Why Does a Spinning Coin Tend to Stand Upright?

In summary, the conversation is about the motion of spinning coins and the questions that arise from it. The main question is whether the coin will spin on its edge or on one of its corners, and it is hypothesized that it will spin on the corners due to minimized friction and the center of mass being at its highest point. However, it is noted that objects spinning at high speeds do not necessarily have their center of mass at the highest point, as seen with the Tippe Top and hard-boiled egg. It is also discussed that friction can cause small perturbations in the coin's perfectly balanced state, leading to a wobbling effect. The question is raised about what constitutes a "large enough" angular velocity to stand the coin back
  • #1
hapefish
19
0
I have several questions about the motion of spinning coins. I won't get to them all in this post, but hopefully some of you can help get me started. (Note: I am a mathematician, not a physicist - that might help color your responses.)

First I want to think about spinning an idealized penny - a perfect disk with radius, R, width W, and constant density, ρ.

1. Would you expect such a coin to tend to spin on the flat of it's edge or on one of the corners? I would expect the corners for two reasons: First, friction is minimized when the coin is on a corner and second the center of mass is at its highest point when the coin spins on a corner:

1'. I have noticed that objects spinning at very high speeds seem to move their center of mass to the highest point possible. Two prime examples are the Tippe Top and the hard-boiled egg. Is this a general phenomenon, or are these two examples special cases? I would expect it to be a general phenomenon due to the very large angular velocity causing an upward force on the object, but I really can't say why...

2. I would expect the coin to ideally spin in a perfectly balanced state; however, as the coin spins I expect friction to cause small perturbations in this state making the coin wobble from a perfectly balanced state. When such a wobble occurs, I would expect the coin to stand itself back up into an upright state if the angular velocity is large enough and start the slow descent downwards if the angular velocity is not large enough. But, the question is: What is "large enough?" If given a perturbation that causes the coin to tilt to an angle of θ with the z-axis, is it possible to determine the angular velocity needed to "stand the coin back up?"

Thanks for any insight you can give me!
 
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  • #2
1) Your assumption that friction is the smallest on the edge is not necessarily true. In the most simple model the area does not make a difference.

1') Objects that are spinning do not have a tendency to bring the centre of mass to the highest point. Your mentioned examples are special cases that took the experts a lot of time to understand. They depend on an interaction of the rotation with the friction on the surface leading to something called precession. In special cases this can cause the object to find a configuration that is more stable even though it has a higher centre of mass.

2) The coin starts its descend immediately, but it doesn't tip because the torque induced precession causes the axis to rotate instead of the coin to tip. http://en.wikipedia.org/wiki/Precession
 
  • #3
0xDEADBEEF said:
1) Your assumption that friction is the smallest on the edge is not necessarily true. In the most simple model the area does not make a difference.

1') Objects that are spinning do not have a tendency to bring the centre of mass to the highest point. Your mentioned examples are special cases that took the experts a lot of time to understand. They depend on an interaction of the rotation with the friction on the surface leading to something called precession. In special cases this can cause the object to find a configuration that is more stable even though it has a higher centre of mass.

2) The coin starts its descend immediately, but it doesn't tip because the torque induced precession causes the axis to rotate instead of the coin to tip. http://en.wikipedia.org/wiki/Precession

Thanks for the response - I really appreciate it.

let me see if I can clarify (or have clarified) some of these comments:

It sounds to me that you believe the axis about which an object will spin is most strongly determined by the stability of its axes. I was going to approach this problem by finding the eigenvectors of the its moment of inertia tensor - is that reasonable?

You seem to believe that the coin enters precession immediately after being spun. Here are some observations I have made about the inconsistent precession of the coin, and I would love to know how others interpret these observations:
  • If you observe a coin spinning, you will see that the angle of the rotational axis and the z-axis can vary quite a bit, with the coin "wobbling" to a comparatively large angle between the two axes and then "recovering" to a small (zero?) angle. This makes me believe there is something in the motion of the coin that is standing it up as it spins rapidly.
  • As an experiment, I colored the bottom half of a coin black and watched it as it spun. What happened was the black portion of the coin quickly stabilized and the coin rotated on a single point on its edge instead of rolling along its edge. Occasionally the edge would roll slightly then stabilize again (corresponding with the wobbling effect I described earlier). Eventually the coin would slow to a point that it would roll constantly - at this point the side that it would land on was determined; however, I believe that prior to this point the coin had the opportunity to land on either side.
 
  • #4
hapefish said:
Thanks for the response - I really appreciate it.

let me see if I can clarify (or have clarified) some of these comments:

It sounds to me that you believe the axis about which an object will spin is most strongly determined by the stability of its axes.
I did not make that statement. It is half true. An object can only have a stable rotation about its main inertial axes with the larges and the smallest moment of inertia. Otherwise small deviations quickly build up.

I was going to approach this problem by finding the eigenvectors of the its moment of inertia tensor - is that reasonable?

The coin is a special case, where this is probably not helpful. If we ignore the embossing, then the largest moment of inertia is around axis through the centre of the coin's faces pointing perpendicular to the surface. Apart from the rim, this is the reason why coins roll so well and don't tend to tip especially when they roll fast.

The smallest axis of inertia and the second smallest are degenerate (this is why the coins is special). Any axis from the rim through the centre of the coin has the same moment of inertia, this also stabilizes the coin against tipping sideways and makes it indifferent against rolling / shifting of the axis along the rim.

You seem to believe that the coin enters precession immediately after being spun.
Yes due to friction and slight tilting.
Here are some observations I have made about the inconsistent precession of the coin, and I would love to know how others interpret these observations:
  • If you observe a coin spinning, you will see that the angle of the rotational axis and the z-axis can vary quite a bit, with the coin "wobbling" to a comparatively large angle between the two axes and then "recovering" to a small (zero?) angle. This makes me believe there is something in the motion of the coin that is standing it up as it spins rapidly.
  • As an experiment, I colored the bottom half of a coin black and watched it as it spun. What happened was the black portion of the coin quickly stabilized and the coin rotated on a single point on its edge instead of rolling along its edge. Occasionally the edge would roll slightly then stabilize again (corresponding with the wobbling effect I described earlier). Eventually the coin would slow to a point that it would roll constantly - at this point the side that it would land on was determined; however, I believe that prior to this point the coin had the opportunity to land on either side.
This is pretty complicated. It may or may not be the case, that the coin has a tendency to stand up. There is a tendency for the coin to resist tipping to the side, but no tendency to prevent movement along the rim. But a general tendency to lift the centre of mass does not exist. In the end the spinning coin is a complicated object. When it tips only the outside edge touches the surface producing off axis forces and torque, some of the spinning motion will go into rolling motion or some pure "wobbling". I am sure that there is a long treatise somewhere, probably from the late eighteen-hundreds early nineteen-hundreds. Maybe you can find something. Rotator theory is complicated, especially if there is external torque from friction.

If you want to see something cool look up rattleback.
 
  • #5


I can provide some insights into the motion of a spinning coin based on physics principles.

1. The tendency of a spinning coin to spin on its edge or corner depends on several factors such as the initial conditions of the spin, the shape and mass distribution of the coin, and external forces acting on the coin. In the absence of any external forces, the coin would tend to spin on its edge due to the conservation of angular momentum. This is because the coin's angular momentum is highest when it spins on its edge, as the distance from the axis of rotation (the edge) is greater compared to when it spins on a corner. However, if there is a slight tilt in the initial conditions or external forces such as air resistance, the coin may spin on a corner.

1'. The phenomenon of objects spinning at high speeds moving their center of mass to the highest point is a result of the centrifugal force acting on the object. This is a general phenomenon and can be observed in various objects, not just the Tippe Top and hard-boiled egg. The upward force on the object is due to the object's inertia wanting to continue in a straight line while the rotation pulls it towards the center, causing the object to rise.

2. Friction can indeed cause small perturbations in the perfectly balanced state of a spinning coin. The wobbling of the coin is a result of these perturbations, which can be caused by external forces or imperfections in the coin's shape. The coin may correct itself and stand back up into an upright state if the angular velocity is large enough to overcome these perturbations. The specific value of "large enough" angular velocity depends on the initial conditions and external forces acting on the coin, making it difficult to determine in a general case. However, experimental studies can provide insights into the specific conditions and values for a particular coin.

In conclusion, the motion of a spinning coin is a complex phenomenon that depends on various factors. While we can make predictions based on physics principles, the specific behavior of a spinning coin may vary in different situations. Further research and experiments can provide more insights into the motion of spinning coins.
 

What is the motion of a spinning coin?

The motion of a spinning coin is a combination of rotational and translational motion. As the coin spins, it also moves forward in a straight line.

What causes a spinning coin to eventually fall?

The fall of a spinning coin is due to gravity. As the coin spins, it also experiences a downward force from gravity, causing it to eventually fall to the ground.

Why does a spinning coin appear to stand on its edge when it falls?

When a spinning coin falls, it may appear to stand on its edge because of the conservation of angular momentum. As the coin falls, the force of gravity causes it to rotate around its center of mass, which can give the illusion of it standing on its edge.

Does the mass of a spinning coin affect its motion?

Yes, the mass of a spinning coin can affect its motion. A heavier coin will have more inertia and will be more resistant to changes in its motion, while a lighter coin will be easier to move and accelerate.

How does air resistance impact the motion of a spinning coin?

Air resistance can have a significant impact on the motion of a spinning coin. As the coin moves through the air, it experiences a drag force that can slow down its rotational and translational motion. This can cause the coin to fall faster or slower, depending on its orientation and speed.

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