Solid hemisphere center of mass in spherical coordinates

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SUMMARY

The discussion centers on calculating the center of mass (Cm) of a solid hemisphere with constant density using spherical coordinates. The user initially misapplies the center of mass formula, leading to incorrect results. The correct approach involves integrating the volume element in spherical coordinates, specifically using the formula Cm = 1/V ∫ z (z hat) r^2 sin(θ) dr dθ dφ, which correctly accounts for the density and geometry of the hemisphere. The final result for the center of mass is 3R/8 (z hat).

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  • Familiarity with volume integrals and density concepts
  • Knowledge of vector notation and operations in physics
  • Basic calculus skills, particularly integration techniques
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Ledamien
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Hello,

I am struggling with what was supposed to be the simplest calc problem in spherical coordinates. I am trying to fid the center of mass of a solid hemisphere with a constant density, and I get a weird result.
First, I compute the mass, then apply the center of mass formula. I divide both and voila, obviously wrong result. What is wrong here?

Cm = 1 / M \int \rho r^3 sin \theta dr d\theta d\varphi

M = ρ V → 1/M = 1/ρV

V = 2 \pi R^3 / 3

Cm = 3/ (2 \pi R^3) \int r^3 sin \theta dr d\theta d\varphi

Integrated over:
r → 0 to R
\theta → 0 to \pi/2
\varphi → 0 to 2 \pi

Cm = 3/ (2 \pi R^3) * \pi R^4 / 2
Cm = 3R / 4

So, what do I do wrong?
 
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How did you derive your equation for the Cm?
 
Ledamien said:
\int \rho r^3 sin \theta dr d\theta d\varphi
Isn't there a trig term missing in that integral? There should be one from the Jacobian and another for the fact that you're interested in the displacement in only one Cartesian coordinate.
 
1/M \sum mi ri
1/M\int \rho(r) r dV - this is a volume integral.
1/M\int [\rho(r) r] r^2 dr sin \theta) d\theta d\varphi - this is a volume integral in spherical coordinates.
My idea was that a simple volume integral for a hemisphere, going from 0 to r, 0 to \pi/2 and 0 to 2\pi would be sufficient. As the density is constant I can pull it out of the integral, and \rho/M is simply 1/V, one over the total volume - the same integral but with r^2 instead of r^3. I seem to be missing a 1/2 somewhere, but where?
 
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Ledamien said:
1/M \sum mi ri
1/M\int \rho(r) r dV - this is a volume integral.
What exactly does ri stand for in the first line? What is the appropriate formula to replace it in the second?
 
ri is the vector position of a mass in some direction. I know that by symmetry it should be on the z axis. Should I multiply the whole thing be z hat in spherical (cos\theta - sin\theta). That does not make much sense, and it does not work.
 
Ledamien said:
ri is the vector position of a mass in some direction.
Yes, it's a vector. But you have replaced it by r, the magnitude of the vector. You cannot do that because in the integral the components of the vector in the x and y directions would cancel.
Should I multiply the whole thing be z hat in spherical (cos\theta - sin\theta). That does not make much sense, and it does not work.
Multiplying by sin or cos of theta (depending on which way it's measured) makes sense to me.
 
OK I got it, I skipped a step:
Cm = 1/V\int r (r hat) dV
As I know it's on the z axis:
Cm = 1/V\int z (z hat) dV

z = r cos\theta
dV = r^2 sin\thetadr d\theta d\varphi

Cm = 1/V\intr cos\theta (z hat) r^2 sin\thetadr d\theta d\varphi

I can pull out z hat from the integral.

With V = (2\piR^3)/3, this gives me 3R/8 (z hat).

Well, that was silly...

Thank you guys for your help.
 
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