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PARABOLIC PROBLEM

ABDERRAHMANE EL HACHIMI AND MOULAY RCHID SIDI AMMI Received 22 February 2004 and in revised form 16 February 2005

A time discretization technique by Euler forward scheme is proposed to deal with a nonlocal parabolic problem. Existence and uniqueness of the approximate solution are proved.

1. Introduction

In this work, we study the time discretization by Euler forward scheme of the nonlocal initial boundary value problem

∂u

∂t u=λ f(u)

f(u)dx2 inΩ×]0;T[, u=0 on×]0;T[,

u(0)=u0 inΩ,

(1.1)

withΩRd(d1) a bounded regular domain andλa positive parameter. The hypothe- ses we will assume on f are the same as in [6]. We recall first that (1.1) arises by reducing the following system of two equations modeling the thermistor problem:

ut= ∇·

k(u)u+σ(u)ϕ2,

σ(u)ϕ=0, (1.2)

whereurepresents the temperature generated by the electric current flowing through a conductor,ϕthe electric potential,σ(u) andk(u) are, respectively, the electric and ther- mal conductivities. For more description, we refer to [5,6,7,8,11] among others.

We recall also that the Euler forward method was used by several authors to treat semidiscretization of nonlinear parabolic problems, see [3,4]. Concerning problem (1.1), results of existence and uniqueness of solutions are known under particular forms of f, we refer to [2] and the references therein. On the other hand, little is known about

Copyright©2005 Hindawi Publishing Corporation

International Journal of Mathematics and Mathematical Sciences 2005:10 (2005) 1655–1664 DOI:10.1155/IJMMS.2005.1655

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the solutions to the discrete problem

UnτUn=Un1+λτ fUn

fUndx2 inΩ, Un=0 onΩ,

U0=u0 inΩ.

(1.3)

Whereas, semidiscretization has been involved for the equations of the thermistor problem in [1,9]. Our aim here is to continue the study of problem (1.1) initiated in [6], where an a prioriL-estimate is derived. In addition to habitual existence and uniqueness questions concerning the solutions of (1.3), we will prove some results of stability and proceed to error estimates analysis. In [1], the authors derived anL2andH1-norm error by requiring more regularity on the solutionu, for instanceu,utinH2(Ω)W1,(Ω).

Unfortunately, such smoothness is not always possible since the function f is nonlinear.

2. The semidiscrete problem

2.1. Existence and uniqueness. We consider the Euler scheme (1.3), with=T,T >0 fixed, and 1nN, under the following hypotheses.

(H1) f :RRis a locally Lipschitzian function.

(H2) There exist positive constantsσ,c1,c2, andαsuch thatα <4/(d2) and for all ξR,

σf(ξ)c1ξα+1+c2. (2.1) In the sequel, we will denote the norms in the spacesL(Ω),Lk(Ω) by| · |L()and| · |k, respectively, (·,·) will denote the associated inner product inL2(Ω) or the duality product betweenH01(Ω) and its dualH1(Ω).

Theorem2.1. Let(H1)-(H2)be satisfied. Then, for eachn, there exists a unique solution Unof (1.3) inH01(Ω)L(Ω)provided thatτis small enough.

Proof. For simplicity, we writeU=Un,h(x)=Un1. Then (1.3) becomes UτU=h(x) +λ f(U)

f(U)dx2 inΩ, U=0 on∂Ω.

(2.2)

Existence. Define the mapS(µ,·) byU=S(µ,v),µ[0, 1] if and only if UτU=µg(x,v) inΩ,

U=0 onΩ, U0=µu0,

(2.3)

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whereg(x,v)=h(x) +λ(f(v)/(f(v)dx)2). For a fixedvH01(Ω), (2.3) has a unique solutionUH01(Ω). Then, for eachµ[0, 1], the operatorS(µ,·) is well defined. More- over,S(µ,·) is compact fromH01(Ω) into it self. Indeed, using (H2), we have the estimate

U22+τU22c3. (2.4)

We can easily see thatµS(µ,v) is continuous and thatS(0,v)=U, for anyv, if and only ifU=0. From Leray-Schauder fixed point theorem, there exists therefore a fixed pointU

ofS(µ,·).

Now, we derive an a priori estimate.

Lemma2.2. Ifu0L(Ω), then for alln∈ {1,. . .,N},UnL(Ω).

Proof. The proof is similar to the one used by De Th´elin in [10] concerning a very differ- ent problem and we will give here only a sketch. Suppose thatd2 and define

δ=

2d

d2 if 2< d, 2(α+ 2) ifd=2.

(2.5)

For eachkN∗, we consider the number qk= δ

2 k1

γ)(2γ) δ

δ2, k2, q1=δ,

(2.6)

we have

qk+1=

qk+ 2γδ

2 withγ=α+ 2,kN. (2.7) Lemma2.3. For allkN,UnLqk(Ω), and moreover

Un=limUnq

k<+. (2.8)

Proof. We prove by recurrence thatULqk. The property is true fork=1, sinceH01(Ω) Lδ(Ω). We show now thatULqk+1. LetmN, 1mk. Multiplying (2.2) by|U|qmγU, using (H2), and Young’s inequality, we get

qmγ+ 1

|∇U|2|U|qmγdxc4|U|qqmm+c5. (2.9) On the other hand, we have

|U|qqmm+1+2γc6

1 +qmγ 2

2

|∇U|2|U|qmγdx. (2.10)

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Therefore, we obtain

|U|qqmm+1+2γ

c7+c8|U|qqmm

qm+ 2γ. (2.11)

Thus,

|U|qqk+1k+1

2/δ

c7+c8|U|qqkk

qk+ 2γ. (2.12)

The rest of the proof follows the same lines as in [10, pages 383-384].

Uniqueness. ConsiderU andV two different solutions of (2.2) and definew=UV. Then, we have

wτw= λτ

f(U)dx2

f(U)f(V)

+λτ

f(U)f(V)dxf(V) +f(U)dx

f(U)dx2f(V)dx2 f(V).

(2.13)

Multiplying (2.13) byw, integrating onΩ, and using theL-estimate obtained inLemma 2.2, we get

|w|22+τ|∇w|22c9τ|w|22. (2.14)

Therefore,w=0 ifτ1/c9.

We address now the question of stability.

3. Stability

Theorem3.1. Assume(H1)-(H2)hold. Then, there existsc(T,u0)>0depending on data but not onNsuch that for anyn∈ {1,. . .,N},

(a)|Un|L(Ω)c(T,u0);

(b)|Un|22+τnk=1|∇Uk|22c(T,u0);

(c)nk=1|UkUk1|22c(T,u0).

Proof. (i) Multiplying (1.3) by|Uk|mUkfor some integerm1, usingLemma 2.2, and H¨older’s inequality, we obtain after simplification

Ukm+2Uk1m+2+c10τ. (3.1) By induction and taking the limit in the resulting inequality asm+, we get

UkL()cT,u0

. (3.2)

(ii) Multiplying the first equation of (1.3) byUk and using the hypotheses on f, one easily has

UkUk1,Uk+τUk22c11τUk1. (3.3)

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Using the elementary identity 2a(ab)=a2b2+ (ab)2and summing fromk=1 to n, we obtain

Un22+ n k=1

UkUk122+τ n k=1

Uk22u02

2+τc12

n k=1

Uk1. (3.4)

Then, the inequalities (b)-(c) hold by using the uniform bound ofUn inL which is

established in part (a).

4. Error estimates for solutions

We will adopt the following notations concerning the time discretization for problem (1.1). We denote the time stepτ=T/N,tn=nτ, andIn=(tn,tn1) forn=1,. . .,N. Ifz is a continuous function (resp., summable), defined in (0,T) with values inH1(Ω) or L2(Ω) orH01(Ω), we definezn=z(tn,·),zn=(1/τ)Inz(t,·)dt,z0=z0=z(0,·); the error en=u(t)Unfor all tIn and the local errorseunandendefined byeun=un(t)Un, en=unUn.

We have the following theorem.

Theorem4.1. Let(H1)-(H2)hold. Then, the following error bounds are satisfied:

(1)en2L(0,T,H1(Ω))+0T|en|2dtc13τ, (2)emH1()c14τ1/2,

(3)|∇T

0 en(t)dt|2c15τ1/4.

Proof. For the proof, we consider the following variational formulation of discrete prob- lem (1.3):

UnUn1+τUn,ϕ= λτ

fUndx2

fUn, ϕH01(Ω). (4.1)

Integrating the continuous problem (1.1) overIn, we get unun1,ϕ+τun,ϕ=λτ

fun,ϕ

fundx2, ϕH01(Ω). (4.2) Substracting (4.2) from (4.1) and adding fromn=1 tomwithmN, we obtain

m n=1

enen1+τ m n=1

eun,ϕ

c16τ m n=1

f(u)nfUn+c17τ m n=1

f(Un,ϕ.

(4.3)

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Let ()1be the green operator satisfying

()1ψ,ϕ=(ψ,ϕ)H1(Ω),H10(Ω) (4.4) for allψH1(Ω),ϕH01(Ω). Choosingϕ=()1(en) as test function, we then ob- tain

I1+I2I3+I4, (4.5)

where

I1= m n=1

enen1, ()1en,

I2=τ m n=1

enu,en,

I3c16τ m n=1

f(u)nfUn, ()1en,

I4=c17τ

m n=1

fUn, ()1en .

(4.6)

With the aid of the elementary identity 2a(ab)=a2b2+ (ab)2and the property of ()1,I1reduces after straightforward calculations to

I1=1

2em2H1(Ω)+1 2

m n=1

enen12H1(Ω). (4.7)

On the other hand, I2=τ

m n=1

enu,en

= m n=1

In

u(t)Un,u(t)Undt+ m n=1

In

u(t)Un,unu(t)dt

=I21+I22,

(4.8)

where

I21= m n=1

In

u(t)Un,u(t)Undt= m n=1

In

en2

2dt,

I22= m n=1

In

u(t),unu(t)dt m n=1

In

Un,unu(t)dt

=I221 +I222.

(4.9)

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We now estimateI221.Using the boundedness of∂u/∂s(see [6]), we have I221=

m n=1

In

u(t),

tn

t

∂u

∂sds

dt

m n=1

In

tn

t

∂u

∂s

H1(Ω)ds

u(t)H01(Ω)dt

τ∂u

∂s

L2(0,tm,H1(Ω))uL2(0,tm,H10(Ω))

c18τ.

(4.10)

In the same manner, we have I222τ∂u

∂s

L2(0,tm,H1(Ω))

τ

m n=1

Un2H01(Ω) 1/2

c18τ.

(4.11)

Next, we estimate the first term on the right-hand side of (4.5) by using H¨older’s and Young’s inequalities and (H1),

I3

m n=1

In

f(u)fUndt, ()1en

c20τ1/2 m n=1

In

f(u)fUn22dt 1/2

enH1()

η m n=1

In

f(u)fUn22dt

+c21

η τ m n=1

en2H1(Ω)

c22η m n=1

In

en2

2dt

+c21

η τ m n=1

en2H1(Ω).

(4.12)

Moreover, we have

I4c23τ+c24τ m n=1

en2H1(). (4.13)

Choosing suitableη, we conclude that em2H1(Ω)+

m n=1

enen12H1(Ω)+ m n=1

In

en22dt

c25τ+c26τ m n=1

en2H1(Ω).

(4.14)

On the other hand, settingym=m

n=1en2H1(), then from (4.14), we get

ymym1c25τ+c26τ ym. (4.15)

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By applying the discrete Gronwall inequality, we deduce that ymc(T). Therefore, we have

emH1(Ω)c27τ1/2. (4.16)

On the other hand, we have sup

t(0,tm)

en(t)H1()c27τ1/2 max

1nm

en

tnH1()= max

1nm

enH1(). (4.17)

Thus, we get

enL(0,T,H1(Ω))c27τ1/2 max

1nm

enH1(Ω). (4.18)

From the last inequality, we obtain

en2L(0,T,H1(Ω))+ T

0

en22dtc29τ, m

n=1

enen12H1()c29τ.

(4.19)

Choosingϕ=τmn=1(unUn) in (4.3), we get

τ

umUm m

n=1

unUndx

+τ2 m n=1

unUn

2

2

c30τ2

m n=1

f(u)nfUn m

n=1

unUn

dx +c31τ2

m n=1

fUn,

m n=1

unUn.

(4.20)

Thus,

τ2 m n=1

unUn

2

2

=

tm

0 endt

2 2τ

umUm m

n=1

unUndx +c30τ2

m n=1

f(u)nfUn m

n=1

unUn

dx +c31τ2

m n=1

fUn,

m n=1

unUn

I+II+III.

(4.21)

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Clearly,

IemH1(Ω)

m

n=1

In

u(t)H10(Ω)dt+τ m n=1

UnH10(Ω)

c32emH1()

c33τ1/2.

(4.22)

We also get II

m

n=1

In

f(u)fUndt 2

dx

1/2

×

m

n=1

In

u(t)Undt 2

dx

1/2

T2 m

n=1

In

f(u)fUn22dt 1/2

× m

n=1

In

u(t)Un22dt 1/2

T2 m

n=1

In

f(u)f(Un22dt 1/2

×

2u2L2(0,T,H01(Ω))+ 2τ m n=1

Un22 1/2

c34τ1/2.

(4.23) The last inequality follows by using simultaneously theL-estimate ofu(t) (see [6]),Un, and the error bound given in (a). Arguing exactly as in the previous estimate, we get

IIIT2 m

n=1

In

fUn22dt 1/2

×

2u2L2(0,T,H01(Ω))+ 2τ m n=1

Un22 1/2

. (4.24) Using again the hypothesis (H1) and the estimates above, we obtain

IIIc35τ1/2. (4.25)

Finally collecting these results, it follows that

T

0 endt

2

2c36τ1/2. (4.26)

This completes the proof.

Corollary4.2. Under hypotheses(H1)-(H2), problem (1.3) generates a continuous semi- groupSτdefined bySτUn1=Un.

References

[1] W. Allegretto, Y. Lin, and A. Zhou,A box scheme for coupled systems resulting from microsensor thermistor problems, Dynam. Contin. Discrete Impuls. Systems5(1999), no. 1-4, 209–223.

[2] J. W. Bebernes and A. A. Lacey,Global existence and finite-time blow-up for a class of nonlocal parabolic problems, Adv. Differential Equations2(1997), no. 6, 927–953.

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[3] F. Benzekri and A. El Hachimi,Doubly nonlinear parabolic equations related to thep-Laplacian operator: semi-discretization, Electron. J. Differential Equations2003(2003), no. 113, 1–14.

[4] A. Eden, B. Michaux, and J.-M. Rakotoson,Semi-discretized nonlinear evolution equations as discrete dynamical systems and error analysis, Indiana Univ. Math. J.39(1990), no. 3, 737–

783.

[5] A. El Hachimi and M. R. Sidi Ammi,Existence of weak solutions for the thermistor problem with degeneracy, Proceedings of the 2002 Fez Conference on Partial Differential Equations, Electron. J. Differ. Equ. Conf., vol. 9, Southwest Texas State University, Texas, 2002, pp.

127–137.

[6] ,Existence of global solution for a nonlocal parabolic problem, Electron. J. Qual. Theory Differ. Equ.2005(2005), no. 1, 1–9.

[7] A. A. Lacey,Thermal runaway in a non-local problem modelling Ohmic heating. I. Model deriva- tion and some special cases, European J. Appl. Math.6(1995), no. 2, 127–144.

[8] ,Thermal runaway in a non-local problem modelling Ohmic heating. II. General proof of blow-up and asymptotics of runaway, European J. Appl. Math.6(1995), no. 3, 201–224.

[9] P. Shi, M. Shillor, and X. Xu,Existence of a solution to the Stefan problem with Joule’s heating, J.

Differential Equations105(1993), no. 2, 239–263.

[10] F. de Th´elin,R´esultats d’existence et de non-existence pour la solution positive et born´ee d’une e.d.p. elliptique non lin´eaire[Existence and nonexistence results for a positive bounded solu- tion of a nonlinear elliptic partial differential equation], Ann. Fac. Sci. Toulouse Math. (5)8 (1986/1987), no. 3, 375–389 (French).

[11] D. E. Tzanetis,Blow-up of radially symmetric solutions of a non-local problem modelling Ohmic heating, Electron. J. Differential Equations2002(2002), no. 11, 1–26.

Abderrahmane El Hachimi: UFR Math´ematiques Appliqu´ees et Industrielles, D´epartement de Math´ematiques et Informatique, Facult´e des Sciences, Universit´e Chouaib Doukkali, B.P. 20, El Jadida, Morocco

E-mail address:[email protected]

Moulay Rchid Sidi Ammi: UFR Math´ematiques Appliqu´ees et Industrielles, D´epartement de Math´ematiques et Informatique, Facult´e des Sciences, Universit´e Chouaib Doukkali, B.P. 20, El Ja- dida, Morocco

E-mail address:[email protected]

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Special Issue on

Intelligent Computational Methods for Financial Engineering

Call for Papers

As a multidisciplinary field, financial engineering is becom- ing increasingly important in today’s economic and financial world, especially in areas such as portfolio management, as- set valuation and prediction, fraud detection, and credit risk management. For example, in a credit risk context, the re- cently approved Basel II guidelines advise financial institu- tions to build comprehensible credit risk models in order to optimize their capital allocation policy. Computational methods are being intensively studied and applied to im- prove the quality of the financial decisions that need to be made. Until now, computational methods and models are central to the analysis of economic and financial decisions.

However, more and more researchers have found that the financial environment is not ruled by mathematical distribu- tions or statistical models. In such situations, some attempts have also been made to develop financial engineering mod- els using intelligent computing approaches. For example, an artificial neural network (ANN) is a nonparametric estima- tion technique which does not make any distributional as- sumptions regarding the underlying asset. Instead, ANN ap- proach develops a model using sets of unknown parameters and lets the optimization routine seek the best fitting pa- rameters to obtain the desired results. The main aim of this special issue is not to merely illustrate the superior perfor- mance of a new intelligent computational method, but also to demonstrate how it can be used effectively in a financial engineering environment to improve and facilitate financial decision making. In this sense, the submissions should es- pecially address how the results of estimated computational models (e.g., ANN, support vector machines, evolutionary algorithm, and fuzzy models) can be used to develop intelli- gent, easy-to-use, and/or comprehensible computational sys- tems (e.g., decision support systems, agent-based system, and web-based systems)

This special issue will include (but not be limited to) the following topics:

Computational methods: artificial intelligence, neu- ral networks, evolutionary algorithms, fuzzy inference, hybrid learning, ensemble learning, cooperative learn- ing, multiagent learning

Application fields: asset valuation and prediction, as- set allocation and portfolio selection, bankruptcy pre- diction, fraud detection, credit risk management

Implementation aspects: decision support systems, expert systems, information systems, intelligent agents, web service, monitoring, deployment, imple- mentation

Authors should follow the Journal of Applied Mathemat- ics and Decision Sciences manuscript format described at the journal site http://www.hindawi.com/journals/jamds/.

Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Track- ing System athttp://mts.hindawi.com/, according to the fol- lowing timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

Lean Yu,Academy of Mathematics and Systems Science, Chinese Academy of Sciences, Beijing 100190, China;

Department of Management Sciences, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kong;

[email protected]

Shouyang Wang,Academy of Mathematics and Systems Science, Chinese Academy of Sciences, Beijing 100190, China; [email protected]

K. K. Lai,Department of Management Sciences, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kong; [email protected]

Hindawi Publishing Corporation http://www.hindawi.com

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