• Nenhum resultado encontrado

Existence of three solutions for impulsive multi-point boundary value problems

N/A
N/A
Protected

Academic year: 2017

Share "Existence of three solutions for impulsive multi-point boundary value problems"

Copied!
27
0
0

Texto

(1)

http://dx.doi.org/10.7494/OpMath.2017.37.3.353

EXISTENCE OF THREE SOLUTIONS

FOR IMPULSIVE MULTI-POINT

BOUNDARY VALUE PROBLEMS

Martin Bohner, Shapour Heidarkhani, Amjad Salari,

and Giuseppe Caristi

Communicated by Marek Galewski

Abstract. This paper is devoted to the study of the existence of at least three classical solutions for a second-order multi-point boundary value problem with impulsive effects. We use variational methods for smooth functionals defined on reflexive Banach spaces in order to achieve our results. Also by presenting an example, we ensure the applicability of our results.

Keywords: multi-point boundary value problem, impulsive condition, classical solution, variational method, three critical points theorem.

Mathematics Subject Classification:34B10, 34B15, 34A37.

1. INTRODUCTION

In this paper, we consider the second-order ℓ-point boundary value problem with m-impulsive effects

    

−(φpi(u

i))′ =λFui(t, u1, . . . , un) +µGui(t, u1, . . . , un), t∈(0,1)\Q,

∆φpi(u

i(tj)) =Iij(ui(tj)), j= 1, . . . , m, ui(0) =Pk=1akui(sk), ui(1) =Pk=1bkui(sk)

(φλ,µ)

for i = 1, . . . , n, where Q = {t1, . . . , tm}, pi ∈ (1,∞), φpi(x) = |x|

pi−2x for i =

1, . . . , n, λ > 0, µ ≥ 0 are parameters, m, n, ℓ ∈ N, 0 = t0 < t1 < t2 < . . . <

tm < tm+1 = 1, 0 < s1 ≤s2 ≤ . . .sℓ <1, tj 6=sk, j = 1, . . . , m, k = 1, . . . , ℓ,

F, G: [0,1]×Rn Rare measurable with respect to t, for every (x1, . . . , xn)Rn,

c

(2)

continuously differentiable in (x1, . . . , xn), for almost everyt ∈[0,1] and satisfy the

standard summability condition

sup

|ξ|≤̺1

max{|F, ξ)|, |G(·, ξ)|, |Fξi, ξ)|, |Gξi, ξ)|, i= 1, . . . , n}

∈L1([0,1])

(1.1)

for any̺1>0 withξ= (ξ1, . . . , ξn) and|ξ|= qP

n

i=1ξi2,Fui andGui are the partial

derivatives of F andGwith respect toui, respectively,

∆φpi(u

i(tj)) =φpi(u

i(t+j))−φpi(u

i(t−j)),

where ui(t+j) and ui(t−j) represent the right-hand limit and left-hand limit of ui(t) at t = tj, respectively, Iij ∈ C(R,R), i = 1, . . . , n, j = 1, . . . , m and ak, bk R for

k= 1, . . . , ℓ.

The theory of multi-point boundary value problems for ordinary differential equa-tions arise in different areas of applied mathematics and physics, especially in heat conduction [4, 5, 27, 29], the vibration of cables with nonuniform weights [35], and other problems in nonlinear elasticity [45]. The study of multi-point BVPs for linear second-order ordinary differential equations was initiated by Il’in and Moiseev [26]. From then on, many authors studied more general nonlinear multi-point boundary value problems. Recently, the existence and multiplicity of positive solutions for non-linear multi-point BVPs have received a great deal of attention, we refer the reader to [11, 12, 15, 16, 18–20, 23–25, 34] and the references therein.

On the other hand, impulsive differential equations serve as basic models to study the dynamics of processes that are subjected to sudden changes in their states. These kinds of processes naturally occur in control theory, biology, optimization theory, medicine, and so on (see [6, 10, 28, 36]). The theory of impulsive differential equa-tions has recently received considerable attention, see [2, 3, 6, 30, 33, 39]. There has been increasing interest in the investigation for boundary value problems of nonlin-ear impulsive differential equations during the past few ynonlin-ears, and many works have been published about the existence of solutions for second-order impulsive differential equations. There are some common techniques to approach these problems: Fixed point theorems [8, 9, 31], the method of upper and lower solutions [7], and topological degree theory [37]. In the last few years, variational methods and critical point theory have been used to determine the existence of solutions for impulsive differential equa-tions under certain boundary condiequa-tions, see [1, 21, 43, 44, 46, 48] and the references therein. We note that the difficulties dealing with such problems are that their states are discontinuous. Therefore, the results of impulsive differential equations, especially for higher-order impulsive differential equations, are fewer in number than those for differential equations without impulses.

(3)

and multiplicity of positive solutions of a boundary value problem for second-order three-point nonlinear impulsive integrodifferential equation of mixed type in a real Banach space. In [32], Liu and Yu with the help of the coincidence degree continuation theorem, achieved a general result concerning the existence of solutions of m-point boundary value problems for second-order differential systems with impulses. They also give a definition of autonomous curvature bound set relative to this m-point boundary value problems, and by using this definition and the above existence theo-rem, obtained some simple existence conditions for solutions of these boundary value problems. Meiqiang and Dongxiu in [14], based on fixed point theory in a cone, dis-cussed the existence of solutions for the m-point BVPs for second-order impulsive differential systems, and Thaiprayoon et al. in [42], introduced a new definition of impulsive conditions for boundary value problems of first-order impulsive differential equations with multi-point boundary conditions was introduced, and used the method of lower and upper solutions in reversed order coupled with the monotone iterative technique to obtain the extremal solutions of the boundary value problem.

Motivated by the above works, in this paper we are interested to investigate the ex-istence of at least three nontrivial classical solutions for second-orderℓ-point boundary value problems withm-impulsive effects (φλ,µ) for appropriate values of the parame-tersλand µbelonging to real intervals. Our approach uses variational methods and a three critical points theorem due to Ricceri [38].

Here, we state a special case of our main result.

Theorem 1.1. Let p1, p2>1 such that eithermin{p1, p2} ≥2 ormax{p1, p2}<2,

F :R2Rbe aC1-function satisfying the condition

sup

ξ2 1+ξ

2 2≤̺2

max{|F(ξ1, ξ2)|, |1(ξ1, ξ2)|, |2(ξ1, ξ2)|} ∈L 1([0,1])

for any ̺2 > 0, F(0,0) = 0, I11, I12, I21, I22 ∈ C(R,R) be nondecreasing functions such that Iij(0) = 0 and Iij(s)s > 0,s 6= 0 for i = 1,2, j = 1,2, a1, a2, b1, b2 ∈ R such thata1+a26= 1andb1+b26= 1,0< t1< t2<1,0< s1≤s2<1, andtj6=sk,

j= 1,2,k= 1,2. Assume that

max

(

lim sup

(u1,u2)→(0,0)

F(u1, u2) |u1|p1+|u

2|p2, lim sup |u|→∞

F(u1, u2) |u1|p1+|u

2|p2 )

<0

and

sup uEb1×Eb2

1 R

0

F(u1(t), u2(t))dt

P2

i=1 kuikpipi

pi +

P2

i=1 P2

j=1

uiR(tj)

0

Iij(ζ)dζ >0,

where

b

Ei=

(

ξW1,pi([0,1]) : ξ(0) =a

1ξ(s1)+a2ξ(s2), ξ(1) =b1ξ(s1)+b2ξ(s2) )

(4)

Then, for each compact interval [c, d]⊂(˜λ,∞), where

˜

λ= inf uEb1×Eb2

( P2

i=1 kuikpipi

pi +

P2

i=1 P2

j=1

uiR(tj)

0

Iij(ζ)dζ

1 R

0

F(u1(t), u2(t))dt

:

1 Z

0

F(u1(t), u2(t))dt >0 )

,

there exists R > 0 with the following property: for every λ [c, d] and for every

GC1(R2,R)such that

sup

ξ2 1+ξ

2 2≤̺3

max{|G(ξ1, ξ2)|, |1(ξ1, ξ2)|, |2(ξ1, ξ2)|} ∈L 1([0,1])

for any ̺3 > 0 with G(0,0) = 0, there exists γ > 0 such that, for each µ ∈ [0, γ], the system

    

−|u

i(t)|pi−2ui′′(t) =λFui(u1, u2) +µGui(u1, u2), t∈(0,1)\ {t1, t2},

|ui(t+j)|pi−2u′′i(t+j)− |ui(t−j)|pi−2u′′i(t−j) =Iij(ui(tj)), j= 1,2, ui(0) =a1ui(s1) +a2ui(s2), ui(1) =b1ui(s1) +b2ui(s2)

for i= 1,2, has at least three classical solutions whose norms in the space Eb1×Eb2 are less than R.

2. PRELIMINARIES

In this section, we will introduce some notations, definitions and preliminary facts which are used throughout this paper.

To construct appropriate function spaces and apply critical point theory in order to investigate the existence of solutions for system (φλ,µ), we introduce the following basic notations and results which will be used in the proofs of our main results.

Throughout this article, we letE be the Cartesian product ofnspaces

Ei=

(

ξW1,pi([0,1]) : ξ(0) =

X

k=1

akξ(sk), ξ(1) =

X

k=1

bkξ(sk)

)

fori= 1, . . . , n, i.e.,E=E. . .×En, endowed with the norm

kuk=k(u1, . . . , un)k=

n

X

i=1 kuikpi,

where

kuikpi=

1 Z

0

|ui(t)|pidt

!1

pi

(5)

In this paper, we assume throughout, and without further mention, that the following conditions hold:

(H1) eitherp≥2 orp <2, wherep= min{p1, . . . , pn}andp= max{p1, . . . , pn};

(H2) Pℓk=1ak6= 1 and P

k=1bk 6= 1.

Let

c= max

1≤in

(

sup uiEi\{0}

maxt∈[0,1]|ui(t)|pi kuikpi

pi

)

. (2.1)

Since pi > 1 for i = 1, . . . , n, the embedding E = E. . .×En ֒→ C0([0,1])

n

is compact, and soc <. Moreover, by (H2), from [11, Lemma 3.1], we have

sup vEi\{0}

maxt∈[0,1]|v(t)|pi kvkpi

pi

≤ 12 1 +

P k=1|ak| |1−Pℓk=1ak|

+

P k=1|bk| |1−Pℓk=1bk|

!

(2.2)

fori= 1, . . . , n.

By a classical solution of (φλ,µ), we mean a functionu= (u1, . . . , un) such that,

fori= 1, . . . , n, the left-hand side limit and the right-hand side limit of the derivative uiintj must exist and must be finite,uiC1([0,1]\Q),φp

i(u

i)∈C1([0,1]\Q), and ui satisfies (φλ,µ). We say that a function u = (u1, . . . , un)E is a weak solution

of (φλ,µ) if

1 Z

0 Xn

i=1

φpi(u

i(t))vi′(t)

dt+ n

X

i=1

m

X

j=1

Iij(ui(tj))vi(tj)

λ

1 Z

0

n

X

i=1

Fui(t, u1(t), . . . , un(t))vi(t)dt−µ

1 Z

0

n

X

i=1

Gui(t, u1(t), . . . , un(t))vi(t)dt= 0

for anyv= (v1, . . . , vn)∈W10,p1([0,1])×W 1,p2

0 ([0,1])×. . .×W 1,pn

0 ([0,1]).

Let φpi1 denote the inverse of φpi for everyi = 1, . . . , n. Thenφ

−1

pi =φqi, where

1

pi +

1

qi = 1. It is clear thatφpi is increasing on R,

lim

x→−∞φpi(x) =−∞ and xlim→∞φpi(x) =∞. (2.3) Lemma 2.1. For fixedλ, µ R, u= (u1, . . . , un)∈ (C(tj, tj+1))n,j = 0,1, . . . , m, define αij(x;u) :RR,i= 1, . . . , n,j= 0,1, . . . , m by

αij(x;u)

= tZj+1

tj

φpi1 xλ

δ

Z

0

Fui(t, u1(t), . . . , un(t))dt−µ

δ

Z

0

Gui(t, u1(t), . . . , un(t))dt

!

+

X

k=1

akuk(sk)−

X

k=1

(6)

Then, the equation

αij(x;u) = 0 (2.4)

has a unique solutionxu,i,j.

Proof. Taking (2.3) into account, we have

lim

x→−∞αij(x, u) =−∞ and xlim→∞αij(x, u) =.

Since αij(·, u) is continuous and strictly increasing on R, the conclusion follows

fori= 1, . . . , n andj= 1, . . . , m.

Lemma 2.2. The functionu= (u1, . . . , un)is a solution of the system (φλ,µ)if and only ifui is a solution of the equation

ui(t) =

X

k=1

akuk(sk) + t

Z

0

φpi1 xu,i,jλ δ

Z

0

Fui(t, u1(t), . . . , un(t))dt

µ δ

Z

0

Gui(t, u1(t), . . . , un(t))dt

!

for i = 1, . . . , n, where xu,i,j is the unique solution of (2.4) for j = 0,1, . . . , m, and∆φpi(u

i(tj)) =Iij(ui(tj))fori= 1, . . . , nandj = 0,1, . . . , m.

Proof. This can be verified by direct computations (see [17, Lemma 2.4]).

Lemma 2.3. If a function uE is a weak solution ofλ,µ), then uis a classical solution of (φλ,µ).

Proof. Letu= (u1, . . . , un)E be a weak solution of (φλ,µ). Then

1 Z

0 Xn

i=1

φpi(u

i(t))vi′(t)

dt+ n

X

i=1

m

X

j=1

Iij(ui(tj))vi(tj)

λ

1 Z

0

n

X

i=1

Fui(t, u1(t), . . . , un(t))vi(t)dt

µ

1 Z

0

n

X

i=1

Gui(t, u1(t), . . . , un(t))vi(t)dt= 0

(7)

for anyv = (v1, . . . , vn)∈W10,p1([0,1])×W 1,p2

0 ([0,1])×. . .×W 1,pn

0 ([0,1]). So (2.5)

holds for allv∈W1,p1

0 (tj, tj+1)×W10,p2(tj, tj+1)×. . .×W10,pn(tj, tj+1),v(t) = 0 for

t∈(0,1)\(tj, tj+1) forj= 0,1, . . . , m. Then (2.5) becomes

tZj+1

tj

Xn

i=1

φpi(u′i(t))vi′(t)

dt−λ tZj+1

tj

n

X

i=1

Fui(t, u1(t), . . . , un(t))vi(t)dt

µ tj+1 Z

tj

n

X

i=1

Gui(t, u1(t), . . . , un(t))vi(t)dt= 0

(2.6)

forj = 0,1, . . . , m. Recall that, in one dimension, any weakly differentiable function is absolutely continuous, so that its classical derivative exists almost everywhere, and the classical derivative coincides with the weak derivative. Integrating (2.6) by parts gives

n

X

i=1

tZj+1

tj

[−(φpiu

i)′(t)−λFui(t, u1(t), . . . , un(t))−µGui(t, u1(t), . . . , un(t))]vi(t)dt= 0

forj= 0,1, . . . , m. Thus fori= 1, . . . , n,

−(φpiu

i)′(t)−λFui(t, u1(t), . . . , un(t))−µGui(t, u1(t), . . . , un(t)) = 0 (2.7)

for almost everyt(tj, tj+1),j = 0,1, . . . , m. Then, by Lemmas 2.1 and 2.2, we see

that

ui(t) =

X

k=1

akuk(sk) + t

Z

0

φpi1 xu,i,jλ

δ

Z

0

Fui(t, u1(t), . . . , un(t))dt

µ δ

Z

0

Gui(t, u1(t), . . . , un(t))dt !

fori= 1, . . . , n, wherexu,i,j is the unique solution of (2.4) forj= 0,1, . . . , m. Hence, ui ∈ C1(tj, tj

+1) and φpiu

iC1(tj, tj+1) for i = 1, . . . , n and j = 0,1, . . . , m.

Therefore (2.7) holds fort∈(0,1)\Q. Now we shall show that the impulsive conditions are satisfied. For allv= (v1, . . . , vn)W01,p1([0,1])×W

1,p2

0 ([0,1])×. . .×W 1,pn

0 ([0,1]),

from the equality

(φpiu

i)′(t)vi(t) = d dt

 

t

Z

0

(φpiu

i)′(ζ)dζvi(t)

 

 

t

Z

0

(φpiu

i)′(ζ)dζ

(8)

we have

1 Z

0

piu

i)′(t)vi(t)dt

= 1 Z 0  d dt   t Z 0

(φpiu

i)′(ζ)dζ vi(t)

    t Z 0

(φpiu

i)′(ζ)dζ

 vi′(t)

 dt =vi(1) 1 Z 0

(φpiu

i)′(t)dt

− 1 Z

0  φpi(u

i(t))−φpi(u

i(0))−

X

0≤tj<t

∆φpi(u

i(tj))

 vi′(t)dt

=

 φpi(u

i(1))−φpi(u

i(0))− m

X

j=1

∆φpi(u

i(tj))

 vi(1) − 1 Z 0

φpi(u

i(t))vi′(t)dt+φpi(u

i(0))[vi(1)−vi(0)]

+ m

X

j=1

tZj+1

tj

X

0≤tj<t

∆φpi(u

i(tj))v′i(t)dt

=φpi(u

i(1))vi(1)−φpi(u

i(0))vi(0)− m

X

j=1

∆φpi(u

i(tj))vi(1) − 1 Z 0

φpi(u

i(t))vi′(t)dt− m

X

j=1

∆φpi(u

i(tj))vi(tj) + m

X

j=1

∆φpi(u

i(tj))vi(1)

=−

m

X

j=1

∆φpi(u

i(tj))vi(tj)−

1 Z

0

φpi(u

i(t))vi′(t)dt

(2.8)

fori= 1, . . . , n. Substituting (2.8) into (2.5), we have

n X i=1 1 Z 0

(−(φpiu

i)′(t)−λFui(t, u1(t), . . . , un(t))−µGui(t, u1(t), . . . , un(t)))vi(t)dt

+ n X i=1 m X j=1

[−∆φpi(u

(9)

fori= 1, . . . , n. Sinceusatisfies (2.7), we have

∆φpi(u

(tj))vi(tj) =Iij(ui(tj))vi(tj), j = 0,1, . . . , m

fori= 1, . . . , n. Souis a classical solution of (φλ,µ).

Our main tool is Theorem 2.4 which has been obtained by Ricceri ([38, Theo-rem 2]). It is as follows:

If X is a real Banach space, then denote by WX the class of all functionals Φ :X R possessing the following property: If {un} is a sequence in X converg-ing weakly to u X with lim infn→∞Φ(un)≤ Φ(u), then {un} has a subsequence

converging strongly to u.

For example, if X is uniformly convex and g : [0,∞) → R is a continuous and

strictly increasing function, then, by a classical result, the functional u g(kuk) belongs to the classWX.

Theorem 2.4. LetX be a separable and reflexive real Banach space, letΦ :X →Rbe

a coercive, sequentially weakly lower semicontinuousC1-functional, belonging toW

X,

bounded on each bounded subset of X and whose derivative admits a continuous in-verse on X, and letJ :X →Rbe a C1-functional with compact derivative. Assume

that Φhas a strict local minimumu0 with Φ(u0) =J(u0) = 0. Finally, setting

ρ= max

(

0,lim sup

kuk→∞

J(u)

Φ(u),lim supuu0

J(u) Φ(u)

)

,

σ= sup

u∈Φ−1((0,))

J(u) Φ(u),

assume that ρ < σ. Then for each compact interval [c, d] ⊂ (1

σ,

1

ρ) (with the

con-ventions 10 =∞,1 = 0), there exists R >0 with the following property: for every

λ∈ [c, d] and every C1-functional Ψ : X R with compact derivative, there exists

γ >0such that, for each µ∈[0, γ],

Φ′(u) =λJ′(u) +µΨ′(u)

has at least three solutions inX whose norms are less thanR.

We refer the reader to the papers [22, 41] in which Theorem 2.4 was successfully employed to ensure the existence of at least three solutions for boundary value prob-lems.

Now for every uE, we define

Φ(u) := n

X

i=1 kuikpi

pi

pi +

n

X

i=1

m

X

j=1

uZi(tj)

0

Iij(ζ)dζ, (2.9)

J(u) = T

Z

0

(10)

and

Ψ(u) = T

Z

0

G(t, u1(t), . . . , un(t))dt. (2.11)

Standard arguments show that Φ−µΨλJ is a Gâteaux differentiable functional whose Gâteaux derivative at the pointuE is given by

(Φ′−µΨ′−λJ′)(u)(v)

=

1 Z

0 " n

X

i=1

φpi(u

i(t))v′i(t)

#

dt−λ

1 Z

0

n

X

i=1

Fui(t, u1(t), . . . , un(t))vi(t)dt

µ

1 Z

0

n

X

i=1

Gui(t, u1(t), . . . , un(t))vi(t)dt+

n

X

i=1

m

X

j=1

Iij(ui(tj))vi(tj)

for all v = (v1, . . . , vn) ∈ W10,p1([0,1])×W 1,p2

0 ([0,1])×. . .×W 1,pn

0 ([0,1]). Hence,

a critical point of the functional Φ−µΨλJ gives us a weak solution of (φλ,µ), and in view of Lemma 2.3, every weak solution of the problem (φλ,µ) is a classical one.

We suppose that the impulsive terms satisfy the condition

(I) Iij : R→R is nondecreasing, Iij(0) = 0 and Iij(s)s > 0,s 6= 0 for i= 1, . . . , n and j= 1, . . . , m.

We need the following proposition in the proof of our main result.

Proposition 2.5. Assume that (H1) holds. Let S :EEbe the operator defined by

S(u)(v) =

1 Z

0 " n

X

i=1

φpi(u

i(t))vi′(t)

#

dt+ n

X

i=1

m

X

j=1

Iij(ui(tj))vi(tj)

(11)

Proof. In the proof, we useC1, C2 and C3 to denote appropriate positive constants.

By (I), we have

S(u)(u) = n X i=1 1 Z 0

φpi(u

i(t))u′i(t)dt+ n X i=1 m X j=1

Iij(ui(tj))ui(tj)

= n X i=1 1 Z 0

|ui(t)|pidt+ n X i=1 m X j=1 Iij(ui(tj))ui(tj) ≥ n X i=1      1 Z 0

|ui(t)|pidt

 

1/pi

  pin X i=1      1 Z 0

|ui(t)|pidt

 

1/pi

 

p

C1    n X i=1   1 Z 0

|ui(t)|pidt

 

1/pi

 

p

=C1kukp.

This implies that S is coercive. Now, for any u ∈ (u1, . . . , un)E and v

(v1, . . . , vn)E, we have

hS(u)S(v), uvi=

1 Z 0 " n X i=1

(φpi(u

i(t))−φpi(v

i(t))) (u′i(t)−vi(t))

# dt + n X i=1 m X j=1

(Iij(ui(t))−Iij(vi(t))) (ui(t)−vi(t)).

Then, by [40, Relation (2.2)] and (I), we see that

hS(u)S(v), uvi ≥             

C2Pni=1 1 R

0

|ui(t)−vi′(t)|pidt, p2,

C3Pni=1 1 R

0 |u

i(t)−v

i(t)|

2 (|u

i(t)|+|v

i(t)|)

2−pidt, p <2.

(2.12)

(12)

S−1 exists and it is bounded. So by [17, Relation (2.8)], S−1 is locally Lipschitz continuous and hence continuous. This completes the proof.

Remark 2.6. Suppose that the condition (I) is replaced by the condition

(I’) Iij :RRis odd and nondecreasing inRfor anyi= 1, . . . , nandj= 1, . . . , m.

Then the conclusion of Proposition 2.5 holds again. It is easy to see that the condition (I’) implies the condition (I).

3. MAIN RESULTS

In this section, we formulate our main results. Let us denote by F the class of all functions F : [0,1]×Rn Rthat are measurable with respect to t, for allξRn,

continuously differentiable inξ, for almost everyt[0,1], satisfy the standard summa-bility condition (1.1). Set

A:= 1

2 1 +

P k=1|ak| |1−Pℓk=1ak|

+

P k=1|bk| |1−Pℓk=1bk|

!

.

Let

λ1= inf

uE

( Pn i=1

kuikpipi

pi +

Pn i=1

Pm j=1

uiR(tj)

0

Iij(ζ)dζ

1 R

0

F(t, u(t))dt

:

1 Z

0

F(t, u(t))dt >0

)

andλ2=max{01

0∞}, where

λ0= lim sup |u|→0

1 R

0

F(t, u(t))dt

Pn i=1

kuikpipi

pi +

Pn i=1

Pm j=1

uiR(tj)

0

Iij(ζ)dζ

and

λ∞= lim sup kuk→∞

1 R

0

F(t, u(t))dt

Pn i=1

kuikpipi

pi +

Pn i=1

Pm j=1

uiR(tj)

0

Iij(ζ)dζ

(13)

Theorem 3.1. Suppose that F ∈ F. Assume that

(A1) there exists a constant ε >0 such that

max

(

lim sup u→(0,...,0)

maxt∈[0,1]F(t, u) Pn

i=1|ui|pi

,lim sup

|u|→∞

maxt∈[0,1]F(t, u) Pn

i=1|ui|pi )

< ε,

whereu= (u1, . . . , un) with|u|=pPni=1u2i; (A2) there exists a functionwE such that

n

X

i=1 kwikpi

pi

pi +

n

X

i=1

m

X

j=1

wZi(tj)

0

Iij(ζ)dζ6= 0

and

Apε <

1 R

0

F(t, w(t))dt

Pn i=1

kwikpipi

pi +

Pn i=1

Pm j=1

wiR(tj)

0

Iij(ζ)dζ .

Then, for each compact interval[c, d]⊂(λ1, λ2), there existsR >0with the following property: for every λ[c, d]and every G∈ F, there existsγ >0 such that, for each

µ [0, γ], the system (φλ,µ) has at least three classical solutions whose norms in E

are less than R.

Proof. Take X =E. Clearly, X is a separable and uniformly convex Banach space. Let the functionals Φ, J and Ψ be as given in (2.9), (2.10) and (2.11), respectively. The functional Φ is C1, and due to Proposition 2.5 its derivative admits a contin-uous inverse on X∗. Moreover, by the sequentially weakly lower semicontinuity of

Pn i=1

kuikpipi

pi and the continuity of Iij, i = 1, . . . , n, j = 1, . . . , m, Φ is sequentially

weakly lower semicontinuous inX. On the other hand, we letkuikpi>1,i= 1, . . . , n,

by (I),

Φ(u) = n

X

i=1 kuikpi

pi

pi + n

X

i=1

m

X

j=1

uZi(tj)

0

Iij(ζ)dζ

n

X

i=1 kuikpi

pi

pi

1 pkuk

p (3.1)

for every u= (u1, . . . , un)∈X. Thus Φ is coercive. Moreover, let M be a bounded

subset of X. That is, there exist constantsci >0,i= 1, . . . , n such thatkuikici for eachuM. Then, we have

|Φ(u)| ≤ 1p

n

X

i=1 (

kcikp, ifkuiki≤1,

kcikp, if kuiki>1.

Hence Φ is bounded on each bounded subset of X. Furthermore, Φ ∈ WX. Indeed, let the sequence

(14)

and lim infk→∞Φ(uk) ≤ Φ(u). Since the function Iij is continuous, i = 1, . . . , n,

j= 1, . . . , m, one has

lim inf n→∞

n

X

i=1 kukikpi

pi

pi

n

X

i=1 kuikpi

pi

pi .

Thus,{uk}

k=1 has a subsequence converging strongly to u. Therefore, Φ∈ WX. The

functionalsJand Ψ are two C1-functionals with compact derivatives. Moreover, Φ has

a strict local minimum 0 with Φ(0) = J(0) = 0. In view of (A1), there exist τ1, τ2

with 0< τ1< τ2 such that

F(t, u)≤ε n

X

i=1

|ui|pi (3.2)

for every t ∈[0,1] and everyu= (u1, . . . , un) with |u| ∈[0, τ1)∪(τ2,∞). By (1.1),

F(t, u) is bounded on [0,1]×[τ1, τ2]. Thus we can chooseη >0 andυ > psuch that

F(t, u)≤ε n

X

i=1

|ui|pi+η

n

X

i=1 |ui|υ

for all (t, u)∈[0,1]×Rn. So, by (2.2), we have

J(u) n

X

i=1 kuikpi

pi+η

n

X

i=1

Aυ/pikuikυ

pi (3.3)

for alluX. Hence, from (3.3), we have

lim sup

|u|→0

J(u)

Φ(u) ≤Apε. (3.4)

Moreover, by using (3.2), for eachuX\ {0}, we obtain

J(u) Φ(u) =

R

|u|≤τ2

F(t, u(t))dt

Φ(u) +

R

|u|2

F(t, u(t))dt

Φ(u)

≤supt∈[0,1],|u|∈[02]F(t, u)

Φ(u) +

Pni=1kuikpi

pi

Φ(u)

≤supt∈[0,1],|u|∈[02]F(t, u) Pn

i=1 kuikpipi

pi

+Apε.

So, we get

lim sup

kuk→∞

J(u)

Φ(u) ≤Apε. (3.5)

In view of (3.4) and (3.5), we have

ρ= max

(

0,lim sup

kuk→∞

J(u)

Φ(u),ulim sup→(0,...,0)

J(u) Φ(u)

)

(15)

Assumption (A2) in conjunction with (3.6) yields

σ= sup

u∈Φ−1((0,))

J(u)

Φ(u)= supX\{0}

J(u) Φ(u)

≥ 1 R

0

F(t, w(t))dt

Φ(w(t)) =

1 R

0

F(t, w(t))dt

Pn i=1

kwikpipi

pi +

Pn i=1

Pm j=1

wiR(tj)

0

Iij(ζ)dζ

> Apερ.

Thus, all the hypotheses of Theorem 2.4 are satisfied. Clearly,λ1 = 1β and λ2 = α1. Then, using Theorem 2.4, taking Lemma 2.3 into account, for each compact interval [c, d] ⊂(λ1, λ2), there exists R >0 with the following property: for everyλ∈ [c, d]

and everyG∈ F there existsγ >0 such that, for eachµ[0, γ], the system (φλ,µ) has at least three classical solutions whose norms in Eare less than R.

Another announced application of Theorem 2.4 reads as follows.

Theorem 3.2. Suppose that F ∈ F. Assume that

max

(

lim sup u→(0,...,0)

maxt∈[0,1]F(t, u) Pn

i=1|ui|pi

,lim sup

|u|→∞

maxt∈[0,1]F(t, u) Pn

i=1|ui|pi )

<0 (3.7)

whereu= (u1, . . . , un)with|u|=pPni=1u2i, and

sup uE

1 R

0

F(t, u(t))dt

Pn i=1

kuikpipi

pi +

Pn i=1

Pm j=1

uiR(tj)

0

Iij(ζ)dζ

>0. (3.8)

Then for each compact interval [c, d]⊂(λ1,∞) there existsR >0 with the following property: for everyλ[c, d] and everyG∈ F, there exists γ >0 such that for each

µ [0, γ], the system (φλ,µ) has at least three classical solutions whose norms in E

are less than R.

Proof. In view of (3.7), there exist an arbitrary ε > 0 andτ1, τ2 with 0 < τ1 < τ2

such that

F(t, u)≤ε n

X

i=1 |ui|pi

for every t ∈[0,1] and everyu= (u1, . . . , un) with |u| ∈[0, τ1)∪(τ2,∞). By (1.1),

F(t, u) is bounded on [0,1]×[τ1, τ2]. Thus we can chooseη >0 andυ > pin a manner

that

F(t, u)≤ε n

X

i=1

|ui|pi+η

n

X

(16)

for all (t, u)∈ [0,1]×Rn. So, by the same process as in the proof of Theorem 3.1,

we obtain (3.4) and (3.5). Sinceǫis arbitrary, (3.4) and (3.5) give

max

(

0, lim sup

kuk→+∞

J(u)

Φ(u),ulim sup→(0,...,0)

J(u) Φ(u)

) ≤0.

Then, with the notation of Theorem 2.4, we haveρ= 0. By (3.8), we also haveσ >0. In this case, clearly λ1 = σ1 and λ2 = ∞. Thus, by using Theorem 2.4 and taking

Lemma 2.3 into account, the result is achieved.

Remark 3.3. Theorem 1.1 immediately follows from Theorem 3.2.

Remark 3.4. In Assumption (A2), if we choose

w(t) =w⋆(t) = (0, . . . ,0, wn(t)) (3.9)

with

wn(t) =

               δ P

k=1ak+

2 1−P

k=1

ak

s1 t

, if t∈[0,s1

2),

δ, if t[s1

2, 1+sℓ

2 ],

δ

2−P

k=1

bksℓP k=1

bk

1−sℓ

2(1−P

k=1

bk)

1−sℓ t

, if t∈(1+sℓ

2 ,1],

(3.10)

whereδ >0, then (A2) takes the following form:

(A′

2) there exists a positive constantδ such that

(ωnδ)pn+pn

m

X

j=1

wZn(tj)

0

Inj(ζ)dζ6= 0

and Apε < pn 1 R 0

F(t, w(t))dt

(ωnδ)pn+pnPm

j=1

wnR(tj)

0

Inj(ζ)dζ .

Clearly,w⋆E and

Φ(w) =(ωnδ) pn

pn +

m

X

j=1

wZn(tj)

0

Inj(ζ)dζ,

where

ωn:=

"

2pn−1 s1−pn

1 1− X k=1 ak pn

+ (1−sℓ)1−pn

! 1− X k=1 bk

pn#1/pn

(17)

Now, we point out some results in which the functionF has separated variables. To be precise, we consider the system

    

−(φpi(u

i))′ =λθ(t)Fui(u1, . . . , un) +µGui(t, u1, . . . , un), t∈(0,1)\Q,

∆φpi(u

i(tj)) =Iij(ui(tj)), j= 1, . . . , m, ui(0) =Pk=1akui(sk), ui(1) =Pk=1bkui(sk),

θ λ,µ)

where θ : [0,1]→ Ris a nonzero function such that θ L1([0,1]) and F : Rn R

is a C1-function and G : [0,1]×Rn R is as introduced for the system (φλ,µ) in Section 1.

Set F(t, x1, . . . , xn) = θ(t)F(x1, . . . , xn) for every (t, x1, . . . , xn) ∈ [0,1]×Rn.

The following existence results are consequences of Theorem 3.1.

Theorem 3.5. Assume that

(A′

1) there exists a constant ε >0 such that

sup t∈[0,1]

θ(t).max

(

lim sup u→(0,...,0)

F(u)

Pn i=1|ui|pi

,lim sup

|u|→∞

F(u)

Pn i=1|ui|pi

)

< ε,

whereu= (u1, . . . , un) with|u|=pPni=1u2i; (A′′

2) there exists a positive constantδ such that

(ωnδ)pn+pn

m

X

j=1

wZn(tj)

0

Inj(ζ)dζ6= 0

and

Apε <

pn

1 R

0

F(t, w(t))dt

(ωnδ)pn+pnPm

j=1

wnR(tj)

0

Inj(ζ)dζ

wherew⋆ andω

n are given by (3.9)and (3.10), respectively.

Then, for each compact interval[c, d]⊂(λ3, λ4), where λ3 andλ4are the same asλ1 and λ2, but

R1

0 F(t, u(t))dt is replaced by R1

0 θ(t)F(u(t))dt, respectively, there exists

R > 0 with the following property: for every λ ∈ [c, d] and every G ∈ F, there existsγ >0such that for eachµ∈[0, γ], the systemθ

λ,µ)has at least three classical

solutions whose norms in E are less thanR.

Theorem 3.6. Assume that there exists a positive constantδ such that

(ωnδ)pn+pn

m

X

j=1

wZn(tj)

0

Inj(ζ)dζ >0and 1 Z

0

(18)

wherew⋆ andωn are given by (3.9)and (3.10), respectively. Moreover, suppose that

lim sup u→(0,...,0)

F(u)

Pn i=1|ui|pi

= lim sup

|u|→∞

F(u)

Pn i=1|ui|pi

= 0, (3.12)

whereu= (u1, . . . , un)with|u|=pPni=1u2i. Then, for each compact interval[c, d]⊂ (λ3,∞)whereλ3 is the same asλ1 butR01F(t, u(t))dtis replaced byR01θ(t)F(u(t))dt, there exists R >0 with the following property: for every λ[c, d] and every G∈ F, there exists γ >0 such that for each µ[0, γ], the systemθλ,µ) has at least three

classical solutions whose norms in E are less than R.

Proof. We easily observe that, from (3.12), the assumption (A′

1) is satisfied for every

ε > 0. Moreover, using (3.11), by choosing ε > 0 small enough, one can derive the assumption (A′′

2). Hence, the conclusion follows from Theorem 3.5.

Now, we exhibit an example in which the hypotheses of Theorem 3.6 are satisfied.

Example 3.7. Letn= 2,p1=p2= 2,m=l= 1,t1 = 13, s1= 12,a1=b1= 2 and

I11(x) =I21(x) =x3 for each x∈R. Let θ(t) = [t] + 1 for all t ∈[0,1], where [t] is

the integer part oftand

F(x1, x2) = (

(x2

1+x22)2, ifx21+x22<1,

1, ifx21+x221.

By choosingδ= 1, we havew(t) =w⋆(t) = (0, w2(t)) with

w2(t) =     

2(1−2t) ift[0,14),

1 ift∈[1

4, 3 4], −2(1−2t) ift(34,1],

andω2= 2 √

2. Thus we have

(ω2δ)p2+p2

m

X

j=1

wZ2(tj)

0

I2j(ζ)dζ= (2 √

2)2+ 2

1 Z

0

ζ3dζ= 17 2 >0,

1 Z

0

θ(t)F(w(t))dt=

1 4 Z

0

F(0,2(1−2t))dt+

3 4 Z

1 4

F(0,1)dt+

1 Z

3 4

F(0,−2(1−2t))dt

=

1 4 Z

0

16(1−2t)4dt+

3 4 Z

1 4

dt+

1 Z

3 4

dt= 23 10>0,

lim

(u1,u2)→(0,0)

F(u1, u2)

u21+u22

= lim

(u1,u2)→(0,0)

(u2 1+u22)2

u21+u22

= lim

(u1,u2)→(0,0)

(19)

and

lim

|u|→∞

F(u1, u2)

u2 1+u22

= lim

|u|→∞

1 u2

1+u22

= 0,

where u= (u1, u2) with|u| = p

u21+u22. Hence, by applying Theorem 3.6 for each

compact interval [c, d] ⊂(0,∞), there exists R >0 with the following property: for every λ [c, d] and every G∈ F, there exists γ > 0 such that, for eachµ [0, γ], the system

                  

u′′

1(t) =λ([t] + 1)Fu1(u1, u2) +µGu1(t, u1, u2), t∈(0,1)\ { 1 3},u′′2(t) =λ([t] + 1)Fu2(u1, u2) +µGu2(t, u1, u2), t∈(0,1)\ {

1 3},

u′1(13 +

)−u′1(13 −

) = (u1(13))3,

u′ 2(13

+

)−u′ 2(13

) = (u2(13))3,

u1(0) = 2u1(12), u1(1) = 2u1(12),

u2(0) = 2u2(12), u2(1) = 2u2(12)

has at least three classical solutions whose norms in the space

e

E=

(

(ξ1, ξ2)∈W1,2([0,1])×W1,2([0,1]) :ξ1(0) =ξ1(1) = 2ξ1

1 2

,

ξ2(0) =ξ2(1) = 2ξ2

1 2

)

are less thanR.

4. SINGLE IMPULSE

As an application of the results from Section 3, we consider the problem

    

−(φp(u′))=λf(t, u) +µg(t, u), t(0,1)\ {t 1},

∆φp(u′(t

1)) =I(u(t1)),

u(0) =u(1) =u(s1),

(4.1)

where p > 1, 0 < t1, s1 < 1, t1 6= s1, φp(x) = |x|p−2x, λ > 0, µ ≥ 0, and f, g :

[0,1]×RRare two L1-Carathéodory functions, ∆φpui(t1) =φpu(t+

1)−φpu′(t−1),

whereu(t+

1) andu′(t−1) represent the right-hand limit and left-hand limit ofu′(t) at

t=t1, respectively, and I:R→Ris a continuous and nondecreasing function such

thatI(0) = 0 andI(s)s >0 for alls∈R\ {0}.

We introduce the functionsF : [0,1]×RRandG: [0,1]×RR, respectively,

as

F(t, x) = x

Z

0

(20)

and

G(t, x) = x

Z

0

g(t, ζ)dζ for all (t, x)∈[0,1]×R.

The following two theorems are consequences of Theorems 3.1 and 3.2, respectively.

Theorem 4.1. Assume that

(B1) there exists a constantε >0 such that

max

(

lim sup u→0

maxt∈[0,1]F(t, u)

|u|p , lim sup

|u|→∞

maxt∈[0,1]F(t, u) |u|p

)

< ε;

(B2) there exists a functionwEb, where

b

E=

(

ξW1,p([0,1]) : ξ(0) =ξ(1) =ξ(s1) )

,

such that

kwkpp+p wZ(t1)

0

I(ζ)dζ6= 0

and

p2ε < 2

1 R

0

F(t, w(t))dt

kukpp+p uR(t1)

0

I(ζ)dζ .

Then, for each compact interval [c, d]⊂(¯λ1,¯λ2), where

¯ λ1= inf

uEb

(kukp p+p

uR(t1)

0

I(ζ)dζ

p

1 R

0

F(t, u(t))dt :

1 Z

0

F(t, u(t))dt >0

)

and

¯

λ2= max         

0,lim sup

|u|→0

p

1 R

0

F(t, u(t))dt

kukpp+p uR(t1)

0

I(ζ)dζ

, lim sup

kukp→∞

p

1 R

0

F(t, u(t))dt

kukpp+p u(Rt1)

0

I(ζ)dζ

        

,

there existsR >0 with the following property: for everyλ[c, d], there existsγ >0

(21)

Theorem 4.2. Assume that

max

(

lim sup u→0

supt∈[0,1]F(t, u(t))

|u|p , lim sup

|u|→∞

supt∈[0,1]F(t, u(t)) |u|p

) ≤0

and

sup uEb

p

1 R

0

F(t, u(t))dt

kukpp+p u(Rt1)

0

I(ζ)dζ >0.

Then for each compact interval [c, d]⊂(¯λ1,∞), whereλ¯1 is defined in Theorem 4.1, there existsR >0 with the following property: for everyλ∈[c, d], there existsγ >0

such that for each µ∈ [0, γ], the problem (4.1) has at least three classical solutions whose norms inEb are less than R.

Now letf :RRbe a continuous function. Put

F(x) = x

Z

0

f(ζ)dζ for allx∈R.

The following theorems are immediate consequences of Theorems 3.5 and 3.6, respec-tively.

Theorem 4.3. Assume that

(B′

1) there exists a constantε >0 such that

max

(

lim sup u→0

F(u)

|u|p , lim sup

|u|→∞

F(u)

|u|p

)

< ε;

(B′′

2) there exists a positive constantδ such that

2p(p−1)δps11−p+ (1−s1)1−p

+p δ

Z

0

I(ζ)dζ6= 0

and

pε <

2pn

1 R

0

F(w(t))dt

2p(p−1)δps1−p

1 + (1−s1)1−p

+p δ

R

0

I(ζ)dζ ,

where

w(t) =

    

2δ

s1t, if t∈[0,

s1 2),

δ, if t∈[s1 2,

1+s1 2 ], 2δ

1−s1(1−t), if t∈( 1+s1

2 ,1].

(22)

Then, for each compact interval [c, d] ⊂(¯λ3¯4), where λ¯3 and λ¯4 are the same as

¯

λ1 and λ¯2, but R01F(t, u(t))dt is replaced by R01F(u(t))dt, respectively, there exists

R >0 with the following property: for everyλ[c, d]and every continuous function

g:RR, there existsγ >0such that for eachµ[0, γ], the problem

    

−(φp(u′))′=λf(u) +µg(u), t(0,1)\ {t1},

∆φp(u′(t

1)) =I(u(t1)),

u(0) =u(1) =u(s1)

(4.3)

has at least three classical solutions whose norms in Eb are less than R. Theorem 4.4. Assume that there exists a positive constantδ such that

2p(p−1)δps11−p+ (1−s1)1−p

+p δ

Z

0

I(ζ)dζ >0 and 1 Z

0

F(w(t))dt >0,

wherew is given by (4.2). Moreover, suppose that

lim sup u→0

f(u)

|u|p−1 = lim sup |u|→∞

f(u)

|u|p−1 = 0.

Then, for each compact interval [c, d] ⊂(¯λ3,+∞), where ¯λ3 is the same as ¯λ1, but R1

0 F(t, u(t))dt is replaced by R1

0 F(u(t))dt, there existsR >0with the following prop-erty: for every λ∈[c, d] and every continuous functiong:RR, there existsγ >0

such that for each µ∈ [0, γ], the problem (4.3) has at least three classical solutions whose norms inEb are less than R.

Finally, we present the following example in order to illustrate Corollary 4.4.

Example 4.5. Letp= 3,t1= 23,s1= 12,I(x) =√3xfor allx∈Randf(x) =−x3ex

for allx∈R. By choosing δ= 1, we have

w(t) =

    

4t, if t∈[0,1 4),

1, if t[14,34], 4(1−t), if t∈(3

4,1].

Thus

2p(p−1)δps11−p+ (1−s1)1−p

+p δ

Z

0

I(ζ)dζ= 29+ 3

1 Z

0 3 p

(23)

1 Z

0

F(w(t))dt=− 1 4 Z

0 4t

Z

0

ζ3eζdζdt− 3 4 Z

1 4

1 Z

0

ζ3eζdζdt− 1 Z

3 4

4(1Zt)

0

ζ3eζdζdt

=

1 4 Z

0

e−4t(64t3+ 58t2+ 24t+ 6)−6dt+

16 e −6

3 4 Z

1 4

dt

+ 2 e4

1 Z

3 4

e4t(76−166t+ 125t2−32t3)−6dt

= 29

6 +

8 e

1089 16e4 +

122 64e7 −

70 32e8 >0.

Also limu→0f|u(u|2) = lim|u|→∞

f(u)

|u|2 = 0. Hence, by applying Corollary 4.4 for each

compact interval [c, d] ⊂(0,∞), there exists R >0 with the following property: for every λ [c, d] and every continuous functiong : R R, there exists γ > 0 such that, for eachµ[0, γ], the problem

      

−|u′1(t)|u′′1(t) =−λu(t)3eu(t)+µg(u), t∈(0,1)\ {23}, |u′(2

3 +

)|u′(2 3 +

)− |u′(2 3 −

)|u′1(23 −

) = 3 q

u(2 3),

u(0) =u(1) =u(1 2)

has at least three classical solutions whose norms in the space

e

E1= (

ξ∈W1,3([0,1]) : ξ(0) =ξ(1) =ξ

1 2

)

are less thanR.

REFERENCES

[1] L. Bai, B. Dai,An application of variational method to a class of Dirichlet boundary value problems with impulsive effects, J. Franklin Inst.348(2011) 9, 2607–2624. [2] D.D. Ba˘ınov, P.S. Simeonov,Systems with Impulse Effect. Stability, Theory and

Appli-cations, Ellis Horwood Series in Mathematics and Its Applications, New York, 1989. [3] M. Benchohra, J. Henderson, S.K. Ntouyas,Impulsive Differential Equations and

In-clusions, Contemporary Mathematics and Its Applications, vol. 2, Hindawi Publishing Corporation, New York, 2006.

(24)

[5] J.R. Cannon, The One-dimensional Heat Equation, vol. 23, Encyclopedia of Mathe-matics and its Applications, Addison-Wesley Publishing Company, Advanced Book Program, Reading, MA, 1984.

[6] T.E. Carter,Necessary and sufficient conditions for optimal impulsive rendezvous with linear equations of motion, Dynam. Control10(2000) 3, 219–227.

[7] L. Chen, J. Sun,Nonlinear boundary value problem of first order impulsive functional differential equations, J. Math. Anal. Appl.318(2006) 2, 726–741.

[8] J. Chen, C.C. Tisdell, R. Yuan,On the solvability of periodic boundary value problems with impulse, J. Math. Anal. Appl.331(2007) 2, 902–912.

[9] J. Chu, J.J. Nieto,Impulsive periodic solutions of first-order singular differential equa-tions, Bull. Lond. Math. Soc.40(2008) 1, 143–150.

[10] B. Dai, H. Su, D. Hu,Periodic solution of a delayed ratio-dependent predator-prey model with monotonic functional response and impulse, Nonlinear Anal.70(2009) 1, 126–134. [11] Z. Du, L. Kong,Existence of three solutions for systems of multi-point boundary value

problems, Electron. J. Qual. Theory Diff. Equ., Spec. Ed. I,10(2009).

[12] H.-Y. Feng, W.-G. Ge,Existence of three positive solutions forM-point boundary-value problem with one-dimensionalP-Laplacian, Taiwanese J. Math.14(2010) 2, 647–665. [13] M. Feng, H. Pang, A class of three-point boundary-value problems for second-order impulsive integro-differential equations in Banach spaces, Nonlinear Anal.70(2009) 1, 64–82.

[14] M. Feng, D. Xie,Multiple positive solutions of multi-point boundary value problem for second-order impulsive differential equations, J. Comput. Appl. Math. 223 (2009) 1, 438–448.

[15] W. Feng, J.R.L. Webb,Solvability ofm-point boundary value problems with nonlinear growth, J. Math. Anal. Appl.212(1997) 2, 467–480.

[16] J.R. Graef, L. Kong, Existence of solutions for nonlinear boundary value problems, Comm. Appl. Nonlinear Anal.14(2007) 1, 39–60.

[17] J.R. Graef, S. Heidarkhani, L. Kong,A critical points approach to multiplicity results for multi-point boundary value problems, Appl. Anal.90(2011) 12, 1909–1925. [18] J.R. Graef, S. Heidarkhani, L. Kong,Infinitely many solutions for systems of multi-point

boundary value problems using variational methods, Topol. Methods Nonlinear Anal.42 (2013) 1, 105–118.

[19] J.R. Graef, L. Kong, Q. Kong,Higher order multi-point boundary value problems, Math. Nachr.284(2011) 1, 39–52.

[20] S. Heidarkhani, Multiple solutions for a class of multipoint boundary value systems driven by a one-dimensional(p1, . . . , pn)-Laplacian operator, Abstr. Appl. Anal.2012

(2012), Article ID 389530.

(25)

[22] S. Heidarkhani, A. Salari, Existence of three solutions for impulsive perturbed elastic beam fourth-order equations of Kirchhoff-type, Studia Sci. Math. Hungar. (2016), to appear.

[23] J. Henderson, Solutions of multipoint boundary value problems for second order equa-tions, Dynam. Systems Appl.15(2006) 1, 111–117.

[24] J. Henderson, B. Karna, C.C. Tisdell, Existence of solutions for three-point bound-ary value problems for second order equations, Proc. Amer. Math. Soc. 133(2005) 5, 1365–1369.

[25] J. Henderson, S.K. Ntouyas, Positive solutions for systems of nth order three-point nonlocal boundary value problems, Electron. J. Qual. Theory Differ. Equ.18(2007). [26] V.A. Il′in, E.I. Moiseev,A nonlocal boundary value problem of the second kind for the

Sturm-Liouville operator, Differentsial′nye Uravneniya23(1987) 8, 1422–1431. [27] N.I. Ionkin,The solution of a certain boundary value problem of the theory of heat

con-duction with a nonclassical boundary condition, Differencial′nye Uravnenija13(1977) 2, 294–304.

[28] G. Jiang, Q. Lu, L. Qian,Complex dynamics of a Holling type II prey-predator system with state feedback control, Chaos Solitons Fractals31(2007) 2, 448–461.

[29] L.I. Kamynin, A boundary-value problem in the theory of heat conduction with non-classical boundary conditions, Ž. Vyčisl. Mat. i Mat. Fiz.4(1964), 1006–1024. [30] V. Lakshmikantham, D.D. Ba˘ınov, P.S. Simeonov, Theory of Impulsive Differential

Equations, vol. 6, Series in Modern Applied Mathematics, World Scientific Publishing Co., Teaneck, NJ, 1989.

[31] J. Li, J.J. Nieto,Existence of positive solutions for multipoint boundary value problem on the half-line with impulses, Bound. Value Probl. (2009), 2009:834158.

[32] B. Liu, J. Yu,Existence of solution ofm-point boundary value problems of second-order differential systems with impulses, Appl. Math. Comput.125(2002) 2–3, 155–175. [33] X. Liu, A.R. Willms,Impulsive controllability of linear dynamical systems with

appli-cations to maneuvers of spacecraft, Math. Probl. Eng.2(1996) 4, 277–299.

[34] R. Ma,Existence of positive solutions for superlinear semipositone m-point boundary--value problems, Proc. Edinb. Math. Soc.46(2003) 2, 279–292.

[35] M. Moshinsky,On one-dimensional boundary value problems of a discontinuous nature, Bol. Soc. Mat. Mexicana4(1947), 1–25.

[36] S.I. Nenov,Impulsive controllability and optimization problems in population dynamics, Nonlinear Anal.36(1999), 881–890.

[37] D. Qian, X. Li, Periodic solutions for ordinary differential equations with sublinear impulsive effects, J. Math. Anal. Appl.303(2005) 1, 288–303.

[38] B. Ricceri, A further three critical points theorem, Nonlinear Anal. 71 (2009) 9, 4151–4157.

(26)

[40] J. Simon,Régularité de la solution d’une équation non linéaire dansRN

, [in:] Journées d’Analyse Non Linéaire (Proc. Conf., Besançon, 1977), vol. 665, Lecture Notes in Math., Springer, Berlin, 1978, 205–227.

[41] J. Sun, H. Chen, J.J. Nieto, M. Otero-Novoa,The multiplicity of solutions for perturbed second-order Hamiltonian systems with impulsive effects, Nonlinear Anal.72(2010) 12, 4575–4586.

[42] C. Thaiprayoon, D. Samana, J. Tariboon,Multi-point boundary value problem for first order impulsive integro-differential equations with multi-point jump conditions, Bound. Value Probl.2012, 2012:38.

[43] Y. Tian, W. Ge, Applications of variational methods to boundary-value problem for impulsive differential equations, Proc. Edinb. Math. Soc.51(2008) 2, 509–527. [44] Y. Tian, W. Ge,Variational methods to Sturm-Liouville boundary value problem for

impulsive differential equations, Nonlinear Anal.72(2010) 1, 277–287.

[45] S.P. Timoshenko, Theory of Elastic Stability, 2nd ed., McGraw-Hill Book Co., New York, 1961.

[46] J. Xiao, J.J. Nieto, Z. Luo, Multiplicity of solutions for nonlinear second order im-pulsive differential equations with linear derivative dependence via variational methods, Commun. Nonlinear Sci. Numer. Simul.17(2012) 1, 426–432.

[47] E. Zeidler,Nonlinear functional analysis and its applications. II/A: Linear monotone operators, Springer-Verlag, New York, 1990.

[48] H. Zhang, Z. Li,Variational approach to impulsive differential equations with periodic boundary conditions, Nonlinear Anal. Real World Appl.11(2010) 1, 67–78.

Martin Bohner bohner@mst.edu

Department of Mathematics and Statistics Missouri S&T, Rolla

MO 65409-0020, USA

Shapour Heidarkhani s.heidarkhani@razi.ac.ir

Razi University Faculty of Sciences

(27)

Amjad Salari

amjads45@yahoo.com

Razi University Faculty of Sciences

Department of Mathematics 67149 Kermanshah, Iran

Giuseppe Caristi gcaristi@unime.it

University of Messina Department of Economics Messina, Italy

Referências

Documentos relacionados

T: Não, nós estamos a abrir o espaço para isso acontecer no futuro, mas o que nós não queremos é que venha alguém de fora com 10 anos de murais e muita técnica, fazer um mural

Tendo como objetivos principais o desenvolvimento do pensamento algébrico dos alunos participantes e a exploração das potencialidades do App Inventor, designer de

Durante este período, ao lado dos trabalhos «extraordinários» para A Editora e com o declinar da sua ligação ao jornal O Século e à Empresa da História de Portugal, Roque

Desde 2008 o nosso grupo de investigação tem-se dedicado à síntese e transformação de quinolin-4(1H)-onas e acridin-9(10H)-onas, [23-25] com o objetivo de desenvolver novas

Desenvolver a leitura e atenção, através da leitura de um livro (trazido por ele), com personagens para encontrar (“Cucu, onde está o robot”).. 116 Sessão: Ficha

A sobremesa diet de maracujá acrescida de probiót ico, La ctob acil lus para case i, e de prebióticos, inulina e oligofrutose, obteve boa aceitação pelos provador es e apr esentou

Embora haja disposições legais específicas para esse tipo societário, sua constituição não precisa, necessariamente, limitar-se a esta forma básica, podendo ser

Ambos tratam sobre a confidencialidade localizando-a na fase negocial, ou seja, sobre aquelas informações reputadas confidenciais que são transmitidas entre as