Skip to main content

Theory and Modern Applications

# Existence and multiplicity of positive solutions for singular fractional differential equations with integral boundary value conditions

## Abstract

In this paper, we discuss the existence and multiplicity of positive solutions for singular fractional differential equations with integral boundary value conditions

$$\textstyle\begin{cases} {}^{C} D^{\alpha}u(t)+f(t,u(t))=0,\quad 0< t< 1,\\ u''(0)=u'''(0)=0,\\ u'(0)=u(1)=\eta\int_{0}^{1}u(s)\,ds, \end{cases}$$

where $$3<\alpha<4$$, $$0<\eta< 2$$, $${}^{C} D^{\alpha}$$ is the Caputo fractional derivative and f may be singular at $$u=0$$. Our results are based on the Leray-Schauder nonlinear alternative and a fixed-point theorem in cones.

## 1 Introduction

In this paper, we discuss the following nonlinear fractional differential equations with integral boundary conditions:

$$\textstyle\begin{cases} {}^{C} D^{\alpha}u(t)+f(t,u(t))=0,\quad 0< t< 1,\\ u''(0)=u'''(0)=0,\\ u'(0)=u(1)=\eta\int_{0}^{1}u(s)\,ds, \end{cases}$$
(1.1)

where $$3<\alpha<4$$, $$0<\eta< 2$$, $${}^{C} D^{\alpha}$$ is the Caputo fractional derivative, and f may be singular at $$u=0$$.

Differential equations with fractional derivative have been proved to be strong tools in the modeling of many physical phenomena. In consequence the subject of fractional differential equations is gaining much importance and attention [1â€“3]. Some recent investigations have shown that many physical systems can be represented more accurately using fractional derivative formulations. For details, see [4â€“10].

Cabada and Wang [11] investigated the existence of positive solutions for fractional differential equations with integral boundary value conditions

$$\textstyle\begin{cases} {}^{C} D^{\alpha}u(t)+f(t,u(t))=0,\quad 0< t< 1,\\ u(0)=u''(0)=0,\quad\quad u(1)=\lambda\int_{0}^{1}u(s)\,ds, \end{cases}$$

by the Guo-Krasnoselskii fixed point theorem, where $$2<\alpha<3$$, $$0<\lambda< 2$$, $${}^{C} D^{\alpha}$$ is the Caputo fractional derivative, and f is continuous on $$[0,1]\times[0,\infty)$$.

Zhang et al. [12] considered the fractional boundary value problem with a p-Laplacian operator as below:

$$\textstyle\begin{cases} -D^{\beta}_{t}( \varphi_{p}(D^{\alpha}_{t}x))(t)=\lambda f(t,x(t)),\quad 0< t< 1,\\ x(0)=0,\quad\quad D^{\alpha}_{t}x(0)=0,\quad\quad x(1)=\int_{0}^{1}x(s)\,dA(s), \end{cases}$$

where $$D^{\beta}_{t}$$ and $$D^{\alpha}_{t}$$ are the standard Riemann-Liouville derivatives with $$1<\alpha\leq2$$, $$0<\beta\leq1$$, $$\varphi _{p}(s)=|s|^{p-2}s$$, $$p>1$$, and f may be singular at $$t=0,1$$ and $$x=0$$. A is a function of the bounded variation and $$\int_{0}^{1}x(s)\,dA(s)$$ denotes the Riemann-Stieltjes integral of x with respect to A. By using the method of upper and lower solutions and the Schauder fixed point theorem, the existence of positive solutions was established.

Zhou et al. [13] investigated the multiplicity of positive solutions of the nonlinear fractional differential equation boundary value problem

$$\textstyle\begin{cases} D^{q}_{0^{+}} u(t)=f(t,u(t)),\quad 0< t< 1,\\ u(0)=u'(1)=0, \end{cases}$$

by means of the Leray-Schauder nonlinear alternative, a fixed-point theorem on cones, and a mixed monotone method, where $$1< q\leq2$$, $$D^{q}_{0^{+}}$$ is the standard Riemann-Liouville derivative. The function f is a given function satisfying some assumptions.

But up to now, there are few papers that have considered the multiplicity of positive solutions with two integral boundary conditions and a nonlinear term f possessing a singularity at $$u=0$$. Motivated by the results mentioned above, the aim of this paper is to establish the multiplicity of positive solutions for singular fractional differential equations with two integral boundary value conditions (1.1).

In this paper, in analogy with boundary value problems for differential equations of integer order, we first of all derive the corresponding Greenâ€™s function known as the fractional Greenâ€™s function. Here we give some properties that relate the expressions of $$G(t,s)$$ and $$G(1,s)$$. It is well known that cones play an important role in applying the Greenâ€™s function in research areas. Consequently problem (1.1) is reduced to an equivalent Fredholm integral equation. Finally, by using the Leray-Schauder nonlinear alternative and a fixed-point theorem in cones, the existence and multiplicity of positive solutions are obtained.

## 2 Background materials and Greenâ€™s function

For the readerâ€™s convenience, we present some necessary definitions from fractional calculus, both theory and lemmas. These definitions can be found in the recent literature such as [14].

### Definition 2.1

[14]

For a function $$f:[0,\infty ]\rightarrow R$$, the Caputo derivative of fractional order Î± is defined as

$${}^{C} D^{\alpha}f(t)=\frac{1}{\Gamma(n-\alpha)} \int_{0}^{t}\frac {f^{(n)}(s)}{(t-s)^{\alpha-n+1}}\,ds,\quad n=[ \alpha]+1,$$

where $$[\alpha]$$ denotes the integer part of the real number Î±.

### Definition 2.2

[14]

The Riemann-Liouville fractional integral of order Î± for a function f is defined as

$$I^{\alpha}f(t)=\frac{1}{\Gamma(\alpha)} \int_{0}^{t}(t-s)^{\alpha -1}f(s)\,ds,\quad \alpha>0,$$

provided that such an integral exists.

### Lemma 2.1

[14]

Let $$\alpha>0$$, then the fractional differential equation

$${}^{C} D^{\alpha}u(t)=0$$

has a solution

$$u(t)=C_{0}+C_{1}t+C_{2}t^{2}+ \cdots+C_{n-1}t^{n-1},$$

where $$C_{i}\in R$$, $$i=0,1,2,\ldots, n-1$$, $$n=[\alpha]+1$$.

### Lemma 2.2

[14]

Let $$\alpha>0$$, then

$$I^{\alpha}{}^{C} D^{\alpha}u(t)=u(t)-C_{0}-C_{1}t-C_{2}t^{2}- \cdots-C_{n-1}t^{n-1},$$

where $$C_{i}\in R$$, $$i=0,1,2,\ldots, n-1$$, $$n=[\alpha]+1$$.

In the following we present the Greenâ€™s function of a fractional differential equation with integral boundary conditions.

### Lemma 2.3

Given $$y\in C(0,1)\cap L(0,1)$$, $$3<\alpha <4$$, and $$0<\eta< 2$$, the unique solution of

$$\textstyle\begin{cases} {}^{C} D^{\alpha}u(t)+y(t)=0,\quad 0< t< 1,\\ u''(0)=u'''(0)=0,\\ u'(0)=u(1)=\eta\int_{0}^{1}u(s)\,ds, \end{cases}$$
(2.1)

is

$$u(t)= \int_{0}^{1}G(t,s)y(s)\,ds,$$

where

$$G(t,s)=\frac{1}{\alpha(2-\eta)\Gamma(\alpha)}\textstyle\begin{cases} \{\alpha(2-\eta)+2\eta t(\alpha-1+s)\}(1-s)^{\alpha-1}-\alpha(2-\eta )(t-s)^{\alpha-1}, \\ \quad 0\leq s\leq t\leq1,\\ \{\alpha(2-\eta)+2\eta t(\alpha-1+s)\}(1-s)^{\alpha -1},\\ \quad0\leq t\leq s \leq1. \end{cases}$$
(2.2)

### Proof

By means of the Lemma 2.2, we can reduce (2.1) to the equivalent integral equation

\begin{aligned} u(t) =&-I^{\alpha}y(t)+C_{0}+C_{1}t+C_{2}t^{2}+C_{3}t^{3} \\ =&-\frac{1}{\Gamma(\alpha)} \int_{0}^{t}(t-s)^{\alpha -1}y(s) \,ds+C_{0}+C_{1}t+C_{2}t^{2}+C_{3}t^{3}. \end{aligned}

From $$u''(0)=u'''(0)=0$$, we have $$C_{2}=C_{3}=0$$. Then

\begin{aligned} &u(t)=-\frac{1}{\Gamma(\alpha)} \int_{0}^{t}(t-s)^{\alpha-1}y(s) \,ds+C_{0}+C_{1}t, \\ &u'(t)=-\frac{\alpha-1}{\Gamma(\alpha)} \int_{0}^{t}(t-s)^{\alpha -2}y(s) \,ds+C_{1}, \end{aligned}
(2.3)

and by the condition $$u'(0)=u(1)=\eta\int_{0}^{1}u(s)\,ds$$, we have

\begin{aligned} &u'(0)=C_{1} =\eta \int_{0}^{1}u(s)\,ds, \\ &u(1)=-\frac{1}{\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha -1}y(s) \,ds+C_{0}+C_{1}=\eta \int_{0}^{1}u(s)\,ds. \end{aligned}
(2.4)

Then,

$$C_{0}=\frac{1}{\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha-1}y(s)\,ds.$$

From the previous equality, we deduce that

$$u(t)=-\frac{1}{\Gamma(\alpha)} \int_{0}^{t}(t-s)^{\alpha-1}y(s)\,ds+ \frac {1}{\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha-1}y(s) \,ds+C_{1}t.$$
(2.5)

Integrating the equation from 0 to 1, we have

\begin{aligned} \int_{0}^{1}u(t)\,dt =&-\frac{1}{\Gamma(\alpha)} \int_{0}^{1} \int _{0}^{t}(t-s)^{\alpha-1}y(s)\,ds\,dt+ \frac{1}{\Gamma(\alpha)} \int_{0}^{1} \int _{0}^{1}(1-s)^{\alpha-1}y(s)\,ds\,dt \\ &{}+C_{1} \int_{0}^{1}t\,dt \\ =& -\frac{1}{\Gamma(\alpha)} \int_{0}^{1}\frac{(1-s)^{\alpha}}{\alpha }y(s)\,ds+ \frac{1}{\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha-1}y(s)\,ds+ \frac{1}{2}C_{1}. \end{aligned}

So equation (2.4) implies that

$$C_{1} =\eta \int_{0}^{1}u(s)\,ds=-\frac{\eta}{\alpha\Gamma(\alpha)} \int _{0}^{1}(1-s)^{\alpha}y(s)\,ds+ \frac{\eta}{\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha -1}y(s)\,ds+ \frac{1}{2}C_{1}\eta.$$

Hence, we have

$$C_{1}=-\frac{2\eta}{\alpha(2-\eta)\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha}y(s)\,ds+ \frac{2\eta}{(2-\eta)\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha-1}y(s)\,ds.$$

Therefore, the unique solution of (2.1) is

\begin{aligned} u(t) =&-\frac{1}{\Gamma(\alpha)} \int_{0}^{t}(t-s)^{\alpha-1}y(s)\,ds+ \frac {1}{\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha-1}y(s)\,ds \\ &{}-\frac{2\eta t}{\alpha(2-\eta)\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha}y(s)\,ds+ \frac{2\eta t}{(2-\eta)\Gamma(\alpha)} \int_{0}^{1}(1-s)^{\alpha -1}y(s)\,ds \\ =&-\frac{1}{\Gamma(\alpha)} \int_{0}^{t}(t-s)^{\alpha-1}y(s)\,ds \\ &{}+\frac {1}{\alpha(2-\eta)\Gamma(\alpha)} \int_{0}^{1}\bigl[\alpha(2-\eta)+2\eta t(\alpha-1+s) \bigr](1-s)^{\alpha-1}y(s)\,ds \\ =&\frac{1}{\alpha(2-\eta)\Gamma(\alpha)} \\ &{}\times \int_{0}^{t} \bigl\{ \bigl[\alpha(2-\eta)+2\eta t( \alpha-1+s)\bigr](1-s)^{\alpha -1}-\alpha(2-\eta) (t-s)^{\alpha-1} \bigr\} y(s)\,ds \\ &{}+\frac{1}{\alpha(2-\eta)\Gamma(\alpha)} \int_{t}^{1}\bigl[\alpha(2-\eta )+2\eta t(\alpha-1+s) \bigr](1-s)^{\alpha-1}y(s)\,ds \\ =& \int_{0}^{1}G(t,s)y(s)\,ds. \end{aligned}

â€ƒâ–¡

### Lemma 2.4

The function $$G(t,s)$$ defined by (2.2) has the following properties:

1. (1)

$$G(1,s)=0$$, for $$s\in[0,1]$$ if and only if $$\eta=0$$;

2. (2)

$$G(1,s)>0$$, for $$s\in(0,1)$$ and $$\eta\in(0,2)$$;

3. (3)

$$tG(1,s)\leq G(t,s)\leq M_{0} G(1,s)$$, for $$3<\alpha<4$$, $$s\in(0,1)$$ and $$\eta\in(0,2)$$ where $$M_{0}=\frac{\alpha(\eta+2)}{2\eta(\alpha-1)}$$;

4. (4)

$$G(t,s)>0$$, for $$t,s\in(0,1)$$ and $$\eta\in(0,2)$$.

### Proof

Observing the expression of $$G(1,s)$$, it is clear that (1) and (2) hold.

Here

$$G(1,s)=\frac{2\eta(\alpha-1+s)(1-s)^{\alpha-1}}{\alpha(2-\eta)\Gamma (\alpha)}.$$

In the following we will only prove (3), as (4) can be deduced directly from (3).

When $$0< t\leq s<1$$, we have

$$h(t,s)=\frac{G(t,s)}{G(1,s)}=\frac{\alpha(2-\eta)+2\eta t (\alpha -1+s)}{2\eta(\alpha-1+s)}.$$

Now, it is immediate to verify the following inequalities:

$$t=\frac{2\eta t (\alpha-1+s)}{2\eta(\alpha-1+s)}\leq h(t,s)\leq\frac {\alpha(2-\eta)+2\eta t \alpha}{2\eta(\alpha-1)}\leq\frac{\alpha(2-\eta )+2\eta\alpha}{2\eta(\alpha-1)}= \frac{\alpha(2+\eta)}{2\eta(\alpha-1)}.$$

When $$0< s\leq t<1$$, we have

$$h(t,s)=\frac{G(t,s)}{G(1,s)}=\frac{[\alpha(2-\eta)+2\eta t (\alpha -1+s)](1-s)^{\alpha-1}-\alpha(2-\eta)(t-s)^{\alpha-1}}{2\eta(\alpha -1+s)(1-s)^{\alpha-1}},$$

and since $$s\geq ts$$, we deduce that

\begin{aligned} h(t,s) \geq&\frac{[\alpha(2-\eta)+2\eta t (\alpha-1+s)](1-s)^{\alpha -1}-\alpha(2-\eta)t^{\alpha-1}(1-s)^{\alpha-1}}{2\eta(\alpha -1+s)(1-s)^{\alpha-1}} \\ =&\frac{\alpha(2-\eta)+2\eta t (\alpha-1+s)-\alpha(2-\eta)t^{\alpha -1}}{2\eta(\alpha-1+s)} \\ \geq&\frac{\alpha(2-\eta)+2\eta t (\alpha-1+s)-\alpha(2-\eta)}{2\eta (\alpha-1+s)}\\ =&t. \end{aligned}

On the other hand, we have

$$h(t,s)\leq\frac{\alpha(2-\eta)+2\eta t (\alpha-1+s)}{2\eta(\alpha -1+s)}\leq\frac{\alpha(2+\eta)}{2\eta(\alpha-1)};$$

then the inequalities (3) are fulfilled.â€ƒâ–¡

### Theorem 2.1

(Leray-Schauder alternative)

Let E be a Banach space, X a closed, convex subset of E, U an open subset of X, and $$p\in U$$. Suppose that $$A:\overline {U}\rightarrow X$$ is a continuous, compact map, then either

1. (i)

A has a fixed point in UÌ…, or

2. (ii)

there is a $$u\in\partial U$$ and $$\lambda\in(0,1)$$ with $$u=\lambda AU+(1-\lambda)p$$.

### Theorem 2.2

Let X be a Banach space, and let $$P\subset X$$ be a cone. Assume $$\Omega_{1}$$, $$\Omega_{2}$$ are open and bounded subsets of X with $$0\in\Omega_{1}\in\overline{\Omega_{1}}\subset\Omega _{2}$$, and let $$T:P\cap(\overline{\Omega_{2}}\setminus\Omega_{1})\rightarrow P$$ be a completely continuous operator such that either

1. (i)

$$\|Tu\|\geq\|u\|$$, $$u\in P\cap\partial\Omega_{1}$$, and $$\|Tu\|\leq\| u\|$$, $$u\in P\cap\partial\Omega_{2}$$; or

2. (ii)

$$\|Tu\|\leq\|u\|$$, $$u\in P\cap\partial\Omega_{1}$$, and $$\|Tu\|\geq \|u\|$$, $$u\in P\cap\partial\Omega_{2}$$.

Then the operator T has at least one fixed point in $$P\cap(\overline {\Omega_{2}}\setminus\Omega_{1})$$.

## 3 Main results

In this section, we consider the existence and multiplicity of positive solutions of nonlinear fractional different equation

$$\textstyle\begin{cases} {}^{C} D^{\alpha}u(t)+f(t,u(t))=0,\quad 0< t< 1,\\ u''(0)=u'''(0)=0,\\ u'(0)=u(1)=\eta\int_{0}^{1}u(s)\,ds, \end{cases}$$
(3.1)

where $$3<\alpha<4$$, $$0<\eta< 2$$, $${}^{C} D^{\alpha}$$ is the Caputo fractional derivative, and f may be singular at $$u=0$$.

### Theorem 3.1

Suppose that the following hypotheses hold:

(H1):

$$f:[0,1]\times(0,\infty)\rightarrow[0,\infty)$$ is continuous and

$$0\leq f(t,u)=g(u)+h(u),\quad\textit{for } (t,u)\in[0,1]\times(0,\infty),$$

with $$g(u)>0$$ is nonincreasing and $$h(u)/g(u)$$ is nondecreasing in $$u\in (0,\infty)$$;

(H2):

there exists a constant $$K_{0}>0$$ such that $$g(ab)\leq K_{0}g(a)g(b)$$ for all $$a,b\geq0$$;

(H3):

$$\int_{0}^{1}g(s)\,ds<\infty$$;

(H4):

there exists a positive number r such that

$$\biggl\{ 1+\frac{h(r)}{g(r)}\biggr\} M_{0}K_{0}g\biggl( \frac{r}{M_{0}}\biggr) \int_{0}^{1}G(1,s)g(s)\,ds< r;$$
(H5):

there exists a positive number $$R>r$$ with

$$\biggl(1-\frac{2}{\alpha}\biggr)g(R) \int_{0}^{1}G(1,s) \biggl\{ 1+\frac{h(\frac {R}{M_{0}}s)}{g(\frac{R}{M_{0}}s)} \biggr\} \,ds\geq R.$$

Then problem (3.1) has a solution u with $$r\leq\|u\|\leq R$$.

### Proof

Let $$E=C[0,1]$$ be endowed with the maximum norm, $$\|u\| =\max_{0\leq t\leq1}|u(t)|$$, define the cone $$K\subset E$$ by

$$K=\biggl\{ u\in E\Big| u(t)\geq\frac{t}{M_{0}}\|u\|,\mbox{ for }t\in[0,1]\biggr\} ,$$

and let

$$\Omega_{1}= \bigl\{ u\in E; \|u\|< r \bigr\} ,\quad\quad\Omega_{2}= \bigl\{ u \in E; \|u\|< R \bigr\} .$$

Next let $$T:K\cap(\overline{\Omega_{2}}\setminus\Omega_{1})\rightarrow E$$ be defined by

$$Tu(t)= \int_{0}^{1}G(t,s)f\bigl(s,u(s)\bigr)\,ds, \quad 0\leq t \leq1.$$
(3.2)

First we show T is well defined. To see this, notice that if $$u\in K\cap(\overline{\Omega_{2}}\setminus\Omega_{1})$$ then $$r\leq\|u\|\leq R$$ and $$u(t)\geq\frac{t}{M_{0}}\|u\|\geq\frac {t}{M_{0}}r>0$$, $$0< t<1$$, from (H1) we have

\begin{aligned} f(t,u) =&g\bigl(u(t)\bigr)+h\bigl(u(t)\bigr) \\ =&g\bigl(u(t)\bigr)\biggl\{ 1+\frac{h(u(t))}{g(u(t))}\biggr\} \\ \leq&g\biggl(\frac{tr}{M_{0}}\biggr)\biggl\{ 1+\frac{h(R)}{g(R)}\biggr\} \\ \leq&K_{0}g(t)g\biggl(\frac{r}{M_{0}}\biggr)\biggl\{ 1+ \frac{h(R)}{g(R)}\biggr\} . \end{aligned}

These inequalities with (H3) guarantee that $$T:K\cap(\overline {\Omega_{2}}\setminus\Omega_{1})\rightarrow E$$ is well defined. If $$u\in K\cap(\overline{\Omega_{2}}\setminus\Omega_{1})$$, then we have

\begin{aligned}& \|Tu\| \leq \int_{0}^{1}M_{0} G(1,s)f\bigl(s,u(s) \bigr)\,ds, \\ & Tu(t) \geq t \int_{0}^{1} G(1,s)f\bigl(s,u(s)\bigr)\,ds \geq \frac{t}{M_{0}}\|Tu\|, \end{aligned}

i.e., $$Tu\in K$$ so $$T: K\cap(\overline{\Omega_{2}}\setminus \Omega_{1})\rightarrow K$$.

Next we show $$T: K\cap(\overline{\Omega_{2}}\setminus\Omega _{1})\rightarrow K$$ is continuous and compact. Let $$u_{n},u\in K\cap (\overline{\Omega_{2}}\setminus\Omega_{1})$$ with $$\|u_{n}-u\|\rightarrow0$$ as $$n\rightarrow\infty$$. Of course $$r\leq\|u_{n}\|\leq R$$, $$r\leq\|u\|\leq R$$, $$u_{n}(t)\geq\frac{tr}{M_{0}}>0$$ and $$u(t)\geq\frac{tr}{M_{0}}>0$$, for $$0< t<1$$. So

$$\rho_{n}(s)=\bigl|f\bigl(s,u_{n}(s)\bigr)-f\bigl(s,u(s)\bigr)\bigr| \rightarrow0,\quad s\in(0,1),$$

and

$$\rho_{n}(s)\leq2K_{0}g(s)g\biggl(\frac{r}{M_{0}} \biggr)\biggl\{ 1+\frac{h(R)}{g(R)}\biggr\}$$

for $$s\in(0,1)$$. Now this together with the Lebesgue dominated convergence theorem guarantees that

$$\|Tu_{n}-Tu\|\leq\sup_{t\in[0,1]} \int_{0}^{1} G(t,s)\rho _{n}(s)\,ds \rightarrow0 \quad\mbox{as }n\rightarrow\infty.$$

Therefore, $$T: K\cap(\overline{\Omega_{2}}\setminus\Omega _{1})\rightarrow K$$ is continuous.

Next, we show that T is uniformly bounded. For $$u\in K\cap (\overline{\Omega_{2}}\setminus\Omega_{1})$$ we have

\begin{aligned} \|Tu\| =&\sup_{t\in[0,1]} \int_{0}^{1} G(t,s)f\bigl(s,u(s)\bigr)\,ds \leq \int_{0}^{1}M_{0}G(1,s)g\bigl(u(s)\bigr) \biggl\{ 1+\frac{h(u(s))}{g(u(s))}\biggr\} \,ds \\ \leq& \int_{0}^{1}M_{0}G(1,s)K_{0}g \biggl(\frac{r}{M_{0}}\biggr)g(s)\biggl\{ 1+\frac{h(R)}{g(R)}\biggr\} \,ds \\ =&M_{0}K_{0}g\biggl(\frac{r}{M_{0}}\biggr)\biggl\{ 1+ \frac{h(R)}{g(R)}\biggr\} \int_{0}^{1}G(1,s)g(s)\,ds. \end{aligned}

Hence, $$T: K\cap(\overline{\Omega_{2}}\setminus\Omega_{1})\rightarrow K$$ is bounded.

Finally, we show that T is equicontinuous.

For all $$\epsilon>0$$, each $$u\in K\cap(\overline{\Omega_{2}}\setminus \Omega_{1})$$, $$t,t'\in[0,1]$$, $$t< t'$$, since $$G(t,s)$$ is uniformly continuous on $$t,s\in[0,1]\times[0,1]$$, there exists $$\eta>0$$, such that when $$t'-t<\eta$$ we have

\begin{aligned}& \bigl|G\bigl(t',s\bigr)-G(t,s)\bigr| < \frac{\epsilon}{K_{0}\int_{0}^{1}g(s)\,dsg(\frac{r}{M_{0}})\{ 1+\frac{h(R)}{g(R)}\}}, \\& \bigl|(Tu) (t)-(Tu) \bigl(t'\bigr)\bigr| \leq \int_{0}^{1}\bigl|G(t,s)-G\bigl(t',s\bigr)\bigr|f \bigl(s,u(s)\bigr)\,ds \\& \hphantom{\bigl|(Tu) (t)-(Tu) \bigl(t'\bigr)\bigr|} \leq \int_{0}^{1}\bigl|G(t,s)-G\bigl(t',s \bigr)\bigr|K_{0}g(s)g\biggl(\frac{r}{M_{0}}\biggr)\biggl\{ 1+ \frac {h(R)}{g(R)}\biggr\} \,ds. \end{aligned}

By means of the Arzela-Ascoli theorem, $$T: K\cap(\overline{\Omega _{2}}\setminus\Omega_{1})\rightarrow K$$ is compactly continuous.

Now we prove that

$$\|Tu\|\leq\|u\|,\quad\forall u\in K\cap\partial \Omega_{1}.$$
(3.3)

To see this, let $$u\in K\cap\partial\Omega_{1}$$, then $$\|u\|=r$$ and $$u(t)\geq\frac{tr}{M_{0}}>0$$ for $$t\in(0,1)$$, and we have

\begin{aligned} (Tu) (t) =& \int_{0}^{1}G(t,s)f\bigl(s,u(s)\bigr)\,ds \\ \leq& \int_{0}^{1}G(t,s)g\bigl(u(s)\bigr)\biggl\{ 1+ \frac{h(u(s))}{g(u(s))}\biggr\} \,ds \\ \leq&M_{0}K_{0}g\biggl(\frac{r}{M_{0}}\biggr)\biggl\{ 1+\frac{h(r)}{g(r)}\biggr\} \int _{0}^{1}G(1,s)g(s)\,ds \\ < &r=\|u\|. \end{aligned}

Therefore, $$\|Tu\|\leq\|u\|$$, i.e. (3.3) holds.

Finally, we prove that

$$\|Tu\|\geq\|u\|,\quad\forall u\in K\cap\partial \Omega_{2}.$$
(3.4)

To see this, let $$u\in K\cap\partial\Omega_{2}$$, then $$\|u\|=R$$ and $$u(t)\geq\frac{tR}{M_{0}}>0$$ for $$t\in(0,1)$$,

\begin{aligned} Tu\biggl(1-\frac{2}{\alpha}\biggr) =& \int_{0}^{1}G\biggl(1-\frac{2}{\alpha},s\biggr)f \bigl(s,u(s)\bigr)\,ds \\ \geq&\biggl(1-\frac{2}{\alpha}\biggr) \int_{0}^{1}G(1,s)g\bigl(u(s)\bigr)\biggl\{ 1+ \frac {h(u(s))}{g(u(s))}\biggr\} \,ds \\ \geq&\biggl(1-\frac{2}{\alpha}\biggr)g(R) \int_{0}^{1}G(1,s)\biggl\{ 1+\frac{h(\frac {R}{M_{0}}s)}{g(\frac{R}{M_{0}}s)}\biggr\} \,ds \\ \geq&R=\|u\|. \end{aligned}

This implies that (3.4) holds.

It follows from Theorem 2.2, (3.3), and (3.4) that T has a fixed point $$\widetilde{u}\in K\cap(\overline{\Omega_{2}}\setminus\Omega _{1})$$. Clearly this fixed point is a positive solution of (3.1) satisfying $$r\leq\|\widetilde{u}\|\leq R$$.â€ƒâ–¡

### Theorem 3.2

Suppose the conditions (H1)-(H4) hold. In addition, assume that

(H6):

for each $$L>0$$, there exists a function $$\varphi_{L}\in C[0,1]$$, $$\varphi_{L}>0$$, for $$t\in(0,1)$$, such that $$f(t,u)>\varphi_{L}(t)$$, for $$(t,u)\in(0,1)\times(0,L]$$. Then (3.1) has a solution u with $$0<\|u\|<r$$.

### Proof

The existence is proved using Theorem 2.1, together with a truncation technique. The idea is that we first show (3.1) has a positive solution u satisfying $$u(t)>0$$ for $$t\in(0,1)$$. Similarly to the proof of Theorem 3.1, we show

$$u(t)= \int_{0}^{1} G(t,s)f\bigl(s,u(s)\bigr)\,ds$$
(3.5)

has a positive solution.

Since (H4) holds, we can choose $$n_{0}\in\{ 1,2,\ldots\}$$ such that

$$\biggl\{ 1+\frac{h(r)}{g(r)}\biggr\} M_{0}K_{0}g\biggl( \frac{r}{M_{0}}\biggr) \int_{0}^{1}G(1,s)g(s)\,ds+\frac {1}{n_{0}}< r.$$

Let $$N_{0}\in\{ n_{0},n_{0}+1,\ldots\}$$. Consider the family of integral equations

$$(A_{n}u) (t)= \int_{0}^{1}G(t,s)f_{n}\bigl(s,u(s)\bigr) \,ds+\frac{1}{n},$$
(3.6)

where $$n\in N_{0}$$ and

$$f_{n}(t,u)=\textstyle\begin{cases} f(t,u)&\mbox{if } u\geq\frac{1}{n},\\ f(t,\frac{1}{n})&\mbox{if } u\leq\frac{1}{n}. \end{cases}$$

Similarly to the proof of Theorem 3.1, we can easily verify that $$A_{n}$$ is well defined and maps E to K. Moreover, $$A_{n}$$ is continuous and completely continuous. By the Leray-Schauder alternative principle, we need to consider

$$u=\lambda A_{n}u+(1-\lambda)\frac{1}{n}$$

i.e.

$$u(t)=\lambda \int_{0}^{1}G(t,s)f_{n}\bigl(s,u(s)\bigr) \,ds+\frac{1}{n},$$
(3.7)

where $$\lambda\in(0,1)$$. We claim that any fixed point u of (3.7) for any $$\lambda\in(0,1)$$ must satisfy $$\|u\|\neq r$$. Otherwise, assume that u is a fixed point of (3.7) for some $$\lambda \in(0,1)$$ such that $$\|u\|= r$$. Then $$u(t)\geq\frac{1}{n}$$ for $$t\in [0,1]$$. Note that

$$\bigl\| u(t)\bigr\| \leq\frac{1}{n}+\lambda M_{0} \int_{0}^{1}G(1,s)f_{n}\bigl(s,u(s)\bigr) \,ds.$$

Hence, for all $$t\in[0,1]$$, we have

\begin{aligned} \bigl\| u(t)\bigr\| \geq& \frac{1}{n}+\lambda t \int_{0}^{1}G(1,s)f_{n}\bigl(s,u(s)\bigr) \,ds \\ \geq&\frac{1}{n}+ \frac{t}{M_{0}}\biggl\{ \bigl\| u(t)\bigr\| -\frac{1}{n} \biggr\} \\ \geq& \frac{t}{M_{0}}\bigl\| u(t)\bigr\| =\frac{t}{M_{0}}r. \end{aligned}

Thus we have the condition (H1), for all $$t\in[0,1]$$,

\begin{aligned} u(t) =&\lambda \int_{0}^{1}G(t,s)f_{n}\bigl(s,u(s)\bigr) \,ds+\frac{1}{n} \\ =&\lambda \int_{0}^{1}G(t,s)f\bigl(s,u(s)\bigr)\,ds+ \frac{1}{n} \\ \leq& \int_{0}^{1}M_{0}G(1,s)f\bigl(s,u(s) \bigr)\,ds+\frac{1}{n} \\ \leq& \int_{0}^{1}M_{0}G(1,s)g\bigl(u(s)\bigr) \biggl\{ 1+\frac{h(u(s))}{g(u(s))}\biggr\} \,ds+\frac {1}{n} \\ \leq&\biggl\{ 1+\frac{h(r)}{g(r)}\biggr\} \int_{0}^{1}M_{0}G(1,s)K_{0}g \biggl(\frac {r}{M_{0}}\biggr)g(s)\,ds+\frac{1}{n} \\ \leq&\biggl\{ 1+\frac{h(r)}{g(r)}\biggr\} M_{0}K_{0}g \biggl(\frac{r}{M_{0}}\biggr) \int _{0}^{1}G(1,s)g(s)\,ds+\frac{1}{n_{0}}. \end{aligned}

Therefore,

$$r=\|u\|\leq\biggl\{ 1+\frac{h(r)}{g(r)}\biggr\} M_{0}K_{0}g \biggl(\frac{r}{M_{0}}\biggr) \int _{0}^{1}G(1,s)g(s)\,ds+\frac{1}{n_{0}} .$$

This a contradiction to the choice of $$n_{0}$$ and the claim is proved.

Now the Leray-Schauder alternative (Theorem 2.1) guarantees $$A_{n}$$ has a fixed point, denoted by $$u_{n}$$, $$u_{n}(t)\geq\frac{1}{n}$$ in $$\overline {B_{r}}=\{u\in E: \|u\|< r\}$$, and it satisfies

\begin{aligned} u_{n}(t) =& \int_{0}^{1}G(t,s)f_{n} \bigl(s,u_{n}(s)\bigr)\,ds+\frac{1}{n} \\ =& \int_{0}^{1}G(t,s)f\bigl(s,u_{n}(s)\bigr) \,ds+\frac{1}{n}. \end{aligned}

Next we claim that $$u_{n}(t)$$ have a uniform positive lower bound, i.e., there exists a constant $$\delta>0$$, independent of $$n\in N_{0}$$, such that

$$\min_{t\in[0,1]}u_{n}(t)\geq\delta t,$$
(3.8)

for all $$n\in N_{0}$$. Since (H6) holds, there exists a continuous function $$\varphi_{r}(t)>0$$ such that $$f(t,u(t))>\varphi_{r}(t)$$ for all $$(t,u)\in(0,1)\times(0,r]$$. Since $$u_{n}(t)< r$$, we have

\begin{aligned} u_{n}(t) =& \int_{0}^{1}G(t,s)f\bigl(s,u_{n}(s)\bigr) \,ds+\frac{1}{n} \\ \geq& \int_{0}^{1}G(t,s)\varphi_{r}(s)\,ds \\ \geq&t \int_{0}^{1}G(1,s)\varphi_{r}(s)\,ds:= \delta t. \end{aligned}

In order to pass the fixed point $$u_{n}$$ of the truncation equations (3.6) to that of the original equation (3.5) we need the following fact:

$$\{u_{n}\}\mbox{ is equicontinuous on }[0,1]\mbox{ for all }n\in N_{0}.$$
(3.9)

In fact, for all $$\epsilon>0$$, each $$u_{n}\in B_{r}$$, $$t,t'\in[0,1]$$, $$t< t'$$, since $$G(t,s)$$ is uniformly continuous on $$(t,s)\in[0,1]\times[0,1]$$, there exists $$\tau>0$$, such that when $$t'-t<\tau$$ we have

$$\bigl|G\bigl(t',s\bigr)-G(t,s)\bigr| < \frac{\epsilon}{K_{0}g(\delta)\{1+\frac{h(r)}{g(r)}\}\int _{0}^{1}g(s)\,ds};$$

then

\begin{aligned} \bigl|u_{n}(t)-u_{n}\bigl(t'\bigr)\bigr| \leq& \int_{0}^{1}\bigl|G\bigl(t',s\bigr)-G(t,s)\bigr|f \bigl(s,u_{n}(s)\bigr)\,ds \\ \leq&K_{0}g(\delta) \int_{0}^{1}\bigl|G\bigl(t',s \bigr)-G(t,s)\bigr|g(s)\biggl\{ 1+\frac{h(r)}{g(r)}\biggr\} \,ds< \epsilon. \end{aligned}

The facts $$\|u_{n}\|< r$$ and (3.9) show that $$\{u_{n}\}_{n\in N_{0}}$$ is a bounded and equicontinuous family on $$[0,1]$$. Now the Arzela-Ascoli theorem guarantees that $$\{u_{n}\} _{n\in N_{0}}$$ has a subsequence $$\{u_{n_{k}}\}_{n_{k}\in N_{0}}$$, converging uniformly on $$[0,1]$$ to a function $$u\in E$$. From the facts $$\|u_{n}\|< r$$ and (3.8), u satisfies $$\delta t< u(t)< r$$ for all $$t\in[0,1]$$. Moreover, $$u_{n_{k}}$$ satisfies the integral equation

$$u_{n_{k}}= \int_{0}^{1}G(t,s)f\bigl(s,u_{n_{k}}(s)\bigr) \,ds+\frac{1}{n_{k}}.$$

Letting $$k\rightarrow\infty$$, we arrive at

$$u= \int_{0}^{1}G(t,s)f\bigl(s,u(s)\bigr)\,ds.$$

Therefore, u is a positive solution of (3.1) and satisfies $$0<\|u\|<r$$.â€ƒâ–¡

### Theorem 3.3

Suppose that (H1)-(H6) are satisfied. Then problem (3.1) has two positive solutions u, Å© with $$0<\|u\|<r\leq\|\widetilde{u}\|\leq R$$.

### Proof

From the proof of Theorem 3.1, we see that (3.1) has a positive solution $$\widetilde{u(t)}$$ with $$r\leq\|\widetilde{u}\|\leq R$$, and by Theorem 3.2, we see that (3.1) has another positive solution $$u(t)$$ with $$0<\| u\|<r$$. Thus (3.1) has at least two positive solutions.â€ƒâ–¡

### Example 3.1

Consider the boundary value problem

$$\textstyle\begin{cases} {}^{C} D^{\alpha}u(t)+u^{-a}(t)+\omega u^{b}(t)=0,\quad 0< t< 1,\\ u''(0)=u'''(0)=0,\\ u'(0)=u(1)=\eta\int_{0}^{1}u(s)\,ds, \end{cases}$$
(3.10)

where $$3<\alpha<4$$, $$0<\eta<2$$, $$0< a<1$$, $$b\geq0$$ and $$\omega>0$$ is a given parameter. Then:

1. (i)

if $$b<1$$, then (3.10) has at least one nonnegative solution for each $$\omega>0$$;

2. (ii)

if $$b>1$$, then (3.10) has at least one nonnegative solution for each $$0<\omega<\omega_{1}$$, where $$\omega_{1}$$ is some positive constant;

3. (iii)

if $$b>1$$, then (3.10) has at least two nonnegative solutions for each $$0<\omega<\omega_{1}$$.

### Proof

We apply Theorem 3.3. Note that (H6) holds with $$\phi _{L}(t)=L^{-\alpha}$$. Let

$$g(u)=u^{-a},\quad\quad h(u)=\omega u^{b},\quad\quad K_{0}=1.$$

Then (H1) and (H2) are satisfied. Since $$0< a<1$$, condition (H3) is also satisfied. Now for (H4) to be satisfied we need

$$\omega< \frac{Ar^{1+a}-1}{r^{a+b}}$$

for some $$r>0$$, where

$$A=\biggl[M_{0}^{1+a} \int_{0}^{1}G(1,s)s^{-a}\,ds \biggr]^{-1}.$$

Therefore (3.10) has at least one nonnegative solution for

$$0< \omega< \omega_{1}:=\sup_{r>0}\frac{Ar^{1+a}-1}{r^{a+b}}.$$

Note that $$\omega_{1}=\infty$$ if $$b<1$$, and if $$b>1$$ set

$$l(r):=\frac{Ar^{1+a}-1}{r^{a+b}}.$$

The function $$l(r)$$ possesses a maximum at

$$r_{0}:=\biggl(\frac{a+b}{(b-1)A}\biggr)^{\frac{1}{a+1}}>\biggl( \frac{1}{A}\biggr)^{\frac{1}{a+1}};$$

then $$\omega_{1}=l(r_{0})>0$$. We have the desired results (i) and (ii).

If $$b>1$$, condition (H5) becomes

$$\omega\geq\frac{R^{1+a}-B}{CR^{a+b}},$$
(3.11)

for some $$R>0$$, where

\begin{aligned}& B = \frac{\alpha-2}{\alpha} \int_{0}^{1}G(1,s)\,ds, \\& C = \frac{\alpha-2}{\alpha M_{0}^{a+b}} \int_{0}^{1}G(1,s)s^{a+b}\,ds. \end{aligned}

Since $$b>1$$, the right-hand side goes to 0 as $$R\rightarrow+\infty$$. Thus, for any given $$0<\omega<\omega_{1}$$, it is always possible to find an $$R\gg r$$ such that (3.11) is satisfied. Thus, (3.10) has an additional nonnegative solution Å©. This implies that (iii) holds.â€ƒâ–¡

## References

1. Wang, Y, Liu, L, Wu, Y: Positive solutions for a nonlocal fractional differential equation. Nonlinear Anal., Theory Methods Appl. 74, 3599-3605 (2011)

2. Bai, Z: On positive solutions of a nonlocal fractional boundary value problem. Nonlinear Anal., Theory Methods Appl. 72, 916-924 (2010)

3. Xu, J, Wei, Z, Dong, W: Uniqueness of positive solutions for a class of fractional boundary value problems. Appl. Math. Lett. 25, 590-593 (2012)

4. Jiang, D, Yuan, C: The positive properties of the Green function for Dirichlet-type boundary value problems of nonlinear fractional differential equations and its application. Nonlinear Anal., Theory Methods Appl. 72, 710-719 (2010)

5. Li, S, Zhang, X, Wu, Y, Caccetta, L: Extremal solutions for p-Laplacian differential systems via iterative computation. Appl. Math. Lett. 26, 1151-1158 (2013)

6. Zhao, X, Chai, C, Ge, W: Existence and nonexistence results for a class of fractional boundary value problems. J. Appl. Math. Comput. 41, 17-31 (2013)

7. Zhang, X, Liu, L, Wu, Y, Lu, Y: The iterative solutions of nonlinear fractional differential equations. Appl. Math. Comput. 219, 4680-4691 (2013)

8. Al-Refai, M, Hajji, M: Monotone iterative sequences for nonlinear boundary value problems of factional order. Nonlinear Anal. 74, 3531-3559 (2011)

9. Yao, Q: Successively iterative method of nonlinear Neumann boundary value problems. Appl. Math. Comput. 217, 2301-2306 (2010)

10. Li, CF, Luo, XN, Zhou, Y: Existence of positive solutions of the boundary value problem for nonlinear fractional differential equations. Comput. Math. Appl. 59, 1363-1375 (2010)

11. Cabada, A, Wang, G: Positive solutions of nonlinear fractional differential equations with integral boundary value conditions. J. Math. Anal. Appl. 389, 403-411 (2012)

12. Zhang, X, Liu, L, Wiwatanpataphee, B, Wu, Y: The eigenvalue for a class of singular p-Laplacian fractional differential equations involving the Riemann-Stieltjes integral boundary condition. Appl. Math. Comput. 235, 412-422 (2014)

13. Zhou, WX, Zhang, JG, Li, JM: Existence of multiple positive solutions for singular boundary value problems of nonlinear fractional differential equations. Adv. Differ. Equ. 2014, 97 (2014)

14. Bai, Z, Qiu, T: Existence of positive solutions for singular fractional differential equation. Appl. Math. Comput. 215, 2761-2767 (2009)

Download references

## Acknowledgements

The author sincerely thanks the editor and reviewers for their valuable suggestions and useful comments to improve the manuscript.

## Author information

Authors

### Corresponding author

Correspondence to Ying He.

## Additional information

### Competing interests

The author declares to have no competing interests.

### Authorâ€™s contributions

The whole work was carried out by the author.

## Rights and permissions

Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Reprints and permissions

## About this article

### Cite this article

He, Y. Existence and multiplicity of positive solutions for singular fractional differential equations with integral boundary value conditions. Adv Differ Equ 2016, 31 (2016). https://doi.org/10.1186/s13662-015-0729-7

Download citation

• Received:

• Accepted:

• Published:

• DOI: https://doi.org/10.1186/s13662-015-0729-7