Angular Momentum of a Spinning Coin

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Homework Help Overview

The discussion revolves around calculating the angular momentum of a coin spinning about a vertical diameter at its center of mass. Participants are examining the relationships between mass, diameter, angular velocity, and the resulting angular momentum in various contexts, including points away from the coin and the motion of the coin's center of mass.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to derive angular momentum using different equations and considers the effects of the coin's motion. Some participants question the validity of the terms used in the equations and seek clarification on the motion of the coin and its center of mass.

Discussion Status

The discussion is ongoing, with participants providing insights into the angular momentum of the coin and its rotational inertia. Some guidance has been offered regarding the use of the perpendicular axis theorem and the definitions of rotational inertia, but there is no explicit consensus on the correct approach yet.

Contextual Notes

Participants are working with specific values for mass and diameter, and there is mention of different scenarios regarding the coin's motion, including its center of mass traveling in a straight line. The original poster expresses uncertainty about the formulas and concepts involved, indicating a need for further clarification.

cpuwildman
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I'm trying to calculate the angular momentum of a coin spinning about a vertical diameter about its center of mass. Given is mass, diameter, and angular velocity. I thought it would be [tex]L=\frac{1}{4}MR^2\omega[/tex]. The angular momentum about a point away from the coin I thought would be [tex]L=\frac{1}{4}MR^2\omega + Mh^2\omega[/tex] where [tex]h[/tex] is the distance from the axis containing the diameter of the coin to the point away from the coin. And if the coin's center of mass were moving in a straight line while doing the two above things, then I thought that to each of those would be added [tex]MvR[/tex]. I'm guessing that it is just something simple that I missed in the beginning which propagated the error through the other parts of the problem. Help would be greatly appreciated.
 
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What exactly is the motion of the coin? If it's just spinning about a vertical diameter, you would be correct that the angular momentum is (treating the coin as a thin disk):
[tex]L=\frac{1}{4}MR^2\omega[/tex]
I do not understand the second term in your second equation. Is the coin also revolving about some point with the same angular speed as it is rotating?
 
For the sake of clarity, I will just post the whole question.

A 10 g coin of diameter 1.3 cm is spinning at 16 rev/s about a vertical diameter at a fixed point on a tabletop.

(a) What is the angular momentum of the coin about its center of mass?
(b) What is its angular momentum about a point on the table 10 cm from the coin?
(c) If the coin spins about a vertical diameter at 16 rev/s while its center of mass travels in a straight line across the tabletop at 5 cm/s, what is the angular momentum of the coin about a point on the line of motion?
(d) What is the angular momentum of the coin about a point 10 cm from the line of motion? (There are two answers to this question.)

I appreciate your help.
 
Much clearer. :smile:

This may help you: the angular momentum of an object is the sum of:
(1) the angular momentum of the center of mass
(2) the angular momentum about the center of mass

Thus:
a: See previous post
b: What's the movement of the center of mass?
c: See above
d: See above (there are two answers since you could be on either side of the line of motion)
 
hi, sorry but I am a little slow
Can you explain to me how did you get the formula for the angular momentum please
Thanks for the help
 
Welcome to PF, ChanDdoi.

I'm not sure I understand your question. Which formula are you asking about?

In general, if an object rotates about an axis, the magnitude of the angular momentum will be [itex]L = I\omega[/itex], where I is the rotational inertia about that axis and [itex]\omega[/itex] is the angular speed.
 
Well, why would the inertia of the coin be [tex]\frac{1}{4}MR^2\[/tex] i just can't seem to figure it out *may be because I'm slow*
The book said if you treat it as a disk then the inertia would be [tex]\frac{1}{2}MR^2\[/tex] and if I try to treat it as a sum of bars since it is spinning on a vertical axis then I got lost with the integrals and stuff . Either way I just cannot seem to get that [tex]\frac{1}{4}MR^2\[/tex]

btw, thanks for welcoming me to PF
 
rotational inertia of disk about diameter

Now I see your question: How to find the rotational inertia of a disk spinning about a diameter. If you would like help with the integral, post what you've got and someone will give you a hand.

But the smart way is to use the perpendicular axis theorem.

Note:
[tex]\frac{1}{2}MR^2[/tex]
is the rotational inertia of a disk rotating about a perpendicular axis through its center.
[tex]\frac{1}{4}MR^2[/tex]
is the rotational inertia of a disk rotating about a diameter. The perpendicular axis theorem gives a simple way to calculate one from the other. Here's a link that explains it: http://hyperphysics.phy-astr.gsu.edu/hbase/perpx.html
 

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