Spherical mean

The spherical mean of a function $u$ (shown in red) is the average of the values $u(y)$ (top, in blue) with $y$ on a "sphere" of given radius around a given point (bottom, in blue).

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 Rⁿ 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

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

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

$\frac{1}{{\omega }_{n-1}}\underset{\Vert y\Vert =1}{\int }u(x+ry)\mathrm{d}S(y)$

where ω_n−1 is the area of the (n − 1)-sphere of radius 1.

The spherical mean is often denoted as

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

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 $$r\to \underset{\partial B(x,r)}{\int }-u(y)\mathrm{d}S(y)$$ 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 $\underset{t}{\overset{2}{\partial }}u=c^2\mathrm{\Delta }u$ in odd space dimension. The result, known as Kirchhoff's formula, is derived by using spherical means to reduce the wave equation in ${ℝ}^n$ (for odd $n$) to the wave equation in $ℝ$, and then using d'Alembert's formula. The expression itself is presented in wave equation article.
• If $U$ is an open set in ${ℝ}^n$ and $u$ is a C² 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 $$u(x)=\underset{\partial B(x,r)}{\int }-u(y)\mathrm{d}S(y).$$ This result can be used to prove the maximum principle for harmonic functions.

References

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External links

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