Derivation of the moment of inertia of a cylinder

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SUMMARY

The discussion focuses on the derivation of the moment of inertia of a sphere using the shell method, contrasting it with the disk method. The user initially attempts to derive the moment of inertia as I = 3/5mr² but realizes the need for correction to I = 2/5mr². Key insights reveal that the confusion arises from the dual meanings of 'r' in different contexts, necessitating a proper setup for integration. The correct approach involves using spherical coordinates and integrating over the volume element to accurately compute the moment of inertia.

PREREQUISITES
  • Understanding of moment of inertia concepts
  • Familiarity with integration techniques in calculus
  • Knowledge of spherical coordinates
  • Experience with volume elements in three-dimensional space
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  • Study the derivation of moment of inertia using spherical coordinates
  • Learn about the disk method for calculating moment of inertia
  • Explore the concept of volume elements in calculus
  • Investigate the differences between shell and disk methods in physics
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Physics students, mechanical engineers, and anyone interested in understanding the derivation of moment of inertia for various shapes, particularly spheres and cylinders.

SHawking
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First, this is not a homework assignment even though it may seem like a homework type question.

I have no problem with the derivation of the moment of inertia of a cylinder but am having more trouble with a sphere. I completely understand the often referenced disk method, but, I would like to take a shell method approach. THe following work is wrong conceptually, I think mathematically it is fine, and I hope someone can point me in the right direction. I don't see what one would need to do it using discs, and am assuming that some slight variation on the following should work:
I=\intr2dm
p=dm/dv
dvp=dm
I=\intr2pdv
v=4/3\pir3
dv=4\pir2dr
I=\intr2p4\pir^2dr
I=4\pip\intr^4dr (Evluated between 0 and R)
I=4\pipR5/5
p=m/v=m/(4/3 \pi r3)
Plugging that in and simplifying I get
I=3/5mr2, though I need 2/5mr2.
I think the problem lies in my set up, conceptually, and that I need to set up an equation somewhere subtracting two values (R from r?) though I am not sure.

If you could help me out I would really appreciate it.


And again, I understand and have no problem with the disk method for this, I am just trying to figure out what this method is not working.


Thanks!
 
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The problem is that you are mixing up two meanings of 'r'.

SHawking said:
I=\intr2dm
Here 'r' refers to the distance from the axis of rotation.
v=4/3\pir3
Here 'r' refers to the radius of the sphere. Big difference!

That's why using a 'shell method' is not such a good idea. What's the moment of inertia of a shell? The various parts are all at different distances from the axis, so it's not a trivial integration.
 
For the record, here is one way how you should proceed to determine the moment of inertia of a ballof radius R:

Volume element:
dv=r^{2}\sin\phi{d\phi}{d\theta}dr
Distance d to axis:
d=r\sin\phi
Thus,
I=\int{d}^{2}dm=\rho\int_{0}^{R}\int_{0}^{\pi}\int_{0}^{2\pi}r^{4}\sin^{3}\phi{d\theta}{d\phi}dr=2\pi\rho\int_{0}^{R}\int_{0}^{\pi}r^{4}(\sin\theta-\sin\theta\cos^{2}\theta)d\phi{dr}=2\pi\rho\int_{0}^{R}r^{4}(2-\frac{2}{3})dr=\frac{8\pi\rho}{3}\int_{0}^{R}r^{4}dr=\frac{2}{5}Mr^{2}
 
Last edited:

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