A perfectly inelastic collision is one where both of the colliding objects stick together and move as one.

My questions is, why, of all possible combinations of final velocities that conserve momentum, does this one lead to greatest loss in kinetic energy?

One of the reasoning I found was that this is the only combination in which the total kinetic energy of the system becomes 0 in some frame of reference( com frame). But just because the k.e is 0 in some frame doesn't mean that it is the least possible in every other frame, does it?

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    $\begingroup$ Does this answer your question? What's so perfect about perfectly inelastic collisions? $\endgroup$ – BioPhysicist Aug 12 '20 at 12:36
  • $\begingroup$ @BioPhysicist mostly. A little more elaboration on Why a 0 k.e in the com frame HAS to correspond to least k.e in the laboratory frame would do it. $\endgroup$ – OVERWOOTCH Aug 12 '20 at 12:43
  • $\begingroup$ @OVERWOOTCH I think that's simply the definition of a perfectly inelastic collision, i.e. all energy is dissipated into potential energy (deformation of material) and random thermal energy $\endgroup$ – Carl Witthoft Aug 12 '20 at 12:44
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    $\begingroup$ @CarlWitthoft Depending on the frame of reference not all energy is lost $\endgroup$ – BioPhysicist Aug 12 '20 at 12:46
  • $\begingroup$ I know. But what’s the link between sticking together and maximal k.e lost? $\endgroup$ – OVERWOOTCH Aug 12 '20 at 12:47

As far as I can tell, what we need here is an intuitive understanding rather than a mathematical one. The intuition gets a bit blurred by the mathematical expressions. But, if we take the two colliding bodies to be of equal mass, the expressions get greatly simplified. While not immediately obvious, the results apply to arbitrary combinations of masses.

Let me mass in question be $m$. If we call the initial velocities of the two bodies $\vec{v_1}$ and $\vec{v_2}$, and the final velocities $\vec{v_1'}$ and $\vec{v_2'}$ respectively, our only constraint is that momentum must be conserved. So:

$m \vec{v_1} + m \vec{v_2} = m \vec{v_1'} + m \vec{v_2'}$

Since we took the masses to be equal, this immediately reduces to:

$\vec{v_1} + \vec{v_2} = \vec{v_1'} + \vec{v_2'}$

Now, the velocity of the center of mass (sometimes we call it center of momentum, especially when dealing with relativistic systems) which we will call $\vec{V}$ is:

$ \vec{V} = \frac{m \vec{v_1} + m \vec{v_2}}{m + m}$

Again, by virtue of equal masses readily reduces to:

$ \vec{V} = \frac{\vec{v_1} + \vec{v_2}}{2}$

If we transform the initial velocities to this new frame, and call the respective initial velocities of the bodies in this (center of mass) frame $\vec{u_1}$ and $\vec{u_2}$, they are:

$\vec{u_1} = \vec{v_1} - \vec{V}$

$\vec{u_2} = \vec{v_2} - \vec{V}$

Substitiution of the expression for $\vec{V}$ yields:

$\vec{u_1} = \vec{v_1} - \frac{\vec{v_1} + \vec{v_2}}{2}$

$\vec{u_2} = \vec{v_2} - \frac{\vec{v_1} + \vec{v_2}}{2}$

Simplification leads to:

$\vec{u_1} = \frac{\vec{v_1} - \vec{v_2}}{2}$

$\vec{u_2} = \frac{\vec{v_2} - \vec{v_1}}{2}$

Ooooh... So, $\vec{u_1}$ and $\vec{u_2}$ are equal and opposite! This suggests defition of a relative velocity:

$\vec{r} = \frac{\vec{v_1} - \vec{v_2}}{2}$

Such that now

$\vec{u_1} = \vec{r}$

$\vec{u_2} = -\vec{r}$

Why all this trouble? All this work essentially shows two things:

  • In the center of mass frame, the bodies have same magnitude and opposing direction velocities.

  • In the original frame, the velocities can be expressed as:

$\vec{v_1} = \vec{V} + \vec{r}$

$\vec{v_2} = \vec{V} - \vec{r}$

If we call the kinetic energy in the original frame $T$, we can express it as:

$T = \frac{1}{2}m v_1^2 + \frac{1}{2}m v_2^2$

Well, $v_1^2$ is $\vec{v_1}\cdot\vec{v_1}$ and $v_2^2$ is $\vec{v_2}\cdot\vec{v_2}$. So:

$T = \frac{1}{2}m (\vec{V} + \vec{r})\cdot (\vec{V} + \vec{r}) + \frac{1}{2}m (\vec{V} - \vec{r})\cdot (\vec{V} - \vec{r})$

Let us expand this crazy thing:

$T = \frac{1}{2}m (V^2 + r^2 + 2 \vec{V}\cdot\vec{r}) + \frac{1}{2}m (V^2 + r^2 - 2 \vec{V}\cdot\vec{r}) $

Here, a minor miracle occurs. There is perfect cancellation of the dot products. This perfect cancellation only occurs when $\vec{V}$ is the velocity of the center of mass; for any other frame the cross-terms will remain. As such, the center of mass frame is special. (This works just as well when the masses are not equal, just with more complicated expressions.)

Our kinetic energy expression is now:

$T = \frac{1}{2}m V^2 + \frac{1}{2}m V^2 + \frac{1}{2}m r^2 + \frac{1}{2}m r^2 $

Now, this is really cool. The kinetic energy split itself into two distinct parts. One, we can call $T_c$, which is the kinetic energy due to the motion of the center of mass which is just:

$T_c = \frac{1}{2}m V^2 + \frac{1}{2}m V^2$

The second part, which we can call $T_r$, which is the kinetic energy due to motion relative to the center of mass:

$T_r = \frac{1}{2}m r^2 + \frac{1}{2}m r^2$

And of course:

$T = T_c + T_r$

Now, let us consider what happens after the collision. In the center of mass frame (which is special, as we now know) the initial total momentum is zero ($m \vec{r} - m \vec{r} = \vec{0}$) So, the final momentum must be zero. Following the same transformation reasoning, the final velocities in the original frame can be expressed as:

$\vec{v_1'} = \vec{V} + \vec{r'}$

$\vec{v_2'} = \vec{V} - \vec{r'}$

Here, $\vec{r'}$ is the relative velocity in the final state (after the collision). With pretty much the same derivation, the final kinetic energy $T'$ can be expressed as (obviously, in the original frame):

$T' = T_c + T_r'$

$T_c = \frac{1}{2}m V^2 + \frac{1}{2}m V^2$ (exactly the same as before)

$T_r' = \frac{1}{2}m r'^2 + \frac{1}{2}m r'^2$

So, the kinetic energy due to the motion of the center of mass does not change. That is essentially due to conservation of momentum. What can change is the motion relative to the center of mass, which depends on the details (and elasticity) of the collision.

For a perfectly elastic collision,

$|\vec{r}| = |\vec{r'}|$

In general, due to conservation of energy:

$|\vec{r'}| \leq |\vec{r}|$

(Unless some energy is released from another source, but that is not what we are considering here.)

For a perfectly inelastic collision, $\vec{r'} = \vec{0}$. The kinetic energy after the collision will then just be the energy due to the motion of the center of mass - the system becomes lumped, and its "components" no longer carry any kinetic energy.

Just to re-iterate the key point: The center of mass frame is special in the sense that, the kinetic energy in any_other_reference_frame can be expressed as a sum of the kinetic energy of the center of mass in that reference frame, plus the kinetic energies of the bodies in the center of mass reference frame. So, after a collision, since you can not alter the velocity of the center of mass of a system without the action of external forces, that part of kinetic energy is fixed. What you can lose is the kinetic energy of the bodies in the system due to motion relative to the center of mass. And that happens only in the case of a perfect inelastic collision, where the bodies stick together and are motionless in the center of mass frame.

As such, that is the most kinetic energy that can be lost. QED.

  • $\begingroup$ oh ok. So this result is due to the special property of the center of mass, i.e the energy of any system can be divided into k.e of the center of mass plus the k.e of bodies relative to the center of mass. ThAt is actually a very cool fact and perfectly explains it. $\endgroup$ – OVERWOOTCH Aug 12 '20 at 18:49
  • $\begingroup$ @OVERWOOTCH What do you mean by the k.e. of the center of mass? $\endgroup$ – Deschele Schilder Aug 13 '20 at 9:10
  • $\begingroup$ @descheleschilder take the mass of COM as the sum of the individual masses and then use that and velocity of COM to find the KE $\endgroup$ – FissionChips Aug 13 '20 at 10:32

This can easily be turned into a Calculus-$1$ constrained minimization problem.

You are wanting to minimize the total kinetic energy $$K=\frac12m_1v_1^2+\frac12m_2v_2^2$$

given the constraint from conservation of monmentum $$m_1v_1+m_2v_2=p_0$$

You can then easily show (work left to you) that $K$ is minimized under this constraint when $$v_1=v_2=\frac{p_0}{m_1+m_2}$$

i.e. when the objects are moving at the same velocity. Of course, since this happens in a perfectly inelastic collision, this type of collision minimizes kinetic energy of the system.

  • $\begingroup$ Thankyou for your answer. Is there any intuitive reason behind this or should I just accept this result as a mathematical coincidence? $\endgroup$ – OVERWOOTCH Aug 12 '20 at 13:46
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    $\begingroup$ @OVERWOOTCH It's the squared velocity that makes this so. Visually, you can imagine the "velocity contribution" to the minimum KE result as two squares, each with side length v. When the two squares have the same side length (equal velocities), they have minimum area (minimum KE). If you shift velocity (side length) from one object to another, the total KE (area) will only increase. It gets a little more complicated with objects of unequal mass, since the velocity doesn't shift 1:1, but it balances out since the square area is weighted by mass in the KE formula. $\endgroup$ – Nuclear Hoagie Aug 12 '20 at 15:11

It is an important result that the kinetic energy of a system of any number of particles, is minimum in the reference frame attached to the center of mass. So, if you want to lose the maximum energy possible, you need to end up with such a final configuration in the center of mass frame, such that none of the particles is moving (This is lowest final kinetic energy you can achieve, namely, 0). The above situation is only possible, if all the particles come to rest in the center of mass frame just after the collision,in other words, all the particles "stick" to one another.

This argument is superior than the arguments provided in other answers, since this argument is valid for any number of simultaneously colliding particles.

For the common case of two particles, the kinetic energy in the center of mass frame can be written as

$$KE_{\rm COM}=\frac 1 2 \frac{m_1 m_2}{m_1+m_2} v_{\rm rel}^2$$

where $m_1$ and $m_2$ are the masses of the particles, and $v_{\rm rel}$ is the magnitude of the relative velocity of both the particles. As expected, if both the particles stop moving (become stationary, or stick after the collsion) in the center of mass frame of reference $v_{\rm rel}$ becomes zero and so does the kinetic energy. And this is the physical reason you're looking for.

  • $\begingroup$ what is the proof of this result? Im sorry but this is the first time i am seeing this fact $\endgroup$ – OVERWOOTCH Aug 12 '20 at 18:45
  • $\begingroup$ @OVERWOOTCH That's a new question altogether. It would be better if you asked it as a separate question rather than asking it here, in the comment section. $\endgroup$ – user258881 Aug 12 '20 at 20:33
  • $\begingroup$ It's not really a separate question. In fact, the inelastic collision provides a good motivation for why this would be true, because here the kinetic energy drops to exactly zero in the CM frame, which is clearly the minimal value it can possibly hare. $\endgroup$ – leftaroundabout Aug 13 '20 at 14:42
  • $\begingroup$ @leftroundabout But to conclude that a higher kinetic energy in the center of mass frame implies a higher kinetic energy in the lab frame, we do require some math. It cannot be justified by just hand-waving, and comment section is not really the place to do that math. $\endgroup$ – user258881 Aug 13 '20 at 16:04

But just because the k.e is 0 in some frame doesn't mean that it is the least possible in every other frame, does it?

I would like to stress on something important : ! Kinetic energy can never be negative

Zero is the minimum possible kinetic energy !

Just some context :

The centre of mass frame of reference is especially useful in studying nuclear collisions.

Just look here https://phys.libretexts.org/Bookshelves/University_Physics/Book%3A_Mechanics_and_Relativity_(Idema)/14%3A_Relativistic_Collisions/14.04%3A_Radioactive_Decay_and_the_Center-of-Momentum_Frame

  • $\begingroup$ Simple and intuitive. The zero KE result in one reference frame will have non-zero KE in another reference frame. But if you could find a lower KE in that non-zero frame, that would map back to a negative KE in the zero KE frame, which is impossible. $\endgroup$ – Nuclear Hoagie Aug 12 '20 at 15:18
  • $\begingroup$ @NuclearWang are you sure about that? IF the particle is moving with a velocity of 10ms^-1, in a frame moving at 10ms^-1, its k.e is 0. If the velocity wrt ground then decrease 0, the k.e in the moving frame doesn't become negative $\endgroup$ – OVERWOOTCH Aug 12 '20 at 18:44
  • $\begingroup$ @OVERWOOTCH Exactly, KE can't become negative. In the finish-at-rest frame, KE might go from 100J at the start to 0J in the end. In a 10m/s moving frame, it might go from 400J to 100J. If you could somehow get down to 50J in the moving frame, that would imply that in the rest frame, the object lost more KE than it ever had to begin with - this requires negative KE, which is impossible. The inelastic collision maximizes the change in KE regardless of frame, but it's easiest to see in the finish-at-rest frame since you can't lose more energy than you start with. $\endgroup$ – Nuclear Hoagie Aug 12 '20 at 19:06
  • $\begingroup$ im sorry, Im probably being dumb but I think any kinetic energy value is possible in the moving frame. There is no minimum value set by the k.e in the lab frame. If you could perhaps give a numerical example of this contradiction, it would greatly help $\endgroup$ – OVERWOOTCH Aug 13 '20 at 1:28
  • $\begingroup$ The most simplest answer here , +1 from me. $\endgroup$ – Danny LeBeau Aug 13 '20 at 10:35

According to Noether's Theorem, if we make a Galilean transformation, and give a system of moving particles a total momentum of $\vec p$, then $\vec p - m_{tot}\vec v_{cm}=0 $, where $m_{tot}$ the total mass of the particles, and $\vec v_{cm}$ the velocity of the center of mass frame.
This means that, regardless of $\vec v_{cm}$, we can always transform the moving CM-frame into a CM-frame with zero velocity, in which it is obvious that after an inelastic collision the particles stick together and have zero momentum and thus zero velocity (the very definition of a non-moving CM-frame is the frame in which the total momentum remains zero before and after the collision), which means that kinetic energy has the minimum of zero Joules.


If I understand your question correctly, then the answer would simply be realizing what the C.O.M frame does to a two-body problem. If you recall a two body problem can be converted into a one-body problem in the C.O.M frame. This means that equations of motion for the now new one body are equivalent to the original scenario.

Since Kinetic Energy(at least classically) cannot be negative , minimum corresponds to it being zero (with max loss) , hence it cannot be any lower for any other frame.

Now what I mean by this is. Let's take this inelastic collision from some other frame where the K.E has some value. If this collision instead were elastic , computing K.E from the chosen frame$ will give value greater than that for the previous case. So basically getting the most minimum value possible (=0) for K.E. from C.O.M frame implies that if you had chosen any other frame where K.E. was not zero , an elastic collision observed from this frame will give a greater K.E and hence and lesser loss. The key is that for comparing elastic and inelastic collision you have to stick to one frame whatever that maybe.


If you don't want calculus and need a physical interpretation, here's one:-

Meaning of inelastic collision is some energy of collision transforms into potential energy, either by changing shape or heat or sound etc.

So, in a perfect inelastic collision, the maximum amount of energy is converted into potential energy. And by conservation of energy, maximum kinetic energy is lost. (Considering environment to be a part of system.)


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