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A NNALES DE L ’I. H. P., SECTION C

M ARIANO G IAQUINTA G IUSEPPE M ODICA J I ˇ S OU ˇ CEK

Connectivity properties of the range of a weak diffeomorphism

Annales de l’I. H. P., section C, tome 12, n

o

1 (1995), p. 61-73

<http://www.numdam.org/item?id=AIHPC_1995__12_1_61_0>

© Gauthier-Villars, 1995, tous droits réservés.

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Connectivity properties of the range of

a

weak diffeomorphism (*)

Mariano

GIAQUINTA, Giuseppe

MODICA Dipartimento di Matematica Applicata

Universita di Firenze Via S. Marta, 3 50139 Firenze, Italy.

Ji0159í

SOU010DEK

Akademie ved Ceske republiky Matematicky Ustav

Xitna,

25 11567 Praha, CR.

Vol. 12, 1, 1995, p. 61-73. Analyse non linéaire

ABSTRACT. - We discuss

connectivity properties

of the range of Sobolev

maps, and of weak

diffeomorphisms

or

equivalently

of elastic deformations.

Key words: Calculus of variations, finite elasticity.

RESUME. - On

presente

des resultats sur la connexion de

l’image

d’un

diffeomorphisme

faible.

In this paper we shall

study

some

properties

of the range of a

weak

diffeomorphism

u, where f2 is an open connected domain in R’~ . We denote

by Rn

another copy of Rn and we

recall,

compare

[3] [2],

that a

Classification A.M.S.: 49 Q 20, 73 C 50.

(*) This work has been partially supported by the Ministero dell’Universita e della Ricerca Scientifica, by C.N.R. contract n. 91.01343.CT01, by the European Research Project GADGET, and by Grant n.11957 of the Czech Acad. of Sciences. The second author would like to

aknowledge hospitality of the Mathematisches Institut of ETH Zurich during the preparation of this work.

Annales de l’lnstitut Henri Poincaré - Analyse non linéaire - 0294-1449 Vol. 12/95/01/$ 4.00/@ Gauthier-Villars

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function u E

W 1’ 1 ( SZ, Rn )

is said to

belong

to if

where

M(Du)

denotes the n-vector in

AnRn

x

Rn

ei,..., en

being

the canonical basis of

Rn,

and moreover

where

Gu

denotes the n-dimensional rectifiable current in Rn x Rn carried

by

the

graph

of u. If

and

then

where M := E and is the n-vector

orienting

M

compare

[5].

The class of weak

diffeomorphisms

is then defined as the class of

u E

cart 1 (03A9, Rn )

such that

(i)

det Du > 0 a.e. in

SZ,

(ii) u

is

globally

invertible in the sense that

holds for

all §

E x

Rn ) with §

> 0.

Annales de l’lnstitut Henri Poincaré - Analyse non linéaire

(4)

In the

physical

case n = 3 such a class arises

naturally

in finite

elasticity,

and in fact characterizes elastic

deformations

in the sense of

[4].

In order to discuss

properties

of the range

of u,

of course we should first

identify u(f2).

First we consider Sobolev maps u E

Rn),

p >

l,

and we do it in terms of

approximate continuity,

compare e.g.

[ 1 ] .

Given

a

point x

E H at which H has

positive density, o(SZ, x)

>

0,

one says that

z E is the

approximate

limit of

u(y) for y -

x,

if for every r > 0 the

point x

is a zero

density point

for the set

u-1(Rn B B(z, r)).

Here the

density

is defined in terms of

Lebesgue

measure

It turns out that for a.e. x G H the

approximate

limit of

u(y)

exists and agrees with

Lebesgue’s

value of u. More

precisely, setting

we have

and

finally,

compare

[7], [13]

consequently

We shall now work with the

approximately

continuous

representative 11

on

Au

of u and prove that the

image

of a connected set f2

by

a

W1,p

map is connected.

DEFINITION 1. - We say that A C R" is

d-open if and only if 0 (A, x)

= 1

for

all x E A.

Vol. 12, n° 1-1995.

(5)

The collection of

d-open

sets defines the so-called

d-topology;

it is in fact

easily

seen that unions and finite intersections of

d-open

sets are

d-open

sets. Such a

topology

is studied for instance in

[8] [9]

and

[10],

where the notion of

do-connectedness

is introduced.

LEMMA 1. - Let H

C Rn

be open and connected and let A C SZ be a set

of positive

measure with

finite perimeter

in S~

for

which

~A~

> 0 and

= 0. Then

~SZ B A) =

0.

Proof. -

From

we infer that the distribution xA has zero derivatives in

H,

hence xA is constant in

H,

as H is connected. D

We can now state

THEOREM 1. - Let Q be an open connected set in Rn and let u E

RN),

p > l. Then the set n

Au)

is connected.

Proof - Suppose

that B :=

u(A

n

Au)

is not connected. Then there are

disjoint

open sets

U1

and

U2

in

R~

such that

Since u is

approximately

continuous on

Au

the sets

are contained in

Au

and

d-open

in Rn .

From B C

Ui

U

U2

we then deduce that

Au

=

Ai

U

A2,

hence

As B

n Ui

we have

Ai ~ 0, hence IAi (

>

0,

since the are

d-open.

Also

Consider now the reduced

boundary c~~ Ai

of

Ai

in H. We have

Annales de l’lnstitut Henri Poincaré - Analyse non linéaire

(6)

hence

so that

From Lemma 1 we therefore

deduce S2 B All

= 0 which contradicts

> o. D

Remark 1. - It is

easily

seen that in fact Theorem 1 holds for any

representative v

of u which is

approximately

continuous in with

,~n (SZ B Av)

=

0, replacing Au

and u

respectively

with and v.

Remark 2. - The choice of a

representative

of u in Theorem 1 is

essential. For

example

consider the function

Then

u(B(0, 1)) _ (-1, 0)

U

(0,1)

U

{2},

i.e.

u(B(O, 1))

is not connected.

Only carefully redefining u

on

?~l"-1-a.e. point

of the line

{0}

x

(-1,1)

C

B(0, 1)

in terms of an

approximately

continuous

representative v

we can

infer that

v(B(0, 1))

is connected.

We are now

ready

to discuss

connectivity properties

of the range af weak

diffeomorphisms u

E

dif (0, Rn).

Since has the double Lusin’s

property,

from

[4]

we known that there exists a null set

Nu

C

H, INul

=

0,

such that u is one to one on

Ru B Nu

and

In fact this holds for any Lusin’s

representative

of u,

and,

moreover, we can assume that be defined in all of H.

We shall now introduce a variant of the notion of

connectivity

which

is suited

,for

our purposes. Given two subsets A and B of Rn we define their essential distance

by

We then set

DEFINITION 2. - A set A

C Rn is

said to be

essentially connected, ess-connected, iff

Vol. 12, n° 1-1995.

(7)

We have

THEOREM

2. -

Let SZ ~ Rn be a bounded connected domain and let

u C

1,1 SZ, Rn).

Then

u(SZ)

is

ess-connected for

any Lusin

representative

ic

of

u.

Proof - Suppose ic(SZ)

is not ess-connected. Then we can find

B1, B2

C

ic ( SZ )

such that

Consider now an open set U D

Bi

with smooth

boundary

~Lf such that

dist

(U, B2)

>

0,

and the function

A(y)

is

Lipschitz-continuous

and for some

~o

> 0

Finally

we extend A to all of R" x

Rn by setting

Setting

we see as consequence of the double Lusin’s

property

of ù

(in

fact from

I

= 0 if

~A~

=

0)

that

Now we slice the current

Gu by A,

compare

[11].

For a.e.

8,

0

b $o

the slice

Gu, ~, b

> exists as a

(n - 1)-rectifiable

current and

on

(n - 1 )-forms

with

compact support

in 03A9 x R n. On the other hand

and

Annales de l ’lnstitut Henri Poincaré - Analyse non linéaire

(8)

so that

Since

Rn

=

0,

we

get

and therefore

This

implies

as

o~~ A1 ~ _ Al

x

Rn)

=

0,

where ~ is the map

(x, y)

--~ x.

This

gives

a contradiction since

by

Lemma 1 we then have

|A2|

= 0. D

We shall now show that maps in dif

(Q,

do not cavitate. Results

of these

type

are

relatively simple

if one has some control on the

boundary.

Indeed we have

PROPOSITION l. - Let SZ be a bounded open connected set in Rn and let

u E

dif 1 ( SZ, Rn). Suppose

that

is

compact

and let

the

decomposition of

the

complement of

K into connected

components,

where

Uo

is the unbounded component. Then

and for each I

=

1,

...,

m we have either |(03A9)~Ui|

= = 0.

In

particular, if

m -

1,

then

Vol. 12, n° 1-1995.

(9)

Proof. -

It is an easy

application

of the

constancy theorem,

see e.g.

[11].

In fact

is an n-dimensional rectifiable current in

Rn

with

multiplicity

one and

~ u(S2) n Ui]

is

boundaryless

in

Ui.

The last statement follows then at once

as

]

> 0 because of det Du > 0 a.e. 0

Remark 3. - A

simple

consequence of

Proposition

1 is the result in

[12].

In fact one

easily

sees that the class

Ap,q

introduced in

[12]

is a

subclass of dif

and,

if is the current carried

by

the

graph

of a continuous map u, then K C

Our last theorem concerns the

regularity,

in the sense of

non-cavitation,

of weak

diffeomorphisms

without any control on the

boundary.

We

consider a bounded and

simply

connected domain H in R n. We denote

by

d : S~ ~

(0,oo)

a

Whitney’s regularized

distance

function, i.e.,

a smooth function

d(x)

which is

equivalent

to dist

(x,

for x E H. We then

assume that

(S)

For some

bo

> 0 the open sets

are connected

for

all b with 0 b

bo.

THEOREM 3. - Let 03A9 C Rn be a connected domain

satisfying (S)

and let

u E

dif 1 ( SZ, Rn).

Then

for

almost every

b,

0 b

bo,

the

image ic ( SZs ) of SZs

and

R n B

are both

essentially

connected.

Proof. -

Set

Ob

:=

ic(SZs),

0 b

bo.

We know that

ic(S2s)

is ess-

connected. Assume on the

contrary

that

R n B Os

is not ess-connected for

a non zero measure set of b’ s. For almost every such S’ s

is of course a rectifiable current with finite mass,

consequently Ob

is a

Caccioppoli

set, as

7r

being

the map

(x, y)

-~ y. Fix now one such a 8. We claim that for almost every

81

with 0

81 b

we have

Annales de l ’lnstitut Henri Poincaré - Analyse non linéaire

(10)

and moreover

In order to prove

(10)

we first observe that

where

because f satisfies the double Lusin

property.

From this we

easily

infer

where

On the other hand the trace u of u on

~03A903B41 belongs

for a.e.

81

to

W1,1(~03A903B41, n), Hn-1

almost every

point

in

~03A903B41

is a

regular point

for

u and ~c, and

moreover

compare e.g.

[6]. Denoting

the Lusin

representative of u,

we then

infer that

consequently

Since the set

{x

E

~03A903B41 n Ru

E 9

039403B4}

differs form

E81 by

a null set

and n has the Lusin

property

on

~03A903B41,

we

finally

infer

( 10)

from

( 11 ).

We now choose

81

in such a way that

(9)

and

(10)

hold.

Setting

Vol. 12, n° 1-1995.

(11)

(10) yields

On account or our

assumption,

R :=

Rn B

is not ess-connected.

We can then find

disjoint

open sets

U1, U2 C Rn

such that

Being ic

one-to-one in H we have

and

if we take into account

(13)

and

(14).

From Theorem 2 we know that C is

ess-connected,

hence one of the addenda of

(15),

say C

nul,

must be a null set

consequently

From

(12)

we therefore obtain

Now we define

and

observing

that

B, U1, U2

is a

covering

of

Rn,

we

get

consequently

~- ~ _

0,

if we take into account

(16).

We therefore conclude that either B = R" a.e. or = 0. Because of

(13)

we

finally

infer

B =

Rn

a.e.

and,

because of

(17),

that

which

contradicts

0 in

(13).

Q

Annales de l ’lnstitut Henri Poincaré - Analyse non linéaire

(12)

We shall now show

by

means of a few

examples

that Theorems 2 and

3 are in some sense

optimal.

Our first

example

shows that

u(S2)

may be disconnected.

Example

1. - Let 52 =

(-1, 1)2

C

R2

and let a E

(0,1).

Consider the map u : S2 ~

R 2

defined

by

- 1,1 -

We have u E

dif 1 SZ, Rn

In fact

G u

where u~ is the

family

of maps defined

by

It is

immediately

seen that

is not

connected,

but it is ess-connected. Notice that instead for the

approximately

continuous

representative u

of u we have

in tact x

(-1,1)

is

mapped

to zero and

by

the Hausdorff estimates of the

singular

set of u we cannot have

~0}

x

(-1,1)

C

S2 ~

We therefore

see that is connected

according

to Theorem 1.

Finally

we notice that Theorem 2 does not hold for Cartesian maps as it is shown

by

the

following

variant of the

previous example.

Set

and

Then it is

easily

seen that

is not ess-connected while it is connected in the usual sense.

Vol. 12, n° 1-1995.

(13)

Example

2. - We

identify R2

with the

complex plane C,

we set

and we consider

u(z) .- z2

for z E H. In the a.e. sense we have

Clearly

is not

essentially connected,

while

n Ru)

is

essentially

connected for all 6 > 0.

The map u is of course of class

C1

in H and its exact

image (not

the

a.e.

image)

is

given by

n

Au)

which is

simply

connected in the usual sense.

The next

example

of a discontinuous weak

deffeomorphism

shows that

in

general R2 B

n

Au)

need not be connected

(in

the usual

sense).

Example

3. -LetH=

B(0, 2) C R2, Q = ~(~1, ~2)

-~-

] 1~,

and u =

(u1, U2) : B(0,2)

-~

R2 given by

One can show that u E

dif ( SZ, R2 ) (in

fact u for all

p, q

2), by approximating u by

a sequence of smooth maps for instance

One then sees that

while u is not

approximately

continuous at

(0, 0) .

Thus we have

which is not

simply connected,

but n and

R2 ~

n

Lu)

are

both

essentially

connected.

Example

3 shows that weak

diffeomorphisms

may create holes of zero measure.

Annales de l ’lnstitut Henri Poincaré - Analyse non linéaire

(14)

REFERENCES

[1] H. FEDERER, Geometric measure theory, Grundlehren math. Wissen. 153, Springer-Verlag, Berlin, 1969.

[2] M. GIAQUINTA, G. MODICA and J. SOU010DEK, Cartesian currents and variational problems for mappings into spheres, Ann. Sc. Norm. Sup. Pisa, Vol. 16, 1989, pp. 393-485.

[3] M. GIAQUINTA, G. MODICA and J. SOU010CEK, Cartesian currents, weak diffeomorphisms

and existence theorems in nonlinear elasticity, Arch. Rat. Mech. Anal., Vol. 106, 1989, pp. 97-159. Erratum and addendum, Arch. Rat. Mech. Anal., Vol. 109, 1990, pp. 385-392.

[4] M. GIAQUINTA, G. MODICA and J. SOU010CEK, A weak approach to finite elasticity, Calc. Var., Vol. 2, 1994, pp. 65-100.

[5] M. GIAQUINTA, G. MODICA and J. SOU010CEK, Graphs of finite mass which cannot be approximated in area by smooth graphs, Manuscripta Math., Vol. 78, 1993, pp. 259-271.

[6] M. GIAQUINTA, G. MODICA and J. SOU010CEK, Remarks on the degree theory, 1993.

[7] E. GIUSTI, Precisazione delle funzioni H1,p e singolarità delle soluzioni deboli di sistemi ellittici non lineari, Boll. UMI, Vol. 2, 1969, pp. 71-76.

[8] C. GOFFMAN, C. J. NEUGEBAUER and T. NISHIURA, Density topology and approximate continuity, Duke Math. J., Vol. 28, 1961, pp. 497-505.

[9] C. GOFFMAN and D. WATERMAN, Approximately continuous transformations, Proc. Am.

Mat. Soc., Vol. 12, 1961, pp. 116-121.

[10] J. LUKE0160, J. MALÝ and L. ZAJÍ010CEK, Fine Topology Methods in Real Analysis and Potential

Theory, Lecture notes 1189, Springer-Verlag, Berlin, 1986.

[11] L. SIMON, Lectures on geometric measure theory, The Centre for mathematical Analysis, Canberra, 1983.

[12] V.

0160VERÁK,

Regularity properties of deformations with finite energy, Arch. Rat. Mech.

Anal., Vol. 100, 1988, pp. 105-127.

[13] W. P. ZIEMER, Weakly differentiable functions, Springer-Verlag, New York, 1989.

(Manuscript received November 18, 1993.)

Vol. 12, n° 1-1995.

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