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(1)

R ENDICONTI

del

S EMINARIO M ATEMATICO

della

U NIVERSITÀ DI P ADOVA

S ERGIO C AMPANATO

Partial Hölder continuity of solutions of quasilinear parabolic systems of second order with linear growth

Rendiconti del Seminario Matematico della Università di Padova, tome 64 (1981), p. 59-75

<http://www.numdam.org/item?id=RSMUP_1981__64__59_0>

© Rendiconti del Seminario Matematico della Università di Padova, 1981, tous droits réservés.

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(2)

Continuity

of Solutions of Quasilinear Parabolic Systems

of Second Order with Linear Growth.

SERGIO CAMPANATO

(*)

1. Introduction.

Let S~ be a bounded open set of 2

(1),

with

sufficiently

smooth

boundary aS2,

for instance of class C3. Let N be an

integer

&#x3E; 1, (I)

the scalar

product

and the norm in .RN

(2).

If

~c : we set Du = where

Da -

In

general

p = denotes a vector of

.RnN, x

is a

point

of Rn

t E .R

We say that

Q(Xo, a) cc Q

if

(*)

Indirizzo dell’A.: Istituto Matematico L. Tonelli - Via Buonarroti 2 - 56100 Pisa.

(1)

This is

just

to fix ideas; the case n = 2 can be dealt with

by

trivial

modifications.

(2)

In

general (J)k’

are the scalar

product

and the norm in Rk. We

shall omit the index k if there is not

ambiguity

of

writing.

(3)

and are the usual Sobolev spaces. If p = 2 we write sim-

ply

Hk and

Let us consider the

quasilinear parabolic system

of second order

where

.Ail

are N X N matrices which are

uniformly

continuous and bounded in and

satisfy

the

strong ellipticity

condition

fi(X, u),

i =

1,

..., n, and

f °(X,

are vectors of

RN,

measurable

in and continuous in u and

(u,p) respectively. Suppose

that

have linear

growth

with

We

set,

for the sake of

brevity,

y

(4)

A solution of

system (1.1 )

is a

0, H1(Q, .RN))

such

that

A solution of

Cauchy-Dirichlet problem

is a such that

It is known

that,

even if g is

smooth,

there are solutions of

system (1.1)

which fail to be Holder continuous

in Q (3).

We shall prove, in section

3,

the

following partial

H61der

continuity

result:

THEOREM 1.I.

I f u

E

L2 (- T, 0, H1(Q, RN))

is a solution

of system (1.1 )

and

then there is a set

Qo c Q,

closed in

Q,

such that

and

for

every open subset A cc

(3) i.e. on every

compact

set

(4)

C

depends

on the

L2(Q)-norm

of gi, go and on the distance of A from the

parabolic boundary

of

Q.

(5)

Here is the n-dimensional Hausdorff measure with

respect

to

the metric

and also Holder

continuity

in

(1.16)

is related to this metric.

The

previous

result is

proved

also in

[9]

with a different tech-

nique,

for the

special

case

f i =

0

(5).

The method of this paper can be exstended to the case of

systems

of order

2~n ~ 2

and to more

general growth

conditions on the vec-

tors

f i, 10.

In order to prove theorem 1.1 we need a local Ll

regularity

result

of this kind: We set

where u6

is the average of u on

Q(X,, a)

THEOREM 1.11.

I f

u E

L2(- T, 0, RN))

is a solution

of system

(1.1)

and

(1.14) holds,

then we can

find

q &#x3E; 2 such that

’v’Q(Xo, 2a)

cc

Q

with d c 1

Theorem 1.11

easily follows,

via H61der

inequality,

from the fol-

lowing

local Z~ result

proved

in

[5]:

THEOREM 1.III.

If u is a solution of system (1.1),

we can

f ind

(5)

In this case a can be every real number less than 1, because we are in the situation gi, go E

LOO (Q).

(6)

In

fact, by

Holder

inequality

In the same way, as

pn/(n + 2)

&#x3E; 2 and we can suppose

From

(1.23),

we then

get

and therefore

(1.21).

2. Some

lemmas.

We list in this section a few lemmas that will be used in the rest of the work.

We set =

Q(O, or)

and =

B(O, or).

(6) 2* = 2n/(n - 2)

is the Sobolev exponent.

(7)

Inequality (2.1)

is well

known;

we

give

the

proof

for the reader’s

convenience:

Let

Bii

be N X N constant matrices which

satisfy

the

strong ellip- ticity

condition

Let

f belong

to

L2(Q(a), RN)

and let v E

.~2 (- or2, 0,

be a

solution of the

following parabolic system

(8)

LEMMA 2.11.

If hypotheses (2.2), (2.3) hold,

then

for

every r E

(0, 1)

PROOF. In = V‘

-E-

W where W is the solution of

Cauchy-

Dirichlet

problem

whereas

It is known

[11]

that W E

Hl(- a 27 0, L2 (B(a), RN))

and

where c is invariant with

respect

to the homothetical transformation

V’ verifies the

following inequalities,

as shown

in [1 ] :

Vi E

(0, 1)

here c is invariant under transformation

(2.9).

(9)

(2.4)

follows from

( 2.10 )

and

(2.8)

in a standard way. On the other

hand,

from

(2.11)

we

get

But lemma 2.1 and

(2.8) imply

that

Then

(2.5)

follows from

(2.12), (2.13).

LEMMA 2.III.

If

v E

RN)

then

for

every i E

(0, 1 )

(2.14)

is a trivial consequence of the

following

estimate

LEMMA 2.IV. Let

qJ, 1J’ be

non

negative functions de f ined

in

( 0, 0’],

let oc be

positive,

A &#x3E;

1,

B and

M &#x3E;

0 and suppose that V7: E

(0, 1 )

and

Ve 6

then Vi E

(0, 1)

and Ve E

(0, a)

where

K,

C

depend

on

A,

0153, 8.

The

proof

is the same as in lemma 2.IV of

[4].

(10)

LEMMA 2 . V. Let 99, WI

defined

in

( 0, d],

and W2,

defined

in

( 0, -~- oo)

be non

negative

and

nondecreasing functions. Let A,

a be

positive

con-

stants and 0 0153.

Suppose

that b’z E

(0,1)

E

(0, d]

If for

a

fixed S E (0,

cx -

(3)

we can

find

(feE

(0, d]

such that

See for

example [6],

lemma l.IV.

3. The

partial

Holder

continuity

theorem.

In this section we prove theorem 1.1.

Suppose hypotheses (1.2), (1.3), (1.4), (1.14)

hold and let u c- E

L2(- .~’, 0, RN))

be a solution in

Q

of

system (1.1).

As

we

get

from

(1.3), (1.4)

and

Then

[11]

and a standard

localizing argument (see [5],

n.

4) imply

that for every

cylinder Q *

= Q* X

(- AT, 0)

with and A E

( o,1 )

and

(11)

Here c

depends

on the

L(Q)-norms

of gi, go and on the distance of

Q*

from the

parabolic boundary of Q (7).

Hence, by

lemma

2.I, B1Q(Xo, ~)

cc

Q

where c

depends

on the of gi , go and on the distance of from the

parabolic boundary

of

Q.

For the

hypotheses

we formulated on matrices

u)

we can

find a bounded continuous function

(o(27),

defined for which is

increasing,

concave, such that

w(O)

= 0 and

VX,

Y E

Q

and E

1~N

where

6(X, Y)

is the

parabolic

distance

(1.18).

We can now prove the

following

lemma:

LEMMA 3.1.

If u is a

solution

of system (1.1 )

under the

hypotheses (1.14),

then

0’) cc Q

with

~~2,

E

(0, 1)

and VA E

(n, ~)

2vhere

and w is

defined

as in

(3.3).

PROOF.

By

theorem

1.11,

we can find r &#x3E; 2 such that

20") cc Q

with

J1

(12)

Consider For the sake of

brevity

we set

In

Q {.Xo , 0")

we write u = v

+

w where

whereas

As

there is one and

only

one solution w and

By

H61der

inequality

(13)

Then,

if we take into account

(1.14)

and if we set

we have

On the other

hand,

from

(3.3), (3.6)

and the fact that co is concave

(8),

we

get

From

(3.9), (3.11), (3.12)

and lemma 2.1 we draw the conclusion that

If we use lemma

2.II,

then we

get

the

following

estimate on v : Vi E

E (0, 1) and e 6

(14)

On the other

and, by (1.3)

and Holder

inequality

Lemma 2.111

implies

that b’z E

(0, 1)

and O or

From

(3.14), (3.15)

and lemma 2.IV we conclude that VA E

(n, ~)

and

VTE(0,1)

As it = v

+

w, from

(3.13), (3.16)

we

get by

a standard

argument

that VT E

(0, 1)

The

previous inequality

is trivial for 1 1 2 and we can add

1p(XO, 7:a)

to the left hand side because

by (3.15)

Therefore we have

proved (3.4).

We define

For a well known theorem

(Lebesgue)

(15)

and then

We can even say

something

more. We define the Hausdorff measure

~£¥

with

respect

to the metric

6,

as

usual,

where

6(E,)

is the diameter of

Ei

with

respect

to 6.

Then,

if we argue

as in

[9] (10),

we can show that

LEMMA 3.11. -

If

u is a solution

of system (1.1)

and

hypotheses (1.2), (1.3), (1.4), (1.14)

are

satisfied,

then

QBQo

and E

(0, ~

-

n)

we

can

f ind 0"1]

1 and r &#x3E;

0,

with

Q (.Xo ,

r

+

c

Q,

such that V Y E

E

Q (Xo, r)

and ’Bf 7: E

(0, 1)

In

particular, Qo

is closed in

Q.

. PROOF.

Having

chosen

Xo E QBQo,

we define

(11)

Having fixed q

E

(0, ~

-

n),

we choose 1

== ~ 2013

and qo

= q j2

(1°)

Proof of Theorem 2.

(11)

.g is the constant which appears

(3.4).

(16)

Therefore

By (3.23)

we can find 1 such that

Q(Xo, cc Q

and

As

Y2013~(Y,

is continuous in

Q,

we can find r such that

Q(Xo, r + 6n) c Q and

Then,

and such that

Q ( Y, a) cc Q, inequality (3.1)

and condition

(3.25) hold;

therefore

hypotheses

of lemma 2.IV

are satisfied with

col, W2 are defined as in

(3.22) .

Hence and

In

particular

Therefore

which means that is open and so

Qo

is closed in

Q.

Now the

partial

Holder

continuity

theorem

easily

follows from lemma 3.11. In

fact, recalling

the definition of

fl,

from

(3.21)

we

deduce

that,

if

Xoe

Y E

Q (Xo, r)

and í E

(0, 1),

then

(17)

By (3.2)

Therefore and re

(o, 1)

By [8],

the

previous inequality implies

that

b’oc 1- (n -f- 2)~p

and

This proves the theorem.

BIBLIOGRAPHY

[1] S. CAMPANATO,

Equazioni paraboliche

del secondo ordine e

spazi £2,03B8(03A9, 03B4),

Ann. Mat. Pura e

Appl.,

73 (1966).

[2] S. CAMPANATO - D. SACCHETTI - A. TARSIA, Risultati di

regolarità

per la soluzione del

problema

di

Cauchy

in

spazi

di Hilbert, Boll. U.M.I.,

12 (1975).

[3]

S. CAMPANATO,

Regolarità

C0,03B1 e

regolarità

Lp per soluzioni del

problema

di

Cauchy

astratto senza

l’ipotesi

di simmetria, Boll. U.M.I., 14-A (1977).

[4] S. CAMPANATO, Partial Hölder

continuity of

the

gradient of

solutions

of

some nonlinear

elliptic

systems, Rend. Sem. Mat. Univ. Padova, 59

(1978).

[5] S. CAMPANATO, Lp

regularity for

weak solutions

of parabolic systems,

Ann.

S.N.S. di Pisa, 7

(1980).

[6] S. CAMPANATO - P. CANNARSA, Second order non variational

elliptic systems,

Boll. U.M.I. 17-B

(1980).

[7] S. CAMPANATO, Sistemi ellittici in

forma divergenza. Regolarità

all’interno,

to appear in « Quaderni » S.N.S. di Pisa

(1980).

[8] G. DA PRATO,

Spazi £(p,03B8)(03A9, 03B4)

e loro

proprietà, Ann.

di Matem. Pura

e

Appl.,

69 (1965).

(12)

Hölder

continuity

with

respect

to the metric 6 defined in (1.18).

(18)

[9] M.

GIAQUINTA -

E. GIUSTI, Partial

regularity for

the solutions to nonlinear parabolic systems, Ann. di Matem. Pura e

Appl.,

97 (1973).

[10] O. A. LADYZENSKAJA - V. A. SOLONNIKOV - N. N. URAL’CEVA, Linear and

quasilinear equations of parabolic

type, Amer. Mathem.

Society,

translations of mathematical

monographs

(1968).

[11] J. L. LIONS,

Equations differentielles operationelles, Springer

(1961).

Manoscritto pervenuto in redazione il 17 dicembre 1979.

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