Double layer potential

From Wikipedia, the free encyclopedia

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

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}})

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

u({\mathbf  {x}})=\int _{S}\rho ({\mathbf  {y}}){\frac  {\partial }{\partial \nu }}P({\mathbf  {x}}-{\mathbf  {y}})\,d\sigma ({\mathbf  {y}})

where P(y) is the Newtonian kernel in n dimensions.

See also

References

This article is issued from Wikipedia. The text is available under the Creative Commons Attribution/Share Alike; additional terms may apply for the media files.