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BY 4.0 license Open Access Published by De Gruyter Open Access May 30, 2019

An investigation of fractional Bagley-Torvik equation

  • Hossein Fazli EMAIL logo and Juan J. Nieto
From the journal Open Mathematics

Abstract

In this paper the authors prove the existence as well as approximations of the solutions for the Bagley-Torvik equation admitting only the existence of a lower (coupled lower and upper) solution. Our results rely on an appropriate fixed point theorem in partially ordered normed linear spaces. Illustrative examples are included to demonstrate the validity and applicability of our technique.

MSC 2010: 26A33; 34A08; 34A12

1 Introduction

Fractional differential equations appear naturally in a number of fields such as physics, geophysics, polymer rheology, regular variation in thermodynamics, biophysics, blood flow phenomena, aerodynamics, electro-dynamics of complex medium, viscoelasticity, Bode’s analysis of feedback amplifiers, capacitor theory, electrical circuits, electron-analytical chemistry, biology, control theory, fitting of experimental data, nonlinear oscillation of earthquake, the fluid-dynamic traffic model, etc. For more details and applications, we refer the reader to the books [1, 2, 3, 4, 5, 6] and references [7, 8, 9, 10, 11, 12, 13, 14].

Fractional differential equations also serve as an excellent tool for the description of hereditary properties of various materials and processes [15, 16]. The presence of memory term in such models not only takes into account the history of the process involved but also carries its impact to present and future development of the process. Fractional differential equations are also regarded as an alternative model to nonlinear differential equations [17]. In consequence, the subject of fractional differential equations is gaining much importance and attention.

The Bagley-Torvik equation is a prototype fractional differential equation which was proposed by Bagley and Torvik as an application of fractional calculus to the theory of viscoelasticity [18, 19, 20]. The governing equation is given by the fractional differential equation

MD2+2SμρD3/2+Kx(t)=f(t),0<t1, (1.1)

subject to initial conditions

x(0)=x0,x(0)=x0, (1.2)

where x(t) represents the displacement of the plate of mass M and surface area S. Furthermore, μ and ρ are the viscosity and density, respectively, of the fluid in which the plate is immersed, and K is the stiffness of the spring to which the plate is attached. Finally, f(x) represents the loading force.

In the current paper we investigate the existence and uniqueness as well as approximations of the solutions for the Bagley-Torvik equation admitting only the existence of a lower (coupled lower and upper) solution. Our governing equation is a generalization of (1.1) to an arbitrary α with 1 < α < 2 in the fractional derivative term. In fact, we consider the following initial value equation

D2+ADα+Bx(t)=f(t),0<t1,1<α<2, (1.3)

subject to initial conditions

x(0)=a,x(0)=b, (1.4)

where Dα is the Caputo fractional derivative of order α, f : [0, 1] → ℝ is a given function and a, b, A and B are real numbers.

For various applications in engineering and applied sciences fields, the Bagley-Torvik equation is extensively studied in literature both from numerical and theoretical point of view [3, 21, 22, 23, 24, 25, 26, 27, 28, 29, 30]. Several numerical methods have been proposed for approximate solutions of this type equations, such as successive approximation method [3, Section 8.3], Adams predictor and corrector method [21], Taylor collocation method [22], hybridizable discontinuous Galerkin method [23], Discrete spline method [24] and others [25, 26, 27, 28]. Also, Svatoslav Staněk [29] investigate the existence and uniqueness of solutions for generalized Bagley-Torvik fractional differential equation subject to the boundary conditions. In [30], the authors investigate the general solution of the Bagley-Torvik equation with 1/2-order derivative or 3/2-order derivative. Furthermore, they show that the general solution of the Bagley-Torvik equation involves actually two free constants only, and it can be determined fully by the initial displacement and initial velocity.

Our main aim is to prove the existence and uniqueness as well as construct an approximate solution for (1.3)-(1.4). This is done in Section 3. Our main tools are some applicable partially fixed point theorems which are applied in the suitable partially ordered sets as well as iterative methods, whose description can be found in [31, 32, 33, 34, 35]. The advantage and importance of this method arises from the fact that it is a constructive method that yields sequences that converge to the unique solution of (1.3)-(1.4) admitting only the existence of a lower (coupled lower and upper) solution.

2 Auxiliary facts and results

Here, we recall several known definitions and properties from fractional calculus theory. For details, see [1, 2, 3, 36]. Throughout the paper ACn [0, 1], n ∈ ℕ, denotes the set of functions having absolutely continuous n-th derivative on [0, 1], and AC[0, 1] is the set of absolutely continuous functions on [0, 1]. It is known that xAC[0, 1] if and only if there exists a function φL1[0, 1] such that x(t) = c + 0t φ(τ) dτ.

Definition 2.1

The Riemann-Liouville fractional integral of order α > 0 of a function x : [0, 1] → ℝ is defined as

Iαx(t)=1Γ(α)0t(tτ)α1x(τ)dτ,0t1.

provided that the integral exists. For α = 0, we set Iα := I, the identity operator.

Definition 2.2

The Caputo fractional derivative of order α > 0 of a function x : [0, 1] → ℝ is defined as

Dαx(t)=1Γ(nα)dndtn0t(tτ)nα1x(τ)k=0n1x(k)(0)k!τkdτ=DnInαx(t)k=0n1x(k)(0)k!tk,

where n − 1 < α < n and n ∈ℕ, provided the right side is pointwise defined on [0, 1]. We notice that the Caputo derivative of a constant is zero. Note that if n − 1 < α < n and xACn−1[0, 1], then

Dαx(t)=1Γ(nα)0t(tτ)nα1x(n)(τ)dτ=Inαx(n)(t).

Lemma 2.1

Let α, β ≥ 0. If xL1[0, 1], then Iα Iβ x = Iα+βx.

Lemma 2.2

For 0 < α < 1, Iα is linear and continuous from L1 [0, 1] to Lp [0, 1] where 1p<11α.

Lemma 2.3

For α > 0, Iα is linear and continuous from AC [0, 1] to AC[0, 1].

Lemma 2.4

Let α ≥ 1. If xL1[0, 1], then Iα xAC[0, 1].

Proof

This is an immediate consequence of Lemma 2.1 and Lemma 2.2, because Iα x = IαIα − ⌊αx where ⌊ α ⌋ = max{n ∈ ℕ, nα}. □

Lemma 2.5

Let α > 0, a ∈ ℝ and xL1[0, 1]. If there exists fAC[0, 1] such that x(t) − a Iα x(t) = f(t) on [0, 1], then xAC[0, 1].

Proof

If a = 0 we are done, and so we henceforth assume a ≠ 0. Given α > 0, choose n0 ∈ ℕ so that n0α > 1. Now, by applying the operator Iα to both sides of x(t) = a Iα x(t)+f(t), we have

Iαx(t)=aI2αx(t)+Iαf(t),

or equivalently,

x(t)=a2I2αx(t)+aIαf(t)+f(t).

Continuing this process to the n0-th step, we get

x(t)=a(n0+1)I(n0+1)αx(t)+k=0n0akIkαf(t),

for t ∈ [0, 1]. The desired result is therefore a consequence of Lemma 2.4. □

Definition 2.3

A function xAC1[0, 1] is a solution of (1.3)-(1.4) if it satisfies the initial conditions (1.4) and (1.3) holds for almost everywhere on [0, 1].

Lemma 2.6

x(t) is a solution of the problem (1.3)-(1.4) if and only if it is a solution of the following integral equation

x(t)=a+bt+AΓ(4α)t3αAI3αx(t)+I2f(t)Bx(t), (2.1)

in the set C1[0, 1].

Proof

Let us note that this result is mainly proved in [29]. Let x(t) be a solution of the problem (1.3)-(1.4). Then xAC1[0, 1] and the equality

x(t)+AI2αx(t)+Bx(t)=f(t), (2.2)

holds almost everywhere on [0, 1]. Applying the integral operator I2 to both sides of (2.2) and using Lemma 2.1, we deduce

x(t)=a+btAI4αx(t)+I2f(t)Bx(t)=a+btAI3αI1x(t)+I2f(t)Bx(t)=a+btAI3αx(t)b+I2f(t)Bx(t)=a+bt+AbΓ(4α)t3αAI3αx(t)+I2f(t)Bx(t)=a+bt+AΓ(4α)t3αAI3αx(t)+I2f(t)Bx(t). (2.3)

Note that Iαtβ=Γ(β+1)Γ(α+β+1)tα+β, α ≥ 0, β > −1. Therefore, xC1[0, 1] is a solution of the integral equation (2.1). Now, we suppose that xC1[0, 1] is a solution of the integral equation (2.1). It is obvious that x(0) = a and x’(0) = b. By calculations similar to those in (2.3), we establish that

x(t)=a+bt+AΓ(4α)t3αAI3αx(t)+I2f(t)Bx(t)=a+btAI3α[x(t)b]+I2f(t)Bx(t)=a+btAI2α[x(t)abt]+I2f(t)Bx(t)=a+btAI2α[x(t)x(0)x(0)t]+I2f(t)Bx(t). (2.4)

Differentiating twice, we get

x(t)=AD2I2α[x(t)x(0)x(0)t]+f(t)Bx(t), (2.5)

and so

x(t)+ADαx(t)+Bx(t)=f(t). (2.6)

Now it suffices to show that xAC1[0, 1]. By differentiating both sides of (2.1), we have

x(t)+AI2αx(t)=b1+AΓ(3α)t2α+I1f(t)Bx(t). (2.7)

Since b1+AΓ(3α)t2α +I1[f(t) − Bx(t)] ∈ AC[0, 1], the desired result is therefore a consequence of Lemma 2.5. □

3 Main results

Before continuing our investigation, we introduce a few fundamental concepts related to the required spaces and provide some partial order on them to serve as a background for the materials to be illustrated in the later sections.

By C1 [0, 1] we denote the class of contiuously differentiable functions on a finite interval [0, 1] with the standard norm ∥xC1[0, 1] = max{∥xC[0, 1], ∥x′ ∥C[0, 1]} where ∥xC[0, 1] = supt ∈ [0, 1]| x (t)|. Obviously, C1 [0, 1] is a Banach space. Now, we define an appropriate partial order on C1[0, 1] and prove some essential properties in this partially ordered Banach space.

Definition 3.1

We define the following order relation for C1 [0, 1],

xyx(t)y(t),x(t)y(t),t[0,1].

Lemma 3.1

(C1 [0, 1], ⪯) is a partially ordered set and every pair of elements has a lower bound and an upper bound.

Proof

It is easy to see that (C1 [0, 1], ⪯) is a partially ordered set. Now we prove that every pair of elements in C1 [0, 1] has a lower bound and an upper bound. Let x, yC1 [0, 1] and define

x_(t)=0tmin{x(),y()}(τ)dτ+min{x(0),y(0)},

and

x¯(t)=0tmax{x(),y()}(τ)dτ+max{x(0),y(0)}.

So a simple calculation shows that the functions x and x are in C1 [0, 1] and are the lower and upper bounds of {x, y}, respectively. □

Dividing by A, B (distinguish the cases AB > 0 and AB < 0), we will consider two cases separately.

3.1 Investigation in the case AB < 0

In this subsection we consider the case in which AB < 0. We consider only the case that A > 0 and B < 0. The other case is completely similar. Before continuing, we need to introduce the coupled fixed point theorems which play main role in our discussion. For complete details, see [34].

Definition 3.2

Let (X, ⪯) be a partially ordered set and 𝓖 : X × XX. We say that 𝓖 has the mixed monotone property if 𝓖(x, y) is monotone non-decreasing in x and is monotone non-increasing in y.

Definition 3.3

We call an element (x, y) ∈ X × X a coupled fixed point of the mapping 𝓖 if

G(x,y)=x,andG(y,x)=y.

Theorem 3.1

Let (X, ⪯) be a partially ordered set and suppose there exists a metric d on X such that (X, d) is a complete metric space. Let 𝓖 : X × XX be a mapping having the mixed monotone property on X. Assume that there exists a k ∈ [0, 1) with

d(G(x,y),G(u,v))k2[d(x,u)+d(y,v)],foreachxuandyv.

Suppose either 𝓖 is continuous or X has the following property:

  1. if a non-decreasing sequence {xn} → x, then xnx for all n,

  2. if a non-increasing sequence {yn} → y, then yyn for all n.

    If there exist x0, y0X such that x0 ⪯ 𝓖 (x0, y0) and y0 ⪰ 𝓖 (y0, x0), then 𝓖 has a coupled fixed point (x*, y*) ∈ X × X.

We define the following partial order on the product space X × X:

(x,y),(x~,y~)X×X,(x,y)(x~,y~)xx~,y~y.

Theorem 3.2

In addition to the hypothesis of Theorem 3.1, suppose that for every (x, y), (, ) ∈ X × X, there exists an element (u, v) ∈ X × X that is comparable to (x, y) and (, ), then 𝓖 has a unique coupled fixed point (x*, y*).

Theorem 3.3

In addition to the hypothesis of Theorem 3.2, suppose that every pair of elements of X has an upper bound or a lower bound in X. Then x* = y*. Moreover,

limnGn(x0,y0)=x,

where 𝓖n (x0, y0) = 𝓖(𝓖n−1 (x0, y0), 𝓖n−1 (y0, x0)).

In view of Lemma 2.6, we transform problem (1.3)-(1.4) as the following integral equation

x(t)=a+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αx(τ)dτ+0t(tτ)f(τ)Bx(τ)dτ, (3.1)

in the set C1[0, 1].

Definition 3.4

An element (x0, y0) ∈ C1[0, 1] × C1[0, 1] is called a coupled lower and upper solution of problem (1.3)-(1.4) if

x0(t)b1+AΓ(3α)t2αAΓ(2α)0t(tτ)1αy0(τ)dτ+0tf(τ)+|B|x0(τ)dτ,x0(0)a, (3.2)

and

y0(t)b1+AΓ(3α)t2αAΓ(2α)0t(tτ)1αx0(τ)dτ+0tf(τ)+|B|y0(τ)dτ,y0(0)a, (3.3)

for all t ∈ [0, 1].

Theorem 3.4

Assume that (x0, y0) ∈ C1[0, 1] × C1[0, 1] is a coupled lower and upper solution of problem (1.3)-(1.4) and k=max{2|B|,2AΓ(3α)}<1.

  1. Then the initial value problem (1.3)-(1.4) has a unique solution x*C1[0, 1].

  2. Moreover, there exist two monotone iterative sequences {xn} and {yn} such that both sequences converge to x* in C1[0, 1].

  3. In addition, the following error estimates hold,

    xnxC1[0,1]12kn1kx1x0C1[0,1]+y1y0C1[0,1], (3.4)

    ynxC1[0,1]12kn1kx1x0C1[0,1]+y1y0C1[0,1], (3.5)

    xnynC1[0,1]kn1kx1x0C1[0,1]+y1y0C1[0,1]. (3.6)

Proof

In view of (3.1), we define the operator 𝓖 : C1 [0, 1] × C1 [0, 1] → C1 [0, 1] by

G(x,y)(t)=a+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αy(τ)dτ+0t(tτ)f(τ)+|B|x(τ)dτ. (3.7)

Obviously, for any x, yC1 [0, 1], we have 𝓖(x, y) ∈ C[0, 1]. On the other hand,

G(x,y)(t)=b1+AΓ(3α)t2αAΓ(2α)0t(tτ)1αy(τ)dτ+0t(f(τ)+|B|x(τ))dτ,

and so the operator 𝓖 is well defined.

Now we shall show that 𝓖 has the mixed monotone property. Let x, xC1 [0, 1] with xx. Using the monotonicity of integral operator, we have

G(x,y)(t)G(x¯,y)(t)=|B|0t(tτ)x(τ)x¯(τ)dτ0,

and

G(x,y)(t)G(x¯,y)(t)=|B|0tx(τ)x¯(τ)dτ0,

for every t ∈ [0, 1]. Hence, 𝓖(x, y)(t) ≤ 𝓖(x, y) (t) and 𝓖′(x, y)(t) ≤ 𝓖′(x, y) (t) for every t ∈ [0, 1], that is, 𝓖(x, y) ⪯ 𝓖(x, y). Similarly, let y, yC1 [0, 1] with yy. From the monotonicity of Riemann-Liouville fractional integral operator, we have

G(x,y)(t)G(x,y¯)(t)=AΓ(3α)0t(tτ)2αy(τ)y¯(τ)dτ0.

and

G(x,y)(t)G(x,y¯)(t)=AΓ(2α)0t(tτ)1αy(τ)y¯(τ)dτ0.

for every t ∈ [0, 1]. Hence, 𝓖(x, y)(t) ≥ 𝓖(x, y) (t) and 𝓖′(x, y)(t) ≥ 𝓖′(x, y) (t) for every t ∈ [0, 1], that is, 𝓖(x, y) ⪰ 𝓖(x, y). Thus, 𝓖 (x, y) is monotone non-decreasing in x and monotone non-increasing in y.

Now, for x, y, x, yC1[0, 1] with xx, yy, we have

|G(x,y)(t)G(x¯,y¯)(t)|=||B|0t(tτ)x(τ)x¯(τ)dτAΓ(3α)0t(tτ)2αy(τ)y¯(τ)dτ||B|2supt[0,1]|x(t)x¯(t)|+AΓ(4α)supt[0,1]|y(t)y¯(t)|,|B|2xx¯C1[0,1]+AΓ(4α)yy¯C1[0,1],

and

|G(x,y)(t)G(x¯,y¯)(t)|=||B|0tx(τ)x¯(τ)dτAΓ(2α)0t(tτ)1αy(τ)y¯(τ)dτ||B|supt[0,1]|x(t)x¯(t)|+AΓ(3α)supt[0,1]|y(t)y¯(t)|.|B|xx¯C1[0,1]+AΓ(3α)yy¯C1[0,1].

Therefore,

G(x,y)G(x¯,y¯)C1[0,1]|B|xx¯C1[0,1]+AΓ(3α)yy¯C1[0,1].k2[xx¯C1[0,1]+yy¯C1[0,1]]. (3.8)

Furthermore, it is easy to see that, if {xn} is a monotone non-decreasing sequence in C1 [0, 1] that converges to xC1 [0, 1] and {yn} is a monotone non-increasing sequence in C1 [0, 1] that converges to yC1 [0, 1], then xnx and yyn, for all n.

On the other hand, from (3.2), we have

x0(t)b1+AΓ(3α)t2αAΓ(2α)0t(tτ)1αy0(τ)dτ+0tf(τ)+|B|x(τ)dτ=ddta+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αy0(τ)dτ+0t(tτ)f(τ)+|B|x0(τ)dτ=G(x0,y0)(t), (3.9)

for every t ∈ [0, 1]. Now by applying the integral operator I1 on both sides of inequality (3.9) and using x(0) ≤ a, we deduce

x0(t)x0(0)+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αy0(τ)dτ+0t(tτ)f(τ)+|B|x0(τ)dτa+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αy0(τ)dτ+0t(tτ)f(τ)+|B|x0(τ)dτ=G(x0,y0)(t),

for every t ∈ [0, 1]. Furthermore, using (3.3) and applying similar calculation, we get y0 (t) ≥ 𝓖′(y0, x0)(t) and y0 (t) ≥ 𝓖(y0, x0)(t) for every t ∈ [0, 1]. Therefore,

x0G(x0,y0)andy0G(y0,x0). (3.10)

Consequently, Theorem 3.1 yields the existence of coupled fixed point (x*, y*) ∈ C1 [0, 1] × C1 [0, 1] for the oparator 𝓖.

Also, C1 [0, 1] × C1 [0, 1] is a partially ordered set if we define the following order relation in C1 [0, 1] × C1 [0, 1] :

(x,y)(x¯,y¯)xx¯,y¯y.

Now, if for every (x, y), (x, y) ∈ C1 [0, 1] × C1 [0, 1], we define

x~(t)=0tmax{x(),x¯()}(τ)dτ+max{x(0),x¯(0)},

and

y~(t)=0tmin{y(),y¯()}(τ)dτ+min{y(0),y¯(0)}.

then (, ) ∈ C1 [0, 1] × C1 [0, 1] is comparable to (x, y) and (x, y). The uniqueness of the coupled fixed point (x*, y*) therefore follows from Theorem 3.2. Finally, an application of Theorem 3.3, together with Lemma 3.1, yields x* = y* . This establishes the first assertion.

For the second assertion, we define iterative sequences {xn} and {yn} as follows

xn=G(xn1,yn1),yn=G(yn1,xn1),n=1,2,, (3.11)

where x0 and y0 are the coupled lower and upper solutions of problem (1.3)-(1.4). We intend to prove by induction on n that {xn} and {yn} are non-decreasing and non-increasing sequences, respectively. The case n = 1 being immediate from (3.10). Now we take an arbitrary positive integer n and we assume that xn−1xn and ynyn−1. Then, using the mixed monotone property of 𝓖, we have

xn=G(xn1,yn1)G(xn,yn1)G(xn,yn)=xn+1,

and

yn+1=G(yn,xn)G(yn,xn1)G(yn1,xn1)=yn.

Moreover, both sequences {xn} and {yn} converge to x* which follow from Theorem 3.3. This proves assertion (ii).

Now we prove the error estimates. From (3.8) it follows that

x2x1C1[0,1]k2x1x0C1[0,1]+y1y0C1[0,1], (3.12)

y2y1C1[0,1]k2x1x0C1[0,1]+y1y0C1[0,1]. (3.13)

Again employing (3.8) and using (3.12) and (3.13), we deduce

x3x2C1[0,1]k22x1x0C1[0,1]+y1y0C1[0,1],y3y2C1[0,1]k22x1x0C1[0,1]+y1y0C1[0,1].

By a mathematical induction, we obtain

xn+1xnC1[0,1]kn2x1x0C1[0,1]+y1y0C1[0,1], (3.14)

yn+1ynC1[0,1]kn2x1x0C1[0,1]+y1y0C1[0,1]. (3.15)

Then for any mn ≥ 1,

xmxnC1[0,1]j=0mn1xn+j+1xn+jC1[0,1]j=0mn1kn+j2x1x0C1[0,1]+y1y0C1[0,1]=12knkm1kx1x0C1[0,1]+y1y0C1[0,1]. (3.16)

Letting m → ∞ in both sides of (3.16), we can obtain the error estimate (3.4). A similar argument can also be used to prove error estimate (3.5). Finally, (3.6) follows immediately from (3.4) and (3.5). □

Remark 3.1

In view of Theorem 3.4, the sequences defined by (3.11) generate a sequence {(xn, yn)} which each of its elements is a coupled lower and upper solution of problem (1.3)-(1.4).

Remark 3.2

Let (x0, y0) be a coupled lower and upper solution of problem (1.3)-(1.4) such that x0y0 and let {xn} and {yn} be the sequences defined by (3.11) such thatxnx*C1[0, 1] → 0 andynx*C1[0, 1] → 0. Then

x0x1xnxyny1y0. (3.17)

Example 3.1

Let us consider the following problem

x(t)+25D32x(t)14x(t)=f(t),0<t<1,x(0)=0,x(0)=1, (3.18)

where f(t)=14t214t85tπ2 and the exact solution is x(t) = t(1 − t). Observe that, we have k = max{2|B|,2AΓ(3α)}=0.90267<1. Now, define 𝓖 : C1[0, 1] × C1[0, 1] → C1[0, 1] by setting

G(x,y)(t)=t+25Γ(4α)t3α25Γ(3α)0t(tτ)2αy(τ)dτ+0t(tτ)14τ214τ85τπ2+14x(τ)dτ. (3.19)

A relatively simple calculation, with the help of Maple, shows that (x0(t), y0(t)) = (−3t, 3t) is a coupled lower and upper solution of problem (3.18). Therefore, all the assumptions of Theorem 3.4 hold and consequently, problem (3.18) has a unique solution in C1[0, 1]. Moreover, the unique solution of (3.18) can be obtained as limn → ∞𝓖n (x0, y0) where 𝓖n (x0, y0) = 𝓖(𝓖n−1 (x0, y0), 𝓖n − 1(y0, x0)). For simplicity, we set xn = 𝓖 (xn−1, yn−1) and and yn = 𝓖 (yn−1, xn−1). Using simple calculation, with the help of Maple, we can now form the first few successive approximations as follows

x1=G(x0,y0)=t1615t32π0.24072t52+0.02083t40.16667t3t2,y1=G(y0,x0)=t+3215t32π0.24072t52+0.02083t4+0.08333t3t2.

Therefore, we have

x2=G2(x0,y0)=Gx1,y1=t0.00001t520.03438t720.00764t92+0.00017t60.00208t5+0.05333t31.32t2

and

y2=G2(y0,x0)=G(y1,x1)=t+0.00001t52+0.06877t720.00764t92+0.00017t6+0.00104t5+0.05333t30.83996t2.

Similarly,

x3=G3(x0,y0)=Gx2,y2=t0.03851t520.011t720.00052t1120.00008t1320.00001t7+0.002t50.02t4t2,

and

y3=G3(y0,x0)=G(y2,x2)=t+0.07703t520.011t720.00104t1120.00008t132+0.002t5+0.01t4t2.

It is interesting to point out that (xn, yn) = (𝓖n (x0, y0), 𝓖n(y0, x0)), n = 1, 2, 3 serve as an approximation to the unique coupled fixed point of 𝓖 of increasing accuracy as n → ∞. On the other hand, from Theorem 3.3, the unique solution of (3.18) can be obtained as

x=limnGn(x0,y0)=limnGn(y0,x0).

The graphs of xn and yn, for n = 0, 1, 6 are shown in Figure 1. Furthermore, the graphs of xnandyn, for n = 0, 1, 6 are shown in Figure 2.

Figure 1 
Graphs of xn and yn
Figure 1

Graphs of xn and yn

Figure 2 
Graphs of 

xn′andyn′
$\begin{array}{}
x_n'\, \text{and}\, y_n'
\end{array} $
Figure 2

Graphs of xnandyn

Remark 3.3

To derive the same results for the case in which A < 0 and B > 0, we can apply the same technique as mentioned above. The main difference is the structure of the function 𝓖 and consequently the definition of coupled lower and upper solution of the problem (1.3)-(1.4). We could carry out a similar argument to prove the existence, uniqueness and approximation results.

3.2 Investigation in the case AB > 0

In this subsection we consider the case in which AB > 0. Before continuing, we need to introduce the fixed point theorem which play main role in our discussion. For complete details, see [31, 32, 33].

Theorem 3.5

Let (X, ⪯) be a partially ordered set such that every pair x, yX has a lower bound and an upper bound. Furthermore, let d be a metric on X such that (X, d) is a complete metric space and 𝓖 is monotone (i.e., either order-preserving or order-reversing) map from X into X such that

0k<1:d(G(x),G(y))kd(x,y),xy,x0X:x0G(x0)orx0G(x0).

Suppose also that either 𝓖 is continuous or X is such that if xnx is a sequence in X whose consecutive terms are comparable, then there exists a subsequence {xnk} of {xn} such that every term is comparable to the limit x. Then 𝓖 has a unique fixed point x*. Moreover, for every xX, limn → ∞ 𝓖n (x) = x*.

In view of Lemma 2.6, we transform problem (1.3)-(1.4) as x = 𝓖(x) where 𝓖 : C1[0, 1] → C1[0, 1] is defined by

G(x)(t)=a+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αx(τ)dτ+0t(tτ)f(τ)Bx(τ)dτ.

Definition 3.5

An element x0C1[0, 1] is called a lower solution of problem (1.3)-(1.4) if

x0(t)b1+AΓ(3α)t2αAΓ(2α)0t(tτ)1αx0(τ)dτ+0tf(τ)Bx0(τ)dτ,x0(0)a, (3.20)

for all t ∈ [0, 1] and it is an upper solution of (1.3)-(1.4) if the above inequalities are reversed.

Theorem 3.6

Assume that x0C1[0, 1] is a lower solution of problem (1.3)-(1.4) and k=|B|+|A|Γ(3α)<1.

  1. Then the initial value problem (1.3)-(1.4) has a unique solution x*C1[0, 1].

  2. Moreover, the iterative sequence {xn} defined by

    xn(t)=a+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αxn1(τ)dτ+0t(tτ)f(τ)Bxn1(τ)dτ,

    converges to x* in C1[0, 1].

  3. In addition, the following error estimates hold,

    xnxC1[0,1]kn1kx1x0C1[0,1].xn+1xnC1[0,1]knx1x0C1[0,1].

Proof

The proof is similar to that for Theorem 3.4. It suffices to define 𝓖 : C1[0, 1] → C1[0, 1] by

G(x)(t)=a+bt+AΓ(4α)t3αAΓ(3α)0t(tτ)2αx(τ)dτ+0t(tτ)f(τ)Bx(τ)dτ,

and to apply a similar arguments as in the proof of Theorem 3.4 correspondig to Theorem 3.5. □

Example 3.2

Let us consider the following problem

x(t)25D32x(t)12x(t)=f(t),0<t1,x(0)=0,x(0)=916, (3.21)

where f(t)=12t3+34t2+18332t345t(3+4t)π and the exact solution is x(t)=t332t2+916t.

Here A=25andB=12. Observe that k=|B|+|A|Γ(3α)=0.95135 < 1. Now, define 𝓖 : C1[0, 1] → C1[0, 1] by

G(x)(t)=916t25Γ(4α)t3α+25Γ(3α)0t(tτ)2αx(τ)dτ+0t(tτ)12τ3+34τ2+18332τ345τ(3+4τ)π+12x(τ)dτ.

A relatively simple calculation, with the help of Maple, shows that x0(t) = − 12 t is a lower solution of problem (3.21). Therefore, all the assumption of Theorem 3.6 hold and consequently, problem (3.21) has a unique solution in C1[0, 1]. Moreover, the unique solution of (3.21) can be obtained as limn → ∞xn where xn = 𝓖 (xn−1). The graphs of xn and yn, for n = 0, 1, 6 are shown in Figure 3. Furthermore, the graphs of xnandyn, for n = 0, 1, 6 are shown in Figure 4.

Figure 3 
Graphs of xn and exact solution
Figure 3

Graphs of xn and exact solution

Figure 4 
Graphs of 

xn′
$\begin{array}{}
x_n'
\end{array} $ and derivative of exact solution
Figure 4

Graphs of xn and derivative of exact solution

Acknowledgement

The research of J.J. Nieto has been partially supported by the Agencia Estatal de Innovación (AEI) of Spain under grant MTM2016-75140-P, and Xunta de Galicia, grants GRC 2015-004 and R 2016/022, and co-financed by the European Community fund FEDER.

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Received: 2018-01-30
Accepted: 2019-03-20
Published Online: 2019-05-30

© 2019 Fazli and Nieto, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

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