Applied Mathematics, 2011, 2, 47-56
doi:10.4236/am.2011.21006 Published Online January 2011 (http://www.SciRP.org/journal/am)
Copyright © 2011 SciRes. AM
Permanence and Global Stability for a Non-Autonomous
Predator-Prey Model with Modified Leslie-Gower and
Holling-Type II Schemes with Delays
Lin Hu, Linfei Nie
College of Mathematics and Systems Science, Xinjiang University, Urumqi, China
E-mail: lfnie@163.com
Received August 18, 2010; revised November 11, 2010; accepted November 14, 2010
Abstract
In this paper, a nonautonomous predator-prey system based on a modified version of the Leslie-Gower
scheme and Holling-type II scheme with delayed effect is investigated. The general criteria of integrable
form on the permanence are established. By constructing suitable Lyapunov functionals, a set of easily veri-
fiable sufficient conditions are derived for global stability of any positive solutions to the model.
Keywords: Predator-Prey System, Leslie-Gower and Holling-Type-II Functional Response, Permanence,
Global Stability
1. Introduction
Predator-prey behavior is a form of very common bio-
logical interaction in nature. There are many mathemati-
cal models to model predator-prey behavior such as
Lotka-Volterra system, Chemostat-type system, Kolmo-
gorov system, etc (see [1-6]). In recent years there has
been a growing interest in the study of mathematical
models incorporates a modified version of Leslie-Gower
functional response as well as that of the Holling-type II
(see [7-9]). In particular, in [10] the authors consider the
following model
  

  

1
2
d
d.
d
d
xt cyt
xta bxt
txtk
yt eyt
yt d
txtk










(1.1)
This two species food chain model describes a prey
population x which serves as food for predator y, a, b, c,
e, k1 and k2 are positive parameters. They estab lished the
sufficient conditions for the boundedness, existence of a
positively invariant attracting set and global stability of
coexisting interior equilibrium. In [11] the authors con-
sidered the dynamical behavior of system (1.1) with de-
lays, and establish the sufficient conditions for the exis-
tence positive equilibrium, permanence and global sta-
bility of positive equ ilibrium. The dynamical behavior of
system (1.1) also has been discussed by many authors
(see, for example, [7,12] and the references cited therein).
However, we note that any biological or environmen-
tal parameters are naturally subject to fluctuation in time.
As [13] pointed out that the growth properties of every
natural population vary through time. Most, and perhaps
all, of this variation arises ultimately from fluctuations in
the population's environment. Physical environmental
conditions usually change greatly through the year and
can influence organisms directly. Good weather can sti-
mulate growth in body size and reproduction, and bad
weather can cause death. Similarly, the biological envi-
ronment can fluctuate in ways that influence population
dynamics. These kinds of time variation in population
dynamical events can exert profound effects on the
ecology and evolution of individual species and on the
composition of ecological commu nities.
In this paper, we are concerned with the effects of the
time-dependent of ecological and environmental para-
meters and time delays due to gestation and negative
feedbacks on the global dynamics of predator-prey sys-
tems with Modified Leslie-Gower and Holling-Type II
Schemes. Therefore, we consider the following delayed
differential system:
  

   


1122
11 111
111
2224
22 132
d()
d
d
d
xt atxt
xt rtbtxt
txtkt
xt atxt
xtrt
txtkt








(1.2)
L. HU ET AL.
Copyright © 2011 SciRes. AM
48
with initial conditions
 



1234
,,0,
,0 ,1,2,max,,,,
ii
i
x
Ci
 
 

 (1.3)
where

,0:,0:0, ,0,CCss
 



1
and 00,
x
t
and
2
x
t denote the densities
of prey and predator population, respectively; 0
i

1, 2,3, 4i denote the time delays due to negative
feedbacks of the prey and the predator population,
 
1,,
ii
bt rtat and

1, 2
i
kt i are model para-
meters. These parameters are defined as follows:
1
rt
is the growth rate of prey

11
,
x
bt measures the
strength of competition among individuals of species

11
,
x
at is the maximum value which per capita reduc-
tion rate of 1
x
can attain,

1
kt and

2
kt measure
the extent to which environment provides protection to
prey 1
x
and predator 2
x
, respectively;

2
rt is the
growth rate of predator 2
x
, and

2
at has a similar
meaning to

1
at.
The organization of this paper is as follows. In the
next section, we present some basic assumptions for sys-
tem (1.2) and two important lemmas on the nonauto-
nomous single-species logistic system. In Section 3, we
will state and prove the sufficient conditions of integra-
ble form on the permanence of solutions for system (1.2).
We also by means of suitable Lyapunov functionals, a
set of easily verifiable sufficient conditions are derived
for global stability of any positive solutions of system
(1.2). Numerical result is presented to illustrate the valid-
ity of our main results.
2. Preliminaries
Let
0:0,R and
:0,R
. For a bounded
continuous function

t on R, we use the following
notations:

:sup ,
utR
g
gt

:infR
lt
g
gt
.
For system (1.2), we introduce the following assump-
tions.

1
H Function
 
1,, ,
iii
bt rtat kt are conti-
nuous and bounded on 0
R,

10at for all 0t,
and
 
0
inf0 1,2
ti
tik
.

2
H There a constant 0
such that
 
12
infd 0, inflimd .l0im
tt
tt
tt
ba

 

 



3
H There is a constant 0
such that
 
12
lim linfd 0,infd 0.im
tt
tt
tt
rr

 

 


It is well known by the fundamental theory of func-
tional differential equations [5] that system (1.2) has a
unique solution
 

12
,
x
txtxt satisfying initial
conditions (1.3). If

0 1,2
i
xt i on the interval of
existence, then
x
t is said to be a positive solution. It
is easy to verify that solutions of system (1.2) corres-
ponding to initial conditions (1.3) are defined on
0,
and remain positive for all 0t.
We consider the following single-species nonauto-
nomous logistic system with a parameter
 
 
2
22
)
d:,,.
d
atu
uur tugtu
tkt

 



(2.1)
Obviously, if Assumption

1
H holds, then
,,gtu
is a continuous function defined on
00
,, 0,tuRR

,
where 0
is constant. We easily prove that for any
00 0
,tuRR
and
0
0,
system (2.1) has a
unique solution
ut
satisfying initial condition
00
ut u
. It is easy to see that

ut
is positive for
all 0
tt if the initial value 00u. If Assumptions
13
HH hold, then the following statements can be
prove to be true.
1
A
For any constant

1,, ,gtu
is bounded
on
1
00
,0,R



 .
2
A
There are positive constants 12 1 2
,,,kk
and
12
kk
such that


1
2
1
2
lim
l
inf,,0 d0,
sup ,im,0d0.
t
t
t
t
t
t
gk
gk




3
A
Partial derivative

,,0
g
tu u exists for all
0
,tuRR
, and there are nonnegative continuous
function
qt and a constant 0
, satisfying

inlim fd0
t
t
tq


and a continuous function

pu, satisfying
0pu
for all uR
, such that
 
0
,,0 for all ,.
gtu qt putuRR
u
 
4
A
Partial derivative

,,gtu

exists for all
00
,, 0,tuRR

, and for any constant 0U,
,,gtu
is also bounded on

00
, ,0,0,tu RU
 .
In system (2.1), when parameter 0
we obtain the
following system
 
 
2
22
d:,,0.
d
atu
uur tugtu
tkt

 



(2.2.)
Let
*
0
ut be a fixed positive solution of system
(2.2) defined on 0
R
. We say that

*
0
ut is globally
uniformly attractive on 0
R
, if for any constants 1
and 0
there is a constants

,0T

such that
L. HU ET AL.
Copyright © 2011 SciRes. AM
49
for any initial time 00
tR
and any solution
0
ut of
system (2.1) with

1
00 ,ut


, one has
 
*
00
utut
 for all

0,tt T
 . By Lemma 1
given in [14], we have the following res ult.
Lemma 2.1 Suppose that Assumptions

13
AA
hold, then
a) There is a constants 1
M
such that
 
100
inf sulimlim p
tt
M
utut M
 
 
for any positive solution
00
ut of system (2.2).
b) Each fixed positive solution

*
0
ut of system (2.2)
is globally uniformly attractive on 0
R
Let 0
uR
, 00
tR
and
0
0,
, and further
let

ut
and

0
ut
be the solutions of systems (2.1)
and (2.2) with initial value
00
ut u
and
00 0
utu
,
respectively. By Lemma 2 given in [14], we further have
the following result.
Lemma 2.2 Suppose that assumptions

14
AA
hold, then

ut
converges to

0
ut uniformly for
0,tt
as 0
.
3. Main Results
In this section, we proceed to discussion on the perma-
nence and global stability of any positive solution of
system (1.2) corresponding to initial conditions (1.3).
We first give the result of the ultimate boundedness of
any solution for system (1.2).
Theorem 3.1 Suppose that Assumptions

13
HH
hold, then any solution
 

12
,
x
txtxt of system
(1.2) corresponding to initial conditions (1.3) are ulti-
mately bounded.
Proof: Let
 

12
,
x
txtxt be any solution of
system (1.2) corresponding to initial conditions (1.3).
From the first equation of system (1.2) we have
  
111 11
dfor all0.
d
u
xt xtrt rxtt
t
(3.1)
For any t
and
,0s
 , integrating (3.1) from
ts to t we obtain




1111 1
expexp .
uu
xt sxtrsxtr

By assumptions

1
H, we further have
  

111 111
dexp
d
u
xt xtrtbtxtr
t

 

for all 0t. It is proved in many articles, for example,
see [15], that under Assumptions


13
HH any pos-
itive solution

ut of the following non-autonomous
single-species logistic equation
 

11 1
dexp
d
u
ut utr tbtutr
t

 

is ultimately bounded. Hence, using the comparison
theorem, we can obtain that there is a constant 10M
such that for any solution
 

12
,
x
txtxt of sys-
tem (1.2) corresponding to initial conditions (1.3), there
is a 10t such that
11
x
tM for all 1
tt.
From the second equation of system (1.2) we have
 
222 22
d.
d
u
xt
x
tr trxt
t
(3.2)
For any t
and
,0s
 , integrating (3.2) from
ts
to t we obtain


22222
expexp .
uu
xtsxt rsxtr

By assumptions
1
H, we further have
 


222
22 2
12
dexp
d
u
xt atxt
xtrtr
tMkt

for all 1
tt
. The compar ison equa tion is the logistic
equation
 


2
22
12
dexp .
d
u
yta tyt
ytr tr
tMkt
 
Similarly, by Assumptions

13
HH, we further
can obtain that there is constant 20M such that for
any solution

12
,
x
txtxt of system (1.2) cor-
responding to initial conditions (1.3), there is a 21
tt
such that
22
x
tM for all 2
tt. Therefore, the so-
lution
x
t is ultimately bounded. This completes the
proof of this theorem .
In particular, when parameter 24
0
 in system
(1.2), we obtain the following system
 

   


112
11 111
111
222
22 132
d
d.
d
d
xt atxt
xt rtbtxt
txtkt
xt atxt
xtrt
txtkt








(3.3)
with initial conditions
11 112
,,0,,0,00xCx
 

(3.4)
As a consequence of Theorem 3.1, we have the fol-
lowing corollary on the ultimate boundedness of any
solution for system (3.3) with the initial conditions (3.4).
Corollary 3.1 Suppose that Assumptions

13
HH
hold, then any solution


12
,
x
txtxt of system
(3.3) corresponding to initial conditions (3.4) is ulti-
mately bounded.
Next, on the permanence of component 2
x
of system
(1.2) with the initial conditions (1.3), we have the fol-
lowing result.
Theorem 3.2 Suppose that Assumptions

13
HH
hold, then the component 2
x
of system (1.2) is perma-
nent, in the sense there is a constant 0
such that
L. HU ET AL.
Copyright © 2011 SciRes. AM
50

2
inflim txt
 for all solutions of system (1.2)
corresponding to initial conditions (1.3).
Proof: Let
 

12
,
x
txtxt be any solution of
system (1.2) corresponding to initial conditions (1.3).
From Theorem 3.1, there is constant 0M such that
for any positive solution

x
t of system (1.2), there is a
0T such that

1, 2
i
xt Mi for all tT.
Therefore, from the second equation of system (1.2) we
have
  
 
22
22 12
2
d
d
xt atM
x
trt xt
tkt





(3.5)
for all tT
, where
 

1222
sup .
tR rtatMkt

For any tT
 and
,0s
 , integrating (3.5)
from ts to t we obtain
   
22 121
expexp .xts xts xt

 
Further, we have
   
 
222
22 12
2
dexp
d
xt atxt
xtrt
tkt






for all tT
. By Assumptions


13
HH and
Lemma 2.1, we can obtain that the component u of sys-
tem
  
 
2
212
2
dexp
d
uta tut
utrt
tkt






is permanent. Hence, using the comparison theorem, we
can obtain the component 2
x
of system (1.2) is perma-
nent. This completes the proof of this theorem.
In order to obtain permanence of component 1
x
of
system (1.2), we consider the following auxiliary system
with a parameter
   


222
22 24
2
dexp .
d
u
xt atxt
xtrt r
tkt

 



(3.6)
In particular, when 0
in system (3.6), we obtain
the following system
   


222
22 24
2
dexp .
d
u
xt atxt
xtrt r
tkt

 



(3.7)
By Assumptions


13
HH, we see that system
(3.7) satisfies all conditions of Lemma 2.1. Hence, by
Lemma 2.1, each positive of system (3.7) is globally
asymptotically stable. Let
*
20
x
t be some fixed solu-
tion of system (3.7) with initial value

*
20 00x. On
the permanence of component 1
x
for system (1.2), we
have the following result.
Theorem 3.3 Suppose that Assumptions

13
HH
hold and there is a constant 0
such that
 
 
1*
1202
1
linfd 0im ,
t
t
t
as
rsxss
ks





(3.8)
then the component 1
x
of system (1.2) is permanence.
Proof: Let

12
,
x
txtxt be any solution of
system (1.2) corresponding to initial conditions (1.3).
From Theorems 3.1 and 3.2, there are constants 0M
and 0m such that for any positive solution
x
t of
system (1.2), there is a 0T such that

1
x
tM
and
2
mxt M for all tT.
In fact, if inequality (3.8) is true, then by Assumption
3
H, we can choose enough small positive constants
01
,,

and 01
, and an enough large 0
TT
such that
 
 

1*
1102021
1
0
d
for all+.
t
t
as
rs bsx ss
ks
tT





(3.9)
For any 0
, let
2
x
t
be the solution of system
(3.6) with initial value
 
*
220
00xx
. Hence, by con-
clusion (b) of Lemma 2.1 and Lemma 2.2, there is a con-
stant 00
such that
 
*1
220
2
xt xt
for all 0t and
0
0,
.
Let
01
min ,

,

2
x
t
be any positive solu-
tion of the following system
  


222
22 24
2
dexp
d
u
xt atxt
xtrt r
tkt
 
(3.10)
with initial value

*
220
00xx
.
In the following, we will use two claims to complete
the proof of Theorem 3.3.
Claim 3.1 For the above constant
, there always
exist
1
suplim txt
 for any positive solution
x
t of system (1.2).
In fact, if Claim 3.1 is not true, then there is a positive
solution
12
,
x
txtxt of system (1.2) such that
1
suplim txt

. Hence, there is a 10
TT such that
1
xt
for all 1
tT. Further, using the comparison
theorem and Lemma 2.1, we can obtain that there is a
constant 21
TT such that
 
*
1
22 201
2
xtxtx t
 
(3.11)
for all 2
tT
. From the first equation of system (1.2)
we have
 
 

2
112
1*
11 221
1
exp d
t
T
xt xT
as
rsbsx ss
ks



L. HU ET AL.
Copyright © 2011 SciRes. AM
51
for all 2
tT
. By (3.9) it follows that

1
xt as
t. This is contradictory with

1
xt
for all
2.tT
 From this contradiction we finally conclude
that
1
suplim
txt

Therefore, Claim 3.1 is true.
Claim 3.2 There is a constant 0
such that

1
inflim txt
 for any positive solution
x
t of
system (1.2).
If Claim 3.2 is not true, then there is a sequence of
function

12
,: ,0,1,2
nnnin
Ci
 
 
such that for the solution
 

12
,,,
nn
xt xt of sys-
tem (1.2)

12
inf,, 1,2,.lim n
txt n
n
 
By Claim 3.1, for every n there are two time se-
quences


n
q
s
and


n
q
t, satisfying
   
11 22
0nn nnnn
qq
stst st
and

lim n
qq
s
 , such that




11
2
,, ,
nn
qn qn
xs xt
nn
 (3.12)
and

 

1
2,for all,.
nn
nqq
xtts t
n
n

 (3.13)
From the ultimate boundedness of system (1.2) and
Theorem 3.2, we can choose a positiv e constant

n
T for
every n such that

1,n
x
tM and

2,n
mxt M
for all

n
tT
. Further, there is an integer

10
n
K
such that
 
nn
q
sT
 for all

1n
qK. Let

1n
qK,
then for any
 
,
nn
qq
tst


we have

 


11
111 1
01
d, ,
d
,,
nn
n
xt atM
xtrt btM
tkt
xt

  



 
where
 
001111
suptrtbtMat ktM



. In-
tegrating the above inequality from

n
q
s
to

n
q
t, we
further h av e




 

11 0
,,exp .
nn nn
qnqnq q
xtxst s

 

Consequentl y , by (3. 12)
 

0
2exp .
nn
qq
ts
n
n




Hence,
 
1
0
ln for a. ll
nnn
qq n
ts qK
 (3.14)
By (3.9), there is constant P
such that
 
 

1*
11 221
1
d
t
t
as
rsbsx ss
ks





(3.15)
for all 2
tT and P
.
Let
2
x
t
be the solution of system (3.10) with ini-
tial value


22
,
nn
qqn
xs xs
. Since for any n, q
and
 
,
nn
qq
tst
we have

1,n
xtX
and
   


222
22 24
2
dexp ,
d
u
xt atxt
xtrt r
tkt

by the comparison theorem, we have
()()
22
,for all,.
nn
nqq
xtx ttst

 

(3.16)
Since

lim n
nq
s

and Theorem 3.2, there is con-
stant
 
21
nn
K
K for every n such that

2,
n
qn
x
sM

for all

2n
qK. By the comparison theorem and
2
x
t
is the globally uniformly attractive solution of
system (3.10), we obtain that there is a constant 32
TT
and such that
 

1
22 3
for all++.
2
n
q
xt xttTs

 (3.17)
By (3.14), there is an integer 01
NN such that
 
302
for all,. nn n
qq
tsT PnNqK

Further, by (3.11), (3.16) and (3.17) we ha ve

*
2201
,n
xtx t
 (3.18)
for all
 
3,
nn
qq
ts Tt

and 0
nN. H ence, when
0
nN and

n
qK, integrating the first equation of
system (1.2) from

3
n
q
sT
to

n
q
t, by (3.12), (3.13),
(3.15), and (3.18) we have


 



  




3
3
113
12
111 11
*
120 1
11
21
2
,,
(, )
exp(,)d
(, )
()
expd 8
.
n
q
n
q
n
q
n
q
nn
qn qn
t
n
nn
sT
t
sT
xtxs T
atxt
rt btxtt
xtk t
at xt
rtbtt pt
kt
n
n


 











L. HU ET AL.
Copyright © 2011 SciRes. AM
52
This leads to a contradiction with (3.12). Therefore,
Claim 3.2 is true.
Finally, from Claims 3.1 and 3.2 we see that Theorem
3.3 is proved and this completes the proof of this theo-
rem.
Remark 3.1 Nind ji n an d Azi z -Al aouiIn [11] discussed
the following system
  

  

112
1111 11
222
22
12
d
d.
d
d
xt axt
xt rbxt
txtk
xt axt
xtr
txtk











(3.19)
They stated that if
2
1
21 2112
1
,
r
r
rak erka
b



 (3.20)
then system (3.19) is permanent. We note that, when
system (1.2) degenerates into system (3.19), the condi-
tion (3.20) clearly implies the conditio n (3.8) in Theo rem
3.3. So the theorem of A. F. Nindjin, M. Aziz-AlaouiIn
(Theorem 5 in [11]) is a special case of Theorem 3.3. So
our results are fresh and more general.
A direct consequence of Theorem 3.3 is the following
result on the permanence of system (3.3) and (3.4).
Corollary 3.2 Suppose that Assumptions

13
HH
hold and there is a constant 0
such that
 
 
1*
12
1
ilnf ,imd 0
t
t
t
as
rsx s
ks




where

*
2
x
t is be any solution of the following system
   

222
22 2
d,
d
x
tatxt
xtrt
tkt





then system (3.3) is permanent.
Finally, we proceed to the discussion global stability
of any positive solution of system (1.2). We first derive
certain upperbou nd est imates for sol ut i on of system (1.2).
Theorem 3.4 Let
 
12
,
x
txtxt denote any
solutions of system (1.2) corresponding to initial condi-
tions (1.3). Suppose that Assumptions


13
H,H hold,
and 10
l
b, 20
l
a, then there is a constant 0T
such that if tT,
 
112 2
0,0 ,
x
tM xtM
where

2
1212
1
12
12
,.
u
ur
uu
r
u
ll
reM k
re
MM
ba
 (3.21)
The proof of Theorem 3.4 is similar to that of Theo-
rem 2.1 in [16], we therefore omit it here.
We now formulate the global stability of any positive
solutions of system (1.2).
Theorem 3.5 Let


***
12
,
x
txtxt denote any
positive solu tions of system (1.2). Suppose that Assump-
tions
13
H,H hold, and 10
l
b, 20
l
a, assume
further that

4
Hiim nf0li
tBt

where
 

 
 
 
 






 
  
1
1
1
34
3
12
11 2
1
22
211 1
1
2
11
111121
2
11
2
2322322
22 2
23 23
222
22
12
d
d
d
[]
[]
[
t
t
t
t
t
t
atM
Bt btkt
atM
rtbtMbs s
kt
at
btMMMbss
kt
at Mat Mas
s
ks
ktkt
at atM
Bt rt
Mkt





 
 












 
4
4
4
12
2
2
22
2
12242 2
12 242
121 1
12
d
d
d
]t
t
t
t
t
t
as
s
kt ks
atatMas s
kt ktks
at Mbss
kt







(3.22)
Then the solution


***
12
,
x
txtxt is globally
asymptotically stable.
Proof: Let
12
,
x
txt be any solution of system
(1.2) and (1.3). It follows from Theorem 3.4 that there
exist positive constants T and i
M
(defined by (3.21),
such that for all tT,

*
0,0,1,2.
iii i
xt Mxt Mi  (3.23)
We define

*
111 1
lnln .Vtxt xt
Calculating the upper right derivative of
11
Vt along
solutions of system (1.2), it follows that






 

 

 


*
11
*
1111*1
1
*
11
*
12 212 2
*111
111
*
11111
sgn
sgn
xt xt
DVtxtxtxt
xt
xt xt
atxt atxt
x
tkt
xt kt
bt xtxt



 





 






L. HU ET AL.
Copyright © 2011 SciRes. AM
53
 

 

 


 

  

 

**
11 11111
1*
12222
1
*
112222
*
221111
122
*
11 11
1
*
1111 *
11
sgn
sgn
xtxtbt xtxt
at ktxt xt
t
xtxtxt
xt xtxt
atxt
xt xtbtt
at
xt xtxt

 









 


 











 
  
  

 
1
1
*
2222
12 2*
111
1
*
111
1*
2222
1
d
t
t
kt
xt xt
atxt
btxt xt
t
btxu xuu
atxt xt
kt






 







(3.24)
where
 
*
1111111
txtktxtkt


 







*
2132132
.txt ktxt kt



 


On substituting (1.2) into (3.24), we derive that
  
  

 
   
  

   
 


1
11
12 2*
111
1
1*
2222
1
***
1111111
**
11 22
*
111
11111 1
112 2
111
1
1
d
|
t
t
DV t
atxt
btxt xt
t
atxt xt
kt
btruxu buxuxu
auxuxu
xu ku
ruxu buxuxu
auxuxu u
xu ku
a
bt


 






 


 
  

 
22
*
11
1
1*
2222
1
tx txt xt
t
atxt xt
kt






 

  

 
  


 

1
11111
112 2
1
**
112211
1
*
1112 2
1
*
1111
1*
1111 1
1
*
2222
d.
|t
t
btru buxu
au kuxu
u
x
uxu xuxu
au
buxu xuxu
u
xu xu
au kuxu xuxu
u
xuxuu





 
 



(3.25)
Define
 

 
 
 
  

  

1
1
12111 11
1122
1
**
112211
1
*
1112 2
1
1
**
1111 11
1
1
tt
ts
Vtbsrubuxu
au kuxu
u
xuxuxu xu
au
buxu xuxu
u
au
x
uxukuxu
u
xux




 

 






*
112222
dd.uxu xuus
 

(3.26)
We obtain from (3.25) and (3.26) that
  
  

 


 
  
  

1
11 12
12 2*
111
1
1*
2222
1
11111
1*
12 21122
1
1
**
11 11122
1
*
1111
d
t
t
DV tV t
atxt
btxt xt
t
atxt xt
kt
bss rtbtxt
at ktxtxt xt
t
at
xt xtbtxtxtxt
t
a
xt xt




 











  
 
1*
11
1
*
1112 22 2
.
tktxt
t
xtxtxtxt
 

(3.27)
L. HU ET AL.
Copyright © 2011 SciRes. AM
54
We now define
 

1111213
,VtVt VtVt (3.28)
where
 


1
11
211
1311111 2
2
11
*
11
dd
tl
tl
al
Vtbsbl MMM
kl
xlxlsl









(3.29)
and
 

 
 
 
2
12
22
12
*
1422
12
121
*
122
12
d
dd.
t
t
l
t
tl
as
Vtxs xss
ks
al M
bsxlxl sl
kl







(3.30)
It then follows from (3.23) and (3.27)-(3.30) that for
tT
,

 
  

 

 

 


1
1
1
12
2
1
12 12
1111
21
1
11
1111 12
2
11
2121
*
11112
12
*
122
12
d
d
d.
{
[
t
t
t
t
t
t
DV t
atM atM
btrtbtMkt
kt
at
bss btMMM
kt
at M
bssxt xtkt
at
bssxt xt
kt



  









 
(3.31)
Similarly, we define
 
22122
,VtV tV t (3.32)
where

*
2122
ln lnVtxtxt (3.33)
and
 
  


 






4
4
222
222 *
2132
22
*
22 *
132
*
2424
2
22
*
1313
2
dd.
tt
ts
as auM
Vt ru
ks
x
uku
auM
xu xuxu ku
xu xu
auM
x
uxu us
u













(3.34)
Calculating the upper right derivative of
2
Vt along
solutions of system (1.2), we derive for tT
 that

  


  










 
4
4
4
2
222
2
12 2
2*
22
2
2
22222
22
2
22
22
*
13132
2*
2424
2
d
d
d.
t
t
t
t
t
t
DVt
at atM
rt
Mkt kt
assxt xt
ks
atMatMas
s
ks
kt kt
atM
xt xtkt
assx tx t
ks


 





(3.35)
We define a Lyapuno v f unct ional

Vt as
 
1234
,VtVt VtVt Vt (3.36)
where


 




 
3
34
33
232
*
311
2
23
2
232
2*
11
2
223
d
dd
t
t
l
t
tl
as M
Vtxsxss
ks
al M
as
x
lxlsl
ks kl







(3.37)
and



4
44
22242
*
422
224
dd.
tl
tl
asal M
Vtxlxl sl
ks kl




(3.38)
It then follows from (3.22), (3.31), and (3.35)-(3.38)
that for tT

  
**
1112 22
.DVtBtxt xtBtxt xt
 
(3.39)
where
1
Bt and
2
Bt are defined in (3.22 ).
By Assumption
4
H, there exist positive constants
1
, 2
and *
TT
 such that if *
tT

0, 1,2.
ii
Bt i
 (3.40)
Integrating both sides of (3.39) on interval *,Tt
,
 

*
2**
1d.
t
iii
T
i
VtB sxsx ssVT

(3.41)
It follows from (3.40) and (3.41) that
L. HU ET AL.
Copyright © 2011 SciRes. AM
55
 

*
2***
1dfor all.
t
iii
T
i
Vtxsx ssVTtT
 
Therefore,

Vt is bounded on *,T


and also
 
** d,1,2.
ii
Txs xssi

By Theorem 3.4,


* 1,2
ii
xt xti are bounded
on *,T


.
On the other hand, it is easy to see that
*
i
x
t
and
 
1,2
i
xt i
are bounded for *
tT. Therefore,
 
* 1,2
ii
xt xti are uniformly continuous on
*,T


. By Barbalat’s Lemma ([17], Lemmas 1.2.2 and
1.2.3), we conclude that
 
*
lim0,1, 2.
ii
txt xti
 
This completes the proof of this theorem.
Remark 3.2 If time delays 1
, 233
,,

and 4
are
naturally subject to fluctuation in time in system (1.2).
Similar Theorem 3.1-3.5, we can obtain the sufficient
conditions on the permanence and globally asymptoti-
cally stable of any positive solutio ns for system (1.2).
Finally, we give some examples to illustrate the feasi-
bility of our main results on the permanence of system
(1.2).
Example 3.1 In system (1.2), let 0.2
10.2 0.05re
0.1sin ,t 10.9cos ,bt 20.4,r
12 1
1, 2,aa k
122
0.1, 0.5, 1k
. It is easy to verify that coeffi-
cients of system (1.2) satisfy (3.8). By Theorem 3.2 and
3.3, system (1.2) is permanent.
Example 3.2 In system (1.2), let 0.2
10.2re,
10.1b, 12
1aa, 12k, 20.4r, 10.1,
20.5
, 21k. By Theorem 3.2 we see that the com-
ponent 2
x
of system (1.2) is permanent. However, it is
easy verify that
24 0.2 0.2
1122 12
0.20.42 0
r
rarke kaee

thus (3.8) does not hold for system (1.2) and we cannot
get any information by Theorem 3.3. In this case, we
note that 0.2
112212
0.20.4 20rarkkae and nu-
merical simulation suggests that system (1.2) with a se-
quence initial condition

12
,
is permanent.
In the example 3.2, from numerical simulation, we
note that the time delays are harmless for the permanence.
Therefore, as an improvement of Theorems 3.2 and 3.3,
we give the following interesting conjecture.
Conjecture: Suppose the assumptions of Corollary 3.2
hold, then system (1.2) is permanent.
4. Acknowledgements
This work was supported by the National Natural
Science Foundation of P.R. Chin a (11001235, 10961022)
and the Natural Science Foundation of Xinjiang Univer-
sity (BS100104, BS080105).
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