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Sobolev Norm and Sobolev Spaces

Sobolev Norm and Sobolev Spaces

Definition1

Sobolev Space

Let ΩRn\Omega \subset \mathbb{R}^{n} be an open set. For positive integers mm and 1p1\le p \le \infty, the function space defined as follows is called the Sobolev space.

Wm,p(Ω):={uLp(Ω):DαuLp(Ω)0αm} W^{m, p}(\Omega):=\left\{ u \in L^{p}(\Omega) : D^\alpha u \in L^{p}(\Omega)\quad \forall 0\le |\alpha | \le m \right\}

Here, α\alpha is a multi-index, DαuD^\alpha u is a weak derivative, and LpL^{p} is a Lebesgue space.

Sobolev Norm

For positive integers mm and 1p1\le p \le \infty, let us define the function m,p\left\| \cdot \right\|_{m,p} as follows.

um,p=(0αmDαupp)1p,1p< \|u\|_{m,p} =\left( \sum\limits_{0\le |\alpha| \le m } \|D^\alpha u \|^p_{p} \right)^{\frac{1}{p}}, \quad 1\le p<\infty

um,=max0αmDαu,p= \|u\|_{m,\infty}= \max\limits_{0\le |\alpha| \le m} \|D^\alpha u\|_\infty, \quad p=\infty

This becomes the norm of the Sobolev space.

Explanation

Simply put, the Sobolev space is a set of functions whose derivatives up to the mm-th order all belong to LpL^{p}. While the LpL^{p} space has useful properties and is an important space, it might be somewhat insufficient for solving differential equations. We need to consider spaces with more properties than the LpL^{p} space, and that is precisely the Sobolev space.

Clearly, if m=0m=0 then W0,p=LpW^{0, p}=L^{p}. Also, since C0C_{0}^\infty is dense in LpL^{p}, when 1p<1 \le p < \infty then W00, p=LPW_{0}^{0,\ p}=L^P. Additionally, the following embedding exists, making Wm,pW^{m, p} treatable as a subspace of LpL^{p}.

W0m,p(Ω)Wm,p(Ω)Lp(Ω) W_{0}^{m, p}(\Omega) \to W^{m, p}(\Omega) \to L^{p}(\Omega)

The following three function spaces all have the Sobolev norm m,p\left\| \cdot \right\|_{m,p}. For positive integers mm and 1p1\le p \le \infty,

Wm,p(Ω):={uLp(Ω):DαuLp(Ω)0αm} \begin{equation} W^{m, p}(\Omega):=\left\{ u \in L^{p}(\Omega) : D^\alpha u \in L^{p}(\Omega)\quad \forall 0\le |\alpha | \le m \right\} \end{equation}

Hm,p(Ω):=the completion of {uCm(Ω):um,p<} \begin{equation} H^{m, p}(\Omega):= \text{the completion of } \left\{ u \in C^m(\Omega) : \|u\|_{m, p} < \infty \right\} \end{equation}

W0m,p(Ω):=the closure of C0(Ω) in Wm,p(Ω) \begin{equation} W_{0}^{m, p}(\Omega):= \text{the closure of } C^\infty_{0}(\Omega) \text{ in } W^{m, p}(\Omega) \end{equation}

Here, (1)(1)~(3)(3) are called Sobolev spaces. Hm,pH^{m, p} and Wm,pW^{m, p} can actually be shown to be the same.

Symbols used to denote the Sobolev space include Hm,p,Wm,p,Pm,p,LpmH^{m, p}, W^{m, p}, P^{m, p}, L_{p}^{m}, among others. Also, before the name Sobolev space became established, it was sometimes called a Beppo Levi space.

Properties

(a) Sobolev space is a Banach space.

(b) When 1p<1\le p <\infty, the Sobolev space is separable.

(c) When 1p<1\le p < \infty, the Sobolev space is reflexive and uniformly convex.


  1. Ole Christensen, Functions, Spaces, and Expansions: Mathematical Tools in Physics and Engineering (2010), p59-61 ↩︎