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International Journal of Mathematical Archive-2(5), May - 2011,

Page: 693-697

Available online through

www.ijma.info

STUDY OF NONLINEAR ELASTICITY PROBLEM BY ELLIPTIC REGULARIZATION

WITH LAMÉ SYSTEM

Meflah Mabrouk*

University of K. Merbah Ouargla, Algeria Department of Mathematics Faculty of Sciences

E-mail: [email protected]

(Received on: 06-01-11; Accepted on: 18-01-11)

--- ABSTRACT

I

n this work, we look for the existence and uniqueness of a function u = u(x, t), x , t [0, T] solution of the nonlinear boundary value problem by the elliptic regularization techniques based on theory of monotone operators.

Keywords: Priori estimates, monotone operators, Lamé system, elliptic regularization.

---

1. NOTATIONS AND POSITION OF THE PROBLEM:

Let an open bounded domain of IR , with regular boundary . We denote by Q the cylinder IRt: Q = × [0,T],

with boundary . L designed Lamé system define by + ( + ) div, and are constants Lamé with + 0. and h, f are functions. We look for the existence and uniqueness of a function u = u(x, t), x , t [0,T], solution of the problem (P):

(P) ! " #

$ $ % $ &

$ $ % $ '

(

(1.1)

2. EXISTENCE OF THE SOLUTION:

Theorem: 1 Assume that is bounded open of IR are given f, with f L(Q). Then there exists a function u = w)+w satisfying (P)

*+, -+. / 0 1 / 2 0+. 1 / (1.2)

* , 3 %4 -+. / 5 (1.3)

* , (1.4)

Proof: we use an approach due to G. Prodi [11] we have

6

7+ 7

7+ 89:9 89 ; ! %

< 78; +=

(

(1.5)

We introduce the Prodi idea (1. 5) in (1.1.1) we having

+ (1.6)

We consider the derivative of (1.6) we obtain

> >?

>@

>? (1.7)

---

Meflah Mabrouk*

[email protected]

(2)

Page: 693-697 And

6 < 8;

= +

%

$ $ %

(

(1.8)

We deduce to (1.7)

A+ 7 ;A A+ 89:9 89 ; ! ; (1.9)

For resolve (1.7) and (1.8) we denotes. L = -A; β(

And we define the functional space V:

V=B CD C, 3 % -+

. / 54 C , 3 %

-+. / 5 2 4

C , 3 % / 54 < C ; 8; 4+= C % C 4 C % C ( (1.10)

The Banach structure of V is defined by

ECEF ECEGHI+ = JKL / M EC EGHI+ = JKL / M ECEGNO ECEGHI+ = GH/ M

We define the bilinear form:

P C < Q+= C R C C S8; (1.11)

The weak formulation of (1.7) and (1.8) is to find TU such that

P C <+= C 8; CTU (1.12)

Following some ideas of Lions for obtain the elliptic regularization, given > 0 and C TU we define

VW C X < Q C R C S8Y < Z R C 8Y

= + =

+ (1.13)

The application C [ VW C is continuous on U so there existes an application VWT U D

VW C = (\W C (1.14)

The linear operator \W : U U satisfies the four properties:

\Wis bounded in U for all bounded set in U and is a hemi continuous and is a strictly monotonous and is coercive. In view of these properties and as consequence of theorem of Lions [5], there exist unique a function WT UD

VW W C <+= C 8; C,U (1.15)

2.1 A PRIORI ESTIMATES I:

Explicitly the elliptic regularization (1.15) and setting C = W, we obtain:

X < Q= W E WE S8; < Q+= W W W S8; <+= W 8;

+ (1.16)

Or

<+= 8; E EGNO and < 8;+= = 0 E EGHI+ = JKL / M ]E EGHI+ = JKL / M

Then

Wis bounded in when X [ (1.17)

X < Q= W W E WE S8; ]

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Page: 693-697 Or

<+= W8; we have by (1.17) and (1.18) that:

Wis bounded in (1.19)

X < E= WE 8; ]

+ (1.20)

2.2 A PRIORI ESTIMATES II:

Exchange in (1.15) v with:

C ; < W Y 8 L^< % Y W Y 8Y =

+ =

+ (1.21)

We verify that:

_< C8;+= `C U

C W

( (1.22)

Taking into account (1.21) in (1.15) we get

X a Q W W W W R W W S8; aQ W W W W E WE S8;

=

+ =

+

< b+= W W 8; <+= W 8; (1.23)

By using periodicity of W WT U we obtain:

<= W W 8; < R+= W W 8;

+ (1.24)

And

< 3= W W58; 3 W % W % 5 3 W W 5 <+= W W 8; <+= W 8;

+ (1.25)

By (1.24) and (1.17) we have

c< 3+= W W58;c d ] 7A9 X [ (1.26)

Also, from (1.17) and (1.19) we obtain:

c< b+= W W 8;c d Eb W EGNO E WEGNO d ] #e

]fghijijk #' #l #e *imn #& *o popqro

< E+= WE 8; ] (1.28)

2.3 PASSAGE TO THE LIMIT:

From (1.17) and (1.28) that there exists a subsequence from W , such that

W[ 79st 3 % -+. / 5 (1.29)

W[ 79st (1.30)

b W [ u 79st 1 (1.31)

Passage to the limit in (1.15) we obtain

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Page: 693-697 Use the convolution technical in (1.32) we have

< u+= v wWv wW 8; <+= v wWv wW 8; `C U (1.33)

When

< u+= 8; <+= 8; `C U (1.34)

3. UNIQUENESS OF SOLUTION:

Theorem: Under the hypotheses of the theorem of existence, we consider two solutions ux and uyof the problem (P) then ux= uy

Proof: We subtract the equations (1.5) corresponding to ux and uy and sitting z = ux-uy we have:

z z {z b x b y (2.1)

Denoting by (wW) the regularizing sequence a similar argument by Brézis [2] we obtain

z v wWv wW z v wWv wW (2.2)

Hence, by using (1.2) and (1.3), we have

z | z+} z+ U s 8 | 3 % -+. / 5 (2.3)

From (2.2) we get

z v wWv wW z v wWv wW | v wWv wW # '

Show that

a z z v wWv wW 8; =

+ When

<+=>?> z z v wWv wW 8; < z z v w+= Wv wW 8; < z z v w+= Wv wW 8; # < z z v w+= Wv wW 8;

(2.5)

Therefore

< z z v w+= Wv wW 8; .<+=>?> z z v wWv wW 8; (2.6)

z ~jp wW Periodic then we have

< z z v w+= Wv wW 8; < z z v w+= Wv wW 8; < {z z v w+= Wv wW 8; (2.7)

From (2.1); (2.6) and (2.7) we obtain:

<+= . z v wWv wW (2.8)

Passage to the limit in (2.8) we have

<+= . . 8; (2.9)

Where

. • . (2.10)

This implies that

z= .- .= , independent of t (2.11)

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Page: 693-697

< {+= 8; ` U (2.12)

We deduce from (1.2)

ƒ , -+. / 0 1 / 2 0+. 1 / (2.13)

By (2.12) and (2.13) and using theorem of Green we have (A , ) = 0• = 0.

where the uniqueness of solution.

ACKNOWLEDGEMENT: The author would like his thanks to the Prof. B. Merouani and LAMA Ferhat Abass University.

REFERENCES:

[1] R.A. Adams, Sobolev Spaces, Academic Press, (1976).

[2] H. Brezis, Analyse fonctionnelle, théorie et applications. Masson (1983).

[3] H. Brezis, Equations et inéquations non linéaires dans les espaces vectoriels en dualité, Ann, Ins.Fourier; 18, (1968), 115-175.

[4] G.Duvaut, J.L. Lions, Les inéquations en mécanique et en physique. Dunod. Paris. (1972).

[5] J.L. Lions, Quelques méthodes de résolution des problèmes aux limites non linéaires. Dunod. (1969).

[6] Luc Tartar, Topics in non lineair analysis. Université de Paris-Sud, Publications Mathematiques d'Orsay, novembre (1978).

[7] M. Meflah, A Nonlinear Elasticity Problem by Elliptic Regularization Technics, Int. J. Contemp. Math. Sciences, Vol 6, 2011, no. 25, 1221-1229.

[8] M. Meflah, B Merouani, A Nonlinear Elasticity Problem Governed by Lamé System, Applied Mathematical Sciences, Vol.4, 2010, no. 36, 1785-1796.

[9] B. Merouani, M. Meflah, A. Boulaouad, The Generalized and perturbed Lamé system, Applied Mathematical SciencesVol.2, 2008,no. 49,2425-2430.

[10] F. Messelmi, B. Merouani, M. Meflah, Nonlinear thermoelasticity problem, Analele Universitatii Oradea, Fasc. Matematica,Tom XV (2008), 207-217.

[11] G. Prodi, Soluzioni periodiche dell'equazione delle onde com termine dissipativo nonlineare.Rend. Sem.Mat. Pandova, 35 (1965).

[12] V. Patron, P. Perline, Méthode de la théorie mathématique de l'élasticité, Editions Mir, Moscou, 1981.

[13] Taylor M.E, Partial differential non linear equations III Springer. (1996).

[14] K. Yosida, Functional Analysis, Springer-Verlag Berlin Heidelberg New York 1968.

References

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