Research Article Multiple Positive Solutions to Multipoint Boundary Value

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Hindawi Publishing Corporation
Journal of Applied Mathematics
Volume 2013, Article ID 679316, 12 pages
http://dx.doi.org/10.1155/2013/679316
Research Article
Multiple Positive Solutions to Multipoint Boundary Value
Problem for a System of Second-Order Nonlinear Semipositone
Differential Equations on Time Scales
Gang Wu,1,2 Longsuo Li,1 Xinrong Cong,1 and Xiufeng Miao1
1
2
Department of Mathematics, Harbin Institute of Technology, Harbin, Heilongjiang 150001, China
Basic Science, Harbin University of Commerce, Harbin, Heilongjiang 150076, China
Correspondence should be addressed to Longsuo Li; lilongsuo6982@126.com
Received 13 November 2012; Revised 31 January 2013; Accepted 31 January 2013
Academic Editor: Naseer Shahzad
Copyright © 2013 Gang Wu et al. 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 a system of second-order dynamic equations on time scales (𝑝1 𝑒1∇ )Δ (𝑑) − π‘ž1 (𝑑)𝑒1 (𝑑) + πœ†π‘“1 (𝑑, 𝑒1 (𝑑), 𝑒2 (𝑑)) = 0, 𝑑 ∈
(𝑑1 , 𝑑𝑛 ), (𝑝2 𝑒2∇ )Δ (𝑑) − π‘ž2 (𝑑)𝑒2 (𝑑) + πœ†π‘“2 (𝑑, 𝑒1 (𝑑), 𝑒2 (𝑑)) = 0, satisfying four kinds of different multipoint boundary value conditions, 𝑓𝑖 is
continuous and semipositone. We derive an interval of πœ† such that any πœ† lying in this interval, the semipositone coupled boundary
value problem has multiple positive solutions. The arguments are based upon fixed-point theorems in a cone.
𝑛−2
1. Introduction
𝛼1 𝑒1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) 𝑒1∇ (𝑑1 ) = ∑ π‘Žπ‘– 𝑒1 (𝑑𝑖 ) ,
In this paper, we consider the following dynamic equations
on time scales:
𝑖=2
𝛾1 𝑒1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) 𝑒1∇ (𝑑𝑛 ) = 0,
Δ
(𝑝1 𝑒1∇ ) (𝑑) − π‘ž1 (𝑑) 𝑒1 (𝑑) + πœ†π‘“1 (𝑑, 𝑒1 (𝑑) , 𝑒2 (𝑑)) = 0,
𝑑 ∈ (𝑑1 , 𝑑𝑛 ) , πœ† > 0,
𝑛−2
𝛼2 𝑒2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) 𝑒2∇ (𝑑1 ) = ∑ π‘Žπ‘– 𝑒2 (𝑑𝑖 ) ,
𝛾2 𝑒2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) 𝑒2∇ (𝑑𝑛 ) = 0,
Δ
𝛼1 𝑒1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) 𝑒1∇ (𝑑1 ) = 0,
satisfying one of the boundary value conditions
𝑛−2
𝛾1 𝑒1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) 𝑒1∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 𝑒1 (𝑑𝑖 ) ,
𝛼1 𝑒1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) 𝑒1∇ (𝑑1 ) = 0,
𝛾1 𝑒1 (𝑑𝑛 ) +
𝑖=2
(1)
(𝑝2 𝑒2∇ ) (𝑑) − π‘ž2 (𝑑) 𝑒2 (𝑑) + πœ†π‘“2 (𝑑, 𝑒1 (𝑑) , 𝑒2 (𝑑)) = 0,
𝛿1 𝑝1 (𝑑𝑛 ) 𝑒1∇
𝑖=2
𝑛−2
(𝑑𝑛 ) = ∑ 𝑏𝑖 𝑒1 (𝑑𝑖 ) ,
𝑖=2
𝛼2 𝑒2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) 𝑒2∇ (𝑑1 ) = 0,
𝑛−2
𝛾2 𝑒2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) 𝑒2∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 𝑒2 (𝑑𝑖 ) ,
𝑖=2
(3)
𝛼2 𝑒2 (𝑑1 ) −
(2)
𝛽2 𝑝2 (𝑑1 ) 𝑒2∇
𝑛−2
(𝑑1 ) = ∑ π‘Žπ‘– 𝑒2 (𝑑𝑖 ) ,
𝑖=2
𝛾2 𝑒2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) 𝑒2∇ (𝑑𝑛 ) = 0,
𝑛−2
𝛼1 𝑒1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) 𝑒1∇ (𝑑1 ) = ∑ π‘Žπ‘– 𝑒1 (𝑑𝑖 ) ,
𝑖=2
(4)
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Journal of Applied Mathematics
𝛾1 𝑒1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) 𝑒1∇ (𝑑𝑛 ) = 0,
existence of multiple positive solutions for the boundary
value problem on time scales.
In 2009, Topal and Yantir [3] studied the second-order
nonlinear π‘š-point boundary value problems
𝛼2 𝑒2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) 𝑒2∇ (𝑑1 ) = 0,
𝑛−2
𝛾2 𝑒2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) 𝑒2∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 𝑒2 (𝑑𝑖 ) ,
𝑖=2
(5)
𝑒Δ∇ (𝑑) + π‘Ž (𝑑) π‘’Δ (𝑑) + 𝑏 (𝑑) 𝑒 (𝑑)
+ πœ†π‘ž (𝑑) 𝑓 (𝑑, 𝑒 (𝑑)) = 0,
where
𝑝𝑖 , π‘žπ‘– : [𝑑1 , 𝑑𝑛 ] 󳨀→ (0, +∞)
Δ
with 𝑝𝑖 ∈ 𝐢 [𝑑1 , 𝑑𝑛 ) ,
𝑒 (𝜌 (0)) = 0,
π‘žπ‘– ∈ 𝐢 [𝑑1 , 𝑑𝑛 ]
for 𝑖 = 1, 2;
𝛼𝑖 , 𝛽𝑖 , 𝛾𝑖 , 𝛿𝑖 ∈ [0, +∞)
with 𝛼𝑖 𝛾𝑖 +𝛼𝑖 𝛿𝑖 +𝛽𝑖 𝛾𝑖 > 0
𝑒 (𝜎 (1)) = ∑ 𝛼𝑖 𝑒 (πœ‚π‘– ) ,
(6)
and 𝑓𝑖 is continuously and nonegative functionsquad, π‘Žπ‘– , 𝑏𝑖 ∈
[0, +∞) for 𝑖 ∈ {1, 2, . . . , 𝑛}; the points 𝑑𝑖 ∈ Tπœ…πœ… for 𝑖 ∈
{1, 2, . . . , 𝑛} with 𝑑1 < 𝑑2 < ⋅ ⋅ ⋅ < 𝑑𝑛 .
In the past few years, the boundary value problems of
dynamic equations on time scales have been studied by many
authors (see [1–19] and references). Recently, multipoint
boundary value problems on time scale have been studied,
for instance, see [1–12].
In 2006, Anderson and Ma [1] studied the second-order
multiple time-scale eigenvalue problem:
Δ
(𝑝𝑦∇ ) (𝑑) − π‘ž (𝑑) 𝑦 (𝑑) + πœ†β„Ž (𝑑) 𝑓 (𝑦) = 0,
𝑑 ∈ (𝑑1 , 𝑑𝑛 ) , πœ† > 0,
𝑛−2
(9)
π‘š−2
𝑖=1
for 𝑖 = 1, 2,
𝛼𝑦 (𝑑1 ) − 𝛽𝑝 (𝑑1 ) 𝑦∇ (𝑑1 ) = ∑ π‘Žπ‘– 𝑦 (𝑑𝑖 ) ,
𝑑 ∈ (0, 1)T ,
(7)
𝑖=2
where 𝛼𝑖 ≥ 0, 0 < πœ‚π‘– < πœ‚π‘–+1 < 1; for all 𝑖 = 1, 2, . . . , π‘š −
2; π‘Ž ∈ 𝐢([0, 1], [0, +∞)), 𝑏 ∈ 𝐢([0, 1], (−∞, 0]), 𝑓, π‘ž are
continuously and nonegative functions. The authors deal with
determining the value of πœ†, and the existences of multiple
positive solutions of the equation are obtained. In 2010, Yuan
and Liu [4] also study the second-order π‘š-point boundary
value problems; Yuan and Liu shows the existence of multiple
positive solutions if 𝑓 is semipositone and superlinear.
Motivated by the above results mentioned, we study the
second-order nonlinear π‘š-point boundary value problem (1)
with boundary condition (π‘˜), and nonlinear term may be
singularity and semipositone.
In this paper, the nonlinear term 𝑓𝑖 of (1) is suit to and
semipositone and the superlinear case, we shall prove our
two existence results for the problem (1) with (π‘˜) by using
a nonlinear alternative of Leray-Schauder type and Krasnosel’skii fixed-point theorem. This paper is organized as
follows. In Section 2, we start with some preliminary lemmas.
In Section 3, we give the main result which state the sufficient
conditions for (1) with π‘š-point boundary value (π‘˜) to have
existence of positive solutions (π‘˜ = 2, . . . , 5).
𝑛−2
𝛾𝑦 (𝑑𝑛 ) + 𝛿𝑝 (𝑑𝑛 ) 𝑦∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 𝑦 (𝑑𝑖 ) ,
2. Preliminaries
𝑖=2
where the functions 𝑓 : [0, +∞) → [0, +∞) and β„Ž :
[𝑑1 , 𝑑𝑛 ] → [0, +∞) are continuous. The authors discuss conditions for the existence of at least one positive solution to
the second-order Sturm-Liouville-type multiple eigenvalue
problem on time scales.
In 2009, Feng et al. [2] studied
Δ
(𝑝𝑦∇ ) (𝑑) − π‘ž (𝑑) 𝑦 (𝑑) = 𝑓 (𝑑, 𝑦) ,
𝑑 ∈ (𝑑1 , 𝑑𝑛 ) ,
∇
𝑛−2
𝛼𝑦 (𝑑1 ) − 𝛽𝑝 (𝑑1 ) 𝑦 (𝑑1 ) = ∑ π‘Žπ‘– 𝑦 (𝑑𝑖 ) ,
In this section, we state the preliminary information that we
need to prove the main results.
In this paper, for our constructions, we shall consider the
Banach space 𝐸 = 𝐢[𝜌(𝑑1 ), 𝑑𝑛 ] equipped with standard norm
β€–π‘₯β€– = max𝜌(𝑑1 )≤𝑑≤𝑑𝑛 |π‘₯(𝑑)|, π‘₯ ∈ 𝐸; for each (π‘₯, 𝑦) ∈ 𝐸 × πΈ, we
write ||(π‘₯, 𝑦)||1 = ||π‘₯||+||𝑦||. Clearly, (𝐸×𝐸, ||⋅||1 ) is a Banach
space. Denote by πœ™π‘–1 and πœ™π‘–2 (𝑖 = 1, 2), the solutions of the
equation
Δ
(8)
(𝑝𝑖 𝑒𝑖∇ ) (𝑑) − π‘žπ‘– (𝑑) 𝑒𝑖 (𝑑) = 0,
𝑑 ∈ [𝑑1 , 𝑑𝑛 ) ,
(10)
𝑖=2
∇
𝑛−2
under the initial conditions
𝛾𝑦 (𝑑𝑛 ) + 𝛿𝑝 (𝑑𝑛 ) 𝑦 (𝑑𝑛 ) = ∑ 𝑏𝑖 𝑦 (𝑑𝑖 ) ,
𝑖=2
∑𝑛𝑗=1 𝑐𝑗 (𝑑)𝑦V𝑗 , 𝑐𝑗
where the functions 𝑓(𝑑, 𝑦) =
∈ 𝐢([𝑑1 , 𝑑𝑛 ],
[0, ∞)), V𝑖 ∈ [0, ∞), 𝑗 = 1, 2, . . . , 𝑛. This paper shows the
𝑒𝑖 (𝑑1 ) = 𝛽𝑖 ,
𝑝𝑖 (𝑑1 ) 𝑒𝑖∇ (𝑑1 ) = 𝛼𝑖 ,
𝑒𝑖 (𝑑𝑛 ) = 𝛿𝑖 ,
𝑝𝑖 (𝑑𝑛 ) 𝑒𝑖∇ (𝑑𝑛 ) = −𝛾𝑖 ,
(11)
Journal of Applied Mathematics
3
respectively. So that πœ™π‘–1 and πœ™π‘–2 (𝑖 = 1, 2) satisfy
∇ Δ
(𝑝𝑖 πœ™π‘–1
)
𝐻14 (𝑑, 𝑠)
= 𝐺1 (𝑑, 𝑠) +
(𝑑) − π‘žπ‘– (𝑑) πœ™π‘–1 (𝑑) = 0,
𝑑 ∈ [𝑑1 , 𝑑𝑛 ) ,
πœ™π‘–1 (𝑑1 ) = 𝛽𝑖 ,
∇
𝑝𝑖 (𝑑1 ) πœ™π‘–1
(𝑑1 ) = 𝛼𝑖 ,
(12)
Δ
1
𝑛−1
1
𝑛−1
∑ 𝑏𝑖 𝐺1 (𝑑𝑖 , 𝑠) πœ™11 (𝑑)
𝑑1 − ∑𝑛−1
𝑗=2 𝑏𝑖 πœ™11 (𝑑𝑖 ) 𝑗=2
𝐻24 (𝑑, 𝑠)
= 𝐺2 (𝑑, 𝑠) +
πœ™π‘–2 (𝑑𝑛 ) = 𝛿𝑖 ,
∑ π‘Žπ‘– 𝐺2 (𝑑𝑖 , 𝑠) πœ™22 (𝑑)
𝑑2 − ∑𝑛−1
𝑗=2 π‘Žπ‘– πœ™22 (𝑑𝑖 ) 𝑗=2
= 𝐻23 (𝑑, 𝑠) ,
∇
𝑝𝑖 (𝑑𝑛 ) πœ™π‘–2
(𝑑𝑛 ) = −𝛾𝑖 ,
𝐻15 (𝑑, 𝑠)
∇
respectively. For 𝑖 = 1, 2, set 𝑑𝑖 = 𝛼𝑖 πœ™π‘–2 (𝑑1 ) − 𝛽𝑖 𝑝𝑖 (𝑑1 )πœ™π‘–2
(𝑑1 ) =
∇
𝛾𝑖 πœ™π‘–1 (𝑑𝑛 ) + 𝛿𝑖 𝑝𝑖 (𝑑𝑛 )πœ™π‘–1 (𝑑𝑛 ), the Green’s function of the corresponding homogeneous boundary value problem is defined
by
= 𝐺1 (𝑑, 𝑠) +
𝑑1 −
∑𝑛−1
𝑗=2 π‘Žπ‘– πœ™12
∑ π‘Žπ‘– 𝐺1 (𝑑𝑖 , 𝑠) πœ™12 (𝑑)
(𝑑𝑖 ) 𝑗=2
= 𝐻13 (𝑑, 𝑠) ,
𝐻25 (𝑑, 𝑠)
𝐺𝑖 (𝑑, 𝑠)
=
𝑛−1
= 𝐻12 (𝑑, 𝑠) ,
∇
(𝑝𝑖 πœ™π‘–2
) (𝑑) − π‘žπ‘– (𝑑) πœ™π‘–2 (𝑑) = 0,
𝑑 ∈ [𝑑1 , 𝑑𝑛 ) ,
1
1 πœ™π‘–2 (𝑑) πœ™π‘–1 (𝑠) ,
{
𝑑𝑖 πœ™π‘–1 (𝑑) πœ™π‘–2 (𝑠) ,
𝜌 (𝑑1 ) ≤ 𝑠 ≤ 𝑑 ≤ 𝑑𝑛 ,
𝜌 (𝑑1 ) ≤ 𝑑 ≤ 𝑠 ≤ 𝑑𝑛 ,
for 𝑖 = 1, 2.
(13)
= 𝐺2 (𝑑, 𝑠) +
1
𝑛−1
∑ 𝑏𝑖 𝐺2 (𝑑𝑖 , 𝑠) πœ™21 (𝑑)
𝑑2 − ∑𝑛−1
𝑗=2 𝑏𝑖 πœ™21 (𝑑𝑖 ) 𝑗=2
= 𝐻22 (𝑑, 𝑠) .
(16)
From Lemmas 3.1 and 3.3 in [1], we have the following lemma.
Lemma 1. If 𝑑𝑖 =ΜΈ 0, (𝑒1 , 𝑒2 ) is a solution of (1) with boundary
value condition (π‘˜) if only and if
𝑑𝑛
𝑒1 (𝑑) = πœ† ∫ 𝐻1π‘˜ (𝑑, 𝑠) 𝑓1 (𝑠, 𝑒1 (𝑠) , 𝑒2 (𝑠)) Δ𝑠,
𝑑1
(14)
For the rest of the paper, we need the following assumption:
𝑛−1
𝑛−1
𝑗=2
𝑗=2
0 < ∑ 𝑏𝑗 πœ™π‘–1 (𝑑𝑗 ) ,
∑ π‘Žπ‘— πœ™π‘–2 (𝑑𝑗 ) < 𝑑𝑖 ,
for 𝑖 = 1, 2.
(C)
𝑑 ∈ [𝜌 (𝑑1 ) , 𝑑𝑛 ] ,
𝑑𝑛
𝑒2 (𝑑) = πœ† ∫ 𝐻2π‘˜ (𝑑, 𝑠) 𝑓2 (𝑠, 𝑒1 (𝑠) , 𝑒2 (𝑠)) Δ𝑠,
𝑑1
(15)
From πœ™π‘–1 is nondecreasing on [𝜌(𝑑1 ), 𝑑𝑛 ], πœ™π‘–2 is nonincreasing on [𝜌(𝑑1 ), 𝑑𝑛 ] (see [2, Proposition 2.3]), it is easy to verify
the following inequalities:
where π‘˜ = 2, . . . , 5, and
𝑑𝑖 𝐺𝑖 (𝑑, 𝑠) ≤ πœ™π‘–1 (𝑑) πœ™π‘–2 (𝑑) ,
𝐻𝑖2 (𝑑, 𝑠)
= 𝐺𝑖 (𝑑, 𝑠) +
𝑑𝑖 𝐺𝑖 (𝑑, 𝑠) ≤ πœ™π‘–1 (𝑠) πœ™π‘–2 (𝑠) ,
1
𝑑𝑖 −
∑𝑛−1
𝑗=2 𝑏𝑗 πœ™π‘–1
𝑛−1
∑ 𝑏𝑗 𝐺𝑖 (𝑑𝑗 , 𝑠) πœ™π‘–1 (𝑑) ,
(𝑑𝑗 ) 𝑗=2
(𝑖 = 1, 2) ,
𝐻𝑖3 (𝑑, 𝑠)
= 𝐺𝑖 (𝑑, 𝑠) +
1
𝑛−1
∑ π‘Žπ‘— 𝐺𝑖 (𝑑𝑗 , 𝑠) πœ™π‘–2 (𝑑) ,
𝑑𝑖 − ∑𝑛−1
𝑗=2 π‘Žπ‘— πœ™π‘–2 (𝑑𝑗 ) 𝑗=2
(𝑖 = 1, 2) ,
(17)
1
𝑑𝑖 𝐺𝑖 (𝑑, 𝑠) ≥ σ΅„©σ΅„© σ΅„©σ΅„© σ΅„©σ΅„© σ΅„©σ΅„© πœ™π‘–1 (𝑑) πœ™π‘–2 (𝑑) πœ™π‘–1 (𝑠) πœ™π‘–2 (𝑠) .
σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„© σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©
Lemma 2. The Green’s function 𝐺𝑖 (𝑑, 𝑠) has properties
𝐺𝑖 (𝑑, 𝑠) ≤ 𝐺𝑖 (𝑑, 𝑑) ,
𝑑𝑖
σ΅„©σ΅„© σ΅„©σ΅„© σ΅„©σ΅„© σ΅„©σ΅„© 𝐺𝑖 (𝑑, 𝑑) 𝐺𝑖 (𝑠, 𝑠) ≤ 𝐺𝑖 (𝑑, 𝑠) ≤ 𝐺𝑖 (𝑠, 𝑠) .
σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„© σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©
(18)
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Journal of Applied Mathematics
Lemma 3. For π»π‘–π‘˜ (𝑑, 𝑠), π‘˜ = 2, . . . , 5 and 𝑖 = 1, 2, one has the
conclusions π»π‘–π‘˜ (𝑑, 𝑠) ≤ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) and
𝑐∗ πœ™π‘–1 (𝑑) 𝐺𝑖 (𝑠, 𝑠) ≤ 𝐻𝑖2 (𝑑, 𝑠) ≤ 𝐢∗ πœ™π‘–1 (𝑑) ,
(𝑖 = 1, 2) ,
𝑐∗ πœ™π‘–2 (𝑑) 𝐺𝑖 (𝑠, 𝑠) ≤ 𝐻𝑖3 (𝑑, 𝑠) ≤ 𝐢∗ πœ™π‘–2 (𝑑) ,
(𝑖 = 1, 2) ,
∗
𝑐∗ πœ™π‘–π‘– (𝑑) 𝐺1 (𝑠, 𝑠) ≤ 𝐻𝑖4 (𝑑, 𝑠) ≤ 𝐢 πœ™π‘–π‘– (𝑑) ,
𝑛−1
1
𝑑𝑖 −
≤
∑𝑛−1
𝑗=2 π‘Žπ‘— πœ™π‘–2
∑ π‘Žπ‘— 𝐺𝑖 (𝑑𝑗 , 𝑠) πœ™π‘–2 (𝑑)
(𝑑𝑗 ) 𝑗=2
𝑛−1
1
σ΅„© σ΅„©
∑ π‘Žπ‘— 𝐺𝑖 (𝑠, 𝑠) σ΅„©σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©σ΅„© ,
𝑑𝑖 − ∑𝑛−1
π‘Ž
πœ™
(𝑑
)
𝑗=2 𝑗 𝑖2 𝑗 𝑗=2
(21)
(𝑖 = 1, 2) , (19)
𝑐∗ πœ™12 (𝑑) 𝐺1 (𝑠, 𝑠) ≤ 𝐻15 (𝑑, 𝑠) ≤ 𝐢∗ πœ™12 (𝑑) ,
we have
𝑐∗ πœ™21 (𝑑) 𝐺1 (𝑠, 𝑠) ≤ 𝐻25 (𝑑, 𝑠) ≤ 𝐢∗ πœ™21 (𝑑) ,
π»π‘–π‘˜ (𝑑, 𝑠) ≤ 𝐢1 𝐺𝑖 (𝑠, 𝑠) ≤ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) .
∗
where 𝐢 = 𝐢1 + 𝐢2 and
For π‘˜ = 2 or 3, we have
σ΅„©σ΅„© σ΅„©σ΅„©
𝑛−1
{
σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„©
𝐢1 = max {1 +
∑ 𝑏𝑗
𝑛−1
𝑖=1,2
𝑑𝑖 − ∑𝑗=2 𝑏𝑗 πœ™π‘–1 (𝑑𝑗 ) 𝑖=1
{
+
σ΅„©
σ΅„©σ΅„©
σ΅„©πœ™ (𝑑)σ΅„©σ΅„©
1
𝐻𝑖2 (𝑑, 𝑠) ≤ σ΅„© 𝑖2 σ΅„© πœ™π‘–1 (𝑑) +
𝑛−1
𝑑𝑖
𝑑𝑖 − ∑𝑗=2 𝑏𝑖 πœ™π‘–1 (𝑑𝑖 )
σ΅„©σ΅„© σ΅„©σ΅„©
𝑛−1 }
σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©
∑ π‘Žπ‘— } ,
𝑑𝑖 − ∑𝑛−1
𝑗=2 π‘Žπ‘— πœ™π‘–2 (𝑑𝑗 ) 𝑗=2 }
𝑛−1
× ∑ 𝑏𝑗 𝐺𝑖 (𝑑𝑗 , 𝑑𝑗 ) πœ™π‘–1 (𝑑)
𝑗=2
{ σ΅„©σ΅„©σ΅„©πœ™ σ΅„©σ΅„©σ΅„© + σ΅„©σ΅„©σ΅„©πœ™ σ΅„©σ΅„©σ΅„©
1
𝐢2 = max { σ΅„© 𝑖1 σ΅„© σ΅„© 𝑖2 σ΅„© +
𝑛−1
𝑖=1,2
𝑑𝑖
𝑑𝑖 − ∑𝑗=2 𝑏𝑗 πœ™π‘–1 (𝑑𝑗 )
{
𝑛−1
× ∑ 𝑏𝑗 𝐺𝑖 (𝑑𝑗 , 𝑑𝑗 ) +
𝑗=2
≤ 𝐢∗ πœ™π‘–1 (𝑑) ,
σ΅„©
σ΅„©σ΅„©
σ΅„©πœ™ (𝑑)σ΅„©σ΅„©
1
𝐻𝑖3 (𝑑, 𝑠) ≤ σ΅„© 𝑖1 σ΅„© πœ™π‘–2 (𝑑) +
𝑛−1
𝑑𝑖
𝑑𝑖 − ∑𝑗=2 π‘Žπ‘– πœ™π‘–2 (𝑑𝑖 )
1
𝑑𝑖 −
∑𝑛−1
𝑗=2 𝑏𝑗 πœ™π‘–2
(𝑑𝑗 )
𝑛−1
}
× ∑ π‘Žπ‘— 𝐺2 (𝑑𝑗 , 𝑑𝑗 )} ,
𝑗=2
}
{
𝑑
1
𝑐∗ = min { σ΅„©σ΅„© σ΅„©σ΅„© 󡄩󡄩𝑖 σ΅„©σ΅„©
σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„© σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„© 𝑑𝑖 − ∑𝑛−1
𝑗=2 𝑏𝑗 πœ™π‘–1 (𝑑𝑗 )
{
𝑛−1
× ∑ π‘Žπ‘— 𝐺𝑖 (𝑑𝑗 , 𝑑𝑗 ) πœ™π‘–2 (𝑑)
𝑗=2
(20)
≤ 𝐢∗ πœ™π‘–2 (𝑑) ,
𝐻𝑖2 (𝑑, 𝑠) ≥
𝑗=2
𝑗=2
≥
1
𝑑𝑖 −
≤
∑𝑛−1
𝑗=2 𝑏𝑗 πœ™π‘–1
1
𝑑𝑖 −
∑𝑛−1
𝑗=2 𝑏𝑗 πœ™π‘–1
(𝑑𝑗 )
𝑛−1
𝑑
× ∑ 𝑏𝑗 σ΅„©σ΅„© σ΅„©σ΅„© 󡄩󡄩𝑖 σ΅„©σ΅„© 𝐺𝑖 (𝑑𝑗 , 𝑑𝑗 ) 𝐺𝑖 (𝑠, 𝑠) πœ™π‘–1 (𝑑)
σ΅„©πœ™1 σ΅„©σ΅„© σ΅„©σ΅„©πœ™2 σ΅„©σ΅„©
𝑗=2 σ΅„©
𝑛−1
Proof. From Lemma 2 and
(𝑑𝑗 )
× ∑ 𝑏𝑗 𝐺𝑖 (𝑑𝑗 , 𝑠) πœ™π‘–1 (𝑑)
× ∑ 𝑏𝑗 𝐺𝑖 (𝑑𝑗 , 𝑑𝑗 ) ,
}
× ∑ π‘Žπ‘— 𝐺𝑖 (𝑑𝑗 , 𝑑𝑗 ) ; 𝑖 = 1, 2} .
𝑗=2
}
𝑑𝑖 −
𝑛−1
𝑛−1
𝑑𝑖
1
σ΅„©σ΅„© σ΅„©σ΅„© σ΅„©σ΅„© σ΅„©σ΅„©
σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„© σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„© 𝑑𝑖 − ∑𝑛−1
𝑗=2 π‘Žπ‘— πœ™π‘–2 (𝑑𝑗 )
1
∑𝑛−1
𝑗=2 𝑏𝑗 πœ™π‘–1
≥ 𝑐∗ πœ™π‘–1 (𝑑) 𝐺𝑖 (𝑠, 𝑠) ,
𝐻𝑖3 (𝑑, 𝑠) ≥
𝑛−1
1
𝑑𝑖 −
∑𝑛−1
𝑗=2 π‘Žπ‘— πœ™π‘–2
(𝑑𝑗 )
𝑛−1
∑ 𝑏𝑗 𝐺𝑖 (𝑑𝑗 , 𝑠) πœ™π‘–1 (𝑑)
× ∑ π‘Žπ‘— 𝐺𝑖 (𝑑𝑗 , 𝑠) πœ™π‘–2 (𝑑)
(𝑑𝑗 ) 𝑗=2
𝑗=2
𝑛−1
1
σ΅„© σ΅„©
∑ 𝑏𝑗 𝐺𝑖 (𝑠, 𝑠) σ΅„©σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„©σ΅„© ,
𝑑𝑖 − ∑𝑛−1
𝑏
πœ™
(𝑑
)
𝑗=2 𝑗 𝑖1 𝑗 𝑗=2
≥
1
𝑑𝑖 − ∑𝑛−1
𝑗=2 π‘Žπ‘— πœ™π‘–1 (𝑑𝑗 )
(22)
Journal of Applied Mathematics
5
𝑛−1
𝑑
× ∑ π‘Žπ‘— σ΅„©σ΅„© σ΅„©σ΅„© 󡄩󡄩𝑖 σ΅„©σ΅„© 𝐺𝑖 (𝑑𝑗 , 𝑑𝑗 ) 𝐺𝑖 (𝑠, 𝑠) πœ™π‘–2 (𝑑)
πœ™
σ΅„©
σ΅„©
σ΅„©πœ™2 σ΅„©σ΅„©
𝑗=2 σ΅„© 1 σ΅„© σ΅„©
⊂
(𝑑1 , 𝑑𝑛 ) such that
(H3 ) There exists [πœƒ1 , πœƒ2 ]
lim𝑒1 +𝑒2 ↑+∞ min𝑑∈[πœƒ1 ,πœƒ2 ] (𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 )/(𝑒1 + 𝑒2 )) =
+∞ (𝑖 = 1, 2).
≥ 𝑐∗ πœ™π‘–2 (𝑑) 𝐺𝑖 (𝑠, 𝑠) .
(23)
So, we have
𝑐∗ πœ™π‘–1 (𝑑) 𝐺𝑖 (𝑠, 𝑠) ≤ 𝐻𝑖2 (𝑑, 𝑠) ≤ 𝐢∗ πœ™π‘–1 (𝑑) ,
(𝑖 = 1, 2) ,
𝑐∗ πœ™π‘–2 (𝑑) 𝐺𝑖 (𝑠, 𝑠) ≤ 𝐻𝑖3 (𝑑, 𝑠) ≤ 𝐢∗ πœ™π‘–2 (𝑑) ,
(𝑖 = 1, 2) .
(24)
Since 𝐻14 (𝑑, 𝑠) = 𝐻12 (𝑑, 𝑠), 𝐻24 (𝑑, 𝑠) = 𝐻23 (𝑑, 𝑠), 𝐻15 (𝑑,
𝑠) = 𝐻13 (𝑑, 𝑠), 𝐻25 (𝑑, 𝑠) = 𝐻22 (𝑑, 𝑠), then we also have
𝑑
𝑑
(H4 ) ∫𝑑 𝑛 𝐺𝑖 (𝑠, 𝑠)𝑔(𝑠)∇𝑠 < +∞ and ∫𝑑 𝑛 𝐺𝑖 (𝑠, 𝑠)𝑓𝑖 (𝑠, 𝑧1 ,
1
1
𝑧2 )∇𝑠 < +∞ for any 𝑧𝑖 ∈ [0, π‘š], π‘š > 0 is any constant
(𝑖 = 1, 2).
In fact, we only consider the system
Δ
∗
(𝑝1 π‘₯1∇ ) (𝑑) − π‘ž1 (𝑑) π‘₯1 (𝑑) + πœ† (𝑓1 (𝑑, [π‘₯1 (𝑑) − V1π‘˜ (𝑑)] ,
𝑐∗ πœ™11 (𝑑) 𝐺1 (𝑠, 𝑠) ≤ 𝐻14 (𝑑, 𝑠) = 𝐻12 (𝑑, 𝑠) ≤ 𝐢∗ πœ™11 (𝑑) ,
𝑐∗ πœ™22 (𝑑) 𝐺1 (𝑠, 𝑠) ≤ 𝐻24 (𝑑, 𝑠) = 𝐻23 (𝑑, 𝑠) ≤ 𝐢∗ πœ™22 (𝑑) ,
𝑐∗ πœ™12 (𝑑) 𝐺1 (𝑠, 𝑠) ≤ 𝐻15 (𝑑, 𝑠) = 𝐻13 (𝑑, 𝑠) ≤ 𝐢∗ πœ™12 (𝑑) ,
∗
[π‘₯2 (𝑑) − V2π‘˜ (𝑑)] )
(25)
+𝑔 (𝑑) ) = 0,
𝑐∗ πœ™21 (𝑑) 𝐺1 (𝑠, 𝑠) ≤ 𝐻25 (𝑑, 𝑠) = 𝐻22 (𝑑, 𝑠) ≤ 𝐢∗ πœ™21 (𝑑) .
The proof is complete.
πœ† > 0,
Δ
The following theorems will play a major role in our next
analysis.
∗
(𝑝2 π‘₯2∇ ) (𝑑) − π‘ž2 (𝑑) π‘₯2 (𝑑) + πœ† (𝑓2 (𝑑, [π‘₯1 (𝑑) − V1π‘˜ (𝑑)] ,
∗
[π‘₯2 (𝑑) − V2π‘˜ (𝑑)] )
Theorem 4 (see [20]). Let 𝑋 be a Banach space, and Ω ⊂ 𝑋
closed and convex. Assume π‘ˆ is a relatively open subset of Ω
with 0 ∈ π‘ˆ, and let 𝑆 : π‘ˆ → Ω be a compact, continuous
map. Then either
+𝑔 (𝑑) ) = 0,
πœ† > 0,
(1) 𝑆 has a fixed point in π‘ˆ, or
(26)
(2) there exists 𝑒 ∈ πœ•π‘ˆ and ] ∈ (0, 1), with 𝑒 = ]𝑆𝑒.
Theorem 5 (see [21]). Let 𝑋 be a Banach space, and let 𝑃 ⊂ 𝑋
be a cone in 𝑋. Let Ω1 , Ω2 be bounded open subsets of 𝑋 with
0 ∈ Ω1 ⊂ Ω1 ⊂ Ω2 , and let 𝑆 : 𝑃 → 𝑃 be a completely continuous operator such that, either
(1) ‖𝑆𝑀‖ ≤ ‖𝑀‖, 𝑀 ∈ 𝑃 ∩ πœ•Ω1 , ‖𝑆𝑀‖ ≥ ‖𝑀‖, 𝑀 ∈ 𝑃 ∩ πœ•Ω2 ,
or
(2) ‖𝑆𝑀‖ ≥ ‖𝑀‖, 𝑀 ∈ 𝑃 ∩ πœ•Ω1 , ‖𝑆𝑀‖ ≤ ‖𝑀‖, 𝑀 ∈ 𝑃 ∩ πœ•Ω2 .
Then 𝑆 has a fixed point in 𝑃 ∩ Ω2 \ Ω1 .
𝛼1 π‘₯1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) π‘₯1∇ (𝑑1 ) = 0,
𝑛−2
𝛾1 π‘₯1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) π‘₯1∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 π‘₯1 (πœ‚π‘– ) ,
𝑖=2
𝛼2 π‘₯2 (𝑑1 ) −
𝛽2 𝑝2 (𝑑1 ) π‘₯2∇
(𝑑1 ) = 0,
𝑛−2
𝛾2 π‘₯2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) π‘₯2∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 π‘₯2 (πœ‚π‘– ) ,
3. Main Results
𝑖=2
𝑛−2
We make the following assumptions:
(H1 ) 𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 ) ∈ 𝐢([𝑑1 , 𝑑𝑛 ] × [0, +∞)2 , (−∞, +∞)), moreover there exists a function 𝑔(𝑑) ∈ 𝐿1 ([𝑑1 , 𝑑𝑛 ], (0,
+∞)) such that 𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 ) ≥ −𝑔(𝑑), for any 𝑑 ∈
(𝑑1 , 𝑑𝑛 ), 𝑒𝑖 ∈ [0, +∞), 𝑖 = 1, 2.
(H∗1 )
with one of the boundary value conditions
2
𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 ) ∈ 𝐢((𝑑1 , 𝑑𝑛 ) × [0, +∞) , (−∞, +∞)) may
be singular at 𝑑 = 𝑑1 , 𝑑𝑛 ; moreover, there exists a function 𝑔(𝑑) ∈ 𝐿1 ((𝑑1 , 𝑑𝑛 ), (0, +∞)) such that 𝑓𝑖 (𝑑, 𝑒1 ,
𝑒2 ) ≥ −𝑔(𝑑), for any 𝑑 ∈ (𝑑1 , 𝑑𝑛 ), 𝑒𝑖 ∈ [0, +∞).
(H2 ) 𝑓𝑖 (𝑑, 0, 0) > 0, for 𝑑 ∈ [𝑑1 , 𝑑𝑛 ] (𝑖 = 1, 2).
𝛼1 π‘₯1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) π‘₯1∇ (𝑑1 ) = ∑ π‘Žπ‘– π‘₯1 (πœ‚π‘– ) ,
𝑖=2
𝛾1 π‘₯1 (𝑑𝑛 ) +
𝛿1 𝑝1 (𝑑𝑛 ) π‘₯1∇
(𝑑𝑛 ) = 0,
𝑛−2
𝛼2 π‘₯2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) π‘₯2∇ (𝑑1 ) = ∑ π‘Žπ‘– π‘₯2 (πœ‚π‘– ) ,
𝑖=2
𝛾2 π‘₯2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) π‘₯2∇ (𝑑𝑛 ) = 0,
𝛼1 π‘₯1 (𝑑1 )−𝛽1 𝑝1 (𝑑1 ) π‘₯1∇ (𝑑1 ) = 0,
6
Journal of Applied Mathematics
𝑛−2
𝑛−2
𝛾1 π‘₯1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) π‘₯1∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 π‘₯1 (πœ‚π‘– ) ,
𝛼1 V1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) V1∇ (𝑑1 ) = ∑ π‘Žπ‘– V1 (πœ‚π‘– ) ,
𝑖=2
𝑖=2
𝛾1 V1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) V1∇ (𝑑𝑛 ) = 0,
𝑛−2
𝛼2 π‘₯2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) π‘₯2∇ (𝑑1 ) = ∑ π‘Žπ‘– π‘₯2 (πœ‚π‘– ) ,
𝑖=2
𝑛−2
𝛼2 V2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) V2∇ (𝑑1 ) = ∑ π‘Žπ‘– V2 (πœ‚π‘– ) ,
𝛾2 π‘₯2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) π‘₯2∇ (𝑑𝑛 ) = 0,
𝑖=2
𝑛−2
𝛾2 V2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) V2∇ (𝑑𝑛 ) = 0,
𝑖=2
𝛼1 V1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) V1∇ (𝑑1 ) = 0,
𝛼1 π‘₯1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) π‘₯1∇ (𝑑1 ) = ∑ π‘Žπ‘– π‘₯1 (πœ‚π‘– ) ,
𝛾1 π‘₯1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) π‘₯1∇ (𝑑𝑛 ) = 0,
𝛼2 π‘₯2 (𝑑1 ) −
𝛽2 𝑝2 (𝑑1 ) π‘₯2∇
𝑛−2
𝛾1 V1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) V1∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 V1 (πœ‚π‘– ) ,
(𝑑1 ) = 0,
𝑖=2
𝑛−2
𝑛−2
𝛾2 π‘₯2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) π‘₯2∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 π‘₯2 (πœ‚π‘– ) ,
𝛼2 V2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) V2∇ (𝑑1 ) = ∑ π‘Žπ‘– V2 (πœ‚π‘– ) ,
𝑖=2
𝑖=2
(27)
𝛾2 V2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) V2∇ (𝑑𝑛 ) = 0,
𝑛−2
𝛼1 V1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) π‘₯1∇ (𝑑1 ) = ∑ π‘Žπ‘– V1 (πœ‚π‘– ) ,
where
𝑖=2
𝛾1 V1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) π‘₯1∇ (𝑑𝑛 ) = 0,
𝑦 (𝑑) , 𝑦 (𝑑) ≥ 0,
𝑦(𝑑)∗ = {
0,
𝑦 (𝑑) < 0,
𝛼2 V2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) π‘₯2∇ (𝑑1 ) = 0,
(28)
𝑛−2
𝛾2 V2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) π‘₯2∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 V2 (πœ‚π‘– ) .
𝑖=2
𝑑
and Vπ‘–π‘˜ (𝑑) = πœ† ∫𝑑 𝑛 π»π‘–π‘˜ (𝑑, 𝑠)𝑔(𝑠)Δ𝑠. For π‘˜ = 2, . . . , 5, from
1
Lemma 1, (V1π‘˜ (𝑑), V2π‘˜ (𝑑)) is the solution of the equation
Δ
(𝑝1 V1∇ ) (𝑑) − π‘ž1 (𝑑) V1 (𝑑) + πœ†π‘” (𝑑) = 0,
πœ† > 0, 𝑑1 < 𝑑 < 𝑑𝑛 ,
Δ
(𝑝2 V2∇ ) (𝑑) − π‘ž2 (𝑑) V2 (𝑑) + πœ†π‘” (𝑑) = 0,
(29)
πœ† > 0,
(30)
We will show that there exists a solution (π‘₯1π‘˜ , π‘₯2π‘˜ ) to the
boundary value problem (π‘˜) of the system (26) with π‘₯π‘–π‘˜ (𝑑) ≥
Vπ‘–π‘˜ (𝑑), 𝑑 ∈ [𝜌(𝑑1 ), 𝑑𝑛 ]. If this is true, then π‘’π‘–π‘˜ (𝑑) = π‘₯π‘–π‘˜ (𝑑) − Vπ‘–π‘˜ (𝑑)
is a nonnegative solution (positive on (𝜌(𝑑1 ), 𝑑𝑛 )) of the system
(1) with the boundary value problem (π‘˜), (where 𝑖 = 1, 2; π‘˜ =
2, . . . , 5, π‘˜ = π‘˜ + 11). Since for any 𝑑 ∈ (𝑑1 , 𝑑𝑛 ), from
Δ
∇
∇
) (𝑑) − π‘žπ‘– (𝑑) π‘₯π‘–π‘˜
(𝑝𝑖 π‘₯π‘–π‘˜
(𝑑)
∇ Δ
∇
= (𝑝𝑖 (π‘’π‘–π‘˜ + Vπ‘–π‘˜ ) ) (𝑑) − π‘žπ‘– (𝑑) (π‘’π‘–π‘˜ + Vπ‘–π‘˜ ) (𝑑)
respectively, satisfying the following boundary value conditions:
∗
∗
= −πœ† (𝑓𝑖 (𝑑, [π‘₯1π‘˜ (𝑑)−V1π‘˜ (𝑑)] , [π‘₯2π‘˜ (𝑑)−V2π‘˜ (𝑑)] )+𝑔 (𝑑))
= −πœ† (𝑓𝑖 (𝑑, 𝑒1π‘˜ (𝑑) , 𝑒2π‘˜ (𝑑)) + 𝑔 (𝑑)) ,
(31)
𝛼1 V1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) V1∇ (𝑑1 ) = 0,
𝑛−2
𝛾1 V1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) V1∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 V1 (πœ‚π‘– ) ,
𝑖=2
𝛼2 V2 (𝑑1 ) −
𝛽2 𝑝2 (𝑑1 ) V2∇
(𝑑1 ) = 0,
𝑛−2
𝛾2 V2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) V2∇ (𝑑𝑛 ) = ∑ 𝑏𝑖 V2 (πœ‚π‘– ) ,
𝑖=2
we have
Δ
∇
) (𝑑) − π‘žπ‘– (𝑑) π‘’π‘–π‘˜ (𝑑) = −πœ†π‘“π‘– (𝑑, 𝑒1π‘˜ (𝑑) , 𝑒2π‘˜ (𝑑)) . (32)
(𝑝𝑖 π‘’π‘–π‘˜
As a result, we will concentrate our study on (26) with the
boundary value problem (π‘˜).
Journal of Applied Mathematics
7
Employing Lemma 1, we note that (π‘₯1π‘˜ (𝑑), π‘₯2π‘˜ (𝑑)) is a
solution of the system (26) with boundary value (π‘˜) if and
only if
𝑑𝑛
For π‘˜ = 2, . . . , 5, from (35) and Lemma 3, we have
π‘‡π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ )(𝑑) ≥ 0 on [0, 1], for (π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ 𝑃𝑖𝑗 × π‘ƒπ‘šπ‘› , we
have
π‘‡π‘–π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ) (𝑑)
∗
π‘₯1π‘˜ (𝑑) = πœ† ∫ 𝐻1π‘˜ (𝑑, 𝑠) (𝑓1 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
𝑑𝑛
𝑑1
∗
= πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
𝑑1
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] )
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] )
+𝑔 (𝑠) ) Δ𝑠,
(37)
+𝑔 (𝑠)) Δ𝑠
𝑑 ∈ [𝜌 (𝑑1 ) , 𝑑𝑛 ] ,
(33)
𝑑𝑛
≤ 𝐢∗ πœ†
∗
π‘₯2π‘˜ (𝑑) = πœ† ∫ 𝐻2π‘˜ (𝑑, 𝑠) (𝑓2 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
×∫
𝑑1
𝜎(𝑑𝑛 )
𝜌(𝑑1 )
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] )
𝐺𝑖 (𝑠, 𝑠) (𝑓𝑖 (𝑠, [π‘₯ (𝑠)−V (𝑠)]∗ ) + 𝑔 (𝑠)) Δ𝑠,
𝜎(𝑑 )
then β€–π‘‡π‘–π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ )β€– ≤ 𝐢∗ πœ† ∫𝜌(𝑑 𝑛) 𝐺𝑖 (𝑠, 𝑠)(𝑓(𝑑, [π‘₯(𝑑) − V(𝑑)]∗ ) +
1
𝑔(𝑑))Δ𝑠.
On the other hand, when π‘˜ = 2, we have
+𝑔 (𝑠) ) Δ𝑠.
We define a cone 𝑃𝑖𝑗 (𝑖, 𝑗 = 1, 2) by
𝑇𝑖2 (π‘₯1π‘˜ , π‘₯2π‘˜ ) (𝑑)
𝑃𝑖𝑗 = {π‘₯ ∈ 𝐸 | π‘₯ (𝑑) ≥
𝑐∗
πœ™ (𝑑) β€–π‘₯β€– , 𝑑 ∈ [𝜌 (𝑑1 ) , 𝑑𝑛 ]} .
𝐢∗ 𝑖𝑗
(34)
𝑑𝑛
∗
= πœ† ∫ 𝐻𝑖2 (𝑑, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
𝑑1
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) + 𝑔 (𝑠)) Δ𝑠
It is clearly that 𝑃𝑖𝑗 × π‘ƒπ‘šπ‘› is a cone of 𝐸 × πΈ, (𝑖, 𝑗, π‘š, 𝑛 = 1, 2).
Define the integral operator 𝑇2 : 𝑃11 × π‘ƒ21 → 𝐸 × πΈ, 𝑇3 : 𝑃12 ×
𝑃22 → 𝐸 × πΈ, 𝑇4 : 𝑃12 × π‘ƒ21 → 𝐸 × πΈ, 𝑇5 : 𝑃21 × π‘ƒ12 → 𝐸 × πΈ,
by
π‘‡π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ) = (𝑇1π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ) , 𝑇2π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ )) ,
(π‘˜ = 2, . . . , 5) ,
𝑑𝑛
𝑑1
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] )
+𝑔 (𝑠)) Δ𝑠
(35)
≥
𝑐∗
πœ™ (𝑑) πœ†
𝐢∗ 𝑖1
×∫
𝜎(𝑑𝑛 )
𝜌(𝑑1 )
where operators π‘‡π‘–π‘˜ are defined by
≥
𝑑𝑛
∗
≥ πœ† ∫ 𝑐∗ πœ™π‘–1 (𝑑) 𝐺𝑖 (𝑠, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠)−V1π‘˜ (𝑠)] ,
∗
𝐢∗ 𝐺𝑖 (𝑠, 𝑠) (𝑓𝑖 (𝑠, [π‘₯ (𝑠)−V (𝑠)]∗ )+𝑔 (𝑠)) Δ𝑠
𝑐∗
σ΅„©
σ΅„©
πœ™ (𝑑) 󡄩󡄩𝑇 (π‘₯ , π‘₯ )σ΅„©σ΅„© .
𝐢∗ 𝑖1 σ΅„© 𝑖2 1π‘˜ 2π‘˜ σ΅„©
(38)
π‘‡π‘–π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ) (𝑑) = πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
𝑑1
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] )
Thus, 𝑇𝑖2 (𝑃11 × π‘ƒ21 ) ⊂ 𝑃𝑖1 . Hence 𝑇2 (𝑃11 × π‘ƒ21 ) ⊂ 𝑃11 × π‘ƒ21 .
When π‘˜ = 3, we have
+𝑔 (𝑠) ) Δ𝑠,
𝑇𝑖3 (π‘₯1π‘˜ , π‘₯2π‘˜ ) (𝑑)
𝑑 ∈ [𝜌 (𝑑1 ) , 𝑑𝑛 ] ,
(36)
𝑑𝑛
∗
= πœ† ∫ 𝐻𝑖3 (𝑑, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
𝑑1
where 𝑖 = 1, 2. Clearly, if (π‘₯1π‘˜ , π‘₯2π‘˜ ) is a fixed point of π‘‡π‘˜ ,
then (π‘₯1π‘˜ , π‘₯2π‘˜ ) is a solution of system (26) with (π‘˜) (π‘˜ =
2, . . . , 5, π‘˜ = π‘˜ + 11).
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] )
+𝑔 (𝑠) ) Δ𝑠
8
Journal of Applied Mathematics
𝑑𝑛
claim that β€–(π‘₯1π‘˜ , π‘₯2π‘˜ )β€–1 =ΜΈ 𝑅0 . In fact for (π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ πœ•π‘ˆπ‘˜ and
β€–(π‘₯1π‘˜ , π‘₯2π‘˜ )β€–1 = 𝑅0 , we have
∗
≥ πœ† ∫ 𝑐∗ πœ™π‘–2 (𝑑) 𝐺𝑖 (𝑠, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠)−V1π‘˜ (𝑠)] ,
𝑑1
∗
π‘₯π‘–π‘˜ = ]π‘‡π‘–π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ )
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] )
𝑑𝑛
+𝑔 (𝑠)) Δ𝑠
≥
𝜎(𝑑𝑛 )
𝜌(𝑑1 )
≥
𝑑1
𝑐∗
πœ™ (𝑑) πœ†
𝐢∗ 𝑖2
×∫
∗
≤ πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) + 𝑔 (𝑠)) Δ𝑠
𝐢∗ 𝐺𝑖 (𝑠, 𝑠) (𝑓𝑖 (𝑠, [π‘₯ (𝑠)−V (𝑠)]∗ )+𝑔 (𝑠)) Δ𝑠
𝑑𝑛
𝑑1
𝑐∗
σ΅„©
σ΅„©
πœ™ (𝑑) 󡄩󡄩𝑇 (π‘₯ , π‘₯ )σ΅„©σ΅„© .
𝐢∗ 𝑖2 σ΅„© 𝑖3 1π‘˜ 2π‘˜ σ΅„©
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) + 𝑔 (𝑠)) Δ𝑠
(39)
Thus, 𝑇𝑖3 (𝑃12 × π‘ƒ22 ) ⊂ 𝑃𝑖2 . Hence 𝑇3 (𝑃12 × π‘ƒ22 ) ⊂ 𝑃12 × π‘ƒ22 .
Similarly discussion, we also have 𝑇4 (𝑃12 ×𝑃21 ) ⊂ 𝑃12 ×𝑃21 ,
𝑇5 (𝑃21 × π‘ƒ12 ) ⊂ 𝑃21 × π‘ƒ12 . In addition, standard arguments
show that π‘‡π‘˜ is a completely continuous operator.
For simplicity, we adopt the notation: 𝑃14 = 𝑃25 := 𝑃12
and 𝑃24 = 𝑃15 := 𝑃21 , then, we can write π‘‡π‘˜ (𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) ) ⊂
𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) , that is, π‘‡π‘–π‘˜ (𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) ) ⊂ 𝑃𝑖(π‘˜−1) , (𝑖 =
1, 2, π‘˜ = 2, . . . , 5).
Theorem 6. Suppose that (H1 )-(H2 ) hold. Then there exists
a constant πœ† > 0 such that, for any 0 < πœ† ≤ πœ†, (1) with
boundary value condition (π‘˜) has at least one positive solution
(π‘˜ = 2, . . . , 5).
Proof. Fix 𝛿 ∈ (0, 1) and π‘˜ (π‘˜ = 2, . . . , 5). From (H2 ) let 0 <
πœ€ < 1 be such that
𝑓𝑖 (𝑑, 𝑧1 , 𝑧2 ) ≥ 𝛿𝑓𝑖 (𝑑, 0, 0) ,
for 𝑑1 ≤ 𝑑 ≤ 𝑑𝑛 , 0 ≤ 𝑧𝑖 ≤ πœ€, 𝑖 = 1, 2.
(40)
Let 𝑓(πœ€) = max𝑑1 ≤𝑑≤𝑑𝑛 ,0≤𝑧1 ,𝑧2 ≤πœ€ {max𝑖=1,2 {𝑓𝑖 (𝑑, 𝑧1 , 𝑧2 )} +
𝑑𝑛
≤ πœ† ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) 𝑓 (𝑅0 ) Δ𝑠
𝑑1
≤ πœ†π‘π‘“ (𝑅0 ) .
(44)
It follows that
1
(41)
𝑓 (𝑅0 )
𝑓 (𝑅0 )
1
1
≥
,
>
=
𝑅0
2π‘πœ† 4π‘πœ†
𝑅0
(46)
which implies that β€–(π‘₯1π‘˜ , π‘₯2π‘˜ )β€–1 =ΜΈ 𝑅0 . By the nonlinear alternative of Leray-Schauder type, π‘‡π‘˜ has a fixed point (π‘₯𝑖1 , π‘₯𝑖2 ) ∈
π‘ˆπ‘˜ . Moreover combining (40) and the fact that 𝑅0 < πœ€, we
obtain
𝑑𝑛
∗
π‘₯π‘–π‘˜ = πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) (𝑓𝑖 (𝑑, [π‘₯1π‘˜ (𝑑) − V1π‘˜ (𝑑)] ,
𝑑1
∗
[π‘₯2π‘˜ (𝑑) − V2π‘˜ (𝑑)] ) + 𝑔 (𝑑)) Δ𝑠
≥ πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) (𝛿𝑓 (𝑠, 0, 0) + 𝑔 (𝑑)) Δ𝑠
𝑑1
𝑑𝑛
≥ πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) 𝑔 (𝑑) Δ𝑠
𝑑1
= Vπ‘–π‘˜ (𝑑)
for 𝑑 ∈ (𝜌 (𝑑1 ) , 𝑑𝑛 ) .
(47)
lim
(42)
𝑓 (πœ€)
1
<
,
πœ€
4π‘πœ†
Then there exists a 𝑅0 ∈ (0, πœ€] such that
𝑓 (𝑅0 )
1
=
.
𝑅0
4π‘πœ†
(45)
𝑑𝑛
Set πœ† = πœ€/4𝑐𝑓(πœ€), since for any 0 < πœ† ≤ πœ†, fix the πœ† ∈
(0, πœ†], we always have
𝑓 (𝑧)
= +∞,
𝑧↓0 𝑧
σ΅„©
σ΅„©
𝑅0 = σ΅„©σ΅„©σ΅„©(π‘₯1π‘˜ , π‘₯2π‘˜ )σ΅„©σ΅„©σ΅„©1 ≤ 2πœ†π‘π‘“ (𝑅0 ) ,
that is,
𝑑
𝑔(𝑑)}, and 𝑐 = ∫𝑑 𝑛 𝐢∗ 𝐺𝑖 (𝑠, 𝑠)Δ𝑠. We have
𝑓 (𝑧)
lim
= +∞.
𝑧↓0 𝑧
∗
≤ πœ† ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
(43)
Let π‘ˆπ‘˜ = {(π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ 𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) : β€–(π‘₯1π‘˜ , π‘₯2π‘˜ )β€–1 <
𝑅0 }, (π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ πœ•π‘ˆπ‘˜ and ] ∈ (0, 1) be such that (π‘₯1π‘˜ , π‘₯2π‘˜ ) =
]π‘‡π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ), that is, π‘₯π‘–π‘˜ = ]π‘‡π‘–π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ) (𝑖 = 1, 2). We
Then π‘‡π‘˜ has a positive fixed point (π‘₯𝑖1 , π‘₯𝑖2 ) and
β€–(π‘₯𝑖1 , π‘₯𝑖2 )β€–1 ≤ 𝑅0 < 1; that is, (π‘₯𝑖1 , π‘₯𝑖2 ) is a positive solution
of the boundary value problem (26) with π‘₯π‘–π‘˜ > Vπ‘–π‘˜ (𝑑) for
𝑑 ∈ (𝑑1 , 𝑑𝑛 ).
Let π‘’π‘–π‘˜ (𝑑) = π‘₯π‘–π‘˜ (𝑑)−Vπ‘–π‘˜ (𝑑) ≥ 0 (𝑖 = 1, 2), then (𝑒1π‘˜ , 𝑒2π‘˜ ) is a
nonnegative solution (positive on (𝜌(𝑑1 ), 𝑑𝑛 )) of the boundary
value problem (1).
Theorem 7. Suppose that (H∗1 ) and (H3 )-(H4 ) hold. Then there
exists a constant πœ†∗ > 0 such that, for any 0 < πœ† ≤ πœ†∗ , (1) with
boundary value condition (π‘˜) has at least one positive solution
(π‘˜ = 2, . . . , 5).
Journal of Applied Mathematics
9
Proof. We fix π‘˜ (π‘˜ = 2, . . . , 5). Let Ω1 = {(π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ 𝐸 ×
𝐸 : β€–π‘₯π‘–π‘˜ β€– < 𝑅1 , 𝑖 = 1, 2}, where 𝑅1 = max{1, π‘Ÿ} and π‘Ÿ =
𝑑
2
(𝐢∗ /𝑐∗ ) ∫𝑑 𝑛 𝑔(𝑠)Δ𝑠. Choose
(𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) ) ∩ πœ•Ω2 , we have β€–π‘₯1π‘˜ β€– = 𝑅2 or β€–π‘₯2π‘˜ β€– = 𝑅2 .
Without loss of generality let β€–π‘₯1π‘˜ β€– = 𝑅2 , so we have
1
𝑅
𝑅
πœ† = min {1, 1 (𝑅 + 1)−1 , 1 } ,
2
2π‘Ÿ
∗
𝑑𝑛
(48)
π‘₯1π‘˜ (𝑑) − V1π‘˜ (𝑑) = π‘₯1π‘˜ (𝑑) − πœ† ∫ 𝐻1π‘˜ (𝑑, 𝑠) 𝑔 (𝑠) Δ𝑠
𝑑1
≥ π‘₯1π‘˜ (𝑑) − πœ† ∫
𝑑
where 𝑅 = ∫𝑑 𝑛 𝐢∗ 𝐺𝑖 (𝑠, 𝑠)(max0≤𝑧1 ,𝑧2 ≤𝑅1 𝑓𝑖 (𝑠, 𝑧1 , 𝑧2 ) + 𝑔(𝑠))Δ𝑠
1
and 𝑅 ≥ 0.
Then for any (π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ (𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) ) ∩ πœ•Ω1 , π‘₯π‘–π‘˜ (𝑠) −
Vπ‘–π‘˜ (𝑠) ≤ π‘₯π‘–π‘˜ (𝑠) ≤ β€–π‘₯π‘–π‘˜ β€– ≤ 𝑅1 (𝑖 = 1, 2) and for 0 < πœ† ≤ πœ†∗ , we
have
𝑑1
2
π‘₯1π‘˜ (𝑑)
σ΅„©σ΅„© σ΅„©σ΅„© 𝑔 (𝑠) Δ𝑠
σ΅„©σ΅„©π‘₯1π‘˜ σ΅„©σ΅„©
π‘₯ (𝑑)
≥ π‘₯1π‘˜ (𝑑) − σ΅„©σ΅„©1π‘˜ σ΅„©σ΅„© πœ†π‘Ÿ
σ΅„©σ΅„©π‘₯1π‘˜ σ΅„©σ΅„©
∗
≥ π‘₯1π‘˜ (𝑑) −
∗
≥ (1 −
≤ πœ† ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
𝑑1
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) + 𝑔 (𝑠)) Δ𝑠
𝑑𝑛
≤ πœ† ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) ( max 𝑓𝑖 (𝑠, 𝑧1 , 𝑧2 ) + 𝑔 (𝑠)) Δ𝑠
≥
0≤𝑧1 ,𝑧2 ≤𝑅1
𝑑1
𝐢∗
𝑐∗
π‘₯ (𝑑) 𝑑𝑛 𝐢∗ 2
= π‘₯1π‘˜ (𝑑) − πœ† σ΅„©σ΅„©1π‘˜ σ΅„©σ΅„© ∫
𝑔 (𝑠) Δ𝑠
σ΅„©σ΅„©π‘₯1π‘˜ σ΅„©σ΅„© 𝑑1 𝑐∗
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©π‘‡π‘–π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ) (𝑑)σ΅„©σ΅„©σ΅„©
𝑑𝑛
𝑑𝑛
(53)
π‘₯1π‘˜ (𝑑)
πœ†π‘Ÿ
𝑅2
πœ†π‘Ÿ
) π‘₯1π‘˜ (𝑑)
𝑅2
1
π‘₯ (𝑑) ≥ 0,
2 1π‘˜
𝑑 ∈ [𝜌 (𝑑1 ) , 𝑑𝑛 ] .
≤ πœ†π‘…
≤
Thus
𝑅1
.
2
(49)
∗
∗
min {[π‘₯1π‘˜ (𝑑) − V1π‘˜ (𝑑)] + [π‘₯2π‘˜ (𝑑) − V2π‘˜ (𝑑)] }
πœƒ1 ≤𝑑≤πœƒ2
This implies
σ΅„©
σ΅„©
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©π‘‡π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ )σ΅„©σ΅„©σ΅„©1 ≤ 𝑅1 ≤ σ΅„©σ΅„©σ΅„©(π‘₯1π‘˜ , π‘₯2π‘˜ )σ΅„©σ΅„©σ΅„©1 ,
(π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ (𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) ) ∩ πœ•Ω1 .
1
≥ min {π‘₯1π‘˜ (𝑑) − V1π‘˜ (𝑑)} ≥ min { π‘₯1π‘˜ (𝑑)}
πœƒ1 ≤𝑑≤πœƒ2
πœƒ1 ≤𝑑≤πœƒ2 2
(50)
πœƒ1 ≤𝑑≤πœƒ2
=
Choose a constant 𝑁 > 1 such that
πœ†π‘π›Ύ
πœƒ2
𝑐∗
𝐺 (𝑠, 𝑠) πœ™π‘–1 (𝑠) πœ™π‘–2 (𝑠) Δ𝑠 ≥ 1, (51)
∫
σ΅„© σ΅„© σ΅„© σ΅„©
2 (σ΅„©σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„©σ΅„© + σ΅„©σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©σ΅„©) πœƒ1 𝑖
where 𝛾 = minπ‘˜ minπœƒ1 ≤𝑑≤πœƒ2 {πœ™1π‘˜ (𝑑), πœ™2π‘˜ (𝑑)}.
By assumption (H3 ) and (H4 ), there exists a constant 𝐡 >
𝑅1 such that
𝑓𝑖 (𝑑, 𝑧1 , 𝑧2 )
> 𝑁,
𝑧1 + 𝑧2
≥ min {
𝑐∗
σ΅„© σ΅„© 𝑐
σ΅„© σ΅„©
πœ™ (𝑑) σ΅„©σ΅„©π‘₯ σ΅„©σ΅„© , ∗ πœ™ (𝑑) σ΅„©σ΅„©π‘₯ σ΅„©σ΅„©}
2𝐢∗ 1π‘˜ σ΅„© 1π‘˜ σ΅„© 2𝐢∗ 2π‘˜ σ΅„© 1π‘˜ σ΅„©
𝑐∗
𝑅 min {πœ™ (𝑑) , πœ™2π‘˜ (𝑑)} ≥ 𝐡 + 1 > 𝐡.
2𝐢∗ 2 πœƒ1 ≤𝑑≤πœƒ2 1π‘˜
Now since 𝐡 > 𝑅1 , it follows that
π‘‡π‘–π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ ) (𝑑)
𝑑𝑛
∗
= πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
𝑑1
∗
that is, 𝑓𝑖 (𝑑, 𝑧1 , 𝑧2 ) > 𝑁 (𝑧1 + 𝑧2 ) ,
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) + 𝑔 (𝑠)) Δ𝑠
πœƒ2
for 𝑑 ∈ [πœƒ1 , πœƒ2 ] , 𝑧1 + 𝑧2 > 𝐡 (𝑖 = 1, 2) .
∗
≥ πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) (𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
(52)
πœƒ1
∗
Choose 𝑅2 = max{𝑅1 + 1, 2πœ†π‘Ÿ, 2𝐢∗ (𝐡 + 1)/𝑐∗ 𝛾} and let
Ω2 = {(π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ 𝐸 × πΈ : β€–π‘₯π‘–π‘˜ β€– < 𝑅2 , 𝑖 = 1, 2}. We note
that π‘₯(𝑑) ≥ (𝑐∗ /𝐢∗ )πœ™π‘–π‘— (𝑑)β€–π‘₯β€– for all π‘₯ ∈ 𝑃𝑖𝑗 , by Lemma 3, we
2
have π»π‘–π‘˜ (𝑑, 𝑠) ≤ (𝐢∗ /𝑐∗ )(π‘₯(𝑑)/β€–π‘₯β€–). Then for any (π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) + 𝑔 (𝑠)) Δ𝑠
πœƒ2
∗
≥ πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) 𝑓𝑖 (𝑠, [π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)] ,
πœƒ1
∗
[π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) Δ𝑠
(54)
10
Journal of Applied Mathematics
πœƒ2
≥ πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) 𝑁 ([π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)]
Theorem 8. Suppose that (H1 )–(H3 ) hold. Then (1) with
boundary value condition (π‘˜) has at least two positive solutions
for πœ† > 0 sufficiently small (π‘˜ = 2, . . . , 5).
∗
πœƒ1
∗
+ [π‘₯2π‘˜ (𝑠) − V2π‘˜ (𝑠)] ) Δ𝑠
In fact with 0 < πœ† < min{πœ†, πœ†∗ } then (1) with boundary
value condition (π‘˜) has at least two positive solutions.
πœƒ2
≥ πœ† ∫ π»π‘–π‘˜ (𝑑, s) 𝑁 (π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)) Δ𝑠
πœƒ1
πœƒ2
≥ πœ† ∫ 𝑐∗ min {πœ™1π‘˜ (𝑑) , πœ™2π‘˜ (𝑑)} 𝐺𝑖 (𝑠, 𝑠) 𝑁 (π‘₯1π‘˜ (𝑠) − V1π‘˜ (𝑠)) Δ𝑠
πœƒ1 ≤𝑑≤πœƒ2
πœƒ1
πœƒ2
≥ πœ† ∫ 𝑐∗ min {πœ™1π‘˜ (𝑑) , πœ™2π‘˜ (𝑑)} 𝐺𝑖 (𝑠, 𝑠)
πœƒ1 ≤𝑑≤πœƒ2
πœƒ1
𝑁
π‘₯ (𝑠) 𝑑𝑠
2 1π‘˜
Remark 9. In Theorems 6–8, we use the assumption condition 16. If we have not the condition 16, that is, π‘Žπ‘– = 𝑏𝑖 = 0,
then the system (1) and boundary condition (π‘˜) are
Δ
(𝑝1 𝑒1∇ ) (𝑑)−π‘ž1 (𝑑) 𝑒1 (𝑑)+πœ†π‘“1 (𝑑, 𝑒1 (𝑑) , 𝑒2 (𝑑)) = 0,
≥ πœ† min {πœ™1π‘˜ (𝑑) , πœ™2π‘˜ (𝑑)}
𝑑 ∈ (𝑑1 , 𝑑𝑛 ) , πœ† > 0,
πœƒ1 ≤𝑑≤πœƒ2
πœƒ2
× ∫ 𝑐∗ 𝐺𝑖 (𝑠, 𝑠)
πœƒ1
Δ
(𝑝2 𝑒2∇ ) (𝑑)−π‘ž2 (𝑑) 𝑒2 (𝑑)+πœ†π‘“2 (𝑑, 𝑒1 (𝑑) , 𝑒2 (𝑑)) = 0,
𝑐∗ 𝑁
σ΅„© σ΅„©
σ΅„© σ΅„© σ΅„© σ΅„© πœ™ (𝑠) πœ™π‘–2 (𝑠) σ΅„©σ΅„©σ΅„©π‘₯1π‘˜ σ΅„©σ΅„©σ΅„© Δ𝑠
2 (σ΅„©σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„©σ΅„© + σ΅„©σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©σ΅„©) 𝑖1
𝛼1 𝑒1 (𝑑1 ) − 𝛽1 𝑝1 (𝑑1 ) 𝑒1∇ (𝑑1 ) = 0,
πœƒ2
𝑐
≥ πœ†π‘π›Ύ σ΅„©σ΅„© σ΅„©σ΅„© ∗ σ΅„©σ΅„© σ΅„©σ΅„© ∫ 𝐺𝑖 (𝑠, 𝑠) πœ™π‘–1 (𝑠) πœ™π‘–2 (𝑠) Δ𝑠𝑅2
2 (σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„© + σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©) πœƒ1
≥ 𝑅2 ,
𝛾1 𝑒1 (𝑑𝑛 ) + 𝛿1 𝑝1 (𝑑𝑛 ) 𝑒1∇ (𝑑𝑛 ) = 0,
𝑑 ∈ [πœƒ1 , πœƒ2 ] .
(55)
This implies
σ΅„©σ΅„©
σ΅„©
σ΅„©
σ΅„©
σ΅„©σ΅„©π‘‡π‘˜ (π‘₯1π‘˜ , π‘₯2π‘˜ )σ΅„©σ΅„©σ΅„©1 ≥ σ΅„©σ΅„©σ΅„©(π‘₯1π‘˜ , π‘₯2π‘˜ )σ΅„©σ΅„©σ΅„©1 ,
(π‘₯1π‘˜ , π‘₯2π‘˜ ) ∈ (𝑃1(π‘˜−1) × π‘ƒ2(π‘˜−1) ) ∩ πœ•Ω2 .
(56)
For the Krasnosel’skii’s fixed point theorem, one deduces that
π‘‡π‘˜ has a fixed point (π‘₯1π‘˜ , π‘₯2π‘˜ ) with 𝑅1 < β€–(π‘₯1π‘˜ , π‘₯2π‘˜ )β€– < 𝑅2 ⇔
𝑅1 < β€–π‘₯1π‘˜ β€– + β€–π‘₯2π‘˜ β€– < 𝑅2 .
Since π‘Ÿ ≤ 𝑅1 < β€–π‘₯π‘–π‘˜ β€– < 𝑅2 (𝑖 = 1, 2), then
𝑑𝑛
π‘₯π‘–π‘˜ (𝑑) − Vπ‘–π‘˜ (𝑑) = π‘₯π‘–π‘˜ (𝑑) − πœ† ∫ π»π‘–π‘˜ (𝑑, 𝑠) 𝑔 (𝑠) Δ𝑠
𝑑1
𝑑𝑛
≥ π‘₯π‘–π‘˜ (𝑑) − πœ† ∫
𝑑1
∗2
𝐢
𝑐∗
𝛼2 𝑒2 (𝑑1 ) − 𝛽2 𝑝2 (𝑑1 ) 𝑒2∇ (𝑑1 ) = 0,
𝛾2 𝑒2 (𝑑𝑛 ) + 𝛿2 𝑝1 (𝑑𝑛 ) 𝑒2∇ (𝑑𝑛 ) = 0.
From Lemma 2, an argument similar to those in Theorems
6–8 yields the following theorems.
Theorem 10. Suppose that (H1 ) and (H2 ) hold. Then there
exists a constant πœ† > 0 such that, for any 0 < πœ† ≤ πœ†, the
boundary value problem (58) has at least one positive solution.
Theorem 11. Suppose that (H∗1 ) and (H3 )-(H4 ) hold. Then
there exists a constant πœ†∗ > 0 such that, for any 0 < πœ† ≤ πœ†∗ , the
boundary value problem (58) has at least one positive solution.
Theorem 12. Suppose that (H1 )–(H4 ) hold. Then the boundary value problem (58) has at least two positive solutions for
πœ† > 0 sufficiently small.
π‘₯π‘–π‘˜ (𝑑)
σ΅„©σ΅„© σ΅„©σ΅„© 𝑔 (𝑠) Δ𝑠
σ΅„©σ΅„©π‘₯π‘–π‘˜ σ΅„©σ΅„©
π‘₯ (𝑑)
= π‘₯π‘–π‘˜ (𝑑) − πœ† σ΅„©σ΅„©π‘–π‘˜ σ΅„©σ΅„© π‘Ÿ
σ΅„©σ΅„©π‘₯π‘–π‘˜ σ΅„©σ΅„©
(58)
4. Example
(57)
≥ π‘₯π‘–π‘˜ (𝑑) − πœ†π‘₯π‘–π‘˜ (𝑑)
To illustrate the usefulness of the results, we give some
examples.
= (1 − πœ†) π‘₯π‘–π‘˜ (𝑑)
Example 13. Consider the boundary value problem
≥ (1 − πœ†)
> 0,
𝑐∗ πœ™π‘–1 (𝑑) πœ™π‘–2 (𝑑) σ΅„©σ΅„© σ΅„©σ΅„©
σ΅„©π‘₯ σ΅„©
𝐢∗ σ΅„©σ΅„©σ΅„©σ΅„©πœ™π‘–1 σ΅„©σ΅„©σ΅„©σ΅„© + σ΅„©σ΅„©σ΅„©σ΅„©πœ™π‘–2 σ΅„©σ΅„©σ΅„©σ΅„© σ΅„© π‘–π‘˜ σ΅„©
𝑒󸀠󸀠 − 𝑒 = − πœ† ((𝑒 + V)π‘Ž +
1
𝑑 ∈ (𝜌 (𝑑1 ) , 𝑑𝑛 ) .
Thus (π‘₯1π‘˜ , π‘₯2π‘˜ ) is a positive solution of the boundary value
problem (26) with π‘₯π‘–π‘˜ (𝑑) > Vπ‘–π‘˜ (𝑑) (𝑖 = 1, 2) for 𝑑 ∈ (𝜌(𝑑1 ), 𝑑𝑛 ).
Let π‘’π‘–π‘˜ (𝑑) = π‘₯π‘–π‘˜ (𝑑)−Vπ‘–π‘˜ (𝑑) ≥ 0 (𝑖 = 1, 2), then (𝑒1π‘˜ , 𝑒2π‘˜ ) is a
nonnegative solution (positive on (𝜌(𝑑1 ), 𝑑𝑛 )) of the boundary
value problem (1).
Since condition (H1 ) implies conditions (H∗1 ) and (H4 )
then from the proof of Theorems 6 and 7, we immediately
have the following theorem.
1/2
(𝑑 − 𝑑2 )
cos (2πœ‹ (𝑒 + V))) ,
− 1 < 𝑑 < 1, πœ† > 0,
VσΈ€ σΈ€  − V = −πœ† ((𝑒 − 1)2 + V2 +
𝑒 (−1) = V (1) = 0,
1
1/2
(𝑑 − 𝑑2 )
𝑒 (1) = π‘Žπ‘’ (0) ,
sin (2πœ‹π‘’)) ,
V (−1) = 𝑏V (0) ,
(59)
where π‘Ž > 1. Then if πœ† > 0 is sufficiently small, (59) has a
positive solution 𝑒 with 𝑒(𝑑) > 0 for 𝑑 ∈ (0, 1).
Journal of Applied Mathematics
11
To see this, we will apply Theorem 7 with
𝑓1 (𝑑, 𝑒, V) = (𝑒 + V)π‘Ž +
1
1/4
(𝑑2 − 𝑑4 )
𝑓2 (𝑑, 𝑒, V) = (𝑒 − 1)2 + V2 +
πœ†∗ = min {1,
cos (2πœ‹ (𝑒 + V)) ,
1
sin (2πœ‹π‘’) ,
1/4
(𝑑2 − 𝑑4 )
𝑔1 (𝑑) = 𝑔2 (𝑑) = 𝑔 (𝑑) =
Also let
1
(𝑑2 −
1/4
𝑑4 )
(60)
lim inf
𝑒+V↑+∞
Example 14. Consider the boundary value problem:
.
Δ
(𝑝1 𝑒1∇ ) (𝑑) − π‘ž1 (𝑑) 𝑒1 (𝑑)
= −πœ† (𝑒𝑒1 + 𝑒22 + 7 cos (2πœ‹π‘‘π‘’1 )) ,
for 𝑑 ∈ (0, 1) 𝑖 = 1, 2,
𝑑1 < 𝑑 < 𝑑𝑛 ,
𝑓𝑖 (𝑑, 𝑒, V)
= +∞ for all 𝑑 ∈ [πœƒ1 , πœƒ2 ] ⊂ (0, 1) .
𝑒+V
(61)
Now (H∗1 ), (H3 ), and (H4 ) hold. We note that the boundary
condition of (59) is in accord with (4), and from [1], we have
𝑒𝑑+1 − 𝑒−𝑑−1
πœ™11 = πœ™21 =
,
2
(65)
Now, if πœ† < πœ†∗ , Theorem 7 guarantees that (59) has a positive
solutions (𝑒, V) with ‖𝑒‖ ≥ 1 and β€–Vβ€– ≥ 1.
Clearly for 𝑑 ∈ (0, 1),
𝑓𝑖 (𝑑, 𝑒, V) + 𝑔 (𝑑) > 0,
−1 𝑅
𝑅1
(π‘…π‘Ž+2 + πœ‹) , 1 } .
2π‘Ž+2 𝐢∗ 𝑒4 1
2π‘Ÿ
𝑒−𝑑+1 − 𝑒𝑑−1
πœ™12 = πœ™22 =
,
2
𝑑1 = 𝑑2 = sinh (2) .
(62)
πœ† > 0,
(66)
Δ
(𝑝2 𝑒2∇ ) (𝑑) − π‘ž2 (𝑑) 𝑒2 (𝑑)
2
= −πœ† ((𝑒1 − 1) + 𝑒22 + 5 sin (2πœ‹π‘‘π‘’2 ))
satisfying one of the boundary value conditions (π‘˜), (π‘˜ =
2, . . . , 5).
Then if πœ† > 0 is sufficiently small, (66) has two solutions
(𝑒11 , 𝑒12 ), (𝑒21 , 𝑒22 ) with 𝑒𝑖𝑗 (𝑑) > 0 for 𝑑 ∈ (0, 1), 𝑖, 𝑗 = 1, 2.
To see this, we will apply Theorem 8 with
𝑓1 (𝑑, 𝑒1 , 𝑒2 ) = 𝑒𝑒1 + 𝑒22 + 7 cos (2πœ‹π‘‘π‘’1 ) ,
Then
2
𝑓2 (𝑑, 𝑒1 , 𝑒2 ) = (𝑒1 − 1) + 𝑒22 + 5 sin (2πœ‹π‘‘π‘’2 ) ,
𝐺1 (𝑑, 𝑠) = 𝐺2 (𝑑, 𝑠)
=
1 πœ™12 (𝑑) πœ™11 (𝑠) ,
{
𝑑1 πœ™11 (𝑑) πœ™12 (𝑠) ,
𝐻24 (𝑑, 𝑠) = 𝐺2 (𝑑, 𝑠) +
𝑑𝑛
𝑔1 (𝑑) = 𝑔2 (𝑑) = 𝑔 (𝑑) = 8.
𝜌 (𝑑1 ) ≤ 𝑠 ≤ 𝑑 ≤ 𝑑𝑛 ,
𝜌 (𝑑1 ) ≤ 𝑑 ≤ 𝑠 ≤ 𝑑𝑛 ,
1
𝐻14 (𝑑, 𝑠) = 𝐺1 (𝑑, 𝑠) +
π‘ŽπΊ (0, 𝑠) πœ™11 (𝑑) ,
𝑑1 − π‘Žπœ™11 (0) 1
(63)
Clearly, for 𝑑 ∈ (0, 1),
𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 ) + 𝑔 (𝑑) ≥ 1 > 0,
1
𝑏𝐺 (0, 𝑠) πœ™22 (𝑑) .
𝑑2 − π‘πœ™22 (0) 2
𝑓1 (𝑑, 0, 0) = 8 > 0,
Note π‘Ÿ = ∫𝑑 (𝐢 /𝑐∗ )𝑔(𝑠)Δ𝑠. Let 𝑅1 = π‘Ÿ + 1 and we have
1
lim inf
𝑒+V↑+∞
𝑑𝑛
𝑅 = ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) ( max 𝑓𝑖 (𝑠, 𝑧1 , 𝑧2 ) + 𝑔 (𝑠)) Δ𝑠
0≤𝑧1 ,𝑧2 ≤𝑅1
𝑑𝑛
≤ ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) [2π‘Ž+2 𝑅1π‘Ž+2 +
𝑑1
≤ ∫
−1
= ∫
0
1/4
(𝑠2 − 𝑠4 )
𝐢∗ 𝑒4 π‘Ž+2 π‘Ž+2
2
] Δ𝑠
[2 𝑅1 +
1/4
2
4
(𝑠 − 𝑠4 )
1
1
2
∗ 4
𝐢 𝑒
2
] Δ𝑠
[2π‘Ž+2 𝑅1π‘Ž+2 +
1/4
2
2
(𝑠 − 𝑠4 )
𝐢∗ 𝑒4 π‘Ž+2 π‘Ž+2
2
≤ ∫
] Δ𝑠
[2 𝑅1 +
1/2
2
0
(𝑠 − 𝑠2 )
1
π‘Ž+1
≤2
∗ 4
𝐢 𝑒
(𝑅1π‘Ž+2
+ πœ‹) .
(68)
𝑓2 (𝑑, 0, 0) = 3 > 0,
∗2
𝑑1
(67)
𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 )
= +∞,
𝑒1 + 𝑒2
𝑖 = 1, 2.
Now (H1 )–(H4 ) hold. Let 𝛿 = 1/100, πœ€ = 1/8, and we have
𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 ) ≥ 𝛿𝑓𝑖 (𝑑, 0, 0) ,
] Δ𝑠
(64)
for 0 ≤ 𝑑 ≤ 1, 0 ≤ 𝑒𝑖 ≤ πœ€, 𝑖 = 1, 2.
(69)
Furthermore
let
𝑓(πœ€)
=
max0≤𝑑≤1,0≤𝑒1 ,𝑒2 ≤πœ€ {max𝑖=1,2 𝑓𝑖 (𝑑, 𝑒1 , 𝑒2 ) + 𝑔(𝑑)}, and 𝑐 =
𝑑
∫𝑑 𝑛 𝐢∗ 𝐺𝑖 (𝑠, 𝑠)Δ𝑠. Note
1
πœ€
4𝑐𝑓 (πœ€)
≥
1
1
>
.
32𝑐 (𝑒 + 8) 352𝑐
(70)
Let πœ† = 1/352𝑐. Now, if 0 < πœ† < πœ† then 0 < πœ† < πœ€/4𝑐𝑓(πœ€)
and Theorem 6 guarantees that (66) has positive solutions
(𝑒11 , 𝑒12 ) with ‖𝑒1𝑗 β€– ≤ (1/8) (𝑗 = 1, 2).
12
Journal of Applied Mathematics
2
Next note π‘Ÿ = 8𝐢∗ (𝑑𝑛 − 𝑑1 )/𝑐∗ and let 𝑅1 = π‘Ÿ + 2 so we
have
1
𝑅 = ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) ( max 𝑓𝑖 (𝑠, 𝑧1 , 𝑧2 ) + 𝑔 (𝑠)) Δ𝑠
0≤𝑧1 ,𝑧2 ≤𝑅1
0
1
≤ ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) (𝑒𝑅1 + 2𝑅12 + 7 + 8) Δ𝑠
0
(71)
1
≤ ∫ 𝐢∗ 𝐺𝑖 (𝑠, 𝑠) Δ𝑠 (𝑒𝑅1 + 2𝑅12 + 15)
0
≤ (𝑒𝑅1 + 2𝑅12 + 15) 𝑐.
Also let
πœ†∗ = min {1,
𝑅1
𝑅
, 1}.
2 (𝑒𝑅1 + 2𝑅12 + 15) 𝑐 2π‘Ÿ
(72)
Now, if πœ† < πœ†∗ , Theorem 7 guarantees that (59) has a positive
solutions (𝑒21 , 𝑒22 ) with ‖𝑒2𝑗 β€– ≥ 2, 𝑗 = 1, 2.
Thus, if πœ† < min{πœ†, πœ†∗ }, Theorem 8 guarantees that (66)
has two solutions (𝑒11 , 𝑒12 ) and (𝑒21 , 𝑒22 ) with 𝑒𝑖𝑗 > 0 for 𝑑 ∈
(0, 1), 𝑖, 𝑗 = 1, 2.
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