Spinning Objects in a Rotation: Causes and Effects

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SUMMARY

The discussion centers on the phenomenon of rotational motion, specifically how objects like forks and bicycle wheels behave when tossed or spun. It concludes that a fork requires a 720-degree rotation to return to the original orientation due to the principles of angular momentum and the "Tennis Racket Theorem." This theorem explains that rotation about different axes leads to varying stability, with the longest and shortest axes being stable, while the intermediate axis is unstable. The conversation emphasizes the importance of initial conditions and the effects of torque on rotational motion.

PREREQUISITES
  • Understanding of angular momentum and torque
  • Familiarity with Euler's equations for rotational dynamics
  • Basic knowledge of rotational stability and the Tennis Racket Theorem
  • Experience with practical demonstrations of rotational motion
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  • Study Euler's equations in detail to understand rotational dynamics
  • Research the Tennis Racket Theorem and its applications in physics
  • Experiment with different objects to observe rotational behavior
  • Explore advanced concepts in mechanics related to angular momentum conservation
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Physics students, educators, and anyone interested in understanding the principles of rotational motion and stability in mechanics.

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I was recently casually tosing a fork in my hand so it completed a 360 degree rotation with the handle landing back in my hand. I noticed that everytime I did this, the fork returned to my hand upside down (ie facing downwards). So it took a 720 degree rotation for it to come back in my hand the right way up. I tried this with spoons and my handphone and got a similar result. At first I thought the way in which I was tossing the fork might be causing it to rotate on a plane perpendcular to the plane of which I tossed the object. This may be the case; if not, I was hoping to understand the physical explanation of why an object spins in a perpendiclar plane to the direction of rotation, when it is tossed up. Thanks.
 
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The initial cause-ual conditions of motion account for the eventual effectual conditions of motion.

I do not quite understand what you are asking, a sketch or a re-explanation could help, but keep in mind the above statement. Also think about what determines the direction of spin in a sink of emptying water...
 
It's just a matter of the way you are throwing it. Your hand is angled and you are twisting as you throw it. Put some effort into it and I'm sure you can flip it without twisting it.
 
Thanks Russ, I thought that might be the reason. Just a follow up question... If I spun a wheel in space, say a bicycle wheel, would it keep spining in the initial plane that I set it in motion. I noticed, when fixing my bicycle, that when I spun the wheel and held it at the axel, I could feel it trying to twist in my hand. Why is that?
 
damo_clark said:
Thanks Russ, I thought that might be the reason. Just a follow up question... If I spun a wheel in space, say a bicycle wheel, would it keep spining in the initial plane that I set it in motion.
Yes. Provided there is no net external torque the initial angulur momentum will be conserved - in both magnitude and direction.
 
damo_clark said:
I was recently casually tosing a fork in my hand so it completed a 360 degree rotation with the handle landing back in my hand. I noticed that everytime I did this, the fork returned to my hand upside down (ie facing downwards). So it took a 720 degree rotation for it to come back in my hand the right way up. I tried this with spoons and my handphone and got a similar result. At first I thought the way in which I was tossing the fork might be causing it to rotate on a plane perpendcular to the plane of which I tossed the object. This may be the case; if not, I was hoping to understand the physical explanation of why an object spins in a perpendiclar plane to the direction of rotation, when it is tossed up. Thanks.
This effect is explained in most intermediate level Mechanics books.
Using Euler's equations for rotation about principle axes, you can show that the axis of rotation is stable for rotation about the longest and shortest dimension, but unstable for rotation about the intermediate axis. It is demonstrated most clearly with a book. Use a string to keep it from opening. When tossed rotating about its long or shortest axis it
spins without flipping, but acts like your fork if it is spun about the intermediate axis.
 
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Tennis Racket Theorem

This effect is often called the "Tennis Racket Theorem", derived as clem says from Euler's equations.
 
Thanks Doc Al, I often thought it was just my bad luck that when I dropped a piece of buttered bread it more often that not, landed face down. Now I can blame the laws of physics. I feel much better :)
 

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