Journal ArticleDOI

# A free boundary problem for the Laplacian with a constant Bernoulli-type boundary condition

15 Oct 2007--Vol. 67, Iss: 8, pp 2497-2505
TL;DR: In this article, a free boundary problem for the Laplace operator is studied, where a Bernoulli-type boundary condition is imposed, and a solution to this problem is shown.
Abstract: We study a free boundary problem for the Laplace operator, where we impose a Bernoulli-type boundary condition. We show that there exists a solution to this problem. We use A. Beurling's technique, by defining two classes of sub- and supersolutions and a Perron argument. We try to generalize here a previous work of A. Henrot and H. Shahgholian. We extend these results in different directions.

### 1. Introduction

• This problem arises from various areas, for instance shape-optimization, fluid dy- namics, electrochemistry and electromagnetics.
• In particular, the free boundary (∂Ω \K) meets the fixed boundary (K) tangentially.
• Moreover, the solution has convex level sets.

### 2. Preliminaries

• The results in this subsection are more or less already known, but not proved in detail for this particular case.
• To finish up the preparations the authors show that the gradient is almost uniformly bounded on the boundary.
• Ω since the function used will be the same.

### 3. Beurling’s technique

• As mentioned earlier the authors revisit Beurling’s technique to prove their main result.
• The arguments that the authors will use are more or less the same as the proofs of Henrot and Shahgholian in  and .
• First, the authors give the steps of this technique and then, corresponding theorems.
• The class B is closed under intersection.
• Then there exists a solution of the free boundary problem (P) in a strong sense.

• Let un denote the sequence of functions corresponding to the solution with the free boundary condition |∇un| = λn, and let Ωn be the corresponding domains.
• In the case of the arbritary p-Laplacian there are some small adjustments needed; the authors will have to replace the fact that |∇u|2 is subharmonic by [6, Lemma 2.1] and use that the therein defined operator Lu admits a maximum principle and that Lu|∇u|p ≥.
• Here the authors must use the general expression for the n-dimensional radial symmetric p-capacitary potential, i.e.
• The authors also remark that the C2+α-regularity will not be valid in the general case since the theorem used only applies to elliptic operators.
• As mentioned in the introduction, the result in this paper could probably be extended to results similar to those in  and  for their case.

Did you find this useful? Give us your feedback

Content maybe subject to copyright    Report HAL Id: hal-00128760
https://hal.archives-ouvertes.fr/hal-00128760
Submitted on 2 Feb 2007
HAL is a multi-disciplinary open access
archive for the deposit and dissemination of sci-
entic research documents, whether they are pub-
lished or not. The documents may come from
teaching and research institutions in France or
abroad, or from public or private research centers.
L’archive ouverte pluridisciplinaire HAL, est
destinée au dépôt et à la diusion de documents
scientiques de niveau recherche, publiés ou non,
émanant des établissements d’enseignement et de
recherche français ou étrangers, des laboratoires
publics ou privés.
A free boundary problem for the Laplacian with
constant Bernoulli-type boundary condition
Erik Lindgren, Yannick Privat
To cite this version:
Erik Lindgren, Yannick Privat. A free boundary problem for the Laplacian with constant Bernoulli-
type boundary condition. Nonlinear Analysis: Theory, Methods and Applications, Elsevier, 2007, 67
(8), pp.2497-2505. �10.1016/j.na.2006.08.045�. �hal-00128760� A FREE BOUNDARY PROBLEM FOR THE LAPLACIAN WITH
CONSTANT BERNOULLI-TYPE BOUNDARY CONDITION
ERIK LINDGREN AND YANNICK PRIVAT
Abstract. We study a free boundary problem f or the Laplace operator,
where we impose a Bernoulli-type boundary condition. We show that there
exists a solution to this problem. We use A. Beurling’s technique, by deﬁn-
ing two classes of sub- and s upersolutions and a Perron argument. We try to
generalize here a previous work of A. Henrot and H. Shahgholian. We extend
these results in diﬀerent directions.
1. Introduction
1.1. The problem. The aim of this paper is to prove the existence and uniqueness
of a Bernoulli-type free boundary problem in R
n
. Consider a smooth, bounded
and convex domain K such that K {x
1
= 0}. We seek a bounded domain
R
n
+
= {R
n
: x
1
> 0} with K , together with a function u : R such
that
u = 0 in ,
u = 1 on K ,
u = 0 on \ K ,
|∇u| = 1 on ( \ K) R
n
+
.
This problem arises from various areas, for ins tance shape-o ptimization, ﬂuid dy-
u = 1
u = 0u = 0
|∇u| = 1
u = 0
u = 0
K
Figure 1. The geometric situation in R
2
.
namics, electrochemistry and electromagnetics. See for example ,  and . We
also see a possibility to extend the results in  and  to be valid in our case.
Date: February 2, 2007.
1 2 ERIK LINDGREN AND YANNICK PRIVAT
1.2. The main theorem. The main theorem of the paper is:
Theorem 1. There is a unique solution to the free boundary problem (P) with
being C
2+α
for any 0 < α < 1. In particular, the free boundary ( \ K) meets the
ﬁxed boundary (K) tangentially. Moreover, the solution has convex level sets.
1.3. Outline of the proof. The method used is as follows. Let C be the class of
smooth, bounded and convex domains in R
n
such that K belongs to the boundary
of the domain. Let C, we denote furthermore by u
the function fulﬁlling
u
= 0 ,
u
= 0 in \ K ,
u
= 1 in K .
Let us introduce the following classes of domains
A =
C : lim inf
yx x
|∇u
(y)| 1, x R
n
+
,
A
0
=
C : lim sup
yx x
|∇u
(y)| > 1, x \ K
,
B =
C : lim sup
yx x
|∇u
(y)| 1, x \ K
.
Transla ted into terms of A and B, the aim of this project is to prove that AB 6= .
To do this, we use Beur ling’s technique. In particular, we show that a subclass of
B has, in some sense, a minimal element (if it is non-empty). This part of the proof
relies mainly on Lemma 1, the bound on |∇u| (Lemma 2). These results are proved
using the same arguments as in ,  and .
In what follows we prove that the minimal element of B belongs to A as well.
Mainly, we use Lemma 4 and some barrier arguments together with Lemma 1.
The proof is more or less a synthesis of  and . The big diﬀerence in this problem
is that the free boundary and the ﬁxed boundary do meet. A fbp for the Laplacian with Bernoulli-type boundary condition 3
2. Preliminaries
Before we start tre ating the classes we need a bit of preparations. The results in
this subsection are more or le ss alr eady known, but not proved in detail for this
particular case.
The ﬁrst thing we prove is that the level sets of a Dirichlet solution are convex.
Theorem 2. Let C. Then the level sets of u
, i.e. the sets L
ε
= {x :
u
> ε}, are convex.
Proof. Let
K
n
= {x : dist(x, K) < n/2}
n
= {x : dist(x, Ω) < n} .
Then D
n
=
n
\ K
n
is a convex ring. Therefore, u
n
= u
D
n
has convex level sets
(cf ). By standard arguments, u
n
converges to a harmonic function in every
compact subset of . Furthermore we will have C
0
-convergence in R
n
. Clearly,
u = 1 on I and u = 0 on R
n
\ (Ω K). Hence, u
n
u
. Moreover, L
ε
= ∩L
n
ε
,
where L
n
ε
= {x : u
n
> ε}, which implies that the sets L
ε
are convex.
Now we prove a fundamental (but not trivial) lemma (based on the same idea than
in ), which has some very important consequences when comparing the gradient
on the boundary.
Lemma 1. We denote by x
1
the ﬁrst coordinate in R
n
. Let u = u
with C,
such that u is Lipschitz on the boundary. Suppose that the gradient of u exists on
the boundary and that it is for every r > 0 uniformly bounded by a constant M (r)
in {x : dist(K, x) < r}. Then we will have, after suitable rotations and translations,
u(x) = u(x
0
) + α(x
1
x
0
1
)
+
+ o(r
n
) for x
0
\ {x : dist(K, x) < r},
for some sequences r
n
. In particular, we will have
lim sup
yx
0
|∇u(y)| = lim sup
yx
0
h∇u(y), vi 0 ,
where v is a normal vector orthogonal the t angent plane at x
0
(or to one of them,
if there are several).
Remark 1. We remark an immediate consequence of this theorem; let u and v be
non-negative harmonic functions inside a domain such that u = v = 0 in some
neighborhood of x and u v in . Then
lim sup
yx
|∇u(y)| lim sup
yx
|∇v(y)| .
Indeed, apply Lemma 1 to the functions u and v and use that they both attain a
minimum at x. The result follows immediately.
Now we just o bserve that |∇u|
2
is a subharmonic function if u is harmonic. To
ﬁnish up the prepar ations we show that the gradient is almost uniformly bounded
on the boundary. The proof is more or less taken from .
Lemma 2. Let C. Then the gradient of u
is uniformly bounded outside and
far enough from K, i.e. for each r
0
> 0 there is a constant M (r
0
) such that:
|∇u| M(r
0
) ,
for all x \ N (r
0
), where N (r
0
) = {x : dist(K, x) < r
0
}.
Remark 2. In , the authors prove this lemma in a more simple case, in the
sense that the convex domain K doesn’t belong to the boundary of . Lemma 3
prove that the gradient of u
is bounded even if K
6= . 4 ERIK LINDGREN AND YANNICK PRIVAT
Proof. We observe that, by barrier a rguments and the use of Lemma 1 we have
that away from K, u = 0 where is not C
1
. So we can suppose that is C
1
away from K.
Since |∇u|
2
is subharmonic inside it suﬃces thus to show that the gradient is
bounded on (Ω \ N(r
0
)).
Let r
0
> 0 and let
b
K = K \ N (r
0
).
(i) First Case: x
b
K.
Take B
r
0
/3
and B
r
0
/2
be c e ntered at (x r
0
/3x
2
). Consider now ˆu, the
capacitary potential on B
r
0
/2
\ B
r
0
/3
, i.e. the harmonic function being zero
on B
r
0
/2
and one o n B
r
0
/3
. Then we have by the comparison principle
that u bu inside (B
r
0
/2
\ B
r
0
/3
) , which by Lemma 1 implies
|∇u(x)| |∇bu(x)| M (r
0
) .
We observe that we could repeat this for every point in
b
K without changing
the radius of the balls. Hence, the inequality is valid for all x
b
K.
(ii) Second Case: x N (r
0
) .
We use more or less the same arguments as above; let the balls B
r
0
/3
and B
r
0
/2
be centered at the same point such that B
r
0
/3
{u u(x)} and
B
r
0
/3
{u = u(x)} = x. This is possible since the level sets are by Theorem
2 convex. Le t ˆu denote the harmonic function inside B
r
0
/2
\ B
r
0
/3
such
that ˆu = u(x) on B
r
0
/3
and ˆu = 0 on B
r
0
/2
. The comparison principle
and Lemma 1 together imply
|∇u(x)| |∇ˆu(x)| M(r
0
) .
Clearly, this inequality is valid for all x N(r
0
) since the function
used will be the same.
x
b
K
x N (r
0
)
x \ (K N (r
0
))
N (r
0
)
{u = u(x)}
Figure 2. The picture when n = 2.
(iii) Third Case: x \ (K N(r
0
)).
Let B
r
0
/3
and B
r
0
/2
be centered at the same point such that B
r
0
/3
= x.
We pick again a capa c itary potential ˆu o n B
r
0
/2
\ B
r
0
/3
, such that ˆu = 0
on B
r
0
/3
and ˆu = 1 on B
r
0
/2
. Then, as before, we obtain
|∇u(x)| |∇ˆu(x)| M(r
0
) ,
uniformly.
The result follows.

##### Citations
More filters
Journal ArticleDOI
Yannick Fischer
TL;DR: In this paper, two inverse problems related to the tokamak \textsl{Tore Supra} through the study of the magnetostatic equation for the poloidal flux are considered.
Abstract: We consider two inverse problems related to the tokamak \textsl{Tore Supra} through the study of the magnetostatic equation for the poloidal flux. The first one deals with the Cauchy issue of recovering in a two dimensional annular domain boundary magnetic values on the inner boundary, namely the limiter, from available overdetermined data on the outer boundary. Using tools from complex analysis and properties of genereralized Hardy spaces, we establish stability and existence properties. Secondly the inverse problem of recovering the shape of the plasma is addressed thank tools of shape optimization. Again results about existence and optimality are provided. They give rise to a fast algorithm of identification which is applied to several numerical simulations computing good results either for the classical harmonic case or for the data coming from \textsl{Tore Supra}.

15 citations

Journal ArticleDOI
TL;DR: In this paper, a Bernoulli free boundary problem with geometrical constraints is studied, where the domain Ω is constrained to lie in the half space determined by x 1 ≥ 0 and its boundary to contain a segment of the hyperplane {x 1 = 0 } where non-homogeneous Dirichlet conditions are imposed.
Abstract: A Bernoulli free boundary problem with geometrical constraints is studied. The domain Ω is constrained to lie in the half space determined by x1 ≥ 0 and its boundary to contain a segment of the hyperplane {x1 =0 } where non-homogeneous Dirichlet conditions are imposed. We are then looking for the solution of a partial differential equation satisfying a Dirichlet and a Neumann boundary condition simultaneously on the free boundary. The existence and uniqueness of a solution have already been addressed and this paper is devoted first to the study of geometric and asymptotic properties of the solution and then to the numerical treatment of the problem using a shape optimization formulation. The major difficulty and originality of this paper lies in the treatment of the geometric constraints.

12 citations

Journal ArticleDOI
TL;DR: In this article, a Bernoulli free boundary problem with geometrical constraints is studied, where the domain is constrained to lie in the half space determined by the hyperplane and its boundary to contain a segment of the hyper plane where non-homogeneous Dirichlet conditions are imposed.
Abstract: A Bernoulli free boundary problem with geometrical constraints is studied. The domain $\Om$ is constrained to lie in the half space determined by $x_1\geq 0$ and its boundary to contain a segment of the hyperplane $\{x_1=0\}$ where non-homogeneous Dirichlet conditions are imposed. We are then looking for the solution of a partial differential equation satisfying a Dirichlet and a Neumann boundary condition simultaneously on the free boundary. The existence and uniqueness of a solution have already been addressed and this paper is devoted first to the study of geometric and asymptotic properties of the solution and then to the numerical treatment of the problem using a shape optimization formulation. The major difficulty and originality of this paper lies in the treatment of the geometric constraints.

10 citations

Journal ArticleDOI
TL;DR: In this paper , a free boundary problem in an exterior domain is considered and the authors consider free boundary problems in an interior domain, where the boundary problem is formulated as a set-free boundary problem.
Abstract: Abstract We consider a free boundary problem in an exterior domain \begin{aligned} {\left\{ \begin{array}{ll} Lu=g(u)&{}\text {in }\Omega \setminus K,\\ u=1 &{} \text {on }\partial K,\\ | abla u|=0 &{}\text {on }\partial \Omega , \end{array}\right. } \end{aligned} L u = g ( u ) in Ω \ K , u = 1 on K , | u | = 0 on Ω , where K is a (given) convex and compact set in $${\mathbb R}^n$$ R n ( $$n\ge 2$$ n 2 ), $$\Omega =\{u>0\}\supset K$$ Ω = { u > 0 } K is an unknown set, and L is either a fully nonlinear or the p -Laplace operator. Under suitable assumptions on K and g , we prove the existence of a nonnegative quasi-concave solution to the above problem. We also consider the cases when the set K is contained in $$\{x_n=0\}$$ { x n = 0 } , and obtain similar results.
Posted Content
TL;DR: In this article, two inverse problems related to the tokamak \textsl{Tore Supra} through the study of the magnetostatic equation for the poloidal flux are considered.
Abstract: We consider two inverse problems related to the tokamak \textsl{Tore Supra} through the study of the magnetostatic equation for the poloidal flux. The first one deals with the Cauchy issue of recovering in a two dimensional annular domain boundary magnetic values on the inner boundary, namely the limiter, from available overdetermined data on the outer boundary. Using tools from complex analysis and properties of genereralized Hardy spaces, we establish stability and existence properties. Secondly the inverse problem of recovering the shape of the plasma is addressed thank tools of shape optimization. Again results about existence and optimality are provided. They give rise to a fast algorithm of identification which is applied to several numerical simulations computing good results either for the classical harmonic case or for the data coming from \textsl{Tore Supra}.

### Cites background from "A free boundary problem for the Lap..."

• ...About the literature on free boundary problem with a Bernoulli condition, we refer to [28, 29, 31, 32, 33, 35, 41, 42]....

[...]

##### References
More filters
Book
01 Jan 1982

1,214 citations

Journal ArticleDOI

203 citations

Journal ArticleDOI
TL;DR: In this article, the authors prove the existence of classical solutions for a Bernoulli-type free boundary problem, with the p-Laplacian as the governing operator under convexity assumptions for the data.
Abstract: In this paper we prove, under convexity assumptions for the data, the existence of classical solutions for a Bernoulli-type free boundary problem, with the p-Laplacian as the governing operator. The method employed here originates from a pioneering work of A. Beurling where he proves the existence for the harmonic case in the plane, though with no geometrical restrictions.

58 citations

### "A free boundary problem for the Lap..." refers background or methods or result in this paper

• ...The arguments that we will use are more or less the same as the proofs of Henrot and Shahgholian in [ 6 ] and ....

[...]

• ...Proof. This is more or less the same arguments as in [ 6 ]....

[...]

• ...limsup y!x |ru(y)| = 1. This result is already proved in [ 6 ]...

[...]

• ...Proof. Even if this result is already proved in [ 6 ], we recall it in order to clarify the construction....

[...]

• ...In order to prove that there is a minimal element in some sense (which we will soon see), we first need a theorem on sequences in B. The two following proofs can be found in [ 6 ]....

[...]

Journal ArticleDOI
TL;DR: In this paper, the existence of convex classical solutions for a Bernoulli-type free boundary problem in the interior of a convex domain is proved, where the governing operator is the p-Laplac operator.
Abstract: In this paper, we prove the existence of convex classical solutions for a Bernoulli-type free boundary problem, in the interior of a convex domain. The governing operator considered is the p-Laplac ...

46 citations

Journal ArticleDOI
TL;DR: In this paper, it was shown that the exterior and interior free boundary problem with a Bernoulli law, with a prescribed pressure a(x) on the free streamline of the flow, has convex solutions provided the initial domains are convex.
Abstract: Our objective, here, is to generalize our earlier results on the existence of classical convex solution to a free boundary problem with a Bernoulli-type boundary gradient condition and with the p-Laplacian as the governing operator. The main theorems of this paper assert that the exterior and the interior free boundary problem with a Bernoulli law, i.e. with a prescribed pressure a(x) on the free streamline of the flow, have convex solutions provided the initial domains are convex. The continuous function a(x) is subject to certain convexity properties. In our earlier results we have considered the case of constant a(x). In the lines of the proof of the main results we also prove the semi-continuity (up to the boundary) of the gradient of the p-capacitary potentials in convex rings, with C-1 boundaries.

29 citations