Laplace's equation in spherical co-ords

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SUMMARY

The general solution to Laplace's equation in spherical coordinates is given by the formula: u(r, θ, φ) = ∑(l=0 to ∞) ∑(m=-l to l) (a_{lm}r^{l} + b_{lm}/r^{l+1})P_{lm}(cosθ)e^{imφ}. The coefficients a_{lm} and b_{lm} are determined by the specific boundary conditions of the problem. The limits on the summation, where m ranges from -l to l, correspond to the irreducible representations of SO(3), which have a dimension of 2l + 1, reflecting the properties of angular momentum in physics.

PREREQUISITES
  • Understanding of Laplace's equation
  • Familiarity with spherical coordinates
  • Knowledge of Legendre polynomials, P_{lm}
  • Basic concepts of angular momentum in quantum mechanics
NEXT STEPS
  • Study the derivation of Legendre polynomials and their applications
  • Explore boundary value problems in spherical coordinates
  • Learn about the irreducible representations of SO(3)
  • Investigate the physical implications of angular momentum in quantum mechanics
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Mathematicians, physicists, and students studying partial differential equations, particularly those focusing on potential theory and quantum mechanics.

benabean
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I have a simple question about the general solution to Laplace's equation in spherical co-ords.
The general solution is:

u(r, \theta, \phi) = \sum^{\infty}_{l=0}\sum^{l}_{m=-l}\left(a_{lm}r^{l} + \frac{b_{lm}}{r^{l+1}}\right)P_{lm}(cos\theta)e^{im\phi}

(where the a_{lm}, b_{lm} coefficients can be found using the boundary conditions in question.)

My problem lies in trying to understand the limits on the summation \sum^{l}_{m=-l}. Can anyone offer any help on this please?

Thanks for reading, b.
 
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Probably due to the same reason why the irreducible representation of SO(3) has dimension
2\ell + 1 (physicist tends to use j for spin/orbital angular momentum number).
 

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