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We prove the existence of positive pseudo-symmetric solutions for four-point boundary-value problems with p-Laplacian

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ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp)

EXISTENCE OF POSITIVE PSEUDO-SYMMETRIC SOLUTIONS FOR ONE-DIMENSIONAL p-LAPLACIAN BOUNDARY-VALUE

PROBLEMS

YITAO YANG

Abstract. We prove the existence of positive pseudo-symmetric solutions for four-point boundary-value problems with p-Laplacian. Also we present an monotone iterative scheme for approximating the solution. The interesting point here is that the nonlinear termfinvolves the first-order derivative.

1. Introduction

In this paper, we consider the four-point boundary value problem

p(u0))0(t) +q(t)f(t, u(t), u0(t)) = 0, t∈(0,1), (1.1) u(0)−αu0(ξ) = 0, u(ξ)−γu0(η) =u(1) +γu0(1 +ξ−η), (1.2) where φp(s) =|s|p−2s, p > 1, (φp)−1q, 1p+ 1q = 1,α, γ ≥0, ξ, η ∈(0,1) are prescribed andξ < η.

The study of multipoint boundary-value problems for linear second-order ordi- nary differential equations was initiated by Il’in and Moiseer [7, 8]. Since then, the more general nonlinear multipoint boundary-value problems have been studied by many authors by using the Leray-Schauder continuation theorem, nonlinear al- ternative of Leray-Schauder and coincidence degree theory, we refer the reader to [1, 2, 3, 6] for some recent results. Recently, Avery and Henderson [4] consider the existence of three positive solutions for the problem

p(u0))0(t) +q(t)f(t, u(t)) = 0, t∈(0,1), (1.3)

u(0) = 0, u(η) =u(1). (1.4)

The definition of pseudo-symmetric was introduced in their paper. Based on this definition, Ma [9] studied the existence and iteration of positive pseudo-symmetric solutions for the problem (1.3)-(1.4). However, to the best of our knowledge, no work has been done for BVP (1.1)-(1.2) using the monotone iterative technique.

The aim of this paper is to fill the gap in the relevant literatures. We obtain not only the existence of positive solutions for (1.1)-(1.2), but also give an iterative scheme for approximating the solutions. It is worth stating that the first term of our iterative scheme is a constant function or a simple function. Therefore, the

2000Mathematics Subject Classification. 34B15, 34B18.

Key words and phrases. Iterative; pseudo-symmetric positive solution;p-Laplacian.

c

2007 Texas State University - San Marcos.

Submitted March 12, 2007. Published May 10, 2007.

1

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iterative scheme is significant and feasible. At the same time, we give a way to find the solution which will be useful from an application viewpoint.

We consider the Banach spaceE=C1[0,1] equipped with norm kuk:= max{kuk0,ku0k0},

where kuk0 = max0≤t≤1|u(t)|, ku0k0 = max0≤t≤1|u0(t)|. In this paper, a positive solution u(t) of BVP (1.1), (1.2) means a solution u(t) of (1.1), (1.2) satisfying u(t)>0, for 0< t <1.

We recall that a functionuis said to be concave on [0,1], if

u(λt2+ (1−λ)t1)≥λu(t2) + (1−λ)u(t1), t1, t2, λ∈[0,1].

Definition 1.1. Forξ∈(0,1) a functionu∈Eis said to be pseudo-symmetric ifu is symmetric over the interval [ξ,1]. That is, fort∈[ξ,1] we haveu(t) =u(1+ξ−t).

Remark 1.2. For ξ ∈ (0,1), if u ∈ E is pseudo-symmetric, we have u0(t) =

−u0(1 +ξ−t),t∈[ξ,1].

Define the coneK ofE as

K={u∈C1[0,1] :u(t)≥0, uis concave on[0,1] anduis symmetric on [ξ,1]}.

Forx, yinK a cone ofE, recall that x≤y ify−x∈K.

In the rest of the paper, we make the following assumptions:

(H1) q(t) ∈ L1[0,1] is nonnegative and q(t) = q(1 +ξ−t), a.e. t ∈ [ξ,1], and q(t)6≡0 on any subinterval of [0,1];

(H2) f ∈C([0,1]×[0,∞)×R,[0,∞)) andf(t, x, y) =f(1+ξ−t, x,−y), (t, x, y)∈ [ξ,1]×[0,∞)×R. Moreover,f(t,·, y) is nondecreasing for (t, y)∈[0,ξ+12

R, f(t, x,·) is nondecreasing for (t, x)∈[0,ξ+12 ]×[0,∞).

2. Existence Result

Lemma 2.1 ([9]). Each u∈K satisfies the following properties:

(i) u(t)≥1+ξ2 kuk0min{t,1 +ξ−t},t∈[0,1];

(ii) u(t)≥1+ξ kuk0,t∈[ξ,1+ξ2 ];

(iii) kuk0=u(1+ξ2 ).

Forx∈K, we define a mapping T:K→E given by

(T x)(t) =

















αφq(R1+ξ2

ξ q(τ)f(τ, x(τ), x0(τ))dτ) +Rt

0φq(R1+ξ2

s q(τ)f(τ, x(τ), x0(τ))dτ)ds, 0≤t≤ 1+ξ2 , αφq(R1+ξ2

ξ q(τ)f(τ, x(τ), x0(τ))dτ) +Rξ

0 φq(R1+ξ2

s q(τ)f(τ, x(τ), x0(τ))dτ)ds +R1

t φq(Rs

1+ξ 2

q(τ)f(τ, x(τ), x0(τ))dτ)ds, 1+ξ2 ≤t≤1.

(2.1)

Obviously, T x ∈ E, and we can prove T x is a solution of the boundary-value problem

p(u0))0(t) +q(t)f(t, x(t), x0(t)) = 0, t∈(0,1), (2.2) u(0)−αu0(ξ) = 0, u(ξ)−γu0(η) =u(1) +γu0(1 +ξ−η). (2.3) Therefore, each fixed point ofT is a solution of problem (1.1)-(1.2).

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Lemma 2.2. Suppose (H1), (H2) hold, then T :K→K is completely continuous and nondecreasing.

Proof. Fort∈[ξ,1+ξ2 ], we have 1 +ξ−t∈[1+ξ2 ,1]. Therefore, (T x)(1 +ξ−t)

=αφq( Z 1+ξ2

ξ

q(τ)f(τ, x(τ), x0(τ))dτ) + Z ξ

0

φq( Z 1+ξ2

s

q(τ)f(τ, x(τ), x0(τ))dτ)ds +

Z 1 1+ξ−t

φq( Z s

1+ξ 2

q(τ)f(τ, x(τ), x0(τ))dτ)ds

=αφq( Z 1+ξ2

ξ

q(τ)f(τ, x(τ), x0(τ))dτ) + Z ξ

0

φq( Z 1+ξ2

s

q(τ)f(τ, x(τ), x0(τ))dτ)ds

+ Z t

ξ

φq( Z 1+ξ2

s

q(τ)f(τ, x(τ), x0(τ))dτ)ds

=αφq( Z 1+ξ2

ξ

q(τ)f(τ, x(τ), x0(τ))dτ) + Z t

0

φq( Z 1+ξ2

s

q(τ)f(τ, x(τ), x0(τ))dτ)ds

= (T x)(t).

(2.4) So that,T x is symmetric on [ξ,1] with respect to 1+ξ2 . Obviously, (T x)(t)≥0, T x is concave on [0,1]. Therefore, T :K → K. It is easy to see that T :K →K is completely continuous.

Forx1(t), x2(t)∈K andx1(t)≤x2(t), thusx2(t)−x1(t)∈K. So thatx02(t)− x01(t)≥0,t∈[0,1+ξ2 ] andx02(t)−x01(t)≤0,t∈[1+ξ2 ,1]. Assumption (H2) implies

(T x1)(t)≤(T x2)(t).

Lemma 2.3 ([5]). Let u0, v0∈E, u0 < v0 andT : [u0, v0]→E be an increasing operator such that

u0≤T u0, T v0≤v0. Suppose that one of the following conditions is satisfied:

(C1) K is normal and T is condensing;

(C2) Kis regular andT is semicontinuous, i.e.,xn→xstrongly impliesT xn→ T x weakly.

Then T has a maximal fixed point x and a minimal fixed point x in [u0, v0];

moreover

x= lim

n→∞vn, x= lim

n→∞un, wherevn =T vn−1,un =T un−1 (n= 1,2,3, . . .), and

u0≤u1≤ · · · ≤un≤ · · · ≤vn≤ · · · ≤v1≤v0. Denote the positive quantities

A= 1/max αφq(

Z 1+ξ2

ξ

q(τ)dτ) + Z 1+ξ2

0

φq( Z 1+ξ2

s

q(τ)dτ)ds, φq( Z 1+ξ2

0

q(τ)dτ) , (2.5) B= 1/

Z 1+ξ2

ξ

φq( Z 1+ξ2

s

q(τ)dτ)ds. (2.6)

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Theorem 2.4. Assume (H1), (H2) hold. If there exist two positive numbers a, b with 1+ξ2b < a, such that

sup

t∈[0,1]

f(t, a, a)≤φp(aA), inf

t∈[ξ,1+ξ2 ]

f(t, 2ξb

1 +ξ,0)≥φp(bB). (2.7) Then, (1.1)-(1.2) has at least one positive pseudo-symmetric solution υ∈K with

b≤ kυk0≤a, 0≤ k(υ)0k0≤a, lim

n→∞Tnυ0, whereυ0(t) = 1+ξ2b min{t,1 +ξ−t},t∈[0,1].

Proof. We denote K[b, a] = {ω ∈K : b ≤ kωk0 ≤ a, 0 ≤ kω0k0 ≤a}. Next, we first proveT K[b, a] ⊂K[b, a]. Let ω ∈K[b, a], then 0≤ω(t) ≤maxt∈[0,1]ω(t)≤ kωk0≤a,

t ∈ [0,1], 0 ≤ω0(t) ≤maxt∈[0,1]0(t)| =kω0k0 ≤a, t∈ [0,1+ξ2 ]. By lemma 2.1 (ii), mint∈[ξ,1+ξ

2 ]ω(t) ≥ 1+ξ kωk01+ξ2ξb, mint∈[ξ,1+ξ

2 ]ω0(t)≥ω0(1+ξ2 ) = 0. So, by assumption (2.7), we have

0≤f(t, ω(t), ω0(t))≤f(t, a, a)≤ sup

t∈[0,1]

f(t, a, a)≤φp(aA), t∈[0,1 +ξ

2 ], (2.8) f(t, ω(t), ω0(t))≥f(t, 2ξb

1 +ξ,0)≥ inf

t∈[ξ,1+ξ2 ]

f(t, 2ξb

1 +ξ,0)≥φp(bB), t∈[ξ,1 +ξ 2 ].

(2.9) By lemma 2.2, we knowT ω∈K. So, lemma 2.1 (iii) implies kT ωk0= (T ω)(1+ξ2 ).

As a result, kT ωk0

= (T ω)(1 +ξ 2 )

=αφq( Z 1+ξ2

ξ

q(τ)f(τ, x(τ), x0(τ))dτ) + Z 1+ξ2

0

φq( Z 1+ξ2

s

q(τ)f(τ, x(τ), x0(τ))dτ)ds

≤aA(αφq( Z 1+ξ2

ξ

q(τ)dτ) + Z 1+ξ2

0

φq( Z 1+ξ2

s

q(τ)dτ)ds)≤a;

k(T ω)0k0= (T ω)0(0)

q( Z 1+ξ2

0

q(τ)f(τ, x(τ), x0(τ))dτ)

≤aAφq( Z 1+ξ2

0

q(τ)dτ)≤a;

kT ωk0= (T ω)(1 +ξ 2 )

≥ Z 1+ξ2

ξ

φqZ 1+ξ2

s

q(τ)f(τ, x(τ), x0(τ))dτ ds

≥bB Z 1+ξ2

ξ

φq

Z 1+ξ2

s

q(τ)dτ ds=b.

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Thus,b≤ kT ωk0≤a, 0≤ k(T ω)0k0≤a, which impliesT K[b, a]⊂K[b, a].

Letυ0(t) = 1+ξ2b min{t,1 +ξ−t},t∈[0,1], thenkυ0k0=bandkυ00k0=1+ξ2b < a, soυ0∈K[b, a]. Letυ1=T υ0, thenυ1∈K[b, a], we denote

υn+1=T υn =Tn+1υ0, (n= 0,1,2, . . .). (2.10) SinceT K[b, a]⊂K[b, a], we haveυn ∈K[b, a], (n= 0,1,2, . . .). Fromυ1∈K[b, a], thus

υ1(t)≥ 2

1 +ξkυ1k0min{t,1 +ξ−t} ≥ 2b

1 +ξmin{t,1 +ξ−t}=υ0(t), t∈[0,1], which impliesT υ0≥υ0. K is normal andT is completely continuous. By Lemma 2.3, we have T has a fixed point υ ∈K[b, a]. Moreover,υ = limn→∞υn. Since kυk0 ≥ b > 0 and υ is a nonnegative concave function on [0,1], we conclude that υ(t)>0,t∈(0,1). Therefore, υ is a positive pseudo-symmetric solution of

(1.1)-(1.2).

Corollary 2.5. Assume (H1),(H2)hold. If lim sup

l→0

inf

t∈[ξ,1+ξ2 ]

f(t, l,0)

φp(l) ≥φp(1 +ξ

2ξ B), (2.11)

particularly,lim supl→0inft∈[ξ,1+ξ 2 ]

f(t,l,0)

φp(l) = +∞, lim inf

l→+∞ sup

t∈[0,1]

f(t, l, l)

φp(l) ≤φp(A), (2.12)

particularly, lim infl→+∞supt∈[0,1] f(t,l,l)φ

p(l) = 0. Where A, B are defined as (2.5), (2.6). Then there exist two positive numbers a, bwith 1+ξ2b < a, such that problem (1.1), (1.2) has at least one positive pseudo-symmetric solution υ∈K with

b≤ kυk0≤a, 0≤ k(υ)0k0≤a, lim

n→∞Tnυ0, whereυ0(t) = 1+ξ2b min{t,1 +ξ−t},t∈[0,1].

Remark 2.6. Problem (1.1)-(1.2) may have two positive pseudo-symmetric so- lutions ω, υ ∈ K, if we make another iteration by choosing ω0(t) = a and ωn = limn→∞Tnω0. However,ω andυ may be the same solution.

Example 2.7. We consider the problem (|u0|3u0)0(t) + 1

t12(43−t)12[(u0(t))2+ ln((u(t))2+ 1)] = 0, t∈(0,1), (2.13) u(0)−2u0(1

3) = 0, u(1

3)−3u0(1

2) =u(1) + 3u0(5

6). (2.14)

We notice that p = 5, α = 2, ξ = 13, γ = 3, η = 12. Obviously, f(t, u, u0) = (u0(t))2+ln((u(t))2+1) is nondecreasing for (t, u0)∈[0,23]×R,f(t, u, u0) = (u0(t))2+ ln((u(t))2 + 1) is nondecreasing for (t, u) ∈ [0,23]×[0,∞), q(t) = 1

t12(43−t)12

is nonnegative and pseudo-symmetric about 23. So, conditions (H1),(H2) are satisfied.

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On the other hand, lim sup

l→0

inf

t∈[ξ,1+ξ2 ]

f(t, l,0)

φp(l) = lim sup

l→0

inf

t∈[13,23]

ln(l2+ 1) l4 =∞, lim inf

l→+∞ sup

t∈[0,1]

f(t, l, l)

φp(l) = lim inf

l→+∞ sup

t∈[0,1]

l2+ ln(l2+ 1)

l4 = 0.

Therefore, from Corollary 2.5, it follows that (2.13)-(2.14) has at least one positive pseudo-symmetric solution.

References

[1] R. P. Agarwal and D. O’Regan;Nonlinear boundary-value problems on time scales, Nonlinear Anal. 44 (2001), 527-535.

[2] R. P. Agarwal and D. O’Regan;Lidstone continuous and discrete boundary-value problems, Mem. Diff. Equ. Math. Phys. 19 (2000), 107-125.

[3] R. P. Agarwal, H. L¨u and D. O’Regan; Positive solutions for the boundary-value problem (|u00|p−2u00)λq(t)f(u(t)) = 0, Mem. Diff. Equ. Math. Phys. 28 (2003), 33-44.

[4] R. I. Avery, J. Henderson;Existence of three positive pseudo-symmetric solutions for a one- dimensional p-laplacian, J. Math. Anal. Appl. 277 (2003), 395-404.

[5] D. Guo, V. Lakshmikantham;Nonlinear problems in abstrat cone, Academic Press, Sandiego, 1988.

[6] X. He, W. Ge;A remark on some three-point boundary value problem for the one-dimensional p-laplacian, ZAMM. 82 (2002), 728-731.

[7] V. A. Il’in, E. I. Moiseer; Nonlocal boundary value problem of the first kind for a sturm- liouville operator in its differential and finite difference aspects, Differential Equations. 23 (1987), 803-810.

[8] V. A. Il’in, E. I. Moiseer; Nonlocal boundary value problem of the second kind for a sturm- liouville operator, Differential Equations. 23 (1987), 979-987.

[9] Dexiang Ma, Weigao Ge; Existence and iteration of positive pseudo-symmetric solutions for a three-point second-order p-Laplacian BVP, Appl. Math. Lett. (2007), doi: 10.1016 j.aml.2006.05.025.

Yitao Yang

Institute of Automation, Qufu Normal University, Qufu, Shandong 273165, China E-mail address:[email protected]

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