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Periodic boundary value problems for nonlinear first-order impulsive dynamic equations on time scales Advances in Difference Equations 2012, 2012:12 doi:10.1186/1687-1847-2012-12 Da-Bin

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Periodic boundary value problems for nonlinear first-order impulsive dynamic

equations on time scales

Advances in Difference Equations 2012, 2012:12 doi:10.1186/1687-1847-2012-12

Da-Bin Wang (wangdb@lut.cn)

ISSN 1687-1847

Article type Research

Submission date 23 August 2011

Acceptance date 15 February 2012

Publication date 15 February 2012

Article URL http://www.advancesindifferenceequations.com/content/2012/1/12

This peer-reviewed article was published immediately upon acceptance It can be downloaded,

printed and distributed freely for any purposes (see copyright notice below)

For information about publishing your research in Advances in Difference Equations go to

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Periodic boundary value problems for nonlinear first-order impulsive dynamic

equations on time scales

Da-Bin Wang

Department of Applied Mathematics, Lanzhou University of Technology,

Lanzhou, Gansu 730050, People’s Republic of China

Email address: wangdb@lut.cn

Abstract

By using the classical fixed point theorem for operators on cone, in this article, someresults of one and two positive solutions to a class of nonlinear first-order periodicboundary value problems of impulsive dynamic equations on time scales are obtained.Two examples are given to illustrate the main results in this article

Keywords: time scale; periodic boundary value problem; positive solution; fixedpoint; impulsive dynamic equation

Mathematics Subject Classification: 39A10; 34B15

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1 Introduction

Let T be a time scale, i.e., T is a nonempty closed subset of R Let 0, T be points in T,

an interval (0, T )T denoting time scales interval, that is, (0, T )T := (0, T ) ∩ T Other types

of intervals are defined similarly

The theory of impulsive differential equations is emerging as an important area of vestigation, since it is a lot richer than the corresponding theory of differential equationswithout impulse effects Moreover, such equations may exhibit several real world phenom-ena in physics, biology, engineering, etc (see [1–3]) At the same time, the boundary valueproblems for impulsive differential equations and impulsive difference equations have re-ceived much attention [4–18] On the other hand, recently, the theory of dynamic equations

in-on time scales has become a new important branch (see, for example, [19–21]) Naturally,some authors have focused their attention on the boundary value problems of impulsivedynamic equations on time scales [22–36] However, to the best of our knowledge, few pa-pers concerning PBVPs of impulsive dynamic equations on time scales with semi-positioncondition

In this article, we are concerned with the existence of positive solutions for the followingPBVPs of impulsive dynamic equations on time scales with semi-position condition

(1.1)

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where T is an arbitrary time scale, T > 0 is fixed, 0, T ∈ T, f ∈ C (J × [0, ∞) , (−∞, ∞)),

Ik ∈ C ([0, ∞) , [0, ∞)) , tk ∈ (0, T )T, 0 < t1 < · · · < tm < T, and for each k = 1, 2, , m,x(t+

k) = limh→0+x(tk+ h) and x(t−

k) = limh→0−x(tk+ h) represent the right and left limits ofx(t) at t = tk We always assume the following hypothesis holds (semi-position condition):(H) There exists a positive number M such that

In the remainder of this section, we state the following fixed point theorem [37]

Theorem 1.1 Let X be a Banach space and K ⊂ X be a cone in X Assume Ω1, Ω2

are bounded open subsets of X with 0 ∈ Ω1 ⊂ Ω1 ⊂ Ω2 and Φ : K ∩ (Ω2\Ω1) → K is acompletely continuous operator If

(i) There exists u0 ∈ K\{0} such that u − Φu 6= λu0, u ∈ K ∩ ∂Ω2, λ ≥ 0; Φu 6= τ u,

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X = {x : x ∈ P C, x(0) = x(σ(T ))}

with the norm kxk = supt∈[0,σ(T )]T|x(t)| , then X is a Banach space

Lemma 2.1 Suppose M > 0 and h : [0, T ]T → R is rd-continuous, then x is a solutionof

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Proof Since the proof similar to that of [34, Lemma 3.1], we omit it here.

Lemma 2.2 Let G(t, s) be defined as in Lemma 2.1, then

1

eM(σ(T ), 0) − 1 ≤ G(t, s) ≤

eM(σ(T ), 0)

eM(σ(T ), 0) − 1 for all t, s ∈ [0, σ(T )]T.Proof It is obviously, so we omit it here

Remark 2.1 Let G(t, s) be defined as in Lemma 2.1, then Rσ(T )

0 G(t, s)△s = 1

M.For u ∈ X, we consider the following problem:

k) = Ik(x(t−

k)), k = 1, 2, , m,x(0) = x(σ(T ))

We define an operator Φ : X → X by

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It is obvious that fixed points of Φ are solutions of the problem (1.1).

Lemma 2.3 Φ : X → X is completely continuous

Proof The proof is divided into three steps

Step 1: To show that Φ : X → X is continuous

which leads to kΦun− Φuk → 0 (n → ∞) That is, Φ : X → X is continuous

Step 2: To show that Φ maps bounded sets into bounded sets in X

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Let B ⊂ X be a bounded set, that is, ∃ r > 0 such that ∀ u ∈ B we have kuk ≤ r Then,for any u ∈ B, in virtue of the continuities of f (t, u) and Ik(u), there exist c > 0, ck>0 suchthat

Then we can conclude that Φu is bounded uniformly, and so Φ(B) is a bounded set

Step 3: To show that Φ maps bounded sets into equicontinuous sets of X

The right-hand side tends to uniformly zero as |t1− t2| → 0

Consequently, Steps 1–3 together with the Arzela–Ascoli Theorem shows that Φ : X → X

is completely continuous

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K = {u ∈ X : u(t) ≥ δ kuk , t∈ [0, σ(T )]T} ,where δ = eM(σ(T ), 0)1 ∈ (0, 1) It is not difficult to verify that K is a cone in X.From condition (H) and Lemma 2.2, it is easy to obtain following result:Lemma 2.4 Φ maps K into K

Theorem 3.1 Suppose that

(H1) f0 >0, f∞

<0, I0 = 0 for any k; or(H2) f∞>0, f0 <0, I∞ = 0 for any k

Then the problem (1.1) has at least one positive solutions

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Proof Firstly, we assume (H1) holds Then there exist ε > 0 and β > α > 0 such that

f(t, u) ≥ εu, t∈ [0, T ]T, u∈ (0, α] , (3.1)

Ik(u) ≤ [eM(σ(T ), 0) − 1]ε

2M meM(σ(T ), 0)u, u∈ (0, α] , for any k, (3.2)and

f(t, u) ≤ −εu, t ∈ [0, T ]T, u∈ [β, ∞) (3.3)Let Ω1 = {u ∈ X : kuk < r1} , where r1 = α Then u ∈ K ∩ ∂Ω1, 0 < δα = δ kuk ≤u(t) ≤ α, in view of (3.1) and (3.2) we have

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Φu 6= τ u, u∈ K ∩ ∂Ω1, τ ≥ 1 (3.4)

On the other hand, let Ω2 = {u ∈ X : kuk < r2} , where r2 = βδ

Choose u0 = 1, then u0 ∈ K\{0}.We assert that

u− Φu 6= λu0, u∈ K ∩ ∂Ω2, λ≥ 0 (3.5)Suppose on the contrary that there exist u ∈ K ∩ ∂Ω2 and λ ≥ 0 such that

u− Φu = λu0.Let ζ = mint∈[0,σ(T )]Tu(t), then ζ ≥ δ kuk = δr2 = β, we have from (3.3) that

ζ = min

t∈[0,σ(T )]Tu(t) ≥ (M + ε)

M ζ+ λ > ζ,which is a contradiction

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It follows from (3.4), (3.5) and Theorem 1.1 that Φ has a fixed point u ∈ K ∩ (Ω2\Ω1),and u∗

is a desired positive solution of the problem (1.1)

Next, suppose that (H2) holds Then we can choose ε′

f(t, u) ≤ −ε′u, t∈ [0, T ]T, u∈ (0, α′] (3.8)Let Ω3 = {u ∈ X : kuk < r3} , where r3 = α′

Then for any u ∈ K ∩ ∂Ω3, 0 < δ kuk ≤u(t) ≤ kuk = α′

It is similar to the proof of (3.5), we have

u− Φu 6= λu0, u∈ K ∩ ∂Ω3, λ≥ 0 (3.9)Let Ω4 = {u ∈ X : kuk < r4} , where r4 = βδ′ Then for any u ∈ K ∩ ∂Ω4, u(t) ≥ δ kuk =

δr4 = β′, by (3.6) and (3.7), it is easy to obtain

Φu 6= τ u, u∈ K ∩ ∂Ω4, τ ≥ 1 (3.10)

It follows from (3.9), (3.10) and Theorem 1.1 that Φ has a fixed point u∗

∈ K ∩ (Ω4\Ω3),and u∗

is a desired positive solution of the problem (1.1)

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Theorem 3.2 Suppose that

Proof By (H3), from the proof of Theorem 3.1, we should know that there exist

β′′ > ρ > α′′

>0 such that

u− Φu 6= λu0, u∈ K ∩ ∂Ω5, λ≥ 0, (3.13)

u− Φu 6= λu0, u∈ K ∩ ∂Ω6, λ≥ 0, (3.14)where Ω5 = {u ∈ X : kuk < r5} , Ω6 = {u ∈ X : kuk < r6} , r5 = α′′

, r6 = βδ′′

By (3.11) of (H4), we can choose ε > 0 such that

f(t, u) ≥ (1 + ε)u, t∈ [0, T ]T, δρ≤ u ≤ ρ (3.15)Let Ω7 = {u ∈ X : kuk < ρ} , for any u ∈ K ∩ ∂Ω7, δρ = δ kuk ≤ u(t) ≤ kuk = ρ, from(3.12) and (3.15), it is similar to the proof of (3.4), we have

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are two positive solution of the problem (1.1).

Similar to Theorem 3.2, we have:

Theorem 3.3 Suppose that

(4.1)

where T = 3, f (t, x) = x − (t + 1)x2, and I(x) = x2

Let M = 1,then, it is easy to see that

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M x− f (t, x) = (t + 1)x2 ≥ 0 for x ∈ [0, ∞) , t∈ [0, 3]T,and

(4.2)

where T = 3, f (t, x) = 4e1−4e 2

x− (t + 1)x2e−x, and I(x) = x2e−x.Choose M = 1, ρ = 4e2, then δ = 1

2e 2, it is easy to see that

M x− f (t, x) = x(1 − 4e1−4e2) + (t + 1)x2e−x ≥ 0 for x ∈ [0, ∞) , t∈ [0, 3]T,

f0 ≥ 4e1−4e2 >0, f∞≥ 4e1−4e2 >0, I0 = 0 , I∞= 0,and

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max{f (t, u)|t ∈ [0, T ]T, δρ ≤ u ≤ ρ} = max©f(t, u)|t ∈ [0, 3]T,2 ≤ u ≤ 4e2ª = 16e3−4e (1−e) < 0.

Therefore, together with Theorem 3.3, it follows that the problem (4.2) has at least two

positive solutions

Competing interests

The authors have no competing interests to declare

Acknowledgment

The author thankful to the anonymous referee for his/her helpful suggestions for the

im-provement of this article This work is supported by the Excellent Young Teacher Training

Program of Lanzhou University of Technology (Q200907)

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