Positive Solutions For A Singular Second Order Boundary Value Problem ∗
Wen-Shu Zhou
†Received 28 January 2008
Abstract
In this paper we obtain sufficient conditions of existence of positive solutions for a singular second order boundary value problem. Our argument is based on regularization technique, upper and lower solutions method and the Arzel´a-Ascoli theorem.
1 Introduction
In [1], Bertsch and Ughi investigated the following BVP which arises in study of a class of degenerate parabolic equations (also see [2, 3]):
u00+N−1
t u0−γ|u0|2
u + 1 = 0, 0< t <1, u(1) =u0(0) = 0,
(1)
whereN is a positive integer andγ >0, and obtained one decreasing positive solution via theories of ordinary differential equation. In the very recent paper [4], the authors considered the following BVP:
u00+λ
tu0−γ|u0|2
u +f(t) = 0, 0< t <1, u(1) =u0(0) = 0,
(2)
and proved, by the classical method of elliptic regularization, that BVP (2) has one positive solution which is not decreasing in the case: λ >0, γ > 1+λ2 , f ∈C[0,1] and f >0 on [0,1].
This paper considers the more general problem:
u00+λu0
tm −γ|u0|2
up +f(t) = 0, 0< t <1, u(1) =u0(0) = 0,
(3)
∗Mathematics Subject Classifications: 34B18
†Department of Mathematics, Dalian Nationalities University, 116600, P.R. China
154
whereλ, m, γ, p >0,f(t)∈C[0,1] andf(t)>0 on [0,1]. By a solution to BVP (3) we mean a functionu∈C2(0,1)∩C1[0,1] which is positive in (0, 1) and satisfies (3). By an argument based on the regularization technique, upper and lower solutions and the Arzel´a-Ascoli theorem, we obtain sufficient conditions of existence of solutions. Our main result reads
THEOREM 1. Let λ∈ (0,+∞), p∈ [1,2), m∈ (0, p/(2−p)], and let f ∈C[0,1]
and f(t)>0 on [0,1]. Ifγ >inf
t>1G(t), whereG(t) :R+→R+ is defined by G(t) =p+λ(2−p)
2 tp−1+(2−p)2max[0,1]f
4 tp−2,
then BVP (3) has at least one solution.
REMARK 1. Ifp= 1, then inf
t>1G(t) = 1+λ2 . Clearly, Theorem 1 is an extension of the existence results of [1, 4].
REMARK 2. Letp∈(1,2), and denote T0= (2−p)3max[0,1]f
2(p−1)[p+λ(2−p)], T∗=
(T0, T0>1, 1, T0<1.
Then inf
t>1G(t) =G(T∗).Indeed, since lim
t→0+G(t) = lim
t→+∞G(t) = +∞,G(t) must reach a minimum at some pointt∈(0,∞) such thatG0(t) = 0, and then, solving this equation yields t=T0 and hence, inf
t>0G(t) =G(T0). SinceG0(t)>0 for all t>T0, we see that
t>1infG(t) = inf
t>0G(t) =G(T0) ifT0>1, and inf
t>1G(t) =G(1) ifT0<1.
2 Proof of Theorem 1
Let∈(0,1), and defineH(t, v, ξ) : (0,1)×R×R→Rby H(t, v, ξ) =−λ ξ
(t+1/α)m+γ |ξ|2
[I(v)]p −f(t), where α= 2−p2 , andI(v) =v+2 ifv>0,I(v) =2 ifv <0. We have
|H(t, v, ξ)|6 λ
m/α|ξ|+γ|ξ|2 2p + max
[0,1]f
6 λ
m/α(1 +|ξ|2) + γ
2p|ξ|2+ max
[0,1] f 6
λ m/α + γ
2p + max
[0,1] f H(|ξ|)
(4)
for all (t, v, ξ) ∈ (0,1)×R×R, where H(s) = 1 +s2 for s > 0. Define operator L :C2(0,1)→C(0,1) by
(Lu)(t) =−u00+H(t, u, u0), 0< t <1.
Consider the problem:
((Lu)(t) = 0, 0< t <1,
u(1) =u(0) = 0. (5)
We calluan upper solution (lower solution) of problem (5) ifLu>(6)0 in (0,1), and u(t)>(6)0 fort= 0,1.
We will apply the upper and lower solutions method (see [5, pp.153, Theorem 2.5.4]
or [6, Theorem 1 and Remark 2.4]) to obtain one positive solution of problem (5). Note thatR+∞
0 s
H(s)ds= +∞.Then it suffices to find a lower solution and an upper solution to obtain a solution.
LEMMA 1. LetU =C1Wα with α= 2−p2 , where W(t) =t(1−t) andC1∈(0,1) such that 2C1α+C1αλ2α−1−m+γC12−pα26min
[0,1]f(t). ThenU is a lower solution of problem (5).
PROOF. Note thatW00=−2, W 6tand|W0|61 on [0,1]. Since U >0 in (0,1), some calculations give by noticingα>1 +m
LU=−U00−λ U0
(t+1/α)m +γ |U0|2
(U+2)p −f(t) 6−U00−λ U0
(t+1/α)m +γ|U0|2 Up −f(t)
= 2C1αWα−1−C1α(α−1)Wα−2|W0|2 +C1αλ Wα−1W0
(t+1/α)m +γC12−pα2|W0|2−f(t) 62C1αWα−1+C1αλ Wα−1W0
(t+1/α)m+γC12−pα2|W0|2−f(t) 62C1α+C1αλ(t+1/α)α−1−m+γC12−pα2−f(t) 62C1α+C1αλ2α−1−m+γC12−pα2−min
[0,1]f(t) 60, 0< t <1.
Thus, U is a lower solution of problem (5). The lemma follows.
Let inf
s>1H(s)≡ δ. Then it follows from the definition of infimum and γ > δ that forδ0=γ−δ2 >0, there existsC∗>1, such thatH(C∗)< δ+δ0< γ.
LEMMA 2. There exists a positive constant0∈(0,1), such that for any∈(0, 0), V=C∗(t+1α)αis an upper solution of problem (5).
PROOF. Noticingα>2 and 1 +m6α, we have LV=−V00−λ V0
(t+1/α)m+γ |V0|2
(V+2)p −f(t)
=−C∗α(α−1)(t+1/α)α−2−λαC∗(t+1/α)α−1−m +γC∗2−pα2[1 +2C∗−1(t+1/α)−α]−p−f(t)
>−C∗α(α−1)[1 +1/α]α−2−λαC∗[1 +1/α]α−1−m +γC∗2−pα2[1 +C∗−1]−p−max
[0,1] f(s)
=γC∗2−pα2−C∗α(α−1)−λαC∗−max
[0,1] f(s) +e
=C∗2−pα2(γ− G(C∗)) +e, 0< t <1,
wheree=C∗α(α−1)[1−(1+1/α)α−2]+λαC∗[1−(1+1/α)α−1−m]+[1+C∗−1]−p−1.
Clearly,e→0, (→0).Sinceγ >G(C∗), there exists 0∈(0,1) such that C∗2−pα2(γ− G(C∗)) +e>0.
This shows that for any∈(0, 0), LV>0,0< t <1.The lemma follows.
According to [5, pp.153, Theorem 2.5.4] or [6, Theorem 1 and Remark 2.4], for any fixed∈(0, 0), problem (5) has a solutionu∈C1[0,1] satisfyingu0∈C1(0,1) and
V>u>U >0, t∈(0,1). (6) Hence u satisfies
u00+λ u0
(t+1/α)m−γ |u0|2
(u+2)p+f(t) = 0, 0< t <1. (7) LEMMA 3. There exists a positive constantC2 independent of, such that for all ∈(0, 0)
|u0(t)|6C2, t∈[0,1]. (8) PROOF. It follows fromu(1) =u(0) = 0 andu>0 for allt∈[0,1] that
u0(0)>0>u0(1). (9) Integrating (7) over (0, 1) and integrating by parts give
u0(t)
1
0+ λu(t) (t+1/α)m
1
0
+mλ Z 1
0
u
(t+1/α)1+mdt
−γ Z 1
0
|u0|2 (u+2)pdt+
Z 1 0
f(t)dt= 0, and then, we obtain by (9)
γ Z 1
0
|u0|2
(u+2)pdt6 λu(t) (t+1/α)m
1
0
+mλ Z 1
0
u
(t+1/α)1+mdt+ Z 1
0
f(t)dt.
Since m 6 2−pp , 1 +m 6 α = 2−p2 . From (6), it is easy to see that (t+λu1/α(t))m
1 0+ mλR1
0 u
(t+1/α)1+mdt is uniformly bounded and hence, there exists a positive constant C3 independent of, such that
Z 1 0
|u0|2
(u+2)pdt6C3. (10)
By the inequality: a6a2+ 1 (a∈R), we obtain
|u0|
(t+1/α)m 6 |u0|2
(t+1/α)2m+ 1, t∈[0,1]. (11) By (6), we haveu+2 62C∗(t+1/α)α, t∈[0,1].Noticingαp>2m, we see that there exists a positive constant C4independent of, such that
(u+2)p6C4(t+1/α)2m, t∈[0,1].
Combining this and (11) we obtain
|u0|
(t+1/α)m 6C4
|u0|2
(u+2)p + 1, t∈[0,1], which and (10) imply that
Z 1 0
|u0|
(t+1/α)mdt6C3C4+ 1≡C5. (12) On the other hand, integrating (7) over (t1, t2), we have
u0(t)
t2
t1
=−λ Z t2
t1
u0
(t+1/α)mdt+γ Z t2
t1
|u0|2 (u+2)pdt−
Z t2
t1
f(t)dt.
Combining this with (10) and (12) we obtain for all∈(0, 0)
|u0(t2)−u0(t1)|6C6, ∀t1, t2∈[0,1], (13) where C6 =λC5+γC3+R1
0 f(t)dt. Noticing u(1) =u(0) = 0 and using the mean value theorem, there exists t ∈(0,1), such that u0(t) = 0. Then takingt1 =t in (13), we obtain the desired result.
By (6) and (8), we derive from (7) that there exists for anyδ∈(0,1/2) a positive constant Cδ independent of, such that for all∈(0, 0)
|u00(t)|6Cδ, δ6t61−δ.
From this and (8) and using Arzel´a-Ascoli theorem, there exist a subsequence of{u}, still denoted by{u}, and a functionu∈C1(0,1)∩C[0,1] such that, as→0,
u→u, uniformly in C[0,1], u→u, uniformly in C1[δ,1−δ],
and hence, by u(1) =u(0) = 0 and (6), usatisfies u(1) =u(0) = 0,C∗tα >u(t)>
C1[t(1−t)]αfor allt∈[0,1], thereforeu(t)>0 for allt∈(0,1), andu0(0) = lim
t→0 u(t)
t = 0. Then usatisfies the boundary conditions in (3).
Below, we show thatusatisfies the equation in (3). Integrating (7) over [t0, t] yields u0(t) =γ
Z t t0
|u0|2
(u+2)pds−λ Z t
t0
u0
(s+1/α)mds− Z t
t0
f(s)ds+u0(t0), and letting→0 and using Lebesgue dominated convergence theorem, we have
u0(t) =γ Z t
t0
|u0|2 up ds−λ
Z t t0
u0 smds−
Z t t0
f(s)ds+u0(t0), 0< t <1. (14) From this, we see that u∈C2(0,1) and satisfies the equation in (3).
It remains to show thatu0 is continuous att= 0 andt= 1. Letting→0 in (10) and (12) and using Fatou’s Lemma, we have
Z 1 0
|u0|2
up dt6C3,
Z 1 0
|u0|
tmdt6C5,
which show that |uu0p|2,|utm0| ∈ L1[0,1]. By the absolute continuity of integral, we see from (14) that u0 ∈C[0,1]. Theorem 1 is proved.
Acknowledgment.The author wants to thank the referee for his important com- ments which improve this paper. This research is supported by Dalian Nationalities University (no.20076209).
References
[1] M. Bertsch and M. Ughi, Positivity properties of viscosity solutions of a degenerate parabolic equation, Nonlinear Anal., 14(1990), 571–592.
[2] M. Bertsch, R. Dal Passo and M. Ughi, Discontinuous viscosity solutions of a de- generate parabolic equation, Trans. Amer. Math. Soc., 320(2)(1990), 779–798.
[3] G. I. Barenblatt, M. Bertsch and A. E. Chertock, V.M. Prostokishin, Self-similar intermediate asymptotic for a degenerate parabolic filtration-absorption equation.
Proc. Nat. Acad. Sci. (USA), 18(97)(2000), 9844–9848.
[4] W. Zhou and S. Cai, Positive solutions to a singular differential equation of second order, Nonlinear Anal., 68 (2008), 2319-2327.
[5] D. Guo, J. Sun and Z. Liu, Functional Methods for Nonlinear Ordinary Differential Equations, Shandong Science and Technology Press, Jinan, 2005. (Chinese) [6] D. Jiang and W. Gao, Singular boundary value problems for the one-dimension
p-Laplacian, J. Math. Anal. Appl., 270 (2002), 561–581.