Calculating Quadrupole Moment of Sphere w/ Surface Charge

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SUMMARY

The discussion focuses on calculating the quadrupole moment of a spherical shell with a surface charge density defined as σ = σ₀ cos(θ), where σ₀ is a constant and the sphere has a radius of 'a'. Participants confirm that the monopole moment is zero and the dipole moment is the only non-zero term due to the orthogonality of spherical harmonics. The quadrupole moment is concluded to be zero because the integration of the charge density against the spherical harmonics results in non-contributing terms for l=2. The use of vector products versus dot products is clarified, emphasizing that only the dipole moment remains significant.

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  • Understanding of spherical harmonics and their properties
  • Knowledge of multipole expansion in electrostatics
  • Familiarity with vector calculus, particularly vector products and dot products
  • Basic concepts of surface charge density and its implications in electrostatics
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  • Study the properties of spherical harmonics and their applications in multipole expansions
  • Learn about the mathematical derivation of the quadrupole moment in electrostatics
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1.

Looking for quadrupole moment of spherical shell with surface charge (sigma)=(sigma_o)*cos(theta) and (sigma_o) => constant
Sphere is at the origin with radius=a.

2.

Well, I think I am using the right equation, by integration of the quadrapole moment taken from the quadrupole term, but I am questioning my [(r')^2] factor. 3.

I use vector product I get a zero. I guess a vector crossed with itself is always zero because of no span. I have already found the monopole and dipole (monopole =0), and I think I take the vector product of r', and not the dot product, because the dot product is a scalar... and I found by another theorem that whether it is shell or sphere, the quadrapole and higher terms are zero. So is this where the quadrapole zeroes out?? from the [(r')^2] factor?
 
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i'm pretty sure only the dipole moment should be non-zero. you can write all the moments in terms of the charge density integrated against spherical harmonics. E.g., Y_{0,0} for monopole term, Y_{1,m} for dipole term, Y_{2,m} for quadrupole term, etc. But since the charge density itself is proportional to Y_{1,0} only the l=1 multipole moments should be non-zero due to orthogonality of spherical harmonics.
 

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