Problem with going from plane polar coordinates to spherical polars/harmonics. I've read that in plane polars, the function 1/R-r where R(R, theta1) and r(r, theta2) are different and at different angles can be expanded by the cosine rule(I think it is) and the binomial expansion. Seems to produce a Legendre series. BUT that's for the case of R and r being in the same plane. If they're not, I THINK that I've read that spherical polar coordinates are needed, and that the expansion becomes a series in spherical harmonics. R(R, theta1, phi1), r(r, theta2, phi2) My source, an old book on
My source, an old book on Elec and Mag goes throug it in about a page and a half, most of which is ... well ... hmmmmm. Anyone got any thoughts ?
Could you post a picture of the text? It might help to see how exactly the material is treated.
@HolsterEmission Rather loud title for the scan of two of the pages.
4-4 Our galaxy is about 10^5 light years across, and the most energetic particles known have an energy of about 10^19eV. How long would it take a proton with this energy to traverse the galaxy as measured in the rest frame of The galaxy ? (10^5 yrs) The particle ? (5 mins)
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