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Volume 2010, Article ID 325415,16pages doi:10.1155/2010/325415

Research Article

Variational Approach to Impulsive Differential

Equations with Dirichlet Boundary Conditions

Huiwen Chen and Jianli Li

Department of Mathematics, Hunan Normal University, Changsha, Hunan 410081, China

Correspondence should be addressed to Jianli Li,[email protected]

Received 18 September 2010; Accepted 9 November 2010

Academic Editor: Zhitao Zhang

Copyrightq2010 H. Chen and J. Li. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

We study the existence ofndistinct pairs of nontrivial solutions for impulsive differential equations

with Dirichlet boundary conditions by using variational methods and critical point theory.

1. Introduction

Impulsive effects exist widely in many evolution processes in which their states are changed abruptly at certain moments of time. Such processes are naturally seen in control theory1,2, population dynamics3, and medicine4,5. Due to its significance, a great deal of work has been done in the theory of impulsive differential equations. In recent years, many researchers have used some fixed point theorems6,7, topological degree theory8, and the method of lower and upper solutions with monotone iterative technique9to study the existence of solutions for impulsive differential equations.

On the other hand, in the last few years, some researchers have used variational methods to study the existence of solutions for boundary value problems10–16, especially, in 14–16, the authors have studied the existence of infinitely many solutions by using variational methods.

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Motivated by the above facts, in this paper, our aim is to study the existence of n

distinct pairs of nontrivial solutions to the Dirichlet boundary problem for the second-order impulsive differential equations

ut λht, ut 0, t /tj, a.e. t∈0, T,

−Δutj

Ij

utj

, j1,2, . . . , p,

u0 uT 0,

1.1

where 0t0 < t1 <· · ·< tp < tp1T,λ >0,hC0, T×R, R,IjCR, R,j 1,2, . . . , p,

Δutj utjutj−,utjandutjdenote the right and the left limits, respectively, of

utjatttj,j1,2, . . . , p.

2. Preliminaries

Definition 2.1. Suppose thatEis a Banach space andϕC1E, R. If any sequence{u

k} ⊂ E

for whichϕukis bounded andϕuk → 0 ask → ∞possesses a convergent subsequence

inE, we say thatϕsatisfies the Palais-Smale condition.

LetEbe a real Banach space. Define the setΣ {A|AE\ {θ}as symmetric closed set}.

Theorem 2.2 see 17, Theorem 3.5.3. Let E be a real Banach space, and let ϕC1E, R

be an even functional which satisfies the Palais-Smale condition, ϕ is bounded from below and

ϕ0 0; suppose that there exists a setK ⊂ Σ and an odd homeomorphismh : KSn−1n

one-dimensional unit sphereandsupxKϕx<0, thenϕhas at least n distinct pairs of nontrivial critical points.

To begin with, we introduce some notation. Denote byX the Sobolev spaceH1 00, T,

and consider the inner product

u, v

T

0

utvtdt 2.1

and the norm

u

T

0

ut2 dt

1/2

. 2.2

Hence,Xis reflexive. We define the norm inC0, Tasx∞maxt∈0,T|xt|.

ForuH20, T, we have thatuanduare absolutely continuous andu L20, T.

Hence,Δut utut− 0 for everyt ∈ 0, T. If uH1

00, T, thenuis absolutely

continuous anduL20, T. In this case, the one-sided derivatives ut−,ut may not exist. As a consequence, we need to introduce a different concept of solution. Suppose that

uC0, Tsuch that for everyj 1,2, . . . , p,uj u|tj,tj1satisfiesujH2tj, tj1, and

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j1,2, . . . , pexist, and impulsive conditions and boundary conditions in problem1.1hold, we say it isa classical solutionof problem1.1.

Consider the functional

ϕ:X−→R, 2.3

defined by

ϕu 1

2u

2λ

T

0

Ht, utdt

p

j1

utj

0

Ijsds, 2.4

whereHt, u 0uht, sds. Clearly,ϕis a Fr´echet differentiable functional, whose Fr´echet derivative at the pointuXis the functionalϕuX∗given by

ϕuv

T

0

utvtdtλ

T

0

ht, utvtdt

p

j1 Ij

utj

vtj

, 2.5

for anyvX. Obviously,ϕis continuous.

Lemma 2.3. IfuXis a critical point of the functionalϕ, then u is a classical solution of problem

1.1.

Proof. The proof is similar to the proof of16, Lemma 2.4, and we omit it here.

Lemma 2.4. LetuX, thenu∞≤√Tu.

Proof. ForuX, thenu0 uT 0. Hence, fort∈0, T, by H ¨older’s inequality, we have

|ut|

t

0

usds

T

0

usdsTT

0

us2 ds

1/2

Tu, 2.6

which completes the proof.

3. Main Results

Theorem 3.1. Suppose that the following conditions hold.

iThere exista, b >0andγ∈0,1such that

|ht, u| ≤ab|u|γ for anyt, u∈0, T×R. 3.1

iiht, uis odd about u andHt, u>0for everyt, u∈0, T×R\ {0}.

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Then for anynN, there existsλnsuch thatλ > λn, and problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Proof. By2.4,ii, andiii,ϕC1X, Ris an even functional andϕ0 0.

Next, we will verify thatϕis bounded from below. In view ofi,iii, andLemma 2.4, we have

ϕu 1

2u

2λ

T

0

Ht, utdt

p

j1

utj

0

Ijsds

≥ 1 2u

2λ

T

0

a|ut|b|ut|γ1dt

≥ 1 2u

2λaT3/2uλbTγ3/2uγ1

>−∞,

3.2

for anyuX. That is,ϕis bounded from below.

In the following we will show thatϕsatisfies the Palais-Smale condition. Let{uk} ⊂X,

such that{ϕuk}is a bounded sequence and limk→ ∞ϕuk 0. Then, there existsM > 0

such that

ϕukM. 3.3

In view of3.2, we have

M≥ 1

2uk

2λaT3/2u

kλbTγ3/2ukγ1. 3.4

So {uk} is bounded inX. From the reflexivity of X, we may extract a weakly convergent

subsequence that, for simplicity, we call {uk},uk uinX. Next, we will verify that {uk}

strongly converges touinX. By2.5, we have

ϕukϕu

uku uku2−λ

T

0

ht, uktht, utuktutdt

p

j1

Ij uk tjIj

utj

uk

tj

utj

.

3.5

Byuk uinX, we see that{uk}uniformly converges touinC0, T. So,

λ

T

0

ht, uktht, utuktutdt−→0,

p

j1

Ij uk tjIj

utj

uk

tj

utj

−→0 ask−→ ∞.

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By limk→ ∞ϕuk 0 anduk u, we have

ϕukϕu

uku−→0 ask−→ ∞. 3.7

In view of3.5,3.6, and3.7, we obtainuku → 0 as k → ∞. Then,ϕsatisfies the

Palais-Smale condition. Letvmt

2T/mπsinmπ/Tt,m1,2, . . . , n, then

vm2 1 m

2π2 T2

T

0

|vmt|2dt, m1,2, . . . , n. 3.8

Define

Knr

n

m1 cmvm|

n

m1 c2mr2

, r >0. 3.9

Then, for anyr >0, there exists an odd homeomorphismf:KnrSn−1. Let 0< r <1/

T, thenu∞≤√TuTr <1 for anyuKnr. Byii, we have

Ht, ut

ut

0

ht, sds >0 asut/0, 3.10

then 0THt, utdt >0 for anyuKnr.

Letαn infuKnr

T

0 Ht, utdt,βninfuKnr

p j1

utj

0 Ijsds, thenαn >0,βn ≤0.

Letλn 1/2r2−βnαn−1>0, then whenλ > λn, for anyuKnr, we have

ϕu≤ 1

2r

2λα

nβn

< 1

2r

2λ

nαnβn

0.

3.11

By Theorem 2.2, ϕ possesses at least n distinct pairs of nontrivial critical points. That is, problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Corollary 3.2. Let the following conditions hold:

iht, uis bounded,

iiht, uis odd about u andHt, u>0for everyt, u∈0, T×R\ {0},

iiiIju j1,2, . . . , pare odd and 0uIjsds≤0for anyuRj 1,2, . . . , p.

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Proof. Letγ0 inTheorem 3.1, thenCorollary 3.2holds.

Theorem 3.3. Suppose that the following conditions hold.

iThere existsa, b >0andγ∈0,1such that

|ht, u| ≤ab|u|γ for anyt, u∈0, T×R. 3.12

iiThere existsaj, bj>0andγj ∈0,1 j1,2, . . . , psuch that

Ijuajbj|u|γj for anyuRj1,2, . . . , p. 3.13

iiiht, u and Iju j 1,2, . . . , p are odd about u and Ht, u > 0 for everyt, u

0, T×R\ {0}.

Then, for anynN, there existsλnsuch thatλ > λn, and problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Proof. By2.4andiii,ϕC1X, Ris an even functional andϕ0 0.

Next, we will verify thatϕis bounded from below. LetM1max{a1, a2, . . . , ap},M2

max{b1, b2, . . . , bp}. In view ofi,ii, andLemma 2.4, we have

ϕu 1

2u

2 λ

T

0

Ht, utdt

p

j1

utj

0

Ijsds

≥ 1 2u

2 λ

T

0

a|ut|b|ut|γ1dt

p

j1

aju

tjbju

tjγj1

≥ 1 2u

2

λaT3/2uλbTγ3/21−pM1Tu

M2

p

j1

Tγj1/2uγj1

>−∞,

3.14

for anyuX. That is,ϕis bounded from below.

In the following, we will show thatϕ satisfies the Palais-Smale condition. As in the proof ofTheorem 3.1, by3.3and3.14, we have

M≥ 1

2uk

2

λaT3/2ukλbTγ3/2ukγ1−pM1

TukM2 p

j1

Tγj1/2ukγj1.

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It follows that{uk}is bounded inX. In the following, the proof of the Palais-Smale condition

is the same as that inTheorem 3.1, and we omit it here.

Take the same Knr as in Theorem 3.1, then for any r > 0, there exists an odd

homeomorphismf : KnrSn−1. Let 0 < r < 1/

T, then u∞ ≤ √TuTr < 1

for anyuKnr. Byiii, we have

Ht, ut

ut

0

ht, sds >0 asut/0. 3.16

Then, 0THt, utdt >0 for anyuKnr.

Let αn infuKnr

T

0 Ht, utdt,βn infuKnr

p j1

utj

0 Ijsds, thenαn > 0. Let λnmax{0,1/2r2−βnαn1}, then whenλ > λn, for anyuKnr, we have

ϕu≤ 1

2r

2λα

nβn< 1

2r

2λ

nαnβn≤0. 3.17

By Theorem 2.2, ϕ possesses at least n distinct pairs of nontrivial critical points. That is, problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Corollary 3.4. Let the following conditions hold:

iht, uis bounded,

iiIju j1,2, . . . , pare bounded,

iiiht, u and Iju j 1,2, . . . , p are odd about u and Ht, u > 0 for everyt, u

0, T×R\ {0}.

Then, for anynN, there existsλnsuch thatλ > λn, and problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Proof. Letγ0 andγj0 j1,2, . . . , pinTheorem 3.3, thenCorollary 3.4holds.

Theorem 3.5. Suppose that the following conditions hold.

iThere exist constantsσ >0such thatht, σ 0, ht, u>0for everyu∈0, σ.

iiht, uis odd aboutu.

iiiIju j1,2, . . . , pare odd and 0uIjsds≤0for anyuRj 1,2, . . . , p.

Then, for anynN, there existsλnsuch thatλ > λn, and problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Proof. Let

h1t, u

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

ht, σ, u > σ,

ht, u, |u| ≤σ,

ht,σ, u <σ,

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thenh1t, uis continuous, bounded, and odd. Consider boundary value problem

ut λh1t, ut 0, t /tj, a.e. t∈0, T,

−Δutj

Ij

utj

, j1,2, . . . , p,

u0 uT 0.

3.19

Next, we will verify that the solutions of problem3.19are solutions of problem1.1. In fact, letu0tbe the solution of problem3.19. If max0≤tTu0t> σ, then there exists an interval

a, b⊂0, Tsuch that

u0a u0b σ, u0t> σ for anyta, b. 3.20

Whenta, b, byi, we have

u0tλh1t, uλht, σ 0. 3.21

Thus, there exist constantscsuch thatu0t cfor anyta, b. We consider the following two possible cases.

Case 1. c≥0, thenu0is nondecreasing ina, b. Byu0a≥0 andu0b≤0, we have

0≤u0au0tu0b≤0 for everyta, b. 3.22

That is,u0t ≡ 0 for anyta, b. So, there exists a constantdsuch thatu0td, which contradicts3.20. Then, max0≤tTu0tσ. Similarly, we can prove that min0≤tTu0t≥ −σ.

Case 2. c <0, the arguments are analogous, thenu0tis solution of problem1.1.

For everyuX, we consider the functional

ϕ1:X−→R, 3.23

defined by

ϕ1u 1

2u

2 λ

T

0

H1t, utdt

p

j1

utj

0

Ijsds, 3.24

whereH1t, u 0uh1t, sds.

It is clear thatϕ1is Fr´echet differentiable at anyuXand

ϕ1uv

T

0

utvtdtλ

T

0

h1t, utvtdt

p

j1 Ij

utj

vtj

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for anyvX. Obviously,ϕ1is continuous. By Lemma2.3, we have the critical points ofϕ1as solutions of problem3.19. By3.24,ii, andiii,ϕ1C1X, Ris an even functional and ϕ10 0.

In the following, we will show thatϕ1 is bounded from below. sinceh1t, u 0 for |u| ≥σ, thus

T

0

H1t, utdt

T

0

ut

0

h1t, sds dt

T

0

σ

0

h1t, sds dte >0. 3.26

Byiii, we have

ϕ1u 1

2u

2 λ

T

0

H1t, utdt

p

j1

utj

0

Ijsds

≥ 1 2u

2λe≥ −λe,

3.27

for anyuX. That is,ϕ1is bounded from below.

In the following we will show thatϕ1satisfies the Palais-Smale condition. Let{uk} ⊂X

such that{ϕ1uk}is a bounded sequence and limk→ ∞ϕ1uk 0. Then, there existsM3 >0

such that

ϕ1ukM3. 3.28

By3.27, we have

1 2uk

2

M3λe. 3.29

It follows that{uk}is bounded inX. In the following, the proof of the Palais-Smale condition

is the same as that inTheorem 3.1, and we omit it here.

Take the same Knr as in Theorem 3.1, then, for any r > 0, there exists an odd

homeomorphismf : KnrSn−1. Let 0 < r < σ/

T, thenu∞ ≤ √TuTr < σ

for anyuKnr. Byiandii, we have

H1t, ut

ut

0

h1t, sds

ut

0

ht, sdt >0 asut/0. 3.30

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LetαninfuKnr 0TH1t, utdt,βninfuKnr

p j1

utj

0 Ijsds, thenαn>0,βn≤0.

Letλn 1/2r2−βnαn−1>0, then whenλ > λn, for anyuKnr, we have

ϕ1u≤ 1

2r

2λα

nβn

< 1

2r

2λ

nαnβn

0.

3.31

By Theorem 2.2, ϕ1 possesses at least n distinct pairs of nontrivial critical points. Then, problem3.19has at leastndistinct pairs of nontrivial classical solutions, that is, problem

1.1has at leastndistinct pairs of nontrivial classical solutions

Theorem 3.6. Let the following conditions hold.

iThere exist constantsσ >0such thatht, σ 0, ht, u>0for everyu∈0, σ.

iiThere existaj, bj>0, andγj∈0,1 j 1,2, . . . , psuch that

Ijuajbj|u|γj for anyuRj1,2, . . . , p. 3.32

iiiht, uandIju j1,2, . . . , pare odd aboutu.

Then, for anynN, there existsλnsuch thatλ > λn, and problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Proof. The proof is similar to the proof ofTheorem 3.5, and we omit it here.

Theorem 3.7. Let the following conditions hold.

iThere exist constantsσ1>0such thatht, σ1≤0.

iiThere existaj, bj>0, andγj∈0,1 j 1,2, . . . , psuch that

Ijuajbj|u|γj for anyuRj1,2, . . . , p. 3.33

iiiht, uandIju j1,2, . . . , pare odd aboutuandlimu→0ht, u/u1uniformly for

t∈0, T.

Then, for anynN, there existsλnsuch thatλ > λn, and problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Proof. Let

h2t, u

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

ht, σ1, u > σ1,

ht, u, |u| ≤σ1,

ht,σ1, u <σ1,

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thenh2t, uis continuous, bounded, and odd. Consider boundary value problem

ut λh2t, ut 0, t /tj, a.e. t∈0, T,

−Δutj

Ij

utj

, j1,2, . . . , p,

u0 uT 0.

3.35

Next, we will verify that the solutions of problem3.35are solutions of problem1.1. In fact, letu0tbe the solution of problem3.35. If max0≤tTu0t> σ1, then there exists an interval

a, b⊂0, Tsuch that

u0a u0b σ1, u0t> σ1 for anyta, b. 3.36

Whenta, b, byi, we have

u0tλh2t, uλht, σ1≥0. 3.37

Thus,u0tis nondecreasing ina, b. Byu0a≥0 andu0b≤0, we have

0≤u0au0tu0b≤0 for everyta, b. 3.38

That is,u0t ≡ 0 for anyta, b. So, there exists a constantdsuch thatu0td, which contradicts3.36. Then max0≤tTu0tσ1. Similarly, we can prove that min0≤tTu0t≥ −σ1.

Then,u0tis solution of problem1.1.

For everyuX, we consider the functional

ϕ2:X−→R, 3.39

defined by

ϕ2u 1

2u

2λ

T

0

H2t, utdt

p

j1

utj

0

Ijsds, 3.40

whereH2t, u 0uh2t, sds.

It is clear thatϕ2is Fr´echet differentiable at anyuXand

ϕ2uv

T

0

utvtdtλ

T

0

h2t, utvtdt

p

j1 Ij

utj

vtj

, 3.41

for anyvX. Obviously,ϕ2 is continuous. ByLemma 2.3, we have the critical points ofϕ2

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Next, we will show that ϕ2 is bounded from below. Let M1 max{a1, a2, . . . , ap},

M2max{b1, b2, . . . , bp}. sinceuh2t, u≤0 for|u| ≥σ1, thus

T

0

H2t, utdt

T

0

ut

0

h2t, sds dt

T

0

σ1

0

h2t, sds dte. 3.42

ByiiandLemma 2.4, we have

ϕ2u 1

2u

2 λ

T

0

H2t, utdt

p

j1

utj

0

Ijsds

≥ 1 2u

2

λepM1TuM2

p

j1

Tγj1/2uγj1

>−∞,

3.43

for anyuX. That is,ϕ2is bounded from below.

In the following we will show thatϕ2satisfies the Palais-Smale condition. Let{uk} ⊂X

such that{ϕ2uk}is a bounded sequence and limk→ ∞ϕ2uk 0. Then, there existsM4 >0

such that

ϕ2ukM4. 3.44

By3.43, we have

1 2uk

2

M4λepM1TukM2 p

j1

Tγj1/2ukγj1. 3.45

It follows that{uk}is bounded inX. In the following, the proof of the Palais-Smale condition

is the same as that inTheorem 3.1, and we omit it here.

Take the same Knr as in Theorem 3.1, then for any r > 0, there exists an odd

homeomorphismf : KnrSn−1. By iii, for any 0 < ε < 1, there existsδ > 0, when

|u| ≤δ, we have

h2t, uuε|u|. 3.46

Let 0< r <min{σ1/T, δ/T}, thenu∞≤√TuTr <min{σ1, δ}for anyuKnr.

Then, 0TH2t, utdt 0T 0uth2t, sdt0T1/21−ε|ut|2dt >0 for anyuK

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Letαn infuKnr 0TH2t, utdt,βn infuKnr

p j1

utj

0 Ijsds, thenαn > 0. Let λnmax{1/2r2−βnαn−1,0}, then whenλ > λn, for anyuKnr, we have

ϕ1u≤ 1

2r

2λα

nβn

< 1

2r

2λ

nαnβn

≤0.

3.47

By Theorem 2.2, ϕ2 possesses at least n distinct pairs of nontrivial critical points. Then, problem3.35has at leastndistinct pairs of nontrivial classical solutions, that is, problem

1.1has at leastndistinct pairs of nontrivial classical solutions.

Theorem 3.8. Let the following conditions hold.

iThere exist constantsσ1>0such thatht, σ1≤0.

iilimu→0ht, u/u1uniformly fort∈0, T.

iiiht, uandIju j 1,2, . . . , pare odd aboutuand 0uIjsds≤0for anyuR j

1,2, . . . , p.

Then, for anynN, there existsλnsuch thatλ > λn, and problem1.1has at leastndistinct pairs of nontrivial classical solutions.

Proof. The proof is similar to the proof ofTheorem 3.7, and we omit it here.

4. Some Examples

Example 4.1. Consider boundary value problem

ut λ1t3

ut 0, t /tj, a.e. t∈0, π,

−Δutj

utj

, j1,2,

u0 0.

4.1

It is easy to see that conditionsi,ii, andiiiofTheorem 3.1hold. Let

αn inf uKnr

3 4

π

0

1t|ut|4/3dt > inf

uKnr 3 4

π

0

|ut|2dt > 3r 2

4n2,

βn inf uKnr

2

j1

utj

0

sds inf

uKnr

2

j1

u

tj2

2 ≥ −πr

2,

4.2

thenλn 1/2r2 −βnαn1 < 24π/3n2. ApplyingTheorem 3.1, then for anynN,

whenλ > 24π/3n2, problem4.1has at leastndistinct pairs of nontrivial classical

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Example 4.2. Consider boundary value problem

ut λ1t3

ut 0, t /tj, a.e. t∈0, π,

−Δutj

−3

utj

, j1,2,

u0 0.

4.3

It is easy to see that conditionsi,ii, andiiiofTheorem 3.3hold. Letr 1/2√π,

αn inf uKnr

3 4

π

0

1t|ut|4/3dt > inf

uKnr 3 4

π

0

|ut|2dt > 3r 2

4n2,

βn inf uKnr

2

j1

utj

0

s1/3ds inf

uKnr

2

j1

3 4u

tj4/3>

3 2,

4.4

thenλn 1/2r2−βnαn−1 < 224π/3n2. Applying Theorem 3.3, then for any

nN, whenλ > 224π/3n2, problem4.3has at least ndistinct pairs of nontrivial

classical solutions.

Example 4.3. Consider boundary value problem

ut λ1t2utut30, t /tj, a.e. t∈0, π,

−Δutj

utj

, j1,2,

u0 0.

4.5

Letσ1, it is easy to see that conditionsi,ii, andiiiofTheorem 3.5hold. Let

αn inf uKnr

π

0

1t21

2|ut|

21

4|ut|

4

dt > inf

uKnr

1 4

π

0

|ut|2dt > r 2

4n2,

βn inf uKnr

2

j1

utj

0

sds inf

uKnr

2

j1

u

tj2

2 ≥ −πr

2,

4.6

thenλn 1/2r2−βnαn−1 <24πn2. ApplyingTheorem 3.5, then for anynN,

whenλ >24πn2, problem4.5has at leastndistinct pairs of nontrivial classical solutions.

Example 4.4. Consider boundary value problem

ut λut−1tut30, t /tj, a.e. t∈0, π,

−Δutj

−3

utj

, j1,2,

u0 0.

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Letσ1 1, it is easy to see that conditionsi,ii, andiiiofTheorem 3.7hold. Let

r1/4√π,

αn inf uKnr

π

0

1 2|ut|

2 1

41t|ut|

4

dt > inf

uKnr 1 4

π

0

|ut|2dt > r 2

4n2,

βn inf uKnr

2

j1

utj

0

s1/3ds inf

uKnr

2

j1

3 4u

tj4/3>

3 2,

4.8

thenλn 1/2r2 −βnαn−1 < 224πn2. Applying Theorem 3.7, then for anyn

N, whenλ > 224πn2, problem4.7has at least ndistinct pairs of nontrivial classical

solutions.

Acknowledgments

This work was supported by the NNSF of Chinano. 10871062and a project supported by Hunan Provincial Natural Science Foundation of Chinano. 10JJ6002.

References

1 R. K. George, A. K. Nandakumaran, and A. Arapostathis, “A note on controllability of impulsive systems,”Journal of Mathematical Analysis and Applications, vol. 241, no. 2, pp. 276–283, 2000.

2 G. Jiang and Q. Lu, “Impulsive state feedback control of a predator-prey model,” Journal of Computational and Applied Mathematics, vol. 200, no. 1, pp. 193–207, 2007.

3 S. I. Nenov, “Impulsive controllability and optimization problems in population dynamics,”Nonlinear Analysis. Theory, Methods & Applications, vol. 36, pp. 881–890, 1999.

4 M. Choisy, J.-F. Gu´egan, and P. Rohani, “Dynamics of infectious diseases and pulse vaccination: teasing apart the embedded resonance effects,”Physica D, vol. 223, no. 1, pp. 26–35, 2006.

5 S. Gao, L. Chen, J. J. Nieto, and A. Torres, “Analysis of a delayed epidemic model with pulse vaccination and saturation incidence,”Vaccine, vol. 24, no. 35-36, pp. 6037–6045, 2006.

6 J. Li and J. J. Nieto, “Existence of positive solutions for multipoint boundary value problem on the half-line with impulses,”Boundary Value Problems, vol. 2009, Article ID 834158, 12 pages, 2009. 7 J. Chu and J. J. Nieto, “Impulsive periodic solutions of first-order singular differential equations,”

Bulletin of the London Mathematical Society, vol. 40, no. 1, pp. 143–150, 2008.

8 D. Qian and X. Li, “Periodic solutions for ordinary differential equations with sublinear impulsive effects,”Journal of Mathematical Analysis and Applications, vol. 303, no. 1, pp. 288–303, 2005.

9 L. Chen and J. Sun, “Nonlinear boundary value problem of first order impulsive functional differential equations,”Journal of Mathematical Analysis and Applications, vol. 318, no. 2, pp. 726–741, 2006.

10 J. J. Nieto and D. O’Regan, “Variational approach to impulsive differential equations,” Nonlinear Analysis. Real World Applications, vol. 10, no. 2, pp. 680–690, 2009.

11 Y. Tian and W. Ge, “Applications of variational methods to boundary-value problem for impulsive differential equations,”Proceedings of the Edinburgh Mathematical Society. Series II, vol. 51, no. 2, pp. 509–527, 2008.

12 Y. Tian, W. Ge, and D. Yang, “Existence results for second-order system with impulse effects via variational methods,”Journal of Applied Mathematics and Computing, vol. 31, no. 1-2, pp. 255–265, 2009. 13 H. Zhang and Z. Li, “Variational approach to impulsive differential equations with periodic boundary

conditions,”Nonlinear Analysis. Real World Applications, vol. 11, no. 1, pp. 67–78, 2010.

14 Z. Zhang and R. Yuan, “An application of variational methods to Dirichlet boundary value problem with impulses,”Nonlinear Analysis. Real World Applications, vol. 11, no. 1, pp. 155–162, 2010.

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16 J. Sun and H. Chen, “Variational method to the impulsive equation with Neumann boundary conditions,”Boundary Value Problems, vol. 2009, Article ID 316812, 17 pages, 2009.

References

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