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The - P
_{0}(x) = 1 - P
_{1}(x) = x - P
_{n+1}(x) = ( (2n+1)xP_{n}(x)-nP_{n-1}(x) ) / (n+1)
where P - Fields that adhere to
**Laplace's Equation**: ∇^{2}*f*= 0, where*f*is a scalar field. - Phenomena subject to an Inverse Square Law.
- Multipole Expansions of Gravitational Potential for non-spherical masses (e.g., as uses J
_{2}). - General Relativity.
(Items in this list of applications are not necessarily distinct from each other.) mathematics,gravity) |