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Applied Mathematics and Computation 217 (2011) 7692–7702
Contents lists available at ScienceDirect
Applied Mathematics and Computation
journal homepage: www.elsevier .com/ locate /amc
Positive periodic solution for a neutral Logarithmic population modelwith feedback control q
Rui Wang ⇑, Xiaosheng ZhangSchool of Mathematical Sciences, Capital Normal University, Beijing 100048, People’s Republic of China
a r t i c l e i n f o
Keywords:Neutral Logarithmic population modelFeedback controlPositive periodic solutionGlobal asymptotically stability
0096-3003/$ - see front matter � 2011 Elsevier Incdoi:10.1016/j.amc.2011.02.072
q Supported by the Natural Science Foundation o⇑ Corresponding author.
E-mail address: [email protected] (R. Wan
a b s t r a c t
In this paper, a neutral delay Logarithmic population model with feedback control is stud-ied. By using the abstract continuous theorem of k-set contractive operator, some newresults on the existence of the positive periodic solution are obtained; after that, by con-structing a suitable Lyapunov functional, a set of easily applicable criteria is establishedfor the global asymptotically stability of the positive periodic solution.
� 2011 Elsevier Inc. All rights reserved.
1. Introduction
In the past few years, many authors have studied the existence of the Logarithmic population model.Gopalsamy [3] and Kirlinger [5] had proposed the following single species Logarithmic model:
dNðtÞdt¼ NðtÞ½a� b � ln NðtÞ � c � ln Nðt � sÞ�: ð1:1Þ
System (1.1) is then generalized by Li [8] to the non-autonomous case
dNðtÞdt¼ NðtÞ½aðtÞ � bðtÞ ln NðtÞ � cðtÞ ln Nðt � sðtÞÞ�: ð1:2Þ
In [8], by using the coincidence degree theory, sufficient conditions for the existence of positive periodic solutions of sys-tem (1.2) are established.
As was pointed out by Gopalsamy [3], in some case, the neutral delay population models are more realistic. There weremany scholars done works on the periodic solution of neutral type Logistic model or Lotka–Volterra model, but only a littlescholars considered the neutral Logarithmic model. Li [9] had studied the following single species neutral Logarithmicmodel:
dNðtÞdt¼ NðtÞ½rðtÞ � aðtÞ ln Nðt � rÞ � bðtÞðln Nðt � gÞÞ0�: ð1:3Þ
Lu and Ge [6] investigated the following system:
dNðtÞdt¼ NðtÞ rðtÞ �
Xn
j¼1
ajðtÞ ln Njðt � rðtÞÞ �Xn
j¼1
bjðtÞðln Nðt � gjðtÞÞÞ0
" #: ð1:4Þ
. All rights reserved.
f China (10871005) and the Foundation of Beijing City’s Educational Committee (KM200610028001).
g).
R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702 7693
Some results on the existence of positive periodic solution of system (1.4) are obtained by employing an abstract continuoustheorem of k-set contractive operator.
The authors [13], by using an abstract continuous theorem of k-set contractive operator, investigated the existence, glob-ally attractive of the positive periodic solution of the following neutral multi-delays Logarithmic population model:
dNðtÞdt¼ NðtÞ rðtÞ � aðtÞ ln NðtÞ �
Xn
j¼1
bjðtÞ ln Nðt � sjðtÞÞ �Xn
j¼1
cjðtÞZ t
�1kjðt � sÞ ln NðsÞds�
Xn
j¼1
djðtÞðln Nðt � gjðtÞÞÞ0
" #:
ð1:5Þ
For the neutral multi-species Logarithmic population model, we refer the reader to [1].On the other hand, in some situation, people may wish to change the position of the existing periodic solution but to keepits stability. This is of significance in the control of ecology balance. One of the methods to realize such a control is to alter thesystem structurally by introducing some feedback control variables so as to get the population stability of another periodicsolution. The realization of the feedback control mechanism might be implemented by means of some biological controlscheme or by harvesting procedure. In fact, during the last decade, the qualitative behaviors of the population dynamics withfeedback control have been studied extensively. Recently, many scholars focus on the existence and global attractivity of thepositive periodic solution of the system. The authors [12] have studied the existence, uniqueness and global attractivity ofthe periodic solution of the delay multispecies Logarithmic population model with feedback control, by using the contractionmapping principle and a suitable Lyapunov functional. By means of the Cauchy matrix, the authors [14] investigate the exis-tence and exponential stability of almost periodic solutions and periodic solutions for the delay impulsive Logarithmic pop-ulation. The impulses can be considered as a kind of control.
However, to this day, there are few papers published on the existence and global asymptotically stability of positive peri-odic solution of the neutral Logarithmic population model with feedback control. This motivates us to consider the followingequation:
dNðtÞdt ¼ NðtÞ rðtÞ � aðtÞ ln NðtÞ �
Pnj¼1
bjðtÞ ln Nðt � s1jðtÞÞ �Pnj¼1
cjðtÞR t�1 kjðt � sÞ ln NðsÞds
(
�Pnj¼1
djðtÞðln Nðt � g1jðtÞÞÞ0 �Pnj¼1
fjðtÞuðt � s2jðtÞÞ)
;
duðtÞdt ¼ �a0ðtÞuðtÞ þ
Pnj¼1
gjðtÞNðt � g2jðtÞÞ;
8>>>>>>>>>><>>>>>>>>>>:
ð1:6Þ
where u(t) denotes the feedback control variable. It is assumed that:
(H1) r(t), cj(t), fj(t), a0(t), gj(t) are continuous, positive x-periodic functions on R a(t), bj(t), dj(t) are continuous differentiable,positive x-periodic functions on R.
(H2) s1j(t), g1j(t) 2 C(R, [0,+1)), g2j(t), s2j(t) 2 C(R, (0,+1)) are all x-periodic functions, and kj(t) 2 C([0,+1), (0,+1))j = 1, . . . ,n with 1� s01jðtÞ > 0; 1� g01jðtÞP 0; 1� s02jðtÞ > 0; 1� g02jðtÞ > 0 and
Rþ10 kjðsÞds ¼ 1;
Rþ10 skjðsÞds < þ1.
We consider (1.6) together with following initial conditions:
NðtÞ ¼ uðtÞ; N0ðtÞ ¼ u0ðtÞ; uð0Þ > 0; u 2 C1ðð�1;0�; ½0;1ÞÞ;uðhÞ ¼ wðhÞP 0; h 2 ½�s2;0�; wð0Þ > 0; where s2 ¼ max
t2½0;x�;j¼1;...;nfs2jðtÞg:
8<: ð1:7Þ
The aim of this paper is to give a set of new conditions to guarantee the existence and global stability of the positive peri-odic solution of the system (1.6) and (1.7).
2. Main lemmas
We will investigate the existence of positive periodic solution of system (1.6) and (1.7) in this section, and to do this, somelemmas are needed.
Since each x-periodic solution of the equation
duðtÞdt¼ �a0ðtÞuðtÞ þ
Xn
j¼1
gjðtÞNðt � g2jðtÞÞ
is equivalent to that of the equation
uðtÞ ¼Z tþw
tGðt; sÞ
Xn
j¼1
gjðsÞNðs� g2jðsÞÞ !
ds :¼ ðUNÞðtÞ; ð2:1ÞR
where, Gðt; sÞ ¼exp
s
ta0ðhÞdh
expR x
0a0ðhÞdh�1
; s 2 ½t; t þx�; t 2 R.
7694 R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702
Therefore, the existence problem of positive x-periodic solution of system (1.6) and (1.7) is equivalent to that of positivex-periodic solution of the equation:
dNðtÞdt¼ NðtÞ rðtÞ � aðtÞ ln NðtÞ �
Xn
j¼1
bjðtÞ ln Nðt � s1jðtÞÞ �Xn
j¼1
cjðtÞZ t
�1kjðt � sÞ ln NðsÞds�
Xn
j¼1
djðtÞðln Nðt � g1jðtÞÞÞ0
(
�Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞNðs� g2jðsÞÞ !
ds
): ð2:2Þ
Taking the transformation N(t) = ey(t), then (2.2) can be rewritten as
y0ðtÞ ¼ rðtÞ � aðtÞyðtÞ �Xn
j¼1
bjðtÞyðt � s1jðtÞÞ �Xn
j¼1
cjðtÞZ t
�1kjðt � sÞyðsÞds�
Xn
j¼1
djðtÞy0ðt � g1jðtÞÞð1� g01jðtÞÞ
�Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞeyðs�g2jðsÞÞ
!ds: ð2:3Þ
It is obvious that if Eq. (2.3) has a x-periodic solution y⁄(t), then Eq. (2.2) has a positive x-periodic solution N�ðtÞ ¼ ey�ðtÞ.Let E be a Banach space. For a bounded subset A � E, denote the Kuratoskii measure of non-compactness:
aEðAÞ ¼ inffd > 0jThere is a finite number of subsets fAig � A such that A ¼ [ðAiÞ and diamðAiÞ 6 dg;
where diam(Ai) denotes the diameter of set Ai. Let X, Y be two Banach spaces and X be a bounded open subset of X. A con-tinuous and bounded map N : X! Y is called k-set contractive if for any bounded set A � X, we have
aYðNðAÞÞ 6 kaXðAÞ;
where k is a non-negative constant.Also, for a Fred-holm L : X ? Y with index zero, according to [4], we define:
lðLÞ ¼ supfr P 0 : raXðAÞ 6 aYðLðAÞÞ; for all bounded subset A � Xg:
Lemma 2.1 [11]. Let L : X ? Y be a Fred-holm operator with zero index, and r 2 Y be a fixed point. Suppose that N : X ? Y iscalled a k-set contractive with k < l(L), where X � X is bounded, open and symmetric about 0 2X. Further, we also assume that:
(1) Lx – kNx + kr, for x 2 oX, k 2 (0,1), and(2) [QN(x) + Qr,x] � [QN(�x) + Qr,x] < 0 for x 2 kerL \ oX; where [�, �] is a bilinear form on Y � X and Q is the projection of Y
onto Coker(L), where Coker(L) is the co-kernel of the operator L.
Then there is a x 2 X such that Lx � Nx = r.In order to use Lemma 2.1 to study (2.3), we setY ¼ Cx ¼ fxjx 2 CðR;RnÞ; xðt þxÞ ¼ xðtÞg
with the norm defined by kxk = jxj0 = maxt2[0,x]{jx(t)j}, and
X ¼ C1x ¼ fxjx 2 C1ðR;RnÞ; xðt þxÞ ¼ xðtÞg
with the norm defined by jxj1 = max{jxj0, jx0 j0}.Then both Cx and C1
x are Banach spaces. We also denote:
�h ¼ 1x
Z x
0jhðsÞjds; ðhÞm ¼ min
t2½0;x�hðtÞ; ðhÞM ¼ max
t2½0;x�hðtÞ:
Let L : C1x ! Cx defined by Ly = y0(t) and N : C1
x ! Cx defined by
Ny ¼ �aðtÞyðtÞ �Xn
j¼1
bjðtÞyðt � s1jðtÞÞ �Xn
j¼1
cjðtÞZ t
�1kjðt � sÞyðsÞds�
Xn
j¼1
djðtÞy0ðt � g1jðtÞÞð1� g01jðtÞÞ
�Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞeyðs�g2jðsÞÞ
!ds: ð2:4Þ
Thus (2.3) has a positive x-periodic solution if and only if Ly = Ny + r for some y 2 C1x, where r = r(t).
Lemma 2.2 [10]. The differential operator L is a Fred-holm operator with index zero, and satisfies l(L) P 1.
R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702 7695
Lemma 2.3. Let c0, c1 be two positive constants, and X ¼ fxjx 2 C1x; jxj0 < c0; jx0j0 < c1g, if k ¼
Pnj¼1kdjð1� g01jÞk, then N :
X ? Cx is a k-set contractive map.
Proof. Let A � X be a bounded subset and let g ¼ aC1xðAÞ. Then, for any e > 0, there is a finite family of subsets of Ai satisfying
A = [(Ai) with diam (Ai) 6 g + e.Now we define:
ðHyÞðtÞ ¼ ðUeyÞðtÞ;
Fðt; x; y1; . . . ; yn; z1; . . . ; zn;w1; . . . ;wn;v1; . . . ;vnÞ ¼ aðtÞxþXn
j¼1
bjðtÞyj þXn
j¼1
cjðtÞzj þXn
j¼1
djðtÞwjð1� g01jðtÞÞ þXn
j¼1
fjðtÞv j:
For convenience, in the following discussion we denote
JiðxÞðtÞ ¼Z t
�1kiðt � sÞxðsÞds; for x 2 C1
x; i ¼ 1;2; . . . ;n:
Since F(t,x,y1, . . . ,yn,z1, . . . ,zn,w1, . . . ,wn,v1, . . . ,vn) is uniformly continuous on any compact subset of R � R4n+1, A and Ai areprecompact in Cx, it follows that there is a finite family of subsets Aij of Ai such that Ai = [jAij with
jFðt; xðtÞ; xðt � s11ðtÞÞ; . . . ; xðt � s1nðtÞÞ; J1ðxÞðtÞ; . . . ; JnðxÞðtÞ;u0ðt � g11ðtÞÞ; . . . ;u0ðt � g1nðtÞÞ; ðHxÞðt � s21ðtÞÞ; . . . ;
ðHxÞðt � s2nðtÞÞÞ � Fðt;uðtÞ; uðt � s11ðtÞÞ; . . . ;uðt � s1nðtÞÞ; J1ðuÞðtÞ; . . . ; JnðuÞðtÞ;u0ðt � g11ðtÞÞ; . . . ;u0ðt � g1nðtÞÞ;ðHuÞðt � s21ðtÞÞ; . . . ; ðHuÞðt � s2nðtÞÞÞj 6 e; for any x;u 2 Aij:
Therefore, we have
kNx� Nuk ¼ supt2½0;x�
jFðt; xðtÞ; xðt � s11ðtÞÞ; . . . ; xðt � s1nðtÞÞ; J1ðxÞðtÞ; . . . ; JnðxÞðtÞ;
x0ðt � g11ðtÞÞ; . . . ; x0ðt � g1nðtÞÞ; ðHxÞðt � s21ðtÞÞ; . . . ; ðHxÞðt � s2nðtÞÞÞ
� Fðt;uðtÞ;uðt � s11ðtÞÞ; . . . ; uðt � s1nðtÞÞ; J1ðuÞðtÞ; . . . ; JnðuÞðtÞ;
u0ðt � g11ðtÞÞ; . . . ;u0ðt � g1nðtÞÞ; ðHuÞðt � s21ðtÞÞ; . . . ; ðHuÞðt � s2nðtÞÞÞj
6 supt2½0;x�
jFðt; xðtÞ; xðt � s11ðtÞÞ; . . . ; xðt � s1nðtÞÞ; J1ðxÞðtÞ; . . . ; JnðxÞðtÞ;
x0ðt � g11ðtÞÞ; . . . ; x0ðt � g1nðtÞÞ; ðHxÞðt � s21ðtÞÞ; . . . ; ðHxÞðt � s2nðtÞÞÞ
� Fðt; xðtÞ; xðt � s11ðtÞÞ; . . . ; xðt � s1nðtÞÞ; J1ðxÞðtÞ; . . . ; JnðxÞðtÞ;
u0ðt � g11ðtÞÞ; . . . ;u0ðt � g1nðtÞÞ; ðHxÞðt � s21ðtÞÞ; . . . ; ðHxÞðt � s2nðtÞÞÞj
þ supt2½0;x�
jFðt; xðtÞ; xðt � s11ðtÞÞ; . . . ; xðt � s1nðtÞÞ; J1ðxÞðtÞ; . . . ; JnðxÞðtÞ;
u0ðt � g11ðtÞÞ; . . . ;u0ðt � g1nðtÞÞ; ðHxÞðt � s21ðtÞÞ; . . . ; ðHxÞðt � s2nðtÞÞÞ
� Fðt;uðtÞ;uðt � s11ðtÞÞ; . . . ; uðt � s1nðtÞÞ; J1ðuÞðtÞ; . . . ; JnðuÞðtÞ;
u0ðt � g11ðtÞÞ; . . . ;u0ðt � g1nðtÞÞ; ðHuÞðt � s21ðtÞÞ; . . . ; ðHuÞðt � s2nðtÞÞÞj
6
Xn
j¼1
kdjð1� g01jÞk � jx0ðt � g1jðtÞÞ � u0ðt � g1jðtÞÞj þ e 6 kðgþ eÞ þ e:
As e is arbitrarily small, it is easy to get that aCx ðNðAÞÞ 6 kaC1xðAÞ. The proof is complete. h
Lemma 2.4 [7]. Suppose s 2 C1x and s0(t) < 1, t 2 [0,x]. Then the function t � s(t) has a unique inverse l(t) satisfying l 2 C(R,R)
with l(a + x) = l(a) + x, "a 2 R. And if g(�) 2 Cx then g(l(t)) 2 Cx.
Lemma 2.5 [7]. Let 0 6 a 6x be a constant, s(t) 2 Cx, such that maxt2[0,x]js(t)j 6 a. Then for 8x 2 C1x, we haveRx
0 jxðtÞ � xðt � sðtÞÞj2dt 6 2a2Rx
0 jx0ðtÞj2dt. If, in addition, sðtÞ 2 C1
x, and s0(t) < 1, t 2 R, then for x 2 C1x, we have the following
conclusions:
(1) There exists a unique integer m such that l = js(t) �mxj0 < x;(2)
Rx0 jxðtÞ � xðt � sðtÞÞj2dt 6 2l2 Rx
0 jx0ðtÞj2dt.
As s01jðtÞÞ < 1, t 2 [0,x], from Lemma 2.5, we can choose an integer mj(s1j(t)), j = 1, . . . ,n. Such that lj = js1j �mjxj0 and
Z x0jxðtÞ � xðt � s1jðtÞÞj2dt 6 2l2
j
Z x
0jx0ðtÞj2dt; x 2 C1
x: ð2:5Þ
7696 R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702
Lemma 2.6 [15] . Suppose x(t) is a differently continuous x-periodic function on R with x > 0. Then to any t� 2 R;maxt�6t6ðt�þxÞjxðtÞj 6 jxðt�Þj þ 1
2
Rx0 jx0ðtÞjdt.
3. Existence of periodic solution
Since s01jðtÞ < 1; g01jðtÞ < 1, t 2 [0,x] we see that t � s1j(t), t � g1j(t) all have its inverse function. In the rest of this paper,we set l1j(t), c1j(t) represent the inverse function of t � s1j(t), t � g1j(t), respectively.
For convenience, throughout this paper, we also use the notations:
C1ðtÞ ¼ aðtÞ þXn
j¼1
bjðl1jðtÞÞ1� s01jðl1jðtÞÞ
�Xn
j¼1
d0jðc1jðtÞÞ1� g01jðc1jðtÞÞ
;
CðtÞ ¼ C1ðtÞ þXn
j¼1
cjðtÞ; H ¼ ln�r
Cþ A
��������;
A ¼ 1x
Z x
0
Xn
j¼1
fjðtÞZ t�s2jðtÞþx
t�s2jðtÞGðt � s2jðtÞ; sÞ
Xn
j¼1
gjðsÞ !
dsdt;
I ¼ maxt2½0;x�
Z t�s2jðtÞþx
t�s2jðtÞGðt � s2jðtÞ; sÞ
Xn
j¼1
gjðsÞ !
ds:
Theorem 3.1. If in addition to (H1)–(H2) assume further that:(H3):
�r > 0; cjðtÞP 0; C1ðtÞ > 0; t 2 ½0;x�; and �aþXn
j¼1
�bj þXn
j¼1
�cj > 0;
(H4):
�r � ACþ A
6 lnr
Cþ A; ln
�r þ CCþ A
P�r
Cþ A;
(H5):
B , 212Xn
j¼1
kbjklj þXn
j¼1
k1� g01jk12kdjk þ
x12
2
Z x
0
Xn
j¼1
jcjðtÞj2dt
!12
24
35
12
þ x2ffiffiffi2p ka0k þ
Xn
j¼1
b0j��� ���
!12
< 1;
(H6):
Xn
j¼1
kdjkk1� g01jk < 1:
Then (1.6) and (1.7) has at least one positive x-periodic solution.
Proof. Suppose u(t) is a x-periodic solution of the following operator equation
Lu ¼ kNuþ kr; k 2 ð0;1Þ: ð3:1Þ
Then u(t) satisfies the following equation
u0ðtÞ ¼ k rðtÞ � aðtÞuðtÞ �Xn
j¼1
bjðtÞuðt � s1jðtÞÞ �Xn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞds
"
�Xn
j¼1
djðtÞu0ðt � g1jðtÞÞð1� g01jðtÞÞ �Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞGðt � s2jðtÞ; sÞ
Xn
j¼1
gjðsÞeuðs�g2jðsÞÞÞds
#: ð3:2Þ
R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702 7697
Integrating (3.2) on [0,x], we have
�rx ¼Z x
0aðtÞuðtÞ þ
Xn
j¼1
bjðtÞuðt � s1jðtÞÞ þXn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞdsþ
Xn
j¼1
djðtÞu0ðt � g1jðtÞÞð1� g01jðtÞÞ"
þXn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞGðt � s2jðtÞ; sÞ
Xn
j¼1
gjðsÞeuðs�g2jðsÞÞ
!ds
#dt ¼
Z x
0aðtÞuðtÞ þ
Xn
j¼1
bjðtÞuðt � s1jðtÞÞ"
þXn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞds�
Xn
j¼1
d0jðtÞuðt � g1jðtÞÞ#
dt
þZ x
0
Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞeuðs�g2jðsÞÞ
!dsdt: ð3:3Þ
Let t � s1j(t) = s, then t = l1j(s), and
Z x0bjðtÞuðt � s1jðtÞÞdt ¼
Z x�s1jðxÞ
�s1jð0Þ
bjðl1jðsÞÞ1� s01jðl1jðsÞÞ
uðsÞds:
From Lemma 2.4, it follows that
Z x0bjðtÞuðt � s1jðtÞÞdt ¼
Z x
0
bjðl1jðsÞÞ1� s01jðl1jðsÞÞ
uðsÞds: ð3:4Þ
Similarly, we have
Z x
0d0jðtÞuðt � g1jðtÞÞdt ¼
Z x
0
d0jðc1jðsÞÞ1� g01jðc1jðsÞÞ
uðsÞds: ð3:5Þ
Combining (3.3)–(3.5), we have
Z x
0C1ðtÞuðtÞdt ¼
Z x
0aðtÞuðtÞ þ
Xn
j¼1
bjðtÞuðt � s1jðtÞÞ �Xn
j¼1
d0jðtÞuðt � g1jðtÞÞ" #
dt: ð3:6Þ
From Lemma 2.4, we get
l1jðxÞ ¼ l1jð0Þ þx; c1jðxÞ ¼ c1jð0Þ þx; j ¼ 1; . . . ;n; then
Z x
0
bjðl1jðtÞÞ1� s01jðl1jðtÞÞ
dt ¼Z l1jðxÞ
l1jð0Þ
bjðtÞð1� s01jðl1jðtÞÞÞ1� s01jðl1jðtÞÞ
dt ¼Z l1jð0Þþx
l1jð0ÞbjðtÞdt ¼
Z x
0bjðtÞdt ¼ �bjx;
Z x
0
d0jðc1jðtÞÞ1� g01jðc1jðtÞÞ
dt ¼Z c1jðxÞ
c1jð0Þ
d0jðtÞð1� g01jðc1jðtÞÞÞ1� g1j0ðc1jðtÞÞ
dt ¼Z x
0d0jðtÞdt ¼ 0:
Then C1x ¼Rx
0 C1ðtÞdt ¼ aþPn
j¼1�bj
� �x;
Cx ¼Z x
0CðtÞdt ¼
Z x
0C1ðtÞdt þ
Z x
0
Xn
j¼1
cjðtÞ !
dt ¼ �aþXn
j¼1
bj þXn
j¼1
�cj
!x: ð3:7Þ
By (H3), we have C1(t) > 0,Pn
j¼1cjðtÞP 0, t 2 [0,x]. From (3.3)
�rx ¼Z x
0C1ðtÞuðtÞdt þ
Z x
0
Xn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞdsdt þ
Z x
0
Xn
j¼1
fjðtÞ
�Z t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞeuðs�g2jðsÞÞ
!dsdt
P ðuÞmCxþ eðuÞm Ax P ðuÞmCxþ ð1þ ðuÞmÞAx:
Then �r P ðuÞmCþ ð1þ ðuÞmÞA, we obtain
ðuÞm 6�r � ACþ A
6r
Cþ A: ð3:8Þ
In the same manner, we get
�rx 6 ðuÞMCxþ eðuÞM Ax 6 eðuÞMxðCþ AÞ:
7698 R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702
Then �r 6 eðuÞM ðCþ AÞ, we obtain
ðuÞM P ln�r
Cþ A: ð3:9Þ
By Lemma 2.6, (H4), (3.8) and (3.9), we have
uðtÞP ðuÞM �12
Z x
0ju0ðsÞjds P ln
�rCþ A
� 12
Z x
0ju0ðsÞjds;
uðtÞ 6 ðuÞm þ12
Z x
0ju0ðsÞjds 6 ln
�rCþ A
þ 12
Z x
0ju0ðsÞjds:
So
kuk 6 H þ 12
Z x
0ju0ðsÞjds: ð3:10Þ
Also, from (3.3), we have
�rx ¼Z x
0C1ðtÞuðtÞdt þ
Z x
0
Xn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞdsdt þ
Z x
0
Xn
j¼1
fjðtÞ
�Z t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞeuðs�g2jðsÞÞ
!dsdt
6 ðuÞMCxþ eðuÞM Ax ¼ ððuÞM þ 1ÞCx� Cxþ eðuÞM Ax 6 eðuÞM xðCþ AÞ � Cx:
Then �r 6 eðuÞM ðCþ AÞ � C, from (H4), we obtain
ðuÞM P ln�r þ CCþ A
P�r
Cþ A: ð3:11Þ
Multiplying both sides of (3.2) by u0(t) and integrating them over [0,x], we have
Z x0ju0ðtÞj2dt 6
Z x
0rðtÞu0ðtÞdt �
Z x
0aðtÞuðtÞu0ðtÞdt �
Xn
j¼1
Z x
0bjðtÞuðt � s1jðtÞÞu0ðtÞdt
������Z x
0
Xn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞds
u0ðtÞdt
�Xn
j¼1
Z x
0djðtÞu0ðt � g1jðtÞÞð1� g01jðtÞÞu0ðtÞdt
�Z x
0
Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞGðt � s2jðtÞ; sÞ
Xn
j¼1
gjðsÞeuðs�g2jðsÞÞ
!ds
!u0ðtÞdt
�����6
Z x
0rðtÞu0ðtÞdt �
Z x
0aðtÞuðtÞu0ðtÞdt �
Xn
j¼1
Z x
0bjðtÞuðt � s1jðtÞÞu0ðtÞdt
������Z x
0
Xn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞds
u0ðtÞdt
�Xn
j¼1
Z x
0djðtÞu0ðt � g1jðtÞÞð1� g01jðtÞÞu0ðtÞdt
�����þXn
j¼1
jfjj0IeHþ12
R x
0ju0 ðsÞjds
Z x
0u0ðtÞdt
¼Z x
0rðtÞu0ðtÞdt �
Z x
0aðtÞuðtÞu0ðtÞdt �
Xn
j¼1
Z x
0bjðtÞuðt � s1jðtÞÞu0ðtÞdt
������Z x
0
Xn
j¼1
cjðtÞZ t
�1kjðt � sÞuðsÞds
u0ðtÞdt
�Xn
j¼1
Z x
0djðtÞu0ðt � g1jðtÞÞ 1� g01jðtÞ
� �u0ðtÞdt
�����
R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702 7699
6
Z x
0jrðtÞj2dt
12Z x
0ju0ðtÞj2dt
12
þ 12ka0k
Z x
0juðtÞj2dt þ 1
2
Xn
j¼1
kb0jkZ x
0juðtÞj2dt
þXn
j¼1
kbjkZ x
0ju0ðtÞj2dt
12Z x
0juðtÞ � uðt � s1jðtÞÞj2dt
12
þZ x
0
Xn
j¼1
jcjðtÞZ t
�1kjðt � sÞuðsÞdsj2dt
!12 Z x
0ju0ðtÞj2dt
12
þXn
j¼1
Z x
0ju0ðtÞj2dt
12Z x
0jdjðtÞu0ðt � g1jðtÞÞð1� g01jðtÞÞj
2dt 1
2
6
Z x
0jrðtÞj2dt
12Z x
0ju0ðtÞj2dt
12
þ 12ka0k
Z x
0juðtÞj2dt þ 1
2
Xn
j¼1
kb0jkZ x
0juðtÞj2dt
þXn
j¼1
kbjkZ x
0ju0ðtÞj2dt
12 ffiffiffi
2p
lj
Z x
0ju0ðtÞj2dt
12
þZ x
0
Xn
j¼1
jcjðtÞj2dt
!12
kukZ x
0ju0ðtÞj2dt
12
þXn
j¼1
k1� g01jðtÞk12kdjk
Z x
0ju0ðtÞj2dt
2�12
¼ffiffiffi2p Xn
j¼1
kbjklj þXn
j¼1
k1� g01jðtÞk12kdjk
" #Z x
0ju0ðtÞj2dt
þZ x
0jrðtÞj2dt
12
þZ x
0
Xn
j¼1
jcjðtÞj2dt
!12
kuk
24
35 Z x
0ju0ðtÞj2dt
12
þ 12ka0k þ
Xn
j¼1
kb0jk !Z x
0juðtÞj2dt:
ð3:12Þ
Using the notation ku0kL2¼
Rx0 ju0ðtÞj
2dt� �1
2, by
Rx0 juðtÞj
2dt 6 kuk2x (3.10) and (3.12), we have
ku0k2L26
ffiffiffi2p Xn
j¼1
kbjklj þXn
j¼1
k1� g01jðtÞk12kdjk
!ku0k2
L2
þZ x
0jrðtÞj2dt
12
þZ x
0
Xn
j¼1
jcjðtÞj2dt
!12
H þx12
2ku0kL2
!24
35ku0kL2
þx2ka0k þ
Xn
j¼1
kb0jk !
H þx12
2ku0kL2
!2
¼ffiffiffi2p Xn
j¼1
kbjklj þXn
j¼1
k1� g01jðtÞk12kdjk þ
x12
2
Z x
0
Xn
j¼1
jcjðtÞj2dt
!12
24
35� ku0k2
L2
þZ x
0jrðtÞj2dt
12
þZ x
0
Xn
j¼1
jcjðtÞj2dt
!12
H
24
35ku0kL2
þx2ka0k þ
Xn
j¼1
kb0jk !
H þx12
2ku0kL2
!2
: ð3:13Þ
From a26 b2 + c2 + d2) a 6 b + c + d, where a, b, c, d are all non-negative.
Then, we get
ku0kL26
ffiffiffi2p Xn
j¼1
kbjklj þXn
j¼1
k1� g01jðtÞk12kdjk þ
x12
2
Z x
0
Xn
j¼1
jcjðtÞj2dt
!12
24
35
12
� ku0kL2
þZ x
0jrðtÞj2dt
12
þZ x
0
Xn
j¼1
jcjðtÞj2dt
!12
H
24
35
12
� ku0k12L2þ x
2ka0k þ
Xn
j¼1
kb0jk !" #1
2
H þx12
2ku0kL2
!
¼ Bku0kL2þ
Z x
0jrðtÞj2dt
12
þZ x
0
Xn
j¼1
jcjðtÞj2dt
!12
H
24
35
12
� ku0k12L2þ x1
2ffiffiffi2p ka0k þ
Xn
j¼1
kb0jk !1
2
H: ð3:14Þ
7700 R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702
By (H5), then there exists a constant M > 0 such that ku0kL26 M, that is
Rx0 ju0ðtÞj
2dt� �1
26 M. From (3.10) and Hölder inequal-
ity, we obtain
kuk 6 H þ 12
Z x
0ju0ðtÞjdt 6 H þx1
2
2
Z x
0ju0ðtÞj2dt
12
6 H þx12
2M :¼ M1: ð3:15Þ
Again from (3.2), we get
ku0k 6 krk þ kakkuk þXn
j¼1
kbjkkuk þXn
j¼1
kcjkkuk þXn
j¼1
kdjkk1� g01jkku0k þXn
j¼1
kfjkeM1 I: ð3:16Þ
From (H6) and (3.15), we have
ku0k 6krk þ kak þ
Pnj¼1kbjk þ
Pnj¼1kcjk
� �M1 þ
Pnj¼1kfjkeM1 I
1�Pn
j¼1kdjkk1� g01jk:¼ M2: ð3:17Þ
Let X ¼ xjx 2 C1x; jxj1 > max M1;M2;
�rCþA
n on o. Then k ¼
Pnj¼1kdjð1� g01jÞk < lðLÞ. Defined a bounded bilinear form [�, �] on
Cx � C1x by ½y; x� ¼
Rx0 yðtÞxðtÞdt. Also we define Q : Y ? Coker(L) by y!
Rx0 yðtÞdt. It is obvious that {u : u 2 Ker L \ oX} =
{u : u � r0 or �r0}, without loss of generality, suppose that u � r0, then
½QNðuÞ þ QðrÞ;u� � ½QNð�uÞ þ QðrÞ; u�
¼ r20
Z x
0rðtÞdt � r0
Z x
0aðtÞ þ
Xn
j¼1
bjðtÞ þXn
j¼1
cjðtÞ !
dt
"
�er0
Z x
0
Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞ !
dsdt
#
�Z x
0rðtÞdt � ð�r0Þ
Z x
0aðtÞ þ
Xn
j¼1
bjðtÞ þXn
j¼1
cjðtÞ !
dt
"
�e�r0
Z x
0
Xn
j¼1
fjðtÞZ t�s2jðtÞþw
t�s2jðtÞG t � s2jðtÞ; s� � Xn
j¼1
gjðsÞ !
dsdt
#ð3:18Þ
¼ r20x
2 �r � r0 aþXn
j¼1
bj þXn
j¼1
cj
!� er0 A
" #� �r � ð�r0Þ aþ
Xn
j¼1
bj þXn
j¼1
cj
!� e�r0 A
" #
< r20x
2 �r � r0 aþXn
j¼1
bj þXn
j¼1
cj
!� r0A
" #� �r þ r0 aþ
Xn
j¼1
bj þXn
j¼1
cj
!þ r0A
" #
< r20x
2 �r � r0 Cþ A� �� �
� �r þ r0 Cþ A� �� �
:
Since r0 >�r
CþA
��� ���, then r0 >�r
CþA
��� ��� P �rCþA
, and �r0 < � rCþA
��� ��� 6 �rCþA
.Thus
�r � r0ðCþ AÞ < 0;
r þ r0ðCþ AÞ > 0:
By (3.18), we get [QN(u) + Q(r),u] � [QN(�u) + Q(r),u] < 0.Then all of the conditions required in Lemma 2.1 are hold. It follows from Lemma 2.1 that Eq. (2.3) has at least one x-
periodic solution. Therefore, system (1.6) and (1.7) has at least one positive x-periodic solution. The proof is complete. h
4. Global asymptotic stability
In this section, we devote ourselves to the study of the global asymptotic stability of periodic solution of system (1.6) and(1.7). Our method involves the construction of a suitable Lyapunov functional, which is based on the Lyapunov functionalintroduced by [12].
Definition 4.1. Let (N⁄(t),u⁄(t))T be a periodic solution of (1.6) and (1.7). We say (N⁄(t),u⁄(t))T is globally asymptotically stableif any other solution (N(t),u(t))T of (1.6) and (1.7) has the property:
limt!þ1
jN�ðtÞ � NðtÞj ¼ 0; limt!þ1
ju�ðtÞ � uðtÞj ¼ 0: ð4:1Þ
Now we state our main results of this section below.
R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702 7701
Theorem 4.1. Assume that the conditions in Theorem 3.1 hold. Moreover, if there is a positive constant k such that:
inft2½0;þ1Þ
k aðtÞ �Pnj¼1
bjðl1jðtÞÞ1�s0
1jðl1jðtÞÞ
�Pnj¼1
Rþ10 kjðsÞcjðt þ sÞds
" #( )> 0;
inft2½0;þ1Þ
k a0ðtÞ �Pnj¼1
fjðl2jðtÞÞ1�s0
2jðl2jðtÞÞ
" #( )> 0;
Rþ10
gjðc2jðsÞÞ1�g0
2jðc2jðsÞÞ
ds < þ1; j ¼ 1; . . . ;n;Rþ10
djðc1jðsÞÞ1�g0
1jðc1jðsÞÞ
ds < þ1; j ¼ 1; . . . ;n:
8>>>>>>>>>>>><>>>>>>>>>>>>:
ð4:2Þ
where l1j(t), l2j(t), c1j(t), c2j(t) are the inverse function of t � s1j(t), t � s2j(t), t � g1j(t), t � g2j(t), respectively. Then system(1.6) and (1.7) has a unique periodic solution which is globally asymptotically stable.
Proof. By Theorem 3.1, there exists a periodic solution of (1.6) and (1.7), say (N⁄(t),u⁄(t))T. To complete the proof, we onlyneed to show that (N⁄(t),u⁄(t))T is globally asymptotically stable. Let (N(t),u(t))T be any solution of (1.6) and (1.7). Consider aLyapunov functional V(t) = V(t, (N⁄(t),u⁄(t))T, (N(t),u(t))T) defined by
VðtÞ ¼ V1ðtÞ þ V2ðtÞ þ V3ðtÞ þ V4ðtÞ þ V5ðtÞ þ V6ðtÞ; for t P 0;
where
V1ðtÞ ¼ kðj ln N�ðtÞ � ln NðtÞj þ ju�ðtÞ � uðtÞjÞ;
V2ðtÞ ¼ kXn
j¼1
Z t
t�s1jðtÞ
bjðl1jðsÞÞ1� s01jðl1jðsÞÞ
j ln N�ðsÞ � ln NðsÞjds;
V3ðtÞ ¼ kXn
j¼1
Z þ1
0kjðsÞ
Z t
t�scjðhþ sÞj ln N�ðhÞ � ln NðhÞjdhds;
V4ðtÞ ¼ kXn
j¼1
Z t
t�s2jðtÞ
fjðl2jðsÞÞ1� s02jðl2jðsÞÞ
ju�ðsÞ � uðsÞjds;
V5ðtÞ ¼ kXn
j¼1
Z þ1
t�g2jðtÞ
gjðc2jðsÞÞ1� g02jðc2jðsÞÞ
jN�ðsÞ � NðsÞjds;
V6ðtÞ ¼ kXn
j¼1
Z þ1
t�g1jðtÞ
djðc1jðsÞÞ1� g01jðc1jðsÞÞ
jðln N�ðsÞÞ0 � ðln NðsÞÞ0jds:
From the definition of V(t), it is easy to see that
Vð0Þ < þ1 ð4:3Þand
VðtÞP kðj ln N�ðtÞ � ln NðtÞj þ ju�ðtÞ � uðtÞjÞ; t P 0: ð4:4Þ
Calculating the upper right derivative D+V(t) of V(t) along the solution of (1.6) and (1.7), by computation, one could obtain
DþVðtÞ 6 �kaðtÞj ln N�ðtÞ � ln NðtÞj
þ kXn
j¼1
bjðtÞj ln N�ðt � s1jðtÞÞ � ln Nðt � s1jðtÞÞj þ kXn
j¼1
cjðtÞZ t
�1kjðt � sÞj ln N�ðsÞ � ln NðsÞjds
þ kXn
j¼1
djðtÞjðln N�ðt � g1jðtÞÞÞ0 � ðln Nðt � g1jðtÞÞÞ
0j þ kXn
j¼1
fjðtÞju�ðt � s2jðtÞÞ � uðt � s2jðtÞÞj
� ka0ðtÞju�ðtÞ � uðtÞj þ kXn
j¼1
gjðtÞjN�ðt � g2jðtÞÞ � Nðt � g2jðtÞÞj
þ kXn
j¼1
bjðl1jðtÞÞ1� s01jðl1jðtÞÞ
j ln N�ðtÞ � ln NðtÞj � kXn
j¼1
bjðtÞj ln N�ðt � s1jðtÞÞ � ln Nðt � s1jðtÞÞj
þ kXn
j¼1
Z þ1
0kjðsÞcjðt þ sÞj ln N�ðtÞ � ln NðtÞjds� k
Xn
j¼1
Z þ1
0kjðsÞcjðtÞj ln N�ðt � sÞ � ln Nðt � sÞjds
þ kXn
j¼1
fjðl2jðtÞÞ1� s02jðl2jðtÞÞ
ju�ðtÞ � uðtÞj � kXn
j¼1
fjðtÞju�ðt � s2jðtÞÞ � uðt � s2jðtÞÞj
� kXn
j¼1
gjðtÞjN�ðt � g2jðtÞÞ � Nðt � g2jðtÞÞj � kXn
j¼1
djðtÞjðln N�ðt � g1jðtÞÞÞ0 � ðln Nðt � g1jðtÞÞÞ
0j
¼ �S1j ln N�ðtÞ � ln NðtÞj � S2ju�ðtÞ � uðtÞj;
7702 R. Wang, X. Zhang / Applied Mathematics and Computation 217 (2011) 7692–7702
where, " #
S1 ¼ k aðtÞ �Xn
j¼1
bjðl1jðtÞÞ1� s01jðl1jðtÞÞ
�Xn
j¼1
Z þ1
0kjðsÞcjðt þ sÞds ;
S2 ¼ k a0ðtÞ �Xn
j¼1
fjðl2jðtÞÞ1� s02jðl2jðtÞÞ
" #:
From (4.2), it follows that there exists a constant K > 0 such that
S1 > K; S2 > K:Hence, it follows that
DþVðtÞ < �K j ln N�ðtÞ � ln NðtÞj þ ju�ðtÞ � uðtÞjð Þ: ð4:5Þ
Then, by using (4.3) and (4.5) and the analysis of that in [2, p. 816], one could obtain:
limt!þ1
j ln N�ðtÞ � ln NðtÞj ¼ 0; limt!þ1
ju�ðtÞ � uðtÞj ¼ 0:
From this, one could easily obtain:
limt!þ1
jN�ðtÞ � NðtÞj ¼ 0; limt!þ1
ju�ðtÞ � uðtÞj ¼ 0:
which means (N⁄(t),u⁄(t))T is globally asymptotically stable. This completes the proof. h
Remark. From Theorems 3.1 and 4.1, we can get the system (1.6) and (1.7) has only one positive periodic solution.
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