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The Boundary Value Problems of Higher Order

Mixed Type of Delay Differential Equations

Meiyu Fang, Bo Du

Abstract—In this paper, by using a fixed-point theorem in cones to study the boundary value problem for a class of higher order mixed type of delay differential equations with singularity. The sufficient condition of existence of their solutions is derived. Some examples are included to illustrate the results.

Index Terms—Boundary value problem, higher order mixed type of delay differential equations, positive solution, fixed point.

I. INTRODUCTION

I

N this paper, we consider the existence of positive solutions to the following higher order mixed-type of delay differential equations

     

    

−u(n)(t) =λp(t)f[t, u(tτ),Rt

0k(t, s)u(s)ds],

0< t <1, τ >0,

u(t) =u0(t) =· · ·=u(n−3)(t) =u(n−2)(t) = 0,

−τ ≤t≤0, (1.1)

u(n−2)(1) = (n1)!au(η).

whereλis a positive real parameter;n≥2is an integer.

In equation (1.1), we assume that the following conditions

(H1)−(H5)hold

(H1)f ∈C(J×R×R, R), J= [0,1],0< a≤1,

0< η <1,0< τ < 12.

(H2)p(s)∈C(J1, R+), J1= (0,1).

(H3)v(t) =R

t

0k(t, s)u(s)ds, D={(t, s)∈J×J :

t > s}, k(t, s)∈C(D, R+).

k0= min{k(s, t) : (s, t)∈D},

k1= max{k(s, t) : (s, t)∈D}

(H4)u∈C[−τ,1]TC(n)[0,1];u(t)≥0, t∈[−τ,1].

(H5) R1

0 s(1−s)p(s)ds <∞,∃θ[

τ

2, 1−τ

2 )

such thatRθ1+τθ+τG2(s, s)p(s)ds >0.

Boundary value problems(BVPS) for higher-order delay differential equations arise naturally in various applications to physical, biological, and chemical processes. Frequently, these occur in the form of a multipoint boundary value

Manuscript received April , 2016; revised June 15, 2016. This work is supported in part by the Ministry of Education, Humanities, and Social Sciences Research Project Fund of China (No.z14YJAZH018), Zhejiang provincial higher education teaching reform project (No. jg2015134).

M.Y. Fang is with School of Science and Technology, Zhejiang Inter-nationnal Studies University, Hangzhou, Zhejiang, 310012 P.R.China e-mail:[email protected].

B.Du is with Department of Mathematics,Huaiyin Normal Universi-ty,Huaian 241005, P.R.China.

problem for an nth-order ordinary differential equations,

such as an n-degrees of freedom in which n states are observed at ntimes[2,3]. In recent years, many researchers have done a great deal of research works upon lower order differential equations with delay, and some good results were produced, see, for example [4-22]. But higher order cases haven not been focused. BVPS of higher-order differential equations have received a few of attention (see [23,24,25,26]).

For n = 2, v = 0, in the case of ordinary differential equations, BVPs analogous to (1.1) with singularity has been widely studies by many authors, see,for example, [12,15-17]. For the caseτ = 0, v= 0,anda= 0, Graef and Yang [23] obtain respectfully the existence of positive solutions to two-point and multi-two-point BVPs (1.1) whenu(n)=λp(t)f(u(t)). In the casev= 0, a= 0, Shen and Dong [24]have applied a fixed-point theorem to derive the sufficient conditions which assure that the equation (−u(n) =λp(t)f(t, u(tτ)),0 <

t <1) with the boundary conditions (u(0) =u0(0) =· · ·= u(n−3)=u(n−2)= 0,τ t0;u(n−2)(1) = 0) have the

positive solutions, andp(t) has some suitable singularity at the ends of (0,1).

In the paper, we prove that the existence of positive solutions of the more general BVPs for n-order (n ≥ 2)

differential equations (1.1).

For the existence of positive solutions of the boundary value problem of two or higher order differential equations, we mainly adopt the scheme which transforms it into integral equations. During the process of transformation, several kinds of Green functions play important roles. Here Green functions are defined as follows

G2(t, s) =

(1−t)s,0≤s≤t≤1, t(1−s),0≤t≤s≤1.

Forn≥3, we define

Gn(t, s) =

Z t

0

Gn−1(v, s)dv.

Lemma 1.1.Gn(t, s)satisfies:

(i)Gn(t, s)≤G2(s, s), (t, s)∈[0.1]×[0,1],

n≥2, n∈N.

(ii) Let 0< θ≤1−θ≤1−τ, Jθ= [θ,1−θ],

fort∈Jθ, s∈[0,1], one has

G2(t, s)≥min{t,1−t}G2(s, s)≥θG2(s, s), (1.2)

Gn(t, s)≥θn−1G2(s, s), t∈Jθ, n≥2, n∈N. (1.3)

Proof At first, we prove the conclusion (i) of Lemma 1.1 by induction.

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Clearly,G2(t, s)≤G2(s, s).

Assuming that whenn=k,Gk(t, s)≤G2(s, s).

Thenn=k+ 1, for (t, s)∈[0.1]×[0,1]

Gk+1(t, s) = Z t

0

Gk(v, s)dv,

≤ Z 1

0

G2(s, s)dv,

= G2(s, s).

Therefore the conclusion (i) of Lemma 1.1 holds.

For the conclusion (ii) of Lemma 1.1, the relation formula (1.2) is clear. We prove the relation formula (1.3) in the following.

Fort∈Jθ, by (1.2) we haveG2(t, s)≥θG2(s, s).

Assuming when n=k,Gk(t, s)≥θk−1G2(s, s).

Then when n=k+ 1,t∈Jθ

Gk+1(t, s) = Z t

0

Gk(v, s)dv,

≥ Z t

0

θk−1G2(s, s)dv,

= tθk−1G2(s, s), ≥ θkG2(s, s).

Therefor (1.3) holds.

Let

E={u∈C[−τ,1] :u(t)≥0, f or t∈J; u(t) = u0(t) =· · ·=u(n−3)(t) =u(n−2)(t) = 0,

f or t∈[−τ,0]; u(n−2)(1) = (n1)!au(η)}.

With the norm k · k given by||u|| = sup{|u(t)|: −τ ≤

t ≤ 1}, then (E, k · k) is a Banach space. It is obvious thatk · k=k · k[0,1] for u∈E.

Define a cone K∈E by

K={u∈E:u(t)≥0, f ort∈[0,1]; min t∈Jθ

u(t)≥γ||u||},

whereγ=θn1+−1a(1aηnn−−11).

II. SOME PRELIMINARIES

For convenience of the reader, in the section, we also present some definitions and some lemmas.

Definition 2.1. LetX be a real Banach space andK∈X

be a closed, convex set. K is a cone if only if the following conditions are satisfied

(i) λu∈K,if λ >0 andu∈K.

(ii) if u∈K and−u∈K,thenu= 0.

Definition 2.2. u(t) is the positive solution of BVP(1.2) if and only if it satisfies the following conditions:

(i)u⊂C[−τ,1]∩Cn;u(t)>0, t∈(0,1).

(ii) Whent∈[−τ,0], u(t) =u0(t) =· · ·=u(n−3)(t) =

u(n−2)(t) = 0, andu(1) = (n1)!au(η)(0< η <1).

(iii)u(n)(t) =−λp(s)f(t, u(t−τ), v(t)),∀t∈(0,1).

If u(t) is the solution of BVP (1.1), then u(t) can be represented as

u(t) =

  

 

0,−τ≤t≤0. λR1

0 Gn(t, s)p(s)f(s, u, v)ds+

aλtn−1

1−aηn−1

R1

0 Gn(η, s)p(s)f(s, u, v)ds,0< t <1.

We define the operatorΦ :C[−τ,1]→C[−τ,1]by

Φu(t) =

  

 

0,−τ≤t≤0.

λR01Gn(t, s)p(s)f(s, u, v)ds+ aλtn−1

1−aηn−1

R1

0 Gn(η, s)p(s)f(s, u, v)ds,0< t <1.

Based on the above, we derive the following lemmas.

Lemma 2.1. The fixed-point of the mapΦis the solution of equation (1.1).

ProofIt’s easy to get

Φu(t) = Φ0u(t) = · · · = Φ(n−3)u(t) = Φ(n−2)u(t) =

0,−τ ≤t≤0,

Φ(n−2)u(1) = (n1)!aΦu(η).

We prove by reduction that Φ(n)u(t) =λp(t)f(t, u, v)

also hold.

Forn= 2, calculate easilyΦ00u(t) =λp(t)f(t, u, v).

Assuming that whenn=k,Φ(k)u(t) =λp(t)f(t, u, v).

Thenn=k+ 1, from

Φu(t) = λ Z 1

0

Gk+1(t, s)p(s)f(s, u, v)ds

+ aλt

k 1−aηk

Z 1

0

Gk+1(η, s)p(s)f(s, u, v)ds,

= λ Z 1

0 Z t

0

Gk(x, s)dx

p(s)f(s, u, v)ds

+ aλt

k 1−aηk

Z 1

0

Gk+1(η, s)p(s)f(s, u, v)ds.

one has that

Φ0u(t) =λR1

0 Gk(t, s)p(s)f(s, u, v)ds

+akλt1k−k1 R1

0 Gk+1(η, s)p(s)f(s, u, v)ds,

Φ(k+1)u(t) = (Φ0u(t))(k)=−λp(t)f(t, u, v).

Therefore the fixed point ofΦis the solution of the equation (1.1). The proof is complete.

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Lemma 2.2. Φ : K → K is a completely continuous operator.

Proof Clearly, we have ||Φu|| = ||Φu||[0,1],Φu(t) ≥

0,∀u(t)∈K, and

||Φu|| ≤ λ Z 1

0

G2(s, s)p(s)f(s, u, v)ds

+ aλ

1−aηn−1 Z 1

0

G2(s, s)p(s)f(s, u, v)ds,

= λ(1 +a−aη n−1)

1−aηn−1 Z 1

0

G2(s, s)p(s)f(s, u, v)ds.

for t∈Jθ, we have

Φu(t) ≥ λ Z 1

0

Gn(t, s)p(s)f(s, u, v)ds

≥ λθn−1 Z 1

0

G2(s, s)p(s)f(s, u, v)ds,

= θ

n−1(1n−1)

1 +a−aηn−1 ||Φu||[0,1]≥γ||Φu||.

Then Φ :K →K. Because Φ is a sequential compact set, we can conclude thatΦis a completely continuous operator by Arzela-Ascoli Theorem.

Lemma 2.3 [1] . LetX be a Banach space,Ka conic in

X,Ω1,Ω2two open subsets inX, and0∈Ω1⊂Ω1⊂Ω2. If

Φ :K∩(Ω2\Ω1)→K is a completely continuous operator

and satisfies

(i) ||Φu|| ≤ ||u||, u∈K∩∂Ω1 and||Φu|| ≥ ||u||, u ∈

K∩∂Ω2, or

(ii) ||Φu|| ≤ ||u||, u∈K∩∂Ω2 and||Φu|| ≥ ||u||, u∈

K∩∂Ω1,

thenΩhas a fixed point in K∩(Ω2\Ω1).

Let α, β, ϕ and φ be non-negative continuous concave functional on K. Then for positive real numbers b, c, dand

m, we define the following convex sets:

P(β, m) ={x∈K|β(x)< m},

P(β, α, b, m) ={x∈K|b≤α(x), β(x)≤m},

P(β, ϕ, α, b, d, m) = {x ∈ K|b ≤ α(x), ϕ(x) ≤

d, β(x)≤m},and a closed set

R(β, φ, c, m) ={x∈K|c≤φ(x), β(x)≤m}.

Lemma 2.4 [4]. LetKbe a cone in a real Banach spaceX. Letβ andϕbe non-negative continuous convex functionals on K, α be a non-negative continuous concave functional onK, andφbe a non-negative continuous functional onK

satisfyingφ(λu)≤λφ(u)for0≤λ≤1, such that for some positive numbers M andm,

α(u)≤φ(u), kuk ≤M β(u), f or all u∈P(β, m).

SupposeΦ :P(β, m)−→P(β, m)is completely continuous and there exist positive numbersb, candmwithb > csuch that

(S1){u ∈ P(β, ϕ, α, b, d, m)|α(u) > b} 6= 0, and

α(Φu)> bfor u∈P(β, ϕ, α, b, d, m).

(S2)α(Φ(u))> bfor P(β, α, b, m)withϕ(Φ(u))> d.

(S3)0 ∈/ R(β, φ, c, m) and φ(Φ(u)) < c for u ∈

R(β, φ, b, m)withφ(Φ(u)) =c.

thenΦ has at least three fixed points u1,u2, u3∈P(β, m),

such that

β(ui)≤m, fori= 1,2,3; b < α(u1);

c < φ(u2),withα(u2)< b;

φ(u3)< c.

III. THE CASE OF NO LESS THAN ONE SOLUTION

Let

M0= lim

u→0

v→0

inf min t∈[−τ,1]

f(t, u, v)

u2+v2.

M∞= lim

u→∞

v→∞

inf min t∈[−τ,1]

f(t, u, v)

u2+v2.

M0= lim u→0

v→0

sup max t∈[−τ,1]

f(t, u, v)

u2+v2.

M∞= lim u→∞

v→∞

sup max t∈[−τ,1]

f(t, u, v)

u2+v2.

L1=λγθn−1 Z 1−θ

θ+τ

G2(s, s)p(s)(1 +k0s)ds.

L2=

1 +a−aηn−1 1−aηn−1

Z 1

0

G2(s, s)p(s)(1 +k1s)ds.

In the following, we discuss the existence of at least the positive solutions for all kinds of values and compositions of

M0, M∞, M0andM∞. In the theorem 3.1 and theorem 3.2,

we takeε >0, such that satisfy(M0−ε)>0,(M∞−ε)>0. Theorem 3.1If the conditions(H1)−(H5)and the

follow-ing conditions

0< M∞<+∞, (3.1)

0< M0<+∞, (3.2)

1 L1(M∞−ε)

≤λ≤ 1

L2(M0+ε)

, (3.3)

hold, then the equation (1.2) has at least one solution.

Proof By (3.2),(3.3), for a given ε > 0,∃r1 >0, when

0<√u2+v2r

1, f(t, u, v)≤(M0+ε) √

u2+v2. Let

Ω1={t∈[−τ,1] :|| p

u2+v2||< r1},

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for u, v∈K∩∂Ω1, we have

||Φu|| ≤ λ Z 1

0

Gn(s, s)f(s, u(s−τ), v)ds

+ λa

1−aηn−1 Z 1

0

Gn(s, s)f(s, u(s−τ), v)ds,

= λ(1 +a−aη n−1)

1−aηn−1 × Z 1

0

Gn(s, s)p(s)f(s, u(s−τ), v)ds,

≤ λ(M

0+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s) p

u2(sτ) +v2ds,

≤ λ(M

0+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s)[u(s−τ) +v]ds,

≤ λ(M

0+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s)u(s−τ)ds

+

Z 1

0

G2(s, s)p(s) Z s

0

k(t, s)u(t)dtds

,

≤ λ(M

0+ε)(1 +an−1)

1−aηn−1 × Z 1−τ

0

G2(s+τ, s+τ)p(s+τ)u(s)ds

+k1 Z 1

0

G2(s, s)p(s) Z s

0

u(t)dtds

,

≤ λ(M

0+ε)(1 +an−1)

1−aηn−1 × Z 1−τ

0

G2(s+τ, s+τ)p(s+τ)ds

+k1 Z 1

0

G2(s, s)p(s)sds

||u||,

≤ λ(M

0+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s)(1 +k1s)ds

||u||

= λ(M0+ε)L2||u|| ≤ ||u||.

For the same aboveε >0, from (3.1) and (3.3),∃R1> r,

when √u2+v2 R

1, f(t, u, v) > (M∞−ε)

u2+v2.

Since γ < 1−2τ, thenγ+τ <1−γ. Let

Ω2={t∈[−τ,1] :|| p

u2+v2||< R1},

for u, v∈K∩∂Ω2, we get

||Φu|| ≥ λsup t∈J

Z 1

0

Gn(t, s)p(s)f(s, u, v)ds,

≥ λ(M∞−ε) sup

t∈J

Z 1

0

Gn(t, s)P(s)pu2+v2ds,

≥ λ(M∞−ε) sup

t∈J

Z 1

0

Gn(t, s)P(s)u+v 2 ds,

= λ(M∞−ε) 2 supt∈J

Z 1

0

Gn(t, s)P(s)u(s−τ)ds

+

Z 1

0

Gn(t, s)p(s)

Z s 0

K(t, s)u(t)dtds

,

≥ λ(M∞−ε)

2 supt∈J

Z 1−τ

−τ

Gn(t, s+τ)p(s+τ)

u(s)ds+k0 Z 1

0

Gn(t, s)p(s

Z s 0

k0)u(t)dtds

,

≥ λ(M∞−ε)

2 supt∈J

Z 1−θ

θ

Gn(t, s+τ)p(s+τ)γ

||u||ds+k0 Z 1−θ

θ

Gn(t, s)p(s)sγ||u||dtds

,

≥ λγ(M∞−ε)

2 supt∈J

Z 1−θ+τ

θ+τ

Gn(t, s)p(s)||u||ds

+k0||u|| Z 1−θ

θ

Gn(t, s)p(s)sds

,

≥ (M∞−ε)λγθ

n−1

2 ×

Z 1−θ

θ+τ

G2(s, s)p(s)(1 +k0s)ds

||u||,

= λ(M∞−ε)L1≥ ||u||.

Therefore, by Lemma 2.3, Φ has a fixed point

u ∈ K ∩ (Ω2\Ω1), and u(t) is a positive solution of

equation (1.2), completing the proof of Theorem 3.1

Theorem 3.2 If the conditions (H1)− (H5) and the

following conditions

0< M0<+∞, (3.4)

0< M∞<+∞, (3.5)

1 L1(M0−ε)

≤λ≤ 1

L2(M∞+ε)

, (3.6)

hold, then the equation (1.2) has at least one solution.

Proof By (3.4) and (3.6), for a given ε > 0,∃r2 > 0,

when√u2+v2r

2, f(t, u, v)≥(M0−ε) √

u2+v2. Let

Ω1={t∈[−τ,1] :|| p

u2+v2||< r2},

foru, v ∈K∩∂Ω1, we have

||Φu|| ≥ λsup t∈J

Z 1

0

Gn(t, s)p(s)f(s, u, v)ds,

≥ λ(M0−ε) sup

t∈J

Z 1

0

Gn(t, s)p(s)

p

u2+v2ds,

≥ λ(M0−ε) sup

t∈J

Z 1

0

Gn(t, s)p(s) u+v

2 ds,

= λ(M0−ε) 2 supt∈J

Z 1

0

Gn(t, s)p(s)u(s−τ)ds

+

Z 1

0

Gn(t, s)p(s)

Z s 0

K(t, s)u(t)dtds

,

≥ λ(M0−ε)

2 supt∈J

Z 1−τ

−τ

Gn(t, s+τ)p(s+τ)

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u(s)ds+k0 Z 1

0

Gn(t, s)p(s

Z s 0

k0)u(t)dtds

,

≥ λ(M0−ε)

2 supt∈J

Z 1−θ

θ

Gn(t, s+τ)p(s+τ)

γ||u||ds+k0 Z 1−θ

θ

Gn(t, s)p(s)sγ||u||dtds

,

≥ λγ(M0−ε)

2 supt∈J

Z 1−θ+τ

θ+τ

Gn(t, s)p(s)||u||ds

+k0||u|| Z 1−θ

θ

Gn(t, s)p(s)sds

,

≥ (M0−ε)λγθ

n−1

2 ×

Z 1−θ

θ+τ

G2(s, s)p(s)(1 +k0s)ds

||u||,

= λ(M0−ε)L1≥ ||u||.

For the same aboveε >0, from (3.5) and (3.6), ∃R2>

r2, when √

u2+v2R

2, f(t, u, v)>(M∞+ε) √

u2+v2.

Let

Ω2={t∈[−τ,1] :|| p

u2+v2||< R2},

for u, v∈K∩∂Ω2, we get

||Φu|| ≤ λ Z 1

0

Gn(s, s)f(s, u(s−τ), v)ds

+ λa

1−aηn−1 Z 1

0

Gn(s, s)f(s, u(s−τ), v)ds,

= λ(1 +a−aη n−1)

1−aηn−1 × Z 1

0

Gn(s, s)p(s)f(s, u(s−τ), v)ds},

≤ λ(M

+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s) p

u2(sτ) +v2ds,

≤ λ(M

+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s)[u(s−τ) +v]ds,

≤ λ(M

+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s)u(s−τ)ds

+

Z 1

0

G2(s, s)p(s) Z s

0

k(t, s)u(t)dtds

,

≤ λ(M

+ε)(1 +an−1)

1−aηn−1 × Z 1−τ

0

G2(s+τ, s+τ)p(s+τ)u(s)ds

+ k1 Z 1

0

G2(s, s)p(s) Z s

0

u(t)dtds

,

≤ λ(M

+ε)(1 +an−1)

1−aηn−1 × Z 1−τ

0

G2(s+τ, s+τ)p(s+τ)ds

+ k1 Z 1

0

G2(s, s)p(s)sds

||u||,

≤ λ(M

+ε)(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s)(1 +k1s)ds

||u||

= λ(M∞+ε)L2||u|| ≤ ||u||..

Therefore, by Lemma 2.3, Φ has a fixed point

u ∈ K ∩ (Ω2\Ω1), and u(t) is a positive solution of

equation (1.2), completing the proof of Theorem 3.2.

Theorem 3.3 If the conditions(H1)−(H5) satisfy and

M∞=∞, M0= 0. Then there exists two positive numbers

λ1, λ2, when λ1 ≤ λ ≤ λ2 , BVP (1.2) has at least a

positive solution.

ProofSinceM∞=∞, we can choose a positive constant

M > 0 such that f(t, u, v) ≥ M = αR3(α > 0) for any √

u2+v2R

3, t∈J. Let

λ1=

αθn−1 Z 1

0

G2(s, s)p(s)ds −1

.

Ω1={t∈[−τ,1] :|| p

u2+v2|| ≥R3},

foru, v ∈K∩∂Ω1, λ≥λ1, we have

||Φu|| ≥ λsup t∈J

Z 1

0

G(t, s)f(s, u, v)ds

≥λMsup t∈J

Z 1

0

Gn(t, s)p(s)ds,

≥ λMsup t∈Jθ

Z 1

0

Gn(t, s)p(s)ds

≥λM θn−1 Z 1

0

G2(s, s)p(s)ds,

≥ λαR3θn−1 Z 1

0

G2(s, s)p(s)ds=

λ λ1

R3,

≥ kpu2+v2k ≥ kuk.

BecauseM0= 0, we choose a value small enough forε >0, so that

λ2=

λθn−1ε(1+a−aηn−1) 1−aηn−1

R1

0 G2(s, s)(1 +k1s)p(s)ds −1

> λ, and∃0 < r3 < R3, such thatf(t, u, v) ≤ε √

u2+v2

for any√u2+v2r 3. Let

Ω1={t∈[−τ,1] :|| p

u2+v2||< r3},

foru, v ∈K∩∂Ω, we have

||Φu|| ≤ λ Z 1

0

Gn(s, s)p(s)f(s, u, v)ds

+ λa

1−aηn−1 Z 1

0

Gn(s, s)p(s)f(s, u, v)ds,

≤ λε(1 +a−aη

n−1)

1−aηn−1

Z 1

0

Gn(s, s)p(s)

p

u2+v2)ds,

≤ λε(1 +a−aη

n−1)

1−aηn−1

Z 1

0

Gn(s, s)p(s)(u+v)ds,

= λε(1 +a−aη n−1)

1−aηn−1

Z 1

0

Gn(s, s)p(s)u(s−τ)ds

IAENG International Journal of Applied Mathematics, 47:2, IJAM_47_2_05

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+

Z 1

0

Gn(s, s)p(s)

Z s 0

K(t, s)u(t)dtds

,

≤ λε(1 +a−aη

n−1)

1−aηn−1 × Z 1−τ

−τ

Gn(s+τ, s+τ)p(s+τ)u(s)ds

+k1 Z 1

0

Gn(s, s)p(s)

Z s 0

u(t)dtds

,

≤ λθ

n−1ε(1 +an−1)

1−aηn−1 × Z 1

0

G2(s, s)(1 +k1s)p(s)ds||u||

≤ λ

λ2

||u|| ≤ ||u||.

Therefore, by Lemma 2.3,Φ has at least one fixed point

u∈K∩(Ω2\Ω1), andu(t)has at least one positive solution

of equation (1.2), completing the proof of Theorem 3.3.

Remark 3.1 If M0 = ∞, M∞ = 0, similarly we can

verify that BVP (1.2) has at least one positive solution.

IV. THE CASE OF NO LESS THAN THREE SOLUTIONS

In this section, by Lemma (2.4), we prove that BVP (1.1) has at least three solutions when f(t, u, v) satisfies some certain conditions. First, we define four the non-negative continuous concave functions in Kα, β, ϕ andφ

α(u) = min

θ≤t≤1−θ|u(t)|, β(u) = max0≤t≤1|u(t)|,

ϕ(u) =φ(u) = max

θ−τ≤t≤1|u(t)|. (4.1)

Set

(1) ω1(t),ω2(t)are two non-negative characteristic

func-tions andω1(t)∈C[0,1], ω2(t)∈C[θ+τ,1−θ].

(2) L3=1+a−aη

n−1

1−aηn−1 [

R1

0 G2(s, s)p(s)ω1(s)(1 +k1s)ds].

(3) N1=λL3(cm+c),

N2= 1

λγθn−1√k0R1−γ

γ+τ

sG2(s,s)p(s)ω2(s)ds

.

As we know, some researchers [27,28] had discussed BVPs with at least three solutions. In these papers, the relative conclusions were based on the assumption that

f(t, u(t)) be more than or less than a given constant. In fact, it’s very difficult to find such functions. In our paper, f(t, u, v) is assumed to be a function which satisfies the conditions f(t, u, v) ≤ N1ω1(u + v)

or f(t, u, v) ≥ N2ω2 √

uv. Meanwhile, we introduce two characteristic ω1, ω2. The conditions

f(t, u, v)≤N1ω1(u+v) or f(t, u, v)≥N2ω2 √

uvcan be easily satisfied for some equations when we choose suitable characteristic functions. The conclusion is described in Theorem 4.1. In section 5, we give example 2 to illustrate our conclusion.

Theorem 4.1 If the conditions (H1)−(H5) hold and

there exist positive numbers b, c, m with m > b > c > 0

such that the following conditions are satisfied

(i)f(t, u, v) ≤ N1ω1(t)(u+v),(t, u) ∈ [0,1]×[0, m],

whereN1≤λL2(cm+c),

(ii)f(t, u, v) ≥ N2ω2(t) √

uv,(t, u) ∈ [θ+τ,1−θ]×

[b,(θ+1)γ 2b],

whereN2≥[λγγ1 √

k0R 1−γ γ+τ G(s, s)

sds]−1.

Then BVP(1.2) has at least three solutions u1,u2, u3 ∈

P(β, m), such that

β(ui)≤m, fori= 1,2,3; b < α(u1);

c < φ(u2),withα(u2)< b;

φ(u3)< c.

Proof By Lemma 2.1, we can derive that Φ : K → K

is completely continuous. It is easy to verify that

φ(λu) = λφ(u) for 0 ≤ λ ≤ 1 and α(u) ≤ φ(u).

According to the definition of norm and (4.1), if taking

M ≥1, then we have that||u||=β(u)and||u|| ≤M β(u)

for all u ∈ P(β, m). Therefore if u ∈ P(β, m), then

β(u) =||u|| ≤m, in addition

max

t∈[0,1]|u(t−τ)| = t∈[max−τ,1−τ]|u(t)| = t∈max[0,1−τ]|u(t)| ≤

max t∈[0,1]

|u(t)| ≤m.

From the conditions(i)of theorem 4.1, we have

β(Φu) = max

t∈[0,1]|(Φu)(t)| ≤λ Z 1

0

Gn(s, s)p(s)f(s, u, v)ds

+ aλ

1−aηn−1 Z 1

0

Gn(s, s)p(s)f(s, u, v)ds,

≤ λN1(1 +a−aη

n−1)

1−aηn−1 × Z 1

0

Gn(s, s)p(s)ω1(s)(u+v)ds,

= λN1(1 +a−aη n−1)

1−aηn−1 × Z 1

0

Gn(s, s)p(s)ω1(s)u(s−τ)ds

+

Z 1

0

Gn(s, s)p(s)ω1(s) Z s

0

K(t, s)u(t)dtds

,

≤ λN1(1 +a−aη

n−1)

1−aηn−1 × Z 1

0

G2(s, s)p(s)ω1(s)(m+k1m Z s

0

dt)ds,

= λN1(1 +a−aη)m

1−aη ×

Z 1

0

(1 +k1s)G2(s, s)p(s)ω1(s)ds

= λN1mL2≤

mc

(m+c) < m.

SoΦ :P(β, m)→P(β, m).

If one choosing

u0(t) =−4γb(t−1+2θ)2+ (1+θ)2b

γ , t∈[0,1],

we have thatϕ(u0) =(1+θ)

2b

γ andα(u0) = min

t∈[θ,1−θ]

|u0(t)|=u0(θ) = 4γbθ > b, then

u0∈P(β, ϕ, α, b, (1+θ)2b

γ , m).

IAENG International Journal of Applied Mathematics, 47:2, IJAM_47_2_05

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Therefore{u∈P(β, ϕ, α, b,(1+γθ)2b, m)|α(u)> b} 6= 0. On the other hand, if u∈P(β, ϕ, α, b,(1+γθ)2b, m), then

min t∈[θ+τ,1−θ]|

u(t−τ)|= min t∈[θ,1−θ−τ]|

u(t)|

≥ min

t∈[θ,1−θ]

|u(t)| ≥b

,

min

t∈[θ+τ,1−θ]|u(t)| ≥t∈min[θ,1−θ]|u(t)| ≥b.

From the conditions(ii)of theorem 4.1 and Lemma 1.1, we have

α(Φu) = min t∈[θ,1−θ]

|(Φu)(t)| ≥γ||(Φu)(t)||,

≥ λγsup t∈Jθ

Z 1

0

Gn(t, s)f(s, u, v)ds

≥ λγN2sup

t∈Jθ Z 1

0

Gn(t, s)p(s)ω2(s) √

uvds,

= λγN2sup

t∈Jθ Z 1

0

Gn(t, s))p(s)ω2(s)

s

u(t−τ)

Z s

0

k(t, s)u(t)dtds,

≥ λγN2sup

t∈Jθ Z 1−θ

θ+τ

Gn(t, s)p(s)ω2(s)

s

u(t−τ)

Z s 0

k(t, s)u(t)dtds,

≥ [λθn−1γN2 p

k0 Z 1−θ

θ+τ

G2(s, s)

p(s)ω2(s) √

sds]b≥b.

So the condition(S1)of Lemma 2.4 is satisfied.

For all u ∈ P(β, α, b, m) with ϕ(Φu) > b(1+γθ)2, then one has

α(Φu)≥γϕ(Φu)> γb(1+γθ)2 > b.

So the condition(S2)of Lemma 2.4 is also satisfied.

Finally, we verify the condition(S3)of Lemma 2.4 holds.

Obviously, 0∈/ R(β, φ, c, m). As if0∈R(β, φ, c, m), then it is conflicts wit φ(0) = 0 < c. For all u∈ R(β, φ, c, m)

withφ(u) =c, then

max t∈[0,1]|

u(t)| ≤m,

max

t∈[θ,1]|u(t−τ)|=t∈[θmax−τ,1−τ]|u(t)| ≤t∈max[θ−τ,1]|u(t)|=c.

From the conditions (i)of theorem 4.1, we have

φ(Φu) = max

t∈[θ−τ,1]|(Φu)(t)| ≤tmax∈[0,1]|(Φu)(t)|,

≤ λ

Z 1

0

Gn(s, s)p(s)f(s, u, v)ds

+ aλ

1−aηn−1 Z 1

0

Gn(s, s)p(s)f(s, u, v)ds,

≤ λN1(1 +a−aη

n−1)

1−aηn−1 × Z 1

0

Gn(s, s)p(s)(u+v)ds,

= λN1(1 +a−aη n−1)

1−aηn−1 [ Z 1

0

Gn(s, s)p(s)u(s−τ)ds

+

Z 1

0

Gn(s, s)p(s)

Z s 0

K(t, s)u(t)dtds],

= λN1(1 +a−aη n−1)

1−aηn−1

Z θ

0

Gn(s, s)p(s)u(s−τ)ds

+

Z 1

θ

Gn(s, s)p(s)u(s−τ)ds

+

Z θ−τ 0

Gn(s, s)p(s)

Z s 0

K(t, s)u(t)dtds

+

Z 1

θ−τ

Gn(s, s)p(s)

Z s

0

K(t, s)u(t)dtds

,

≤ λN1(1 +a−aη

n−1)

1−aηn−1

m Z θ

0

Gn(s, s)p(s)ds

+c Z 1

θ

Gn(s, s)p(s)ds

+mk1 Z θ−τ

0

Gn(s, s)p(s)sds

+k1c Z 1

θ−τ

Gn(s, s)p(s)sds

,

≤ λN1(m+c)(1 +a−aη

n−1)

1−aηn−1 Z 1

0

G2(s, s)p(s)(1 +k1s)ds

= λN1(m+c)L2≤c.

Therefore, by Lemma 2.4, Φ has at least three fixed pointsu1,u2, u3∈P(β, m), thenu1,u2, u3are three positive

solution of equation (1.2), andu1,u2, u3 satisfy that

β(ui)≤m, fori= 1,2,3; b < α(u1);

c < φ(u2),withα(u2)< b;

V. EXAMPLE

Consider the equation

  

 

−u(5)(t) =1000

t

t2+ 1[u2(t−16)+v

2(t)][1+u(t1 6)+v(t)]

2+u(t−1 6)+v(t)

,

0< t <1, u(t) = 0,−τ≤t≤0, (5.1) u(1) = 4!1

2u( 1 2).

Wheref(t, u, v) =√t2+ 1[u2(t−16)+v

2(t)][1+u(t1 6)+v(t)]

2+u(t−1 6)+v(t)

;

v(t) =R1

0(t+s+ 1)u(s)ds, k(s, t) =t+s+ 1, then

k1= 3;p(t) =1t, t= 0is its singularity. Here we have

M∞ = ∞, M0 = 0.If we choose M = 100, θ = 18, λ =

1000, η= 12, a= 12, α = 10011. Then when √u2+v2 11,

f(t, u, v) ≥ M. We can calculate that λ1 = 2252825 . If we

chooseε= 0.01,Calculations show thatλ2=1267960047 .

From Theorem 3.3, we have that if 2252825 = λ1 ≤ λ ≤

λ2 = 1267960047 , the problem (5.1) has at least one positive

solution.

Example 2 Consider the boundary value problem

  

 

−u(4)(t) =103(124mint)(2+(1−tt))

q

u2(t1

4) +v2(t) +u(t− 1 4)v(t)

t∈(0,1), u(t) = 0, −τ ≤t≤0, (5.2) u(1) = 3!1

2u( 1 2).

where λ = 1 3;τ =

1

4;k(t, s) = 2ts + 1, v(t) = R1

0 k(t, s)u(s)ds,(t, s) ∈ [0,1] × [0,1];f(t, u, v) =

IAENG International Journal of Applied Mathematics, 47:2, IJAM_47_2_05

(8)

1024min(1−t)

2+t

q

u2(t1

4) +v2(t) +u(t− 1

4)v(t);p(t) = 1

1−t, t = 1 is its singularity; u(t) satisfies the definition

of (4.1). If setting m = 2, c = 1, θ = 1

4, such that

max

0≤t≤1|u(t)| ≤m,φ(u) =θ−maxτ≤t≤1|u(t)|> c, we can easily

derive that

L2=

11 6 , N1=

6

11, N2= 60857.88.

Obviously, we have that

f(t, u, v)≤1

2(u+v)< N1(u+v), t∈[0,1],

f(t, u, v)≥10 6√3uv

3 > N2

uv, t∈[1 2,

3 4].

From Theorem 4.1, the problem (5.2) has at least three positive solutions.

ACKNOWLEDGMENT

The authors would like to thank reviewers for their sug-gestions which help us to improve our work.

REFERENCES

[1] D.Guo, V.Lakshmikantham, ”Nonlinear Problems in Abstract Cones,”

Academic Press, 1988.

[2] J.Henderson, ”Boundary Value Problems for Functional Equations,”

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[3] A. Alibeigloo, H. Jafarian, ”Three-Dimensional Static and Free Vibra-tion Analysis of Carbon Nano Tube Reinforced Composite Cylindrical Shell Using Differential Quadrature Method,”International Journal of Applied Mechanics, DOI: 10.1142/S1758825116500332, 2016. [4] M. M. KIPNIS, I. S. LEVITSKAYA, ”STABILITY OF DELAY

D-IFFERENCE AND DIFFERENTIAL EQUATIONS: SIMILARITIES AND DISTINCTIONS,”Difference Equations, Special Functions and Orthogonal Polynomials, 2007, 315-324.

[5] R.I.Avery and A.C. Peterson, ”Three positive fixed points of nonlinear operators on ordered Banach space,”Comput.Math.Appl., 42(2001)313-322.

[6] J.W.Lee and D.O’Regan, ”Existence results for differential delay equa-tions,”J. Differ.Eq., 102(1993)342-359.

[7] J.K.Hale, W.Huang, ”Global geometry of stable regions for two delay differential equations,”J.Math.Anal.Appl., 178(1993)344-362. [8] R.Y. Ma, ”Existence theorem for second order boundary value problem,”

J. Math.Anal. Appl., 212(1997)430-442.

[9] J.Henderson, H.Y.Wang, ”Positive solutions for nonlinear eigenvalue problems,”J.Math.Anal.Appl., 208(1997)252-259.

[10] J.Henderson, H.B. Thompson, ”Existence and multiple solutions for second order boundary value problems,”J.Differ.Eqs., 166(2000)443-454.

[11] D.Q.Jiang, J.Y.Wang, ”On boundary value problems for singular second-order functional differential equations,”J.Comput.Appl. Math., 116(2000)231-241.

[12] D.Q.Jiang, ”Multiple positive solutions for boundary value prob-lems of second-order delay differential equations,” Appl.Math.Lett., 15(2002)575-583.

[13] Z.G.Zhang, J.Y.Wang, ”Positive solutions to a second order three-point boundary value problem,”J.Math. Anal.Appl., 285(2003)273-294 . [14] D.Y.Bai, Y.T.Xu, ”Existence of positive solutions for boundary-value

problems of second-order delay differential equations,”Appl.Math.Lett., 18(2005)621-630.

[15] D.Bai,Y.Xu, ”Positive solutions and eigenvalue regions of two-delay singular systems with a twin parameter,” Nonlinear.Anal., 66(2007)2547-2564.

[16] W.B.Wang, J.H.Shen, ”Positive solutions to a multi-point boundary value problem with delay,” Applied Mathematics and Computation., 188(2007)96-102.

[17] B.Du, X.P.Hu, W.G.Ge, ”Positive solutions to a type of multi-point boundary value problem with delay and one-dimensional p-Laplacian,”

Applied Mathematics and Computation., 208(2009)501-510.

[18] Z.M.He, J.H.Shen, ”Existence of periodic solutions for p-Laplacian neutral Rayleigh equation,”Advance in Difference Equations., http://www.advancesindifferenceequations.com/content/2014/1/67. [19] Y.Lee, ”Multiplicity of Positive solutions for multiparamter semiliear

elliptic systems,”J. Differ.Eq., 174(2007)420-441.

[20] Z.M.He, X.M.He, ”Periodic boundary value problems for first order impulsive integro differential equations of mixed type,”

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[21] G.P.Chen, J.H.Shen, W.B.Wang, ”Solvability of three point boundary value problems for second order integro-differential equations of mixed type,”Journal of integral equations and applications, 21(1)(2009)21-37.

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[23] J.R.Graef, Bo Yang, ”Positive solutions to a multi-point higher order boundary-value problem,”J.Math.Anal.Appl.316(2006)409-421. [24] J.H.Shen, J.Dong, ”Existence of positive solutions to BVPS of higher

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[25] D.CHALISHAJAR, K.KARJHIKEYAN, ”Existence and uniqueness results for boundary value problems of higher order fractional intergro-differential equations involving grownwall’s inequality in banach s-paces,”Acta Mathematic Scientia, 33(2013)758-772.

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IAENG International Journal of Applied Mathematics, 47:2, IJAM_47_2_05

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