Eckmann–Hilton duality: Difference between revisions
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In [[potential theory]], an area of [[mathematics]], a '''double layer potential''' is a solution of [[Laplace's equation]] corresponding to the [[electrostatic potential|electrostatic]] or [[magnetic potential]] associated to a [[dipole]] distribution on a closed surface ''S'' in three-dimensions. Thus a double layer potential ''u''('''x''') is a scalar-valued function of '''x''' ∈ '''R'''<sup>3</sup> given by | |||
:<math>u(\mathbf{x}) = \frac {-1} {4\pi} \int_S \rho(\mathbf{y}) \frac{\partial}{\partial\nu}\frac{1}{|\mathbf{x}-\mathbf{y}|} \,d\sigma(\mathbf{y})</math> | |||
where ρ denotes the dipole distribution, ∂/∂ν denotes the directional derivative in the direction of the outward unit normal in the ''y'' variable, and dσ is the surface measure on ''S''. | |||
More generally, a double layer potential is associated to a [[hypersurface]] ''S'' in ''n''-dimensional [[Euclidean space]] by means of | |||
:<math>u(\mathbf{x}) = \int_S \rho(\mathbf{y})\frac{\partial}{\partial\nu} P(\mathbf{x}-\mathbf{y})\,d\sigma(\mathbf{y})</math> | |||
where ''P''('''y''') is the [[Newtonian kernel]] in ''n'' dimensions. | |||
==See also== | |||
*[[Potential theory]] | |||
*[[Electrostatics]] | |||
*[[Laplacian of the indicator]] | |||
==References== | |||
* {{citation|first1=Richard|last1=Courant|authorlink1=Richard Courant|first2=David|last2=Hilbert|authorlink2=David Hilbert|title=Methods of Mathematical Physics, Volume II|publisher=Wiley-Interscience|year=1962}}. | |||
* {{Citation | last1=Kellogg | first1=O. D. | title=Foundations of potential theory | publisher=[[Dover Publications]] | location=New York | isbn=978-0-486-60144-1 | year=1953}}. | |||
* {{springer|id=d/d033880|title=Double-layer potential|first=I.A.|last=Shishmarev}}. | |||
* {{springer|id=m/m065210|title=Multi-pole potential|first=E.D.|last=Solomentsev}}. | |||
[[Category:Potential theory]] |
Latest revision as of 10:11, 26 September 2013
In potential theory, an area of mathematics, a double layer potential is a solution of Laplace's equation corresponding to the electrostatic or magnetic potential associated to a dipole distribution on a closed surface S in three-dimensions. Thus a double layer potential u(x) is a scalar-valued function of x ∈ R3 given by
where ρ denotes the dipole distribution, ∂/∂ν denotes the directional derivative in the direction of the outward unit normal in the y variable, and dσ is the surface measure on S.
More generally, a double layer potential is associated to a hypersurface S in n-dimensional Euclidean space by means of
where P(y) is the Newtonian kernel in n dimensions.
See also
References
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