Did I do this right or get lucky? Deriving spherical shell moment of inertia

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SUMMARY

The moment of inertia of a spherical shell is derived using the integral formula I = ∫(r² dm). The user correctly identifies the mass density as φ = M/(4πR²) and integrates over half the sphere, leading to the result I = (2/3)MR². This calculation is validated through the integration of sin(θ) and the appropriate limits for θ and R. The approach is confirmed as correct, demonstrating a solid understanding of the principles involved in deriving the moment of inertia for a spherical shell.

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  • Understanding of moment of inertia concepts
  • Familiarity with integral calculus
  • Knowledge of spherical coordinates
  • Basic physics principles related to mass distribution
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  • Study the derivation of moment of inertia for different shapes, such as solid spheres and cylinders
  • Learn about the application of spherical coordinates in physics problems
  • Explore advanced integration techniques in calculus
  • Investigate the physical significance of mass density in rotational dynamics
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Students in high school physics, particularly those studying mechanics and rotational motion, as well as educators looking for clear examples of moment of inertia calculations.

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Homework Statement


Basically just to find moment of inertia of a spherical shell


Homework Equations


Moment of Inertia = Int(r^2 dm)


The Attempt at a Solution



I am in 12th grade and don't know much about integrals? Did I get lucky or am I right?

I = Int(r^2dM)

dM= (phi)(dA)

I = Int(r^2 phi dA)

Pull out phi, which equals M/4piR^2

I started by looking at half a sphere so I made that M/2piR^2. To get dA I figured you think of a bunch of hoops all going up to one point with a circumferance of 2piR, as you get higher up the radius changes however. A triangle says that R sin theta will get you the new radiuses, so for dA I wrote the integral of 2 pi R sin theta, dTheta. I put that in as dA, this R is a constant so now I have (M 2 pi R)/(2 pi R ^2) on the outside which cancels to M/R

Now I have

(M/R) Int(r^2 sin Theta, dTheta, dR) the R goes from 0 to R the theta from 0 to pi/2. The integral of sin Theta over that integral is 1, so it ends up

(MR^3)/(3R)

R's cancel

MR^2/3

That's half a sphere so multiply by 2

2/3 M R^2

Was that luck or does that work?
 
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I would use Cartesian co-ordinates. Put the centre of the sphere at the origin. Divide the sphere into thin rings of area [itex]dA = 2\pi y dz[/itex] and express y as a function of z.

See this calculation for a solid sphere: http://hyperphysics.phy-astr.gsu.edu/hbase/isph.html#sph

AM
 

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