In mathematics, a Lipschitz domain (or domain with Lipschitz boundary) is a domain in Euclidean space whose boundary is "sufficiently regular" in the sense that it can be thought of as locally being the graph of a Lipschitz continuous function. The term is named after the German mathematician Rudolf Lipschitz.
Let
n\inN
\Omega
Rn
\partial\Omega
\Omega
\Omega
p\in\partial\Omega
H
n-1
p
g:H → R
r>0
h>0
\Omega\capC=\left\{x+y\vec{n}\midx\inBr(p)\capH, -h<y<g(x)\right\}
(\partial\Omega)\capC=\left\{x+y\vec{n}\midx\inBr(p)\capH, g(x)=y\right\}
\vec{n}
H,
Br(p):=\{x\inRn\mid\|x-p\|<r\}
r
C:=\left\{x+y\vec{n}\midx\inBr(p)\capH, {-h}<y<h\right\}.
In other words, at each point of its boundary,
\Omega
A more general notion is that of weakly Lipschitz domains, which are domains whose boundary is locally flattable by a bilipschitz mapping. Lipschitz domains in the sense above are sometimes called strongly Lipschitz by contrast with weakly Lipschitz domains.
A domain
\Omega
p\in\partial\Omega,
r>0
\ellp:Br(p) → Q
\ellp
\ellp
-1 | |
l | |
p |
\ellp\left(\partial\Omega\capBr(p)\right)=Q0;
\ellp\left(\Omega\capBr(p)\right)=Q+;
Q
B1(0)
Rn
Q0:=\{(x1,\ldots,xn)\inQ\midxn=0\};
Q+:=\{(x1,\ldots,xn)\inQ\midxn>0\}.
A (strongly) Lipschitz domain is always a weakly Lipschitz domain but the converse is not true. An example of weakly Lipschitz domains that fails to be a strongly Lipschitz domain is given by the two-bricks domain [1]
Many of the Sobolev embedding theorems require that the domain of study be a Lipschitz domain. Consequently, many partial differential equations and variational problems are defined on Lipschitz domains.