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I happened to notice this while fidgeting with a coin. It is a common trick to hold up a coin between the index finger and the thumb, place it on the table and give it a good spin. The coin spins about its diametrical axis, while its center of mass follows a trajectory(not circular in general) about some external axis. My observation corresponds to the point of time, when the coin begins to wobble significantly(i.e: it has lost most of its kinetic energy, and will come to rest face down soon.) While wobbling, the C.O.M velocity is non zero,as it keeps moving in trajectories having progressively smaller radii. One will see this while performing this trick. We will notice a peculiar thing. As the velocity of the plane of the coin as it wobbles, decreases, so does the C.O.M velocity, and both reach zero at the same time. In other words, the damped oscillation of the plane of the coin, and the velocity of the coin moving across the table ceases to zero at the exact same time. Why dosen't it happen like:

1) The coin wobbles in a certain region, with the C.O.M coordinate along the table being constant.(it can rise up and down, based on the wobbling, but no horizontal motion)

2) The wobbling stops first, and then the coin skids to a halt across some distance over the table.

How do we prove that both types of motion stop at the same time? Neither of the 2 possibilities i mentioned above are observed in the real phenomenon. Can someone explain?

PS: I forgot to add, but the rotation of the coin stops simultaneously with the wobbling motion, and sliding as well.

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You are correct in saying that the two forms of motion appear to stop simultaneously. It would be interesting to look at it with a high-speed camera to see if that is really true, and also to look at various surfaces to consider different friction conditions. With physics, it is essentially impossible to measure a zero, since there is always some measurement error, so determining the simultaneity of the two events is not trivial (in fact it is probably impossible in principle).

However, within your experiment it seems that way, and that in itself is enough to be interesting. The only reason the coin stops spinning at all is because there is some dissipation of the energy. This comes primarily from rolling friction, although towards the very end (which is the part you are looking at), air drag comes into play also. This means that you are looking at an area of messy physics.

However, this does not stop us looking at the physics roughly. Note that the kinetic energy before it stops is, by definition, very close to 0. This is because there is a very tiny amount of dissipation that is gradually bringing the system to a stop, so just before it stops, it has only a tiny amount of energy.

The two main forms of dissipation going on are (1) rolling friction, which is the edge of the coin rolling along a surface, and (2) air friction.

Rolling by its nature has a very low amount of dissipation, far less than sliding in general. So let us consider your two scenarios:

  1. The coin wobbles, with the C.O.M. moving up and down. In general, the issue with this is that the coin would need to roll around on a circle which has a smaller circumference than the coin (see diagram below). For the C.O.M. to remain stationary, the circumference of the coin could not roll on the (smaller) circle, basically because the coin is at an angle, so the horizontal distance from the C.O.M. is less than the radius of the coin. So to do this, it would need to slip rather than roll. Slip friction is significantly higher than rolling friction, so it is virtually impossible to imagine the roll-slip happening in a uniform way, which enables the C.O.M. to remain stationary. The energy it takes to move the C.O.M. sideways is essentially zero. There is some small amount associated with changing its direction. But in general it is going to be easier to move the C.O.M. that it is to slip while rolling.

CoinWobble

  1. Wobbling stops, and the coin slides. This probably does happen on a tiny scale. There is some miniscule momentum in the system which cannot dissipate instantaneously. However, the friction associated with sliding a coin across the table is enormous compared with the air friction and rolling friction which have dissipated the coin's energy to get it to stop. In other words, by the time the coin is flat on the table, its kinetic energy is so tiny (since it can be stopped by tiny dissipative forces), that it is unable to slide very far.

My guess is that number 2 will be detectable in a laboratory setting though.


Edit: I took some 1000fps video of a coin wobbling. It is available here. As I mentioned earlier, it's probably a strong function of the kind of surface you're spinning on and the relative friction. But what is apparent (at least here) is that as the coin gets closer to the surface, the two radii in the diagram above approach each other, and so you might expect the C.O.M. to spiral in to a central point, but only hitting that central point when the coin is flat on the table. In this sense, there is a physical, geometrical reason for the two to converge together and stop simultaneously.

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  • $\begingroup$ There must be a small amount of slipping, because that's presumably what dissipates most of the coin's energy. Air friction alone would take much longer to slow and stop the coin, and dissipation through rolling friction on a hard surface is probably even smaller. Note also that the motion can be produced in a way that makes the skidding visible. It's not unusual for a hockey puck on an ice rink to have both wobble and skid. It's harder to do with a coin on a table, where there's more friction, but can happen e.g. if you release the coin awkwardly. $\endgroup$ – pwf Nov 3 '16 at 16:49
  • $\begingroup$ My understanding is that the dissipation is largely through the (tiny) rolling friction. I'm sure there is some slipping, but as you say that has much higher friction, so the tendency will be to roll. The case where lateral movement has been imparted separately is different. What makes coin spinning special is that it lasts so long, largely because the dissipative forces are small. When it is still vertical, of course, it's sliding friction, but at a point contact. $\endgroup$ – Dr Xorile Nov 3 '16 at 17:37
  • $\begingroup$ My first idea was to conserve some quantity, and then draw the contradiction, that one motion cannot keep on happening without the other. However, by simple observation i could not find such a quantity. Can this approach work? $\endgroup$ – Lelouch Nov 4 '16 at 4:34
  • $\begingroup$ I doubt it. I think a continuity argument shows that the second event happens, and the energy argument shows that it is a very low energy event which is hard to detect without precise equipment $\endgroup$ – Dr Xorile Nov 4 '16 at 4:37
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Energy and therefore momentum of the coin is lost through friction. The different "types" of motion all stem from the original momentum of the coin combined with friction and gravity.

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  • $\begingroup$ it is obvious that the friction is enough to stop the coin. What is not obvious is that all sorts of motion (apparently not linked appreciably) stops at the same time. $\endgroup$ – Lelouch Nov 8 '16 at 7:58
  • $\begingroup$ They stop similarly because the coin loses energy through friction. Less energy equals less momentum for all components of the coin's motion. $\endgroup$ – Yogi DMT Nov 8 '16 at 13:52
  • $\begingroup$ Why does it distribute like that? Supplying less energy can also mean great momentum for one component and negligible for the other. $\endgroup$ – Lelouch Nov 8 '16 at 16:05
  • $\begingroup$ The net momentum of the coin approaches zero as it loses energy. Although the momentum vector of a fixed point on the coin may decrease/increase disproportionately to another point at a given point in time, the sum approaches zero. $\endgroup$ – Yogi DMT Nov 8 '16 at 16:23

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