Home Positive solutions for boundary value problems of a class of second-order differential equation system
Article Open Access

Positive solutions for boundary value problems of a class of second-order differential equation system

  • Dan Wang , Yongxiang Li EMAIL logo and Yi Su
Published/Copyright: May 26, 2023

Abstract

This article discusses the existence of positive solutions for the system of second-order ordinary differential equation boundary value problems

u ( t ) = f ( t , u ( t ) , v ( t ) , u ( t ) ) , t [ 0 , 1 ] , v ( t ) = g ( t , u ( t ) , v ( t ) , v ( t ) ) , t [ 0 , 1 ] , u ( 0 ) = u ( 1 ) = 0 , v ( 0 ) = v ( 1 ) = 0 ,

where f , g : [ 0 , 1 ] × R + × R + × R R + are continuous. Under the related conditions that the nonlinear terms f ( t , x , y , p ) and g ( t , x , y , q ) may be super-linear growth or sub-linear growth on x , y , p , and q , we obtain the existence results of positive solutions. For the super-linear growth case, the Nagumo condition ( F 3 ) is presented to restrict the growth of f ( t , x , y , p ) and g ( t , x , y , q ) on p and q . The super-linear growth or sub-linear growth of the nonlinear terms f and g is described by related inequality conditions instead of the usual independent inequality conditions about f and g . The discussion is based on the fixed point index theory in cones.

MSC 2010: 34A34; 34B18; 47H11

1 Introduction

This article discusses the existence of positive solutions for the boundary value problem (BVP) of second-order ordinary differential equation system

(1.1) u ( t ) = f ( t , u ( t ) , v ( t ) , u ( t ) ) , t [ 0 , 1 ] , v ( t ) = g ( t , u ( t ) , v ( t ) , v ( t ) ) , t [ 0 , 1 ] , u ( 0 ) = u ( 1 ) = 0 , v ( 0 ) = v ( 1 ) = 0 ,

where f , g : [ 0 , 1 ] × R + × R + × R R + are continuous, R + = [ 0 , + ) . This problem has an important application background in the fields of fluid dynamics and physics; many authors have studied some special cases where the nonlinear terms do not contain derivative terms (see [121]).

In [5], Yang and Sun studied the BVP:

(1.2) u ( t ) = f ( t , v ( t ) ) , t [ 0 , 1 ] , v ( t ) = g ( t , u ( t ) ) , t [ 0 , 1 ] , u ( 0 ) = u ( 1 ) = 0 , v ( 0 ) = v ( 1 ) = 0 .

In the case of the nonlinear terms f and g are non-negative, the existence of the positive solution is obtained under super-linear conditions or sub-linear conditions.

For the special case of BVP (1.1) that the nonlinear terms f and g does not contain derivative terms u and v , namely, BVP

(1.3) u ( t ) = f ( t , u ( t ) , v ( t ) ) , t [ 0 , 1 ] , v ( t ) = g ( t , u ( t ) , v ( t ) ) , t [ 0 , 1 ] , u ( 0 ) = u ( 1 ) = 0 , v ( 0 ) = v ( 1 ) = 0 .

There have been many meaningful results (see [3,7,9]). In [7,9], Cheng established the product formula of fixed point index on product cone, under conditions (H1) and (H2), the existence results of positive solutions for BVP (1.3) are obtained.

(H1) lim u 0 + sup max t I f ( t , u , v ) u < λ 1 < lim u + inf min t I f ( t , u , v ) u ,

(H2) lim v 0 + inf min t I g ( t , u , v ) v > λ 1 < lim v + sup max t I g ( t , u , v ) v ,

where λ 1 is the first eigenvalue of the corresponding linear eigenvalue problem, for BVP (1.3), λ 1 = π 2 . Condition (H1) represents that f ( t , u , v ) is the super-linear growth on u , and condition (H2) represents that g ( t , u , v ) is the sub-linear growth on v . The aforementioned article discusses the existence of positive solutions for the equation system of which the nonlinear terms do not contain derivative terms u and v , and the inequality conditions for the nonlinear terms f and g are independent.

Inspired by the aforementioned article, we extend the fixed point index theory on the cone to the product space in this article. Under the related inequality conditions that the nonlinear terms f ( t , x , y , p ) and g ( t , x , y , q ) may be super-linear growth or sub-linear growth on x , y , p , and q , we obtain the existence results of positive solution for BVP (1.1), and we need that f ( t , x , y , p ) and g ( t , x , y , q ) satisfy the Nagumo condition on p and q .

The existence conditions of positive solutions proposed in this article correlate the two nonlinear terms, rather than separate assumptions for the two nonlinear terms, referring to the existing results. The results of this article better reflect the property of the equation system, which is the promotion of the previous literature.

The proof of main theorems is based on the fixed point index theory on the cone, which will be given in Section 3. Some preliminaries are presented in Section 2.

2 Preliminaries

Let I = [ 0 , 1 ] . C ( I ) denote the Banach space of all continuous function on I with norm u C = max t I u ( t ) . For all n N , C n ( I ) denote the Banach space of all n-order continuous differentiable function on I with norm u C n = max t I { u C , u C u n C } . L 2 ( I ) denote the Hilbert space composed of all Lebesgue square integrable functions on I with inner product ( u , v ) = 0 1 u ( t ) v ( t ) d t , and its inner product norm is u 2 = ( 0 1 u ( t ) 2 d t ) 1 2 . Let H 1 ( I ) = { u C ( I ) : u be absolutely continuous on I , and u L 2 ( I ) } .

Let X and Y be Banach spaces with norms X , Y , respectively. X × Y represents the product space of X and Y and forms Banach spaces with norm ( x , y ) = max { x X , y Y } .

Given h C ( I ) , we consider the linear boundary value problem (LBVP)

(2.1) u ( t ) = h ( t ) , t I , u ( 0 ) = u ( 1 ) = 0 .

It is well known that LBVP (2.1) has a unique solution expressed by:

u = S h C 2 ( I ) ,

where the solution operator S : C ( I ) C 1 ( I ) is a completely continuous linear operator.

Lemma 2.1

[22] Let h L 2 ( I ) . Then, the solution u = S h H 2 ( I ) of LBVP (2.1) satisfies u 2 1 π u 2 , u 2 1 π u 2 .

Lemma 2.2

[13] Let h C + ( I ) . Then, the solution u = S h of LBVP (2.1) has the following properties:

  1. u ( t ) t ( 1 t ) u C for all t I ;

  2. u C π 3 4 0 1 u ( t ) sin π t d t ;

  3. u C u C , and u C 1 = u C ;

  4. there exists a constant ξ ( 0 , 1 ) such that u ( ξ ) = 0 , u ( t ) 0 for all t [ 0 , ξ ) , and u ( t ) 0 for all t ( ξ , 1 ] . Moreover, u C = max { u ( 0 ) , u ( 1 ) } .

For every ( h 1 , h 2 ) C ( I ) × C ( I ) , we consider the corresponding LBVP

(2.2) u ( t ) = h 1 ( t ) , t I , v ( t ) = h 2 ( t ) , t I , u ( 0 ) = u ( 1 ) = 0 , v ( 0 ) = v ( 1 ) = 0 .

We easily see that LBVP (2.2) has a unique solution ( u , v ) = S ( h 1 , h 2 ) C 2 ( I ) × C 2 ( I ) , and the solution operator S : C ( I ) × C ( I ) C 1 ( I ) × C 1 ( I ) is a completely continuous linear operator.

Next, we define a closed convex cone K in E × E = C 1 ( I ) × C 1 ( I ) as follows:

(2.3) K = { ( u , v ) C 1 ( I ) × C 1 ( I ) : u ( t ) t ( 1 t ) u C , v ( t ) t ( 1 t ) v C , t I } ,

then S : C + ( I ) × C + ( I ) K is completely continuous. Define a nonlinear mapping F : K C + ( I ) × C + ( I ) as follows:

F ( u , v ) ( t ) = ( f ( t , u ( t ) , v ( t ) , u ( t ) ) , g ( t , u ( t ) , v ( t ) , v ( t ) ) ) , t I ,

then F : K C + ( I ) × C + ( I ) is continuous and it maps every bounded set in K into a bounded set in C + ( I ) × C + ( I ) . We define a mapping

A = S F : K K .

By the complete continuity of the operator S , A is a completely continuous mapping. According to the definitions of S and K , the positive solution of BVP (1.1) is equivalent to the non-zero fixed point of A .

In order to find the non-zero fixed point of A , we also need the following lemmas (see [23]).

Lemma 2.3

Let Ω be a bounded open subset of E × E with ( θ , θ ) Ω (namely, Ω contains zero elements ( θ , θ ) ), and mapping A : Ω ¯ K K is completely continuous. If A satisfies

μ A ( u , v ) ( u , v ) , for a l l ( u , v ) Ω K , μ ( 0 , 1 ] ,

then, the fixed point index i ( A , Ω K , K ) = 1 on cone K .

Lemma 2.4

Let Ω be a bounded open subset of E × E , and mapping A : Ω ¯ K K are completely continuous. If there exist ( x 0 , y 0 ) K \ { ( θ , θ ) } , such that

( u , v ) A ( u , v ) τ ( x 0 , y 0 ) , f o r a l l ( u , v ) Ω K , τ 0 ,

then, i ( A , Ω K , K ) = 0 .

Lemma 2.5

Let Ω be a bounded open subset of E × E , Ω ¯ K , and mappings A , A 1 : Ω ¯ K K are completely continuous. If A and A 1 satisfy

( 1 s ) A ( u , v ) + s A 1 ( u , v ) ( u , v ) , f o r a l l ( u , v ) Ω K , s [ 0 , 1 ] ,

then i ( A , Ω K , K ) = i ( A 1 , Ω K , K ) .

In the next section, we give the main results and use the three lemmas to prove the main results.

3 Main results

Theorem 3.1

Let f , g : [ 0 , 1 ] × R + × R + × R R + be continuous. If f and g satisfy the following conditions:

( F 1 ) there exist positive constants a, b, c, and d satisfying a + b π 2 + c + d π < 1 and δ > 0 , such that

(3.1) f ( t , x , y , p ) + g ( t , x , y , q ) a x + b y + c p + d q ,

where ( t , x , y ) I × R + × R + , p , q R , ( x , p ) = x 2 + p 2 < δ , ( y , q ) < δ ;

( F 2 ) there exist positive constants e > π 2 and H > 0 , such that

(3.2) f ( t , x , y , p ) + g ( t , x , y , q ) e ( x + y ) ,

where ( t , x , y ) I × R + × R + , p , q R , ( x , p ) > H , ( y , q ) > H ;

( F 3 ) given any M > 0 , there exists a positive continuous function G M : R + R + satisfies

(3.3) 0 + ρ d ρ G M ( ρ ) + 1 = + ,

such that f and g satisfy

(3.4) f ( t , x , y , p ) G M ( p ) , g ( t , x , y , q ) G M ( q ) ,

where ( t , x , y ) I × [ 0 , M ] × [ 0 , M ] , p , q R ;

then BVP (1.1) has at least one positive solution.

Proof

Choose E = C 1 ( I ) , K E × E is a closed convex cone defined by equation (2.3). Let 0 < r < R < + and set

Ω 1 = { ( u , v ) C 1 ( I ) × C 1 ( I ) : ( u , v ) C 1 < r } , Ω 2 = { ( u , v ) C 1 ( I ) × C 1 ( I ) : ( u , v ) C 1 < R } .

We prove that A has a fixed point in ( Ω 2 \ Ω ¯ 1 ) K when r is small enough or R is large enough in two steps.

Step I. We prove that i ( A , Ω 1 K , K ) = 1 when r is sufficiently small. Let r 0 , δ 2 , where δ is the positive constant in condition ( F 1 ) . Applying Lemma 2.3 to A on Ω 1 K , namely,

(3.5) ( u , v ) μ A ( u , v ) , μ ( 0 , 1 ] , ( u , v ) Ω 1 K .

In fact, if (3.5) does not hold, there exists μ 0 ( 0 , 1 ] and ( u 0 , v 0 ) Ω 1 K , such that ( u 0 , v 0 ) = μ 0 A ( u 0 , v 0 ) . Since ( u 0 , v 0 ) = μ 0 A ( u 0 , v 0 ) = μ 0 ( S F ( u 0 , v 0 ) ) = S ( μ 0 F ( u 0 , v 0 ) ) , then by definition of S , ( u 0 , v 0 ) is a solution of LBVP (2.2) for ( h 1 , h 2 ) = μ 0 F ( u 0 , v 0 ) C + ( I ) × C + ( I ) . Hence, ( u 0 , v 0 ) C 2 ( I ) × C 2 ( I ) satisfies the differential equation

(3.6) u 0 ( t ) = μ 0 f ( t , u 0 ( t ) , v 0 ( t ) , u 0 ( t ) ) , t I , v 0 ( t ) = μ 0 g ( t , u 0 ( t ) , v 0 ( t ) , v 0 ( t ) ) , t I , u 0 ( 0 ) = u 0 ( 1 ) = 0 , v 0 ( 0 ) = v 0 ( 1 ) = 0 .

Since ( u 0 , v 0 ) Ω 1 , for all t I , we have

( u 0 ( t ) , v 0 ( t ) ) ( u 0 , v 0 ) C = max { u 0 C , v 0 C } max { u 0 C , v 0 C } = max { u 0 C 1 , v 0 C 1 } = ( u 0 , v 0 ) C 1 < r < δ 2 .

Therefore,

u 0 C < δ 2 , v 0 C < δ 2 .

Since

( u 0 ( t ) , v 0 ( t ) ) ( u 0 , v 0 ) C = max { u 0 C , v 0 C } = max { u 0 C 1 , v 0 C 1 } = ( u 0 , v 0 ) C 1 < r < δ 2 ,

therefore,

u 0 C < δ 2 , v 0 C < δ 2 .

Hence,

( u 0 ( t ) , u 0 ( t ) ) = u 0 C 2 + u 0 C 2 < δ , ( v 0 ( t ) , v 0 ( t ) ) < δ .

By condition ( F 1 ) , for all t I , we have

f ( t , u 0 ( t ) , v 0 ( t ) , u 0 ( t ) ) + g ( t , u 0 ( t ) , v 0 ( t ) , v 0 ( t ) ) a u 0 ( t ) + b v 0 ( t ) + c u 0 ( t ) + d v 0 ( t ) .

Add the first formula of equation (3.6) to the second formula of equation (3.6), from the aforementioned inequality, we can obtain

u 0 ( t ) v 0 ( t ) = μ 0 ( f ( t , u 0 ( t ) , v 0 ( t ) , u 0 ( t ) ) + g ( t , u 0 ( t ) , v 0 ( t ) , v 0 ( t ) ) ) a u 0 ( t ) + b v 0 ( t ) + c u 0 ( t ) + d v 0 ( t ) , t I .

Taking 2 on both sides, we obtain that

u 0 2 + v 0 2 a u 0 2 + b v 0 2 + c u 0 2 + d v 0 2 a + b π 2 + c + d π ( u 0 2 + v 0 2 ) .

Owing to a + b π 2 + c + d π < 1 , therefore u 0 2 + v 0 2 = 0 , namely, u 0 = 0 , v 0 = 0 , this contradicts with ( u 0 , v 0 ) Ω 1 . So (3.5) holds, namely, A satisfies the condition of Lemma 2.3 in Ω 1 K . By Lemma 2.3, we can see

(3.7) i ( A , Ω 1 K , K ) = 1 .

Step II. We prove that i ( A , Ω 2 K , K ) = 0 when R is sufficiently large. Let

e 1 = max { f ( t , x , y , p ) e x : t I , ( x , p ) H } + 1 and e 2 = max { g ( t , x , y , q ) e y : t I , ( y , q ) H } + 1 .

By condition ( F 2 ) , we have

(3.8) f ( t , x , y , p ) + g ( t , x , y , q ) e ( x + y ) ( e 1 + e 2 ) ,

where ( t , x , y ) I × R + × R + , p , q R . Define a nonlinear mapping F 1 : K C + ( I ) × C + ( I ) as follows:

F 1 ( u , v ) ( t ) = ( f ( t , u ( t ) , v ( t ) , u ( t ) ) + e 1 , g ( t , u ( t ) , v ( t ) , v ( t ) ) + e 2 ) F ( u , v ) ( t ) + ( e 1 , e 2 ) , t I ,

and set A 1 = S F 1 , then A 1 : K K is completely continuous.

First, we prove that i ( A 1 , Ω 2 K , K ) = 0 . Choose ( x 0 ( t ) , y 0 ( t ) ) = ( sin π t , sin π t ) . Since ( x 0 ( t ) , y 0 ( t ) ) = ( π 2 sin π t , π 2 sin π t ) = π 2 ( x 0 ( t ) , y 0 ( t ) ) , then by the definition of S , there are ( x 0 , y 0 ) = S ( π 2 ( x 0 , y 0 ) ) K . Now, we show that A 1 satisfies Lemma 2.4, namely,

(3.9) ( u , v ) A 1 ( u , v ) τ ( x 0 , y 0 ) , τ 0 , ( u , v ) Ω 2 K .

In fact, if (3.9) does not hold, there exist τ 0 0 and ( u 1 , v 1 ) Ω 2 K , such that ( u 1 , v 1 ) A 1 ( u 1 , v 1 ) = τ 0 ( x 0 , y 0 ) . Since ( u 1 , v 1 ) = A 1 ( u 1 , v 1 ) + τ 0 ( x 0 , y 0 ) = S ( F 1 ( u 1 , v 1 ) + τ 0 π 2 ( x 0 , y 0 ) ) , then by definition of S , ( u 1 , v 1 ) is the solution of LBVP (2.2) for ( h 1 , h 2 ) = F 1 ( u 1 , v 1 ) + τ 0 π 2 ( x 0 , y 0 ) C + ( I ) × C + ( I ) . Hence, ( u 1 , v 1 ) C 2 ( I ) × C 2 ( I ) satisfies the differential equation

(3.10) u 1 ( t ) = f ( t , u 1 ( t ) , v 1 ( t ) , u 1 ( t ) ) + e 1 + τ 0 π 2 sin π t , t I , v 1 ( t ) = g ( t , u 1 ( t ) , v 1 ( t ) , v 1 ( t ) ) + e 2 + τ 0 π 2 sin π t , t I , u 1 ( 0 ) = u 1 ( 1 ) = 0 , v 1 ( 0 ) = v 1 ( 1 ) = 0 .

Add the first formula of equation (3.10) to the second formula of equation (3.10), from (3.8), we can obtain

u 1 ( t ) v 1 ( t ) = f ( t , u 1 ( t ) , v 1 ( t ) , u 1 ( t ) ) + g ( t , u 1 ( t ) , v 1 ( t ) , v 1 ( t ) ) + e 1 + e 2 + 2 τ 0 π 2 sin π t e ( u 1 ( t ) + v 1 ( t ) ) , t I .

Multiply both sides of the aforementioned inequality by sin π t and integrate on I , we have

π 2 0 1 u 1 ( t ) sin π t d t + 0 1 v 1 ( t ) sin π t d t e 0 1 u 1 ( t ) sin π t d t + 0 1 v 1 ( t ) sin π t d t .

Since 0 1 u 1 ( t ) sin π t d t 4 π 3 u 1 C > 0 , 0 1 v 1 ( t ) sin π t d t 4 π 3 v 1 C > 0 by Lemma 2.2 (2), it follows that π 2 e , this contradicts with e > π 2 . Hence (3.9) holds, namely, A 1 satisfies the condition of Lemma 2.4 in Ω 2 K . By Lemma 2.4, we can see

(3.11) i ( A 1 , Ω 2 K , K ) = 0 .

Second, we show that i ( A , Ω 2 K , K ) = i ( A 1 , Ω 2 K , K ) . When R is sufficiently large, A and A 1 satisfy Lemma 2.5, namely,

(3.12) ( 1 s ) A ( u , v ) + s A 1 ( u , v ) ( u , v ) , ( u , v ) Ω 2 K , s [ 0 , 1 ] .

In fact, if (3.12) does not hold, there exist s 0 [ 0 , 1 ] and ( u 2 , v 2 ) Ω 2 K , such that ( 1 s 0 ) A ( u 2 , v 2 ) + s 0 A 1 ( u 2 , v 2 ) = ( u 2 , v 2 ) . Since ( u 2 , v 2 ) = ( 1 s 0 ) S ( F ( u 2 , v 2 ) ) + s 0 S ( F 1 ( u 2 , v 2 ) ) = S ( ( 1 s 0 ) F ( u 2 , v 2 ) + s 0 F 1 ( u 2 , v 2 ) ) , then by definition of S , ( u 2 , v 2 ) is the solution of LBVP (2.2) for ( h 1 , h 2 ) = ( 1 s 0 ) F ( u 2 , v 2 ) + s 0 F 1 ( u 2 , v 2 ) = F ( u 2 , v 2 ) + s 0 ( e 1 , e 2 ) C + ( I ) × C + ( I ) . Hence, ( u 2 , v 2 ) C 2 ( I ) × C 2 ( I ) satisfies the differential equation

(3.13) u 2 ( t ) = f ( t , u 2 ( t ) , v 2 ( t ) , u 2 ( t ) ) + s 0 e 1 , t I , v 2 ( t ) = g ( t , u 2 ( t ) , v 2 ( t ) , v 2 ( t ) ) + s 0 e 2 , t I , u 2 ( 0 ) = u 2 ( 1 ) = 0 , v 2 ( 0 ) = v 2 ( 1 ) = 0 .

Arguing as before, we have

0 1 ( u 2 ( t ) + v 2 ( t ) ) sin π t d t 2 e 0 π ( e π 2 ) ,

where e 0 = ( 1 s 0 ) ( e 1 + e 2 ) . By Lemma 2.2 (2), we can find

u 2 C + v 2 C π 2 e 0 2 ( e π 2 ) M .

For this M > 0 , by condition ( F 3 ) , there exists a positive continuous function G M on [ 0 , + ) . It satisfies (3.3), such that f and g satisfy (3.4). By (3.3), we have

0 + ρ d ρ G M ( ρ ) + e i = + , i = 1 , 2 .

Hence, there exists M 1 > 0 , such that

(3.14) 0 M 1 ρ d ρ G M ( ρ ) + e i > M , i = 1 , 2 .

By Lemma 2.2 (4), there exists ξ 1 , ξ 2 ( 0 , 1 ) , such that u 2 ( ξ 1 ) = 0 , v 2 ( ξ 2 ) = 0 . We have u 2 ( t ) 0 for all t [ 0 , ξ 1 ) ; u 2 ( t ) 0 for all t ( ξ 1 , 1 ] ; and u 2 C = max { u 2 ( 0 ) , u 2 ( 1 ) } . Similarly, v 2 ( t ) 0 for all t [ 0 , ξ 2 ) ; v 2 ( t ) 0 for all t ( ξ 2 , 1 ] ; and v 2 C = max { v 2 ( 0 ) , v 2 ( 1 ) } . Set u 2 C = u 2 ( 0 ) , v 2 C = v 2 ( 1 ) ; other similar cases can be proved. When t [ 0 , ξ 1 ) , from equation (3.13), we have

u 2 ( t ) = f ( t , u 2 ( t ) , v 2 ( t ) , u 2 ( t ) ) + s 0 e 1 G M ( u 2 ( t ) ) + e 1 , t [ 0 , ξ 1 ) ,

namely,

u 2 ( t ) u 2 ( t ) G M ( u 2 ( t ) ) + e 1 u 2 ( t ) , t [ 0 , ξ 1 ) .

Integrating from 0 to ξ 1 and making the variable transformation ρ = u 2 ( t ) for the left side, we can obtain

0 u 2 C ρ d ρ G M ( ρ ) + e 1 u 2 ( ξ 1 ) u 2 C M .

By (3.14), we have u 2 C M 1 , namely, u 2 C 1 = u 2 C M 1 . Arguing as earlier, we have v 2 C 1 = v 2 C M 1 . Let R > max { r , M 1 } , for every ( u , v ) Ω 2 K , (3.12) holds, namely, A and A 1 satisfy the condition of Lemma 2.5 in Ω 2 K . By Lemma 2.5, we can see

(3.15) i ( A , Ω 2 K , K ) = i ( A 1 , Ω 2 K , K ) = 0 .

Hence, from (3.7) and (3.15), we have

i ( A , ( Ω 2 \ Ω ¯ 1 ) K , K ) = i ( A , Ω 2 K , K ) i ( A , Ω 1 K , K ) = 0 1 = 1 0 .

Thus, A has a non-zero fixed point on ( Ω 2 \ Ω ¯ 1 ) K , which is the positive solution of BVP (1.1).□

The aforementioned conditions ( F 1 ) and ( F 2 ) are super-linear growth conditions of f ( t , x , y , p ) and g ( t , x , y , q ) with respect to x , y , p , and q , but the Nagumo condition ( F 3 ) restricts f ( t , x , y , p ) and g ( t , x , y , q ) on p and q to quadric growth. Next, the sub-linear growth conditions of f ( t , x , y , p ) and g ( t , x , y , q ) with respect to x , y , p , and q are given as follows:

Theorem 3.2

Let f , g : [ 0 , 1 ] × R + × R + × R R + be continuous. If f and g satisfy the following conditions

( F 4 ) there exist positive constants e > π 2 and δ > 0 , such that

(3.16) f ( t , x , y , p ) + g ( t , x , y , q ) e ( x + y ) ,

where ( t , x , y ) I × R + × R + , p , q R , ( x , p ) < δ , ( y , q ) < δ ;

( F 5 ) there exist positive constants a, b, c, and d satisfying a + b π 2 + c + d π < 1 and H > 0 , such that

(3.17) f ( t , x , y , p ) + g ( t , x , y , q ) a x + b y + c p + d q ,

where ( t , x , y ) I × R + × R + , p , q R , ( x , p ) > H , ( y , q ) > H , then BVP (1.1) has at least one positive solution.

Proof

This proof is similar to Theorem 1, and it is also divided into two steps.

Step I. We prove that i ( A , Ω 1 K , K ) = 0 when r is sufficiently small. Applying Lemma 2.4 to A on Ω 1 K .

Step II. We prove that i ( A , Ω 2 K , K ) = 1 when R is sufficiently large. Applying Lemma 2.3 to A on Ω 2 K .

Finally, we have

i ( A , ( Ω 2 \ Ω ¯ 1 ) K , K ) = i ( A , Ω 2 K , K ) i ( A , Ω 1 K , K ) = 1 0 = 1 0 .

Thus, A has a non-zero fixed point on ( Ω 2 \ Ω ¯ 1 ) K , which is the positive solution of BVP (1.1).□

4 Application

Example 4.1

Consider the following BVP:

(4.1) u ( t ) = u α ( t ) + v β ( t ) + u ( t ) γ , t [ 0 , 1 ] , α , β , γ > 1 , v ( t ) = u α ( t ) + v β ( t ) + v ( t ) ε , t [ 0 , 1 ] , α , β , ε > 1 , u ( 0 ) = u ( 1 ) = 0 , v ( 0 ) = v ( 1 ) = 0 .

The corresponding nonlinear terms are

f ( t , x , y , p ) = x α + y β + p γ , g ( t , x , y , q ) = x α + y β + q ε .

When α , β , γ , ε > 1 , f and g satisfy conditions ( F 1 ) and ( F 2 ) . For all ( t , x , y ) I × R + × R + , p , q R , and ( x , p ) = x 2 + p 2 < δ < 1 , ( y , q ) = y 2 + q 2 < δ < 1 , we have

f ( t , x , y , p ) + g ( t , x , y , q ) = 2 x α + 2 y β + p γ + q ε = 2 x α 1 x + 2 y β 1 y + p γ 1 p + q ε 1 q 2 δ α 1 x + 2 δ β 1 y + δ γ 1 p + δ ε 1 q = a x + b y + c p + d q ,

when δ is appropriately small, 2 δ α 1 + 2 δ β 1 π 2 + δ γ 1 + δ ε 1 π < 1 , thus f and g satisfy condition ( F 1 ) .

When ( x , p ) > H > 1 , ( y , q ) > H > 1 , let ξ = min { α , β , γ , ε } , then ξ > 1 , we can obtain

f ( t , x , y , p ) + g ( t , x , y , q ) = 2 x α + 2 y β + p γ + q ε 2 x ξ + 2 y ξ + p ξ + q ξ x ξ + p ξ + y ξ + q ξ 1 2 ξ ( ( x + p ) ξ + ( y + q ) ξ ) 1 2 ξ ( ( x , p ) ξ + ( y , q ) ξ ) = 1 2 ξ ( x , p ) ξ 1 ( x , p ) + 1 2 ξ ( y , q ) ξ 1 ( y , q ) min 1 2 ξ ( x , p ) ξ 1 , 1 2 ξ ( y , q ) ξ 1 ( x + y ) = e ( x + y ) ,

when H is large enough, min 1 2 ξ ( x , p ) ξ 1 , 1 2 ξ ( y , q ) ξ 1 > π 2 , thus f and g satisfy condition ( F 2 ) .

But only when 1 < γ , ε 2 , f and g satisfy condition ( F 3 ) . From Theorem 3.1, we can know that BVP (4.1) has at least one positive solution.

Acknowledgements

The authors are most grateful to the editor and anonymous referees for the careful reading of the manuscript and valuable suggestions that helped in significantly improving an earlier version of this article.

  1. Funding information: This work was supported by NNSF of China (Nos 12061062 and 11661071).

  2. Author contributions: Wang carried out the first draft of this manuscript. All authors read and approved the final manuscript.

  3. Conflict of interest: All authors declare that they have no competing interest.

  4. Data availability statement: Data sharing is not applicable to this article as no datasets were generated or analyzed during this study.

References

[1] A. M. Fink and J. A. Gatica, Positive solutions of second order systems of boundary value problems, J. Math. Anal. Appl. 180 (1993), 93–108. 10.1006/jmaa.1993.1385Search in Google Scholar

[2] R. Ma, Multiple nonnegative solutions of second-order systems of boundary value problems, Nonlinear Anal. 42 (2000), 1003–1010. 10.1016/S0362-546X(99)00152-2Search in Google Scholar

[3] L. Wu, T. Sun, and X. He, The existence and uniqueness of solutions to systems of second-order ordinary differential equations boundary value problem in abstract space, Chinese Quart. J. Math. 26 (2011), 573–577. 10.1155/2011/192156Search in Google Scholar

[4] Z. Yang, X. Wang, and H. Li, Positive solutions for a system of second-order quasilinear boundary value problems, Nonlinear Anal. 195 (2020), 111749. 10.1016/j.na.2020.111749Search in Google Scholar

[5] Z. L. Yang and J. X. Sun, Positive solutions of boundary value problems for systems of nonlinear second order ordinary differential equations, Acta Math. Sinica 47 (2004), 111–118. Search in Google Scholar

[6] B. Liu and L. Liu, The unique solution for systems of second-order equations, Chinese J. Engrg. Math. 24 (2007), 757–760. Search in Google Scholar

[7] X. Cheng, Positive solutions for a second-order super-sublinear elliptic system (Chinese), J. LanZhou Univ. Nat. Sci. 44 (2008), 113–117. Search in Google Scholar

[8] X. Cheng and C. Zhong, Existence of positive solutions for a second-order ordinary differential system, J. Math. Anal. Appl. 312 (2005), 14–23. 10.1016/j.jmaa.2005.03.016Search in Google Scholar

[9] X. Cheng, Existence of positive solutions for a class of second-order ordinary differential systems, Nonlinear Anal. 69 (2008), 3042–3049. 10.1016/j.na.2007.08.074Search in Google Scholar

[10] X. Cheng and Z. Zhang, Positive solutions for a multi-parameter system of second-order ordinary differential equations, Sci. China Math. 54 (2011), 959–972. 10.1007/s11425-011-4213-xSearch in Google Scholar

[11] Y. Li, Positive solutions of fourth-order boundary value problems with two parameters, J. Math. Anal. Appl. 281 (2003), 477–484. 10.1016/S0022-247X(03)00131-8Search in Google Scholar

[12] Y. Li, On the existence of positive solutions for the bending elastic beam equations, Appl. Math. Comput. 189 (2007), 821–827. 10.1016/j.amc.2006.11.144Search in Google Scholar

[13] Y. Li, Positive solutions for second order boundary value problems with derivative terms, Math. Nachr. 289 (2016), 2058–2068. 10.1002/mana.201500040Search in Google Scholar

[14] Y. Li and T. Zhang, Infinitely many periodic solutions for second-order (p, q)-Laplacian differential systems, Nonlinear Anal. 74 (2011), 5215–5221. 10.1016/j.na.2011.05.024Search in Google Scholar

[15] Q. Zhang, Existence of positive solutions for a class of p(x)-Laplacian systems, J. Math. Anal. Appl. 333 (2007), 591–603. 10.1016/j.jmaa.2006.11.037Search in Google Scholar

[16] B. Thomas, Z. Wang, and J. Wei, Bound states for a coupled Schrodinger system, J. Fixed Point Theory Appl. 2 (2007), 353–367. 10.1007/s11784-007-0033-6Search in Google Scholar

[17] R. Precup, The role of matrices that are convergent to zero in the study of semilinear operator systems, Math. Comput. Model. 49 (2009), 703–708. 10.1016/j.mcm.2008.04.006Search in Google Scholar

[18] X. Cheng and X. Yan, A multiplicity result of positive solutions for a class of multi-parameter ordinary differential systems, Acta Math. Appl. Sin. Engl. Ser. 28 (2012), 653–662. 10.1007/s10255-012-0180-4Search in Google Scholar

[19] X. Cheng and Z. Zhang, Positive solutions for a class of multi-parameter elliptic systems, Nonlinear Anal. Real World Appl. 14 (2013), 1551–1562. 10.1016/j.nonrwa.2012.10.018Search in Google Scholar

[20] J. Jiang, J. Henderson, J. Xu, and Z. Fu, Positive solutions for a system of Neumann boundary value problems of second order difference equations involving sign-changing nonlinearities, J. Funct. Spaces 2019 (2019), 3203401. 10.1155/2019/3203401Search in Google Scholar

[21] X. Han, Y. He and H. Wei, Existence of positive periodic solutions for a nonlinear system of second-order ordinary differential equations, Electron. J. Differential Equations 83 (2022), 1–11. 10.58997/ejde.2022.83Search in Google Scholar

[22] K. Deimling, Nonlinear Functional Analysis, Springer-Verlag, Berlin, 1985. 10.1007/978-3-662-00547-7Search in Google Scholar

[23] D. Guo and V. Lakshmikantham, Nonlinear Problems in Abstract Cones, Academic Press Inc., Boston, 1988. Search in Google Scholar

Received: 2022-03-03
Revised: 2023-03-21
Accepted: 2023-04-14
Published Online: 2023-05-26

© 2023 the author(s), published by De Gruyter

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

Articles in the same Issue

  1. Special Issue on Future Directions of Further Developments in Mathematics
  2. What will the mathematics of tomorrow look like?
  3. On H 2-solutions for a Camassa-Holm type equation
  4. Classical solutions to Cauchy problems for parabolic–elliptic systems of Keller-Segel type
  5. Control of multi-agent systems: Results, open problems, and applications
  6. Logical perspectives on the foundations of probability
  7. Subharmonic solutions for a class of predator-prey models with degenerate weights in periodic environments
  8. A non-smooth Brezis-Oswald uniqueness result
  9. Luenberger compensator theory for heat-Kelvin-Voigt-damped-structure interaction models with interface/boundary feedback controls
  10. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part II)
  11. Positive solution for a nonlocal problem with strong singular nonlinearity
  12. Analysis of solutions for the fractional differential equation with Hadamard-type
  13. Hilfer proportional nonlocal fractional integro-multipoint boundary value problems
  14. A comprehensive review on fractional-order optimal control problem and its solution
  15. The θ-derivative as unifying framework of a class of derivatives
  16. Review Articles
  17. On the use of L-functionals in regression models
  18. Minimal-time problems for linear control systems on homogeneous spaces of low-dimensional solvable nonnilpotent Lie groups
  19. Regular Articles
  20. Existence and multiplicity of solutions for a new p(x)-Kirchhoff problem with variable exponents
  21. An extension of the Hermite-Hadamard inequality for a power of a convex function
  22. Existence and multiplicity of solutions for a fourth-order differential system with instantaneous and non-instantaneous impulses
  23. Relay fusion frames in Banach spaces
  24. Refined ratio monotonicity of the coordinator polynomials of the root lattice of type Bn
  25. On the uniqueness of limit cycles for generalized Liénard systems
  26. A derivative-Hilbert operator acting on Dirichlet spaces
  27. Scheduling equal-length jobs with arbitrary sizes on uniform parallel batch machines
  28. Solutions to a modified gauged Schrödinger equation with Choquard type nonlinearity
  29. A symbolic approach to multiple Hurwitz zeta values at non-positive integers
  30. Some results on the value distribution of differential polynomials
  31. Lucas non-Wieferich primes in arithmetic progressions and the abc conjecture
  32. Scattering properties of Sturm-Liouville equations with sign-alternating weight and transmission condition at turning point
  33. Some results for a p(x)-Kirchhoff type variation-inequality problems in non-divergence form
  34. Homotopy cartesian squares in extriangulated categories
  35. A unified perspective on some autocorrelation measures in different fields: A note
  36. Total Roman domination on the digraphs
  37. Well-posedness for bilevel vector equilibrium problems with variable domination structures
  38. Binet's second formula, Hermite's generalization, and two related identities
  39. Non-solid cone b-metric spaces over Banach algebras and fixed point results of contractions with vector-valued coefficients
  40. Multidimensional sampling-Kantorovich operators in BV-spaces
  41. A self-adaptive inertial extragradient method for a class of split pseudomonotone variational inequality problems
  42. Convergence properties for coordinatewise asymptotically negatively associated random vectors in Hilbert space
  43. Relating the super domination and 2-domination numbers in cactus graphs
  44. Compatibility of the method of brackets with classical integration rules
  45. On the inverse Collatz-Sinogowitz irregularity problem
  46. Positive solutions for boundary value problems of a class of second-order differential equation system
  47. Global analysis and control for a vector-borne epidemic model with multi-edge infection on complex networks
  48. Nonexistence of global solutions to Klein-Gordon equations with variable coefficients power-type nonlinearities
  49. On 2r-ideals in commutative rings with zero-divisors
  50. A comparison of some confidence intervals for a binomial proportion based on a shrinkage estimator
  51. The construction of nuclei for normal constituents of Bπ-characters
  52. Weak solution of non-Newtonian polytropic variational inequality in fresh agricultural product supply chain problem
  53. Mean square exponential stability of stochastic function differential equations in the G-framework
  54. Commutators of Hardy-Littlewood operators on p-adic function spaces with variable exponents
  55. Solitons for the coupled matrix nonlinear Schrödinger-type equations and the related Schrödinger flow
  56. The dual index and dual core generalized inverse
  57. Study on Birkhoff orthogonality and symmetry of matrix operators
  58. Uniqueness theorems of the Hahn difference operator of entire function with a Picard exceptional value
  59. Estimates for certain class of rough generalized Marcinkiewicz functions along submanifolds
  60. On semigroups of transformations that preserve a double direction equivalence
  61. Positive solutions for discrete Minkowski curvature systems of the Lane-Emden type
  62. A multigrid discretization scheme based on the shifted inverse iteration for the Steklov eigenvalue problem in inverse scattering
  63. Existence and nonexistence of solutions for elliptic problems with multiple critical exponents
  64. Interpolation inequalities in generalized Orlicz-Sobolev spaces and applications
  65. General Randić indices of a graph and its line graph
  66. On functional reproducing kernels
  67. On the Waring-Goldbach problem for two squares and four cubes
  68. Singular moduli of rth Roots of modular functions
  69. Classification of self-adjoint domains of odd-order differential operators with matrix theory
  70. On the convergence, stability and data dependence results of the JK iteration process in Banach spaces
  71. Hardy spaces associated with some anisotropic mixed-norm Herz spaces and their applications
  72. Remarks on hyponormal Toeplitz operators with nonharmonic symbols
  73. Complete decomposition of the generalized quaternion groups
  74. Injective and coherent endomorphism rings relative to some matrices
  75. Finite spectrum of fourth-order boundary value problems with boundary and transmission conditions dependent on the spectral parameter
  76. Continued fractions related to a group of linear fractional transformations
  77. Multiplicity of solutions for a class of critical Schrödinger-Poisson systems on the Heisenberg group
  78. Approximate controllability for a stochastic elastic system with structural damping and infinite delay
  79. On extremal cacti with respect to the first degree-based entropy
  80. Compression with wildcards: All exact or all minimal hitting sets
  81. Existence and multiplicity of solutions for a class of p-Kirchhoff-type equation RN
  82. Geometric classifications of k-almost Ricci solitons admitting paracontact metrices
  83. Positive periodic solutions for discrete time-delay hematopoiesis model with impulses
  84. On Hermite-Hadamard-type inequalities for systems of partial differential inequalities in the plane
  85. Existence of solutions for semilinear retarded equations with non-instantaneous impulses, non-local conditions, and infinite delay
  86. On the quadratic residues and their distribution properties
  87. On average theta functions of certain quadratic forms as sums of Eisenstein series
  88. Connected component of positive solutions for one-dimensional p-Laplacian problem with a singular weight
  89. Some identities of degenerate harmonic and degenerate hyperharmonic numbers arising from umbral calculus
  90. Mean ergodic theorems for a sequence of nonexpansive mappings in complete CAT(0) spaces and its applications
  91. On some spaces via topological ideals
  92. Linear maps preserving equivalence or asymptotic equivalence on Banach space
  93. Well-posedness and stability analysis for Timoshenko beam system with Coleman-Gurtin's and Gurtin-Pipkin's thermal laws
  94. On a class of stochastic differential equations driven by the generalized stochastic mixed variational inequalities
  95. Entire solutions of two certain Fermat-type ordinary differential equations
  96. Generalized Lie n-derivations on arbitrary triangular algebras
  97. Markov decision processes approximation with coupled dynamics via Markov deterministic control systems
  98. Notes on pseudodifferential operators commutators and Lipschitz functions
  99. On Graham partitions twisted by the Legendre symbol
  100. Strong limit of processes constructed from a renewal process
  101. Construction of analytical solutions to systems of two stochastic differential equations
  102. Two-distance vertex-distinguishing index of sparse graphs
  103. Regularity and abundance on semigroups of partial transformations with invariant set
  104. Liouville theorems for Kirchhoff-type parabolic equations and system on the Heisenberg group
  105. Spin(8,C)-Higgs pairs over a compact Riemann surface
  106. Properties of locally semi-compact Ir-topological groups
  107. Transcendental entire solutions of several complex product-type nonlinear partial differential equations in ℂ2
  108. Ordering stability of Nash equilibria for a class of differential games
  109. A new reverse half-discrete Hilbert-type inequality with one partial sum involving one derivative function of higher order
  110. About a dubious proof of a correct result about closed Newton Cotes error formulas
  111. Ricci ϕ-invariance on almost cosymplectic three-manifolds
  112. Schur-power convexity of integral mean for convex functions on the coordinates
  113. A characterization of a ∼ admissible congruence on a weakly type B semigroup
  114. On Bohr's inequality for special subclasses of stable starlike harmonic mappings
  115. Properties of meromorphic solutions of first-order differential-difference equations
  116. A double-phase eigenvalue problem with large exponents
  117. On the number of perfect matchings in random polygonal chains
  118. Evolutoids and pedaloids of frontals on timelike surfaces
  119. A series expansion of a logarithmic expression and a decreasing property of the ratio of two logarithmic expressions containing cosine
  120. The 𝔪-WG° inverse in the Minkowski space
  121. Stability result for Lord Shulman swelling porous thermo-elastic soils with distributed delay term
  122. Approximate solvability method for nonlocal impulsive evolution equation
  123. Construction of a functional by a given second-order Ito stochastic equation
  124. Global well-posedness of initial-boundary value problem of fifth-order KdV equation posed on finite interval
  125. On pomonoid of partial transformations of a poset
  126. New fractional integral inequalities via Euler's beta function
  127. An efficient Legendre-Galerkin approximation for the fourth-order equation with singular potential and SSP boundary condition
  128. Eigenfunctions in Finsler Gaussian solitons
  129. On a blow-up criterion for solution of 3D fractional Navier-Stokes-Coriolis equations in Lei-Lin-Gevrey spaces
  130. Some estimates for commutators of sharp maximal function on the p-adic Lebesgue spaces
  131. A preconditioned iterative method for coupled fractional partial differential equation in European option pricing
  132. A digital Jordan surface theorem with respect to a graph connectedness
  133. A quasi-boundary value regularization method for the spherically symmetric backward heat conduction problem
  134. The structure fault tolerance of burnt pancake networks
  135. Average value of the divisor class numbers of real cubic function fields
  136. Uniqueness of exponential polynomials
  137. An application of Hayashi's inequality in numerical integration
Downloaded on 13.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2022-0586/html
Scroll to top button