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![Page 1: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/1.jpg)
Dynamics of Continuous, Discrete and Impulsive SystemsSeries A: Mathematical Analysis 8 (2001) 373-382Copyright c©2001 Watam Press
POSITIVE SOLUTIONS OF SINGULARSTURM-LIOUVILLE BOUNDARY VALUE
PROBLEMS
B.G. Zhang and Lingju KongDepartment of MathematicsOcean University of Qingdao
Qingdao 266003 P.R. China
Abstract. This paper studies the Sturm-Liouville boundary value problem(p(t)u′(t))′ + λa(t)f(t, u(t)) = 0, 0 < t < 1,αu(0)− βp(0)u′(0) = 0,γu(1) + δp(1)u′(1) = 0,
where λ > 0 and a is allowed to be singular at both end points t = 0 and t = 1. We shall
show the existence of this problem for λ on a suitable interval.
Keywords. Positive Solutions, boundary value problems, singular, fixed point theorem,
cone.
AMS (MOS) subject classification: 34B15
1 Introduction
Consider the Sturm-Liouville boundary value problem (p(t)u′(t))′ + λa(t)f(t, u(t)) = 0, 0 < t < 1,αu(0)− βp(0)u′(0) = 0,γu(1) + δp(1)u′(1) = 0,
(1)λ
where(H1) p(t) ∈ C([0, 1], [0,+∞)) and 0 <
∫ 1
0dtp(t) < +∞;
(H2) λ > 0, α, β, γ and δ are nonnegative, and βγ + αγ + αδ > 0;(H3) f(t, u) ∈ C([0, 1]× [0,+∞), R+) and a ∈ C((0, 1), [0,+∞));(H4) 0 <
∫ 1
0G(s, s)a(s)ds < +∞,
where
G(s, s) =1ρ(β + α
∫ s
0
dr
p(r))(δ + γ
∫ 1
s
dr
p(r)), 0 ≤ s ≤ 1,
and
ρ = αδ + αγ
∫ 1
0
dr
p(r)+ βγ.
For any t ∈ [0, 1], let
f0(t) = limu→0+
f(t, u)u
and f∞(t) = limu→+∞
f(t, u)u
.
![Page 2: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/2.jpg)
374 B.G. Zhang and L. Kong
Consider the following cases:(L1) f0(t) = +∞, t ∈ [0, 1]; (L2) f∞(t) = +∞, t ∈ [0, 1];(L3) f0(t) = 0, t ∈ [0, 1]; (L4) f∞(t) = 0, t ∈ [0, 1];(L5) f0(t) = l1 > 0, t ∈ [0, 1]; (L6) f∞(t) = l2 > 0, t ∈ [0, 1].
For the special case a(t) = 1, the boundary value problem (1)λ has beeninvestigated in [1] and [3]. In this paper, we want to obtain some existenceresults of positive solutions to the singular boundary value problem (1)λ forλ on a suitable interval. Our results improve and generalize some results in[2, 4]. The other results, we refer to [6, 7]. Some of our ideas are borrowedfrom [5].
2 Preliminaries
It is well known that
G(t, s) =
1ρ (β + α
∫ s0
drp(r) )(δ + γ
∫ 1
tdrp(r) ), 0 ≤ s ≤ t ≤ 1,
1ρ (β + α
∫ t0
drp(r) )(δ + γ
∫ 1
sdrp(r) ), 0 ≤ t ≤ s ≤ 1,
(2)
is the Green’s function of the following boundary value problem (p(t)u′(t))′ = 0, 0 < t < 1,αu(0)− βp(0)u′(0) = 0,γu(1) + δp(1)u′(1) = 0,
where
ρ = αδ + αγ
∫ 1
0
dr
p(r)+ βγ.
ClearlyG(t, s) ≤ G(s, s), 0 ≤ t, s ≤ 1. (3)
By (H4), there exits t0 ∈ (0, 1) such that a(t0) > 0. We may choose θ ∈ (0, 12 )
such that t0 ∈ (θ, 1− θ).Define a cone Kθ as follows:
Kθ = u ∈ C([0, 1])| u(t) ≥ 0, minθ≤t≤1−θ
u(t) ≥Mθ||u||, (4)
where
Mθ = minδ + γ
∫ 1
1−θdrp(r)
δ + γ∫ 1
0drp(r)
,β + α
∫ θ0
drp(r)
β + α∫ 1
0drp(r)
and||u|| = sup
t∈[0,1]
|u(t)|.
We donote
φ(t) = δ + γ
∫ 1
t
dr
p(r), 0 ≤ t ≤ 1,
![Page 3: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/3.jpg)
Positive Solutions of Boundary Value Problems 375
ψ(t) = β + α
∫ t
0
dr
p(r), 0 ≤ t ≤ 1.
Then
G(t, s) = 1
ρψ(s)φ(t), 0 ≤ s ≤ t ≤ 1,1ρψ(t)φ(s), 0 ≤ t ≤ s ≤ 1.
For θ ≤ t ≤ 1− θ, we have
G(t, s)G(s, s)
=
φ(t)φ(s) ≥
δ+γ∫ 1
1−θ
drp(r)
δ+γ∫ 1
0dr
p(r)
, s ≤ t,
ψ(t)ψ(s) ≥
β+α∫ θ
0dr
p(r)
β+α∫ 1
0dr
p(r)
, t ≤ s,
ThereforeG(t, s)G(s, s)
≥Mθ, θ ≤ t ≤ 1− θ.
i.e.,G(t, s) ≥MθG(s, s), θ ≤ t ≤ 1− θ. (5)
Define an operator Tλ on Kθ as follows:
Tλu(t) = λ
∫ 1
0
G(t, s)a(s)f(s, u(s))ds, λ > 0, u ∈ Kθ. (6)
Lemma 2.1. Tλ(Kθ) ⊂ Kθ.Proof. By (3), we have, for any t ∈ [0, 1] and u ∈ Kθ,
Tλu(t) = λ
∫ 1
0
G(t, s)a(s)f(s, u(s))ds
≤ λ
∫ 1
0
G(s, s)a(s)f(s, u(s))ds.
Hence
||Tλ|| ≤∫ 1
0
G(s, s)a(s)f(s, u(s))ds. (7)
By (5), we have
minθ≤t≤1−θ
Tλu(t) = minθ≤t≤1−θ
λ
∫ 1
0
G(t, s)a(s)f(s, u(s))ds
≥Mθλ
∫ 1
0
G(s, s)a(s)f(s, u(s))ds. (8)
In view of (7) and (8), we have
minθ≤t≤1−θ
Tλu(t) ≥Mθ||Tu||, u ∈ Kθ.
![Page 4: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/4.jpg)
376 B.G. Zhang and L. Kong
Therefore Tλ(Kθ) ⊂ Kθ, The proof is complete.Lemma 2.2. Tλ : Kθ → Kθ is completely continuous.The proof is similar to that of Lemma 2 in [4], we omit it here.Lemma 2.3.([7],[8]) Let K be a cone in a Banach space E and Ω1, Ω2
be two bounded open sets in E such that 0 ∈ Ω1 and Ω1 ⊂ Ω2. Let T :K
⋂(Ω2\Ω1) → K be a completely continuous operator. If
||Tu|| ≤ ||u||, u ∈ K⋂∂Ω1 and ||Tu|| ≥ ||u||, u ∈ K
⋂∂Ω2,
or||Tu|| ≥ ||u||, u ∈ K
⋂∂Ω1 and ||Tu|| ≤ ||u||, u ∈ K
⋂∂Ω2,
Then T has at least one fixed point in K⋂
(Ω2\Ω1).Let
A = max0≤t≤1
∫ 1
0
G(t, s)a(s)ds
and
Bθ = minθ≤t≤1−θ
∫ 1−θ
θ
G(t, s)a(s)ds.
Lemma 2.4. Assume that (H1) − (H4) hold and there exist two differentpositive numbers a and b such that
max0≤t≤1,0≤u≤a
f(t, u) ≤ a
λA(9)
andmin
θ≤t≤1−θ,Mθb≤u≤bf(t, u) ≥ b
λBθ. (10)
Then the BV P (1)λ has at least one positive solution u ∈ Kθ and mina, b ≤||u|| ≤ maxa, b.Proof. Without loss of generality, we may assume that a < b.Let
Ωa = u ∈ C([0, 1])| ||u|| < a, Ωb = u ∈ C([0, 1])| ||u|| < b.
For any t ∈ [0, 1] and u ∈ Kθ
⋂∂Ωa, by (9), we have
f(t, u(t)) ≤ a
λA.
Hence
Tλu(t) = λ
∫ 1
0
G(t, s)a(s)f(s, u(s))ds
≤ (λ∫ 1
0
G(s, s)a(s)ds)a
λA≤ a.
i.e.,||Tλu|| ≤ ||u||, u ∈ Kθ
⋂∂Ωa.
![Page 5: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/5.jpg)
Positive Solutions of Boundary Value Problems 377
By (10), for any t ∈ [θ, 1− θ] and u ∈ Kθ
⋂∂Ωb, we have
f(t, u) ≥ b
λBθ.
Hence
Tλu(12) = λ
∫ 1
0
G(12, s)a(s)f(s, u(s))ds
≥ λ
∫ 1−θ
θ
G(12, s)a(s)f(s, u(s))ds
≥ (λ∫ 1−θ
θ
G(12, s)a(s)ds)
b
λBθ≥ b.
i.e.,
||Tλu|| ≥ Tλu(12) ≥ ||u||, u ∈ Kθ
⋂∂Ωb.
It follows from Lemma 2.3 that there exists a u ∈ Kθ
⋂(Ωb\Ωa ) such that
Tλu(t) = u(t) and ||u|| is between a and b. This means that u(t) is a solutionof the BV P (1)λ and mina, b ≤ ||u|| ≤ maxa, b. The proof is complete.
3 Main Results
In this section, we denote
λ1 =1A
supr>0
r
max0≤t≤1,0≤u≤r
f(t, u)
andλ2 =
1Bθ
infr>0
r
min0≤t≤1,Mθr≤u≤r
f(t, u).
Under conditions of (H1) − (H4), it is obvious that 0 < λ1 ≤ +∞ and0 ≤ λ2 < +∞.Theorem 3.1. Assume that (H1) − (H2), (L1) and (L2) hold. Then thereexists λ1 > 0 such that the BV P (1)λ has at least two positive solutions for0 < λ < λ1.Proof. Define
s(r) =r
A max0≤t≤1,0≤u≤r
f(t, u).
By (H3), we know that s : (0.+∞) → (0,+∞).Clearly, S is continuous in (0,+∞). In view of (L1) and (L2), we havelimr→0+
s(r) = limr→+∞
s(r) = 0. Hence there exists r0 ∈ (0,+∞) such that
![Page 6: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/6.jpg)
378 B.G. Zhang and L. Kong
s(r0) = maxr>0
s(r) = λ1. For 0 < λ < λ1, there exist two positive numbers a1
and a2 such that 0 < a1 < r0 < a2 < +∞ and
s(a1) = s(a2) = λ.
i.e.,a1
A max0≤t≤1,0≤u≤a1
f(t, u)=
a2
A max0≤t≤1,0≤u≤a2
f(t, u)= λ.
Hencemax
0≤t≤1,0≤u≤a1f(t, u) =
a1
λA
andmax
0≤t≤1,0≤u≤a2f(t, u) =
a2
λA.
On the other hand, by (L1) and (L2), there exist b1 and b2 such that 0 <b1 < a1 < r0 < a2 < b2 < +∞ and
f(t, u)u
≥ 1λMθBθ
, t ∈ [0, 1], u ∈ (0, b1)⋃
[Mθb2,+∞).
Hencef(t, u) ≥ u
λMθBθ≥ b1λBθ
, t× u ∈ [0, 1]× [Mθb1, b1],
andf(t, u) ≥ u
λMθBθ≥ b2λBθ
, t× u ∈ [0, 1]× [Mθb2, b2].
Therefore, we have
minθ≤t≤1−θ,Mθb1≤u≤b1
f(t, u) ≥ min0≤t≤1,Mθb1≤u≤b1
f(t, u) ≥ b1λBθ
andmin
θ≤t≤1−θ,Mθb2≤u≤b2f(t, u) ≥ min
0≤t≤1,Mθb2≤u≤b2f(t, u) ≥ b2
λBθ.
By Lemma 2.4, the BV P (1)λ has at least two positive solutions. The proofis complete.From the proof of Theorem 3.1, the following conclusion is obvious.Theorem 3.2. Assume that (H1) − (H4) and one of (L1) and (L2) hold.Then the BV P (1)λ has at least one positive solution for 0 < λ < λ1.Theorem 3.3. Assume that (H1) − (H4), (L3) and (L4) hold. Then thereexists λ2 ≥ 0 such that the BV P (1)λ has at least two positive solutions forλ2 < λ < +∞.Proof. Define
w(r) =r
Bθ min0≤t≤1,Mθr≤u≤r
f(t, u).
![Page 7: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/7.jpg)
Positive Solutions of Boundary Value Problems 379
Clearly, w(r) is continuous in (0,+∞). From (L3) and (L4), we have
limr→0+
w(r) = limr→+∞
w(r) = +∞.
Hence there exists r0 ∈ (0,+∞) such that
w(r0) = minr>0
w(r) = λ2 ≥ 0.
Since λ2 < λ < +∞, we can find two positive numbers b1 and b2 such that0 < b1 < r0 < b2 < +∞ and
w(b1) = w(b2) = λ.
i.e.,
b1Bθ min
0≤t≤1,Mθb1≤u≤b1f(t, u)
=b2
Bθ min0≤t≤1,Mθb2≤u≤b2
f(t, u)= λ.
Hencemin
0≤t≤1,Mθb1≤u≤b1f(t, u) =
b1λBθ
andmin
0≤t≤1,Mθb2≤u≤b2f(t, u) =
b2λBθ
.
On the other hand, (L3) implies that there exists a1 ∈ (0, b1) such that
f(t, u)u
≤ 1λA
, t× u ∈ [0, 1]× [0, a1].
Hencef(t, u) ≤ a1
λA, t× u ∈ [0, 1]× [0, a1].
From (L4), there exists a ∈ (b2,+∞) such that
f(t, u)u
≤ 1λA
, t× u ∈ [0, 1]× [a,+∞).
Let M = max0≤t≤1,0≤u≤a
f(t, u). We can choose a2 > a such that a2 ≥ λMA.
Hencef(t, u) ≤ a2
λA, t× u ∈ [0, 1]× [0, a2].
By Lemma 2.4, the BV P (1)λ has at least two positive solutions for λ2 < λ <+∞. The proof is complete.From the proof of Theorem 3.3, we have the following results.Theorem 3.4. Assume that (H1) − (H4) and one of (L3) and (L4) hold.Then the BV P (1)λ has at least one positive solution for λ2 < λ < +∞.Corollary 3.1 Assume that (H1)−(H4) hold. Moreover, one of the following
![Page 8: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/8.jpg)
380 B.G. Zhang and L. Kong
conditions is true:(i) (L1) and (L4) hold;(ii) (L2) and (L3) hold.Then the BV P (1)λ has at least one positive solution for λ > 0.Proof. First, we prove the case (i).By Theorem 3.2, to prove the conclusion, we only need to prove λ1 = +∞.If
sup0≤t≤1,0≤u≤+∞
f(t, u) = M < +∞.
Thenλ1 ≥
1A
supr>0
r
M= +∞.
If f is unbounded, there exist tn ∈ [0, 1] and rn → +∞ such that
f(tn, rn) = max0≤t≤1,0≤u≤rn
f(t, u).
By (L4)
limrn→+∞
f(tn, rn)rn
= 0,
λ1 = maxr>0
s(r) ≥ maxrn>0
s(rn)
= maxrn>0
rnA max
0≤t≤1,0≤u≤rn
f(t, u)= maxrn>0
rnAf(tn, rn)
= +∞.
Hence λ1 = +∞.Now, we assume that (ii) holds. By Theorem 3.4, it is sufficient to proveλ2 = 0.By (L2), for t ∈ [0, 1], f(t, u) → +∞ as u→ +∞. There exist tn ∈ [0, 1] andrn → +∞ such that
f(tn,Mθrn) = min0≤t≤1,Mθrn≤u≤rn,
f(t, u).
Again by (L2),
limrn→0
f(tn,Mθrn)rn
= +∞,
λ2 = minr>0
w(r) ≤ minrn>0
w(rn)
= minrn>0
rnBθ min
0≤t≤1,Mθrn≤u≤rn
f(t, u)= minrn>0
rnf(tn,Mθrn)
= 0.
Hence λ2 = 0. The proof is complete.Remark 3.1. Corollary 3.1 improves and generalizes the results in [2] and[4].Similarly, we have
![Page 9: POSITIVE SOLUTIONS OF SINGULAR STURM-LIOUVILLE …monotone.uwaterloo.ca/~journal/parta/v8n3a/d362a.pdf · 376 B.G. Zhang and L. Kong Therefore T λ(K θ) ⊂ K θ, The proof is complete.](https://reader038.fdocument.org/reader038/viewer/2022100806/5a7435ac7f8b9a63638babd2/html5/thumbnails/9.jpg)
Positive Solutions of Boundary Value Problems 381
Corollary 3.2. Assume that (H1)− (H4) hold. Moreover, one of the follow-ing conditions is true:(i) (L1) and (L6) hold;(ii) (L2) and (L5) hold.Then the BV P (1)λ has at least one positive solution for 0 < λ < 1
Al1.
Corollary 3.3. Assume that (H1)− (H4) hold. Moreover, one of the follow-ing conditions is true:(i) (L3) and (L6) hold;(ii) (L4) and (L5) hold.Then the BV P (1)λ has at least one positive solution for 1
MθBθl2< λ < +∞.
Similarly to the proof of Corollary 3.1, we need only to prove λ1 ≥ 1Al1
forCorollary 3.2 and λ2 ≤ 1
MθBθl2for Corollary 3.3.
Example 3.1. Consider the singular boundary value problem: ((t12 + 1)u′(t))′ + λt−
12 (1− t)−
12 1+tu
u = 0, 0 < t < 1,u(0)− βu′(0) = 0,u(1) + 2δu′(1) = 0,
(11)λ
where p(t) = t12 + 1, a(t) = t−
12 (1 − t)−
12 , f(t, u) = (1+tu)
u , α = γ =1, β, δ ≥ 0. Then
∫ 1
0dtp(t) = 2 ln 2, ρ = β + δ + 2 ln 2, and G(s, s) =
(β+2 ln(1+s12 ))(δ+2 ln 2−2 ln(1+s
12 ))
β+δ+2 ln 2 . It is easy to check that (H1) − (H4) aresatisfied. Moreover, f0(t) = +∞ and f∞(t) = 0. Thus (L1) and (L4) hold.By Corollary 3.1, the boundary value problem (11)λ has at least one solutionfor λ > 0.Remark 3.2. Even if λ ≡ 1, the existence of positive solution of (11)λ cannot be obtained by the results in [2] and [4].
4 Acknowledgement
The research of this paper was supported by NNSF of China.
5 References
[1] R.P. Agarwal, Huei-Lin Hong and Chen-Chin Yeh, The existence of positive solu-tions for the Sturm-Liouville boundary value problems, Computers Math. Applic.,35, (1998), 89-96.
[2] L.H. Erbe and H. Wang, On the existence of positive solutions of ordinary differen-tial equations, Proc. Amer. Math. Soc., 120, (1994), 743-748.
[3] V. Anuradha, D.D. Hai and R. Shivaji, Existence results for superlinear semipositiveBVP’s, Proc. Amer. Math. Soc., 124, (1996), 757-763.
[4] Ruyun Ma, Positive solutions of singular second order boundary value problems,(in Chinese) Acta Mathematica Sinica, 41, (1998), 1225-1230.
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382 B.G. Zhang and L. Kong
[5] Qingliu Yao and Zhanbing Bai, Existence of positive solutions for boundary valueproblem of u(4)(t)−λh(t)f(u(t)) = 0, (in Chinese) Chinese Annals of Mathematics,20A:5, (1999), 575-578.
[6] W.C. Lian, F.H. Wong and C.C. Yeh, On the existence of positive solutions ofnonlinear second order differential equations, Proc. Amer. Math. Soc., 124, (1996),1117-1126.
[7] R.P. Agarwal and D. O’Regan, Singular boundary value problems for second orderordinary and delay differential equations, J. Differential Equations, 130, (1996),333-355.
[8] D. Guo and V. Lakshmikantham, Nonlinear Problems in Abstract Cones, AcademicPress, New York, 1988.
[9] M.A. Krasnosel’skii, Positive Solutions of Operator Equations, Noordhoff, Grohin-gen, The Netherlands, 1964.
Email: [email protected] June 2000; revised September 2000.http://monotone.uwaterloo.ca/∼journal