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ISSN Online: 2327-4379 ISSN Print: 2327-4352

DOI: 10.4236/jamp.2018.66116 Jun. 28, 2018 1388 Journal of Applied Mathematics and Physics

The Dynamics of an Impulsive Competitive

System with Infinite Delay and Diffusion

Hairu Chen, Yuanfu Shao

*

College of Science, Guilin University of Technology, Guilin, China

Abstract

In this paper, we consider an impulsive competitive system with infinite delay and diffusion. Firstly, on basis of inequality estimation techniques and com-parison theorem of impulsive differential equations, we obtain some sufficient conditions for the permanence and extinction of the system. Then, we estab-lish sufficient conditions for the globally attractive of the system by con-structing appropriate Lyapunov function. Besides, under different impulsive conditions, we discuss the effect of time delay and diffusion on dynamic be-havior of the competitive system.

Keywords

Diffusion, Infinite Delay, Permanence, Extinction, Attractive

1. Introduction

In practical world, owing to many natural and man-made factors (e.g., fire, drought, flooding, crop-dusting, deforestation, hunting, harvesting, etc.), the bi-ological species or ecbi-ological environments usually undergo some discrete changes of relatively short duration at some fixed times. Such sudden changes can often be characterized mathematically in the form of impulses. With the de-velopment of impulsive differential equations, many experts have adequate ma-thematical models to investigate the dynamical behaviors of such ecosystems with impulsive effects [1] [2] [3] [4] [5]. On the other hand, the Lotka-Volterra competition systems are very important and significant mathematical models in a non-autonomous environment. Many interesting results of the competitive systems on the existence of positive periodic solutions, permanence, extinction, global stability had been studied extensively (see [6] [7] [8] [9] [10]). For exam-ple, Wang [10] investigated the following competitive system with impulsive

ef-How to cite this paper: Chen, H.R. and Shao, Y.F. (2018) The Dynamics of an Impulsive Competitive System with Infinite Delay and Diffusion. Journal of Applied Mathematics and Physics, 6, 1388-1407. https://doi.org/10.4236/jamp.2018.66116

Received: May 31, 2018 Accepted: June 25, 2018 Published: June 28, 2018

Copyright © 2018 by authors and Scientific Research Publishing Inc. This work is licensed under the Creative Commons Attribution International License (CC BY 4.0).

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DOI: 10.4236/jamp.2018.66116 1389 Journal of Applied Mathematics and Physics

fects:

( )

( ) ( )

(

( ) ( )

( ) ( )

)

( )

( ) ( )

(

( ) ( )

( ) ( )

)

( )

(

) ( )

( )

(

) ( )

1 11 12

2 21 22

,

1

, , 1,2, .

1

k

k k k

k

k k k

u t u t b t a t u t a t v t

t t

v t u t b t a t u t a t v t

u t h u t

t t k

v t g v t

+

+

 ′ = − − 

 ′ = − − 

= +

 =

=

 

= +



The author obtained sufficient conditions on the uniform persistence and ex-tinction of the system by applying the theorem of differential equations.

In ecological environment, because of the natural enemy, severe competition, deterioration of the patch environment, spatial heterogeneity and human activi-ties, species dispersal in two or more patches becomes one of widespread phe-nomena of nature. It is an important subject to study the effects of dispersion on the dynamics of species living in patchy environments. Many works on popula-tion dynamics in patch environment have been investigated [11] [12] [13] [14]. Moreover, in real ecology environment, the existed number on the history will affect indirectly the number of the species at the moment. Therefore, in order to establish more realistic models, the past history of systems should be taken into account, which has led to the introduction of time-delays in differential equa-tions. Such biological system with infinite delay can be found in [15] [16] [17].

Motivated by above arguments, we establish an impulsive competitive system with infinite delay and diffusion as follows:

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( ) ( )

(

( )

)

( )

( ) ( )

(

( ) ( )

)

( ) ( )

(

( )

)

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( )

( )

( )

( )

( )

( )

0

1 1 1 1 1 1 1

12 2 1

2 2 2 2 2 21 1 2

0

3 3 2 2 1

1 1 1

2 2 2

d

,

d

, 1,2,

k

k k k

k k k

k k k

x t x t a t b t x t c t k s y t s s

D t x t x t

t t

x t x t a t b t x t D t x t x t

y t y t a t b t y t c t k s x t s s

x t h x t

x t h x t k

y t g y t

−∞

−∞

+

+

+

= +

 

+

 ≠

 ′ = − + −

 ′ = − − + 

 = 

 

= =

=

 

(1.1)

where x t ii

( )(

=1,2

)

and y t

( )

represent the population densities at time t,

respectively. Let 0= < <t0 tk tk+1,k=1,2, and tk→ ∞ as k→ ∞. Species 1

x competes with y in patch 1, while x1 can disperse between patch 1 and

patch 2, and y is confined to patch 1. D t D t12

( )

, 21

( )

denotes the diffusion

coef-ficients of species x. h h1k, 2k and gk are impulsive coefficients at time tk,

re-spectively.

We consider system (1.1) with the following initial conditions

( )

( )

( )

( )

( )

( )

(

)

(

]

[

)

1 1 , 2 2 , 3 ,

, , 1,2,3, ,0 , 0, .

i

x x y

PC R R i R R

θ

φ θ

θ

φ θ

θ

φ θ

φ

+ − + − +

= = =

∈ = = −∞ = +∞ (1.2)

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DOI: 10.4236/jamp.2018.66116 1390 Journal of Applied Mathematics and Physics

for i=1,2,3. PC is the space of bounded function φ

( )

s : R R3

−→ which is

continuous everywhere expect at the point t t= ∈k I and

φ

( ) ( )

tk+ ,

φ

tk− exists

with

φ

( )

tk− =

φ

( )

tk and with norm sup

R θ

θ

φ φ

= .

In this paper, for any continuous function f t

( )

, we denote

( )

maxi I

{

i

( )

}

f t f t

= , f t

( )

=mini I

{

f ti

( )

}

.

Throughout this paper, we assume that the system (1.1) satisfies ((C1), (C2) see [12], (C3) see [17]):

(C1) all functions are positive, continuous and bounded defined on R+,

( )

( )

12 21

0<D t D t, ≤D.

(C2) h h1k, 2k and gk are positive constants for all

k

=

1,2,

.

(C3) k s ii

( )(

=1,2

)

is a non-negative, piece-wise continuous function

de-fined on R− and satisfy 0 k s si

( )

d 1

+∞

=

.

Applying some inequality techniques, comparison theorem of impulsive dif-ferential equations and Lyapunov function, we study the dynamic behaviors of an impulsive competitive system with infinite delay and diffusion, included permanence, extinction and globally attractive. This paper is organized as fol-lows. Section 2 contains some preliminaries and presents the proof of the lem-ma. In Section 3, we establish some sufficient conditions which guarantee the system is permanence. In finally section, we give some conditions on the extinc-tion of the system. In Secextinc-tion 4, we study the globally attractive of system (1.1).

2. Preliminaries

We consider the following impulsive non-autonomous logistic model

( )

( ) ( )

(

( ) ( )

)

( )

( )

,

, 1,2, ,

k

k k k

x t x t t t x t t t

x t h x t k

α β

+

 ′ = − ≠

 

= =

  (2.1)

where α

( )

t and β

( )

t are bounded and continuous functions defined onR+,

( )

t 0

β ≥ for all t R∈ + and impulsive coefficients hk are positive constants

for any k=1,2,. Then we have the following Lemma 2.1.

Lemma 2.1. Suppose that there is a constant σ >0 such that

( )

(

)

liminf tt d 0

t s s

σ

β

+

→∞

> (2.2)

( )

liminf d ln 0

k t

k t

t s s t t t f

σ

σ

α

+

→∞ ≤ < +

 

+ >

 

 (2.3)

and function

( )

, ln

k

k t t t

h t h

µ

µ ≤ < +

=

(2.4)

is bounded on t R∈ + and µ∈

[

0,σ

)

. Then we have

1) There exist constant M >0 and m>0 such that

( )

( )

liminf limsup

t t

m x t x t M

→∞ →∞

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DOI: 10.4236/jamp.2018.66116 1391 Journal of Applied Mathematics and Physics

for any positive solution x t

( )

of system (2.1). 2) If all conditions of (1) hold, further if

( )

1

limsup d ln 0

k t

k t

t t t t

s s f

σ

σ

α

+

→∞ ≤ < +

 

+ ≤

 

 (2.6)

then we have lim

( )

0

t→∞x t = for any positive solution x t

( )

of system (2.1).

The proof of this Lemma can be found in [18], here we omit it.

Next we consider the following impulsive periodic single species logistic sys-tem with diffusion

( )

( ) ( )

(

( )

)

(

( )

( )

)

( )

( )

1 , ,

, 1,2, , , 1,2, ,

n

i i i i ij j i k

j i k ik i k

x t x t r t a t D x t x t t t

x t h x t i n k

= +

 ′ = − + − ≠

 

= = =

 

(2.5)

Assume that r t a t D t i j Ii

( ) ( )

, i , ij

( )(

, ∈

)

are positive, continuous and

bounded functions defined on R+. D2≥DijD1>0

(

i j

)

, Dii=0 for all

(

)

, 1,2, ,

i j I I∈ =  n and t R∈ +, hik >0 for all i I∈ ,

k

=

1,2,

, then we

have the following conclusions.

Lemma 2.2. Suppose that there is a positive constant σ such that

( )

(

)

liminf tt d 0

t a s s

σ +

→∞

> (2.6)

( )

( )

1

liminf d ln 0

k n

t

ij k

t

t r t j D t t t t t h

σ

σ +

→∞ = ≤ < +

 

− + >

 

 (2.7)

and function

( )

, ln

k

k t t t

h t h

µ

µ ≤ < +

=

,

( )

, ln

k k t t t

h t h

µ

µ

≤ < +

=

(2.8) is bounded on t R∈ + and µ∈

[

0,σ

)

. Then we have

1) There are constants M >0 and m>0 such that

( )

( )

liminft i limsup i t

m x t x t M

→∞ →∞

≤ ≤ ≤

for any positive solution x ti

( )

of system(2.1). t R i I∈ +, ∈ .

2) If all conditions of (1) hold, further if

( )

(

1

)

liminf tt d 0

t t t

σ

β

+

→∞

> , (2.9)

where 1

( )

( )

( )

1

min n ij 0

i

i I j

D t

t a t

m

β

=

 

 

=

 

 for all t R i j I∈ +, , ∈ , then system

(2.2) is globally attractive.

Proof: Firstly, we prove system (2.5) is permanent. Let

(

x t1

( )

, , x ti

( )

)

be

any solution of system (2.5). Define the function V t1

( )

=maxi I

{

x ti

( )

}

, when k

t tcalculating the upper-right derivative of V t1

( )

, we have

( )

( ) ( )

(

( ) ( )

)

( ) ( ) ( ) ( )

(

)

1 i i i i 1 1

D V t+ x t r t a t x t V t r t a t V t

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DOI: 10.4236/jamp.2018.66116 1392 Journal of Applied Mathematics and Physics

( )

{

( )

}

{

( )

}

{ }

{

( )

}

( )

1 k maxi I i k maxi I ik i k maxi I ik maxi I i k k 1 k

V t+ x t+ h x t h x t h V t

∈ ∈ ∈ ∈

= = ≤ =

Consider the following auxiliary system

( )

( ) ( )

(

( ) ( )

)

( )

( )

, , 1,2,

k

k k k

D w t w t r t a t w t t t

w t h w t k

+

+

 = − ≠

 

= =

  (2.10)

with initial condition w

( )

0 =V1

( )

0 . Obviously, from condition (2.6), (2.8) and

Lemma 2.1, there exists a constant M >0 such that limsup

( )

t→∞ w tM . Then

according to comparison theorem of impulsive differential equations, we derive

( )

1

( )

( )

limsup i limsup limsup

t→∞ x tt→∞ V tt→∞ w tM for i I∈ . (2.11)

Now we prove there is a constant m>0 such that liminf i

( )

t→∞ x tm. Defined

( )

{

( )

}

2 mini I i

V t x t

= , calculating the right-lower derivative of V t2

( )

when k

t t≠ , similar to above conclusion, we can obtain

( )

( ) ( )

(

( ) ( )

)

( ) ( ) ( ) ( )

(

)

2 i i i i 2 2

D V t+ x t r t a t x t V t r t a t V t

when t t= k, we have

( )

{ }

{

( )

}

{ }

{

( )

}

{ }

{ }

{ }

{

( )

}

( )

2 k imin= 1,2 i k imin= 1,2 ik i k imin= 1,2 ik imin= 1,2 i k k 2 k

V t+ = x t+ = h x t h x t =h V t

by comparison theorem of impulsive differential equations, we derive

( ) ( )

2

V tv t for all t R∈ +, where v t

( )

is the solution of the auxiliary equation

( ) ( ) ( ) ( ) ( )

(

)

( )

( )

2 ,

, 1,2, ,

k

k k k

D v t v t r t a t v t t t

v t h v t k

+

+

 = − ≠

 

= =

  (2.12)

with initial condition V2

( )

0 =v

( )

0 . Clearly, from condition (2.7), (2.8) and

Lemma 2.1, there is a constant m>0 such that liminf

( )

t→∞ v tm. Therefore we

have

( )

2

( )

( )

liminf i liminf liminf

t→∞ x tt→∞ V tt→∞ v tm for i I∈ .

Next we consider the globally attractive of system (2.5). Construct a Lyapunov function

( )

( )

( )

1

ln ln

n

i i

i

V t x t x t

=

=

− 

when t t= k, we always have

( )

( )

( )

( )

1

ln ln

n

k ik i k ik i k k

i

V t h x t h x t V t+

=

=

−  =

then V t

( )

is continuous for all t R∈ +. In addition, when t R∈ + and t tk

we have

( )

( )

( )

( )

( )

( )

1 ln ln 1

i i i i i i

x t x t x t x t x t x t

B − ≤ −  ≤A − (2.13)

Moreover, calculating the derivative of V t

( )

, we also have

( )

(

( )

( )

)

( )

( )

( )

( )

( ) ( )

( )

(

)

( )

1 1

1

1 1 1

sgn

n

i i

i i i

n n n

i i i ij

i i j

x t x t

D V t x t x t

x t x t

a t x t x t D t

+

=

= = =

 ′ ′ 

= −  − 

 

≤ − − +

∑∑

 

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DOI: 10.4236/jamp.2018.66116 1393 Journal of Applied Mathematics and Physics

where

( )

( )

( )

( )

( )

( )

( )

( )

( )

( )

( )

( )

( )

( )

( )

, ,

, .

j j

ij i i

i i

ij

j j

ij i i

i i

x t x t

D t x t x t

x t x t

D t

x t x t

D t x t x t

x t x t

  

− >

 

  

= 

 

<

 

  

 

 

 

For all t R∈ +, we think about under the following two cases:

Case 1: if x ti

( )

>x ti

( )

, then

( )

ij

( )

( )

(

( )

( )

)

ij

( ) ( ) ( )

ij j j j j

i

D t D t

D t x t x t x t x t

x t A

≤ − ≤ −

Case 2: if x ti

( )

<x ti

( )

, then

( )

ij

( )

( )

(

( )

( )

)

ij

( ) ( ) ( )

ij j j j j

i

D t D t

D t x t x t x t x t

x t A

≤  − ≤ −

From Case 1, Case 2 and (2.14), we can obtain

( )

(

( ) ( )

( )

)

( )

( )

( )

( )

( )

( )

( )

1 1 1

1 1

n n n

ij

i i i j j

i i j

n n ij

i i i

i j

D

D V t a t x t x t x t x t

A D

a t x t x t

A t AV t

β +

= = =

= =

≤ − − + −

 

≤ −

 

≤ −

∑∑

 

 (2.15)

By (2.15) and condition (2.9), we have V t V

( )

( )

0 exp

(

A

0t

β

( )

s sd

)

→0

as t→ ∞. Furthermore, by (2.13), we have tlim→∞

(

x ti

( )

x ti

( )

)

=0, that is,

sys-tem (2.5) has globally attractive positive solution. This completes the proof of Lemma 2.2.

3. Permanence

Note that system (1.1) always has a positive solution for all t R∈ + if it has a

positive initial condition. Here we state and prove the permanent of system (1.1).

Theorem 3.1. There exists a constant M >0 such that limsup i

( )

t→∞ x tM

and limsup

( )

t→∞ y tM for any positive solution of system (1.1) if there exists a

constant ω>0 such that

( )

(

)

liminf tt d 0

t b s s

ω +

→∞

> (3.1)

( )

(

3

)

liminf tt d 0

t b s s

ω +

→∞

> (3.2)

and function

( )

, ln

k

k t t t v

h t µ h

≤ < +

=

,

( )

, ln

k

k t t t

g t g

µ

µ ≤ < +

=

(3.3) are bounded on t R∈ + and µ∈

[

0,ω

)

for all t R k∈ +, =1,2,.

Proof. Firstly, we prove that there is a constant M1>0 such that

( )

1

(

)

limsup i 1,2

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DOI: 10.4236/jamp.2018.66116 1394 Journal of Applied Mathematics and Physics

have two cases when t tk.

1) If V t

( )

=x t1

( )

, we have

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( ) ( )

(

( )

)

( ) ( )

(

( ) ( )

)

( ) ( )

(

( ) ( )

)

0

1 1 1 1 1 1

12 2 1

1 1 1 1

d

D V t x t a t b t x t c t k s y t s s

D t x t x t

x t a t b t x t V t a t b t V t

+

−∞

= − − +

+ −

≤ −

≤ −

(3.4)

2) If V t

( )

=x t2

( )

, we have

( )

( ) ( )

(

( ) ( )

)

( ) ( )

(

( )

)

( ) ( )

(

( ) ( )

)

( ) ( ) ( ) ( )

(

)

2 2 2 2 21 1 2

2 2 2 2

D V t x t a t b t x t D t x t x t

x t a t b t x t V t a t b t V t

+ = +

≤ −

≤ −

(3.5)

clearly, from (3.4) and (3.5), we get

( )

( ) ( ) ( ) ( )

(

)

D V t+ V t a t b t V t for all t R

+

On the other hand, when t t= k, we have

( )

{ }

{

( )

}

{ }

{

( )

}

{ }

{ }

{ }

{

( )

}

( )

1,2 1,2 1,2 1,2

max max max max

k i i k i ik i k i ik i i k k k

V t+ x t+ h x t h x t h V t

= = = =

= = ≤ = .

Consider the following auxiliary equation

( ) ( ) ( ) ( ) ( )

(

)

( )

( )

,

, 1,2,

k

k k k

D v t v t a t b t v t t t

v t h v t k

+ +

=

 

= =

  (3.6)

with initial condition v

( )

0 =V

( )

0 . Since the condition of Lemma 2.1 holds from (3.1) and (3.3), using Lemma 2.1, we get that there exists a constant

1 0

M > such that limsup

( )

1

t→∞ v tM . Applying the comparison theorem of

im-pulsive differential equation, we obtain V t

( ) ( )

v t for all t R∈ +. Finally, we

have

( )

( )

( )

1

limsup i limsup limsup

t→∞ x tt→∞ V tt→∞ v tM for i=1,2 (3.7)

Then we prove that there is a constant M2>0 such that limsup

( )

2

t→∞ y tM .

From the third and sixth equations of system (1.1), we obtain

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( ) ( )

(

( ) ( )

)

( )

( )

0

3 3 2 2 1

3 3

d ,

, 1,2,

k

k k k

y t y t a t b t y t c t k s x t s s

y t a t b t y t t t

y t g y t k

−∞

+

 ′ = − − −

 

= =

 

considering the following subsystem

( )

( ) ( )

(

( ) ( )

)

( )

( )

3 3 ,

, 1,2,

k

k k

u t u t a t b t u t t t

u t+ g u t k

 ′ = − ≠

 

= =

  (3.8)

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DOI: 10.4236/jamp.2018.66116 1395 Journal of Applied Mathematics and Physics

( )

2

limsup

t→∞ u tM . Similar to the prove process of the bounded of species x, we

have limsup

( )

2

t→∞ y tM .

Let M=max

{

M M1, 2

}

, evidently, we have

( )

(

)

limsup i 1,2

t→∞ x tM i= , limsupt→∞ y t

( )

M

The proof of Theorem 3.1 is completed.

Theorem 3.2. Assume that all conditions of Theorem 3.1 are satisfied. In ad-dition, there is a constant ω>0 such that

( )

liminf d ln 0

k t

k t

t a s s t t t h

ω

ω +

→∞ ≤ < +

 

+ >

 

 (3.9)

( )

( )

( ) (

(

)

)

(

0 *

)

3 2 2 1

liminf d d ln 0

k t

k t

t a t c t k s x t s s s t t t g

ω

τ ω

+

→∞ ≤ < +

 

− + + >

 

 (3.10)

( )

(

2

)

liminf tt d 0

t t t

ω

β

+

→∞

> (3.11)

and function

( )

, ln

k k t t t

h t h

µ

µ

≤ < +

=

,

( )

, ln

k

k t t t

g t g

µ

µ ≤ < +

=

(3.12)

are bounded on t R∈ + andµ∈

[

0,ω

)

, where

( )

( )

2

( )

(

)

2 =1,2

1

min ij 0

i

i j

D t

t a t i j

p

β

=

 

 

= ≥ ≠

 

 for all t R∈ +.

Then the system is permanent.

Proof. Above all, we must prove that there exists a constant m>0 such that

( )

(

)

liminft→∞ x tim i=1,2 , liminft→∞ y t

( )

m.

Firstly, we prove liminft→∞ x ti

( )

m i

(

=1,2

)

. Defined V t

( )

=min

{

x t x t1

( ) ( )

, 2

}

and

(

) (

)

{

}

sup i , : , , 1,2

H = x t s y t s t R s R i+ + ∈ + ∈ − = (3.13)

When t tk, consider the following two cases.

Case 1: If V t

( )

=x t1

( )

, we can choose a constant τ>0 such that

( )

1 d

H

−∞−τk s s M< , then we have

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( ) ( )

(

( )

)

( ) ( )

(

( ) ( )

( )

(

( ) (

)

( ) (

)

))

( ) ( )

(

( )

)

0

1 1 1 1 1 1

12 2 1

1 1 1 1 1 1

0

1 12 2 1

d

d d

V t x t a t b t x t c t k s y t s s

D t x t x t

x t a t b t x t c t k s y t s s

k s y t s s D t x t x t

τ

τ

−∞

− −∞

′ = − − +

+ −

= − − +

+ + + −

( ) ( )

(

( ) ( )

( )

(

( )

( ) (

)

)

)

( ) ( )

(

( )

( ) ( )

)

( ) ( )

(

( )

( ) ( )

)

0

1 1 1 1 1 1 1

1 1 1 1 1

1

d d

2

2 ,

x t a t b t x t c t H k s s k s y t s s

x t a t c t M b t x t

V t a t c t M b t V t

τ

τ

−∞ −

≥ − − + +

≥ − −

≥ − −

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DOI: 10.4236/jamp.2018.66116 1396 Journal of Applied Mathematics and Physics

( )

( ) ( )

(

( ) ( )

)

( ) ( )

(

( )

)

( ) ( )

(

( ) ( )

)

( ) ( ) ( ) ( )

(

)

2 2 2 2 21 1 2

2 2 2 2

.

V t x t a t b t x t D t x t x t

x t a t b t x t V t a t b t V t

′ = − + −

≥ −

≥ −

By Case 1 and Case 2, we derive V t V t a t b t V t

( )

( ) ( ) ( ) ( )

(

)

. When t t= k, we can obtain

( )

k imin{ }1,2

{

i

( )

k

}

imin{ }1,2

{

ik i

( )

k

}

imin{ }1,2

{ }

ik imin{ }1,2

{

i

( )

k

}

k

( )

k

V t+ x t+ h x t h x t h V t

= = = =

= = ≥ = .

Research the following equation with impulsive

( ) ( ) ( ) ( ) ( )

(

)

( )

( )

, , 1,2,

k

k k

v t v t a t b t v t t t

v t+ h v t k

 ′ = − ≠

 

= =

  (3.14)

By condition (3.9) and (3.12), we know that condition of Lemma 2.1 is satis-fied. Consequently, there exists a constant m1>0 such that

( )

( )

( )

1

liminf i liminf liminf

t→∞ x tt→∞ V tt→∞ v tm for i=1,2. (3.15)

Then we investigate the following system:

( )

( ) ( )

(

( ) ( )

)

( ) ( )

(

( )

)

( )

( ) ( )

(

( ) ( )

)

( ) ( )

(

( )

)

( )

( )

( )

( )

1 1 1 1 1 12 2 1

2 2 2 2 2 21 1 2

1 1 1

2 2 2

,

, 1,2, ,

k

k k k

k k k

u t u t a t b t u t D t u t u t

t t

u t u t a t b t u t D t u t u t

u t h u t

k

u t h u t

+

+

 ′ = − + − 

 ′ = − + − 

=

 =

 

=



(3.16)

From Lemma 2.2 and condition (3.1), (3.10), (3.12) and (3.13), we can know that there are positive constants p and P such that

( )

* i p x t≤ ≤P

where *

( )(

1,2

)

i

x t i= is globally attractive for the system (3.16). In addition, we assume that

(

u t u t1

( ) ( )

, 2

)

is a positive solution of system (3.16) with initial

condition ui

( )

0 =xi

( )

0 . Evidently, we obtain that there exists a constant

0 0

ε > small enough such that

( )

( )

( )

* *

0 0

i i i

x t −ε ≤u tx t (3.17)

Similar to the discussion in [18], we obtain that condition (3.10) is indepen-dent of the choice of *

( )

i x t .

From condition (3.10), there are constant ε >0 0 small enough and T>0

large enough such that

( )

( )

( )

( )

( ) (

(

)

)

(

0 *

)

3 3 0 2 0 2 2 1

0

2 d d

ln k

t t

k t t t

a t b t c t c t k s x t s s s

g

ω

τ

ω

ε ε

ε +

≤ < +

− − − +

+ >

(3.18)

for all t T. By (3.12), we can get a positive constant G such that

( )

, ln

k k t t t

g t g G

µ

µ

≤ < +

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DOI: 10.4236/jamp.2018.66116 1397 Journal of Applied Mathematics and Physics

From system (1.1), we consider the following subsystem,

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( ) ( )

(

( )

)

( )

( ) ( )

(

( ) ( )

)

( ) ( )

(

( )

)

( )

( )

( )

( )

0

1 1 1 1 1 1 1

12 2 1

2 2 2 2 2 21 1 2

1 1 1

2 2 2

d ,

, 1,2, .

k

k k k

k k k

x t x t a t b t x t c t k s y t s s

D t x t x t t t

x t x t a t b t x t D t x t x t

x t h x t

k

x t h x t

−∞ + +  = +     +     ′ = − + −   = == 

By (3.16), (3.17) and comparison theorem of impulsive differential equations, we get that

( )

( )

*

( )

1 1 1 0

x tu tx t for all t T T≥ ≥1 . (3.20)

Next we prove there is a constant m2>0 such that liminft→∞ y t

( )

m2.

In the beginning, we prove limsup

( )

0

t→∞ y t

ε

. Suppose that the proposition is

not true, we have limsup

( )

0

t→∞ y t <

ε

, that is y t

( )

<ε0 for all t T T≥ 2> 1.

Fur-thermore, we can choose a constant τ>0 such that

( )

2 d 0

H

−∞−τk s s≤ε (3.21) Consequently, we have

( )

( ) ( )

(

( ) ( )

( )

(

( )

( ) (

(

)

)

)

)

( ) ( )

(

( )

( )

( )

( ) (

(

)

)

)

0 *

3 3 2 2 2 1 0

0 *

3 3 0 2 0 2 2 1

d d

2 d

y t

y t a t b t y t c t H k s s k s x t s s

y t a t b t c t c t k s x t s s

τ τ τ ε ε ε − −∞ − − ′ ≥ − − + + + ≥ − − − +

(3.22)

For any t T≥ +2 τ and t tk, we can choose an integer l≥0 such that 2

t T= + +τ lω+v, where v

[

0,ω

)

is a constant. Integrating (3.22) from

2

Tto t, due to (3.18) and (3.19), we derive

( )

(

)

(

( )

( ) ( )

( )

( ) (

)

)

(

)

(

( )

( )

( )

( )

( ) (

)

)

2 2 2 2

2 3 3

0

2 2 1

2 3 3 0 2 0

0 *

2 2 1

exp

d d ln

exp 2 d ln k k t T k T t t t

T

k T t t

y t y T a t b t y t

c t k s x t s s s g

y T a t b t c t

c t k s x t s s g

τ

τ

τ

τ τ

τ

τ ε ε

+

−∞ + ≤ <

+

+ ≤ <  ≥ + −   − + +    ≥ + − −   − + +  

(

)

( )

(

( )

( )

( )

( )

( ) (

)

)

( )

(

)

(

)

2 2

2 2 2

2 2 2 2 2

2 1 3 3 0

0 *

2 0 2 2 1

1 2 0 exp 2 d ln exp ,

k k k

T T l t

T T l T l

k T t T T l t T l T l t t

y T a t b t

c t c t k s x t s s

g

y T l G

τ ω τ ω

τ τ ω τ ω

τ

τ τ ω τ ω τ ω τ ω

τ ε

ε

τ ε βω

+ + + +

+ + + − + +

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DOI: 10.4236/jamp.2018.66116 1398 Journal of Applied Mathematics and Physics

where

(

( )

( )

( )

( )

0

( ) (

*

)

)

3 3 0 2 0 2 2 1

sup 2 d

t R a t b t c t c t τk s x t s s

β ε ε

+ −

= + + +

+ .

There-fore, we can get y t

( )

→ ∞ as t→ ∞ , which is contradiction with

( )

0

limsup

t→∞ y t <

ε

. Obviously, we have

( )

0

limsup

t→∞ y t

ε

.

Then we prove there exists a constant α>0 such that liminf

( )

t→∞ y t ≥α.

As-sume that the proposition is not true, then there exists a sequence

( )

{

φm t

}

PC m+, =1,2, such that liminft y t

(

, k

)

k02

ε

φ

→∞ ≤ for all

k

=

1,2,

.

From (3.19), we have

eG eG

k

g

. (3.23)

we choose an integer K>eG such that for all k K and any solution y t

( )

of system (1.1) satisfied: 1) If

( )

0

l y t

k

ε

≥ , then

( )

( )

0 0

2

e G

l k l

y t g y t

k k

ε

ε

+ = , for some

1,2,

l= ,

2) If

( )

0 2 l y t

k

ε

, then

( )

( )

0 0

2

eG

l k l

y t g y t

k k

ε

ε

+ =

, for some l=1,2,. From above inequality, there exist two time sequences

{ }

( )k

q

s and

{ }

( )k q t

such that for each

k K

= +

1,

K

+

2,

, we have

( ) ( ) ( ) ( ) ( ) ( )

1 1 2 2

0 k k k k k k

q q

s t s t s t

< < < < << < <

and

( )

{ }

k ,

{ }

( )k

q q

s → ∞ t → ∞ as t→ ∞ (3.24)

( )

(

)

0 0

(

( )

)

0

2

, , , ,

k k

q k q k

y s y s

k k k

ε ε

ε

φ

< +

φ

(3.25)

( )

(

)

(

( )

)

0 0 0

2 , , , 2,

k k

q k q k

y t y t

k

k k

ε

φ

<

ε

+

φ

ε

(3.26)

(

)

0 0

2 y t, k k k

ε

φ

ε

for all

(

( ) ( )k, k

)

.

q q

ts t (3.27)

Let ( )k sup

{

(

,

) (

, ,

)

: , , 1,2

}

i k k

H = x t s+ φ y t s+ φ t R s R i∈ + ∈ − = for each

1, 2,

k K= + K+ , we choose a constant

τ

( )k >0 such that

( ) (

)

( ) ( )

( )

( )

1 , d d 0

k k

k k

k s x t s s H k s s

τ τ

φ ε

− −

−∞ + ≤ −∞ <

, (3.28)

by (3.20), for each k K= +1,K+2,, there is a T1( )k >T such that

(

)

*

( )

1 , k 1 0

x tφ ≤x t for all t T 1( )k . (3.29)

Clearly, from (3.22), there is an N1( )k >0 such that sq( )k >T1( )k +

τ

( )k for

( )

1k

q N≥ . Hence for any k, k q q

t∈ s t and t tl, q N 1( )k . By (3.27) and (3.28),

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DOI: 10.4236/jamp.2018.66116 1399 Journal of Applied Mathematics and Physics

(

)

(

) ( )

(

( ) (

)

( )

( ) (

)

)

(

) ( )

( ) (

)

( )

( )

( ) (

)

( ) (

(

)

)

( ) 0

3 3 2 2 1

3 3 2 2 1

0 *

2 1 0

, , , , d

, , , d

d

k

k

k k k k

k k k

y t y t a t b t y t c t k s x t s s

y t a t b t y t c t k s x t s s

k s x t s s

τ

τ

φ φ φ φ

φ φ φ

ε −∞ − −∞ − ′ = − − +   ≥ − − +     + + +  

(

) ( )

( )

( )

( ) ( )

( )

( ) (

(

)

)

( )

(

) ( )

(

( )

( )

( ) (

)

)

3 3 0 2 2

0 *

2 1 0

0 *

3 3 0 2 0 2 1

, d

d

, 2 d ,

k

k

k k

k

y t a t b t c t H k s s

k s x t s s

y t a t b t c t k s x t s s

τ

τ

φ ε

ε

φ ε ε

− −∞ − −∞   ≥ − −     + + +   ≥ − − − +

choose an integer lq( )k such that tq( )k =sqk+lqk

ω

. Integrating above inequality

from sq( )k to tq( )k , we obtain

( )

(

)

(

( )

)

( )

( )

( )

( ) ( )

( ) (

)

( ) ( ) ( ) ( )

(

)

( )

(

)

( )

3 3 0 2 0

0 *

2 1

, , exp 2

d ln

, exp 2

k q k q k k k

q k q

k q k q t k k

q k q k s

k s t t t

k

q k s

y t y s a t b t c t

k s x t s s g

y s G

τ

φ φ ε ε

φ β + − ≤ ≤  ≥  − −    − + +   ≥ − −

Consequently, from (3.25) and (3.26), we have

( ) ( ) ln

2

k k

q q k

t s

G

β

− ≥

+ (3.30)

For any ( )k q

t s≥ and q N≥ 1( )k , we have

(

) (

)

( )

( ) ( )

( )

1 1

2 , d 2 d

k k

T k T t

k

k u t y uφ u Hk s s

−∞ − ≤ −∞

(3.31)

and

(

) (

)

( ) ( )

( )

( )

1 2 , d 2 d .

k k

q q

k

s s t

k

T k u t y uφ u H k s s

− −∞

− ≤

(3.32)

For each k K= +1,K+2,, there exist an N2kN1k and a constant L>0 such that

( ) 1( ) ( )

( )

2 d 12 0

k k

q

T s k

Hk s s ε

−∞ ≤

for all q N≥ 2( )k (3.33)

and

( )

2 d 12 0

L

H

−∞k s s≤ ε (3.34)

We can choose an integer ( )k 0

q

r ≥ such that ( )k ( )k ( )k ( )k

q q q q

t =s + +L r

ω

+w , where ( )k

[ )

0,

q

w

ω

is a constant. By (3.30), there exists a large enough K1≥K

such that

( )

0 2 0

k q

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DOI: 10.4236/jamp.2018.66116 1400 Journal of Applied Mathematics and Physics

For all k K q N≥ 1, ≥ 2( )k , tsq( )k +L t, q( )k and t tl , by (3.27) and

(3.31)-(3.34), we have

(

)

(

) ( )

( ) (

)

( )

( )

(

) (

)

( ) ( )

(

) ( )

( )

( )

( ) ( )

( )

( )

( )

(

) ( )

(

)

( ) 1 1 1

3 3 2 2 1

0

3 3 2 2

*

2 2 1 0

,

, , , d

, d d d k k q k k q k k q k q k

T s t

k k T s k

T t

k k

s t t

s y t

y t a t b t y t c t k u t x u u

y t a t b t c t H k s s

k

H k s s k u t x u u

φ

φ φ φ

ε φ ε −∞ − −∞ − −∞ ′    ≥ − − + + −       ≥ − −     + + − + 

(

) ( )

( )

( )

( ) (

)

(

) ( )

(

( )

( )

( )

( ) (

)

)

0 * 0 0

3 3 0 2 0 1

0 *

3 3 0 2 0 2 2 1

, d

2 2

, 2 d .

k t

k t

y t a t b t c t k s x t s s

y t a t b t c t c t k s x t s s

ε ε

φ ε ε

φ ε ε

− −    ≥ − − + + + +     = − − − +

Integrating above system from sq( )k +L to tq( )k , we derive

( )

(

)

( )

(

)

( ) ( )

(

( )

( )

( ) ( )

( )

( ) ( ) ( ) ( ) ( )

( )

( )

( ) (

(

)

)

)

( ) ( ) ( ) ( )

( )

( ) ( ) ( ) ( ) ( ) 0 2

3 3 0

1

0 *

2 0 2 1

1

,

, exp

2 d d

ln

k k k k

q q q q

k k k k k

q q q q q

k k k k k k k k k

q q q q q q q q q

k

q k

s L s L r t

k

q k s L s L r s L r

t

k

s L t s L s L r t s L r s L r t t

y t k

y s L a t b t

c t c t k s x t s s s

g

ω ω

ω ω

ω ω ω ω

ε φ φ ε ε + + + + + + + + − + + − + ≤ ≤ + + + + − ≤ ≤ + + + + ≤ ≤ ≥  ≥ + + + + −  − − +       + + + +    

  ( )

(

)

( )

0 0 0

0 0

2exp 2 2exp 2,

k q

r G

k k k

ε ε βω ε ε ε



≥ − − ≥ >

which is a contradiction. This contradiction shows that there exists a constant

2 0

m > such that liminft→∞ y t

( )

m2. Hence, choose a constant m=min

{

m m1, 2

}

,

then we finally have

( )

(

)

( )

liminft→∞ x tim i=1,2 , liminft→∞ y tm

Therefore Theorem 3.2 holds. This completes the proof.

4. Extinction

In this section, we investigate the extinction of system (1.1). We note that, under conditions of Theorem 3.2, system (1.1) is always permanent.

Theorem 4.1. Assume that there is a constant η≥0 such that

( )

limsup d ln 0

k t

k t

t t t t

s s h

η

η

γ

+

→∞ ≤ < +

 

+ ≤

 

 (4.1)

( )

( )

(

3 2

)

limsup d ln 0

k t

k t

t t t t

a s mc s s g

η

η +

→∞ ≤ < +

 

− + ≤

 

 (4.2)

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DOI: 10.4236/jamp.2018.66116 1401 Journal of Applied Mathematics and Physics

( )

, ln

k

k t t t

h t h

µ

µ ≤ < +

=

(4.3)

( )

, ln

k

k t t t

g t g

µ

µ ≤ < +

=

(4.4)

are bounded function on t R∈ + and v

[

0,η

)

, where

( )

t a t1

( )

a t2

( )

D t

( )

γ = + + , then we can obtain

( )

( )

(

)

lim

i

0, lim

0,

1,2

t→∞

x t

=

t→∞

y t

=

i

=

(4.5)

for any positive solution

(

x t x t y t1

( ) ( ) ( )

, 2 ,

)

of system (1.1).

Proof. Firstly, we prove the extinction of species x. DefineV t

( )

=x t1

( )

+x t2

( )

.

When t tk, calculating the right-upper derivative of V t

( )

, we have

( )

( )

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( ) ( )

(

( )

)

( ) ( )

(

( ) ( )

)

( ) ( )

(

( )

)

( ) ( )

(

( ) ( )

( )

( )

)

1 2

0

1 1 1 1 1 1

12 2 1 2 2 2 2

21 1 2

1 1 1 1 12 21

d

D V t x t x t

x t a t b t x t c t k s y t s s

D t x t x t x t a t b t x t

D t x t x t

x t a t b t x t D t D t

+

−∞

′ ′

= +

= − − +

+ − + −

+ −

≤ − − +

( ) ( )

(

( ) ( )

( )

( )

)

( )

( )

(

)

(

( )

( ) ( )

( )

)

( )

( )

(

)

(

( )

( ) ( )

( )

)

( )

( )

(

)

(

( )

( )

( )

( ) ( )

(

( )

)

)

( ) ( )

(

( ) ( )

)

2 2 2 2 21 12

1 2 1 1 1

1 2 2 2 2

1 2 1 2 +2 2 1 2

2 ,

x t a t b t x t D t D t

x t x t a t b t x t D t

x t x t a t b t x t D t

x t x t a t a t D t b t x t x t

V t γ t b t V t

+ − − +

≤ + − +

+ + − +

≤ + + − +

= −

when t t= k, we get

( ) ( ) ( )

k 1 k 2 k 1 1k

( )

k 2k 2

( )

k max

{

1k, 2k

} ( )

k k

( )

k V t+ =x t+ +x t+ =h x t +h x t h h V t =h V t

By the comparison theory of impulsive differential equations, we have

( ) ( )

V tv t for all t≥0, where v t

( )

is a solution of the auxiliary equation

( ) ( ) ( )

(

( ) ( )

)

( )

( )

2 ,

, 1,2, ,

k

k k k

v t v t t b t v t t t

v t h v t k

γ

+

 ′ = − ≠

 

= =

  (4.6)

with the initial condition v

( )

0 =V

( )

0 . Since system (4.6) satisfies all conditions of Lemma 2.1 from conditions (4.1) and (4.3), we obtain lim

( )

0

t→∞v t = for any

positive solution of system (4.6). Then we get

( )

( )

( )

(

)

lim i lim lim 0, 1,2 .

t→∞x tt→∞V tt→∞v t = i= (4.7)

In the following, we prove the extinction of species y. From third equation and sixth equation of system (1.1), we have

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( )

( )

0

3 3 2 2 1 d ,

, 1,2,

k

k k k

y t y t a t b t y t c t k s x t s s t t

y t g y t k

−∞ +

 ′ = − − − ≠

 

 = =

 (4.8)

(15)

DOI: 10.4236/jamp.2018.66116 1402 Journal of Applied Mathematics and Physics 0

t T. Obviously, when t tk, for any t T0, we obtain

( )

( ) ( )

(

( ) ( )

( )

( ) (

)

)

( ) ( )

(

( ) ( )

( )

)

0

3 3 2 2 1

3 3 2

d

y t y t a t b t y t c t k s x t s s

y t a t b t y t mc t

−∞

′ = − − −

≤ − −

Then we consider the following auxiliary system

( )

( ) ( )

(

( ) ( )

( )

)

( )

( )

3 3 2 ,

, 1,2,

k

k k k

w t w t a t b t w t mc t t t

w t+ g w t k

 ′ = − − ≠

 

= =

  (4.9)

with the initial condition w T

( )

0 =y T

( )

0 . Since all condition of Lemma 2.1

holds from condition (4.2) and (4.4), we can obtain lim

( )

0

t→∞w t = for any

posi-tive solution of system (4.9). Clearly, we have

( )

( )

lim lim 0.

t→∞y tt→∞w t = (4.10)

From (4.7) and (4.10), we finally obtain (4.5) holds. This completes the proof of Theorem 4.1.

5. Globally Attractive

In this section, by constructing appropriate Lyapunov function, we establish the sufficient conditions on the globally attractive of system (1.1).

Theorem 5.1. Assume that all conditions of Theorem3.2 hold, further, there exists a constant λ>0 such that

( )

(

)

liminft tt+λψ s sd 0

→∞

> , (5.1)

where

( )

( )

( )

( ) (

)

( )

( ) ( )

( ) (

)

21

1 0 2 2

1

12

2 3 0 1 1

1

min d ,

, d

t R

D t

t b t k s c t s s

m D t

b t b t k s c t s s

m

ψ + +∞

+∞

=  − − −

− − − 

and ψ

( )

t ≥0. Then system (1.1) is globally attractive, that is, for any two posi-tive solutions

(

x t x t y t1

( ) ( ) ( )

, 2 ,

)

and

(

x t x t y t1

( ) ( ) ( )

,2 ,

)

of system (1.1), the

following limit hold.

( )

( )

( )

( )

( ) ( )

1 1 2 2

lim 0,lim 0,lim 0.

t→∞ x tx t = t→∞ x tx t = t→∞ y ty t = (5.2)

Proof. For any two positive solutions

(

x t x t y t1

( ) ( ) ( )

, 2 ,

)

,

(

x t x t y t1

( ) ( ) ( )

,2 ,

)

,

by Theorem 3.2, we obtain that there exist constants m M1, 1 such that

( ) ( ) ( ) ( )

1 i , i , , 1, 1,2.

mx t x t y t y t  ≤M i= (5.3)

Then we have for any t R∈ + and t tk,

( )

( )

( )

( )

( )

( ) (

)

1 1

1 ln ln 1 1,2

i i i i i i

x t x t x t x t x t x t i

m − ≤ −  ≤M − = (5.4)

( ) ( )

( )

( )

( ) ( )

1 1

1 y t y t lny t lny t 1 y t y t

m −  ≤ −  ≤M −  (5.5)

References

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