Spherical mean
# Spherical mean

In mathematics, the spherical mean of a function around a point is the average of all values of that function on a sphere of given radius centered at that point.

## Definition

Consider an open set U in the Euclidean space $R^n$ and a continuous function u defined on U with real or complex values. Let x be a point in U and r > 0 be such that the closed ball B(x, r) of center x and radius r is contained in U. The spherical mean over the sphere of radius r centered at x is defined as

    ${\frac {1}{\omega _{n-1}(r)}}\int \limits _{\partial B(x,r)}\!u(y)\,\mathrm {d} S(y)$

where ∂B(x, r) is the (n − 1)-sphere forming the boundary of B(x, r), dS denotes integration with respect to spherical measure and $ω_{n−1}(r)$ is the "surface area" of this (n − 1)-sphere.

Equivalently, the spherical mean is given by

    ${\frac {1}{\omega _{n-1}}}\int \limits _{\|y\|=1}\!u(x+ry)\,\mathrm {d} S(y)$

where $ω_{n−1}$ is the area of the (n − 1)-sphere of radius 1.

The spherical mean is often denoted as

    $\int \limits _{\partial B(x,r)}\!\!\!\!\!\!\!\!\!-\,u(y)\,\mathrm {d} S(y).$

The spherical mean is also defined for Riemannian manifolds in a natural manner.

## Properties and uses

* From the continuity of $u$ it follows that the function $r\to \int \limits _{\partial B(x,r)}\!\!\!\!\!\!\!\!\!-\,u(y)\,\mathrm {d} S(y)$ is continuous, and that its limit as $r\to 0$ is $u(x).$
* Spherical means can be used to solve the Cauchy problem for the wave equation $\partial _{t}^{2}u=c^{2}\,\Delta u$ in odd space dimension. The result, known as Kirchhoff's formula, is derived by using spherical means to reduce the wave equation in $\mathbb {R} ^{n}$ (for odd $n$) to the wave equation in $\mathbb {R}$, and then using d'Alembert's formula. The expression itself is presented in wave equation article.
* If $U$ is an open set in $\mathbb {R} ^{n}$ and $u$ is a $C^2$ function defined on $U$, then $u$ is harmonic if and only if for all $x$ in $U$ and all $r>0$ such that the closed ball $B(x,r)$ is contained in $U$ one has $u(x)=\int \limits _{\partial B(x,r)}\!\!\!\!\!\!\!\!\!-\,u(y)\,\mathrm {d} S(y).$ This result can be used to prove the maximum principle for harmonic functions.
