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Double layer potential

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Inpotential theory, an area ofmathematics, adouble layer potential is a solution ofLaplace's equation corresponding to theelectrostatic ormagnetic potential associated to adipole distribution on a closed surfaceS in three-dimensions. Thus a double layer potentialu(x) is a scalar-valued function ofxR3 given byu(x)=14πSρ(y)ν1|xy|dσ(y){\displaystyle 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} )}whereρ denotes the dipole distribution,/∂ν denotes the directional derivative in the direction of the outward unit normal in they variable, and dσ is the surface measure onS.

More generally, a double layer potential is associated to ahypersurfaceS inn-dimensionalEuclidean space by means ofu(x)=Sρ(y)νP(xy)dσ(y){\displaystyle u(\mathbf {x} )=\int _{S}\rho (\mathbf {y} ){\frac {\partial }{\partial \nu }}P(\mathbf {x} -\mathbf {y} )\,d\sigma (\mathbf {y} )}whereP(y) is theNewtonian kernel inn dimensions.

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