Coarea formula

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In the mathematical field of geometric measure theory, the coarea formula expresses the integral of a function over an open set in Euclidean space in terms of the integral of the level sets of another function. A special case is Fubini's theorem, which says under suitable hypotheses that the integral of a function over the region enclosed by a rectangular box can be written as the iterated integral over the level sets of the coordinate functions. Another special case is integration in spherical coordinates, in which the integral of a function on Rn is related to the integral of the function over spherical shells: level sets of the radial function. The formula plays a decisive role in the modern study of isoperimetric problems.

For smooth functions the formula is a result in multivariate calculus which follows from a simple change of variables. More general forms of the formula for Lipschitz functions were first established by Herbert Federer (Federer 1959), and for BV functions by Fleming & Rishel (1960).

A precise statement of the formula is as follows. Suppose that Ω is an open set in Rn, and u is a real-valued Lipschitz function on Ω. Then, for an L1 function g,

\int _{\Omega }g(x)|\nabla u(x)|\,dx=\int _{{-\infty }}^{\infty }\left(\int _{{u^{{-1}}(t)}}g(x)\,dH_{{n-1}}(x)\right)\,dt

where Hn  1 is the (n  1)-dimensional Hausdorff measure. In particular, by taking g to be one, this implies

\int _{\Omega }|\nabla u|=\int _{{-\infty }}^{\infty }H_{{n-1}}(u^{{-1}}(t))\,dt,

and conversely the latter equality implies the former by standard techniques in Lebesgue integration.

More generally, the coarea formula can be applied to Lipschitz functions u defined in Ω  Rn, taking on values in Rk where k < n. In this case, the following identity holds

\int _{\Omega }g(x)|J_{k}u(x)|\,dx=\int _{{{\mathbb  {R}}^{k}}}\left(\int _{{u^{{-1}}(t)}}g(x)\,dH_{{n-k}}(x)\right)\,dt

where Jku is the k-dimensional Jacobian of u.

Applications

  • Taking u(x) = |x  x0| gives the formula for integration in spherical coordinates of an integrable function ƒ:
\int _{{{\mathbb  {R}}^{n}}}f\,dx=\int _{0}^{\infty }\left\{\int _{{\partial B(x_{0};r)}}f\,dS\right\}\,dr.
\left(\int _{{{\mathbb  {R}}^{n}}}|u|^{{n/(n-1)}}\right)^{{{\frac  {n-1}{n}}}}\leq n^{{-1}}\omega _{n}^{{-1/n}}\int _{{{\mathbb  {R}}^{n}}}|\nabla u|
where ωn is the volume of the unit ball in Rn.

See also

References

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