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R ENDICONTI

del

S EMINARIO M ATEMATICO

della

U NIVERSITÀ DI P ADOVA

G. D A P RATO M. I ANNELLI

Linear abstract integro-differential equations of hyperbolic type in Hilbert spaces

Rendiconti del Seminario Matematico della Università di Padova, tome 62 (1980), p. 191-206

<http://www.numdam.org/item?id=RSMUP_1980__62__191_0>

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(2)

Integro-Differential Equations

of Hyperbolic Type in Hilbert Spaces.

G. DA PRATO - M.

IANNELLI (*)

Introduction.

This paper is concerned with the

study

of the

problem:

where for

t:&#x3E;O, A(t)

is the infinitesimal

generator

of a

strongly

con-

tinuous

semi-group

in a Hilbert

space H and

X is of the form

where

B(~)

is

self-adjoint

and

semi-bounded;

K is then a vectorial

generalization

of a

completely positive

kernel.

We

study

this

problem

with the same methods of sum of linear

operators

as in

[8].

We are

able,

under suitable

hypotheses,

y to show existence and

uniqueness

of a continuous

strong

solution u for every and

x E g;

moreover u is a classical solution if

T; K),

where K is a Hilbert space

densely

and

continuously

embedded in H and x E K.

(*) Indirizzo

degli

AA.:

Dipartimento

di Matematica, Universita di Trento - Povo.

Lavoro svolto nell’ambito del G.N.A.F.A.

(3)

Similar

problems

have been studied

by

several authors

by

different

methods,

in the autonomous case. We remark that we do not assume

that the domains of

A(t)

and

B(~)

are constant.

For the

proofs

we need an « energy

equality » (see

formula

(21))

that we think will be useful to

study asymptotic properties

of u.

1. Notations.

We note

by

H a real Hilbert space

(1) (inner product ( , ),

norm

(.)

and

by L2(o, T; H)

the Hilbert space of the measurables map-

pings

~c :

[0, T] - H

such that

JU 12

is

integrable

in

[0, T],

endowed

with the inner

product:

We

put:

It is well known that every u E

T] ; H)

can be identified with

a continuous function

(2);

in the

following

we

always

make such an

identification.

We note also

by 0([0, T]; H) (resp. 01([0, T]; H))

the set of map-

pings

continuous

(resp. continuously derivable);

it is

~’] ~ H) c C( Co, z’] ~ .g) .

Finally

we

put:

We

write,

for

brevity, L2(g),

7

Wo(.t1), C(H), 01(H).

We

study

the

problem:

(1)

We

suppose H

real for

simplicity.

(2) See for

exemple

[3].

(4)

We assume:

B is and

3WB

E R such that B - WB

0,

7

~ c :

[0, l ]

-~ measurable and bounded such that

We write

(P)

in the

following

form:

x}

is

given

in and yo is defined

by:

We consider also the

approximating problem:

where

Bn

=

n2R(n, B) - n.

It is well known

([8])

that

(Pn)

has a

unique strong

solution un E

C(.8’) ;

moreover if

f

E and x e

j9~

it is:

because 7~ E

01([0, T] ~ .

(3) If L: is a linear operator we note

by (resp.

the resolvent set (resp. the spectrum) of L and

by

L) the resolvent operator of L.

(4) It is known that

DA

is dense in H.

(5) This

hypothesis implies

that the operator Lu = k * u is

completely positive

in

L2(0,

T; H); for the existence of a solution of (P) it will be suf- ficient to assume L

positive.

(s )

D~

and

D,

are endowed with the

graph

norm.

(5)

2. A

priori

bound.

PROPOSITION 1. Assume

(H)

and let Un be the solution

of (Pn),

then

it is :

PROOF. Choose

f

E E

D,4; put

exp

[- t~~ ~ ~cn

= it is

u~ =

vn~ -E- multiply by

then it is :

integrating

from 0 to t we

get:

(6)

and the conclusion follows from the Gronwall lemma for

f

E

W((H);

in the

general

case we use the

density

of

w’1(g)

in

L2(H).

COROLLARY 2. Under the

hypotheses of

the

Proposition 1, if

u is

a classical solution

of (P) (7)

it is :

where K is a suitable constant.

PROOF. It is :

using (3)

we obtain

and the conclusion follows

by

dominated convergence.

3.

Strong

solutions.

PROPOSITION 3. Assume

(H)

and suppose

DA n DB

dense in

H;

then yo is

pre-closed.

PROOF. Let c

DYo

such that :

(7)

we have to show that

f

=

0,

x = 0. From

(5)

it follows

therefore is a

Cauchy

sequence in

O(H)

and furthermore

Ui -+ 0

in

C(H);

then .r = == 0.

We,

now, go to show that

f

= 0.

i - oo

Remark

that,

since

A - WA,

I

(B - CùB) k *

are

positive operators

in

L2(H)

it is:

Choose g

in n which is dense in

L2(H),

from

(7)

it follows

Then f or i - o0

and

Finally

for

which

implies f

= 0.

In the

following

we denote

by y

the closure of yo. We call u E

L2(H)

a

strong

solution of

(P)

if it is :

(8)

i.e. if there exists E r1 r1

L2(DB)

such that

It is not easy in

general

to characterize the domain

D(y)

of y; how-

ever we can show that

D(y)

c

C(H)

and that if u E

D(y),

y - u

= ff, t x}

then

n ( o )

= x.

The

following proposition

is

straightforward:

PROPOSITION 4. Under the

hypotheses of

the

Proposition

3

if

u E

D(y~.

and

= (f, x~

then

(5)

and

(6)

hold.

Moreover y is one-to-one and has a closed range;

consequently (P) has,

at

most,

one

strong

solution.

PROPOSITION 5. Assume that the

hypotheses of Proposition

3 are

fulfilled. Let

u

E D(y), = (f, xl;

then u E

O(H)

and it is:

PROOF. Let c

D(yo)

such that

from

(6)

it follows

Thus is a

Cauchy

sequence in

C(H)

which

implies

vi -’7- U

in

C(H). Finally put

then z is a

strong

solution of the

problem:

(9)

from

(5)

it follows

and in

C(H).

4. Existence.

If Z : is a linear

mapping

and g a

sub-space

of H we

denote

by LK

the

following mapping

in K:

It is easy to see that if A E

e(L)

r1

e(LK)

then it is

R(A, L)(K)

c K

and

RK(Â, L)

=

R(A, LK) (8).

THEOREM 6. Assume that the

hypothesis (H)

holds and that there ,exists a Hilbert space K

(inner products ((,)),

norm

II densely

em-

bedded in H such that:

a) K n DA

is dense in H

(9),

b)

such that

+ cxJ[ ((A. y,

2

c) BK

is

self -adjoint

and such that

Then

b’ f

E

L2(.H),

b’x E

H,

the

problem (P)

has a

unique strong

solu- tion u such that u E

C(H), u(O)

= x.

lVloreover

’BIf

E

Wi(K)

and x E K r1

DA

the solution u

belongs

to

i.e. it is a classical solution.

(8) L) is the restriction of L) to K.

(9)

K4DB

means that .K is

continuously

and

densely

embedded in

DB,

(10)

PROOF.

By

virtue of the closed

graph

theorem it is B E

H) put

It is clear that

DAn DB

is dense in

1~,

therefore yo is

pre-closed (Proposition 3). Finally,

due to the

Corollary 4,

to show existence it is sufficient to prove

that y

has a range dense in

L2 (H) O

H.

Take and let un be the classical solution in H of the

problem ( lo ) :

from

Proposition

1 there exists N &#x3E; 0 such that

it follows

due to

(18) ~N’ &#x3E;

0 such that

It is

then

if T

E

L2(DB)

it is

By

virtue of

(19)

is bounded in

L2(H),

it follows

because

L2(DB)

is dense in

L2(g).

(lo)

See inclusion (2).

(11)

- means weak convergence.

(11)

Consequently

the range of y, is

weakly

dense in

y is onto.

We prove now the

regularity

result. Recall that Un - u in

(Proposition 5);

moreover due to

(19)

3 a

sub-sequence

such

that is

weakly Cauchy; consequently u E DB

and

by

virtue

of

(18)

u E

LOO(K).

Consider now the

problem:

and the

approximating

one

It is in =

~n and vn

2013~

(Proposition 5);

it follows v = u’ and because

Finally

it is easy to see that u E

DA

and Au = u’ -

f

- E

E L2(H).

~

5. Generalizations.

We

generalize

now the

problem (P).

We consider two families

A = &#x3E; of linear

operators

in H. We

put:

and the

study

the

problem:

(12)

We write

( P ‘ )

in the

following

form:

where

yo

is defined

by:

We consider also the

approximating problem:

If u E

multiplying (P’ )

for

u(t)

and

putting

v~ = exp

[- t~] ~

u

we

get

the energy

equality:

We prove the theorem:

THEOREM 7. Assume that:

(13)

Then E

L2(H),

x E

H, 3a unique strong

solution

C(H).

More-

over

if

U E

_L2(.g),

x E K then it is u E

W1(.g)

f1

We can write the

problem (P[)

in the

following

f orm :

where

Z(t,8)

are the evolutions

operators

attached to the

family

A.

If we can solve

(22) by

the contraction

principle (1~) ~

therefore

+ f

E

L2(K)

which

implies

Un E n

([8]).

Using

the energy

equality

in the I~ space we

get:

Via

e

L2(K), x c-

&#x3E;

0;

Proceeding

as in

previous

sections we are able to show:

a) yo is preclosed

and its closure

y’

is one-to-one and with a

closed range.

b )

3N’ &#x3E; 0 such that

c)Itis

It follows that

y’

is onto and 3 a

unique strong

solution u of

(P’ )

for

every

f c-L2 (H);

moreover u in

L2(H).

Concerning regularity

we remark that if x E

K, f

E

L2(g),

then

by

virtue of

(24)

Bu

belongs

to

L2(H)

and

recalling (23) u

E

L°°(.K), consequently

Au E

L2(H)

and

REMARK 8. For sake of

simplicity

we have assumed K c

D(A(t))

r)

r1

D(B(~))

instead of K c

D(B($))

as in

previous section; actually

similar results can be

proved

with this latter

assumption.

(12)

In fact Z is

strongly

measurable and bounded in .K [8].

(14)

6. Resolvent

family.

Assume that the

hypotheses

either

(H’ )

or

(H)

and

(HE)

hold.

Consider the

problem:

where K = Bk if

(H)

and

(HE)

hold.

Due to Theorem 7

(PS )

has a

unique strong

solution. Moreover if

(H’) (resp. (H)

and

(HE))

hold and x c K

(resp.

then u

is classical. Put:

it is

G(t, s)

E

C(H).

The

mapping:

is called the evolution

operator

for the

problem (P~)

and the

family

~G(t,

the resolvent

family.

Consider also the

approximating problem:

and

put Un(t)

=

Gn(t, s) x.

PROPOSITION 9. For every x E H it is :

Therefore

(7( -, -) .r

E

H).

PROOF. It is sufhcient to prove

(27)

for

(resp. DA

r1

~)~

Put v = ~ - un, then it is:

(15)

from which

and the thesis follows from dominated convergence. #

PROPOSITION 10. Assume that the

hypotheses (H’) (resp. (H)

and

(H~))

hold.

If strong

solution

of (P’)

(resp. (P))

it is:

PROOF. Go to the limit in the

equality:

REMARK 11.

By

similar

arguments

we can

study

the

problem:

where

and p : [0, T]x[0,1] - R+

is continuous.

The energy

equality

is in this case:

(16)

where

is the solution of the

problem

EXAMPLE 12. Let H =

L2(R),

99 E

Co (R2 , R)

and

Then

(P’ )

is

equivalent

to

If U,

E L2(R)

and

f

E

.L2 ( [o, T]

X

R)

then

(35)

has a

unique strong

solu-

tion

T]; .L2(ll~)) ;

if moreover

T]

X

R)

and Uo E

W2(R)

then u is classical and it is

REFERENCES

[1] V. BARBU, Nonlinear Volterra

equations

in a Hilbert space, SIAM J.

Math. Anal., 6 (1975), pp. 728-741.

[2] V. BARBU, Nonlinear Volterra

integro-differential equations

in Hilbert

space, Sem. Mat. Bari, 143

(1976).

(17)

[3] H. BRÉZIS,

Opérateurs

maximaux monotones et

sémi-groupes

de con-

tractions dans les espaces de Hilbert, Math. Studies, 5, North Holland

(1973).

[4] M. G. CRANDALL - S. O. LONDEN - J. A. NOHEL, An abstract nonlinear Volterra

integro-differential equation,

J. Math. Anal.

Appl.,

64

(1978),

pp. 701-735.

[5]

C. M. DAFERMOS, An abstract Volterra

equation

with

applications

to linear

viscoelasticity,

J. Diff.

Eq.,

7

(1970),

pp. 554-569.

[6] C. M. DAFERMOS - J. A. NOHEL,

Energy

methods

for nonlinearhyperbolic integro-differential equations,

Comm. PDE, 4 (1979), pp. 219-278.

[7] G. DA PRATO - P. GRISVARD, Sommes

d’opérateurs

linéaires et

équations differentielles opérationnelles,

J. Math. Pures et

Appl.,

54 (1975), pp. 305-387.

[8] G. DA PRATO - M. IANNELLI, On a method to

study

abstract evolution equa- tions in the

hyperbolic

case, Comm. PDE, 1 (1976), pp. 585-608.

[9] G. DA PRATO - M. IANNELLI, Linear

integro-differential equations

in Banach

spaces, Rend. Sem. Mat. Padova, 62

(1980),

pp. 207-219.

[10] S. O. LONDEN, On an

integral equation in a

Hilbert space, SIAM J. Math.

Anal., 8 (1977), pp. 950-970.

[11]

S. O. LONDEN, On an

integro-differential

Volterra

equation

with a maximal

monotone

mapping,

J. Diff.

Eq.,

27 (1978), pp. 405-420.

[12] R. C. MAC CAMY,

Approximations for

a class

of functional differential equations,

SIAM J.

Appl.

Math., 23 (1972), pp. 70-83.

[13] R. C. MAC CAMY,

Stability

theorems

for

a class

of functional differential equations,

SIAM J.

Appl.

Math., 30

(1976),

pp. 557-576.

[14] R. C. MAC CAMY - J. S. W. WONG,

Stability

theorems

for

some

functiona.

equations,

Trans.

AMS,

164 (1972), pp. 1-37.

[15] R. K. MILLER - R. L. WHEELER,

Asymptotic

behavior

for

a linear Volterra

integral equation

in Hilbert space, J. Diff.

Eq.,

23 (1977), pp. 270-284.

Manoscritto pervenuto in redazione il 5

giugno

1979.

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