v1+m2v2=m1vs'+m2v2' , if car hits small fluffy object m2, initially v2=0, and v1'=v2' ... so
m1v1=[m1+m2](v2')
but why not energy? Why is there a KElost in Cons of Energy?
Cons of Energy
.5m1v1^2+.5m2v2^2=.5m1v1'^2+.5m2v'2^2 +KElost , and again v2=0, v1'=v2'
.5m1v1^2=.5[m1+m2]v2'^2+KElost
I know you could say deformation, but do you somehow have to take the derrivative of energy [wrt what i dont know] to find a maximum, which is dependent on the initial and final masses and velocities?
m1v1+m2v2=m1vs'+m2v2' , if car hits small fluffy object m2, initially v2=0, and v1'=v2' ... so
m1v1=[m1+m2](v2')

but why not energy? Why is there a KElost?
.5m1v1^2+.5m2v2^2=.5m1v1'^2+.5m2v'2^2 +KElost , and again v2=0, v1'=v2'
.5m1v1^2=.5[m1+m2]v2'^2+KElost
using consv of momentum...
KElost=.5[m1v1^2[1-m1/(m1+m2)] ?
.. and if m1>>m2, this is zero,,, how? Some energy should still be lost?
I know you could say deformation, but do you somehow have to take the derrivative of energy [wrt what i don't know] to find a maximum, which is dependent on the initial and final masses and velocities?
 
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You don't have to take a derivative to find the maximum energy lost in an inelastic collision. Maximum kinetic energy is lost when the two masses are not moving relative to each other after the collision. That amount of energy is $$\Delta (KE)=\frac{1}{2}\frac{m_1m_2}{m_1+m_2}(v_2-v_1)^2$$where ##v_1## and ##v_2## are the velocities of the masses before the collision.
 
kuruman said:
Maximum kinetic energy is lost when the two masses are not moving relative to each other after the collision.
That's certainly true for perfectly inelastic collisions in one dimension (head-on collisions), but unqualified "inelastic" is anything that is not perfectly elastic.

@richengle: That momentum is conserved follows from Newton's action/reaction law. If A exerts force F(t) on B then B exerts -F(t) on A. The change in momentum due to a force is its integral over time, so the changes in momentum from the collision are ∫F.dt and -∫F.dt, which clearly add to zero.
The work done on B is ∫F.dx, where the range is the displacement of B in the direction of F. So the work they do on each other also adds to zero, but this time there is no guarantee that the work will all reappear as KE.

For oblique collisions, I'm not sure perfectly inelastic implies sticking together. I would think it only means the coefficient of restitution is zero. So if the bodies are smooth, it is only the velocity components in the direction of the line of centres at collision that will become equal.
 
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Just to help state the statement of the OP a bit more accurately, in inelastic collision momentum is conserved, and energy is conserved too, it is kinetic energy that is not necessarily conserved.
haruspex said:
@richengle: That momentum is conserved follows from Newton's action/reaction law. If A exerts force F(t) on B then B exerts -F(t) on A. The change in momentum due to a force is its integral over time, so the changes in momentum from the collision are ∫F.dt and -∫F.dt, which clearly add to zero.
The work done on B is ∫F.dx, where the range is the displacement of B in the direction of F. So the work they do on each other also adds to zero, but this time there is no guarantee that the work will all reappear as KE.
So the "moral" lesson of this is that impulse always transfers momentum between bodies, but work doesn't necessarily transfer kinetic energy, some work might go to heat or potential energy of deformation .e.t.c..
 
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haruspex said:
That's certainly true for perfectly inelastic collisions in one dimension (head-on collisions), but unqualified "inelastic" is anything that is not perfectly elastic.
I agree, but I also think that we are looking at OP's question about a maximum
richengle said:
##\dots~## but do you somehow have to take the derrivative of energy [wrt what i don't know] to find a maximum, which is dependent on the initial and final masses and velocities?
from different standpoints. Mine is goal-oriented. Given that one is looking for maximum kinetic energy loss and since the kinetic energy of the CM is conserved, the inelastic collision must be head-on and perfectly inelastic. In order to achieve this maximum, the parameters to be varied are two: the impact parameter and the coefficient of restitution. When both are set equal to zero, one has a head-on, perfectly inelastic collision that maximizes the loss of kinetic energy.
 
When I was at school I always thought the conservation of momentum was inferior, in some way, to the great conservation of energy law which applies to everything. It was only when I read Principia that I finally understood - that Aha! moment - what momentum is.

Newton defines it beautifully: Momentum is the quantity of motion a body possesses.

As momentum is mv, and kinetic energy is 1/2 mv^2 how can both be conserved when their equations are so different?

Because when two things collide we get sound , which takes energy away; the bodies deform and heat a little, which takes energy away. When you add up all those bits of energy loss it explains why momentum (the quantity of motion) is conserved and also why energy (kinetic energy of motion + sound loss + heating loss + whatever else ...) is also conserved, even though their equations are so different.

The conservation of momentum follows as Corollary III from Action and reaction are equal and opposite.

Newton.png
 
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