II.4 Boundary Inequalities and the Trace of Functions of W
m,q
61
II.4 Boundary I nequalities and the Trace of Functions of
W
m,q
As a next problem, we wish to investigate if, analogously to what happens
for smooth functions, it is po ssible to ascribe a value at the boundary (the
trace) to functions in W
m,q
(Ω). If Ω is sufficiently regular, the considerations
developed in the preceding section assure that this is certainly true if mq > n,
since, in such a case, every function from W
m,q
(Ω) can be redefined on a
set of zero measure in such a way that it becomes (at least) continuous up to
the boundary. However, if mq ≤ n we can nevertheless prove some inequalities
relating W
m,q
-norms of a smooth function with L
r
-norms of the same function
at the boundary, which will allow us to define, in a suitable sense, the trace
of a function belonging to any Sobol ev space of order (m, q), m ≥ 1. To this
end, given a sufficiently smooth domain with a bounded boundary (locally
Lipschitz, say) we denote by L
q
(∂Ω), 1 ≤ q ≤ ∞ the space of (equivalence
classes of) real functions u defined on ∂Ω and such that
kuk
q,∂Ω
≡
Z
∂Ω
|u|
q
dσ
1/q
< ∞, 1 ≤ q < ∞,
kuk
∞,∂Ω
≡ ess sup
∂Ω
|u| < ∞, q = ∞,
where σ denotes the Lebesgue (n −1)-dimensional measure.
1
It can be proved
that the space L
q
(∂Ω) enjoys all the relevant functional properties of the
spaces L
q
(Ω). In pa rticular, it is a Banach space wi th respect to the norm
k · k
q,∂Ω
, 1 ≤ q ≤ ∞, which is separable for 1 ≤ q < ∞ and reflexive fo r
1 < q < ∞ (see Miranda 1978, §60).
In order to accomplish our objective, we need some preliminary consider-
ations and results that we shall next describe.
We shall often use the classical Gauss divergence theorem for sm ooth vec-
tor functions. It is well known that this theorem certainly holds if the domain
is (piecewise) of class C
1
. However, we need to consider more general sit-
uations and, in this respect, we quote the following result of Neˇcas (1967,
Chapitre 2, Lemme 4.2 and Chapi tre 3, Th´eor`eme 1.1).
Lemma II.4.1 Let Ω be a bounded, locally Lipschitz domain in R
n
. Then
the unit outer normal n exists almost everywhere on ∂Ω (see Lemma II.1.2)
and the following identity holds
Z
Ω
∇ · u =
Z
∂Ω
u ·n,
for a ll vector fields u with components in C
1
(Ω).
1
As usual, if no confusion arises, the infinitesimal surface element dσ in the integral
will be omitted.