Existence and Uniqueness of Generalized Solutions to a Telegraph Equation with an Integral Boundary Condition via Galerkin′s Method
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 [1–10] 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.
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 [17–21], 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.
We define the space .
2.1. Some Useful Inequalities: Gronwall Inequalities [23]
Cauchy Schwarz inequality:
ɛ-Cauchy inequality:
Trace inequality:
2.2. Definition of Generalized Solution
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 φ ∈ W1,2(Ω), ψ ∈ L2(Ω),f ∈ L2(Q), K(x, y) ∈ C(Ω × Ω), and
Proof. Suppose that there exist two different generalized solutions u1 and u2 for the problem (1.6)–(1.8); then obviously their difference u = u1 − u2 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 < t ≤ τ ≤ T}. Consider the function
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
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 u ∈ W1,2(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
Lemma 4.2. The sequence (u(n)) is bounded.
Proof. Multiplying (4.4) by and summing over i from 1 to n, we get
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).
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 v ∈ Sn. 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
Example 4.5. Now we present an example to demonstrate the applications of the results established in the earlier sections. We consider the following:
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.