p-Laplacian

In mathematics, the p-Laplacian, or the p-Laplace operator, is a quasilinear elliptic partial differential operator of 2nd order. It is a nonlinear generalization of the Laplace operator, where p is allowed to range over 1 < p < \infty. It is written as

\Delta_p u:=\nabla \cdot (|\nabla u|^{p-2} \nabla u).

Where the |\nabla \cdot |^{p-2} is defined as

\quad |\nabla u|^{p-2} = \left[ \textstyle \left(\frac{\partial u}{\partial x_1}\right)^2 
+ \cdots + \left(\frac{\partial u}{\partial x_n}\right)^2 
\right]^\frac{p-2}{2}


In the special case when p=2, this operator reduces to the usual Laplacian. [1] In general solutions of equations involving the p-Laplacian do not have second order derivatives in classical sense, thus solutions to these equations have to be understood as weak solutions. For example, we say that a function u belonging to the Sobolev space W^{1,p}(\Omega) is a weak solution of

 \Delta_p u=0 \mbox{ in } \Omega

if for every test function \varphi\in C^\infty_0(\Omega) we have

 \int_\Omega |\nabla u|^{p-2} \nabla u\cdot \nabla\varphi\,dx=0

where \cdot denotes the standard scalar product.

Energy formulation

The weak solution of the p-Laplace equation with Dirichlet boundary conditions

\begin{cases}
-\Delta_p u = f& \mbox{ in }\Omega\\
u=g & \mbox{ on }\partial\Omega
\end{cases}

in a domain \Omega\subset\mathbb{R}^N is the minimizer of the energy functional

J(u) = \int_\Omega |\nabla u|^p \,dx-\int_\Omega f\,u\,dx

among all functions in the Sobolev space W^{1,p}(\Omega) satisfying the boundary conditions in the trace sense.[1] In the particular case f=1, g=0 and \Omega is a ball of radius 1, the weak solution of the problem above can be explicitely computed and is given by

u(x)=C\, \left(1-|x|^\frac{p}{p-1}\right)

where C is a suitable constant depending on the dimension N an on p only. Observe that for p>2 the solution is not twice differentiable in classical sense.

Notes

  1. 1 2 Evans, pp 356.

Sources

Further reading

This article is issued from Wikipedia - version of the Friday, January 08, 2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.