Gauss variational problem
A variational problem, first studied by C.F. Gauss (1840) , which may be formulated in modern terms as follows. Let $\mu$ be a positive measure in a Euclidean space $\mathbf R^n$, $n\geq3$, of finite energy (cf. Energy of measures), and let
define the Newton potential $U^\mu$ of $\mu$. Out of all measures $\lambda$ with compact support $K\subset\mathbf R^n$ it is required to find a measure $\mu_0$ giving the minimum of the integral
which is the scalar product ($\lambda-2\mu,\lambda$) in the pre-Hilbert space of measures of finite energy.
The importance of the Gauss variational problem consists in the fact that the equilibrium measure (cf. Robin problem) may be obtained as a solution of the Gauss variational problem for a certain choice of $\mu$; for example, $\mu$ may be taken to be a homogeneous mass distribution over a sphere with centre in the coordinate origin that includes $K$.
|||C.F. Gauss, "Allgemeine Lehrsätze in Beziehung auf die im verkehrten Verhältnisse des Quadrats der Entfernung wirkenden Anziehung- und Abstössungs-Kräfte" , Werke , 5 , K. Gesellschaft Wissenschaft. Göttingen (1877) pp. 195–242|
|||N.S. [N.S. Landkov] Landkof, "Foundations of modern potential theory" , Springer (1972) (Translated from Russian)|
|||M. Brélot, "Eléments de la théorie classique du potentiel" , Sorbonne Univ. Centre Doc. Univ. , Paris (1959)|
The measure $\mu_0$ is the projection of $\mu$ on the convex cone of all positive measures $\lambda$, of finite energy, and with support contained in $K$. See also [a1], Chapt. I.XIII for a treatment of this subject.
|[a1]||J.L. Doob, "Classical potential theory and its probabilistic counterpart" , Springer (1984)|
Gauss variational problem. Encyclopedia of Mathematics. URL: http://www.encyclopediaofmath.org/index.php?title=Gauss_variational_problem&oldid=32602