Volume 2013, Issue 1 606454
Research Article
Open Access

On a New Class of Antiperiodic Fractional Boundary Value Problems

Bashir Ahmad

Bashir Ahmad

Department of Mathematics, Faculty of Science, King Abdulaziz University, P.O. Box 80203, Jeddah 21589, Saudi Arabia kau.edu.sa

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Juan J. Nieto

Corresponding Author

Juan J. Nieto

Department of Mathematics, Faculty of Science, King Abdulaziz University, P.O. Box 80203, Jeddah 21589, Saudi Arabia kau.edu.sa

Departamento de Análisis Matemático, Facultad de Matemáticas, Universidad de Santiago de Compostela, 15782 Santiago de Compostela, Spain usc.es

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Ahmed Alsaedi

Ahmed Alsaedi

Department of Mathematics, Faculty of Science, King Abdulaziz University, P.O. Box 80203, Jeddah 21589, Saudi Arabia kau.edu.sa

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Nadia Mohamad

Nadia Mohamad

Department of Mathematics, Faculty of Science, King Abdulaziz University, P.O. Box 80203, Jeddah 21589, Saudi Arabia kau.edu.sa

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First published: 18 March 2013
Citations: 2
Academic Editor: Ağacık Zafer

Abstract

This paper investigates a new class of antiperiodic boundary value problems of higher order fractional differential equations. Some existence and uniqueness results are obtained by applying some standard fixed point principles. Some examples are given to illustrate the results.

1. Introduction

Boundary value problems of fractional differential equations involving a variety of boundary conditions have recently been investigated by several researchers. It has been mainly due to the occurrence of fractional differential equations in a number of disciplines such as physics, chemistry, biology, economics, control theory, signal and image processing, biophysics, blood flow phenomena, aerodynamics, andfitting of experimental data. For details and examples, see [15]. The recent development of the subject can be found, for example, in papers [616].

The mathematical modeling of a variety of physical processes gives rise to a class of antiperiodic boundary value problems. This class of problems has recently received considerable attention; for instance, see [1724] and the references therein. In [22], the authors studied a Caputo-type antiperiodic fractional boundary value problem of the form
()
In this paper, we investigate a new class of antiperiodic fractional boundary value problems given by
()
where  cDq denotes the Caputo fractional derivative of order q and f is a given continuous function. Some new existence and uniqueness results are obtained for problem (2) by using standard fixed point theorems.

2. Preliminaries

Let us recall some basic definitions [13].

Definition 1. The Riemann-Liouville fractional integral of order q for a continuous function g : [0, +) → is defined as

()
provided the integral exists.

Definition 2. For (n − 1) times absolutely continuous function g : [0, +) → , the Caputo derivative of fractional order q is defined as

()
where [q] denotes the integer part of the real number q.

Notice that the Caputo derivative of a constant is zero.

Lemma 3. For any yC[0,1], the unique solution of the linear fractional boundary value problem

()
is
()
where GT(t, s) is Green’s function (depending on q and p) given by
()

Proof. We know that the general solution of equation  cDqx(t) = y(t), 2 < q ≤ 3 can be written as [3]

()
for some constants b0, b1, and b2. Using the facts   cDpb = 0 (b is a constant),
()
we get
()
Applying the boundary conditions for the problem (5), we find that
()
Substituting the values of b0, b1, and b2 in (8), we get the solution (6). This completes the proof.

Remark 4. For p = 1, the solution of the antiperiodic problem

()
is given by [18]
()
where g(t, s) is
()

If we let p → 1 in (7), we obtain

()
We note that the solutions given by (14) and (15) are different. As a matter of fact, (15) contains an additional term: (−t2T2 + 3tT)(Ts) q−3/4Γ(q − 2). Therefore the fractional boundary conditions introduced in (2) give rise to a new class of problems.

Remark 5. When the phenomenon of antiperiodicity occurs at an intermediate point η ∈ (0, T), the parametric-type antiperiodic fractional boundary value problem takes the form

()
whose solution is
()
where Gη(t, s) is given by (7). Notice that Gη(t, s) → GT(t, s) when ηT.

3. Existence Results

Let = C([0, T], R) denotes a Banach space of all continuous functions defined on [0, T] into R endowed with the usual supremum norm.

In relation to (2), we define an operator : as
()

Observe that the problem (2) has a solution if and only if the operator has a fixed point.

For the sequel, we need the following known fixed point theorems.

Theorem 6 (see [25].)Let X be a Banach space. Assume that T : XX is a completely continuous operator and the set V = {uXu = μTu, 0 < μ < 1} is bounded. Then T has a fixed point in X.

Theorem 7 (see [25].)Let X be a Banach space. Assume that Ω is an open bounded subset of X with θ ∈ Ω and let be a completely continuous operator such that

()
Then T has a fixed point in .

Now we are in a position to present the main results of the paper.

Theorem 8. Assume that there exists a positive constant L1 such that |f(t, x(t))| ≤ L1 for t ∈ [0, T], x. Then the problem (2) has at least one solution.

Proof. First, we show that the operator is completely continuous. Clearly continuity of the operator follows from the continuity of f. Let Ω ⊂ be bounded. Then, for all x ∈ Ω together with the assumption |f(t, x(t))| ≤ L1, we get

()
which implies that ∥(x)(t)∥≤M1.

Furthermore,

()
Hence, for t1, t2 ∈ [0, T], we have
()

This implies that is equicontinuous on [0, T], by the Arzela-Ascoli theorem, the operator : is completely continuous.

Next, we consider the set

()
and show that the set V is bounded. Let xV, then x = μx, 0 < μ < 1. For any t ∈ [0, T], we have
()
Thus, ∥x∥≤M3 for any t ∈ [0, T]. So, the set V is bounded. Thus, by the conclusion of Theorem 6, the operator has at least one fixed point, which implies that (2) has at least one solution.

Theorem 9. Let there exists a positive constant r such that |f(t, x)| ≤ δ | x| with 0<|x | < r, where δ is a positive constant satisfying

()
Then the problem (2) has at least one solution.

Proof. Define Ω1 = {x : ∥x∥<r} and take x such that ∥x∥ = r; that is, xΩ. As before, it can be shown that is completely continuous and that

()
for xΩ, where we have used (25). Therefore, by Theorem 7, the operator has at least one fixed point which in turn implies that the problem (2) has at least one solution.

Theorem 10. Assume that f : [0, T] × is a continuous function satisfying the condition

()
with Lκ < 1, where
()
Then the problem (2) has a unique solution.

Proof. Let us fix sup t∈[0,T] | f(t, 0)| = M < and select

()
where κ is given by (28). Then we show that BrBr, where Br = {x : ∥x∥≤r}. For xBr, we have
()
Thus we get xBr. Now, for x, y and for each t ∈ [0, T], we obtain
()
which, in view of the condition κL < 1 (κ is given by (28)), implies that the operator is a contraction. Hence, by Banach′s contraction mapping principle, the problem (2) has a unique solution.

Example 11. Consider the following antiperiodic fractional boundary value problem:

()

Clearly |f(t, x(t))|≤(3ln 7). So, the hypothesis of Theorem 8 holds. Therefore, the conclusion of Theorem 8 applies to antiperiodic fractional boundary value problem (32).

Example 12. Consider the following antiperiodic fractional boundary value problem:

()
where q = 5/2, p = 3/4, , and T = 2. Clearly,
()
where we have used the fact that . Further,
()
With L < 1/κ, all the assumptions of Theorem 10 are satisfied. Hence, the fractional boundary value problem (33) has a unique solution on [0,2].

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