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Mixed exterior Laplace’s problem
Chérif Amrouche, Florian Bonzom
To cite this version:
Chérif Amrouche, Florian Bonzom. Mixed exterior Laplace’s problem. 2007. �hal-00199734�
Mixed exterior Laplace’s problem
Chérif Amrouche
∗, Florian Bonzom
Laboratoire de mathématiques appliquées, CNRS UMR 5142, Université de Pau et des Pays de l’Adour, IPRA, Avenue de l’Université, 64000 Pau cedex, France
Abstract
In [3], authors study Dirichlet and Neumann problems for the Laplace operator in exterior domains of R
n. This paper extends this study to the resolution of a mixed exterior Laplace’s problem. Here, we give existence, unicity and
regularity results in L
p’s theory with 1 < p < ∞, in weighted Sobolev spaces.
Keywords :Weighted Sobolev spaces ; Laplacian ; Mixed boundary conditions ; Poincaré type inequality
1 Introduction and preliminaries
Let ω
0and ω
1be two compact, disconnected and not empty regions of R
n, n ≥ 2, with Lipschitz-continuous boundaries, respectively, Γ
0and Γ
1and let Ω be the complement of ω
0∪ ω
1. We set Γ = Γ
0∪ Γ
1= ∂Ω.
This paper is devoted to solve the following problem :
(P )
−∆u = f in Ω, u = g
0on Γ
0,
∂u
∂n = g
1on Γ
1.
Since these problems are setted in an exterior domain, we must complete their statements with adequate asymptotic conditions at infinity. We have chosen to impose such conditions by setting our problem in weighted Sobolev spaces where the growth or decay of functions at infinity are expressed by means of weights. These weighted Sobolev spaces provide a correct functional setting for the exterior Laplace equation, in particular because the functions in these spaces satisfy an optimal weighted Poincaré type inequality. This gives them a great advantage over the two families of spaces currently used for the Laplace operator, namely, the completion of D(Ω) for the norm of the gradient in L
p(Ω) and the subspace in L
ploc(Ω) of functions whose gradients belong to L
p(Ω). On one hand, when p ≥ n, some very treacherous Cauchy sequences exist in D(Ω) that do not converge to distributions, a behaviour carefully described in 1954 by Deny and Lions (cf. [5]) but unfortunately overlooked by many authors. These sequences are eliminated in our spaces because we equip
∗Corresponding author. E-mail addresses: [email protected] (C.Amrouche), [email protected] (F. Bonzom).
them with the full Sobolev norm instead of the norm of the gradient alone. On the other hand, this full Sobolev norm avoids the imprecision at infinity inherent to the L
plocnorm. In an unbounded region, it is important to describe sharply the behaviour of functions at infinity and not just their gradient. This is vital from the mathematical point of view, not only because it permits to characterize easily the data from which we can solve our problems, but also because the analysis done here for one exponent of the weight extends readily to a wide range of real exponents. This is even more crucial from the
numerical point of view because in most formulations, the function itself is the primary unknown that engineers discretize, the gradient being only secondary and usually deduced from the function values.
This paper is organized as follows. Sections 2, 3 and 4 are devoted to the study of questions of existence and unicity of the solution respectively in cases p = 2, p > 2 and p < 2 and the section 5 deals with different behaviours at the infinity of the solution according to the data.
We complete this introduction with a short review of the weighted Sobolev spaces and their isomorphisms that we shall use in the sequel. For any integer q we denote by P
qthe space of polynomials in n variables, smaller than or equal to q, with the convention that P
qis reduced to {0} when q is negative.
For any real number p ∈ ]1, +∞[, we denote by p
0the dual exponent of p : 1
p + 1 p
0= 1.
Let x = (x
1, . . . , x
n) be a typical point of R
nand let
r = |x| = (x
21+ · · · + x
2n)
1/2denote its distance to the origin. We shall use two basic weights :
ρ(r) = (1 + r
2)
1/2and lg r = ln(2 + r
2)
Then, for any nonnegative integers n and m and real numbers p > 1, α and β, setting
k = k(m, n, p, α) =
−1 if n
p + α / ∈ {1, . . . , m},
m − n
p − α if n
p + α ∈ {1, . . . , m}, we define the following space :
W
m,pα,β(Ω) = {u ∈ D
0(Ω);
∀λ ∈ N
n: 0 6 |λ| 6 k, ρ
α−m+|λ|(lg r)
β−1D
λu ∈ L
p(Ω);
∀λ ∈ N
n: k + 1 6 |λ| 6 m, ρ
α−m+|λ|(lg r)
βD
λu ∈ L
p(Ω)}.
It is a reflexive Banach space equipped with its natural norm : kuk
Wm,pα,β(Ω)
= ( X
06|λ|6k
kρ
α−m+|λ|(lg r)
β−1D
λuk
pLp(Ω)+ X
k+16|λ|6m
kρ
α−m+|λ|(lg r)
βD
λuk
pLp(Ω))
1/p.
We also define the semi-norm :
|u|
Wm,pα,β(Ω)
= ( X
|λ|=m
kρ
α(lg r)
βD
λuk
pLp(Ω))
1/p.
When β = 0, we agree to drop the index β and denote simply the space by W
m,pα(Ω).
The weights defined previously are chosen so that the space D(Ω) is dense in W
m,pα,β(Ω) and so that theorem 1.1 below is satisfied.
The constants 1 and 2 in ρ(r) and lg r are added so that they do not modify the behaviour of the functions near the origin, in case it belongs to Ω. Thus, the functions of W
m,pα,β(Ω) belong to W
m,p(O) on all bounded domains O contained in Ω. As a consequence, the traces of these functions on Γ,
γ
0, γ
1, . . . , γ
m−1, satisfy the usual trace theorems (cf. Adams [1] or Nečas [8]).
This allows to define in particular the space
◦
W
m,pα,β(Ω) = {v ∈ W
m,pα,β(Ω); γ
0v = γ
1v = · · · = γ
m−1v = 0}.
It can be proved that D(Ω) is dense in W
◦ m,pα,β(Ω) and therefore, its dual space, W
−m,p−α,−β0(Ω) is a space of distributions.
If n ∈ N
∗is the dimension of spaces, we set E = E
n. Now, we define the space Y
p(Ω) = W
−1,p0(Ω) ∩ L
p(Ω) equipped with the following norm :
kuk
Yp(Ω)= (kuk
pW−1,p0 (Ω)
+ kuk
pLp(Ω))
1/p. We easily check that Y
p(Ω) is complete.
We introduce the partition of unity (we use the lemma of Urysohn) : ψ
1, ψ
2∈ C
∞( R
n), 0 ≤ ψ
1, ψ
2≤ 1, ψ
1+ ψ
2= 1 in R
n,
ψ
1= 1 in B
R, supp ψ
1⊂ B
R+1, where R > 0 is such that ω
0∪ ω
1⊂ B
R.
For any v ∈ W
1,p0 0(Ω), we set v
1= ψ
1v and v
2= ψ
2v. We have supp v
1⊂ Ω
R+1= B
R+1∩ Ω ans so v
1∈ W
1,p0(Ω
R+1). Furthermore v
2= 0 on Γ because ψ
2= 0 on Ω
R= B
R∩ Ω, so v
2∈ W
◦ 1,p0
0
(Ω). For f ∈ Y
p(Ω), we set :
∀v ∈ W
1,p0 0(Ω), T
f(v) = Z
ΩR+1
f v
1dx + < f, v
2>,
where < ., . > denotes the duality pairing between W
−1,p0(Ω) and W
◦ 1,p0
0
(Ω).
We easily notice that T
fis well defined, linear and we check that :
∀ϕ ∈ D(Ω), T
f(ϕ) = Z
Ω
f ϕ dx, (1)
and for any f ∈ Y
p(Ω) and v ∈ W
1,p0 0(Ω),
|T
f(v)| ≤ C kf k
Yp(Ω)kvk
W1,p00 (Ω)
, (2)
where C > 0 is a constant which does not depend of f and v.
The next results are demonstrated by Amrouche, Girault and Giroire [2] and
[3] and will be used in the sequel.
Theorem 1.1. Let α and β be two real numbers and m ≥ 1 an integer not satisfying simultaneously :
n
p + α ∈ {1, . . . , m} and (β − 1)p = −1
Let q
0= min(q, m − 1), where q is the highest degree of the polynomials contained in W
m,pα,β(Ω). Then :
i) the semi-norm | . |
Wm,pα,β(Ω)
defined on W
m,pα,β(Ω)/P
q0is a norm equivalent to the quotient norm.
ii) the semi-norm | . |
Wm,pα,β(Ω)
is a norm on W
◦ m,pα,β(Ω), which is equivalent to the full norm k . k
Wm,pα,β(Ω)
.
Theorem 1.2. The following Laplace operators are isomorphisms :
i) ∆ : W
1,p0( R
n)/P
[1−n/p]→ W
−1,p0( R
n) ⊥ P
[1−n/p0], ii) ∆ : W
2,p1( R
n)/P
[1−n/p]→ W
0,p1( R
n) ⊥ P
[1−n/p0], iii) ∆ : W
2,n n−1
1
( R
n)/P
2−n→ (W
0,n n−1
1
( R
n) ∩ W
−1,n n−1
0
( R
n)) ⊥ R , where the symbol ⊥ has the following meaning : for E and F two spaces such that E ⊂ F,
F
0⊥ E = {f ∈ F
0, ∀x ∈ E, < f, x >
F0,F= 0}.
Proposition 1.3. Assume that p > 2 and f ∈ W
−1,p0( R
n) with compact support and satisfying, if n = 2, the compatibility condition
< f, 1 >
W−1,20 (R2),W1,20 (R2)
= 0.
Then, the problem
−∆u = f in R
n,
has a solution u ∈ W
1,20( R
n) ∩ W
1,p0( R
n), unique up to an additive constant if n = 2.
2 Case p=2
We begin to introduce the space
V
2= {v ∈ W
1,20(Ω), v = 0 on Γ
0}.
and to establish a Poincaré type inequality :
Proposition 2.1. There exists a constant C > 0 such that :
∀u ∈ V
2, kuk
W1,20 (Ω)
≤ C |u|
W1,2 0 (Ω). Proof - We use an absurd argument ; so, assume that
∀n ∈ N
∗, ∃ w
n∈ V
2, kw
nk
W1,20 (Ω)
> n |w
n|
W1,2 0 (Ω).
Then the sequence defined by u
n= w
nkw
nk
W1,2 0 (Ω)satisfy
ku
nk
W1,20 (Ω)
= 1 and |u
n|
W1,2 0 (Ω)< 1
n . (3)
Here, we define an other partition of unity :
ϕ
1, ϕ
2∈ C
∞( R
n), 0 ≤ ϕ
1, ϕ
2≤ 1, ϕ
1+ ϕ
2= 1 in R
n, ϕ
1= 1 in B
R1, supp ϕ
1⊂ B
R1+1,
where R
1> 0 is such that ω
1⊂ B
R1and ω
0∩ B
R1+1= ∅. We set u
1n= ϕ
1u
nand u
2n= ϕ
2u
n, so that u
n= u
1n+ u
2n. We deduce by (3) the existence of u ∈ V
2such that :
u
n* u in W
1,20(Ω) and ∇u = 0 in Ω.
As Ω is connected and u ∈ V
2, then u = 0 in Ω and
u
n* 0 in W
1,20(Ω). (4)
Thanks to the Rellich’s compactness theorem, u
n→ 0 in L
2(Ω
R1+1) and thanks to (3), we easily deduce that u
1n→ 0 in W
1,20(Ω). Now, we prove that u
2n→ 0 in W
1,20(Ω). First, we notice that u
2n∈ W
◦ 1,20(Ω). Setting Ω
0= Ω \ B
R1and Ω
0= Ω
0∪ ω
0, we call again u
2nthe restriction of u
2nto Ω
0and we define :
u e
2n= u
2non Ω
0, u e
2n= 0 on ω
0We easily check that e u
2n∈ W
◦ 1,20(Ω
0) with k u e
2nk
W1,20 (Ω0)
= ku
2nk
W1,20 (Ω0)
. Noticing that Ω
0= B
cR1
and applying a result established by Giroire [6], we have :
k u e
2nk
W1,20 (Ω0)
≤ C | u e
2n|
W1,2 0 (Ω0). We easily show that | e u
2n|
W1,20 (Ω0)
→ 0, so in particular ku
2nk
W1,20 (Ω0)
→ 0. To finish, like Ω
0= Ω \ Ω
R1and u
2n= 0 on Ω
R1, we have :
ku
2nk
W1,20 (Ω)
= ku
2nk
W1,20 (Ω0)
→ 0. So, u
2n→ 0 in W
1,20(Ω) which implies that u
n= u
1n+ u
2n→ 0 in W
1,20(Ω), and which contradicts (3). In consequence, we have the result searched.
Theorem 2.2. For any f ∈ Y
2(Ω), g
0∈ H
12(Γ
0) and g
1∈ H
−12(Γ
1), there exists a unique u ∈ W
1,20(Ω) solution of the problem (P) and a constant C > 0 such that
kuk
W1,20 (Ω)
≤ C( kf k
Y2(Ω)+ kg
0k
H12(Γ0)
+ kg
1k
H−12(Γ1)
).
Proof - First, according to [3], there exists a unique u
0∈ W
1,20(Ω
1) where Ω
1= Ω ∪ ω
1, solution of :
(P
D)
( ∆u
0= 0 in Ω
1,
u
0= g
0on Γ
0,
and checking
ku
0|Ωk
W1,20 (Ω)
≤ C kg
0k
H12(Γ0)
.
We notice that like u
0|Ω∈ W
1,20(Ω) and 0 = ∆u
0∈ L
2(Ω), then
∂u
0∂n ∈ H
−12(Γ
1). Moreover, we know that there exists a unique v ∈ V
2solution of the following problem (F V ) :
(F V ) ∀w ∈ V
2, a(v, w) = L(w), where for v, w ∈ V
2,
a(v, w) = Z
Ω
∇v · ∇w dx and L(w) = T
f(w) + < g
1− ∂u
0∂n , w >
Γ1, and where < ., . >
Γ1is the duality pairing H
−12(Γ
1), H
12(Γ
1). Indeed, this result is a simply consequence of the Lax-Milgram theorem and of the propriety 2.1 which shows that the form a is coercive.
Then, we easily check that this solution v ∈ W
1,20(Ω) satisfies
(P
0)
−∆v = f in Ω,
v = 0 on Γ
0,
∂v
∂n = g
1− ∂u
0∂n on Γ
1, and
kvk
W1,20 (Ω)
≤ C (kf k
Y2(Ω)+ kg
1− ∂u
0∂n k
H−12(Γ1)
).
Finally, the function u = u
0|Ω+ v is the solution of (P ) and the estimate searched is a consequence of the two previous inequalities.
3 Case p > 2
We propose the following approach : first we solve the harmonic problem, this will enable us to establish an "inf-sup" condition which in turn will solve the full problem thanks to the theorem of Babuška-Brezzi.
In all this section we suppose p > 2 (except for the subsection 3.5. where we suppose p ≥ 2) and Γ of class C
1,1.
3.1 Resolution of the harmonic problem
Let g
0be in W
1−1 p,p
(Γ
0) and g
1be in W
−1 p,p
(Γ
1). Here, we consider the problem : find u in W
1,p0(Ω) ∩ W
1,20(Ω) solution of
(P
0)
∆u = 0 in Ω, u = g
0on Γ
0,
∂u
∂n = g
1on Γ
1. Theorem 3.1. For any g
0∈ W
1−1 p,p
(Γ
0) and g
1∈ W
−1 p,p
(Γ
1), there exists a unique u ∈ W
1,p0(Ω) ∩ W
1,20(Ω), solution of (P
0), and we have :
kuk
W1,p0 (Ω)
+ kuk
W1,20 (Ω)
≤ C ( kg
0k
W1−
1 p,p
(Γ0)
+ kg
1k
W−
1 p,p
(Γ1)
). (5)
Proof - By [3], we know there exists u
0∈ W
1,p0(Ω
1) ∩ W
1,20(Ω
1) solution of (P
D), where we remind that Ω
1= Ω ∪ ω
1, with the following estimate :
ku
0k
W1,p0 (Ω1)
+ ku
0k
W1,20 (Ω1)
6 C kg
0k
W
1−1 p,p
(Γ0)
. (6)
We notice that like u
0|Ω∈ W
1,p0(Ω) and 0 = ∆u
0∈ L
p(Ω), we have
∂u
0∂n ∈ W
−1 p,p
(Γ
1). Moreover
k ∂u
0∂n k
W−
1 p,p
(Γ1)
≤ C kg
0k
W1−
1 p,p
(Γ0)
Then, we are going to show that there exists a unique v in W
1,20(Ω) ∩ W
1,p0(Ω) solution of the following problem :
(P
00)
∆v = 0 in Ω,
v = 0 on Γ
0,
∂v
∂n = g
1− ∂u
0∂n on Γ
1. with the estimate :
kvk
W1,p0 (Ω)
+ kvk
W1,20 (Ω)
6 C ( kg
0k
W1−
1 p,p
(Γ0)
+ kg
1k
W−
1 p,p
(Γ1)
). (7)
As p > 2, g
1− ∂u
0∂n ∈ H
−12(Γ
1) and thanks to theorem 2.2, there exists a unique v ∈ W
1,20(Ω) solution of (P
00) and checking (7) with p = 2. There stays to show that v ∈ W
1,p0(Ω). For this, we use the partition of the unity
previously defined :
ϕ
1, ϕ
2∈ C
∞( R
n), 0 ≤ ϕ
1, ϕ
2≤ 1, ϕ
1+ ϕ
2= 1 in R
n, ϕ
1= 1 in B
R1, supp ϕ
1⊂ B
R1+1,
where R
1> 0 is such that ω
1⊂ B
R1and ω
0∩ B
R1+1= ∅. We set v
1= ϕ
1v, v
2= ϕ
2v and
v e
2= v
2in Ω, v e
2= 0 in ω
1.
We remind that v
2∈ W
◦ 1,20(Ω) and so that v e
2∈ W
1,20(Ω
1). Moreover, we have :
−∆v
2= ∆v
1= v ∆ψ
1+ 2∇ψ
1· ∇v := f
1in Ω.
Setting
f e
1= f
1in Ω, f e
1= 0 in ω
1,
it is obvious that f e
1∈ L
2(Ω
1) with supp f e
1⊂ Ω
R1+1and that −∆ v e
2= f e
1in Ω
1.
Now, we set s = v e
2and we are going to show that s ∈ W
1,p0(Ω
1). For this, we define an other partition of the unity :
ξ
1, ξ
2∈ C
∞( R
n), 0 ≤ ξ
1, ξ
2≤ 1, ξ
1+ ξ
2= 1 in R
n,
ξ
1= 1 in B
R0, supp ξ
1⊂ B
R0+1,
where R
0> 0 is such that ω
0⊂ B
R0and ω
1∩ B
R0+1= ∅. We set s
1= ξ
1s and s
2= ξ
2s, and we notice that :
−∆s
2= f e
1+ ∆s
1= f e
1+ s ∆ξ
1+ 2∇ξ
1· ∇s := F in Ω
1. Finally, we set :
s e
2=
s
2in Ω
1,
0 in ω
0, and F e =
F in Ω
1, 0 in ω
0.
We have s e
2∈ W
1,20( R
n) because s
2∈ W
◦ 1,20(Ω
1), F e ∈ L
2( R
n) with supp F e ⊂ Ω
R0+1∩ Ω
R1+1, and also −∆ s e
2= F e in R
n.
i) Case 2 < p ≤ 2n
n − 2 and n ≥ 3 or p > 2 and n = 2.
Thanks to the injections of Sobolev, , we have F e ∈ W
−1,p0( R
n). In consequence, thanks to the theorem 1.2 i), (there is no condition of compatibility because p > 2), we show that s e
2∈ W
1,p0( R
n) and so s
2∈ W
1,p0(Ω
1) and we easily check that :
k s e
2k
W1,p0 (Rn)/P[1−n
p]
≤ C kg
1− ∂u
0∂n k
W−
1 p,p
(Γ1)
. (8)
Outside of B
R0+1, ξ
1= 0 so s = s
2and the trace of s
2on ∂B
R0+1belongs to W
1−p1,p(∂B
R0+1). So s checks :
−∆s = f e
1in Ω
R0+1, s = s
2on ∂B
R0+1, s = 0 on Γ
0. Consequently, (see Lions and Magenes [7] ), s ∈ W
1,p(Ω
R0+1) and :
ksk
W1,p(ΩR0 +1)≤ C (k f e
1k
W−1,p(ΩR0 +1)
+ ks
2k
W1−p1,p(∂BR0 +1)
) (9) We deduce of this that s ∈ W
1,p0(Ω
1) ; and with (8) and (9), we have :
ksk
W1,p0 (Ω1)
≤ C kg
1− ∂u
0∂n k
W−
1 p,p
(Γ1)
. (10)
ii) Case n ≥ 3 and p > 2n n − 2 .
The argument used above with p = 2n
n − 2 shows that s ∈ W
1,2n n−2
0
(Ω
1) and we use the same demonstration that i) with s ∈ W
1,2n n−2
0
(Ω
1) instead of s ∈ W
1,20(Ω
1). So, we obtain the result for n = 3, n = 4 and n = 5 if p < 2n
n − 4 ; then we take 2n
n − 4 instead of 2n
n − 2 , and we start again ; so we reach for all dimension, all values of p.
Consequently, we have s = ˜ v
2∈ W
1,p0(Ω
1), v
2∈ W
1,p0(Ω) and kv
2k
W1,p0 (Ω)
≤ C kg
1− ∂u
0∂n k
W
−1 p,p
(Γ1)
. (11)
Outside of B
R1+1, ϕ
1= 0 and v = v
2and the trace of v
2on ∂B
R1+1belongs to W
1−1p,p(∂B
R1+1). So v checks :
∆v = 0 in Ω
R1+1, v = v
2on ∂B
R1+1, ∂v
∂n = g
1− ∂u
0∂n on Γ
1.
In consequence, (see Lions and Magenes [7] ), v ∈ W
1,p(Ω
R1+1) and : kvk
W1,p(ΩR1 +1)≤ C (k g
1− ∂u
0∂n k
W−
1 p,p
(Γ1)
+ kv
2k
W1−
1 p,p
(∂BR1 +1)
) (12) We deduce of this that v ∈ W
1,p0(Ω) and with (11) and (12), we have :
kvk
W1,p0 (Ω)
≤ C k g
1− ∂u
0∂n k
W
−1 p,p
(Γ1)
.
Then, we easily check (7). Finally the function
u = u
0|Ω+ v ∈ W
1,20(Ω) ∩ W
1,p0(Ω) suits and with (6) and (7), we have (5).
3.2 An “inf-sup” condition
Setting for any p > 1,
V
p= {v ∈ W
1,p0(Ω), v = 0 on Γ
0}.
we notice that, equipped with the norm k∇.k
Lp(Ω), V
pis a reflexive Banach space. In this subsection, we are interested in the existence of β > 0 a constant such that :
inf
w∈Vp0
w6=0
sup
v∈Vp
v6=0
Z
Ω
∇v · ∇w dx k∇vk
Lp(Ω)k∇wk
Lp0(Ω)
≥ β
We define :
◦
H
p(Ω) = {z ∈ L
p(Ω), div z = 0 in Ω, z · n = 0 on Γ
1}
Proposition 3.2. For any g ∈ L
p(Ω), there exists z ∈ H
◦p(Ω) and ϕ ∈ V
p, such that :
g = ∇ϕ + z,
k∇ϕk
Lp(Ω)≤ C kgk
Lp(Ω)where C > 0 is a constant which depends only on Ω and p.
Proof - Let g be in L
p(Ω) and g e the extension by 0 of g in R
n; so we have g e ∈ L
p( R
n) and thanks to a result established in [2],
div e g ∈ W
−1,p0( R
n) ⊥ P
[1−n/p0]with k div gk e
W−1,p0 (Rn)
≤ C k gk e
Lp(Rn)= C kgk
Lp(Ω).
According to the theorem 1.2 i), we know there exists v ∈ W
1,p0( R
n) such that
∆v = div g e in R
n, and we show that k∇vk
Lp(Rn)≤ C
1kgk
Lp(Ω). So, we have : g e − ∇v ∈ L
p( R
n) and div( g e − ∇v) = 0 in R
n.
Consequently, (g − ∇v) · n ∈ W
−1 p,p
(Γ
1) and v
|Γ0∈ W
1−1 p,p
(Γ
0). Here, we apply the results of the theorem 3.1. There exists a unique
w ∈ W
1,p0(Ω) ∩ W
1,20(Ω) solution of :
∆w = 0 in Ω, w = −v on Γ
0, ∂w
∂n = (g − ∇v) · n on Γ
1,
and we show that k∇wk
Lp(Ω)≤ C
2kgk
Lp(Ω).
Finally the functions ϕ = v
|Ω+ w and z = g − ∇ϕ comply with the question.
Theorem 3.3. There exists a constant β > 0 such that
w∈V
inf
p0w6=0
sup
v∈Vp
v6=0
Z
Ω
∇v · ∇w dx k∇vk
Lp(Ω)k∇wk
Lp0(Ω)
≥ β (13)
Proof - Let w be in V
p0with w 6= 0. We notice that ∇w 6= 0 because otherwise w is constant in the connected open region Ω, ie w = 0 in Ω because w = 0 on Γ
0. We have
k∇wk
Lp0(Ω)
= sup
g∈Lp(Ω) g6=0
Z
Ω
∇w · g dx kgk
Lp(Ω).
We easily check that for any z ∈ H
◦p(Ω) and any v ∈ V
p0, we have Z
Ω
z · ∇v dx = 0, what means that superior boundary defined above can not be reached for a g ∈ H
◦p(Ω). Let g be in L
p(Ω) with g 6= 0. We can suppose that g ∈ / H
◦p(Ω) and thanks to the proposition 3.2, there exists z ∈ H
◦p(Ω) and ϕ ∈ V
p, with ∇ϕ 6= 0 such that g = z + ∇ϕ and k∇ϕk
Lp(Ω)≤ C kgk
Lp(Ω). Thus,
Z
Ω
∇w · g dx kgk
Lp(Ω)≤ C Z
Ω
∇w · ∇ϕ dx k∇ϕk
Lp(Ω)≤ C sup
ϕ∈Vp
ϕ6=0
Z
Ω
∇w · ∇ϕ dx k∇ϕk
Lp(Ω).
This is checked for any g in L
p(Ω), so :
k∇wk
Lp0(Ω)
= sup
g∈Lp(Ω) g6=0
Z
Ω
∇w · g dx
kgk
Lp(Ω)≤ C sup
ϕ∈Vp
ϕ6=0
Z
Ω
∇w · ∇ϕ dx k∇ϕk
Lp(Ω).
We deduce the estimate (13) with β = 1
C > 0.
3.3 The full problem
We remind here the following result :
Theorem 3.4. Let X and M be two reflexive Banach spaces and X
0and M
0their dual spaces. Let b be a bilinear form defined and continuous on X × M , let B ∈ L(X; M
0) and B
0∈ L(M, X
0) be the operators defined by :
∀v ∈ X, ∀w ∈ M, b(v, w) = < Bv, w > = < v, B
0w >
The following statements are equivalent :
i) There exists β > 0, such that inf
w∈Mw6=0
sup
v∈Xv6=0
b(v, w) kvk
Xkwk
M≥ β.
ii) The operator B is an isomorphism from X/Ker B to M
0and 1 β is the continuity constant of B
−1.
iii) The operator B
0is an isomorphism from M to X
0⊥ Ker B and 1 β is the continuity constant of B
0−1.
Here, we apply this theorem with X = V
p, M = V
p0and : b(v, w) =
Z
Ω
∇v · ∇w dx.
According to (13),
B is an isomorphism from V
p/Ker B to (V
p0)
0. (14) Then, we define for f ∈ Y
p(Ω) and g ∈ W
−1p,p
(Γ
1) the linear form T by
∀w ∈ V
p0, T (w) = T
f(w) + < g, w >
Γ1,
where < ., . >
Γ1denotes the duality pairing between W
−1 p,p
(Γ
1), W
1−p10,p0(Γ
1).
We check that T ∈ (V
p0)
0and thanks to (14), we deduce the existence of v ∈ V
p, unique up to an element of Ker B, such that Bv = T , ie :
(F V) ∀w ∈ V
p0, Z
Ω
∇v · ∇w dx = T
f(w) + < g, w >
Γ1.
Corollary 3.5. For any f ∈ Y
p(Ω) and g ∈ W
−p1,p
(Γ
1), there exists a unique v ∈ W
1,p0(Ω)/Ker B, solution of
−∆v = f in Ω, v = 0 on Γ
0, ∂v
∂n = g on Γ
1. and checking the following inequality :
kvk
W1,p0 (Ω)/Ker B
≤ C (kf k
Yp(Ω)+ kgk
W
−1 p,p
(Γ1)
). (15)
Proof - As we have done in the theorem 2.2, we show that the solution of the problem (F V ) is also solution of this problem.
Theorem 3.6. For any f ∈ Y
p(Ω), g
0∈ W
1−1 p,p
(Γ
0) and g
1∈ W
−1 p,p
(Γ
1), there exists a unique u ∈ W
1,p0(Ω)/Ker B, solution of (P) and there exists a constant C > 0 such that :
kuk
W1,p0 (Ω)/Ker B
≤ C( kfk
Yp(Ω)+ kg
0k
W1−
1 p,p
(Γ0)
+ kg
1k
W−
1 p,p
(Γ1)
).
Proof - First of all, thanks to [3], we know there exists a unique u
0∈ W
1,p0(Ω
1) where Ω
1= Ω ∪ ω
1, solution of (P
D) and checking
ku
0k
W1,p0 (Ω1)
≤ Ckg
0k
W
1−1 p,p
(Γ0)
. (16)
Thanks to corollary 3.5, we deduce that there exists a unique
v ∈ W
1,p0(Ω)/Ker B, solution of (P
0). Finally, the function u = u
0|
Ω+ v is
solution of (P) and the estimate comes from (15) and (16).
3.4 Characterization of the kernel of the operator B
We set :
M
p0(Ω) = {v ∈ W
1,p0(Ω); ∆v = 0 in Ω, v = 0 on Γ
0, ∂v
∂n = 0 on Γ
1}.
Thanks to the density of D(Ω) in W
1,p0 0(Ω), we easily check that Ker B = M
p0(Ω).
Now, we characterize M
p0(Ω). For this, first of all, we define : µ
0= U ∗ ( 1
|Γ| δ
Γ), where U = 1
2π ln(r) is the fundamental solution of Laplace’s equation in R
2and δ
Γis the distribution defined by :
∀ϕ ∈ D( R
2), < δ
Γ, ϕ > = Z
Γ
ϕ dσ
Proposition 3.7. We have the following statements : i) If p < n, then M
p0(Ω) = {0}.
ii) If p ≥ n ≥ 3, then M
p0(Ω) = {c(λ − 1), c ∈ R } where λ is the only solution in W
1,20(Ω) ∩ W
1,p0(Ω) of the following problem (P
1) :
∆λ = 0 in Ω, λ = 1 on Γ
0, ∂λ
∂n = 0 on Γ
1.
iii) If p > n = 2, then M
p0(Ω) = {c(µ − µ
0), c ∈ R } where µ is the only solution in W
1,20(Ω) ∩ W
1,p0(Ω) of the following problem (P
2) :
∆µ = 0 in Ω, µ = µ
0on Γ
0, ∂µ
∂n = ∂µ
0∂n on Γ
1. Proof - Let z ∈ M
p0(Ω) and let η be the trace of z on Γ
1. We have η ∈ W
−1 p,p
(Γ
1). We know there exists a unique ξ ∈ W
1,p( ω
◦1), where ω
◦1is the interior of the compact ω
1, checking :
∆ξ = 0 in ω
◦1, ξ = η on Γ
1. Let e z be defined by
e z = z in Ω, e z = ξ in ω
1, e z = 0 in ω
0.
It is obvious that e z ∈ W
1,p0( R
n) and ∆ z e ∈ W
−1,p0( R
n). Moreover, for any ϕ ∈ D( R
n), we have :
< ∆ z, ϕ > e
D0(Rn),D(Rn)= − < ∂z
∂n , ϕ >
Γ0− < ∂ξ
∂n , ϕ >
Γ1.
We set h = ∆ z. Then, e h ∈ W
−1,p0( R
n) and h has a compact support. At this stage, the discussion splits into two parts according to the dimension n : i) Case n ≥ 3. Thanks to the proposition 1.3, we know there exists a unique w such that :
w ∈ W
1,p0( R
n) ∩ W
1,20( R
n) and ∆w = h in R
n.
The difference e z − w is in W
1,p0( R
n) and is harmonic in R
n. If p < n, then w = z e in R
n, the restriction of w to Ω is in W
1,p0(Ω) ∩ W
1,20(Ω), and like z = w in Ω, the section 2 implies that w = 0 in Ω i.e M
p0(Ω) = {0}.
If p ≥ n ≥ 3, we have w = e z + c in R
nso w ∈ W
1,p0(Ω) ∩ W
1,20(Ω) is the only solution of the problem :
∆w = 0 in Ω, w = c on Γ
0, ∂w
∂n = 0 on Γ
1.
Consequently M
p0(Ω) = {c(λ − 1), c ∈ R } where λ is the solution of (P
1).
ii) Case n = 2. The problem
∆w = h in R
2,
does not have a solution in W
1,20( R
2) unless h satisfies the necessary condition
< h, 1 > = 0. In this case, with the arguments above, we obtain z = c(λ − 1).
However, when n = 2, the constant functions are in W
1,p0(Ω) ∩ W
1,20(Ω) so λ = 1 ∈ W
1,p0(Ω) ∩ W
1,20(Ω) is solution of (P
1). So z = 0, which is the trivial case. Thus, we suppose that < h, 1 > 6= 0 and we consider the problem :
∆w = h − < h, 1 > ∆µ
0in R
2. (17) We know that µ
0∈ W
1,q0( R
2) for any q > 2 and moreover
∆µ
0= 0 in Ω ∪ ω
◦0∪ ω
◦1and < ∆µ
0, 1 >= 1.
The right-hand side of (17) is orthogonal to constants, has compact support and belongs to W
−1,p0( R
2). So, thanks to proposition 1.3, the problem (17) has a solution (unique up to an additive constant) w ∈ W
1,20( R
2) ∩ W
1,p0( R
2).
Moreover, the function w + < h, 1 > µ
0− e z is harmonic in R
2. So, there exists c > 0 such that w + < h, 1 > µ
0− z e = c. The restriction of w to Ω is in W
1,p0(Ω) ∩ W
1,20(Ω) and w = c + w
1where w
1is the only solution in W
1,20(Ω) ∩ W
1,p0(Ω) of the problem :
∆w
1= 0 in Ω, w
1= − < h, 1 > µ
0on Γ
0, ∂w
1∂n = − < h, 1 > ∂µ
0∂n on Γ
1. The function µ being the only solution in W
1,20(Ω) ∩ W
1,p0(Ω) of the problem (P
2). We have M
p0(Ω) = {c(µ − µ
0), c ∈ R }.
3.5 A regularity result
We suppose, in this subsection, that p ≥ 2. Here, we propose to study the question of the regularity of the solutions when the data are more regular.
More precisely, we suppose that :
g
0∈ W
2−p1,p(Γ
0), g
1∈ W
1−1p,p(Γ
1) and f ∈ X
0,p1(Ω) where
X
0,p1(Ω) =
( W
0,p1(Ω) if p 6= n n − 1 , W
0,p1(Ω) ∩ W
−1,p0(Ω) otherwise,
equipped with its natural norm : (we remind that W
0,p1(Ω) is included in W
−1,p0(Ω) if and only if W
1,p0 0(Ω) ⊂ W
−1,p0 0(Ω), this last inclusion taking place if and only if p 6= n
n − 1 ).
Theorem 3.8. For any
g
0∈ W
2−1p,p(Γ
0), g
1∈ W
1−1p,p(Γ
1), and f ∈ X
0,p1(Ω), there exists a unique u ∈ W
2,p1(Ω)/M
p0(Ω) solution of (P ), and we have :
kuk
W2,p1 (Ω)/Mp0(Ω)
≤ C (kf k
X0,p1 (Ω)
+ kg
0k
W2−
1 p,p
(Γ0)
+ kg
1k
W1−
1 p,p
(Γ1)
) (18) Proof - For p ≥ 2 and g
0∈ W
2−1p,p(Γ
0), we have, thanks to [3] that the solution u
0∈ W
1,p0(Ω
1) (where Ω
1= Ω ∪ ω
1) of the problem (P
D) is in W
2,p1(Ω
1) and it checks :
ku
0k
W2,p1 (Ω1)
≤ C kg
0k
W2−1p,p(Γ0)
. (19) now, we notice that ∂u
0∂n ∈ W
1−1p,p(Γ
1) because u
0∈ W
2,p1(Ω
1). Thus, as f ∈ X
0,p1(Ω) ⊂ Y
p(Ω) and g
1− ∂u
0∂n ∈ W
1−p1,p(Γ
1) ⊂ W
−1 p,p
(Γ
1), applying the corollary 3.5 when p > 2 and the theorem 2.2 when p = 2, there exists, for p ≥ 2, a unique v ∈ W
1,p0(Ω) solution of the problem (P
0). It stays to show that v ∈ W
2,p1(Ω) and that
kvk
W2,p1 (Ω)/Mp0(Ω)
≤ C (kf k
X0,p1 (Ω)
+ kg
0k
W2−1p,p(Γ0)
+ kg
1k
W1−1p,p(Γ1)
). (20) For this, we follow the same reasoning as theorem 3.1 using theorem 1.2 ii) if p 6= n
n − 1 and theorem 1.2 iii) otherwise, and using regularity results in bounded open regions (see Lions and Magenes [7] for instance).
Finally, the function u = u
0|
Ω+ v ∈ W
2,p1(Ω) is solution of (P ) and the estimate (18) is a consequence of (19) and (20).
4 Case p < 2
We are going to proceed in two steps. First of all, thanks to an argument of duality, which allows us to use results of the previous section, we solve the problem in the case where f = 0 and g
1= 0. The sum of the solution of this problem and of a solution of a Neumann problem will permit us to solve the general problem (P).
In all the section, we suppose that p < 2 and that Γ is of class C
1,1.
4.1 Case where f = 0 and g
1= 0.
Let g
0∈ W
1−1 p,p
(Γ
0) checking the condition of compatibility
∀z ∈ M
p00(Ω) , < ∂z
∂n , g
0>
Γ0= 0, (21) where < , >
Γ0denotes the duality pairing W
−1 p0,p0
(Γ
0), W
1−1 p,p
(Γ
0).
With this hypothesis, we consider the problem : find v ∈ W
1,p0(Ω) solution of :
(Q)
∆v = 0 in Ω, v = g
0on Γ
0,
∂v
∂n = 0 on Γ
1.
and this other problem (Q
0) : find v ∈ W
1,p0(Ω) such that for any u ∈ X
p0(Ω) satisfying u = 0 on Γ
0and ∂u
∂n = 0 on Γ
1, we have : T
−∆u(v) = − < ∂u
∂n , g
0>
Γ0(22) where
X
p0(Ω) = {u ∈ W
1,p0 0(Ω), ∆u ∈ L
p0(Ω)}.
We easily check that the problem (Q) is equivalent to the problem (Q
0).
Theorem 4.1. For any g
0∈ W
1−1 p,p
(Γ
0) satisfying the compatibility condition (21), there exists a unique v ∈ W
1,p0(Ω) solution of the problem (Q) and we have the following estimate :
kvk
W1,p0 (Ω)
≤ kg
0k
W1−
1 p,p
(Γ0)
.
Proof - Let f be in Y
p0(Ω). It is obvious that T
f∈ (W
1,p0(Ω))
0. Like p
0> 2, thanks to the theorem 3.6, we know there exists a unique
u ∈ W
1,p0 0(Ω)/M
p00(Ω) such that
−∆u = f in Ω, u = 0 on Γ
0, ∂u
∂n = 0 on Γ
1, checking
kuk
W1,p00 (Ω)/Mp00(Ω)
≤ C kT
fk
(W1,p0 (Ω))0
(23)
Let L be the linear form defined on (W
1,p0(Ω))
0by : L(T
f) = − < ∂u
∂n , g
0>
Γ0.
We are going to show that L is continuous. Let z be in M
p00(Ω), then, thanks to (21), we have < ∂u
∂n , g
0>
Γ0= < ∂(u + z)
∂n , g
0>
Γ0. Now, let θ be an open region of class C
1,1such that ω
0⊂ θ ⊂ B
Rwhere R is the radius associated to the partition of the unity used in the definition of T
f. We set Ω
θ= θ\ω
0and let ϕ ∈ W
1,p(Ω
θ) be such that ϕ = 0 on ∂θ. We have :
| < ∂(u + z)
∂n , ϕ >
Γ0| ≤ k∇(u + z)k
Lp0(Ωθ)k∇ϕk
Lp(Ωθ)+ | Z
Ωθ
ϕ ∆(u + z) dx| .
But,
| Z
Ωθ
ϕ ∆(u + z) dx| = | Z
Ωθ
ϕ ∆u dx| = |T
−∆u( ϕ)|, e
where ϕ e ∈ W
1,p0(Ω) is defined by ϕ e = ϕ in Ω
θ, ϕ e = 0 in Ω \ θ. In consequence,
| < ∂(u + z)
∂n , ϕ >
Γ0| ≤ k∇(u+z)k
Lp0(Ωθ)
k∇ϕk
Lp(Ωθ)+ kT
fk
(W1,p0 (Ω))0
kϕk
W1,p(Ωθ). Now, for any µ ∈ W
1−1p,p(Γ
0), we know there exists ϕ ∈ W
1,p(Ω
θ) such that ϕ = µ on Γ
0and ϕ = 0 on ∂θ checking
kϕk
W1,p(Ωθ)≤ C kµk
W1−1p,p(Γ0)
,
where C > 0 is a constant which depends only on Ω
θand on µ. So
| < ∂(u + z)
∂n , µ >
Γ0| ≤ C ( k∇(u+z)k
Lp0(Ωθ)
+ kT
fk
(W1,p0 (Ω))0
) kµk
W1−
1 p,p
(Γ0)
. Thus, we deduce of (23) that
inf
z∈Mp00(Ω)
k ∂(u + z)
∂n k
W−1/p0,p0(Γ0)≤ C kT
fk
(W1,p 0 (Ω))0. So
|L(T
f)| = | < ∂u
∂n , g
0> | ≤ C kT
fk
(W1,p0 (Ω))0
kg
0k
W
1−1 p,p
(Γ0)
,
and the linear form L is continuous on (W
1,p0(Ω))
0. Like the space W
1,p0(Ω) is reflexive, we can identify L to an element of W
1,p0(Ω), i.e there exists a unique v ∈ W
1,p0(Ω) such that :
T
f(v) = − < ∂u
∂n , g
0>
Γ0,
and checking the estimate searched. In consequence, the function v is solution of the problem (Q
0) equivalent to the problem (Q).
4.2 The general problem when p<2.
Let f ∈ Y
p(Ω), g
0∈ W
1−1 p,p
(Γ
0) and g
1∈ W
−1 p,p
(Γ
1). We remind that we search u ∈ W
1,p0(Ω) solution of the problem (P). Assuming that a such solution u ∈ W
1,p0(Ω) exists, for any ϕ ∈ M
p00(Ω), we have thanks to the density of D(Ω) in W
1,p0 0(Ω) :
T
f(ϕ) = Z
Ω
∇u · ∇ϕ dx − < g
1, ϕ >
Γ1. (24) Like D(Ω) is also dense in W
1,p0(Ω), we have, for any ϕ ∈ M
p00(Ω) :
Z
Ω
∇ϕ · ∇u dx = < ∂ϕ
∂n , g
0>
Γ0. (25) We deduce of (24) and (25) that if u ∈ W
1,p0(Ω) is solution of the problem (P ), the data must checking the following condition of compatibility :
∀ϕ ∈ M
p00(Ω), T
f(ϕ) = < ∂ϕ
∂n , g
0>
Γ0− < g
1, ϕ >
Γ1. (26) Theorem 4.2. Let p < 2, f ∈ Y
p(Ω), g
0∈ W
1−1 p,p
(Γ
0), g
1∈ W
−1 p,p
(Γ
1) be satisfying the condition of compatibility (26) if 1 < p ≤ n
n − 1 , then there exists a unique u ∈ W
1,p0(Ω) solution of the problem (P ) and there exists C > 0 such that
kuk
W1,p0 (Ω)
≤ C( kf k
Yp(Ω)+ kg
0k
W1−
1 p,p
(Γ0)
+ kg
1k
W−
1 p,p
(Γ1)