Determining Moment of Inertia of a sphere.

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Homework Help Overview

The discussion revolves around determining the moment of inertia of a sphere about its central axis, following an initial exploration of the moment of inertia for a cylinder. The original poster expresses difficulty in transitioning from the cylinder to the sphere.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants suggest using spherical coordinates and integrating over small volume elements. There are discussions about dividing the sphere into hemispheres and considering the moment of inertia as a sum of disks. Questions arise regarding the choice of coordinate system and the setup of the integral.

Discussion Status

Some participants have offered guidance on the use of spherical coordinates and the importance of correctly defining volume elements. There is an ongoing exploration of different methods to approach the problem, with no explicit consensus on a single method yet.

Contextual Notes

The original poster has successfully calculated the moment of inertia for a cylinder but is struggling with the sphere. There is a mention of potential confusion regarding the integration process and the choice of multiplying by two when considering hemispheres.

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Determining Moment of Inertia of a Sphere

I'm having some troubles determining the moment of inertia of a sphere about it's central axis. My original question was to calculate it for a cylinder, which I've done, but I'd like to know how to find it for a sphere.
Here is the problem solved for a cylinder:

Problem:
A uniform solid cylinder has radius R, mass M, and length L. Calculate its moment of inertia about its central axis (the z axis).

Solution:
I divided the cylinder into infinitesimally small layers because I knew that [tex]dV = (2\pi*r*dr)*L[/tex]. From here I calculated the integral [tex]I = \int \rho*r^2 dV = \int_{0}^R \rho*r^2*(2\pi*r*L)dr = 2*\pi*\rho*L*R^4[/tex]
I substituted [tex]\frac {M}{\pi*R^2*L}[/tex] (or [tex]\frac{M}{V}[/tex]) for [tex]\rho[/tex] into the equation to get [tex]I = \frac{1}{2}*\pi*(\frac {M}{\pi*R^2*L})*L*R^4 = \frac{1}{2}*M*R^2[/tex]

I understand this, but when I tried to get it as a sphere I ended up getting the wrong answer. Could anyone please show me how to start the problem with a sphere?
 
Last edited:
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Do it in spherical coordinates, being careful to take the sin(theta) for each little volume piece (since the spherical r value is from the origin, not from the axis of rotation). And be careful to use the correct value for dV in spherical coordinates.
 
For the solid spere, I like to add up the moment of inertia of a bunch of disks form -R to R.
 
How did you try to perform your integral for the sphere? Think of your choice of coordinate system--hint: spherical polar coordinates.

damn: really should have refreshed quicker!
 
Couldn't I divide the sphere into a hemisphere and multiply it by 2? E.G. [tex]2*\pi*\int_{0}^R (\sqrt{R^2-r^2}*r^2)*r^2 dr[/tex] Where R is the radius of the sphere. So essentially I'm adding a bunch of [tex]\pi*r^2[/tex] (circles) to get a half of a sphere. Then multiplying the whole thing times two.
 
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hmm, why don't you show a little more work so that it is easier to follow.
one thing though, you might want to reconsider muliplying it by two--think about it.
 
I have no idea how to integrate that, so I don't have much work to show. The idea makes sense in my head, but I don't know how to follow through with it.
 

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