Electronic Journal of Differential Equations, Vol. 2011 (2011), No. 22, pp. 1–11. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu POSITIVE SOLUTIONS FOR SECOND-ORDER MULTI-POINT BOUNDARY-VALUE PROBLEMS AT RESONANCE IN BANACH SPACES WEIHUA JIANG, BIN WANG Abstract. In this article, we study the existence and multiplicity of positive solutions for a nonlinear second-order multi-point boundary-value problem at resonance in Banach spaces. The arguments are based upon a specially constructed equivalent equation and the fixed point theory in a cone for strict set contraction operators. 1. Introduction The theory of ordinary differential equations in Banach spaces has become a new important branch (see, for example, [2, 6, 7, 12] and references cited therein). In 1988, Guo and Lakshmikantham [8] discussed the existence of multiple solutions for two-point boundary value problem of ordinary differential equations in Banach spaces. Since then, nonlinear second-order multi-point boundary value problems at non-resonance in Banach spaces have been studied by several authors (see, for example, [5, 13, 14, 18] and references cited therein). Recently, the existence of solutions for boundary value problems at resonance have been studied by many papers, (see, for example [3, 4, 9, 10, 11, 15, 16, 19]). Using the Krasnolsel’skii-Guo fixed point theorem, Han [9] studied a second order three-point BVP at resonance by rewriting the original BVP as an equivalent one. Motivated by their results, in this paper, we will discuss the existence of positive solutions for the second-order m-point boundary value problem at resonance y 00 (t) = f (t, y), y 0 (0) = θ, y(1) = 0 < t < 1, m−2 X ki y(ξi ) (1.1) (1.2) i=1 2000 Mathematics Subject Classification. 34B15. Key words and phrases. Banach space; positive solution; strict set contraction; boundary value problem. c 2011 Texas State University - San Marcos. Submitted July 14, 2010. Published February 9, 2011. Supported by grants 10875094 from the Natural Science Foundation of China, A2009000664 from the Natural Science Foundation of Hebei Province, 2008153 from the Foundation of Hebei Education Department, and XL200814 from the Foundation of Hebei University of Science and Technology. 1 2 W. JIANG, B. WANG EJDE-2011/22 in a real Banach space E, where θ is P the zero element of E, 0 < ξ1 < ξ2 < · · · < m−2 ξm−2 < 1, ki > 0, i = 1, 2, . . . , m − 2, i=1 ki = 1. Pm−2 The boundary value problem (1.1)-(1.2) is at resonance when i=1 ki = 1; that is, the corresponding homogeneous boundary value problem y 00 (t) = 0, y 0 (0) = 0, t ∈ [0, 1], y(1) = m−2 X ki y(ξi ) i=1 has nontrivial solutions. To the best of our knowledge, no paper has considered the existence of positive solutions for the boundary value problems at resonance in Banach spaces. We shall fill this gap in the literature. The organization of this paper is as follows. We shall introduce a theorem and some notations in the rest of this section. In Section 2, we provide some necessary background. In particular, we state some properties of Green’s function associated with the equivalent problem of (1.1)-(1.2). In Section 3, the main results will be stated and proved. Theorem 1.1 ([1, 17]). Let K be a cone of the real Banach space X and Kr,R = {x ∈ K|r ≤ kxk ≤ R} with R > r > 0. Assume that A : Kr,R → K is a strict set contraction such that one of the following two conditions is satisfied (i) Ax 6≤ x for all x ∈ K, kxk = r and Ax 6≥ x for all x ∈ K, kxk = R. (ii) Ax ≥ 6 x for all x ∈ K, kxk = r and Ax 6≤ x for all x ∈ K, kxk = R. Then A has at least one fixed point x ∈ K satisfying r < kxk < R. Let the real Banach space E with norm k · k be partially ordered by a normal cone P of E; i.e., x ≤ y if and only if y − x ∈ P , and P ∗ denotes the dual cone of P ; i.e., P ∗ = {ϕ ∈ E ∗ : ϕ(x) ≥ 0, x ∈ P }. Denote the normal constant of P by N ; i.e., θ ≤ x ≤ y implies kxk ≤ N kyk. Take I = [0, 1]. For any x ∈ C[I, E], evidently, (C[I, E], k·kc ) is a Banach space with kxkc = maxt∈I kx(t)k, and Q = {x ∈ C[I, E] : x(t) ≥ θ for t ∈ I} is a cone of the Banach space C[I, E]. A function y ∈ C 2 [I, E] is called a positive solution of the boundary value problem (1.1)-(1.2) if it satisfies (1.1)-(1.2) and y ∈ Q, y(t) 6≡ θ. In this paper, we denote α(·) the Kuratowski measure of non-compactness of a bounded set in E and C[I, E]. The closed balls in spaces E and C[I, E] are denoted by Tr = {x ∈ E : kxk ≤ r}(r > 0) and Br = {y ∈ C[I, E] : kykc ≤ r}(r > 0), respectively. Define F (t, y) := f (t, y) + β 2 y, where β ∈ (0, π2 ). Obviously, y(t) is a solution of the problem (1.1)-(1.2) if and only if it is a solution of the problem y 00 (t) + β 2 y(t) = F (t, y(t)), y 0 (0) = θ, y(1) = m−2 X i=1 and the problem (1.3)-(1.4) is at non-resonance. 0 < t < 1, ki y(ξi ), (1.3) (1.4) EJDE-2011/22 POSITIVE SOLUTIONS 3 For convenience, we set a0 = m−2 X ki cos βξi − cos β, a1 = (a0 + 1) sin β + i=1 m−2 X ki sin βξi , i=1 a2 = 1 − m−2 X ki cos β(1 − ξi ). i=1 In this paper, we assume the following conditions hold. Pm−2 (H1) ki > 0, i = 1, 2, . . . , m − 2, 0 < ξ1 < ξ2 < · · · < ξm−2 < 1, i=1 ki = 1. (H2) P is a normal cone of E and N is the normal constant; F : I × P → P , F (t, θ) = θ for all t ∈ I; for any r > 0, F (t, x) is uniformly continuous and bounded on I × (P ∩ Tr ) and there exists a constant Lr with 0 ≤ Lr < (βa0 )/(2a1 ) such that α(F (I × D)) ≤ Lr α(D), ∀D ⊂ P ∩ Tr . 2. Preliminary lemmas Pm−2 Lemma 2.1. Assume i=1 ki = 1, then for h(t) ∈ C[I, E], the problem y 00 (t) + β 2 y(t) = h(t), y 0 (0) = θ, y(1) = 0 < t < 1, m−2 X ki y(ξi ) (2.1) (2.2) i=1 has a unique solution Z Z cos βt 1 1 t [ sin β(1 − s)h(s)ds sin β(t − s)h(s)ds + y(t) = β 0 βa0 0 m−2 X Z ξi − ki sin β(ξi − s)h(s)ds] Z i=1 1 =: (2.3) 0 G(t, s)h(s)ds, 0 where 1 Pm−2 cos βt β sin β(t − s) + βa0 [sin β(1 − s) − j=i kj sin β(ξj − s)], if ξi−1 ≤ s ≤ min{t, ξi }, ; i = 1, 2, . . . , m − 1; G(t, s) = Pm−2 cos βt [sin β(1 − s) − j=i kj sin β(ξj − s)], βa 0 if max{ξi−1 , t} ≤ s ≤ ξi , i = 1, 2, . . . , m − 1. The proof of the above lemma is easy, so we omit it. Lemma 2.2. There exist c1 , c2 > 0 such that c1 (1 − s) ≤ G(t, s) ≤ c2 (1 − s), t, s ∈ [0, 1]. Proof. Take H(t, s) = c(1 − s) − G(t, s). We will prove that H(t, s) ≥ 0, t, s ∈ [0, 1], when c is sufficiently large. For t, s ∈ [0, 1], we have 1 cos βt H(t, s) ≥ c(1 − s) − sin β(t − s) − sin β(1 − s) β βa0 1 sin β(1 − s) ≥ c(1 − s) − sin β(1 − s) − β βa0 4 W. JIANG, B. WANG 1 1 [1 + ] sin β(1 − s) β a0 = c(1 − s) − ≥ (c − 1 − EJDE-2011/22 1 )(1 − s). a0 Take c2 ≥ 1 + a10 , then H(t, s) ≥ 0, t, s ∈ [0, 1]. Now, we prove H(t, s) ≤ 0, t, s ∈ [0, 1], when c is sufficiently small. For t ∈ [0, 1], s ∈ (ξ1 , 1], we have H(t, s) ≤ c(1 − s) − m−2 X cos βt [sin β(1 − s) − kj sin β(ξj − s)] βa0 j=i ≤ c(1 − s) − m−2 X cos β [sin β(1 − s) − kj sin β(ξj − s)] βa0 j=2 ≤ c(1 − s) − k1 cos β sin β(1 − s). βa0 Since ( g(x) = sin x x , 1, 0 < x ≤ π/2, x=0 is continuous on [0, π/2]. So, we obtain min x∈[0,π/2] g(x) := m0 > 0; i.e., sin x ≥ m0 x, x ∈ [0, π/2]. Therefore, m0 k1 cos β (1 − s) a0 m0 k1 cos β = (c − )(1 − s). a0 H(t, s) ≤ c(1 − s) − For t ∈ [0, 1], s ∈ [0, ξ1 ], we obtain H(t, s) ≤ c(1 − s) − ≤ c(1 − s) − ≤c− m−2 X cos βt [sin β(1 − s) − kj sin β(ξj − s)] βa0 j=1 m−2 β(1 + ξj − 2s) β(1 − ξj ) cos β X 2 kj cos sin βa0 j=1 2 2 m−2 2 cos β X β(1 + ξi ) β(1 − ξi ) ki cos sin . βa0 i=1 2 2 Take P β(1+ξi ) i) m0 k1 cos β 2 cos β( m−2 sin β(1−ξ ) i=1 ki cos 2 2 0 < c1 ≤ min , . a0 βa0 Then we have c1 (1 − s) ≤ G(t, s), t, s ∈ [0, 1]. The proof is complete. Lemma 2.3. Assume (H1) holds. If h ∈ Q, then the unique solution y of (2.1)(2.2) satisfies y(t) ≥ θ, t ∈ I and y(t) ≥ γy(s) for all t, s ∈ I, where γ = c1 /c2 . EJDE-2011/22 POSITIVE SOLUTIONS 5 Proof. Obviously, y(t) ≥ θ for all t ∈ I. By Lemma 2.2, we obtain Z Z 1 c1 1 y(t) ≥ c1 c2 (1 − s)h(s)ds ≥ γy(r), ∀t, r ∈ I. (1 − s)h(s)ds = c2 0 0 The proof is complete. Define an operator A : Q → C[I, E] as follows Z Z 1 t cos βt 1 [ A(y(t)) := sin β(t − s)F (s, y(s))ds + sin β(1 − s)F (s, y(s))ds β 0 βa0 0 m−2 X Z ξi − ki sin β(ξi − s)F (s, y(s))ds]. i=1 0 (2.4) By Lemmas 2.1 and 2.3, we obtain that A : Q → C 2 [I, E] ∩ Q, and y(t) is a positive solution of (1.1)-(1.2) if and only if y(t) ∈ C 2 [I, E] ∩ Q and y(t) 6≡ θ is a fixed point of the operator A. Lemma 2.4. Assume (H1), (H2) hold. Then, for any r > 0, the operator A is a strict set contraction on Q ∩ Br . Proof. Since F (t, x) is uniformly continuous and bounded on I × (P ∩ Tr ), we see from (2.4) that A is continuous and bounded on Q ∩ Br . For any S ⊂ Q ∩ Br , by (2.4), we can easily get that functions A(S) = {Ay|y ∈ S} are uniformly bounded and equicontinuous. By [12], we have α(A(S)) = sup α(A(S(t))), (2.5) t∈I where A(S(t)) = {Ay(t) : y ∈ S, t ∈ I is fixed}. For any y ∈ C[I, E], g ∈ C[I, I], Rt by 0 g(s)y(s)ds ∈ co({g(t)y(t)|t ∈ I} ∪ {θ}) ⊂ co({y(t)|t ∈ I} ∪ {θ}), we obtain α(A(S(t))) Z Z 1 t cos βt h 1 sin β(1 − s)F (s, y(s))ds = α({ sin β(t − s)F (s, y(s))ds + β 0 βa0 0 m−2 i X Z ξi − ki sin β(ξi − s)F (s, y(s))ds : y ∈ S}) i=1 0 sin β α(co({F (s, y(s)) : s ∈ I, y ∈ S} ∪ {θ})) β sin β + α(co({F (s, y(s)) : s ∈ I, y ∈ S} ∪ {θ})) βa0 Pm−2 ki sin βξi α(co({F (s, y(s)) : s ∈ I, y ∈ S} ∪ {θ})) + i=1 βa0 a1 = α({F (s, y(s)) : s ∈ I, y ∈ S}) βa0 a1 ≤ α(F (I × B)), βa0 ≤ where B = {y(s) : s ∈ I, y ∈ S} ⊂ P ∩ Tr . By (H2), we obtain α(A(S(t))) ≤ a1 Lr α(B). βa0 (2.6) 6 W. JIANG, B. WANG EJDE-2011/22 For any given ε > 0, there exists a partition S = ∪lj=1 Sj such that ε (2.7) diam(Sj ) < α(S) + , j = 1, 2, . . . , l. 3 Now, choose yj ∈ Sj , j = 1, 2, . . . , l and a partition 0 = t0 < t1 < · · · < tk = 1 such that ε (2.8) kyj (t) − yj (t)k < , ∀t, t ∈ [ti−1 , ti ], j = 1, 2, . . . , l, i = 1, 2, . . . , k. 3 Obviously, B = ∪lj=1 ∪ki=1 Bij , where Bij = {y(t) : y ∈ Sj , t ∈ [ti−1 , ti ]}. For any y(t), y(t) ∈ Bij , by (2.7) and (2.8), we obtain ky(t) − y(t)k ≤ ky(t) − yj (t)k + kyj (t) − yj (t)k + kyj (t) − y(t)k ε ≤ ky − yj kc + + kyj − ykc 3 ε ≤ 2 diam(Sj ) + < 2α(S) + ε, 3 which implies diam(Bij ) ≤ 2α(S)+ε, and so, α(B) ≤ 2α(S)+ε. Since ε is arbitrary, we obtain α(B) ≤ 2α(S). (2.9) It follows from (2.5), (2.6) and (2.9) that 2a1 Lr α(S), ∀S ⊂ Q ∩ Br . α(A(S)) ≤ βa0 By (H2), we obtain that A is a strict set contraction on Q ∩ Br . 3. Main results Let K = {y ∈ Q : y(t) ≥ γy(s), ∀t, s ∈ I}. Clearly, K ⊂ Q is a cone of C[I, E]. By Lemmas 2.1 and 2.3, we obtain AQ ⊂ K. So, AK ⊂ K. For convenience, for any x ∈ P and ϕ ∈ P ∗ , we set F 0 = lim sup sup kxk→0 t∈I F0ϕ = lim inf inf kxk→0 t∈I kF (t, x)k , kxk F ∞ = lim sup sup ϕ(F (t, x)) , ϕ(x) ϕ F∞ = lim inf inf kxk→∞ t∈I kxk→∞ t∈I kF (t, x)k , kxk ϕ(F (t, x)) ϕ(x) and list the following assumptions: (H3) There exists ϕ ∈ P ∗ such that ϕ(x) > 0 for any x > θ and F0ϕ > ϕ (H4) There exists ϕ ∈ P ∗ such that ϕ(x) > 0 for any x > θ and F∞ > β 2 a0 γa2 . β 2 a0 γa2 . β 2 a0 N (1+a0 )(1−cos β) . 2 a0 F ∞ < N (1+aβ0 )(1−cos β) . (H5) F 0 < (H6) (H7) There exists r0 > 0 such that kF (t, x)k < sup t∈I, x∈P β 2 a0 r0 . N (1 + a0 )(1 − cos β) γr0 /N ≤kxk≤r0 (H8) There exist R0 > 0 and ϕ ∈ P ∗ with ϕ(x) > 0 for any x > θ such that inf t∈I,x∈P γR0 /N ≤kxk≤R0 ϕ(F (t, x)) β 2 a0 . > ϕ(x) γa2 EJDE-2011/22 POSITIVE SOLUTIONS 7 Theorem 3.1. Assume (H1), (H2) hold. If one of the following conditions is satisfied: (i) (H4) and (H5) hold. (ii) (H3) and (H6) hold. Then the problem (1.1)-(1.2) has at least one positive solution. 2 Proof. (i) By (H4), we obtain that there exist constants M > βγaa20 and r1 > 0 such that ϕ(F (t, x)) ≥ M ϕ(x), ∀t ∈ I, x ∈ P, kxk > r1 . (3.1) For any R > N r1 /γ, we will show that Ay 6≤ y, ∀y ∈ K, kykc = R. (3.2) In fact, if not, there exists y0 ∈ K, ky0 kc = R such that Ay0 ≤ y0 . By y0 (t) ≥ γy0 (s) ≥ θ, we have ky0 (t)k ≥ ∀t, s ∈ I, γ ky0 kc > r1 , N ∀t ∈ I. (3.3) (3.4) By (2.4), for any t ∈ I, we have Z Z 1 t cos βt h 1 sin β(1 − s)F (s, y0 (s))ds A(y0 (t)) = sin β(t − s)F (s, y0 (s))ds + β 0 βa0 0 m−2 i X Z ξi − ki sin β(ξi − s)F (s, y0 (s))ds i=1 0 Z 1 m−2 cos βt X sin β(1 − s)F (s, y0 (s))ds. ki ≥ βa0 i=1 ξi This inequality, (3.1), (3.3) and (3.4), imply Z 1 m−2 1 X sin β(1 − s)M γϕ(y0 (0))ds ϕ(Ay0 (0)) ≥ ki βa0 i=1 ξi a2 = 2 M γϕ(y0 (0)). β a0 Considering Ay0 ≤ y0 , we obtain ϕ(y0 (0)) ≥ γa2 M ϕ(y0 (0)). β 2 a0 (3.5) It is easy to see that ϕ(y0 (0)) > 0 (In fact, if ϕ(y0 (0)) = 0, by (3.3), we obtain ϕ(y0 (0)) ≥ γϕ(y0 (s)) ≥ 0 for all s ∈ I. So, we have ϕ(y0 (s)) ≡ 0 for all s ∈ I. That is, y0 (s) ≡ θ. This is a contradiction with ky0 kc = R). So, (3.5) contradicts with 2 M > βγaa20 . Therefore, (3.2) is true. On the other hand, by (H5) and F (t, θ) = θ, we obtain that there exist constants 2 a0 0 < ε < N (1+aβ0 )(1−cos β) and 0 < r2 < R such that kF (t, x)k ≤ εkxk, ∀t ∈ I, x ∈ P, kxk < r2 . (3.6) For any 0 < r < r2 , we now prove that Ay 6≥ y, ∀y ∈ K, kykc = r. (3.7) 8 W. JIANG, B. WANG EJDE-2011/22 In fact, if not, there exists y0 ∈ K, ky0 kc = r such that Ay0 ≥ y0 . Since (2.4) implies Z a0 + cos βt 1 Ay0 (t) ≤ sin β(1 − s)F (s, y0 (s))ds, ∀t ∈ I. (3.8) βa0 0 So, we have Z a0 + cos βt 1 sin β(1 − s)F (s, y0 (s))ds, ∀t ∈ I. θ ≤ y0 (t) ≤ βa0 0 This, together with (3.6), imply Z N (1 + a0 )ε 1 N (1 + a0 )(1 − cos β)εky0 kc ky0 (t)k ≤ , sin β(1 − s)ky0 (s)kds = βa0 β 2 a0 0 for all t ∈ I. Therefore, we obtain ε ≥ β 2 a0 /N (1 + a0 )(1 − cos β). This is a contradiction. So, (3.7) is true. By (3.2), (3.7), Lemma 2.4 and Theorem 1.1, we obtain that the operator A has at least one fixed point y ∈ K satisfying r < kykc < R. (ii) By (H3), in the same way as establishing (3.2) we can assert that there exists r2 > 0 such that for any 0 < r < r2 , Ay 6≤ y, ∀y ∈ K, kykc = r. (3.9) On the other hand, by (H6), we obtain that there exist constants r1 > 0 and ε, 2 a0 with 0 < ε < N (1+aβ0 )(1−cos β) , such that kF (t, x)k ≤ εkxk, ∀t ∈ I, x ∈ P, kxk > r1 . By (H2), we obtain kF (t, x)k =: b < ∞. sup t∈I, x∈P ∩Tr1 So, we have kF (t, x)k ≤ εkxk + b, ∀t ∈ I, x ∈ P. (3.10) Take R > max r2 , N b(1 + a0 )(1 − cos β) , − N ε(1 + a0 )(1 − cos β) β 2 a0 we will prove that Ay 6≥ y, ∀y ∈ K, kykc = R. (3.11) In fact, if there exists y0 ∈ K, ky0 kc = R such that Ay0 ≥ y0 . Then, by (3.8) and (3.10), we obtain Z N (a0 + cos βt) 1 sin β(1 − s)(εky0 (s)k + b)ds ky0 (t)k ≤ βa0 0 N (1 + a0 )(1 − cos β) ≤ (εky0 kc + b), ∀t ∈ I. β 2 a0 So, we have N b(1 + a0 )(1 − cos β) < R. − N ε(1 + a0 )(1 − cos β) A contradiction. Therefore, (3.11) holds. By (3.9), (3.11), Lemma 2.4 and Theorem 1.1, we obtain that the operator A has at least one fixed point y ∈ K satisfying r < kykc < R. The proof is complete. ky0 kc ≤ β 2 a0 EJDE-2011/22 POSITIVE SOLUTIONS 9 Theorem 3.2. Assume (H1), (H2) hold. If one of the following conditions is satisfied: (i) (H3), (H4), (H7) hold. (ii) (H5), (H6), (H8) hold. Then (1.1)-(1.2) has at least two positive solutions. Proof. (i) By (H3), (H4) and the proof of Theorem 3.1, we obtain that there exist r, R with 0 < r < r0 < R such that Ay 6≤ y, ∀y ∈ K, kykc = r, Ay 6≤ y, ∀y ∈ K, kykc = R. Now, we prove that Ay 6≥ y, ∀y ∈ K, kykc = r0 . (3.12) In fact, if there exists y0 ∈ K, ky0 kc = r0 such that Ay0 ≥ y0 . By (3.8) and (H7), we obtain Z N (1 + a0 ) 1 β 2 a0 ky0 kc < r0 ds = r0 . sin β(1 − s) βa0 N (1 + a0 )(1 − cos β) 0 A contradiction. So, (3.12) is true. By Lemma 2.4 and Theorem 1.1, we obtain that the operator A has at least two fixed points y1 , y2 ∈ K satisfying r < ky1 kc < r0 < ky2 kc < R. (ii) By (H5), (H6) and the proof of Theorem 3.1, we obtain that there exist r, R with 0 < r < R0 < R such that Ay 6≥ y, ∀y ∈ K, kykc = r, Ay 6≥ y, ∀y ∈ K, kykc = R. On the other hand, by (H8) and the same way as used in the proof of (3.2), we can prove that Ay 6≤ y, ∀y ∈ K, kykc = R0 . (3.13) By Lemma 2.4 and Theorem 1.1, we obtain that the operator A has at least two fixed points y1 , y2 ∈ K satisfying r < ky1 kc < R0 < ky2 kc < R. The proof is complete. Similar to the proofs of Theorem 3.1 and Theorem 3.2, we can easily get the following corollaries. Corollary 3.3. Assume (H1), (H2) hold. If one of the following conditions is satisfied: (i) (H4), (H5), (H7), (H8) hold with R0 < γr0 /N . (ii) (H3), (H6), (H7), (H8) hold with r0 < γR0 /N . Then (1.1)-(1.2) has at least three positive solutions. Corollary 3.4. Assume (H1), (H2) hold. If one of the following conditions is satisfied: (i) (H5)–(H7) hold, and there exist Ri > 0, ϕi ∈ P ∗ with ϕi (x) > 0 for x > θ, i = 1, 2 such that inf t∈I, x∈P, γRi /N ≤kxk≤Ri β 2 a0 ϕi (F (t, x)) > , ϕi (x) γa2 where R1 < γr0 /N , r0 < γR2 /N . i = 1, 2, 10 W. JIANG, B. WANG EJDE-2011/22 (ii) (H3), (H4), (H8) hold, and there exist r1 , r2 > 0 such that sup kF (t, x)k < t∈I, x∈P, γri /N ≤kxk≤ri β 2 a0 ri , N (1 + a0 )(1 − cos β) i = 1, 2, where r1 < γR0 /N , R0 < γr2 /N . Then (1.1)-(1.2) has at least four positive solutions. We can prove easily the existence of multiple positive solutions for (1.1)-(1.2). References [1] N. P. Cac, J. A. Gatica; Fixed point theorems for mappings in ordered Banach spaces, J. Math. Anal. Appl., 71 (1979), 545-557. [2] K. Demling; Ordinary Differential Equations in Banach Spaces Springer, Berlin, 1977. [3] Z. Du, X. Lin, W. Ge; Some higher-order multi-point boundary value problem at resonance, J. Comput. Appl. Math. 177(2005), 55-65. [4] B. Du, X. Hu; A new continuation theorem for the existence of solutions to P -Lpalacian BVP at resonance, Appl. Math. Comput. 208(2009), 172-176. [5] M. Feng, D. Ji, W. Ge; Positive solutions for a class of boundary-value problem with integral boundary conditions in Banach spaces, J. Comput. Appl. Math., 222(2008), 351-363. [6] D. Guo, V. Lakshmikantham, X. Liu; Nonlinear Integral Equation in Abstract spaces, Kluwer Academic Publishers, Dordrecht, 1996. [7] D. Guo, V. Lakshmikantham; Nonlinear Problems in Abstract Cones, Academic Press, San Diego, 1988. [8] D. Guo, V. Lakshmikantham; Multiple solutions of two-point boundary value problem of ordinary differential equations in Banach space, J. Math. Anal. Appl., 129(1988), 211-222. [9] X. Han; Positive solutions for a three-point boundary value problem at resonance, J. Math. Anal. Appl., 336(2007) 556-568. [10] N. Kosmatov; A multi-point boundary value problem with two critical conditions, Nonlinear Anal., 65(2006), 622-633. [11] N. Kosmatov; Multi-point boundary value problems on an unbounded domain at resonance, Nonlinear Anal., 68(2008), 2158-2171. [12] V. Lakshmikantham, S. Leela; Nonlinear Differential Equations in Abstract Spaces, Pergamon Press, Oxford, 1981. [13] B. Liu; Positive solutions of a nonlinear four-point boundary value problems in Banach spaces, J. Math. Anal. Appl., 305(2005), 253-276. [14] L. Liu, Z. Liu, Y. Wu; Infinite boundary value problems for nth-order nonlinear impulsive integro-differential equations in Banach spaces, Nonlinear Analysis, 67(2007), 2670-2679. [15] Y. Liu, W. Ge; Solvability of nonlocal boundary value problems for ordinary differential equations of higher order, Nonlinear Anal., 57(2004), 435-458. [16] S. Lu, W. Ge; On the existence of m-point boundary value problem at resonance for higher order differential equation, J. Math. Anal. Appl. 287(2003), 522-539. [17] A. J. B. Potter; A fixed point theorem for positive k-set contractions, Proc. Edinburgh Math. Soc., 19(1974), 93-102. [18] X. Zhang, M. Feng, W. Ge; Existence and nonexistence of positive solutions for a class of nthorder three-point boundary value problems in Banach spaces, Nonlinear Analysis, 70(2009), 584-597. [19] X. Zhang, M. Feng, W. Ge; Existence result of second-order differential equations with integral boundary conditions at resonance, J. Math. Anal. Appl. 353(2009), 311-319. Weihua Jiang College of Sciences, Hebei University of Science and Technology, Shijiazhuang, 050018, Hebei, China E-mail address: weihuajiang@hebust.edu.cn EJDE-2011/22 POSITIVE SOLUTIONS 11 Bin Wang Department of Basic Courses, Hebei Professional and Technological College of Chemical and, Pharmaceutical Engineering, Shijiazhuang, 050026, Hebei, China E-mail address: wb@hebcpc.cn