Electronic Journal of Differential Equations, Vol. 2010(2010), No. 52, pp. 1–10. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu MULTIPLICITY OF POSITIVE SOLUTIONS FOR FOUR-POINT BOUNDARY VALUE PROBLEMS OF IMPULSIVE DIFFERENTIAL EQUATIONS WITH p-LAPLACIAN LI SHEN, XIPING LIU, ZHENHUA LU Abstract. Using a fixed-point theorem in cones, we obtain sufficient conditions for the multiplicity of positive solutions for four-point boundary value problems of third-order impulsive differential equations with p-Laplacian. 1. Introduction Recently, there has been much attention focused on the theory of impulsive differential equation as it is widely used in various areas such as mechanics, electromagnetism, chemistry. A lot of theories have been established to solve these problems, see [9], [3] and the references therein. Guo [4] obtained the existence of solutions, via cone theory, for second-order impulsive differential equation x00 = f (t, x, T x), t ≥ 0, t 6= tk k = 1, 2, 3, . . . , ∆x|t=tk = Ik (x(tk )), k = 1, 2, 3, . . . , 0 ∆x |t=tk = I k (x(tk )), k = 1, 2, 3, . . . , 0 x (0) = x∗0 . x(0) = x0 , In [1], using Leggett-Williams fixed point theorem, authors studied the multiplicity result for second order impulsive differential equations y 00 + φ(t)f (y(t)) = 0, t ∈ (0, 1) \ {t1 , t2 , . . . , tm }, ∆y(tk ) = Ik (y(t− k )), 0 ∆y (tk ) = Jk (y(t− k )), k = 1, 2, 3, . . . , m, k = 1, 2, 3, . . . , m, y(0) = y(1) = 0. Kaufmann [8] studied a second-order nonlinear differential equation on an unbounded domain with solutions subject to impulsive conditions and the SturmLiouville type boundary conditions. In [5]-[7], the authors studied positive solutions of multiple points boundary value problems for second order impulsive differential equations. 2000 Mathematics Subject Classification. 34A37, 34B37. Key words and phrases. p-Laplacian; impulsive; positive solutions; boundary value problem. c 2010 Texas State University - San Marcos. Submitted November 16, 2009. Published April 14, 2010. Supported by grant 10ZZ93 from Innovation Program of Shanghai Municipal Education Commission. 1 2 L. SHEN, X. LIU, Z. LU EJDE-2010/52 All the works above concern boundary value problems with second-order impulsive equations, and there are just a few works that consider multiplicity of positive solutions for third-order impulsive equations with p-Laplacian. Motivated by all the works above, we concentrate on getting multiple positive solutions for four-point boundary value problems of third-order impulsive differential equations with p-Laplacian (φp (u00 (t)))0 = f (t, u(t), u0 (t)), 00 ∆u (t)|t=tk = 0, t ∈ (0, 1)\{t1 , t2 , . . . , tm }, k = 1, 2, . . . , m, 0 ∆u (t)|t=tk = Ik (u(tk )), k = 1, 2, . . . , m, ∆u(t)|t=tk = Jk (u(tk )), k = 1, 2, . . . , m, 00 0 u (0) = αu (ξ) + βu0 (η), u (0) = 0, 0 (1.1) u(1) = δu(0), where φp is p-Laplacian operator φp (s) = |s|p−2 s, p > 1, (φp )−1 = φq , 1 1 + = 1, p q tk , k = 0, 1, 2, . . . , m, m + 1, are constants which satisfy 0 = t0 < t1 < t2 < · · · < tk < · · · < tm < tm+1 = 1, − + − ∆u|t=tk = u(t+ k ) − u(tk ), in which u(tk ) (u(tk ) respectively) denote the right limit (left limit respectively) of u(t) at t = tk , and α, β > 0, α + β < 1; 0 < ξ, η < 1; ξ, η 6= tk (k = 1, 2, . . . , m); δ > 1; f ∈ C([0, 1] × [0, +∞) × R, [0, +∞)), Ik , Jk ∈ C([0, +∞), [0, +∞)). 2. Preliminaries Let J = [0, 1]\{t1 , t2 , . . . , tm }, P C[0, 1] = {u : [0, 1] → R, u is continuous at − − 1 t 6= tk , u(t+ k ), u(tk ) exist, and u(tk ) = u(tk ), k = 1, 2, . . . , m}, P C [0, 1] = {u ∈ 0 0 + 0 − P C[0, 1] | u is continuous at t 6= tk , u (tk ), u (tk ) exist, k = 1, 2, . . . , m}, with the norm kukP C 1 =max {kukP C , ku0 kP C }. kukP C = sup |u(t)|, t∈J t∈J Obviously P C[0, 1] and P C 1 [0, 1] are Banach spaces. Lemma 2.1. u ∈ P C 1 [0, 1] T C 3 [J] is a solution of (1.1) if and only if s u(t) = u(0) + u (0)t + (t − s)φq f (r, u(r), u0 (r))dr ds 0 X X 0 + (t − tk )Ik (u(tk )) + Jk (u(tk )), 0 tk <t Z t Z tk <t (2.1) EJDE-2010/52 MULTIPLICITY OF POSITIVE SOLUTIONS 3 where u(0) = α Rs Rη Rs φq ( 0 f (r, u(r), u0 (r))dr)ds + β 0 φq ( 0 f (r, u(r), u0 (r))dr)ds (δ − 1)(1 − α − β) P P α tk <ξ Ik (u(tk )) + β tk <η Ik (u(tk )) Rξ 0 + R1Rs + + 0 0 1 δ−1 (δ − 1)(1 − α − β) Rr φq ( 0 f (w, u(w), u0 (w))dw) dr ds δ−1 m X (1 − tk )Ik (u(tk ) + Jk (u(tk )) , (2.2) k=1 Rs Rs Rη φq ( 0 f (r, u(r), u0 (r))dr)ds + β 0 φq ( 0 f (r, u(r), u0 (r))dr)ds u (0) = 1−α−β (2.3) P P α tk <ξ Ik (u(tk )) + β tk <η Ik (u(tk )) + . 1−α−β T Proof. Suppose u ∈ P C 1 [0, 1] C 3 [J] is a solution of (1.1), for all k = 1, 2, . . . , m, from Lagrange’s mean value theorem we have α 0 Rξ 0 u(tk ) − u(tk − h) = u0 (ξk )h, 0 < h < tk − tk−1 , ξk ∈ (tk − h, tk ), because u0 (t− k ) exists, we get u0− (tk ) = lim+ h→0 u(tk ) − u(tk − h) = lim− u0 (ξk ) = u0 (t− k ). h ξk →tk Let u0 (tk ) = u0− (tk ) = u0 (t− k ), k = 1, 2, . . . , m. We use Lagrange’s mean value theorem again and obtain u0 (tk ) − u0 (tk − h) = u00 (ηk )h, we can get u00− (tk ) 0 < h < tk − tk−1 , ηk ∈ (tk − h, tk ), 00 − exists from ∆u (t)|t=tk = u00 (t+ k ) − u (tk ) = 0, and 00 u00− (tk ) = lim+ h→0 u0 (tk ) − u0 (tk − h) = lim− u00 (ξk ) = u00 (t− k ). h ξk →tk Let u00 (tk ) = u00 (t− k ), k = 1, 2, . . . , m. Integrating the differential equation (1.1) we have Z t φp (u00 (t)) − φp (u00 (0)) = f (s, u(s), u0 (s))ds, 0 By u00 (0) = 0, we have Z t u00 (t) = φq ( f (s, u(s), u0 (s))ds); 0 that is, Z t u00 (t) = φq ( f (s, u(s), u0 (s))ds), 0 and Z u (t1 ) = φq ( 00 0 t1 f (s, u(s), u0 (s))ds). 0 ≤ t ≤ t1 . 4 L. SHEN, X. LIU, Z. LU EJDE-2010/52 00 − Since ∆u00 (t)|t=t1 = u00 (t+ 1 ) − u (t1 ) = 0, for t1 < t ≤ t2 , we obtain Z t 00 f (s, u(s), u0 (s))ds). u (t) = φq ( 0 00 Similarly, by ∆u (t)|t=tk = u all t ∈ [0, 1], 00 − u00 (t− k ) = 0, k = 1, 2, . . . , m, we can show for (t+ k) Z t u (t) = φq ( f (s, u(s), u0 (s))ds). 00 (2.4) 0 For each t ∈ (0, 1), there exist 0 ≤ tk < tk+1 ≤ 1, such that tk < t ≤ tk+1 , by integrating both sides of (2.4), we obtain Z t1 Z s 0 u0 (t− ) − u (0) = φ ( f (r, u(r), u0 (r))dr)ds, q 1 0 0 Z t2 Z s 0 + u0 (t− ) − u (t ) = φ ( f (r, u(r), u0 (r))dr)ds, q 2 1 t1 0 ... 0 + u0 (t− k ) − u (tk−1 ) = Z φq ( tk−1 t Z u0 (t) − u0 (t+ k)= tk Z f (r, u(r), u0 (r))dr)ds, 0 Z φq ( tk s s f (r, u(r), u0 (r))dr)ds. 0 Hence, 0 t Z 0 u (t) = u (0) + Z φq ( 0 s f (r, u(r), u0 (r))dr)ds + 0 X Ik (u(tk )). tk <t We have αu0 (ξ) = αu0 (0) + α ξ Z Z φq ( 0 βu0 (η) = βu0 (0) + β Z 0 η s f (r, u(r), u0 (r))dr)ds + α 0 Z φq ( X Ik (u(tk )), tk <ξ s f (r, u(r), u0 (r))dr)ds + β 0 X Ik (u(tk )). tk <η It follows that Rη Rs Rξ Rs α 0 φq ( 0 f (r, u(r), u0 (r))dr)ds + β 0 φq ( 0 f (r, u(r), u0 (r))dr)ds 0 u (0) = 1−α−β P P α tk <ξ Ik (u(tk )) + β tk <η Ik (u(tk )) + 1−α−β from u0 (0) = αu0 (ξ) + βu0 (η). Similarly, we get the results as follows with the method above Z t Z s 0 u(t) = u(0) + u (0)t + (t − s)φq f (r, u(r), u0 (r))dr ds 0 X X 0 + (t − tk )Ik (u(tk )) + Jk (u(tk )). tk <t tk <t EJDE-2010/52 MULTIPLICITY OF POSITIVE SOLUTIONS 5 Note that by the boundary condition u(1) = δu(0), Rξ Rs Rη Rs α 0 φq ( 0 f (r, u(r), u0 (r))dr)ds + β 0 φq ( 0 f (r, u(r), u0 (r))dr)ds u(0) = (δ − 1)(1 − α − β) P P α tk <ξ Ik (u(tk )) + β tk <η Ik (u(tk )) + (δ − 1)(1 − α − β) R1Rs Rr φq ( 0 f (w, u(w), u0 (w))dw) dr ds + 0 0 δ−1 m 1 X [(1 − tk )Ik (u(tk ) + Jk (u(tk ))]. + δ−1 k=1 T On the other hand, let u ∈ P C 1 [0, 1] C 3 [J] be a solution of (2.1), differentiate (2.1) when t 6= tk , we have Z t u00 (t) = φq ( f (s, u(s), u0 (s))ds); 0 that is, φp (u00 (t)) = t Z f (s, u(s), u0 (s))ds . 0 Differentiating again, (φp (u00 (t)))0 = f (t, u(t), u0 (t)). By (2.1), we can easily get ∆u00 (t)|t=tk = 0, k = 1, 2, . . . , m, 0 00 ∆u (t)|t=tk = Ik (u(tk )), k = 1, 2, . . . , m, ∆u(t)|t=tk = Jk (u(tk )), k = 1, 2, . . . , m, u (0) = 0, 0 0 u (0) = αu (ξ) + βu0 (η), u(1) = δu(0). Next, we give the Bai-Ge fixed point theorem which is used in the proof of our main result. Let E be a Banach space, P ⊂ E be a cone, θ, ψ : P → [0, +∞) be nonnegative convex functions which satisfy kxk ≤ k max{θ(x), ψ(x)}, for all x ∈ P, (2.5) where k is a positive constant. Ω = {x ∈ P : θ(x) < r, ψ(x) < L} = 6 φ, where r > 0, L > 0. (2.6) Let r > a > 0, L > 0 be constants, θ, ψ : P → [0, +∞) be two nonnegative continuous convex functions which satisfy (2.5) and (2.6), and γ be a nonnegative concave function on P . We define convex sets as follows P (θ, r; ψ, L) = {x ∈ P : θ(x) < r, ψ(x) < L}, P (θ, r; ψ, L) = {x ∈ P : θ(x) ≤ r, ψ(x) ≤ L}, P (θ, r; ψ, L; γ, a) = {x ∈ P : θ(x) < r, ψ(x) < L, γ(x) > a}, P (θ, r; ψ, L; γ, a) = {x ∈ P : θ(x) ≤ r, ψ(x) ≤ L, γ(x) ≥ a}. 6 L. SHEN, X. LIU, Z. LU EJDE-2010/52 Lemma 2.2 ([2]). Let E be Banach space, P ⊂ E be a cone and r2 ≥ d > b > r1 > 0, L2 ≥ L1 > 0 be constants. Assume θ, ψ : P → [0, +∞) are nonnegative continuous convex functions which satisfy (2.5) and (2.6). γ is a nonnegative concave function on P such that for all x in P (θ, r2 ; ψ, L2 ) satisfies γ(x) ≤ θ(x). T : P (θ, r2 ; ψ, L2 ) → P (θ, r2 ; ψ, L2 ) is a completely continuous operator. Suppose (C1) {x ∈ P (θ, d; ψ, L2 ; γ, b) : γ(x) > b} = 6 φ, and γ(T x) > b, for x ∈ P (θ, d; ψ, L2 ; γ, b); (C2) θ(T x) < r1 , ψ(T x) < L1 , for x ∈ P (θ, r1 ; ψ, L1 ); (C3) γ(T x) > b, for x ∈ P (θ, r2 ; ψ, L2 ; γ, b) with θ(T x) > d. Then T has at least three fixed points x1 , x2 , x3 in P (θ, r2 ; ψ, L2 ). Further, x1 ∈ P (θ, r1 ; ψ, L1 ), x2 ∈ {P (θ, r2 ; ψ, L2 ; γ, b) : γ(x) > b}, x3 ∈ P (θ, r2 ; ψ, L2 )\ P (θ, r1 ; ψ, L1 ) ∪ P (θ, r2 ; ψ, L2 ; γ, b) . 3. Main results Let closed cone P be defined by P = {u ∈ P C 1 [0, 1] : u(t) ≥ 0}. Define operator T : P → P C 1 [0, 1] by Z t Z s T u(t) = u(0) + u0 (0)t + (t − s)φq f (r, u(r), u0 (r))dr ds 0 X 0 X + (t − tk )Ik (u(tk )) + Jk (u(tk )), t ∈ [0, 1], tk <t tk <t 0 which u(0), u (0) are defined in (2.2), (2.3). The nonnegative continuous convex functions θ, ψ, and nonnegative continuous concave function γ are defined by θ(u) = sup u(t), ψ(u) = sup |u0 (t)|, 0≤t≤1 for all u ∈ P , where am = l = R bm am R Iu = M1 = R 1 0 γ(u) = 3tm +tm+1 , 4 bm = min u(t), t∈[am ,bm ] 0≤t≤1 tm +3tm+1 . 4 δ−1 (bm − r)φq (r − am )ds Let q+1 = q(q + 1)(δ − 1) , (1 − tm )q+1 2 max{I1 (u), I2 (u), . . . , Im (u)}, 1−α−β φq (s)ds + m(1 − α − β) + xα + yβ = u ∈ [0, R], 1−α−β , 1/q + m(1 − α − β) + xα + yβ where x and y satisfy tx < ξ < tx+1 , ty < η < ty+1 . Theorem 3.1. Suppose there exist constants r2 ≥ d ≥ δb > b > r1 > 0, L2 ≥ L1 > 0 such that blδ(m + 1/q) blδ(m + 1/q) r2 ≥ , L2 ≥ , (δ − 1)(1 − α − β) 1−α−β and the following conditions hold (H1) f (t, u, v) < φp (min{ δ−1 δ M1 r1 , M1 L1 }), (t, u, v) ∈ [0, 1] × [0, r1 ] × [−L1 , L1 ]; (H2) φp (bl) < f (t, u, v), (t, u, v) ∈ [am , bm ] × [b, d] × [−L2 , L2 ]; (H3) f (t, u, v) < φp (min{ δ−1 δ M1 r2 , M1 L2 }), (t, u, v) ∈ [0, 1) × [0, r2 ] × [−L2 , L2 ]; EJDE-2010/52 MULTIPLICITY OF POSITIVE SOLUTIONS 7 (H4) tk Ik (u) > Jk (u) for u ∈ [0, r2 ], Iur1 < min{ δ−1 δ M1 r1 , M1 L1 }, Iur2 < min{ δ−1 M r , M L }. 1 2 1 2 δ Then boundary-value problem (1.1) has at least three positive solutions u1 , u2 , u3 ∈ P (θ, r2 ; ψ, L2 ) which satisfy sup u1 (t) ≤ r1 , 0≤t≤1 b< min t∈[am ,bm ] sup |u01 (t)| ≤ L1 ; 0≤t≤1 u2 (t) ≤ sup u2 (t) ≤ r2 , 0≤t≤1 sup u3 (t) ≤ δd, 0≤t≤1 sup |u02 (t)| ≤ L2 ; 0≤t≤1 sup |u03 (t)| ≤ L2 . 0≤t≤1 Proof. We need to prove δ−1 δ M1 r1 ≥ bl in order to make sure that the theorem m+1/q makes sense, since we have r2 ≥ blδ (δ−1)(1−α−β) , and (δ − 1)(1 − α − β) δ−1 M1 r 1 = r1 δ δ(1/q + m(1 − α − β) + xα + yβ) m + 1/q δ−1 1−α−β × × blδ ≥ δ 1/q + m (δ − 1)(1 − α − β) = bl. Similarly, we have M1 L2 ≥ M1 r2 (δ − 1) ≥ blδ > bl, so there has no contradiction among conditions. It is easy to see that (1.1) has a solution if and only if Z s Z t T u(t) = u(0) + u0 (0)t + (t − s)φq f (r, u(r), u0 (r))dr ds 0 0 X X + (t − tk )Ik (u(tk )) + Jk (u(tk )), t ∈ [0, 1] tk <t tk <t has a fixed point. Next, we will check the conditions (C1), (C2) and (C3) of Lemma 2.2 are satisfied for the operator T . Obviously, we can get T u(t) ≥ 0, (T u)0 (t) ≥ 0, for all t ∈ [0, 1] and u ∈ P , that also means T u is a monotone increasing function. Firstly, we have θ(u) ≤ r2 , ψ(u) ≤ L2 for all u ∈ P (θ, r2 ; ψ, L2 ). By the condition (H4) tk Ik (u) > Jk (u) and Iur2 < min{ δ−1 δ M1 r2 , M1 L2 }, we get m X k=1 m X δ−1 (1 − tk )Ik (u(tk )) + Jk (u(tk )) ≤ Ik (u(tk )) ≤ m M1 r 2 . δ k=1 φp ( δ−1 δ M1 r2 ), By condition (H3), f (t, u, v) < we obtain Z s δ−1 φq f (t, u(r), u0 (r))dr ≤ M1 r2 φq (s). δ 0 Hence, u(0) ≤ α/q + β/q + xα + yβ 1 m M1 r 2 + M1 r 2 + M1 r 2 . δ(1 − α − β) qδ δ Similarly, u0 (0) ≤ (δ − 1)(α + β + q(xα + yβ)) M1 r 2 . qδ(1 − α − β) 8 L. SHEN, X. LIU, Z. LU EJDE-2010/52 Therefore, we can show that (t − s)φq 0≤t≤1 + X t Z θ(T u) = sup (u(0) + u0 (0)t + 0 s f (r, u(r), u0 (r))dr ds 0 (t − tk )Ik (u(tk )) + tk <t Z X Jk (u(tk ))) tk <t α/q + β/q + xα + yβ 1 m M1 r 2 + M 1 r 2 + M1 r 2 δ(1 − α − β) qδ δ (δ − 1)(1 + mq) (δ − 1)(α + β + q(xα + yβ)) M1 r 2 + M1 r2 + qδ(1 − α − β) qδ 1/q + m(1 − α − β) + xα + yβ = M1 r2 . 1−α−β ≤ 1−α−β Since M1 = 1/q+m(1−α−β)+xα+yβ , we have θ(T u) ≤ r2 . Similarly, we have ψ(T u) = sup |(T u)0 (t)| 0≤t≤1 = sup |u0 (0) + Z 0≤t≤1 ≤ t Z φq ( 0 s f (r, u(r), u0 (r))dr)ds + 0 X Ik (u(tk ))| tk <t 1/q + m(1 − α − β) + xα + yβ M1 L2 = L2 . 1−α−β Therefore, T : P (θ, r2 ; ψ, L2 ) → P (θ, r2 ; ψ, L2 ), and it is easy to see that T is a completely continuous operator. The proof of the condition (C2) in Lemma 2.2 is similar to the one above. To check condition (C1) of Lemma 2.2, we choose u0 = d. It is easy to see that u0 ∈ P (θ, d; ψ, L2 ) and γ(u) = d > b, so {x ∈ P (θ, d; ψ, L2 ; γ, b) : γ(x) > b} = 6 φ. 0 For u ∈ P (θ, d; ψ, L2 ; γ, b), we have b ≤ u(t) ≤ d, |u (t)| ≤ L2 for all t ∈ [am , bm ]. Since T u is a monotone increasing function, and (T u)(t) ≥ 0, t ∈ [0, 1], we have γ(T u) = 0 Z t Z (t − s)φq ( s min u(0) + u (0)t + f (r, u(r), u0 (r))dr)ds t∈[am ,bm ] 0 0 X X + [(t − tk )Ik (u(tk ) + Jk (u(tk )) tk <t tk <t = T u(am ). By (H2) and u(0), u0 (0) defined before, we have φp (bl) < f (t, u, v), (t, u, v) ∈ [am , bm ] × [b, d] × [−L2 , L2 ], EJDE-2010/52 MULTIPLICITY OF POSITIVE SOLUTIONS 9 Z s Z am f (r, u(r), u0 (r))dr)ds (am − s)φq ( T u(am ) = u(0) + u0 (0)am + 0 0 X X + (am − tk )Ik (u(tk )) + Jk (u(tk )) tk <am tk <am ≥ u(0) ≥ > = = 1 δ−1 Z 1 δ−1 Z bl δ−1 bl δ−1 1 s Z 0 0 r Z φq ( bm Z s ds am Z bm f (w, u(w), u0 (w))dw) dr ds 0 Z φq ( am Z s φp (bl)dw)dr am φq (r − am )dr ds am Z bm r am (bm − r)φq (r − am )dr = b. am Thus γ(T u) > b and the condition (C1) of Lemma 2.2 also holds. Finally to prove (C3) of Lemma 2.2, we check γ(T u) > b to be satisfied for all u ∈ P (θ, r2 ; ψ, L2 ; γ, b) with θ(T u) > d. Since T u is a nonnegative monotone increasing function, we can get θ(T u) = sup T u(t) = T u(1), 0≤t≤1 γ(T u) = min t∈[am ,bm ] T u(t) = T u(am ), T u(am ) ≥ T u(0) = d 1 T u(1) > ≥ b; δ δ that is, γ(T u) > b. We have checked Lemma 2.2 to make sure all the conditions are satisfied with the work we have done in the section above. Then T has at least three fixed points u1 , u2 , u3 in P (θ, r2 ; ψ, L2 ). Further, u1 ∈ P (θ, r1 ; ψ, L1 ), u2 ∈ {P (θ, r2 ; ψ, L2 ; γ, b) : γ(x) > b}, u3 ∈ P (θ, r2 ; ψ, L2 )\{P (θ, r1 ; ψ, L1 ) ∪ P (θ, r2 ; ψ, L2 ; γ, b)}. Therefore (1.1) has at least three positive solutions u1 , u2 , u3 . From the boundary conditions we have u3 (1) = δu3 (0) and u3 is a monotone increasing function, so we have 1 1 b > γ(u3 ) = min u3 (t) = u3 (am ) ≥ u3 (0) = u3 (1) = θ(u3 ), am ≤t≤bm δ δ so θ(u3 ) ≤ δb, that means sup0≤t≤1 u3 (t) ≤ δd, and u1 , u2 , u3 satisfy sup u1 (t) ≤ r1 , 0≤t≤1 b< min t∈[am ,bm ] sup |u01 (t)| ≤ L1 ; 0≤t≤1 u2 (t) ≤ sup u2 (t) ≤ r2 , 0≤t≤1 sup u3 (t) ≤ δd, 0≤t≤1 sup |u02 (t)| ≤ L2 ; 0≤t≤1 sup |u03 (t)| ≤ L2 . 0≤t≤1 10 L. SHEN, X. LIU, Z. LU EJDE-2010/52 References [1] Ravi P. Agarwal, Donal O’Regan; A multiplicity result for second order impulsive differential equations via the Leggett-Williams fixed point therom, Appl. Math. Comput. 161 (2005): 433439. [2] Z. Bai, W. Ge; Existence of three positive solutions for some second-order boundary value problems, Comput. Math. Appl. 48 (2004): 699-707. [3] X. Fu, B. Yan, Y. Liu; Introduction of impulsive differential equations system, Science Press, Beijing, 2005 (in Chinese). [4] D. Guo; Second order impulsive integro-differential equation on unbounded domains in Banach spaces, Nonlinear Analysis, 35(1999): 217-221. [5] T. Jankowski; Positive solutions of three-point boundary value problems for second order impulsive differential equations with advanced arguments, Applied Mathematics and Computation, 2008, 197: 179-189. [6] T. Jankowski; Positive solutions to second order four-point boundary value problems for impulsive differential equations, Applied Mathematics and Computation, 2008, 202: 550-561. [7] M. Jia, and X. Liu; Three nonnegative solutions of three-point boundary value problem for second-order impulsive differential equations, Journal of Mathematical Research and Exposition, 2008, 28 (3): 567-574. [8] Eric R. Kaufmanna, N. Kosmatov, Y. N. Raffoul; A second-order boundary value problem with impulsive effects on an unbounded domain, Nonlinear Analysis 2008, 69: 2924-2929. [9] V. Lakshmikantham, D. D. Bainov, P. S. Simeonov; Theory of Impulsive Differential Equations, World Scientific, Singapore, 1989. Li Shen College of Science, University of Shanghai for Science and Technology, Shanghai 200093, China E-mail address: eric0shen@gmail.com Xiping Liu College of Science, University of Shanghai for Science and Technology, Shanghai 200093, China E-mail address: xipingliu@163.com Zhenhua Lu College of Science, University of Shanghai for Science and Technology, Shanghai 200093, China E-mail address: ehuanglu@163.com