Volume 2009, Article ID 219251, 14 pagesdoi:10.1155/2009/219251 Research Article Boundary Value Problems on Time Scales 1 School of Science, Beijing Information Science & Technology Univ
Trang 1Volume 2009, Article ID 219251, 14 pages
doi:10.1155/2009/219251
Research Article
Boundary Value Problems on Time Scales
1 School of Science, Beijing Information Science & Technology University,
Beijing 100192, China
2 Department of Mathematics and Physics, North China Electric Power University,
Beijing 102206, China
3 Department of Applied Mathematics, Beijing Institute of Technology,
Beijing 100081, China
Correspondence should be addressed to Xuemei Zhang,zxm74@sina.com
Received 1 December 2008; Revised 15 April 2009; Accepted 10 June 2009
Recommended by Victoria Otero-Espinar
By constructing an available integral operator and combining Krasnosel’skii-Zabreiko fixed point theorem with properties of Green’s function, this paper shows the existence of multiple positive
solutions for a class of m-point second-order Sturm-Liouville-like boundary value problems on
time scales with polynomial nonlinearity The results significantly extend and improve many known results for both the continuous case and more general time scales We illustrate our results
by one example, which cannot be handled using the existing results
Copyrightq 2009 Meiqiang Feng et al 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
1 Introduction
Recently, there have been many papers working on the existence of positive solutions to boundary value problems for differential equations on time scales; see, for example, 1
20 This has been mainly due to its unification of the theory of differential and difference equations An introduction to this unification is given in 11, 12,18, 19 Now, this study
is still a new area of fairly theoretical exploration in mathematics However, it has led to several important applications, for example, in the study of insect population models, neural networks, heat transfer, and epidemic models; see, for example, 10, 11 For some other excellent results and applications of the case that boundary value problems on time scales
to a variety of problems from Khan et al.21, Agarose et al 22, Wang 23, Sun 24, Feng
et al.25, Feng et al 26 and Feng et al 27
Motivated by the works mentioned above, we intend in this paper to study the
existence of multiple positive solutions for the second-order m-point nonlinear dynamic
Trang 2equation on time scales with polynomial nonlinearity:
−p tx∇Δ
t q t x t f t, x t , t1 < t < t m ,
αx t1 − βp t1 x∇t1 m−1
i 2
a i x t i ,
γx t m δp t m x∇t m m−1
i 2
b i x t i ,
1.1
whereT is a time scale,
the points t i∈ Tk
k for i ∈ {1, 2, , m} with t1 < t2< · · · < t m;
α, γ, β, δ ∈ 0, ∞ αγ αδ βγ > 0, a i , b i ∈ 0, ∞ , i ∈ {2, 3, , m − 1} ; 1.3
f t, x n
j 1
c j t x υ j , c j ∈ C t1 , t m , 0, ∞ , υ j ∈ 0, ∞ , j 1, 2, , n. 1.4
Recently, Xu28 considered the following second-order two-point impulsive singular differential equations boundary value problem:
y n
j 1
a j t x α j 0, 0 < t < 1, t / t1 ,
Δy| t t1 Iy t1,
y 0 y 1 0.
1.5
By means of fixed point index theory in a cone, the author established the existence of two nonnegative solutions for problem1.5
More recently, by applying Guo-Krasnosel’skii fixed point theorem in a cone, Anderson and Ma 6 established the existence of at least one positive solution to the multipoint time-scale eigenvalue problem:
py∇Δ
t − q t y t λh t fy
0, t1 < t < t n ,
αy t1 − βp t1 y∇t1 n−1
i 2
a i y t i ,
γx t n δp t n x∇t n n−1
i 2
b i y t i ,
1.6
where f : 0, ∞ → 0, ∞ is continuous.
Trang 3As far as we know, there is no paper to study the existence of multiple positive solutions to problem1.1 on time scales with polynomial nonlinearity The objective of the present paper is to fill this gap On the other hand, many difficulties occur when we study BVPs on time scales For example, basic tools from calculus such as Fermat’s theorem, Rolle’s theorem and the intermediate value theorem may not necessarily hold So it is interesting and important to discuss the problem1.1 The purpose of this paper is to prove that the problem
1.1 possesses at least two positive solutions Moreover, the methods used in this paper are different from 6,28 and the results obtained in this paper generalize some results in 6,28
to some degree
The time scale related notations adopted in this paper can be found, if not explained specifically, in almost all literature related to time scales The readers who are unfamiliar with this area can consult for example11,12,18,19 for details
For convenience, we list the following well-known definitions
for t > inf T by σt inf{τ > t : τ ∈ T} ρt sup{τ < t : τ ∈ T} for all t ∈ T.
We assume throughout that T has the topology that it inherits from the standard topology onR and say t is right-scattered, left-scattered, right-dense and left-dense if σt >
t, ρ t < t, σt t and ρt t, respectively Finally, we introduce the sets T kandTk which are derived from the time scaleT as follows If T has a left-scattered maximum t∗
1, thenTk T−t∗
1, otherwiseTk T If T has a right-scattered minimum t∗
2, thenTk T − t∗
2, otherwise Tk T
the property that given ε > 0 there is a neighborhood U of t with
y σ t − y s − yΔt σ t − s < ε |σ t − s| 1.7
for all s ∈ U, where yΔdenotes thedelta derivative of y with respect to the first variable,
then
g t : t
a
ω t, τ Δτ 1.8 implies
gΔt t
a
ωΔt, τ Δτ ω σ t , τ 1.9
with the property that given ε > 0 there is a neighborhood U of t with
y
ρ t− y s − y∇tρ t − s < ερ t − s 1.10
for all s ∈ U Call y∇t the nabla derivative of yt at the point t.
Trang 4IfT R then fΔt f∇t ft If T Z then fΔt ft 1 − ft is the forward
difference operator while f∇t ft − ft − 1 is the backward difference operator.
right dense points ofT and its left sided limit exists finite at left dense points of T We let
C0
rdT denote the set of rd-continuous functions f : T → R.
all left dense points of T and its right sided limit exists finite at right dense points of T
We let C0
ldT denote the set of ld-continuous functions f : T → R.
FΔt ft holds for all t ∈ T k In this case we define the delta integral of f by
t a
f s Δs F t − F a , 1.11
for all a, t∈ T
providedΦ∇t ft holds for all t ∈ T k In this case we define the nabla integral of f by
t a
f s ∇s Φ t − Φ a , 1.12
for all a, t∈ T
2 Preliminaries
In this section, we provide some necessary background In particular, we state some properties of Green’s function associated with problem1.1, and we then state a fixed-point theorem which is crucial to prove our main results
The basic space used in this paper is E Cρt1, t m It is well known that E is a
Banach space with the norm|| · || defined by ||x|| sup t ∈ρt1,t m|xt| Let P be a cone of E,
P r {x ∈ P : x ≤ r}, ∂P r {x ∈ P : x r}, where r > 0.
In this paper, the Green’s function of the corresponding homogeneous BVP is defined by
G t, s 1
d
⎧
⎨
⎩
ψ t φ s , if ρ t1 ≤ t ≤ s ≤ t m ,
ψ s φ t , if ρ t1 ≤ s ≤ t ≤ t m , 2.1 where
d : αφ t1 − βp t1 φ∇t1 γψ t m δp t m ψ∇t m , 2.2
Trang 5and φ and ψ satisfy
−pψ∇Δ
t q t ψ t 0, ψ t1 β, p t1 ψ∇t1 α,
−pφ∇Δ
t q t φ t 0, φ t m δ, p t m φ∇t m −γ,
2.3
respectively
Lemma 2.1 see 6 Assume that 1.2 and 1.3 hold Then d > 0 and the functions ψ and φ
satisfy
ψ t ≥ 0, t ∈ρ t1 , t m
, ψ t > 0, t ∈ρ t1 , t m
,
p t ψ∇t ≥ 0, t ∈ρ t1 , t m
, φ t ≥ 0, t ∈ρ t1 , t m
,
φ t > 0, t ∈ρ t1 , t m
, p t φ∇t ≤ 0, t ∈ρ t1 , t m
.
2.4
following properties
Proposition 2.2 For t, s ∈ ξ1, ξ2, one has
G t, s > 0, 2.5
where ξ1, ξ2∈ Tk
k , ρ t1 < ξ1 < ξ2< t m
In fact, fromLemma 2.1, we have ψt > 0, φt > 0 for t ∈ ξ1 , ξ2 Therefore 2.5 holds
Proposition 2.3 If 1.2 holds, then for t, s ∈ ρt1, t m × ρt1, t m , one has
0≤ G t, s ≤ G s, s 2.6
Proof In fact, fromLemma 2.1, we obtain ψt ≥ 0, φt ≥ 0 for t ∈ ρt1, t m So Gt, s ≥ 0.
On the other hand, fromLemma 2.1, we know that ptψ∇t ≥ 0, ptφ∇t ≤ 0 for
t ∈ ρt1, t m This together with pt > 0 implies that ψ∇t ≥ 0, φ∇t ≤ 0 for t ∈ ρt1, t m
Hence ψt is nondecreasing on ρt1, t m , φ is nonincreasing on ρt1, t m So 2.6 holds
Proposition 2.4 For all t ∈ ξ1, ξ2, s ∈ ρt1, tm one has
G t, s ≥ σ t G s, s , 2.7
Trang 6σ t : min
ψ t
ψ t m,
φ t
φ
ρ t1
Proof In fact, for t ∈ ξ1 , ξ2, we have
G t, s
G s, s ≥ min
ψ t
ψ s ,
φ t
φ s
≥ min
ψ t
ψ t m,
φ t
φ
ρ t1
: σ t 2.9
Therefore2.7 holds
It is easy to see that 0 < σt < 1, for t ∈ ξ1 , ξ2 Thus, there exists γ > 0 such that
G t, s ≥ γGs, s for t ∈ ξ1 , ξ2, where
γ min {σ t : t ∈ ξ1 , ξ2} 2.10
We remark thatProposition 2.2implies that there exists τ > 0 such that for t, s ∈ ξ1 , ξ2
G t, s ≥ τ. 2.11 Set
D :
−m−2
i 1
a i ψ t i d − m−2
i 1
a i φ t i
d−m−2
i 1
b i ψ t i −m−2
i 1
b i φ t i
Lemma 2.5 see 6 Assume that 1.2 and 1.3 hold If D / 0 and u ∈ C rd t1 , t m , then the
nonhomogeneous boundary value problem
−p t x∇Δ
t q t x t u t , t1 < t < t m ,
αx t1 − βp t1 x∇t1 m−1
i 2
a i x t i ,
γx t m δp t m x∇t m m−1
i 2
b i x t i
2.13
has a unique solution x for which the formula
x t t m
t
G t, s u s Δs Γ u t ψ t Υ u t φ t 2.14
Trang 7holds, where
Γ u s : D1
m−1
i 2
a i
t m
t1
G t i , s u s Δs d − m−1
i 2
a i φ t i
m−1
i 2
b i
t m
t1
G t i , s u s Δs − m−1
i 2
b i φ t i
, 2.15
Υ u s : D1
−m−1
i 2
a i ψ t i m−1
i 2
a i
t m
t1
G t i , s u s Δs
d−m−1
i 2
b i ψ ξ i m−1
i 2
b i
t m
t1
G t i , s u s Δs
. 2.16
By similar method, one can define
Γ0f t, x0 t, Γ1f t, x1 t, Γ2f t, x2 t, Γ∗f t, x∗t,
Υ0f t, x0 t, Υ1f t, x1 t, Υ2f t, x2 t, Υ∗f t, x∗ t. 2.17 The following lemma is crucial to prove our main results
Lemma 2.6 see29,30 Let Ω1 andΩ2be two bounded open sets in a real Banach space E, such
P is a cone in E Suppose that one of the two conditions
i Ax /≥ x, ∀x ∈ P ∩ ∂Ω1; Ax / ≤ x, ∀x ∈ P ∩ ∂Ω2 , 2.18
or
ii Ax /≤ x, ∀x ∈ P ∩ ∂Ω1; Ax / ≥ x, ∀x ∈ P ∩ ∂Ω2 , 2.19
is satisfied Then A has at least one fixed point in P∩ Ω2\ Ω1
3 Main Results
In this section, we applyLemma 2.6to establish the existence of at least two positive solutions for BVP1.1
The following assumptions will stand throughout this paper
H1 There exist υ j1 < 1, υ j2 > 1 such that
inf
t ∈ξ1,ξ2 c j1 t τ1 > 0, inf
t ∈ξ1,ξ2 c j2 t τ2 > 0, j 1, 2, , n, 3.1
where υ j1 , υ j2 , c j1 t and c j2 t are defined in 1.4, respectively
Trang 8H2 We have
D < 0, d−m−1
i 2
a i φ t i > 0, d−m−1
i 2
b i ψ t i > 0 3.2
for d and D given in2.2 and 2.12, respectively
If H2 holds, then we can show that Γft, x, Υft, x have the following
properties
Proposition 3.1 If 1.2–1.4 and H2 hold, then from 2.15, for x ∈ Cρt1, t m , one has
Γf t,x ≤ 1
D
m−1
i 2
a i d−m−1
i 2
a i φ t i
m−1
i 2
b i −m−1
i 2
b i φ t i
M
n
j 1
c j
L x υ j : ΓMn
j 1
c j
L x υ j , 3.3
where c jL: t m
t1|c j s|Δs, M max t,s∈ρt1,t m ×ρt1,t mG t, s.
Proof Let
G m−1
i 2
a i
t m
t1
G t i , s f s, x s Δs, H d − m−1
i 2
a i φ t i ,
F m−1
i 2
b i
t m
t1
G t i , s f s, x s Δs, Q −m−1
i 2
b i φ t i
3.4
Then from1.2–1.4 and H2, we obtain G ≥ 0, F ≥ 0, H > 0, Q ≤ 0 Therefore, GQ ≤
0, −FH ≤ 0.
On the other hand, since
t m
t1
G t i , s f s, x s Δs ≤ Mn
j 1
c j
L x υ j : Λ, 3.5
we have G≤m−1
i 2 a i Λ, F ≤m−1
i 2 b i Λ So one has
m−1
i 2
a i ΛQ − H m−1
i 2
b i Λ ≤ GQ − FH ≤ 0. 3.6
This and D < 0 imply3.3 holds
Trang 9Proposition 3.2 If 1.2–1.4 and H2 hold, then from 2.16, x ∈ Cρt1, t m , one has
Υf t,x ≤ 1 D
−m−1
i 2
a i ψ t i m−1
i 2
a i
d−m−1
i 2
b i ψ ξ i m−1
i 2
b i
M
n
j 1
c j
L x υ j : ΥMn
j 1
c jL x υ j 3.7
Proof The proof is similar to that ofProposition 3.1 So we omit it
For the sake of applying fixed point theorem on cone, we construct a cone in E
C ρt1, t m by
x ∈ E : x t ≥ 0, t ∈ρ t1 , t m
, min
t ∈ξ1,ξ2 x t ≥ γx
, 3.8
where γ is defined in2.10
Define A : P → P by
Ax t t m
t1
G t, s f s, x s Δs Γf t, x tψ t Υf t, x tφ t 3.9
By2.14, it is well known that the problem 1.1 has a positive solution x if and only
if x ∈ P is a fixed point of A.
Lemma 3.3 Suppose that 1.2–1.4 and H1-H2 hold Then AP ⊂ P and A : P → P is
completely continuous.
Ax ≤ t m
t1
G s, s f s, x s Δs Γf t, x tψ t m Υf t, x tφ
ρ t1. 3.10
On the other hand, for t ∈ ξ1 , ξ2, by 3.9,3.10 and 2.7, we obtain
min
t ∈ξ1,ξ2 Ax t min
t ∈ξ1,ξ2
t m
t1
G t, s f s, x s Δs Γf t, x tψ t Υf t, x tφ t
≥σ t t m
t1
G s, s f s, x s ΔsΓf t, x tψ t mΥf t, x tφ
ρ t1
≥ σ t Ax ≥ γAx.
3.11
Therefore Ax ∈ P, that is, AP ⊂ P.
Next by standard methods and the Ascoli-Arzela theorem one can prove that A : P →
P is completely continuous So it is omitted.
Trang 10Theorem 3.4 Suppose that 1.2–1.4 and H1-H2 hold Then problem 1.1 has at least two
positive solutions provided
n
j 1
c j
L
1 Γψ t n Υφ t1< M−1, 3.12
where Γ, Υ and M are defined in 3.3, 3.7 and in Proposition 3.1 , respectively.
Proof Let A be the cone preserving, completely continuous operator that was defined by
3.9
Let S l {x ∈ E : x < l}, where l > 0 Choosing r and r satisfy
0 < r < min
1, ττ1ξ2 − ξ1 1/1−υ j1γ υ j1 / 1−υ j1
,
r > max
1, ττ2ξ2 − ξ1 −1/υ j2−1γ −υ j2 /υ j2−1
.
3.13
Now we prove that
Ax / ≤ x, ∀x ∈ P ∩ ∂S r , 3.14
Ax / ≤ x, ∀x ∈ P ∩ ∂S r 3.15
In fact, if there exists x1 ∈ P ∩ ∂S r such that Ax1 ≤ x1, then for t ∈ ξ1 , ξ2, we have
x1t ≥ Ax1 t
t m
t1
G t, s f s, x1 s Δs Γ1f t, x1 tψ t Υ1f t, x1 tφ t
≥ t m
t1
G t, s f s, x1 s Δs
≥ ξ2
ξ1
G t, s c j1 s x1s υ j1 Δs
≥ ττ1 ξ2 − ξ1 γ υ j1 x1 υ j1 ,
3.16
whereΓ1ft, xt, Υ1ft, xt defined by 2.17
Therefore r ≥ ττ1ξ2 − ξ1γ υ j1 r υ j1 , that is, r ≥ ττ1ξ2 − ξ1 1/1−υ j1γ υ j1 / 1−υ j1, which is a contradiction Hence3.14 holds