Moment of Inertia of a Hemispherical Shell

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SUMMARY

The moment of inertia of a hemispherical shell about the z-axis is derived from the mass distribution given by σ(x,y,z) = (σ0/R^2)(x^2+y^2). The total mass of the shell is calculated as 4πR^2σ0/3. The correct moment of inertia is determined to be 16πR^4σ0/15, following integration of the formula ∫ r^2 dm, where r is defined as Rsinϕ. The initial miscalculation was attributed to a misunderstanding of the cosine function, specifically that cos(0) equals 1.

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Prompt: Find the moment of inertia about the z-axis of the hemispherical shell of problem II-6.

Additional Info.:

-Problem II-6 states: the distribution of mass on the hemispherical shell z=(R^2-x^2-y^2)^1/2 is given by o(x,y,z) = (o/R^2)(x^2+y^2) where σ0 is a constant. Find an expression in terms of o and R for the total mass of the shell.

-My solution to II-6 (verified by the text): 4(pi)R2σ0/3.

Solution Attempts:


1. Looked up a formula for the moment of inertia of a hemisphere, 2mr^(2)/5, where m is mass and r is radius. This gives us 8(pi)R^(4)o/15, which is off by a factor of 2.

2. Found another formula ∫ r^2 dm. Simplified ∫ dm into σ0R2∫∫sin3ϕ dϕ dθ. Took r to mean distance from the z-axis and not radius (it was not specified where I found this formula). Let r=psinϕ, or in this case r=Rsinϕ. Determined ∫ r^2 dm = σ0R4∫∫sin5ϕ dϕ dθ. Tried to integrate this and got:
-5 Cos[x]...5 Cos[3 x]...Cos[5 x]
---------- + ----------- - ----------
...8...48.....80
over the integral [O,pi/2], which equals zero.

Real Solution: 16(pi)R^(4)o/15
 
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It looks like you just integrated incorrectly. Mathematica says
$$\int_0^{2\pi}\int_0^{\pi/2} \sin^5\phi \,d\phi\,d\theta = \frac{16\pi}{15}$$which is what you want.

Actually, it looks like you integrated correctly but mistakenly thought cos 0 is 0, but it's equal to 1.
 
cos(0) is equal to 1? No way! Haha, thanks very much vela. A teacher of mine once said a mathematician spends most of his time searching for that missing factor of 2.
 

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