Volume 2011, Issue 1 451492
Research Article
Open Access

Existence and Uniqueness of Generalized Solutions to a Telegraph Equation with an Integral Boundary Condition via Galerkin′s Method

Assia Guezane-Lakoud

Corresponding Author

Assia Guezane-Lakoud

Laboratory of Advanced Materials, Badji Mokhtar University, P.O. Box 12, 23000 Annaba, Algeria univ-annaba.org

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Jaydev Dabas

Jaydev Dabas

Department of Mathematics, Motilal Nehru National Institute of Technology Allahabad, Allahabad 211 004, India mnnit.ac.in

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Dhirendra Bahuguna

Dhirendra Bahuguna

Department of Mathematics and Statistics, Indian Institute of Technology Kanpur, Kanpur 208 016, India iitk.ac.in

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First published: 09 May 2011
Citations: 4
Academic Editor: Christian Corda

Abstract

We consider a telegraph equation with nonlocal boundary conditions, and using the application of Galerkin′s method we established the existence and uniqueness of a generalized solution.

1. Introduction

The initial work devoted to the second-order partial differential equations with nonlocal integral conditions goes back to Cannon [1]. Subsequent investigations include [110] and many other references therein.

Nonlocal problems for some classes of partial differential equations have attracted much interest in the last few years, and several papers have been devoted to this subject. The problem of existence and uniqueness of solutions is of growing interest, as well as methods of obtaining explicit or approximate solutions for this kind of problems. The main reason of such a wide interest in this type of problems is that the non-local conditions occur in various equations of mathematical physics and in mathematical biology.

Nonlocal conditions come up when values of the function on the boundary are connected to values inside the domain. There are various types of non-local integral conditions for hyperbolic, parabolic, or elliptic equations; we point out an important non-local problem (see [11, 12]), studied for a parabolic equation with the following non local conditions.
(1.1)
connected with quasistationary thermoelasticity theory. The non-local boundary conditions of type
(1.2)
arise in modeling the technology of integral circuits, studied in [13].
Problems with nonlocal integral conditions for multidimensional hyperbolic equations have been intensively studied in recent years. However, the nonlocal integral conditions for equations were in the form of second kind as
(1.3)
or  
(1.4)
where Ω is a bounded domain in n  with a smooth boundary, u/η is the inward normal vector to Ω; see [14, 15]. Non-local integral conditions of first kind as
(1.5)
are studied in [15]. Under some assumptions on the kernel K, existence and uniqueness of the generalized solution are established.
The present work deals with the application of the Galerkin method to determine a function u = u(x, t), x ∈ Ω ∈ n is a bounded domain with a smooth boundary Ω, tI = (0, T), which satisfies, in weak sense, the telegraph equation
(1.6)
subject to the initial conditions
(1.7)
and the integral condition
(1.8)
where u/η is the inward normal vector to Ω. This equation arises in the analysis of propagation of electrical signals in a cable transmission line. Both the current and voltage satisfy an equation of this form. This equation arises also in the propagation of pressure waves in the study of pulsate blood flow in arteries.

Cannon et al. [5] have developed and analyzed finite-difference and finite-element Galerkin’s methods for the solution of one-dimensional heat equation with the Neumann and integral conditions. Cannon and van der Hoek [4] presented numerical schemes based on the finite difference method. In [16], the authors have applied the Galerkin method to a parabolic problem with an integral boundary condition and established the existence, uniqueness, and continuous dependence upon the data of a weak solution. In [1721], the authors have used the method of semidiscretization in time and have established the existence and uniqueness of a weak solution. In [22], the authors have discussed some existence uniqueness results for a neutral functional differential equation with a nonlocal initial condition via the Galerkin approximation.

The paper is organized as follows. In Section 2, we specify notations, state some inequalities and make the sense of the desired solution precise. In Section 3, we establish the uniqueness of the solution. Finally, Section 4, is devoted to the construction of the approximate solution and its existence via the Galerkin method.

2. Notation and Definition

Let L2(Q) be the usual space of Lebesgue square integrable real functions on Q whose inner product and norm will be denoted by ( , ) and ∥·∥, respectively.

W1,2(Q) is the Sobolev space consisting of functions such that all derivatives lower than one belong to L2(Q) equipped with the norm
(2.1)

We define the space .

2.1. Some Useful Inequalities: Gronwall Inequalities [23]

Let h(t) and y(t) be two integrable nonnegative functions on the interval I with h(t) nondecreasing. If
(2.2)
where c is a positive constant, then y(t) ≤ h(t)ect, ∀tI.

Cauchy Schwarz inequality:

(2.3)

ɛ-Cauchy inequality:

(2.4)

Trace inequality:

(2.5)
where c(ɛ) is a positive constant that depends only on ɛ and on the domain Ω.

2.2. Definition of Generalized Solution

We define the generalized solution of the problem (1.6)–(1.8) as a weak solution that satisfies for all
(2.6)
Integrating by parts, we get
(2.7)
Regrouping the identities (2.7), then (2.6) becomes
(2.8)

Definition 2.1. By a generalized solution of problem (1.6)(1.8) one means a function uW1,2(Q) such that the identity (2.8) holds for all function .

3. Uniqueness of the Generalized Solution

Now we will show that the generalized solution of problem (1.6)–(1.8), if it exists, is unique.

Theorem 3.1. Assume that φW1,2(Ω), ψL2(Ω),fL2(Q), K(x, y) ∈ C(Ω × Ω), and

(3.1)
then the generalized solution of problem (1.6)–(1.8), if it exists, is unique.

Proof. Suppose that there exist two different generalized solutions u1 and u2 for the problem (1.6)–(1.8); then obviously their difference u = u1u2 is a generalized solution of the problem (1.6)–(1.8) with homogeneous equation and homogeneous initial and non local conditions, that is, f = φ = ψ = 0. We will prove that u = 0 in Q. Let , and denote Qτ = {(x, t); 0 < x < 1,0 < tτT}. Consider the function

(3.2)
The identity (2.8) becomes
(3.3)
Substituting v into (3.3), integrating by parts, and then using the fact that vt(x, t) = −u(x, t), it follows that
(3.4)
Using the assumption on the function K, we get
(3.5)
where C1 = max (2ck1, 2a)/min (c, 1, b). Now, applying Cauchy Schwarz inequality to the first term in the right-hand side of (3.5), then ɛ-Cauchy inequality with ɛ = 1, yields
(3.6)
Using the trace inequality, we obtain
(3.7)
Considering the function
(3.8)
it is easy to see that v(x, t) = w(x, τ) − w(x, t), ∇v(x, 0) = ∇w(x, τ), and (∇v(x,t))2 ≤ 2(∇w(x,τ))2 + 2(∇w(x,t))2. Consequently, substituting w in (3.7), we get
(3.9)
Seting
(3.10)
it follows that
(3.11)
Since τ is arbitrary chosen, let 1 − τC2 > 0; then (3.11) becomes
(3.12)
Applying Gronwall Lemma, we get
(3.13)
Consequently, we obtain u(x, τ) = 0, for all x ∈ Ω and τ  ]0, 1/C2[.

If T ≤ 1/C2, then u = 0 in Q. In the case where T ≥ 1/C3, we see that , where n0 = [C2T] + 1,[C2T] is the entire part of C2T; then repeating the preceding reasoning for τ  ](n − 1)/C2, n/C2[, we get u(x, τ) = 0, for all τ  ](n − 1)/C2,   n/C2[, and then u(x, t) = 0 in Q. Thus, the uniqueness is proved.

Remark 3.2. It should be noted that we can prove the uniqueness theorem by using a priori estimates, so we establish that the generalized solution, if it exists, satisfies the inequality

(3.14)

4. Existence of Generalized Solution

Theorem 4.1. Assume that the assumptions of Theorem 4.1 hold; then the non-local problem (1.6)–(1.8) has a unique solution uW1,2(Q).

Proof. In order to prove the existence of the generalized solution we apply Galerkin’s method. Let {wk(x)} be a fundamental system in W1,2(Ω), such that . Now we will try to find an approximate solution of the problem (1.6)–(1.8) in the form

(4.1)
The approximates of the functions φ(x) and ψ(x) are denoted, respectively, by
(4.2)
Substituting the approximation solution in (1.6), multiplying both sides by wi(x), and then integrating according to x on Ω, we get
(4.3)
Substituting (4.1) in (4.3), we obtain
(4.4)
This implies that
(4.5)
Denote
(4.6)
Then (4.5) becomes
(4.7)
We obtain a system of differential equations of second order according to the variable t with smooth coefficients and the initial conditions
(4.8)
Consequently, we get a Cauchy problem of linear differential equations with smooth coefficients that is uniquely solvable. So it has a unique solution u(n) satisfying (4.3).

Lemma 4.2. The sequence (u(n)) is bounded.

Proof. Multiplying (4.4) by and summing over i from 1 to n, we get

(4.9)
Integrating by parts the left-hand side of (4.9) over t on (0, τ) yields
(4.10)
Substituting the four last identities into (4.9), we get
(4.11)
Applying Cauchy Schwarz inequality, ϵ-Cauchy inequality, the hypothesis on the operator K, and the fact that to the second term in the right hand side of (4.11), we get
(4.12)
We may obtain similar inequalities for the third and the fourth terms in the right-hand side of (4.11). Now if we apply Cauchy Schwarz inequality to the last term in (4.11) we get
(4.13)
Using the result inequalities in (4.11) and then regrouping the same terms yield
(4.14)
Choose ϵ such that (1 − ɛ) > 0 and and let
(4.15)
then (4.14) becomes
(4.16)
Now, we apply Gronwall Lemma to get
(4.17)
Since φ(n) and ψ(n) are the orthogonal projections of φ and ψ, respectively, from the Pythagorean relation we have that and . Integrating (4.17) according to τ on [0, T] yields
(4.18)
Consequently, the sequence {u(n)} is bounded.

Remark 4.3. We have proved that the sequence {u(n)} is bounded, so we can extract a subsequence which we denote by that is weakly convergent; then we prove that its limit is the desired solution of the problem (1.6)–(1.8).

Lemma 4.4. The limit of the subsequence is the solution of the problem (1.6)–(1.8).

Proof. For this we prove that the limit of the subsequence satisfies the identity (2.8) for all functions . Since the set Sn is such that is dense in , it suffices to prove (2.8) for vSn. Multiplying (4.3) by the function vi(t) ∈ W1,2(0, T),  vi(T) = 0, and then taking the sum from i = 0 to n, we obtain

(4.19)
Integrating by parts on [0, T], we get
(4.20)
Denote the weak limit of the subsequence by u. When k tends to infinity, we get
(4.21)
Indeed, using Cauchy Schwarz inequality then ɛ-Cauchy inequality, we obtain
(4.22)
and then by passing to the limit in (4.20) we get that the limit u satisfies(2.8).

Example 4.5. Now we present an example to demonstrate the applications of the results established in the earlier sections. We consider the following:

(4.23)
with the initial conditions
(4.24)
and the nonlocal boundary condition
(4.25)

The results of the earlier sections guarantee the existence and uniqueness of a solution. It may be noted that u(x, t) = sinxsint is the unique solution of (4.23)–(4.25).

Acknowledgment

The authors thank the referees for their helpful suggestions and corrections to improve the paper.

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