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Electronic Journal of Qualitative Theory of Differential Equations 2011, No. 98, 1-16;http://www.math.u-szeged.hu/ejqtde/

Even Number of Positive Solutions for 3 n

th

Order Three-Point Boundary Value Problems on Time Scales

K. R. Prasad

1

and N. Sreedhar

2

1Department of Applied Mathematics, Andhra University, Visakhapatnam, 530 003, India.

rajendra92@rediffmail.com

2Department of Mathematics,

GITAM University, Visakhapatnam, 530 045, India.

sreedharnamburi@rediffmail.com Abstract

We establish the existence of at least two positive solutions for the 3nth order three-point boundary value problem on time scales by using Avery-Henderson fixed point theorem. We also establish the existence of at least 2m positive solutions for an arbitrary positive integer m.

Key words: Green’s function, boundary value problem, time scale, positive solution, cone.

AMS Subject Classification: 39A10, 34B05.

1 Introduction

The theory of time scales was introduced and developed by Hilger [13] to unify both continuous and discrete analysis. Time scales theory presents us with the tools necessary to understand and explain the mathematical structure underpinning the theories of discrete and continuous dynamic systems and allows us to connect them. The theory is widely applied to various situations like epidemic models, the stock market and mathematical modeling of physical and biological systems. Certain economically important phenomena contain processes that feature elements of both the continuous and discrete.

In recent years, the existence of positive solutions of the higher order boundary value problems (BVPs) on time scales have been studied extensively due to their striking applications to almost all area of science, engineering and technology. The existence of positive solutions are studied by many authors.

A few papers along these lines are Henderson [11], Anderson [1, 2], Kaufmann

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[15], Anderson and Avery [3], DaCunha, Davis and Singh [10], Peterson, Raf- foul and Tisdell [18], Sun and Li [19], Luo and Ma [17], Cetin and Topal [8], Karaca [14] and Anderson and Karaca [4].

In this paper, we are concerned with the existence of positive solutions for the 3nth order BVP on time scales,

(−1)ny(3n)(t) =f(t, y(t)), t∈[t1, σ(t3)] (1.1) satisfying the general three-point boundary conditions,

α3i−2,1y(3i−3)(t1) +α3i−2,2y(3i−2)(t1) +α3i−2,3y(3i−1)(t1) = 0, α3i−1,1y(3i−3)(t2) +α3i−1,2y(3i−2)(t2) +α3i−1,3y(3i−1)(t2) = 0, α3i,1y(3i−3)(σ(t3)) +α3i,2y(3i−2)(σ(t3)) +α3i,3y(3i−1)(σ(t3)) = 0,





(1.2)

for 1 ≤ i ≤ n, where n ≥ 1, α3i−2,j, α3i−1,j, α3i,j, for j = 1,2,3, are real constants, t1 < t2 < σ(t3) and f : [t1, σ(t3)]×R+ → R+ is continuous. For convenience, we use the following notations. For 1 ≤ i ≤ n, let us denote βij3i−3+j,1tj3i−3+j,2, γij3i−3+j,1t2j3i−3+j,2(tj+σ(tj)) + 2α3i−3+j,3, where j = 1,2; βi3 = α3i,1σ(t3) +α3i,2 and γi3 = α3i,1(σ(t3))23i,2(σ(t3) + σ2(t3)) + 2α3i,3. Also, for 1≤i≤n, we define

mijk = α3i−3+j,1γik−α3i−3+k,1γij

2(α3i3+j,1βik −α3i3+k,1βij), Mijk = βijγik−βikγij

α3i3+j,1βik −α3i3+k,1βij

,

where j, k = 1,2,3 and let pi = max{mi12, mi13, mi23}, qi = min

mi23 +q

m2i23−Mi23, mi13 +q

m2i13−Mi13

,

di3i−2,1i2γi3−βi3γi2)−βi13i−1,1γi3−α3i,1γi2) +γi13i−1,1βi3−α3i,1βi2) and lij = α3i−3+j,1σ(s)σ2(s)−βij(σ(s) +σ2(s)) +γij, where j = 1,2,3. We assume the following conditions throughout this paper:

(A1) α3i−2,1 > 0, α3i−1,1 > 0, α3i,1 > 0 and αα3i,23i,1 > αα3i−1,2

3i−1,1 > αα3i−2,2

3i−2,1, for all 1≤i≤n,

(A2) pi ≤t1 < t2 < σ(t3)≤qi and 2α3i−2,3α3i−2,1 > α3i−2 2,2, 2α3i−1,3α3i−1,1 < α23i−1,2, 2α3i,3α3i,1 > α23i,2, for all 1≤i≤n,

(A3) m2i23 > Mi23,m2i12 < Mi12, m2i13 > Mi13 and di >0, for all 1≤ i≤n, (A4) The pointt ∈[t1, σ(t3)] is not left dense and right scattered at the same

time.

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This paper is organized as follows. In Section 2, we construct the Green’s function for the homogeneous problem corresponding to (1.1)-(1.2) and esti- mate bounds for the Green’s function. In Section 3, we establish a criteria for the existence of at least two positive solutions for the BVP (1.1)-(1.2) by using an Avery-Henderson fixed point theorem [5]. We also establish the existence of at least 2m positive solutions for an arbitrary positive integer m. Finally as an application, we give an example to illustrate our result.

2 Green’s Function and Bounds

In this section, we construct the Green’s function for the homogeneous prob- lem corresponding to (1.1)-(1.2) and estimate bounds for the Green’s function.

LetGi(t, s) be the Green’s function for the homogeneous BVP,

−y3(t) = 0, t ∈[t1, σ(t3)], (2.1) satisfying the general three-point boundary conditions,

α3i−2,1y(t1) +α3i−2,2y(t1) +α3i−2,3y2(t1) = 0, α3i−1,1y(t2) +α3i−1,2y(t2) +α3i−1,3y2(t2) = 0, α3i,1y(σ(t3)) +α3i,2y(σ(t3)) +α3i,3y2(σ(t3)) = 0,





(2.2)

for 1≤i≤n.

Lemma 2.1 For1≤i≤n, the Green’s function Gi(t, s)for the homogeneous BVP (2.1)-(2.2) is given by

Gi(t, s) =

















Gi(t,s) t∈[t1,t2]=

Gi1(t, s), t1 < σ(s)< t≤t2 < σ(t3) Gi2(t, s), t1 ≤t < s < t2 < σ(t3) Gi3(t, s), t1 ≤t < t2 < s < σ(t3)

Gi(t,s) t∈[t2,σ(t3)] =

Gi4(t, s), t1 < t2 < σ(s)< t≤σ(t3) Gi5(t, s), t1 < t2 ≤t < s < σ(t3) Gi6(t, s), t1 ≤σ(s)< t2 < t < σ(t3)

(2.3)

where

Gi1(t, s) = 1 2di

[−(βi2γi3 −βi3γi2) +t(α3i−1,1γi3 −α3i,1γi2)−t23i−1,1βi3− α3i,1βi2)]li1,

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Gi2(t, s) = 1 2di

{[−(βi1γi3 −βi3γi1) +t(α3i2,1γi3 −α3i,1γi1)−t23i2,1βi3− α3i,1βi1)]li2 + [(βi1γi2 −βi2γi1)−t(α3i−2,1γi2 −α3i−1,1γi1)+

t23i−2,1βi2 −α3i−1,1βi1)]li3}, Gi3(t, s) = 1

2di

[(βi1γi2 −βi2γi1)−t(α3i−2,1γi2 −α3i−1,1γi1) +t23i−2,1βi2− α3i−1,1βi1)]li3,

Gi4(t, s) = 1 2di

{[−(βi2γi3 −βi3γi2) +t(α3i−1,1γi3 −α3i,1γi2)−t23i−1,1βi3− α3i,1βi2)]li1 + [(βi1γi3 −βi3γi1)−t(α3i−2,1γi3 −α3i,1γi1)+

t23i−2,1βi3 −α3i,1βi1)]li2}, Gi5(t, s) = 1

2di

[(βi1γi2 −βi2γi1)−t(α3i−2,1γi2 −α3i−1,1γi1) +t23i−2,1βi2− α3i−1,1βi1)]li3,

Gi6(t, s) = 1 2di

[−(βi2γi3 −βi3γi2) +t(α3i−1,1γi3 −α3i,1γi2)−t23i−1,1βi3− α3i,1βi2)]li1.

Lemma 2.2 Assume that the conditions (A1)-(A4) are satisfied. Then, for 1 ≤ i ≤ n, the Green’s function Gi(t, s) of (2.1)-(2.2) is positive, for all (t, s)∈[t1, σ(t3)]×[t1, t3].

Proof: For 1≤i≤n, the Green’s functionGi(t, s) is given in (2.3). We prove the result for Gi1(t, s). Then, Gi1(t, s) = gi1(t)li1(s), where

gi1(t) = 1 2di

[−(βi2γi3 −βi3γi2) +t(α3i−1,1γi3 −α3i,1γi2)−t23i−1,1βi3− α3i,1βi2)].

Using the conditions (A1) and (A4), gi1(t) has maximum at t = mi23, and hence gi1(t) > 0 on [t1, σ(t3)] by conditions (A2) and (A3). From conditions (A2) and (A4),li1(s)>0 on [t1, t3].

Therefore,

Gi1(t, s)>0, for all (t, s)∈[t1, σ(t3)]×[t1, t3].

Similarly, we can establish the positivity of the Green’s function in the remain-

ing cases. 2

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Theorem 2.3 Assume that the conditions (A1)-(A4) are satisfied. Then, for 1≤i≤n, the Green’s function Gi(t, s) satisfies the following inequality,

miGi(σ(s), s)≤Gi(t, s)≤Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3], (2.4) where

0< mi = min

(Gi1(σ(t3), s)

Gi1(t1, s) , Gi3(t1, s)

Gi3(σ(t3), s), Gi2(t1, s)

Gi2(σ(t3), s),Gi4(σ(t3), s) Gi4(t1, s)

)

<1.

Proof: For 1≤i≤n, the Green’s functionGi(t, s) is given (2.3) in six different cases. In each case, we prove the inequality as in (2.4).

Case 1. Fort1 < σ(s)< t≤t2 < σ(t3).

Gi(t,s)

Gi(σ(s),s)= GGi1(t,s)

i1(σ(s),s)

= [−(βi2γi3 −βi3γi2) +t(α3i−1,1γi3 −α3i,1γi2)−t23i−1,1βi3 −α3i,1βi2)]

[−(βi2γi3 −βi3γi2) +σ(s)(α3i1,1γi3−α3i,1γi2)−(σ(s))23i1,1βi3 −α3i,1βi2)]. From (A1)-(A4), we have Gi1(t, s)≤Gi1(σ(s), s) and also

Gi(t, s)

Gi(σ(s), s) = Gi1(t, s)

Gi1(σ(s), s) ≥ Gi1(t, s)

Gi1(t1, s) ≥ Gi1(σ(t3), s) Gi1(t1, s) . Therefore, Gi(t, s) ≤ Gi(σ(s), s) and Gi(t, s) ≥ GGi1(σ(t3),s)

i1(t1,s) Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3].

Case 2. Fort1 ≤t < t2 < s < σ(t3).

Gi(t,s)

Gi(σ(s),s)= GGi3(t,s)

i3(σ(s),s)

= [(βi1γi2 −βi2γi1)−t(α3i−2,1γi2−α3i−1,1γi1) +t23i−2,1βi2 −α3i−1,1βi1)]

[(βi1γi2 −βi2γi1)−σ(s)(α3i−2,1γi2 −α3i−1,1γi1) + (σ(s))23i−2,1βi2 −α3i−1,1βi1)]. From (A1)-(A4), we have Gi3(t, s)≤Gi3(σ(s), s) and also

Gi(t, s)

Gi(σ(s), s) = Gi3(t, s)

Gi3(σ(s), s) ≥ Gi3(t, s)

Gi3(σ(t3), s) ≥ Gi3(t1, s) Gi3(σ(t3), s). Therefore, Gi(t, s) ≤ Gi(σ(s), s) and Gi(t, s) ≥ GGi3(t1,s)

i3(σ(t3),s) Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3].

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Case 3. Fort1 ≤t < s < t2 < σ(t3).

From (A1)-(A4) and case 2, we have Gi2(t, s)≤Gi2(σ(s), s) and also Gi(t, s)

Gi(σ(s), s) ≥min

( Gi3(t1, s)

Gi3(σ(t3), s), Gi2(t1, s) Gi2(σ(t3), s)

) . Therefore, Gi(t, s)≤Gi(σ(s), s) and

Gi(t, s)≥min

( Gi3(t1, s)

Gi3(σ(t3), s), Gi2(t1, s) Gi2(σ(t3), s)

)

Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3].

Case 4. Fort1 < t2 < σ(s)< t≤σ(t3).

From (A1)-(A4) and case 1, we have Gi4(t, s)≤Gi4(σ(s), s) and Gi(t, s)

Gi(σ(s), s) ≥min

(Gi1(σ(t3), s)

Gi1(t1, s) ,Gi4(σ(t3), s) Gi4(t1, s)

) . Therefore, Gi(t, s)≤Gi(σ(s), s) and

Gi(t, s)≥min

(Gi1(σ(t3), s)

Gi1(t1, s) ,Gi4(σ(t3), s) Gi4(t1, s)

)

Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3].

Case 5. Fort1 < t2 ≤t < s < σ(t3).

From case 2, we haveGi(t, s)≤Gi(σ(s), s) andGi(t, s)≥ GGi3(t1,s)

i3(σ(t3),s)Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3].

Case 6. Fort1 ≤σ(s)< t2 < t < σ(t3).

From case 1, we haveGi(t, s)≤Gi(σ(s), s) andGi(t, s)≥ GGi1(σ(t3),s)

i1(t1,s) Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3].

From all above cases, for 1≤i≤n, we have

miGi(σ(s), s)≤Gi(t, s)≤Gi(σ(s), s), for all (t, s)∈[t1, σ(t3)]×[t1, t3],

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where

0< mi = min

(Gi1(σ(t3), s)

Gi1(t1, s) , Gi3(t1, s)

Gi3(σ(t3), s), Gi2(t1, s)

Gi2(σ(t3), s),Gi4(σ(t3), s) Gi4(t1, s)

)

<1.

2 Lemma 2.4 Assume that the conditions (A1)-(A4) are satisfied and Gi(t, s) is defined as in (2.3). Take H1(t, s) =G1(t, s) and recursively define

Hj(t, s) =

Z σ(t3) t1

Hj1(t, r)Gj(r, s)∆r, f or 2≤j ≤n.

ThenHn(t, s)is the Green’s function for the homogeneous BVP corresponding to (1.1)-(1.2).

Lemma 2.5 Assume that the conditions (A1)-(A4) hold. If we define K =

n−1

Y

j=1

Kj and L=

n−1

Y

j=1

mjLj, then the Green’s function Hn(t, s) in Lemma 2.4 satisfies

0≤Hn(t, s)≤K kGn(·, s)k, for all (t, s)∈[t1, σ(t3)]×[t1, t3] and

Hn(t, s)≥mnLkGn(·, s)k, for all (t, s)∈[t2, σ(t3)]×[t1, t3], where mn is given as in Theorem 2.3,

Kj =

Z σ(t3) t1

kGj(·, s)k∆s >0, f or 1≤j ≤n,

Lj =

Z σ(t3) t2

kGj(·, s)k∆s >0, f or 1≤j ≤n and k · k is defined by

kxk= max

t[t1,σ(t3)]|x(t)|.

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3 Multiple Positive Solutions

In this section, we establish the existence of at least two positive solutions for the BVP (1.1)-(1.2) by using an Avery-Henderson functional fixed point theorem. And then, we establish the existence of at least 2mpositive solutions for an arbitrary positive integer m.

Let B be a real Banach space. A nonempty closed convex set P ⊂ B is called a cone, if it satisfies the following two conditions:

(i) y∈P, λ≥0 implies λy ∈P, and (ii) y∈P and −y∈P impliesy= 0.

Let ψ be a nonnegative continuous functional on a cone P of the real Banach space B. Then for a positive real number c, we define the sets

P(ψ, c) ={y∈P :ψ(y)< c} and

Pa ={y∈P :kyk< a}.

In obtaining multiple positive solutions of the BVP (1.1)-(1.2), the follow- ing Avery-Henderson functional fixed point theorem will be the fundamental tool.

Theorem 3.1 [5]Let P be a cone in a real Banach space B. Supposeα andγ are increasing, nonnegative continuous functionals on P and θ is nonnegative continuous functional onP withθ(0) = 0such that, for some positive numbers c and k, γ(y)≤ θ(y) ≤α(y) and k yk≤ kγ(y), for all y ∈P(γ, c). Suppose that there exist positive numbers a and b with a < b < c such that θ(λy)≤ λθ(y), for all 0≤ λ≤1 and y∈∂P(θ, b). Further, let T :P(γ, c)→P be a completely continuous operator such that

(B1) γ(T y)> c, for all y∈∂P(γ, c), (B2) θ(T y)< b, for ally ∈∂P(θ, b),

(B3) P(α, a)6=∅ and α(T y)> a, for all y∈∂P(α, a).

Then, T has at least two fixed points y1, y2 ∈P(γ, c) such that a < α(y1) with θ(y1)< b and b < θ(y2) withγ(y2)< c. Let

M =mn n−1

Y

j=1

mjLj

Kj

(3.1)

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Let B ={y:y∈C[t1, σ(t3)]} be the Banach space equipped with the norm ky k= max

t∈[t1,σ(t3)]|y(t)|.

Define the cone P ⊂B by

P ={y∈B :y(t)≥0 on [t1, σ(t3)] and min

t[t2,σ(t3)]y(t)≥M kyk}, where M is given as in (3.1).

Define the nonnegative, increasing, continuous functionals γ, θ and α on the cone P by

γ(y) = min

t[t2,σ(t3)]y(t), θ(y) = max

t[t2,σ(t3)]y(t) andα(y) = max

t[t1,σ(t3)]y(t).

We observe that for any y∈P,

γ(y)≤θ(y)≤α(y) (3.2)

and

kyk≤ 1

M min

t∈[t2,σ(t3)]y(t) = 1

Mγ(y)≤ 1

Mθ(y)≤ 1

Mα(y). (3.3) Theorem 3.2 Suppose there exist 0 < a < b < c such that f satisfies the following conditions.

(D1) f(t, y)> Πn c

j=1mjLj, for t∈[t2, σ(t3)] and y∈[c,Mc], (D2) f(t, y)< Πnb

j=1Kj, fort ∈[t1, σ(t3)] and y∈[0,Mb], (D3) f(t, y)> Πn a

j=1mjLj, for t∈[t2, σ(t3)] and y∈[a,Ma],

where mn and M are defined in Theorem 2.3 and (3.1) respectively. Then the BVP (1.1)-(1.2) has at least two positive solutions y1 and y2 such that

a < max

t∈[t1,σ(t3)]y1(t) with max

t∈[t2,σ(t3)]y1(t)< b, b < max

t[t2,σ(t3)]y2(t) with min

t[t2,σ(t3)]y2(t)< c. Proof: Define the operator T :P →B by

T y(t) =

Z σ(t3) t1

Hn(t, s)f(s, y(s))∆s. (3.4) It is obvious that a fixed point of T is the solution of the BVP (1.1)-(1.2). We seek two fixed points y1, y2 ∈ P of T. First, we show that T : P → P. Let

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y ∈ P. From Theorem 2.3 and Lemma 2.5, we have T y(t) ≥ 0 on [t1, σ(t3)]

and also,

T y(t) =

Z σ(t3) t1

Hn(t, s)f(s, y(s))∆s

≤K Z σ(t3)

t1

kGn(·, s)kf(s, y(s))∆s so that

kT y k≤K

Z σ(t3) t1

kGn(·, s)kf(s, y(s))∆s.

Next, if y∈P, then we have T y(t) =

Z σ(t3) t1

Hn(t, s)f(s, y(s))∆s

≥mnL Z σ(t3)

t1

kGn(·, s)kf(s, y(s))∆s

≥ mnL

K kT y k=M kT y k.

HenceT y ∈P and soT :P →P. Moreover,T is completely continuous. From (3.2) and (3.3), for eachy∈P, we haveγ(y)≤θ(y)≤α(y) andky k≤ M1γ(y).

Also, for any 0 ≤ λ ≤ 1 and y ∈ P, we have θ(λy) = maxt∈[t2,σ(t3)](λy)(t) = λmaxt[t2,σ(t3)]y(t) = λθ(y). It is clear that θ(0) = 0. We now show that the remaining conditions of Theorem 3.1 are satisfied.

Firstly, we shall verify that condition (B1) of Theorem 3.1 is satisfied. Since y∈∂P(γ, c), from (3.3) we have thatc = mint[t2,σ(t3)]y(t)≤kyk≤ Mc. Then

γ(T y) = min

t[t2,σ(t3)]

Z σ(t3) t1

Hn(t, s)f(s, y(s))∆s

≥ min

t∈[t2,σ(t3)]

Z σ(t3) t2

Hn(t, s)f(s, y(s))∆s

> c

Πnj=1mjLjmnL Z σ(t3)

t2

kGn(·, s)k∆s=c, using hypothesis (D1).

Now we shall show that condition (B2) of Theorem 3.1 is satisfied. Since y ∈ ∂P(θ, b), from (3.3) we have that 0 ≤ y(t) ≤k y k≤ Mb, for [t1, σ(t3)].

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Thus

θ(T y) = max

t∈[t2,σ(t3)]

Z σ(t3) t1

Hn(t, s)f(s, y(s))∆s

< b Πnj=1Kj

K

Z σ(t3) t1

kGn(·, s)k∆s=b, by hypothesis (D2).

Finally, using hypothesis (D3), we shall show that condition (B3) of Theorem 3.1 is satisfied. Since 0 ∈ P and a > 0, P(α, a) 6= ∅. Since y ∈ ∂P(α, a), a = maxt∈[t1,σ(t3)]y(t)≤kyk≤ Ma, fort ∈[t2, σ(t3)]. Therefore,

α(T y) = max

t∈[t1,σ(t3)]

Z σ(t3) t1

Hn(t, s)f(s, y(s))∆s

Z σ(t3) t1

Hn(t, s)f(s, y(s))∆s

> a Πnj=1mjLj

mnL Z σ(t3)

t2

kGn(·, s)k∆s=a.

Thus, all the conditions of Theorem 3.1 are satisfied and so there exist at least two positive solutionsy1, y2 ∈P(γ, c) for the BVP (1.1)-(1.2). This completes

the proof of the theorem. 2

Theorem 3.3 Let m be an arbitrary positive integer. Assume that there exist numbers ar(r = 1,2,· · ·, m+ 1) and bs(s = 1,2,· · ·, m) with 0 < a1 < b1 <

a2 < b2 <· · ·< am < bm < am+1 such that f(t, y)> ar

Πnj=1mjLj

, f or t∈[t2, σ(t3)] and y ∈[ar, ar

M], r= 1,2,· · ·, m+ 1, (3.5) f(t, y)< bs

Πnj=1Kj, f or t∈[t1, σ(t3)] and y∈[0, bs

M], s= 1,2,· · ·, m. (3.6) Then the BVP (1.1)-(1.2) has at least 2m positive solutions in Pam+1.

Proof: We use induction on m. Form= 1, we know from (3.5) and (3.6) that T : Pa2 → Pa2, then, it follows from Avery-Henderson fixed point theorem that the BVP (1.1)-(1.2) has at least two positive solutions in Pa2. Next, we assume that this conclusion holds for m=l. In order to prove this conclusion holds form=l+ 1. We suppose that there exist numbersar(r = 1,2,· · ·, l+ 2)

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andbs(s= 1,2,· · ·, l+ 1) with 0< a1 < b1 < a2 < b2 <· · ·< al+1 < bl+1 < al+2

such that

f(t, y)> ar

Πnj=1mjLj

, for t ∈[t2, σ(t3)] and y∈[ar, ar

M], r = 1,2,· · ·, l+ 2, (3.7) f(t, y)< bs

Πnj=1Kj

, fort ∈[t1, σ(t3)] andy ∈[0, bs

M], s= 1,2,· · ·, l+ 1.

(3.8) By assumption, the BVP (1.1)-(1.2) has at least 2l positive solutions yi(i = 1,2,· · ·,2l) in Pal+1. At the same time, it follows from Theorem 3.2, (3.7) and (3.8) that the BVP (1.1)-(1.2) has at least two positive solutionsy1, y2inPal+2

such that al+1 < α(y1) with θ(y1) < bl+1 and bl+1 < θ(y2) with γ(y2) < al+2. Obviously y1 and y2 are different from yi(i= 1,2,· · ·,2l). Therefore, the BVP (1.1)-(1.2) has at least 2l+ 2 positive solutions inPal+2, which shows that this

conclusion holds for m=l+ 1. 2

4 Example

Let us consider an example to illustrate the usage of the Theorem 3.2. Let n = 2 andT={0} ∪ {2n+11 :n∈N} ∪[12,32]. Now, consider the following BVP,

y6(t) = 800(y+ 1)4

73(y2+ 999), t∈[0, σ(1)]∩T (4.1) subject to the boundary conditions,

1

2y(0)−y(0) + 2y2(0) = 0, 2y1

2

−3y1 2

+ 2y21 2

= 0, y(σ(1)) + 1

2y(σ(1)) +1

3y2(σ(1)) = 0, 3

4y3(0)−2y4(0) + 3y5(0) = 0, y31

2

−2y41 2

+y51 2

= 0, y3(σ(1)) + 1

2y4(σ(1)) +1

2y5(σ(1)) = 0.





































(4.2)

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Then the conditions (A1)-(A4) are satisfied. The Green’s function G1(t, s) in Lemma 2.1 is

G1(t, s) =

















G1(t,s) t∈[0,12] =

G11(t, s), 0< σ(s)< t≤ 12 < σ(1) G12(t, s), 0≤t < s < 12 < σ(1) G13(t, s), 0≤t < 12 < s < σ(1)

G1(t,s) t[12,σ(1)] =

G14(t, s), 0< 12 < σ(s)< t≤σ(1) G15(t, s), 0< 12 ≤t < s < σ(1) G16(t, s), 0≤σ(s)< 12 < t < σ(1) where

G11(t, s) = 12 481

h91 12+ 23

6 t−5t2ih1

2σ(s)σ2(s) + (σ(s) +σ2(s)) + 4i , G12(t, s) = 12

481 nh26

3 − 8 3t−7

4t2ih

2σ(s)σ2(s) + 2(σ(s) +σ2(s)) + 3 2 i

+h13 2 +29

4 t+t2ih

σ(s)σ2(s)− 3

2(σ(s) +σ2(s)) + 8 3

io , G13(t, s) = 12

481 h13

2 +29

4 t+t2ih

σ(s)σ2(s)− 3

2(σ(s) +σ2(s)) + 8 3

i, G14(t, s) = 12

481 nh91

12+ 23

6 t−5t2ih1

2σ(s)σ2(s) + (σ(s) +σ2(s)) + 4i +h

− 26 3 +8

3t+ 7 4t2ih

2σ(s)σ2(s) + 2(σ(s) +σ2(s)) + 3 2

io , G15(t, s) = 12

481 h13

2 +29

4 t+t2ih

σ(s)σ2(s)− 3

2(σ(s) +σ2(s)) + 8 3 i

, G16(t, s) = 12

481 h91

12+ 23

6 t−5t2ih1

2σ(s)σ2(s) + (σ(s) +σ2(s)) + 4i . The Green’s function G2(t, s) in Lemma 2.1 is

G2(t, s) =

















G2(t,s) t∈[0,12] =

G21(t, s), 0< σ(s)< t≤ 12 < σ(1) G22(t, s), 0≤t < s < 12 < σ(1) G23(t, s), 0≤t < 12 < s < σ(1)

G2(t,s) t∈[12,σ(1)] =

G24(t, s), 0< 12 < σ(s)< t≤σ(1) G25(t, s), 0< 12 ≤t < s < σ(1) G26(t, s), 0≤σ(s)< 12 < t < σ(1) where

G21(t, s) = 16 635

h39 8 +11

4 t−3t2ih3

4σ(s)σ2(s) + 2(σ(s) +σ2(s)) + 6i ,

(14)

G22(t, s) = 16 635

nh15− 15 4 t−25

8 t2ih

σ(s)σ2(s) + 3

2(σ(s) +σ2(s)) + 1 4 i

+h17 2 +93

16t+7 8t2ih

σ(s)σ2(s)− 3

2(σ(s) +σ2(s)) + 3io , G23(t, s) = 16

635 h17

2 + 93 16t+ 7

8t2ih

σ(s)σ2(s)− 3

2(σ(s) +σ2(s)) + 3i , G24(t, s) = 16

635 nh39

8 +11

4 t−3t2ih3

4σ(s)σ2(s) + 2(σ(s) +σ2(s)) + 6i +h

−15 + 15 4 t+25

8 t2ih

σ(s)σ2(s) + 3

2(σ(s) +σ2(s)) + 1 4

io , G25(t, s) = 16

635 h17

2 + 93 16t+ 7

8t2ih

σ(s)σ2(s)− 3

2(σ(s) +σ2(s)) + 3i , G26(t, s) = 16

635 h39

8 +11

4 t−3t2ih3

4σ(s)σ2(s) + 2(σ(s) +σ2(s)) + 6i . From Theorem 2.3 and Lemma 2.5, we get

m1 = 0.4406779661, K1 = 0.6552328771, L1 = 0.183991684, m2 = 0.5596707819, K2 = 0.7449516076, L2 = 0.2551181102.

Therefore, K = 0.6552328771, L = 0.08108108108 and M = 0.06925585335.

Clearly f is continuous and increasing on [0,∞). If we choose a = 0.0001, b = 0.04 and c = 100 then 0< a < b < c and f satisfies

(i) f(t, y)>8637.8676 = Π2 c

j=1mjLj, for t∈[12, σ(1)] and y∈[100,1443.9212], (ii) f(t, y)<0.081947 = Π2b

j=1Kj, for t∈[0, σ(1)] and y ∈[0,0.577568], (iii) f(t, y)>0.008637 = Π2 a

j=1mjLj, for t∈[12, σ(1)] and y∈[0.0001,0.001443].

Then all the conditions of Theorem 3.2 are satisfied. Thus by Theorem 3.2, the BVP (4.1)-(4.2) has at least two positive solutions y1 and y2 satisfying

0.0001< max

t[0,σ(1)]y1(t) with max

t∈[12,σ(1)]

y1(t)<0.04, 0.04< max

t∈[12,σ(1)]y2(t) with min

t∈[12,σ(1)]y2(t)<100.

Acknowledgements: The authors thank the referees for their valuable sug- gestions and comments.

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References

[1] D. R. Anderson, Solutions to second order three-point problems on time scales, J. Difference Eqn. Appl., 8(2002), 673-688.

[2] D. R. Anderson, Nonlinear triple-point problems on time scales, Elec. J.

Diff. Eqns., 47(2004), 1-12.

[3] D. R. Anderson and R. I. Avery, An even order three-point boundary value problem on time scales, J. Math. Anal. Appl., 291(2004), 514-525.

[4] D. R. Anderson and I. Y. Karaca, Higher order three-point boundary value problem on time scales, Comp. Math. Appl., 56(2008), 2429-2443.

[5] R. I. Avery and J. Henderson, Two positive fixed points of nonlinear oper- ators on ordered Banach spaces, Comm. Appl. Nonlinear Anal.,8(2001), 27-36.

[6] M. Bohner and A. C. Peterson, Dynamic Equations on Time Scales, An Introduction with Applications, Birkhauser, Boston, MA, 2001.

[7] M. Bohner and A. C. Peterson,Advances in Dynamic Equations on Time Scales, Birkhauser, Boston, 2003.

[8] E. Cetin and S. G. Topal, Higher order boundary value problems on time scales, J. Math. Anal. Appl., 334(2007), 876-888.

[9] C. J. Chyan, Eigenvalue intervals for 2mth order Sturm-Liouville bound- ary value problems, J. Difference Eqn. Appl.,8(2002), 403-413.

[10] J. J. DaCunha, J. M. Davis and P. K. Singh, Existence results for singular three-point boundary value problems on time scales,J. Math. Anal. Appl., 295(2004), 378-391.

[11] J. Henderson, Multiple solutions for 2mthorder Sturm-Liouville boundary value problems on a measure chain, J. Difference Eqn. Appl., 6(2000), 417-429.

[12] J. Henderson and K. R. Prasad, Comparison of eigenvalues for Lidstone boundary value problems on a measure chain, Comput. Math. Appl., 38(1999), 55-62.

[13] S. Hilger, Analysis on measure chains - A unified approach to continuous and discrete calculus, Results Math., 18(1980), 18-56.

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[14] I. Y. Karaca, Positive solutions to nonlinear three-point boundary value problems on time scales, Panamer. Math. J., 17(2007), 33-49.

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[16] M. A. Krasnosel’skii, Positive Solutions of Operator Equations, Noord- hoff, Groningen, 1964.

[17] H. Luo and Q. Ma, Positive solutions to a generalized second order three-point boundary value problem on time scales, Elec. J. Diff. Eqns., 17(2005), 1-14.

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(Received October 9, 2011)

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