Citation: Min Jiang, Rengang Huang. Existence of solutions for q-fractional differential equations with nonlocal Erdélyi-Kober q-fractional integral condition[J]. AIMS Mathematics, 2020, 5(6): 6537-6551. doi: 10.3934/math.2020421
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The aim of this paper is to establish the existence and uniqueness of solutions for the following nonlinear Riemann-Liouville q-fractional differential equation subject to nonlocal Erdélyi-Kober q-fractional integral conditions
{Dαqx(t)+f(t,x(t),Dδqx(t))=0,t∈(0,T),x(0)=0,ax(T)=n∑i=1λiIηi,μi,βiqx(ξi), | (1.1) |
where Dαq and Dρq are the fractional q-derivative of Riemann-Liouville type of order α and δ on (0,T) respectively, 1<α<2,0<δ<1,f∈C([0,T]×R×R,R), Iηi,μi,βiq denotes the Erdélyi-Kober fractional q-integral of order μi on (0,T), μi>0,βi>0,ηi∈R and ξi∈(0,T), a,λi(i=1,2,⋯,n) are some given constants.
The q-calculus or quantum calculus is an old subject that was initially developed by Jackson [1], basic definitions and properties of q-calculus can be found in [2]. The fractional q-calculus had its origin in the works by Al-Salam [3] and Agarwal [4]. In recent years, considerable interest in q-fractional differential equations has been stimulated due to its applicability in mathematical modeling in different branches like engineering, physics and technical, etc. There are many papers and books dealing with the theoretical development of q-fractional calcaulus and the existence of solutions of boundary value problems for nonlinear q-fractional differential equations, for examples and details, one can see [5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22] and references therein.
In [9], Zhao, Chen and Zhang considered the following nonlocal q-integral boundary value problem of nonlinear fractional q-derivatives equation:
{Dαqx(t)+f(t,x(t))=0,t∈(0,1),x(0)=0,x(1)=μIβqx(η)=μ∫η0(η−qs)(β−1)Γq(β)x(s)dqs, |
where q∈(0,1),1<α≤2,0<β≤2,0<η<1 and μ>0. Dαq is the fractional q-derivative of Riemann-Liouville type of order α. By using the the generalized Banach contraction principle, the monotone iterative method, and Krasnoselskiis fixed point theorem, the authors obtained some existence results of positive solutions to the above problem.
In [10], the authors investigated the q-integral boundary value problem for q-integro-difference equations involving Riemann-Liouville q-derivatives and a q-integral of different orders as follows:
{(λDαq+(1−λ)Dβq)x(t)=af(t,x(t))+bIδqg(t,x(t)),t∈[0,1],a,b∈R+,μ∫10(1−qs)(γ1−1)Γq(γ1)x(s)dqs+(1−μ)∫10(1−qs)(γ2−1)Γq(γ2)x(s)dqs,x(0)=0, |
where, q∈(0,1),1<α,β<2,0<δ<1,0<λ≤1 and 0≤μ≤1,α−β>1. Dαq denotes the Riemann-Liouville fractional q-derivative of order α and f,g:[0,1]×R→R are continuous functions.
In [23], the authors considered the existence of solutions for the following nonlinear Riemann-Liouville fractional differential equation with nonlocal Erdélyi-Kober fractional integral conditions
{(λDqx(t)=f(t,x(t)),t∈(0,T),,x(0)=0,αx(T)=∑mi=1βiIγi,δiηix(ξi), |
where 1<q≤2,Dq is the Riemann-Liouville fractional derivative of order q, Iγi,δiηi is the Erdélyi-Kober fractional integral of order δi>0 with ηi>0 and γi∈R,i=1,2,⋯,m,f:[0,T]×R→R is a continuous function and αi,βi∈R,ξi∈(0,T),i=1,2,⋯,m are given constants.
As we all know, few people solve the existence of solutions for a nonlinear Riemann-Liouville q-fractional differential equation subject to nonlocal Erdélyi-Kober q-fractional integral conditions. Inspired by the paper [23], we consider the existence and uniqueness for problem (1.1) by using Banach contraction principle and Schauder's fixed point theorem.
Here we recall some definitions and fundamental results on fractional q-integral and fractional q-derivative. See the references [4,5,6,7] for complete theory.
For q∈(0,1), define [a]q=1−qa1−q,a∈R. The q-factorial function is defined as (a−b)(n)=n−1∏k=0(a−bqk),a,b∈R, If n is a positive integer. If ν is not a positive integer, then (a−b)(ν)=aν∞∏n=0a−bqna−bqν+n. If b=0, then a(ν)=aν. The q-gamma function is defined by Γq(α)=(1−q)(α−1)(1−q)α−1,α>0, and satisfies Γq(α+1)=[α]qΓq(α).
The q-derivative of a function f is defined by (Dqf)(t)=f(t)−f(qt))(1−q)t,(Dqf)(0)=limt→0(Dqf)(t). The q-integral of a function f defined on the interval [0,b] is given by (Iqf(t)=∫t0f(s)dqs=(1−q)t∞∑i=0qif(qit),t∈[0,b].
Some results about operator Dq and Iq can be found in references [4]. Let us define fractional q-derivative and q-integral and outline some of their properties [4,6,8].
Definition 1 ([4]) Let α≥0 and f be a function. The fractional q-integral of Riemann-Liouville type is given by (I0qf)(t)=f(t) and
(Iαqf)(t)=1Γq(α)∫t0(t−qs)(α−1)f(s)dqs,α>0,t∈[0,b]. |
Definition 2 ([6]) The fractional q-derivative fractional of Riemann-Liouville type of order ν≥0 is defined by D0qf(t)=f(t) and
Dνqf(t)=DlqIl−νqf(t),ν>0, |
where l is the smallest integer greater than or equal to ν.
Definition 3 ([24]) For 0<q<1, the Erdélyi-Kober fractional q-integral of order μ>0 with β>0 and η∈R of a continuous function f:(0,∞)→R is defined by
Iη,μ,βqf(t)=βt−β(η+μ)Γq(μ)∫t0(tβ−sβq)(μ−1)sηf(s)dqs. |
provided the right side is pointwise defined on R+.
Remark 1 For β=1 the above operator is reduced to the q-analogue Kober operator
Iη,μqf(t)=t−(η+μ)Γq(μ)∫t0(t−sq)(μ−1)sηf(s)dqs |
that is given in [4]. For η=0 the q-analogue Kober operator is reduced to the Riemann-Liouville fractional q-integral with a power weight:
Iμqf(t)=t−μΓq(μ)∫t0(t−sq)(μ−1)f(s)dqs,μ>0. |
Lemma 1 ([4]) Let α,β∈R+ and f be a continuous function on [0,b]. The Riemann-Liouville fractional q-integral has the following semi-group property
IβqIαqf(t)=IαqIβqf(t)=Iα+βqf(t). |
Lemma 2 ([8]) Let f be a q-integrable function on [0,b]. Then the following equality holds
DαqIαqf(t)=f(t),forα>0,t∈[0,b]. |
Lemma 3 ([4]) Let α>0 and p be a positive integer. Then for t∈[0,b] the following equality holds
IαqDpqf(t)=DpqIαqf(t)−p−1∑k=0tα−p+kΓq(α+k−p+1)Dkqf(0). |
Lemma 4 ([24]) For f(t)=tλ and β>0,μ>0,η,λ∈R,0<q<1, then
Iη,μ,βqtλ=β[1β]qΓq(η+1+λβ)Γq(μ+η+1+λβ)tλ. |
In this section, we will give the main results of this paper. Let the space E={x∈C([0,T],R),Dδqx∈C([0,T],R)} be endowed with the norm ‖x‖=maxt∈[0,T]|x(t)|+maxt∈[0,T]|Dδqx(t)|. It is known that the space E is a Banach space. To obtain our main results, we need the following lemma.
Lemma 5 Let h(t)∈C([0,T],R). Then for any t∈[0,T], the solution of the following problem
{Dαqx(t)+h(t)=0,t∈(0,T),x(0)=0,ax(T)=n∑i=1λiIηi,μi,βiqx(ξi). | (3.1) |
is given by
x(t)=−Iαqh(t)+tα−1M(aIαqh(T)−n∑i=1λiIηi,μi,βiqIαqh(ξi)), | (3.2) |
where M=aTα−1−n∑i=1λiIηi,μi,βiqξα−1i=aTα−1−n∑i=1λiβi[1βi]qΓq(ηi+1+α−1βi)Γq(μi+ηi+1+α−1βi)ξα−1i≠0.
Proof. Applying the operator Iαq on both sides of the first equation of (3.1) for t∈(0,T) and using Lemma 1 and Lemma 2, we have
x(t)=−Iαqh(t)+c1tα−1+c2tα−2. | (3.3) |
Applying the initial value condition x(0)=0, we get c2=0. By the boundary value condition, we have
−n∑i=1λiIηi,μi,βiqIαqh(ξi)+c1n∑i=1λiIηi,μi,βiqξα−1i=−aIαqh(T)+c1aTα−1, |
that is
c1=aIαqh(T)−n∑i=1λiIηi,μi,βiqIαqh(ξi)aTα−1−n∑i=1λiIηi,μi,βiqIαqξα−1i=aIαqh(T)−n∑i=1λiIηi,μi,βiqIαqh(ξi)M. |
Substituting c1,c2 to (3.3), we obtain the solution (3.2). This completes the proof.
Using the Lemma 5, we can define an operator Q:E→E as follows:
Qx(t)=−Iαqf(s,x(s),Dδqx(s))(t)+tα−1M(aIα−1qf(s,x(s),Dρqx(s))(T)−n∑i=1λiIηi,μi,βiqIαqf(s,x(s),Dδqx(s))(ξi)), | (3.4) |
where
Iαqf(s,x(s),Dδqx(s))(τ)=1Γq(α)∫τ0(τ−qs)(α−1)f(s,x(s),Dδqx(s))dqs |
and τ∈{t,T,ξ1,ξ2⋯,ξn}. Then, the existence of solutions of system (1.1) is equivalent to the problem of fixed point of operator Q in (3.4).
In the following, we will use some classical fixed point techniques to give our main results.
Theorem 1 Suppose that there exists a function L(t):[0,T]→R+ q-integrable such that
|f(t,x,y)−f(t,˜x,˜y)|≤L(t)(|x−˜x|+|y−˜y|), |
for each x,˜x,y,˜y∈R. Then problem (1.1) has an unique solution on [0,T] if
L1+L3+Tα−1|M|(1+T−δΓq(α)Γq(α−δ))(|a|L2+n∑i=0|λi|βi[1βi]qL1Γq(ηi+1)Γq(μi+ηi+1))<1, | (3.5) |
where L1=supt∈[0,T]IαqL(t),L2=supt∈[0,T]Iα−1qL(t),L3=supt∈[0,T]Iα−δqL(t).
Proof. The conclusion will follow once we have shown that the operator Q defined (3.4) is contractively with respect to a suitable norm on E.
For any functions x,y∈E, we have
|(Qx)(t)−(Qy)(t)|≤|1Γq(α)∫t0(t−qs)(α−1)(f(s,x(s),Dδqx(s))−f(s,y(s),Dδqy(s))dqs|+tα−1M(||a|Γq(α−1)∫T0(T−qs)(α−2)(f(s,x(s),Dδqx(s))−f(s,y(s),Dδqy(s))dqs|+n∑i=0|λi||βiξ−βi(ηi+μi)iΓq(μi)∫ξi0(ξβii−sβiq)(μi−1)sβi(ηi+1)−11Γq(α)∫s0(s−qτ)(α−1)(f(τ,x(τ),Dδqx(τ))−f(τ,y(τ),Dδqy(τ))dqτdqs|)≤∥x−y∥Γq(α)∫t0(t−qs)(α−1)L(s)dqs+Tα−1M(|a|Γq(α−1)∫T0(T−qs)(α−2)L(s)dqs+n∑i=0|λi||βiξ−βi(ηi+μi)iΓq(μi)Γq(α)∫ξi0(ξβii−sβiq)(μi−1)sβi(ηi+1)−1∫s0(s−qτ)(α−1)L(τ)dqτdqs)∥x−y∥≤∥x−y∥(L1+Tα−1|M|(|a|L2+L1n∑i=0|λi||βiξ−βi(ηi+μi)iΓq(μi)∫ξi0(ξβii−sβiq)(μi−1)sβi(ηi+1)−1dqs))=(L1+Tα−1|M|(|a|L2+L1n∑i=0|λi|βi[1βi]qΓq(ηi+1)Γq(μi+ηi+1))∥x−y∥. |
on the other hand
Dδq(Qx)(t)=−DδqIαqf(s,x(s),Dδqx(s))(t)+1M(aIα−1qf(s,x(s),Dδqx(s))(T)−n∑i=1λiIηi,μi,βiqIαqf(s,x(s),Dδqx(s))(ξi))Dδqtα−1=−DρqIδqIα−δqf(s,x(s),Dδqx(s))(t)+1M(aIα−1qf(s,x(s),Dδqx(s))(T)−n∑i=1λiIηi,μi,βiqIαqf(s,x(s),Dρqx(s))(ξi))Γq(α)Γq(α−δ)tα−1−δ=−Iα−δqf(s,x(s),Dδqx(s))(t)+1M(aIα−1qf(s,x(s),Dδqx(s))(T)−n∑i=1λiIηi,μi,βiqIαqf(s,x(s),Dδqx(s))(ξi))Γq(α)Γq(α−δ)tα−1−δ. |
Thus
|Dδq(Qx)(t)−Dδq(Qy)(t)|≤|Iα−δq(f(s,x(s),Dδqx(s))(t)−f(s,y(s),Dδqy(s)))(t)|+Γq(α)tα−1−δ|M|Γq(α−δ)(|aIα−1q(f(s,x(s),Dδqx(s))(T)−f(s,y(s),Dδqy(s)))(T)|+n∑i=1|λi||Iηi,μi,βiqIαq((f(s,x(s),Dρqx(s))−f(s,y(s),Dδqy(s)))(ξi))|≤Iα−δqL(s)(t)+Γq(α)Tα−1−δ|M|Γq(α−δ)(|a|Iα−1qL(s)(T)+n∑i=1λiIηi,μi,βiqIαqL(τ)(ξi))≤(L3+Γq(α)Tα−1−δ|M|Γq(α−δ)(|a|L2+n∑i=0|λi|βi[1βi]qL1Γq(ηi+1)Γq(μi+ηi+1)))∥x−y∥, |
which implies that
∥Qx−Qy∥≤{L1+L3+Tα−1|M|(1+T−δΓq(α)Γq(α−δ))(|a|L2+n∑i=0|λi|βi[1βi]qL1Γq(ηi+1)Γq(μi+ηi+1))}∥x−y∥. |
Thus the operator Q is a contraction in view of the condition (3.5). By Banach's contraction mapping principle, the problem (1.1) has an unique solution on [0,T]. This completes the proof.
Corollary 1 Assume that there exists L0>0 such that
|f(t,x,y)−f(t,˜x,˜y)|≤L0(|x−˜x|+|y−˜y|), |
for each t∈[0,T] and x,˜x,y,˜y∈R. Then the problem (1.1) has an unique solution whenever
(TαΓq(α+1)+Tα−δ+1Γq(α−δ+1)+|a||M|(T2α−2Γqα+T2α−2Γq(α−δ))+1|M|(Tα−1−δ[α]qΓq(α−δ)+Tα−1Γq(α+1))n∑i=1|λi|Iηi,μi,ξiqsα(ξi))L0<1, |
where Iηi,μi,ξiqsα(ξi)=βi[1βi]qΓq(ηi+1+α−1βi)Γq(μi+ηi+1+α−1βi)ξαi.
In the following Theorem, the existence results for nontrivial solution for problem (1.1) are presented. For convenience, we denote
ζ=n∑i=1|λi|Iηi,μi,ξiq1(ξi)=n∑i=1|λi|βi[1βi]qΓq(ηi+1)Γq(μi+ηi+1), |
ϱi=maxt∈[0,T]1Γq(α)∫t0(t−qs)(α−1)li(s)dqs,i=1,2,3, |
σi=maxt∈[0,T]1Γq(α−1)∫t0(t−qs)(α−2)li(s)dqs,i=1,2,3, |
ςi=maxt∈[0,T]1Γq(α−δ)∫t0(t−qs)(α−δ−1)li(s)dqs,i=1,2,3, |
where li(t),i=1,2,3 are defined in Theorem 2.
Theorem 2 Let f:[0,T]×R×R→R be a continuous function. Assume there exist three nonnegative continuous functions li(t),i=1,2,3 such that
|f(t,x(t),Dδqx(t))|≤l1(t)+l2(t)|x(t)|r1+l3(t)|Dδqx(t)|r2,0<ri<1,i=1,2, |
and f(t,0,0)≠0 for t∈[0,T]. Then the problem (1.1) has a nontrivial solution.
Proof. We shall use Schauder's fixed point theorem to prove our theorem. Define Ed={x:x∈E,∥x∥≤d}, where d≥max{3(ς1+|a|σ1ρ+ϱ1(1+ρ)ζ),3(ς2+|a|σ2ρ+ϱ2(1+ρ)ζ)11−r1,3(ς3+|a|σ3ρ+ϱ3(1+ρ)ζ)11−r2} and ρ=Tα−1|M|+Tα−δ−1|M|Γq(α)Γq(α−δ−1). Note that Ed is a closed, bounded and convex subset of the Banach space E. We now show that Q:Ed→Ed. In fact, for x∈Ed we have that
|x(t)|≤maxt∈[0,T]|x(t)|≤∥x∥≤d, |
|Dρqx(t)|≤maxt∈[0,T]|Dρqx(t)|≤∥x∥≤d, |
which implies
|f(t,x(t),Dδqx(t)|≤l1(t)+l2(t)dr1+l3(t)dr2. |
Thus
|Qx(t)|≤1Γq(α)∫t0(t−qs)(α−1)(l1(s)+l2(s)dr1+l3(s)dr3dqs+tα−1M(|a|Γq(α−1)∫T0(T−qs)(α−2)(l1(s)+l2(s)dr1+l3(s)dr3dqs+n∑i=1|λi|βiξ−βi(ηi+μi)iΓq(μi)∫ξi0(ξβii−sβiq)(μi−1)sβ(ηi+1)−11Γq(α)∫s0(s−qτ)(α−1)(l1(τ)+l2(τ)dr1+l3(τ)dr3)dqτdqs≤(ϱ1+ϱ2dr1+ϱ3dr2)(1+ζ)Tα−1|M|+Tα−1|a||M|(σ1+σ2dr1+σ3dr2). |
|DρqQx(t)|≤[(ϱ1+ϱ2dr1+ϱ3dr2)ζ+|a|(σ1+σ2dr1+σ3dr2)]Tα−δ−1|M|Γq(α)Γq(α−δ)+(ς1+ς2dr1+ς3dr2). |
From the two inequalities above, we get
∥Qx∥=maxt∈[0,T]|x(t)|+maxt∈[0,T]|Dδqx(t)|≤(ς1+|a|σ1ρ+ϱ1(1+ρ)ζ)+(ς2+|a|σ2ρ+ϱ2(1+ρ)ζ)dr1+(ς3+|a|σ3ρ+ϱ3(1+ρ)ζ)dr2≤d3+d3+d3=d. |
Hence, Q maps Ed into Ed. Also, it is easy to check that Q is continuous, since f is continuous. For each x∈Ed and each 0<t1<t2<T, we have
|(Qx)(t2)−(Qx)(t1)|≤|1Γq(α)∫t10[(t2−qs)(α−1)−(t1−qs)(α−1)]f(s,x(s),Dδqx(s))dqs|+|1Γq(α)∫t2t1(t2−qs)(α−1)f(s,x(s),Dδqx(s))dqs|+|tα−12−tα−11M(||a|Iα−1qf(s,x(s),Dδqx(s))(T)+n∑i=1|λi|Iηi,μi,βiqIαqf(s,x(s),Dδqx(s))(ξi))|. |
|(DρqQx)(t2)−(DδqQx)(t1)|≤|Iα−δqf(s,x(s),Dδqx(s))(t2)−Iα−δqf(s,x(s),Dδqx(s))(t1)|+|1M(aIα−1qf(s,x(s),Dδqx(s))(T)−n∑i=1λiIηi,μi,βiqIαqf(s,x(s),Dδqx(s))(ξi))Γq(α)Γq(α−δ)(tα−1−δ2−tα−1−δ1)|≤|1Γq(α−δ)∫t10[(t2−qs)(α−δ−1)−(t1−qs)(α−δ−1)]f(s,x(s),Dδqx(s))dqs|+|1Γq(α)∫t2t1(t2−qs)(α−1−δ)f(s,x(s),Dδqx(s))dqs|+|tα−12−tα−1−δ1MΓq(α)Γq(α−δ)(||a|Iα−1qf(s,x(s),Dδqx(s))(T)+n∑i=1|λi|Iηi,μi,βiqIαqf(s,x(s),Dδqx(s))(ξi))|. |
Let t2→t1, we get ∥Qx(t2)−Qx(t2)∥→0. Thus, Q is uniformly bounded and equicontinuous. The theorem of Arzelá-Ascoli implies that Q is completely continuous. By Schauder's fixed point theorem, Q has a fixed point in Ed. Clearly x=0 is not a fixed point because f(t,0,0)≠0 for t∈[0,T]. Hence, the problem (1.1) has at least one nontrivial solution. This proves the theorem.
Remark 2 In the Theorem 2, if ri>1,i=1,2, we may choose l2(t),l3(t) and d such that
|f(t,x(t),Dδqx(t)|≤l2(t)|x(t)|r1+l3(t)|Dδqx(t)|r2, |
and
0<d≤min{(12(ς2+|a|σ2ρ+ϱ2(1+ρ)ζ))1r1−1,(12(ς3+|a|σ3ρ+ϱ3(1+ρ)ζ))1r2−1}. |
For ri=1,i=1,2, we have the following theorem.
Theorem 3 Let f:[0,T]×R×R→R be a continuous function. Assume there exist three nonnegative continuous functions li(t),i=1,2,3 such that
|f(t,x(t),Dδqx(t))|≤l1(t)+l2(t)|x(t)|+l3(t)|Dδqx(t)|, |
and max{ς2+|a|σ2ρ+ϱ2(1+ρ)ζ),(ς3+|a|σ3ρ+ϱ3(1+ρ)ζ)}<13. Further, assume that f(t,0,0)≠0 for t∈[0,T]. Then the problem (1.1) has a nontrivial solution.
Proof. Let d>3(ς1+|a|σ1ρ+ϱ1(1+ρ)ζ), The proof is similar to Theorem 2, so it is omitted. This completes the proof.
Although Theorems 2 and Theorem 3 provide some simple conditions on the existence of solution of problem (1.1) and Theorem 1 provides a condition on the existence and uniqueness on the solution of problem (1.1), the following theorem provides an easily verifiable condition for the existence of a nontrivial solution for the problems (1.1).
Theorem 4 Assume that f:[0,T]×R×R→R with f(t,0,0)≠0 for t∈[0,T] and x∈E. Suppose that
lim∥x∥→∞maxt∈[0,T]|f(t,x(t),Dδqx(t))|∥x∥=0 | (3.6) |
holds. Then problem (1.1) has at least one nontrivial solution.
Proof. Choose a constant A such that
A(TαΓq(α+1)+|a|T2α−2|M|Γq(α)+Tα−1κ|M|Γq(α+1)+Tα−δΓq(α−δ+1)+|a|T2α−2−δ|M|Γq(α−δ)+Tα−1−δκ|M|[α]qΓq(α−δ))<1, |
where κ=n∑i=1|λi|βi[1βi]qΓq(ηi+1+αβi)Γq(μi+1+αβi)ξαi.
By the condition (3.6), there exists a constant c1 such that
|f(t,x(t),Dδqx(t))|<A∥x∥for any t∈[0,T]and∥x∥≥c1. |
Since f:[0,T]×R×R→R, we can find another constant A1>0 such that |f(t,x(t),Dδqx(t))|<A1, for t∈[0,T] and ∥x∥≤c1. Let c=max{A1A,c1}, then for any ∥x∥≤c, we have |f(t,x(t),Dδqx(t))|<Ac. Set
Ec={x∈E:∥x∥≤c}. |
Then for any x∈Ec, we have
|Qx(t)|≤1Γq(α)∫t0(t−qs)(α−1)Acdqs+tα−1M(|a|Γq(α−1)∫T0(T−qs)(α−2)Acdqs+n∑i=1|λi|βiξ−βi(ηi+μi)iΓq(μi)∫ξi0(ξβii−sβiq)(μi−1)sβ(ηi+1)−11Γq(α)∫s0(s−qτ)(α−1)Acdqτdqs≤(TαΓq(α+1)+Tα−1|M|(Tα−1|a|Γq(α)+κΓq(α+1)))Ac. | (3.7) |
|Dρq(Qx)(t)|≤1Γq(α−δ)∫t0(t−qs)(α−δ−1)Acdqs+Γq(α)Tα−δ−1|M|Γq(α−δ)(|a|Γq(α−1)∫T0(T−qs)(α−2)Acdqs+n∑i=1|λi|βiξ−βi(ηi+μi)iΓq(μi)∫ξi0(ξβii−sβiq)(μi−1)sβ(ηi+1)−11Γq(α)∫s0(s−qτ)(α−1)Acdqτdqs)=(Tα−δΓq(α−δ+1)+|a|T2α−2−δ|M|Γq(α−δ)+Tα−1−δκ|M|[α]qΓq(α−δ))Ac. | (3.8) |
Thus
‖Qx‖=maxt∈[0,T]|Qx(t)|+maxt∈[0,T]|DδqQx(t)|≤(TαΓq(α+1)+Tα−1|M|(Tα−1|a|Γq(α)+κΓq(α+1)))Ac+(Tα−δΓq(α−δ+1)+|a|T2α−2−δ|M|Γq(α−δ)+Tα−1−ρκ|M|[α]qΓq(α−δ))Ac=A(TαΓq(α+1)+|a|T2α−2|M|Γq(α)+Tα−1κ|M|Γq(α+1)+Tα−δΓq(α−δ+1)+|a|T2α−2−δ|M|Γq(α−δ)+Tα−1−δκ|M|[α]qΓq(α−δ))c<c. | (3.9) |
From (3.9), we obtain Q(Ec)⊂Ec. By Schauder fixed point theorem, Q has at least one fixed point in Ec. Clearly, x=0 is not a fixed point because f(t,0,0)≠0. Therefore, problem (1.1) has at least one nontrivial solution, which completes the proof.
In this section, we illustrate the results obtained in the last section.
Example1 Consider the following fractional-order boundary value problem involving nonlocal Erdélyi-Kober fractional q-integral conditions:
{D3212x(t)+t21+et(|x(t)+D1412x(t)|1+2|x(t)+D1412x(t)|+cost+2)+1=0,x(0)=0,5x(1)=1100I38,54,11012x(14)+3100I18,74,1512x(12), | (4.1) |
where q=12,δ=14,T=1,α=32,a=3,λ1=1100,λ2=3100,β1=110,β2=15,η1=38,η2=18,ξ1=14,ξ2=12,μ1=54,μ1=74, and f(t,,x(t),Dδqx(t))=t21+et(|x(t)+D1212x(t)|1+2|x(t)+D1212x(t)|+cost+2)+1.
By computation, we deduce that
|f(t,,x(t),Dδqx(t))−f(t,,y(t),Dρqy(t))|≤t22(|x(t)−y(t)|+|D1412x(t)−D1412y(t)|), |
then, the first condition is satisfied with L(t)=t22.
M=5−1100×110[10]qΓ12(38+1+302)Γ12(54+38+1+302)−3100×15[5]qΓ12(18+1+152)Γ12(74+18+1+152)>5−1100×15(1−(12)10)(14)12−3100×25(1−(12)5)(12)12>5−1500−6500≐4.986≠0. |
L1=supt∈[0,1]1Γq(32)∫t0(t−qs)(32−1)s22dqs=12Γq(3)Γq(4.5). |
L2=supt∈[0,1]1Γq(32−1)∫t0(t−qs)(32−2)s22dqs=12Γq(3)Γq(3.5). |
L3=supt∈[0,1]1Γq(32−14)∫t0(t−qs)(32−14−1)s22dqs=12Γq(3)Γq(4.25). |
L1+L3+Tα−1|M|(1+T−ρΓq(α)Γq(α−ρ))(|a|L2+n∑i=0|λi|βi[1βi]qL1Γq(ηi+1)Γq(μi+ηi+1))≤12Γq(3)Γq(4.5)+12Γq(3)Γq(4.25)+14.986(52Γq(3)Γq(3.5)+1100×110×12[10]qΓq(3)Γq(4.5)+3100×15×12Γq(3)Γq(4.5)+52Γq(32)Γq(3)Γq(54)Γq(3.5)+1100×110×12[10]qΓq(32)Γq(3)Γq(54)Γq(3.5)+3100×15×12[5]qΓq(32)Γq(3)Γq(54)Γq(3.5))≈0.894875<1. |
Hence, by Theorem 1, the boundary value problem (1.1) has an unique solution on [0, 1].
Example2 Consider the following fractional-order boundary value problem involving nonlocal Erdélyi-Kober fractional q-integral conditions:
{D75qx(t)+12πsin(π|x|)(|x|+|Dδqx|)12|x|+|Dδqx|+1+1=0,t∈(0,1)x(0)=0,5x(1)=17I13,54,110qx(14)+310I18,74,15qx(12). |
Here, q=12,δ=14. f(t,x(t),Dρqx(t))=12πsin(π|x|)(|x|+|Dδqx|)12|x|+|Dδqx|+1+1,
|f(t,x(t),Dδqx(t))|∥x∥=|12πsin(π|x|)(|x|+|Dδqx|)12|x|+|Dδqx|+1+1|∥x∥≤12(|x|+|Dδqx|)12+1∥x∥→0,as∥x∥→∞. |
Therefore, the conclusion of Theorem 4 implies that problem (1.1) has at least one solution on [0, 1].
In this work, we utilize Banach contraction principle and Schauder's fixed point theorem to research the existence, uniqueness of solutions for a q-fractional differential equation with nonlocal Erdélyi-Kober q-fractional integral condition and in which the nonlinear term contains a fractional q-derivative of Rieman-Liouville type. Some existence and uniqueness results of solutions are obtained, we also provide an easily verifiable condition for the existence of nontrivial solution for the problem (1.1).
This research was Supported by Science and Technology Foundation of Guizhou Province (Grant No. [2016]7075, [2019]1162), by the Project for Young Talents Growth of Guizhou Provincial Department of Education under(Grant No. Ky[2017]133), and by the project of Guizhou Minzu University under (Grant No.16yjrcxm002).
The authors declare no conflict of interest.
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