• 検索結果がありません。

Existence of positive solution for a class of singular boundary value problems of the type −x00(t) =f(t, x(t), x0(t

N/A
N/A
Protected

Academic year: 2022

シェア "Existence of positive solution for a class of singular boundary value problems of the type −x00(t) =f(t, x(t), x0(t"

Copied!
10
0
0

読み込み中.... (全文を見る)

全文

(1)

T

he

J

ournal of

N

onlinear

S

cience and

A

pplications http://www.tjnsa.com

POSITIVE SOLUTIONS FOR A CLASS OF SINGULAR TWO POINT BOUNDARY VALUE PROBLEMS

RAHMAT ALI KHAN1,∗ AND NASEER AHMAD ASIF2 Communicated by J. J. Nieto

Abstract. Existence of positive solution for a class of singular boundary value problems of the type

−x00(t) =f(t, x(t), x0(t)), t(0,1) x(0) = 0, x(1) = 0,

is established. The nonlinearityf C((0,1)×(0,∞)×(−∞,∞),(−∞,∞)) is allowed to change sign and is singular at t = 0, t = 1 and/or x = 0. An example is included to show the applicability of our result.

1. Introduction and preliminaries

Singular boundary value problems arise in various fields of Mathematics and Physics such as nuclear physics, boundary layer theory, nonlinear optics, gas dynamics, etc, [1, 5, 9, 12, 14, 17, 18, 19]. For more details on singular BVPs and recent developments, we refer the readers to the recent monograph by R. P.

Agarwal and D. O’ Regan [4] and [6, 8, 9, 15].

In this paper, we consider a class of second order singular boundary value problems of the type

−x00(t) =f(t, x(t), x0(t)), t∈(0,1),

x(0) = 0, x(1) = 0, (1.1)

Date: Received: 2 December 2008; Revised: 25 February 2009.

2000Mathematics Subject Classification. Primary 34A45; Secondary 34B15.

Key words and phrases. Positive solutions, Singular differential equations, Dirichlet bound- ary conditions.

Corresponding author.

126

(2)

wheref ∈C((0,1)×(0,∞)×(−∞,∞),(−∞,∞)) and may be singular att= 0, t = 1 and/or x = 0 and is allowed to change sign. We establish existence of positive solutions for the BVP (1.1) under a weaker hypothesis on f. Recently, existence of positive solutions for singular boundary value problems, in the case when the nonlinearity f is independent of the derivative term, has been studied by many authors, [3, 10, 11, 13, 21]. In these papers, the nonlinearity is assumed to be non-negative and either be sublinear or superlinear. Hence, the results of these papers would be applicable to a limited class of boundary values problems.

Moreover, most of nonlinear problems from the applied sciences, the nonlinearity explicitly depends on the derivative term, for example, the differential equation

x00(t) =−λ 1−t2 x(t)

0

− t

x(t), t∈[0,1),

together with some suitable boundary conditions, that explicitly depends on the derivative, arises in the boundary layer theory in fluid mechanics [19]. Further, the nonlinearity f does not satisfy the sublinear and superlinear conditions in most cases and may change sign. Hence, the study of boundary value problems without the above mentioned restrictions is of great importance.

Recently, existence theory for positive solutions of two point boundary value problems without the first derivative term is studied in [16, 19, 20]. Inspired by the above papers, the aim of the present paper is to improve and generalize the result studied in [20] to the case when the nonlinearity f explicitly depends on the derivative term x0. We study the problem under much weaker hypothesis on f. We include an example to show the applicability of our result.

Throughout this paper, we assume that the following condition holds.

(A1) there existk ∈C((0,1),(0,∞)) and a decreasingF ∈C((0,∞),(0,∞)) such that

Z 1

0

t(1−t)k(t)dt <∞and Z

0

du

F(u) =∞.

The condition R 0

du

F(u) =∞implies that we can choose R >1 such that Z R

1

du

F(u) >max

(Z 1/2

0

sk(s)ds, Z 1

1/2

(1−s)k(s)ds )

. (1.2)

For fixed n ∈ {3,4,5, . . .}, let M = max{F(1n)k(t) : t ∈ [n1,1− n1]} and choose C >√

2M R.

Foru ∈C[0,1] we write kuk= max{|u(t)| :t∈[0,1]} and for u∈C1[0,1], we write kuk1 = max{kxk,γ3kx0k} where γ = n−2n for n ≥ 3. Clearly, C1[0,1] with the norm k.k1 is a Banach space.

The only condition we are imposing on the nonlinearityf is the following:

(A2)

0≤f(t, x(t), x0(t))≤k(t)F(x(t)) on (0,1)×(0, R]×[−C, C].

(3)

For fixed n∈ {3,4,5, ...}, consider the BVPs

−x00(t) =f(t, x(t), x0(t)), t∈[1

n,1− 1 n], x(1

n) = 1

n, x(1− 1 n) = 1

n.

(1.3)

We write (1.3) as an equivalent integral equation x(t) = 1

n +

Z 1−1/n

1/n

Gn(t, s)f(s, x(s), x0(s))ds, t∈[1

n,1− 1

n], (1.4) where

Gn(t, s) = n n−2

((s− n1)(1− 1n−t), if n1 ≤s < t ≤1− n1 (t− n1)(1− n1 −s), if n1 ≤t ≤s≤1−n1, is the Green’s function for the corresponding homogeneous problem

−x00(t) = 0, t∈[1

n,1− 1 n] x(1

n) = 0, x(1− 1 n) = 0.

(1.5)

Notice thatGn(t, s)≥0 on (n1,1−n1)×(n1,1−n1) andGn(t, s)≤Gn(s, s), t∈(0,1).

Moreover,

t∈[0,1]max

Z 1−1/n

1/n

Gn(t, s)ds=

Z 1−1/n

1/n

Gn(s, s)ds = γ2 6 , max

t∈[0,1]|

Z 1−1/n

1/n

∂Gn

∂t (t, s)ds|=

Z 1−1/n

1/n

|∂Gn

∂t (t, s)|ds = γ 2. 2. Main results

Theorem 2.1. Assume that (A1) and (A2) hold. Then boundary value problem (1.3) has a solution x∈ C1[0,1] such that n1 ≤ x(t) < R and |x0(t)| < C for t ∈ [n1,1−n1].

Proof. Define retractionsq: (−∞,∞)→[−C, C] byq(v) = max{−C,min{v, C}}

and p: (−∞,∞)→[n1, R] by pn(x(t)) = max{n1,min{x(t), R}}. Clearly, q, p are continuous and q(v) = v for|v| ≤C, p(v) =v for n1 ≤v ≤R.

Consider the modified BVP

−x00(t) = Fn(t, x(t), x0(t)), t∈[1

n,1− 1 n], x(1

n) = 1

n, x(1− 1 n) = 1

n,

(2.1)

whereFn(t, x(t), x0(t)) =f(t, pn(x(t)), q(x0(t))). Clearly,Fnis continuous, bounded and nonnegative on [1n,1−n1]×R×R. Further, any solutionx∈C1[0,1] of (2.1) such that

1

n ≤x(t)< R, |x0(t)|< C, t∈[1

n,1− 1

n], (2.2)

is a solution of (1.3). Obviously,x(t)≥ n1 on [1n,1−n1] as Fn≥0.

(4)

We write the BVP (2.1) as an equivalent integral equation of the type x(t) = 1

n +

Z 1−1/n

1/n

Gn(t, s)Fn(s, x(s), x0(s))ds (2.3) and define an operator Tn :C1[0,1]→C1[0,1] by

(Tnx)(t) = 1 n +

Z 1−1/n

1/n

Gn(t, s)Fn(s, x(s), x0(s))ds. (2.4) By a solution of (2.1) we mean a solution of the operator equation (I−Tn)(x) = 0, that is, a fixed point of Tn. We show that Tn has a fixed point x ∈ C1[0,1].

Clearly, Tn is continuous and completely continuous as Fn is continuous and bounded.

Choose ¯R >max{R,13 +M16γ2}, where M1 = max{f(t, x, x0) :t∈[1

n,1− 1

n], x∈[1

n, R], x∈[−C, C]}

and define an open, bounded and convex set

R¯ ={x∈C1[0,1] :kxk1 <R}.¯ Forx∈ΩR¯, we have

kTnxk ≤ 1

n + max

t∈[0,1]|

Z 1−1/n

1/n

Gn(t, s)Fn(s, x(s), x0(s))ds|

≤ 1 3 +M1

Z 1−1/n

1/n

|Gn(s, s)|ds = 1

3 +M1γ2 6 ,

k(Tnx)0k ≤ max

t∈[0,1]|

Z 1−1/n

1/n

∂Gn

∂t (t, s)Fn(s, x(s), x0(s))ds| ≤ M1γ 2 . It follows that

kTnxk1 = max{kTnxk,γ

3k(Tnx)0k} ≤ 1

3+ M1γ2

6 <R¯ for every x∈ΩR¯. Hence,Tn(ΩR¯)⊂ΩR¯. Consequently, by Schauder’s fixed point theorem, the BVP (2.1) has a solution in ΩR¯.

Now, we show that any solutionxof (2.1) must satisfies (2.2). Firstly, we show that x < R on [n1,1− n1]. Assume that this is not true and x(t) ≥ R for some t∈[1n,1− 1n]. Let

ξ= min{t∈[1

n,1− 1

n] :x(t) =R}.

We discuss different cases:

Case1: Ifξ ≤1/2, since x(1n) = n1 < R, there exist subintervals, say [ξ2i−1, ξ2i]⊆ [n1, ξ], i= 1,2,3,· · ·, m such that

(1): ξ1 = n12m =ξ, ξ2i−1 < ξ2i for i= 1,2,3,· · · , m,

(2) ξ2i ≤ξ2i+1, x(ξ2i) =x(ξ2i+1) andx02i) = 0 for i= 1,2,3,· · · , m−1, (3) x0(t)≥0 for t∈[ξ2i−1, ξ2i], i= 1,2,3,· · · , m.

(5)

Fort ∈[ξ2i−1, ξ2i],i= 1,2,3,· · · , m, using (A2) and the fact thatx(t)∈[1n, R], we have

−x00(t) = Fn(t, x(t), x0(t)) =f(t, pn(x(t)), q(x0(t)))≤k(t)F(x(t)), t∈[ξ2i−1, ξ2i].

(2.5) Integrating (2.5) from t to ξ2i, using (2) and the decreasing property of F, we obtain

x0(t)≤F(x(t)) Z ξ2i

t

k(s)ds, t∈[ξ2i−1, ξ2i], i= 1,2,3,· · · , m, which implies that

x0(t) F(x(t)) ≤

Z ξ2i

t

k(s)ds, t∈[ξ2i−1, ξ2i], i= 1,2,3,· · · , m. (2.6) Integrating (2.6) fromξ2i−1 to ξ2i, we have

Z ξ2i

ξ2i−1

x0(t) F(x(t))dt ≤

Z ξ2i

ξ2i−1

Z ξ2i

t

k(s)dsdt, which can be written as

Z x(ξ2i)

x(ξ2i−1)

du F(u) ≤

Z ξ2i

ξ2i−1

sk(s)ds, i= 1,2,3,· · · , m. (2.7) Summing fromi= 1 to m and using (2) (x(ξ2i) = x(ξ2i+1)), we obtain

Z R

1/n

du F(u) ≤

Z 1/2

0

sk(s)ds.

Lettingn → ∞, we have Z R

0

du F(u) ≤

Z 1/2

0

sk(s)ds, a contradiction to (1.2).

Case2: Let ξ≥1/2 andη = max{t∈[12,1− n1] :x(t) = R}. Since x(1−n1) =

1

n < R, there exist subintervals [η2i, η2i−1] ⊆ [12,1− 1n], i = 1,2,3,· · · , m0 such that

(4) η1 = 1− n1, η2m0 =η, η2i < η2i−1 for i= 1,2,3,· · · , m0,

(5) η2i+1 ≤η2i, x(η2i) =x(η2i+1),x02i) = 0 for i= 1,2,3,· · · , m0−1 and (6) x0(t)≤0 for t∈[η2i, η2i−1], i= 1,2,3,· · · , m0.

Integrating (2.5) fromη2i tot, using (5), the decreasing property ofF and then integrating from η2i to η2i−1, we obtain

Z x(η2i)

x(η2i−1)

du F(u) ≤

Z η2i−1

η2i

(1−s)k(s)ds, i= 1,2,3,· · · , m0. (2.8) Summing (2.8) fromi= 1 to i=m0 and using (5) (x(η2i) =x(η2i+1)), we obtain

Z R

1/n

du F(u) ≤

Z 1

1/2

(1−s)k(s)ds.

(6)

Letting limitn → ∞, we get Z R

0

du F(u) ≤

Z 1

1/2

(1−s)k(s)ds which is a contradiction to (1.2).

Now we show that any solution x(t) of (2.1) must satisfies |x0(t)| ≤ C, t ∈ [n1,1 − n1]. From the boundary conditions, x(n1) = n1 and x(1− 1n) = n1, it follows that there exist p ∈ (n1,1− n1) such that x0(p) = 0. Suppose there exist t0 ∈ (n1,1−n1) such that x0(t0)> C. As in the first part of this theorem, choose [ξ2i−1, ξ2i]⊆[n1,1−n1] such that

x0(t)≥0 on [ξ2i−1, ξ2i] and x02i) = 0, i= 1,2,3,· · · . Hence, there exist somei0 such that t0 ∈[ξ2i0−1, ξ2i0]. Let

C1 = max{x0(t) :t ∈[ξ2i0−1, ξ2i0]}=x0).

Clearly,C1 ≥C and in view of (A2), we have

−x00(t) = f(t, x(t), q(x0(t)))≤k(t)F(x(t))≤M.

Hence,

−x0(t)x00(t)≤M x0(t), t∈[ξ2i0−1, ξ2i0].

Integrating from ξ to ξ2i0, we have

− Z ξ2i0

ξ

x0(t)x00(t)dt≤M Z ξ2i0

ξ

x0(t)dt, implies that

Z C1

0

vdv ≤M R⇒C1 ≤√ 2M R,

which contradict the definition of C. Hence,x0(t)≤C, t∈[n1,1− n1].

Similarly, we can show thatx0(t)≥ −C, t∈[n1,1− n1].

Theorem 2.2. Assume that(A1)and(A2) hold. Then, the boundary value prob- lem (1.1) has a positive solution x.

Proof. By Theorem 2.1, any solution xn of (1.3) satisfies 1

n ≤xn(t)≤R, |x0n(t)| ≤C for t ∈[1

n,1− 1

n], n= 3,4,5, ....

Hence, for each h∈(0,1/2), there exist a natural number m∈ {3,4,5,· · · } such that xn(t)>0 for all t∈[h,1−h] and n≥m.

Consider the integral equation, xn(t) =xn(1−h)−xn(h)

1−2h (t−h) +xn(h) + Z t

h

(s−h)(1−h−t)

1−2h f(s, xn(s), x0n(s))ds +

Z 1−h

t

(t−h)(1−h−s)

1−2h f(s, xn(s), x0n(s))ds, t∈[h,1−h].

(2.9)

(7)

Differentiating with respect tot, we obtain x0n(t) =xn(1−h)−xn(h)

1−2h − 1

1−2h Z t

h

(s−h)f(s, xn(s), x0n(s))ds

+ 1

1−2h Z 1−h

t

(1−h−s)f(s, xn(s), x0n(s))ds.

(2.10)

For anyt1, t2 ∈[h,1−h], we have

|x0n(t2)−x0n(t1)|=

−1 1−2h

Z t2

h

(s−h)f(s, xn(s), x0n(s))ds

+ 1

1−2h Z 1−h

t2

(1−h−s)f(s, xn(s), x0n(s))ds

+ 1

1−2h Z t1

h

(s−h)f(s, xn(s), x0n(s))ds

− 1 1−2h

Z 1−h

t1

(1−h−s)f(s, xn(s), x0n(s))ds

= 1

1−2h

Z t2

t1

(s−h)f(s, xn(s), x0n(s))ds+ Z t2

t1

(1−h−s)f(s, xn(s), x0n(s))ds

≤L|t2−t1|,

where L = max{f(t, u, v) : (t, u, v) ∈ [h,1−h]×[n1, R]×[−C, C]}. Thus the sequences{xn}and {x0n} are uniformly bounded and equicontinuous. By Arzel`a- Ascoli theorem, there exist a subsequence{xnk} of{xn} converging uniformly on [h,1−h] such that

nlimk→∞xnk(t) =x(t),

nlimk→∞x0n

k(t) =x0(t), where x∈C1[0,1]. Taking limh→0, we have

nlimk→∞xnk(t) = x(t) on (0,1).

Further,x >0 on (0,1). Letting limnk→∞, (2.12) and (2.10) yield x(t) =x(1−h)−x(h)

1−2h (t−h) +x(h) + 1 1−2h

Z t

h

(s−h)(1−h−t)f(s, x(s), x0(s))ds

+ 1

1−2h Z 1−h

t

(t−h)(1−h−s)f(s, x(s), x0(s))ds,

x0(t) = x(1−h)−x(h)

1−2h − 1

1−2h Z t

h

(s−h)f(s, x(s), x0(s))ds

+ 1

1−2h Z 1−h

t

(1−h−s)f(s, x(s), x0(s))ds.

(8)

Hence,

x00(t) =− 1

1−2h(t−h)f(t, x(t), x0(t))− 1

1−2h(1−h−t)f(t, x(t), x0(t)) =−f(t, x(t), x0(t))

−x00(t) =f(t, x(t), x0(t)), t∈(0,1) (2.11) which implies that x satisfies the differential equation (1.1). Moreover,

x(0) = lim

nk→∞x 1 nk

= lim

nk→∞xnk 1 nk

= lim

nk→∞

1 nk = 0, and

x(1) = lim

nk→∞x 1− 1

nk

= lim

nk→∞xnk 1− 1

nk

= lim

nk→∞

1 nk = 0,

which implies thatxalso satisfies the boundary conditions and hence is a solution

of (1.1).

Example 2.3. Consider the boundary value problem

−x00(t) = x0(t) + 5

t(1−t)(x(t))2; t∈(0,1) x(0) = 0, x(1) = 0.

(2.12)

Choose k(t) = t(1−t)1 and F(u) = u92. Clearly F is decreasing and R 0

du

F(u) = ∞.

Since

Z 12

0

tk(t)dt = ln 2, Z 1

1 2

(1−t)k(t)dt = ln 2.

Hence, from the relation RR 1

du

F(u) >ln 2, we haveR >(1 + 27 ln 2)3. Also, M = max{F(1

n)k(t) : t∈[1

n,1− 1

n]}= max{ 9n2

t(1−t) : t∈[1

n,1− 1

n]}= 9.

Hence C = 3. Moreover, 0≤ x0(t) + 5

tµ(1−t)ν(x(t))2 =f(t, x(t), x0(t))≤k(t)F(x(t)) for x0(t)∈[−3,3], t∈(0,1).

By Theorem 2.2, the problem (2.12) has a solutionx such that 0< x(t)≤(1 + 27 ln 2)3, |x0(t)| ≤3, t∈(0,1).

Acknowledgements: Research of R. A. Khan is supported by HEC, Pakistan, Project 2-3(50)/PDFP/HEC/2008/1.

(9)

References

[1] G. A. Afrouzi, M. Khaleghy Moghaddam, J. Mohammadpour and M. Zameni, On the positive and negative solutions of Laplacian BVP with Neumann boundary conditions, J.

Nonlinear Sci. Appl., 2 (2009), 38–45.

[2] R.P. Agarwal and D. O’ Regan, Twin solutions to singular Dirichlet problems, J. Math.

Anal. Appl., 240 (1999), 433–445. 1

[3] R.P. Agarwal and D. O’ Regan, An upper and lower solution approach for a generalized Thomas-Fermi theory of neutral atoms, Mathematical Problems in Engineering, 8 (2002), 135–142.

[4] R. P. Agarwal and D. O’Regan, Singular differential and integral equations with applica- tions, Kluwer Academic Publishers, London, 2003. 1

[5] R. P. Agarwal, D. O’Regan and P. K. Palamides, The generalized Thomas-Fermi singular boundary value problems for neutral atoms, Math. Methods in the Appl. Sci., 29 (2006), 49 – 66. 1

[6] M. van den Berg, P. Gilkey and R. Seeley, Heat content asymptotics with singular initial temperature distributions, J. Funct. Anal., 254 (2008), 3093–3122. 1

[7] A. Callegari and A. Nachman, A nonlinear singular boundary value problem in the theory of pseudoplastic fluids, SIAM J. Appl. Math., 38 (1980), 275–282. 1

[8] J. Chu and D. Franco, Non-collision periodic solutions of second order singular dynamical systems, J. Math. Anal. Appl., 344 (2008), 898–905. 1

[9] J. Chu and J.J. Nieto, Impulsive periodic solutions of first-order singular differential equa- tions, Bull. London Math. Soc., 40 (2008), 143–150. 1

[10] X. Du and Z. Zhao, Existence and uniqueness of positive solutions to a class of singular m-point boundary value problems, Appl. Math. Comput.,198(2008), 487–493. 1

[11] M. Fenga and W. Gea, Positive solutions for a class of m-point singular boundary value problems, Math. Comput. Modelling , 46 (2007), 375-383. 1

[12] J. Janus and J. Myjak, A generalized Emden-Fowler equation with a negative exponent, Nonlinear Anal., 23 (1994), 953–970. 1

[13] R. A. Khan, Positive solutions of four point singular boundary value problems, Appl. Math.

Comput., 201 (2008), 762–773. 1

[14] S. K. Ntouyas and P. K. Palamides, On Sturm-Liouville and Thomas-Fermi Singular Boundary Value Problems, Nonlinear Oscillations, 4 (2001), 326–344. 1

[15] A. Orpel, On the existence of bounded positive solutions for a class of singular BVPs, Nonlinear Anal., 69 (2008), 1389–1395. 1

[16] D. O’Regan, Singular differential equations with linear and nonlinear boundary conditions, Computers Math. Appl., 35 (1998), 81–97. 1

[17] J. V. Shin, A singular nonlinear differential equation arising in the Homann flow, J. Math.

Anal. Appl., 212 (1997) 443-451. 1

[18] E. Soewono, K. Vajravelu and R. N. Mohapatra, Existence and nonuniqueness of solutions of a singular nonlinear boundary layer problem, J. Math. Anal. Appl., 159 (1991), 251–270.

1

[19] G.C. Yang, Existence of solutions to the third-order nonlinear differential equations arising in boundary layer theory, Appl. Math. Lett., 6 (2003),827– 832. 1

[20] G.C. Yang, Positive solutions of singular Dirichlet boundary value problems with sign- changing nonlinearities, Comp. Math. Appl., 51 (2006), 1463–1470. 1, 1

[21] Z. Yong, Positive solutions of singular sublinear Emden-Fower boundary value problems, J. Math. Anal. Appl., 185 (1994), 215–222. 1

(10)

1

1 Centre for Advanced Mathematics and Physics, National University of Sci- ences and Technology, Campus of College of Electrical and Mechanical Engi- neering, Peshawar Road, Rawalpindi, Pakistan

E-mail address: rahmat

¯[email protected]

2 Centre for Advanced Mathematics and Physics, National University of Sci- ences and Technology, Campus of College of Electrical and Mechanical Engi- neering, Peshawar Road, Rawalpindi, Pakistan

E-mail address: [email protected]

参照

関連したドキュメント

Zhang, Positive solutions for boundary value problems of nonlinear fractional differential equation, Nonlinear Anal., 71 (2009), 5545–5550.. Zeddini, Existence and estimates of

Zhang, Solutions to boundary-value problems for nonlinear differ- ential equations of fractional order, Electronic Journal of Differential Equations, 2009(2009), No.. Yuan,

Yang; Existence and nonexistence of positive solutions of fourth order nonlinear boundary-value problems, Appl.. Yang; On a nonlinear boundary-value problem for fourth order

theorems, the author showed the existence of positive solutions for a class of singular four-point coupled boundary value problem of nonlinear semipositone Hadamard

Kiguradze, On some singular boundary value problems for nonlinear second order ordinary differential equations.. Kiguradze, On a singular multi-point boundary

We are interested in the existence of positive solutions to initial-value prob- lems for second-order nonlinear singular differential equations... We try to establish a more general

Leela, Existence of positive solutions for singular initial and boundary value problems via the classical upper and lower solution approach, Nonlinear Anal.. Wong, Positive Solutions

[10℄ Kang P., Wei Z., Three positive solutions of singular nonloal boundary value problems. for systems of nonlinear seond-order ordinary dierential equations,