Infinite series

Multipole expansion of 1/𝔯

Let ⃗𝖗 =⃗𝐫 βˆ’βƒ—π«β€² and let 𝛼 be the angle between ⃗𝐫 and ⃗𝐫′, so that ⃗𝐫 ⋅⃗𝐫′ =π‘Ÿπ‘Ÿβ€²cos⁑𝛼.1 Then we have the multipole expansion

1𝔯=1π‘Ÿβˆžβˆ‘π‘›=0(π‘Ÿβ€²π‘Ÿ)𝑛𝑃𝑛(cos⁑𝛼)

where 𝑃𝑛(π‘₯) is a Legendre polynomial. vec


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Footnotes

  1. Presented here is the multipole expansion as it pertains to Electrodynamics MOC. ↩