Electronic Journal of Differential Equations, Vol. 2010(2010), No. 139, pp. 1–9. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu SOLVABILITY OF A THREE-POINT NONLINEAR BOUNDARY-VALUE PROBLEM ASSIA GUEZANE-LAKOUD, SMAIL KELAIAIA Abstract. Using the Leray Schauder nonlinear alternative, we prove the existence of a nontrivial solution for the three-point boundary-value problem u00 + f (t, u) = 0, 0 0<t<1 u(1) = βu0 (η), u(0) = αu (0), where η ∈ (0, 1), α, β ∈ R, f ∈ C([0, 1] × R, R). Some examples are given to illustrate the results obtained. 1. Introduction and preliminaries During the previous years, many authors have studied three-point boundaryvalue problems (BVP) for second order differential equations. Such problems have potential applications in physics, biology, chemistry, etc. For example, a secondorder three-point (BVP) is used as a model for the membrane response of a spherical cap [10] in nonlinear diffusion generated by nonlinear sources and in chemical reactor theory. In this article, we investigate the existence of a nontrivial solution for the secondorder three-point boundary-value problem u00 + f (t, u) = 0, 0 0 < t < 1, 0 u(0) = αu (0), u(1) = βu (η) (1.1) (1.2) where η ∈ (0, 1), α, β ∈ R, f ∈ C([0, 1] × R, R). We do not assume any monotonicity condition on the nonlinearity f , and the parameters α and β belong to R, so our conditions are more general than the conditions found in the literature. Such problem arises in the study of the equilibrium states of a heated bar. In this situation two controllers at t = 0 and t = η alter the heat according to the temperatures detected by a sensor at t = 1. This study is motivated by Il’in and Moiseev’s results [5], on similar boundary value problems for certain linear ordinary differential equations. Many of the results involving nonlocal boundary value problems are studied in [2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12]. In [12] the author used the Leray-Shauder nonlinear alternative to 2000 Mathematics Subject Classification. 34B10, 34B15. Key words and phrases. Fixed point theorem; three-point boundary-value problem; non trivial solution. c 2010 Texas State University - San Marcos. Submitted March 19, 2010. Published September 27, 2010. 1 2 A. GUEZANE-LAKOUD, S. KELAIAIA EJDE-2010/139 establish some results on the existence of solutions for the equation (1.1) subject to the conditions u(0) = 0, u(1) = αu(η) Gupta [3] studied certain three-point boundary-value problem with the above nonlocal conditions. Similar boundary value problem with the conditions u(0) = αu0 (0), u(1) = βu(η) is considered in [11]. Under some conditions on the nonlinearity of f and by using Leray Schauder nonlinear alternative, we establish the existence of nontrivial solution of the BVP (1.1)-(1.2). Some examples illustrate our results. This article is organized as follows. First, we list some preliminary material to be used later. Then in Section 2, we present and prove our main results which consist in existence theorems and corollaries. We end our work with some illustrating examples. Let E = C[0, 1], with the supremum norm ky(t)k = supt∈[0,1] |y(t)|, for all y ∈ E. Now we state two preliminary results. Lemma 1.1. Let y ∈ E. If β(η + α) 6= α + 1, then the three-point BVP u00 (t) + y(t) = 0, 0 u(1) = βu0 (η) u(0) = αu (0), has a unique solution Z t u(t) = − (t − s)y(s)ds + 0 t+α 1+α−β 0<t<1 Z 1 (1 − s)y(s)ds − β 0 t+α 1+α−β Z η y(s)ds. 0 Proof. Rewriting the differential equation as u00 (t) = −y(t), and integrating twice, we obtain Z t u(t) = − (t − s)y(s)ds + C1 t + C. (1.3) 0 Then u0 (0) = C1 , Z 0 u (η) = − η y(s)ds + C1 , 0 1 Z u(1) = − (1 − s)y(s)ds + C1 + C2 , 0 u(0) = C2 = αC1 . Combining these with the second equality in condition (1.2), we obtain Z 1 Z η − (1 − s)y(s)ds + C1 (1 + α) = −β y(s)ds + C1 β, 0 0 which is equivalent to Z C1 (1 + α − β) = 1 Z (1 − s)y(s)ds − β 0 η y(s)ds. 0 Since 1 + α − β 6= 0, C1 = Z 1 Z η 1 ( (1 − s)y(s)ds − β y(s)ds). 1+α−β 0 0 C2 = αC1 . EJDE-2010/139 SOLVABILITY 3 Substituting C1 and C2 by their values in (1.3), we obtain the solution in the statement of the lemma. This completes the proof. We define the integral operator T : E → E, by Z 1 Z t t+α (1 − s)f (s, u(s))ds T u(t) = − (t − s)f (s, u(s))ds + 1+α−β 0 0 Z η t+α −β f (s, u(s))ds 1+α−β 0 (1.4) By Lemma 1.1, BVP (1.1)-(1.2) has a solution if and only if the operator T has a fixed point in E. By Ascoli Arzela theorem we prove that T is a completely continuous operator. Now we cite the Leray Schauder nonlinear alternative. Lemma 1.2 ([1]). Let F be a Banach space and Ω a bounded open subset of F , 0 ∈ Ω. T : Ω → F be a completely continuous operator. Then, either there exists x ∈ ∂Ω, λ > 1 such that T (x) = λx, or there exists a fixed point x∗ ∈ Ω. 2. Main Results In this section, we present and prove our main results. Theorem 2.1. We assume that f (t, 0) 6= 0, 1 + α 6= β and there exist nonnegative functions k, h ∈ L1 [0, 1] such that |f (t, x)| ≤ k(t)|x| + h(t), a.e. (t, x) ∈ [0, 1] × R, Z 1 Z η |1 + α| 1+α (1 + ) (1 − s)k(s)ds + |β | k(s)ds < 1 |1 + α − β| 0 1+α−β 0 (2.1) (2.2) Then BVP (1.1)-(1.2) has at least one nontrivial solution u∗ ∈ C[0, 1]. Proof. Setting Z 1 Z η |1 + α| 1+α ) | (1 − s)k(s)ds + |β k(s)ds, |1 + α − β| 0 1+α−β 0 Z 1 Z η |1 + α| 1+α N = (1 + ) | (1 − s)h(s)ds + |β (η − s)h(s)ds. |1 + α − β| 0 1+α−β 0 M = (1 + By (2.2), we have M < 1. Since f (t, 0) 6= 0, then there exists an interval [σ, τ ] ⊂ [0, 1] such that min |f (t, 0)| > 0 and as h(t) ≥ |f (t, 0)|, for all t ∈ [0, 1] then N > 0. σ≤t≤r N Let m = (1−M ) , Ω = {u ∈ C[0, 1] : kuk < m}. Assume that u ∈ ∂Ω, λ > 1 such T u = λu, then λm = λkuk = kT uk = max |(T u)(t)| 0≤t≤1 Z 1 Z η h |1 + α| 1+α ≤ kuk (1 + ) (1 − s)k(s)ds + |β | k(s)ds |1 + α − β| 0 1+α−β 0 Z 1 Z η i |1 + α| 1+α + (1 + ) (1 − s)h(s)ds + |β | h(s)ds |1 + α − β| 0 1+α−β 0 = M kuk + N From this we obtain λ≤M+ N N =M+ = M + (1 − M ) = 1, m N (1 − M )−1 4 A. GUEZANE-LAKOUD, S. KELAIAIA EJDE-2010/139 this contradicts λ > 1. By Lemma 1.2 we conclude that operator T has a fixed point u∗ ∈ Ω and then BVP (1.1)-(1.2) has a nontrivial solution u∗ ∈ C[0, 1]. Theorem 2.2. Assume (2.1) and one of the following four conditions: (1) There exists a constant p > 1 such that Z 1 ip h (1 + q)1/q 1 1 k p (s)ds < ( + = 1); 1+α 1+α 1/q p q 1 + | | + (|β |)(η(1 + q)) 0 1+α−β 1+α−β (2.3) (2) There exists constant µ > −1 such that k(s) < (µ + 1)(µ + 2) sµ 1+α 1+α 1 + | 1+α−β | + (|β 1+α−β |)(µ + 2)η µ+1 (2.4) and meas s ∈ [0, 1] : k(s) < (µ + 1)(µ + 2) sµ > 0; 1+α 1+α 1 + | 1+α−β | + |β 1+α−β |(µ + 2)η µ+1 (3) The function k(s) satisfies k(s) < |1 + α − β| |1 + α| + |1 + α − β| + |β(1 + α)|η (2.5) and meas s ∈ [0, 1] : k(s) < |1 + α − β| |1 + α| + |1 + α − β| + |β(1 + α)|η > 0; (4) The function f (t, x) satisfies ω = lim sup max | |x|→∞ t∈[0,1] f (t, x) 1 |1 + α − β| |< ( ). x 2 |1 + α| + |1 + α − β| + |β(1 + α)|η (2.6) Then BVP (1.1)-(1.2) has at least one nontrivial solution u∗ ∈ C[0, 1]. Proof. Let M be defined as in the proof of Theorem 2.1. To prove Theorem 2.2, we only need to prove that M < 1. (1) By using Hölder inequality, we obtain Z 1/p Z 1 1/q 1 + α 1 p M ≤ 1+| | k (s)ds (1 − s)q ds 1+α−β 0 Z 0 1/p Z η 1/q 1+α η p | + |β k (s)ds ds . 1+α−β 0 0 Then M≤ Z 1 k p (s)ds 1/p h 0 1+α + |β 1+α−β 1 + α | 1+α−β Z η 1/q i | ds . Z 1+| 1 (1 − s)q ds 1/q 0 0 Integrating, it yields M< (1 + q)1/q 1+α 1+α (1 + | 1+α−β |) + |β 1+α−β |(η(1 + q))1/q h i 1 1/q 1+α |1 + α| × (1 + )( ) + |β |η 1/q = 1. |1 + α − β| 1 + q 1+α−β EJDE-2010/139 SOLVABILITY 5 (2) Using the same reasoning as in the proof of the first statement we obtain (µ + 1)(µ + 2) 1+α 1+α 1 + | 1+α−β | + (|β 1+α−β |)(µ + 2)η µ+1 Z Z η h i 1+α 1+α 1 (1 − s)sµ ds + |β | | sµ ds × 1+| 1+α−β 1+α−β 0 0 1+α (µ + 1)(µ + 2) 1 1+| = | 1+α 1+α µ+1 1 + α − β (µ + 1)(µ + 2) 1 + | 1+α−β | + |β 1+α−β |(µ + 2)η M< + β 1+α 1+α−β η µ+1 =1 µ+1 (3) we have M = (1 + |1 + α| ) |1 + α − β| Z 1 (1 − s)k(s)ds + |β 0 1+α | 1+α−β Z η k(s)ds. 0 Then |1 + α − β| |(1 + α)| + |1 + α − β| + |β(1 + α)|η Z Z η 1+α 1 1+α × 1+| | (1 − s)ds + |β | ds 1+α−β 1+α−β 0 0 1 |1+α−β| 1+α 1+α = ( |(1+α)|+|1+α−β|+|β(1+α)|η )(1 + | 1+α−β |) + |β 1+α−β |η = 1 2 M< (4) From ω = lim sup|x|→∞ maxt∈[0,1] | f (t,x) x | we deduce that there exists c > 0 such that for |x| > c we have |f (t, x)| ≤ (ω + ε)|x| ∀ε > 0. Set h(t) = max{|f (t, x)| : (t, x) ∈ [0, 1] × (−c, c)}. Then for (t, x) ∈ [0, 1] × R, with ε = ω, we obtain |f (t, x)| ≤ 2ω|x| + h(t) ≤ |1 + α − β| |x| + h(t). |(1 + α)| + |1 + α − β| + |β(1 + α)|η Setting k(t) < |1 + α − β| , |(1 + α)| + |1 + α − β| + |β(1 + α)|η by applying the above statement we complete the proof. Corollary 2.3. Assume the conditions of Theorem 2.2, and one of the following four conditions: (1) There exists a constant p > 1 such that Z 1 h ip (1 + q)1/q k p (s)ds < , 1+α 1+α 1 + | 1+α−β | + |β 1+α−β |(1 + q)1/q 0 1 1 ( + = 1). p q 6 A. GUEZANE-LAKOUD, S. KELAIAIA EJDE-2010/139 (2) There exists a constant µ > −1 such that k(s) < 1+ (µ + 1)(µ + 2) sµ , 1+α + (|β 1+α−β |)(µ + 2) 1+α | 1+α−β | meas s ∈ [0, 1] : k(s) < 1+ (µ + 1)(µ + 2) sµ > 0 1+α + |β 1+α−β |(µ + 2) 1+α | 1+α−β | (3) The function k(s) satisfies |1 + α − β| , |(1 + α)| + |1 + α − β| + |β(1 + α)|η |1 + α − β| meas s ∈ [0, 1], k(s) < >0 |(1 + α)| + |1 + α − β| + |β(1 + α)|η k(s) < (4) The function f (t, x) satisfies ω = lim sup max | |x|→∞ t∈[0,1] < 1/2( f (t, x) | x |1 + α − β| ) |(1 + α)| + |1 + α − β| + |β(1 + α)| Then the BVP (1.1)-(1.2) has at least one nontrivial solution u∗ ∈ C[0, 1]. Proof. Taking into account Z Z η 1+α |1 + α| 1 | (1 − s)k(s)ds + |β k(s)ds |1 + α − β| 0 1+α−β 0 Z Z 1 |1 + α| 1 1+α ≤ 1+ | (1 − s)k(s)ds + |β k(s)ds. |1 + α − β| 0 1+α−β 0 M = 1+ the proof follows. 3. Examples To illustrate our results, we give the following examples. Example 3.1. Consider the three-point BVP √ u u00 + (t sin u − e−t cos u) + tet = 0, 0 < t < 1 2 1 1 u(0) = u0 (0), u(1) = u0 ( 12 ). 2 2 Where α = β = η = 1/2, +α − β = 1/2 6= 0 and √ x f (t, x) = (t sin x − e−t cos x) + tet , 2 It is easy to see that |f (t, x)| ≤ 1 (t + e−t )|x| + tet , 2 (t, x) ∈ [0, 1] × R, set k(t) = 1 (t + e−t ) ≥ 0, 2 h(t) = tet ≥ 0, (3.1) EJDE-2010/139 SOLVABILITY 7 we have k, h ∈ L1 [0, 1], f (t, 0) = tet 6= 0 and Z Z 1 5 1 3 2 M= (1 − s)k(s)ds + k(s)ds 2 0 4 0 Z Z 3 1/2 5 1 (1 − s)(s + e−s )ds + (s + e−s )ds = 0.86261. = 4 0 8 0 Then, by Theorem 2.1, the BVP (3.1) has at least one nontrivial solution u∗ in C[0, 1]. Example 3.2. Consider the three-point BVP u4 u00 + √ + cos et (1 − sin t) = 0, 0 < t < 1, 2 t3 + 1(1 + u3 ) u(0) = −2u0 (0), u(1) = 2u0 (1/3) (3.2) then x4 f (t, x) = √ + cos et (1 − sin t), 2 t3 + 1(1 + x3 ) 1 |x| + cos et (1 − sin t) |f (t, x)| ≤ √ 4 t3 + 1 = k(t)|x| + h(t), where 1 k(t) = √ ≥ 0, 4 t3 + 1 M= = 4 3 Z 1 3 Z 1 (1 − s)k(s)ds + 0 1 (1 − s) √ 0 2 3 h(t) = cos et (1 − sin t) ≥ 0 Z η k(s)ds 0 1 2 ds + 16 s3 + 1 Z 1/3 0 √ 1 ds = 0.201 41 < 1 s3 + 1 Applying the third statement of Theorem 2.2 we obtain max k(s) = s 1 |1 + α − β| 9 < = 0.642 86 , 4 |(1 + α)| + |1 + α − β| + |β(1 + α)|η 14 |1 + α − β| } |(1 + α)| + |1 + α − β| + |β(1 + α)|η 9 = meas{s ∈ [0, 1] : k(s) < = 0.642 86} 14 = meas[0, 1] > 0 . meas{s ∈ [0, 1] : k(s) < Hence, by Theorem 2.2, BVP (3.2) has at least one nontrivial solution u∗ in C[0, 1]. Example 3.3. Consider the three-point BVP √ u3 − t sin t = 0 2 2(1 + e−t )4 (1 + u2 ) 1 −1 0 1 u(0) = u0 (0), u(1) = u ( ). 3 6 4 u00 + (3.3) 8 A. GUEZANE-LAKOUD, S. KELAIAIA EJDE-2010/139 We have √ x3 − t sin t, 2 4 −t 2 2(1 + e ) (1 + x ) 2 (1 + e−t )−4 √ |f (t, x)| ≤ |x| + t sin t = k(t)|x| + h(t) 2 √ 2 t sin t f (t, x) (1 + e−t )−4 1 | |≤ + ≤ 0.142 + . x 2 |x| |x| Applying the fourth statement in Theorem 2.2 we obtain f (t, x) 1 ω = lim sup max | | = lim sup(0.142 + ) x |x| |x|→∞ t∈[0,1] |x|→∞ f (t, x) = = 0.142 < 1 ( 2 43 + 13 9 13 1 9 + 27 ) = 0.25658 Hence, BVP (3.3) has at least one nontrivial solution u∗ in C[0, 1]. Example 3.4. Consider the three-point BVP sin u u00 + √ − t2 cos t + t cos(t2 ) = 0, 0 < t < 1 2 4+t −1 0 1 −1 0 u (0), u(1) = u ( ), u(0) = 4 6 5 where sin x f (t, x) = √ − t2 cos t + t cos(t2 ), 2 4+t |x| |f (t, x)| ≤ √ − t2 cos t + t cos(t2 ) = k(t)|x| + h(t), 2 4+t 1 k(t) = √ ≥ 0, h(t) = −t2 cos t + t cos(t2 ) ≥ 0 2 4+t (3.4) We see that k, h ∈ L1 [0, 1], f (t, 0) = −t2 cos t + t cos(t2 ) 6= 0. The first statement of Corollary 2.3 for p = 2 yields Z Z 1 Z 1 2 1 1 1 1 √ dt = 0.055786 k 2 (s)ds = dt = 4 0 4+t 2( 4 + t) 0 0 h ip (1 + q)1/q < = 0.71083. 1+α 1+α 1 + | 1+α−β | + |β 1+α−β |(1 + q)1/q Hence, BVP (3.4) has at least one nontrivial solution u∗ in C[0, 1]. Acknowledgements. The authors are grateful to the anonymous referees for their helpful comments and fruitful remarks. The second author would like to express his thanks to the Laboratory of advanced material at Annaba university for its support and hospitality. References [1] K. Deimling; Non-linear Functional Analysis, Springer, Berlin, 1985. [2] W. Feng, J. R. L. Webb; Solvability of three-point nonlinear bound-ary value problems at resonance, Nonlinear Analysis TMA, 30 (6), (1997), 3227-3238. [3] C. P. Gupta; Solvability of a three-point nonlinear boundary value problem for a second order ordinary differential equations, J. Math. Anal. Appl. 168 (1992), 540-551. EJDE-2010/139 SOLVABILITY 9 [4] C. P. Gupta; Solvability of a three-point nonnlinear boundary value problem for a second order differential equation, J. Math. Anal. Appl. 168, (1992), 540-551. [5] V. A. Il’in and E. I. Moiseev; Nonlocal boundary value problem of the first kind for a SturmLiouville operator in its differential and finite difference aspects, Differential Equations, 23 (7) (1987), 803–810. [6] G. Infante and J. R. L. Webb; Three point boundary value problems with solutions that change sign, J. Integ. Eqns Appl, 15 (2003), 37-57. [7] S. A. Krasnoselskii; A remark on a second order three-point boundary value problem, J. Math. Anal. Appl. 183, (1994), 581-592. [8] R. Ma; Existence theorems for second order three-point boundary value problems, J. Math. Anal. Appl. 212 (1997), 545-555. [9] R. Ma; A Survey On Nonlocal Boundary Value Problems. Applied Mathematics E-Notes, 7 (2007), 257-279 [10] P. K. Palamides, G. Infante, P. Pietramala; Nontrivial solutions of a nonlinear heat flow problem via Sperner’s Lemma. Applied Mathematics Letters 22 (2009) 1444-1450. [11] L. Shuhong, Y-P. Sun; Nontrivial solution of a nonlinear second order three-point boundaryvalue problem, Appl. math. J (2007), 22(1), 37-47. [12] Y-P. Sun; Nontrivial solution for a three-point boundary-value problem, Electron. J. of Differential Equations, Vol. 2004 (2004), No. 111, 1-10. Assia Guezane-Lakoud Department of Mathematics, Faculty of Sciences, University Badji Mokhtar, B.P. 12, 23000, Annaba, Algeria E-mail address: a guezane@yahoo.fr Smail Kelaiaia Department of Mathematics, Faculty of Sciences, University Badji Mokhtar, B.P. 12, 23000, Annaba, Algeria E-mail address: kelaiaiasmail@yahoo.fr