Partial Sphere Moment (Part 2)

A partial sphere, described below, has radius R R and mass M M .

x = r c o s θ s i n ϕ y = r s i n θ s i n ϕ z = r c o s ϕ 0 r R 0 θ 2 π π 4 ϕ 3 π 4 \large{x = r \, cos \theta \, sin \phi \\ y = r \, sin \theta \, sin \phi \\ z = r \, cos \phi \\ 0 \leq r \leq R \\ 0 \leq \theta \leq 2 \pi \\ \frac{\pi}{4} \leq \phi \leq \frac{3 \pi}{4}}

The object's moment of inertia with respect to the z z -axis can be expressed as:

I = A B M R 2 \large{I = \frac{A}{B} \, M \, R^2}

If A A and B B are positive co-prime integers, what is A + B A + B ?


The answer is 3.

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1 solution

Otto Bretscher
Nov 24, 2018

This works out very nicely! Thank you for posting!

Assuming a constant density ρ \rho , the moment of inertia comes out to be I z = W ρ ( x 2 + y 2 ) d V = ρ 0 2 π π / 4 3 π / 4 0 R r 4 sin 3 ϕ d r d ϕ d θ = ρ × 2 π × 5 3 2 × R 5 5 I_z= \int_W \rho (x^2+y^2) dV= \rho\int_{0}^{2\pi}\int_{\pi/4}^{3\pi/4}\int_{0}^{R}r^4\sin^3\phi dr d\phi d\theta=\rho \times 2\pi\times \frac{5}{3\sqrt{2}}\times \frac {R^5}{5} and the mass is M = W ρ d V = ρ 0 2 π π / 4 3 π / 4 0 R r 2 sin ϕ d r d ϕ d θ = ρ × 2 π × 2 × R 3 3 M=\int_W \rho dV= \rho \int_{0}^{2\pi}\int_{\pi/4}^{3\pi/4}\int_{0}^{R}r^2\sin\phi dr d\phi d\theta=\rho \times 2\pi\times \sqrt{2}\times \frac {R^3}{3} so that I z M = 1 2 R 2 \frac{I_z}{M}=\frac{1}{2}R^2 and the answer is 1 + 2 = 3 1+2=\boxed{3} .

I will add this to me repertoire of homework problems in calculus, if I may.

Feel free, and thanks for the solution. I was amused when I found that this yielded the same answer as for a disk.

Steven Chase - 2 years, 6 months ago

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