Why do two balls launch from the right in a Newton's cradle instead of just one?

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In summary, the conversation revolved around the famous Newton cradle and the question of why two balls launch from the right when two balls are released from the left. The answer lies in the conservation of momentum and energy, which dictate that two balls will be knocked in order to satisfy both laws. The conversation also touched on the idea of an "ideal" universe and the role of dispersionless signal propagation in explaining the behavior of the Newton cradle. It was also proposed that gluing the two motive balls together or using a single ball with twice the mass would result in a different outcome. However, the conversation concluded that there are more than just two conserved quantities at play in this system, making it difficult to predict the exact result.
  • #36
haruspex said:
In another current thread on the subject I modeled the three ball case as three springs.
See post #11 at https://www.physicsforums.com/threads/conservation-of-momentum-elastic-collisions.972238
As has been noted, the "perfect" Newton's Cradle result requires a small separation so that no three balls are in contact simultaneously. On the other hand, I suspect my model exaggerates the discrepancy by ignoring the time it takes for the shock wave to traverse a ball.
There's more to it! To model it with point particles connected by strings you have to adjust the spring constants and masses such as to guarantee a dispersion-free wave (see the AJP papers cited in #26). Newton's craddle is by far not as simple as it looks!
 
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  • #37
vanhees71 said:
There's more to it! To model it with point particles connected by strings you have to adjust the spring constants and masses such as to guarantee a dispersion-free wave (see the AJP papers cited in #26). Newton's craddle is by far not as simple as it looks!
Dimensional analysis suggests adjusting only the spring constants and masses, but keeping the balls identical, is not going to change the qualitative behaviour. Changing the initial conditions, e.g. to construct a phonon, sounds more helpful.
I'll try to get access to the article.
 
  • #38
tech99 said:
I don't think energy is conserved in a collision. I hear a click.
The click is sound which is particles in the air transferring energy to your ear drum. That energy is lost with each impact as is the friction caused between the balls and the air when they swing back and forth.
Also some energy will be lost between the balls?
So the cycle will decay and E is conserved it just gets less each time.
I cannot follow the arguments why two balls produce two balls, not one ball higher.
If I pushed one ball much harder could I eventually produce two?
P=mv so increasing the velocity is essentially the same as increasing the mass?
 
  • #39
pinball1970 said:
I cannot follow the arguments why two balls produce two balls, not one ball higher.
If I pushed one ball much harder could I eventually produce two?
P=mv so increasing the velocity is essentially the same as increasing the mass?
Two balls mass m in at speed v have momentum 2mv and KE mv2. If only one ball comes out and momentum is conserved it has speed 2v and KE 2mv2.
If that works, patent it quickly.
 
  • #40
haruspex said:
Dimensional analysis suggests adjusting only the spring constants and masses, but keeping the balls identical, is not going to change the qualitative behaviour. Changing the initial conditions, e.g. to construct a phonon, sounds more helpful.
I'll try to get access to the article.
Yes, read the article. It's really surprising that you need this condition of ##k \propto \omega##. It's obviously what's realized to good approximation with the real cradle. I wonder, how one can understand this properly from the theory of bouncing metallic spheres!
 
  • #41
PeroK said:
One key point is that if a ball (moving) impacts another ball (at rest) of equal mass, then the first ball stops and the second moves with the velocity/momentum/energy of the first.

The height of the ball, therefore, only determines this momentum.

If, however, a more massive ball impacts a less massive ball, then the larger ball will continue with some of the momentum.
Say you have the initial ball mass 2m hits 4 balls all mass m will 2 balls be produced?
 
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  • #42
pinball1970 said:
Say you have the initial ball mass 2m hits 4 balls all mass m will 2 balls be produced?

The simplest model is what I posted in post #34. If you imagine small gaps between the balls then all four balls will move:

The large ball hits the first ball, which hits the second ball and stops, which hits the third and stops, which hits the fourth and stops; the fourth being propelled.

Meanwhile, the large ball still has some momentum from the first collision, so it hits the first ball again, but with 1/3 of the momentum this time. By the same process as above, the third ball is propelled, with 1/3 of the momentum of the fourth.

This process repeats twice more, with each ball having 1/3 of the momentum of the previous. And, the large ball still has some residual momentum as well.

That's the simplest theoretical analysis that I can see.

PS see post #44 below from @stevendaryl for the same idea for the two-ball case.

PPS this video at 1:15 shows the experiment with a larger sphere. It actually matches quite accurately the analysis above!

 
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  • #43
There is a prior thread about this, link below. It's complicated. Some key issues brought up in the prior thread and linked to articles. Momentum and energy conservation aren't sufficient enough to restrict the result to a single outcome. The center pack shifts. Over time, the central pack will be visibly swinging due to the supporting strings having finite length. Compression of the balls is a key factor, and separation isn't needed.

https://www.physicsforums.com/threads/a-funny-remark-about-Newtons-cradle.913222
 
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  • #44
The behavior becomes pretty understandable if, instead of assuming that the balls are touching, you assume that there is a tiny space between adjacent balls. (And then consider the touching case as the limiting case as the gap size goes to zero.) If there is a tiny space between the balls, then that means that we only need to consider two-ball collisions. In a linear two-ball collision, it's pretty obvious that conservation of momentum and energy implies that in a collision between a ball of speed ##v## with a ball at rest, then afterward, the first ball is at rest and the second ball has speed ##v##. If we assume that the collision takes negligible time, then the behavior follows.

newtons-balls.png


Here's an illustration with two moving balls hitting four at rest. In scene 1, balls number 1 and 2 are moving, and the others are at rest. In scene 2, after the first collision, balls number 1 and 3 are moving. In scene 3, balls number 2 and 4 are moving. Etc. Finally, in scene 6, balls number 5 and 6 are moving.

So the number of balls moving is always two.
 
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  • #45
Let the total falling mass be m and the velocity of impact be v. Let the total rising mass be M and its initial velocity be V.
From conservation of momentum we can write:

mv = MV

Because of the rigidity of the balls and the overall structure of the cradle the collision will be fairly elastic so most of the kinetic energy is conserved. Ignoring losses due to sound etc we can write:

mv2 = MV2
From the above v =V and m =M
 
  • #46
Dadface said:
Let the total falling mass be m and the velocity of impact be v. Let the total rising mass be M and its initial velocity be V.
How do you know that all the rising mass has the same velocity?

And how do you know that the falling mass doesn't rebound?
 
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  • #47
PeroK said:
How do you know that all the rising mass has the same velocity?

And how do you know that the falling mass doesn't rebound?
You don't know and my answer is an approximation only based on the assumption that the collision is perfectly elastic. It's the same sort of analysis you could apply to mono atomic gases where the collisions can be perfectly elastic.
 
  • #48
Dadface said:
You don't know and my answer is an approximation only based on the assumption that the collision is perfectly elastic. It's the same sort of analysis you could apply to mono atomic gas molecules which can collide perfectly elastically.

It's not an approximation. If you drop a ball onto the Earth it rebounds. And, in fact, in any elastic collision where a smaller mass impacts a larger mass at rest, the smaller mass will rebound.

That's another possible solution in the case of Newton's cradle. The falling ball rebounds and the others all move off.

In fact, the impact ball only stops in the special where the object is of the same mass. Which is why we have analysed the problem as though there are small gaps; or, in any case, as a sequence of simple collisions.
 
  • #49
I think #44 is a convincing elementary explanation. The only assumption you have to make is that the collisions are sufficiently elastic.
 
  • #50
PeroK said:
It's not an approximation. If you drop a ball onto the Earth it rebounds. And, in fact, in any elastic collision where a smaller mass impacts a larger mass at rest, the smaller mass will rebound.

That's another possible solution in the case of Newton's cradle. The falling ball rebounds and the others all move off.

In fact, the impact ball only stops in the special where the object is of the same mass. Which is why we have analysed the problem as though there are small gaps; or, in any case, as a sequence of simple collisions.
The Newton's cradle is not the Earth or a solid lump but is made out of separate parts which can be put into contact with each other. I think the experimental results speak for themselves. If you haven't already done so look at the you tube videos on the cradle. There is no noticeable rebound.

You may want to try the following:
Place a small mass coin in contact with a large mass coin on a smooth surface. Now get an identical small mass coin and slide it towards the the large mass coin so that there is a collision. I just used two ten pence pieces and a pile of four two pound coins for the large mass. There was no appreciable rebound.

Also, my analysis is an approximation because it assumes a perfectly elastic collision which it is not. Using your bouncing ball analogy a perfectly elastic collision with the floor would result in the ball bouncing back to the same height it was released from. Of course that doesn't happen ... you can't get perfectly elastic collisions between macroscopic objects. But the smaller the distortion resulting from the collision the more elastic it will be.
 
  • #51
Dadface said:
The Newton's cradle is not the Earth or a solid lump but is made out of separate parts which can be put into contact with each other. I think the experimental results speak for themselves. If you haven't already done so look at the you tube videos on the cradle. There is no noticeable rebound.

This video includes the experiment with a larger ball and a smaller ball (the smaller ball clearly rebounds).

You can also see in slow motion that clearly more that one ball moves in the normal experiment.

 
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  • #52
stevendaryl said:
(And then consider the touching case as the limiting case as the gap size goes to zero.)
I'm wondering if the gap is that relevant. If you glue the two dropped balls together, you still get a body with a specific non uniform distribution of mass and compressive stiffness, that might still result in two pulses, and thus two balls ejected to similar height.

But if you replace the two dropped balls with a single ball of twice the mass (video in post #51 at 1:16), you get just one small ball ejected very high (while the second last just moves slightly). I wonder if the result here would be clearer, if instead a bigger ball of the same material they used a denser ball of the same size and stiffness.

But this again suggests that you cannot treat this as a single collision, but have to analyze it sequentially, like in post #44.
 
  • #53
haruspex said:
Dimensional analysis suggests adjusting only the spring constants and masses,
Can you elaborate on that please? Dimensional analysis arguments always fascinate me...
 
  • #54
stevendaryl said:
a tiny space between adjacent balls. (And then consider the touching case as the limiting case as the gap size goes to zero.)
That assumes there is no minimum requirement on the gap.
If the balls have mass m, and spring constant k, and the incoming ball has velocity v, the oscillation amplitude during each collision is proportional to ##v\sqrt{\frac mk}##. The gap needs to exceed that amplitude if we are to avoid three balls being in contact simultaneously.
So in a typical arrangement with slow moving steel balls the gap can be extremely small, but not arbitrarily so.
 
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  • #55
PeroK said:
This video includes the experiment with a larger ball and a smaller ball (the smaller ball clearly rebounds).

You can also see in slow motion that clearly more that one ball moves in the normal experiment.



I think this video is better in that it considers a cradle of the type that I thought this discussion was about, a cradle where all the balls are identical.
 
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  • #56
erbahar said:
Can you elaborate on that please? Dimensional analysis arguments always fascinate me...
Spring constants, k, have dimension MT-2, masses, m, have dimension M. The qualitative behaviour of a system depends on dimensionless thresholds, i.e. on how some dimensionless function of the variables compares with some magic constants.
To get rid of the M term, k and m must combine as m/k, producing dimension T2. This means that if you quadruple both m and k then you will get the same qualitative behaviour but at a factor of two of the speed. E.g. if there is also a velocity involved then you will need to adjust that correspondingly to be sure of the same behaviour.
See also post #54.
 
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