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Volume 2010, Article ID 878131,13pages doi:10.1155/2010/878131

Research Article

Existence and Multiplicity of Positive

Solutions of a Boundary-Value Problem for

Sixth-Order ODE with Three Parameters

Liyuan Zhang and Yukun An

Nanjing University of Aeronautics and Astronautics, 29 Yudao st., Nanjing 210016, China

Correspondence should be addressed to Liyuan Zhang,[email protected]

Received 13 May 2010; Accepted 14 August 2010

Academic Editor: Kanishka Perera

Copyrightq2010 L. Zhang and Y. An. 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 and multiplicity of positive solutions of the following boundary-value problem:−u6γu4βuαuft, u, 0< t <1,u0 u1 u0 u1 u40 u41

0, wheref:0,RRis continuous,α,β, andγRsatisfy some suitable assumptions.

1. Introduction

The following boundary-value problem:

u6Au4BuCufx, u 0, 0< x < L,

u0 uL u0 uL u40 u4L 0,

1.1

where A, B, andCare some given real constants and fx, u is a continuous function on

R2, is motivated by the study for stationary solutions of the sixth-order parabolic differential

equations

∂u ∂t

6u

∂x6 A

4u

∂x4 B

2u

∂x2 fx, u. 1.2

(2)

transition between the liquid and solid state. Whenfx, u uu3,it was studied by Gardner

and Jones1as well as by Caginalp and Fife2.

Iff is an even 2L-periodic function with respect to xand odd with respect tou, in order to get the 2L-stationary spatial periodic solutions of1.2, one turns to study the two points boundary-value problem1.1. The 2L-periodic extensionuof the odd extension of the solutionuof problems1.1to the interval−L, Lyields 2L-spatial periodic solutions of1.2 Gyulov et al. 3have studied the existence and multiplicity of nontrivial solutions of BVP1.1. They gained the following results.

Theorem 1.1. Letfx, u:R2 Rbe a continuous function andFx, u u

0 fx, sds. Suppose

the following assumptions are held:

H1Fx, u/u2 → ∞as|u| → ∞, uniformly with respect to x in bounded intervals,

H20≤Fx, u ou2asu → 0, uniformly with respect toxin bounded intervals,

then problem1.1has at least two nontrivial solutions provided that there exists a natural number nsuch thatPnπ/L<0, wherePξ ξ642Cis the symbol of the linear dierential

operatorLuu6Au4BuCu.

At the same time, in investigating such spatial patterns, some other high-order parabolic differential equations appear, such as the extended Fisher-Kolmogorov EFK equation

∂u ∂tζ

4u

∂x4

2u

∂x2 uu

3, ζ >0, 1.3

proposed by Coullet, Elphick, and Repaux in 1987 as well as by Dee and Van Saarlos in 1988 and Swift-HohenbergSHequation

∂u ∂t ρu

1

2u

∂x2

2

uu3, ρ >0, 1.4

proposed in 1977.

In much the same way, the existence of spatial periodic solutions of both the EFK equation and the SH equation was studied by Peletier and Troy4, Peletier and Rottsch¨afer 5, Tersian and Chaparova 6, and other authors. More precisely, in those papers, the authors studied the following fourth-order boundary-value problem:

u4AuBufx, u 0, 0< x < L,

u0 uL u0 uL 0. 1.5

The methods used in those papers are variational method and linking theorems.

(3)

to obtain Green’s function and then used the fixed point theorem of cone extension or compression to study the problem.

The purpose of this paper is using the idea of 7 to investigate BVP for sixth-order equations. We will discuss the existence and multiplicity of positive solutions of the boundary-value problem

u6γu4βuαuft, u, 0< t <1, 1.6

u0 u1 u0 u1 u40 u41 0, 1.7

and then we assume the following conditions throughout: H1f:0,1×0,∞→0,∞is continuous, H2α, β, andγRsatisfy

γ <3π2, 3π4−2γπ2−β >0,

α π6

β π4

γ π2 <1,

18αβγ−β2γ24αγ327α2−4β3≤0.

1.8

Note. The set ofα, β,andγwhich satisfiesH2is nonempty. For instance, ifγ π2, β0,

thenH2holds forα: −4π2/27< α <0.

To be convenient, we introduce the following notations:

6−γπ4−βπ2−α,

f

0lim infu→0 tmin∈0,1

ft, u

u

, flim sup

u→ ∞ tmax∈0,1

ft, u

u

,

f

∞lim infu→ ∞ tmin∈0,1

ft, u

u

, f0lim sup u→0

max t∈0,1

ft, u

u

.

1.9

2. Preliminaries

Lemma 2.1see8. Set the cubic equation with one variable as follows:

ax3bx2cxd0, a, b, c, dR, a /0. 2.1

Let

Ab2−3ac, Bbc−9ad, Cc2−3bd, Δ B2−4AC, 2.2

one has the following:

1Equation2.1has a triple root ifAB0,

2Equation2.1has a real root and two mutually conjugate imaginary roots ifΔ B2

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3Equation2.1has three real roots, two of which are reroots ifΔ B24AC0,

4Equation2.1has three unequal real roots ifΔ B24AC <0.

Lemma 2.2. Letλ1, λ2, andλ3be the roots of the polynomialPλ λ3γλ2−βλα. Suppose

that conditionH2holds, thenλ1, λ2, and λ3are real and greater thanπ2.

Proof. There are23β, Bβγ9α, and Cβ23αγ in the equationPλ 0. Since

conditionH2holds, we have

Δ B2−4AC18αβγ−β2γ24αγ327α2−4β3≤0. 2.3

Therefore, the equation has three real roots in reply toLemma 2.1. By Vieta theorem, we have

λ1λ2λ3−α,

λ1λ2λ3 −γ,

λ1λ2λ1λ3λ2λ3−β.

2.4

Thereforeα/π6β/π4γ/π2 <1,γ <2and 3π42γπ2β >0 hold if and only if

λ1π2

λ2π2

λ3π2

>0,

λ1π2

λ2π2

λ3π2

>0,

λ1π2

λ2π2

λ1π2

λ3π2

λ2π2

λ3π2

>0.

2.5

Then, we only prove that the system of inequalities2.5holds if and only ifλ1, λ2, andλ3

are all greater than−π2.

In fact, the sufficiency is obvious, we just prove the necessity. Assume thatλ1, λ2, λ3

are less than−π2. By the first inequality of2.5, there exist two roots which are less thanπ2

and one which is greater than−π2. Without loss of generality, we assume thatλ2<π2, λ3<π2, then we haveλ

1>π2. Multiplying the second inequality of2.5byλ2π2, one gets

λ1π2

λ2π2

λ2π2

2

λ2π2

λ3π2

<0. 2.6

Compare with the third inequality of2.5, we have

λ2π2

2

1π2

λ3π2

<0, 2.7

(5)

LetGit, s i1,2,3be Green’s function of the linear boundary-value problem

ut λiut 0, u0 u1 0. 2.8

Lemma 2.3see7. Git, si1,2,3has the following properties:

iGit, s>0, for allt, s∈0,1,

iiGit, s≤CiGis, s, for allt, s∈0,1, whereCi>0is a constant, iiiGit, s≥δiGit, tGis, s, for allt, s∈0,1, whereδi>0is a constant.

One denotes the following:

Mimax

0≤s≤1Gis, s, mi1/4min≤s≤3/4Gis, s i1,2,3,

C12 1

0

G1δ, δG2δ, δdδ, C23 1

0

G2s, sG3s, sds,

2.9

thenMi, mi, C12, C23 >0. Let · be the maximum norm ofC0,1, and letC0,1be the cone of

all nonnegative functions inC0,1.

LethC0,1, then one considers linear boundary-value problem (LBVP) as follows:

u6−γu4βuαuht, t∈0,1, 2.10

with the boundary condition1.7. Since

u6−γu4βuαu

d2

dt2 λ1

d2

dt2 λ2

d2

dt2 λ3

u, 2.11

the solution of LBVP2.101.7can be expressed by

ut 1

0

G1t, δG2δ, τG3τ, shsds dτ dδ. 2.12

Lemma 2.4. LethC0,1, then the solution of LBVP2.101.7satisfies

utδ1δ2δ3C12C23

C1C2C3M1M2G1t, t u . 2.13

Proof. From2.12andiiofLemma 2.3, it is easy to see that

utC1C2C3M1M2 1

0

(6)

and, therefore,

uC1C2C3M1M2 1

0

G3s, shsds, 2.15

that is,

1

0

G3s, shsds≥ u

C1C2C3M1M2. 2.16

UsingiiiofLemma 2.3, we have

ut 1

0

G1t, δG2δ, τG3τ, shsds dτ dδ

δ1δ2δ3C12C23G1t, t 1

0

G3s, shsds

δ1δ2δ3C12C23G1t, t

C1C2C3M1M2 u .

2.17

The proof is completed.

We now define a mappingA:C0,1 → C0,1by

Aut 1

0

G1t, δG2δ, τG3τ, sfs, usds dτ dδ. 2.18

It is clear thatA:C0,1 → C0,1is completely continuous. ByLemma 2.4, the positive solution of BVP1.6-1.7is equivalent to nontrivial fixed point ofA. We will find the nonzero fixed point of Aby using the fixed point index theory in cones. For this, one chooses the subconeKofC0,1by

K

uC0,1|utσ u ,t

1 4,

3 4

, 2.19

whereσδ1δ2δ3C12C23m1/C1C2C3M1M2, we have the following.

Lemma 2.5. HavingAKK,A:KKis completely continuous.

Proof. For uK, let ht ft, ut, then Autis the solution of LBVP2.10–1.7. By Lemma 2.4, one has

Autδ1δ2δ3C12C23

C1C2C3M1M2G1t, t Auσ Au ,t

1 4,

3 4

, 2.20

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The main results of this paper are based on the theory of fixed point index in cones9. LetEbe a Banach space andKEbe a closed convex cone inE. Assume thatΩis a bounded open subset ofEwith boundary ∂Ω, andK∩Ω/∅. LetA : K∩Ω → K be a completely continuous mapping. IfAu /ufor everyuK∂Ω, then the fixed point indexiA, K∩Ω, K is well defined. We have that ifiA, K∩Ω, K/0, thenAhas a fixed point inK∂Ω.

LetKr {uK| u < r}and∂Kr {uK| u r}for everyr >0.

Lemma 2.6see9. LetA:KKbe a completely continuous mapping. IfμAu /ufor every

u∂Kr and0< μ≤1, theniA, Kr, K 1.

Lemma 2.7 see9. LetA : KK be a completely continuous mapping. Suppose that the

following two conditions are satisfied:

iinfu∂Kr Au >0,

iiμAu /ufor everyu∂Kr andμ≥1,

theniA, Kr, K 0.

Lemma 2.8see9. LetX be a Banach space, and letKX be a cone inX. For p >0, define

Kp {uK| u < p}. Assume thatA:KpKis a completely continuous mapping such that Au /ufor everyu∂Kp{uK| u p}.

iIf uAu for everyu∂Kp, theniA, Kp, K 0. iiIf uAu for everyu∂Kp, theniA, Kp, K 1.

3. Existence

We are now going to state our existence results.

Theorem 3.1. Assume that (H1) and (H2) hold, then in each of the following case:

if0 < L,f> L, iif

0 > L,f< L,

the BVP1.6-1.7has at least one positive solution.

Proof. To prove Theorem 3.1, we just show that the mapping A defined by 2.18 has a nonzero fixed point in the cases, respectively.

Casei: sincef0< L, by the definition off0, we may chooseε >0 andω >0,so that

ft, u≤L−εu, 0≤t≤1, 0≤uω. 3.1

Letr ∈ 0, ω, we now prove thatμAu /ufor everyu∂Kr and 0 < μ ≤1. In fact, if there existu0 ∈ ∂Kr and 0 < μ0 ≤1 such thatμ0Au0 u0, then, by definition ofA,u0tsatisfies

differential equation the following:

(8)

and boundary condition1.7. Multiplying3.2by sinπtand integrating on0,1, then using integration by parts in the left side, we have

L

1

0

u0tsinπt dtμ0 1

0

ft, u0tsinπt dt≤L−ε 1

0

u0tsinπt dt. 3.3

ByLemma 2.4,ut ≥δ1δ2δ3C12C23/C1C2C3M1M2G1t, t u , and then

1

0u0tsinπt dt >

0. We see that L ≤ L−ε, which is a contradiction. Hence, Asatisfies the hypotheses of Lemma 2.6, inKr. ByLemma 2.6we have

iA, Kr, K 1. 3.4

On the other hand, sincef

> L, there existε∈0, LandH >0 such that

ft, u≥Lεu, 0≤t≤1, u≥H. 3.5

LetCmax0≤t≤1,0≤uH|ft, u−Lεu|1, then it is clear that

ft, u≥LεuC, 0≤t≤1, u≥0. 3.6

ChooseR > R0 max{H/σ, ω}. Letu∂KR. Sinceusσ u > H, for alls∈1/4,3/4, from3.5we see that

ft, u≥Lεus≥Lεσ u ,s

1 4,

3 4

. 3.7

ByLemma 2.5, we have

Au

1 2

1

0

G1

1 2, δ

G2δ, τG3τ, sfs, usds dτ dδ

δ1δ2δ3C12C23m1 3/4

1/4

G3s, sfs, usds

≥ 1

2δ1δ2δ3C12C23m1m3Lεσ u .

3.8

Therefore,

AuAu

1 2

≥ 1

(9)

from which we see that infu∂KR Au >0, namely the hypothesesiofLemma 2.7holds.

Next, we show that ifRis large enough, thenμAu /ufor anyu∂KR andμ ≥1. In fact, if there existu0∈∂KRandμ0≥1 such thatμ0Au0u0, thenu0tsatisfies3.2and boundary

condition1.7. Multiplying3.2by sinπtand integrating, from3.6we have

L

1

0

u0tsinπt dtμ0 1

0

ft, u0tsinπt dt≥Lε 1

0

u0tsinπt dt−2C

π . 3.10

Consequently, we obtain that

1

0

u0tsinπt dt≤ 2C

πε. 3.11

ByLemma 2.4,

1

0

u0tsinπt dtδ1δ2δ3C12C23

C1C2C3M1M2 u0 1

0

G1t, tsinπt dt, 3.12

from which and from3.11we get that

u0 ≤ 2CC1C2C3M1M2

δ1δ2δ3C12C23πε 1

0

G1t, tsinπt dt

1

:R. 3.13

Let R > max{R, R0}, then for any u∂KR andμ ≥ 1,μAu /u. Hence, hypothesis ii of Lemma 2.7also holds. ByLemma 2.7, we have

iA, KR, K 0. 3.14

Now, by the additivity of fixed point index, combine3.4and3.14to conclude that

iA, KR\Kr, K

iA, KR, KiA, Kr, K −1. 3.15

Therefore,Ahas a fixed point inKR\Kr, which is the positive solution of BVP1.6-1.7. Caseii: sincef

0 > L, there existε >0 andr0>0 such that

ft, u≥Lεu, 0≤t≤1, 0≤ur0. 3.16

Letr∈0, r0, then for everyu∂Kr, through the argument used in3.9, we have

AuAu

1 2

≥ 1

(10)

Hence, infu∂Kr Au >0. Next, we show thatμAu /ufor anyu∂Kr andμ≥1. In fact, if

there existu0∈∂Kr andμ0 ≥1 such thatμ0Au0 u0, thenu0tsatisfies3.2and boundary

1.7. From3.2and3.16, it follows that

L

1

0

u0tsinπt dtμ0 1

0

ft, u0tsinπt dt≥Lε 1

0

u0tsinπt dt. 3.18

Since 01u0tsinπt dt > 0, we see that L ≥ Lε, which is a contradiction. Hence, by

Lemma 2.7, we have

iA, Kr, K 0. 3.19

On the other hand, sincef< L, there existε∈0, LandH >0 such that

ft, u≤L−εu, 0≤t≤1, u≥H. 3.20

SetCmax0≤t≤1,0≤uH|ft, u−L−εu|1, we obviously have

ft, u≤L−εuC, 0≤t≤1, u≥0. 3.21

If there existu0 ∈Kand 0< μ0 ≤1 such thatμ0Au0 u0, then3.2is valid. From3.2and

3.21, it follows that

L

1

0

u0tsinπt dtμ0 1

0

ft, u0tsinπt dt≤L−ε 1

0

u0tsinπt dt2C

π . 3.22

By the proof of3.13, we see that u0 ≤ R. LetR >max{R, r0}, then for anyu∂KRand 0< μ≤1,μAu /u. Therefore, byLemma 2.6, we have

iA, KR, K 1. 3.23

From3.19and3.23, it follows that

iA, KR\Kr, K

iA, KR, KiA, Kr, K 1. 3.24

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FromTheorem 3.1, we immediately obtain the following.

Corollary 3.2. Assume thatH1andH2hold, then in each of the following cases:

if0 0,f ∞∞, iif0,f

0∞,

the BVP1.6-1.7has at least one positive solution.

4. Multiplicity

Next, we study the multiplicity of positive solutions of BVP1.6-1.7and assume in this section that

H3there is a p > 0 such that 0 ≤ up and 0 ≤ t ≤ 1 imply ft, u < ηp, where η C1C2C3M1M2

1

0G3s, sds

−1

.

H4there is a p > 0 such thatσpup and 0 ≤ t ≤ 1 implyft, uνp, where ν−1δ1δ2δ3C12C23m1

3/4

1/4G3s, sds.

Theorem 4.1. If f

0 > Landf> LandH3is satisfied, then BVP1.6-1.7has at least two positive solutions:u1andu2,such that0≤ u1 ≤pu2 .

Proof. According to the proof ofTheorem 3.1, there exists 0 < r0 < p < R1 < ∞, such that

0< r < r0impliesiA, Kr, K 0 andRR1impliesiA, KR, K 0.

We now prove thatiA, Kp, K 1 ifH3is satisfied. In fact, for everyu∂Kp, from the definition ofAwe have

Au max

1

0

G1t, δG2δ, τG3τ, sfs, usds dτ dδ

C1C2C3M1M2

1

0

G3s, sfs, usds

C1C2C3M1M2 1

0

G3s, sηp ds

u .

4.1

FromiiofLemma 2.8, we have

iA, Kp, K

1. 4.2

Combining3.14and3.19, we have

iA, KR\Kp, K

iA, KR, Ki

A, Kp, K

−1,

iA, Kp\Kr, K

iA, Kp, K

iA, Kr, K 1.

(12)

Therefore,Ahas fixed pointsu1andu2inKp\KrandKR\Kp, respectively, which means that u1tandu2tare positive solutions of BVP1.6-1.7and 0≤ u1 ≤pu2 . The proof is

completed.

Theorem 4.2. If f0 < Landf < LandH4is satisfied, then BVP1.6-1.7has at least two

positive solutions:u1andu2,such that0≤ u1 ≤pu2 .

Proof. According to the proof ofTheorem 3.1, there exists 0 < ω < p < R2 < ∞, such that

0< r < ωimpliesiA, Kr, K 1 andRR2impliesiA, KR, K 1.

We now prove thatiA, Kp, K 0 ifH4is satisfied. In fact, for everyu∂Kp, from the proof ofiofTheorem 3.1, we have

Au

1 2

1

0

G1

1 2, δ

G2δ, τG3τ, sfs, usds dτ dδ

δ1δ2δ3C12C23m1 3/4

1/4

G3s, sνp ds

u .

4.4

Therefore, AuAu1/2u , according toiofLemma 2.8,iA, Kp, K 0. Combining3.4and3.23, we have

iA, KR\Kp, K

iA, KR, Ki

A, Kp, K

1,

iA, Kp\Kr, K

iA, Kp, K

iA, Kr, K −1.

4.5

Therefore,Ahas the fixed pointsu1andu2inKp\KrandKR\Kp, respectively, which means thatu1tand u2tare positive solutions of BVP1.6-1.7and 0 ≤ u1 ≤ pu2 . The

proof is completed.

Theorem 4.3. Iff

0 > Landf< L, and there existsp2> p1>0that satisfies

ift, u< ηp1if0≤t≤1and0≤up1,

iift, uνp2if0≤t≤1andσp2≤up2,

then BVP1.6-1.7has at least three positive solutions:u1,u2,andu3,such that0≤ u1 ≤p1 ≤

u2 ≤p2≤ u3 .

Proof. According to the proof ofTheorem 3.1, there exists 0 < r0 < p1 < p2 < R3 <∞, such

that 0< r < r0impliesiA, Kr, K 1 andRR3impliesiA, KR, K 1. From the proof of Theorems4.1and4.2, we have

iA, Kp1, K

1, iA, Kp2, K

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Combining the four afore-mentioned equations, we have

iA, KR\Kp2, K

iA, KR, Ki

A, Kp2, K

1,

iA, Kp2\Kp1, K

iA, Kp2, K

iA, Kp1, K

−1,

iA, Kp1\Kr, K

iA, Kp1, K

iA, Kr, K 1.

4.7

Therefore,Ahas the fixed pointsu1,u2,andu3inKp1\Kr,Kp2\Kp1,andKR\Kp2, which

means thatu1t,u2t,andu3tare positive solutions of BVP1.6-1.7and 0≤ u1 ≤p1 ≤

u2 ≤p2≤ u3 . The proof is completed.

References

1 R. A. Gardner and C. K. R. T. Jones, “Traveling waves of a perturbed diffusion equation arising in a phase field model,”Indiana University Mathematics Journal, vol. 39, no. 4, pp. 1197–1222, 1990.

2 G. Caginalp and P. C. Fife, “Higher-order phase field models and detailed anisotropy,”Physical Review. B, vol. 34, no. 7, pp. 4940–4943, 1986.

3 T. Gyulov, G. Morosanu, and S. Tersian, “Existence for a semilinear sixth-order ODE,” Journal of Mathematical Analysis and Applications, vol. 321, no. 1, pp. 86–98, 2006.

4 L. A. Peletier and W. C. Troy,Spatial Patterns, vol. 45 ofProgress in Nonlinear Differential Equations and their Applications, Birkh¨auser Boston, Boston, Mass, USA, 2001.

5 L. A. Peletier and V. Rottsch¨afer, “Large time behaviour of solutions of the Swift-Hohenberg equation,” Comptes Rendus Math´ematique. Acad´emie des Sciences. Paris, vol. 336, no. 3, pp. 225–230, 2003.

6 S. Tersian and J. Chaparova, “Periodic and homoclinic solutions of extended Fisher-Kolmogorov equations,”Journal of Mathematical Analysis and Applications, vol. 260, no. 2, pp. 490–506, 2001.

7 Y. Li, “Positive solutions of fourth-order boundary value problems with two parameters,”Journal of Mathematical Analysis and Applications, vol. 281, no. 2, pp. 477–484, 2003.

8 S. Fan, “The new root formula and criterion of cubic equation,”Journal of Hainan Normal University, vol. 2, pp. 91–98, 1989Chinese.

References

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