999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

Global Asymptotic Behavior of a Predator-Prey Diffusion System with Beddington-DeAngelis Function Response

2014-05-03 12:48:12MENGYijieandXIAOShiwu

MENG Yijieand XIAO Shiwu

School of Mathematics and Computer Science,Hubei University of Arts and Science, Xiangfan 441053,China.

Global Asymptotic Behavior of a Predator-Prey Diffusion System with Beddington-DeAngelis Function Response

MENG Yijie?and XIAO Shiwu

School of Mathematics and Computer Science,Hubei University of Arts and Science, Xiangfan 441053,China.

Received 14 April 2013;Accepted 14 October 2013

.Inthispaper,westudyaclassofreaction-diffusionsystemswith Beddington-DeAngelis function response.The global asymptotic convergence is established by using the comparison principle and the method of monotone iterations,which is via successive improvement of upper-lower solutions function.

Predator-prey diffusion system;asymptotic behavior;Beddington-DeAngelis function.

1 Introduction

It is the purpose of this paper to study the global asymptotic behavior of solutions to the predator-prey diffusion system with Beddington-DeAngelis function response and the homogeneous Neumann boundary condition,

where ??RN(N≥1)is a bounded domain with smooth boundary??,u and v represent the population densities of prey and predator,ν is the outward unit normal vector of the boundary??.The constant d1and d2,which are the diffusion coefficients,are positive.a, b,r,m and k are positive constants.The initial data u0(x),v0(x)are continuous functions.

It is known that there exist three equilibria(0,0),(1,0)and(?u,?v)provided that 0<k<(1+a)-1,where?u and?v are positive and satisfy

where

We note that(1.1)has a unique nonnegative global solution(u,v).In addition,if u06≡0,v06≡0,then the solution(u,v)is positive,i.e.,u(x,t)>0,v(x,t)>0 on ?,for all t>0.

In population dynamics,the prey-predator system with Beddington-DeAngelis function response has been extensively studied in[1-6].Reaction-diffusion systems with delays have been treated by many authors.However,most of the systems are mixed quasimonotone,and most of the discussions are in the framework of semi-group theory of dynamical systems[7-10].The method of upper and lower solutions and its associated monotone iterations have been used to investigate the dynamic property of the system, which is mixed quasimonotone with discrete delays[11-13].In[6],the author discussed the dissipation,persistence and the local stability of nonnegative constant steady states for(1.1).In this paper,we give sufficient conditions for the global asymptotic behavior of solutions of(1.1).The method of proof is via successive improvement of upper-lower solutions of some suitable systems,see[14,15].

2 Main results and proof

In thus section,we discuss the global asymptotic behavior of solutions by using the comparison principle and the method of monotone iterations.

Firstly,we give two results in[6].

Lemma 2.1.If k≥(1+a)-1,and b≤m,then

provided that u06≡0.

Lemma 2.2.If k<(1+a)-1and,then the positive constant solution(u?,v?)of(1.1)is locally stable.

Now,we discuss the global asymptotic stability of the solutions of(1.1)(?u,?v).Theorem 2.1.If(1+2a)-1<k<(1+a)-1and b<m,then

provided that u06≡0,v06≡0,where(?u,?v)is given by(1.2).

Proof.From(1.1),we know u satisfies

it follows by the comparison principle that

Thus,for any ?>0,there exists T1>0,such that

It then follows that v satisfies

Let w(t)be a solution of the following ordinary differential equation

Since k<(1+a)-1,for any ?>0,we have(1-k)(1+?)-ka>0.Then,

From the comparison principle,it follows that v(x,t)≤w(t).Thus,we get

From the arbitrariness of ?>0,we can get that

Thus,for any ?>0,there exists T2(≥T1),such that

Therefore,

thus,by the direct computation,we have

An application of the comparison principle gives

The arbitrariness of ? implies that

It is obvious that

thus,we have

By(2.3),for any sufficiently small ?>0,there exists T≥T3(≥T2),such that

Therefore,v satisfies

Since k<(1+a)-1and b<m,we have

The sufficiently small ? implies that

By the same comparison argument,we get

the arbitrariness of ? implies that

It is obvious that

Thus,we have

From(2.1 and(2.5),for any ?,0<??1,there exists T4(≥T3),such that

It follows that u satisfies

Since

thus,for sufficiently small ?>0,

So,by the comparison principle,we get

The arbitrariness of ? implies that

It is obvious that u2≤u1.

From(2.7),for any ?>0,there exists T5(≥T4),such that

It follows that v satisfies

Since

so,by the comparison principle,we get

The arbitrariness of ? implies that

Since

we get

From(2.1)and(2.5),For any ?,0<??1,there exists T6(≥T5),such that

It follows that u satisfies

Since u1≤u2≤u1.,and v1≤v2≤v1.,we have

so,for sufficiently small ?>0,

By by the comparison principle,we get

The arbitrariness of ? implies that

Sine

we have

Thus,we get

From(2.9),for any ?>0,there exists T7(≥T6),such that

It follows that v satisfies

Let Z(t)be a solution of the ordinary differential equation,

By u2(1-k)-ka≥u1(1-k)-ka>0,and the sufficiently small ?>0,we have

Thus,we get

The comparison principle gives that v(x.t)≥Z(t)for all x∈? and t≥T7,such that

The arbitrariness of ? implies that

Since

we have

Thus,we get

Define the sequences un,un,vn,vn(n≥1)as follows

Lemma 2.3.For the above defined sequences,we have

and the solution(u(x,t),v(x,t))satisfies

and

Proof.For n=1,2,we have shown that,and

and

Using induction and repeating the above process,we can complete the proof,and omit the detail.

Lemma2.3implies thatlimn→∞un,limn→∞un,limn→∞vnandlimn→∞vnexist,denoted as u,u,v,v,respectively.It is obvious that 0<u≤u and 0<v≤v.

Thus,u,u,v,and v satisfy that

and

and

Substituting the second equality into the third equality,and by straightforward computation,we have

Substituting the forth equality into the first equality,and by straightforward computation,we have

Let(2.19)minus(2.18),and by straightforward computation,we get

Since

and

from condition k>(1+2a)-1,so,we get u+u>1.Therefore,we can get(b-m)(1-k)+ mk(1-u-u)<0,such that u=u,from(2.20).

Now,from(2.17),we have

By(1-k)/mk>0 and u=u,it follows that v=v.Thus,we get u=u=?u,and v=v=?v, such that

The proof is complete.

Acknowledgments

This work is supported by the Science and Technology Research Plan of the Education Department of Hubei Province(Q20122504 and D20112605).

[1]Cantrell R.S.,Cosner C.,On the dynamics of predator-prey models with Beddington-De Angelis functional response.J.Math.Anal.Appl.,257(2001),206-222.

[2]Hwang T.W.,Global analysis of the predator-prey system with Beddington-De Angelis functional response.Siam J.Math.Anal.Appl.,281(2002),395-401.

[3]Beddingtion J.R.,Mutual interference between parasites or predators and its effect on searching efficiency.J.Animal Ecology,44(1975),331-340.

[4]Deangel D.L.,Goldstein R.A.and O,Neill R.V.,A model for tropic interaction.Ecology,56 (1975),881–892.

[5]Dimitrov D.T.,Kojouharov H.V.,Complete mathematical analysis of predator-prey models with linear prey growth and Beddington-De Angelis functional response.Appl.Math.and Comput.,162(2005),532-538.

[6]Chen W.Y.,Wang M.X.,Qualitative analysis of predator-prey models with Beddington-De Angelis functional response anddiffusion.Math.and ComputerModell.Appl.,42(2005),31-44.

[7]Martin R.H.,Smith H.L.,Abstract functional differential equations and reaction diffusion systems.Trans.Amer.Math.Sco.,321(1990),1-44.

[8]R.Redlinger,Existence theorems for semilinear parabolic syatems with functionals.Nonlinear Anal.,8(1984),667-682.

[9]Ruan S.G.,Zhao X.Q.,Persistence and extinction in two species reaction-diffusion systems with delays.J.Diff.Eqns.,156(1999),71-92.

[10]Martin R.H.,Smith H.L.,Reaction-diffusion systems with time delays:monotonicity,invariance,comparison and convergence.J.Reine Angew Math.,413(1991),1-35.

[11]Lu X.,Persistence and extinction in a competition-diffusion system with time delays.Canad. Appl.Math.Quart.,2(1994),231-246.

[12]Pao C.V.,Systems of parabolic equations with continuous and discrete delays.J.Math.Anal. Appl.,205(1997),157-185.

[13]Pao C.V.,Dynamics of nonlinear parabolic systems with time delays.J.Math.Anal.Appl., 198(1996),751-779.

[14]Wang Y.F.,Meng Y.J.,Asymptotic behavior of a competition-diffusion system with time delays.Math.and Comput.Model.,38(2003),509-517.

[15]Meng Y.J.,Wang Y.F.,Asymptotic behavior of a predator-prey system with time delays.E. J.Diff.Equ.,131(2005),1-11.

10.4208/jpde.v27.n2.3 June 2014

?Corresponding author.Email addresses:yijie-meng@sina.com(Y.Meng),xshiwu@sina.com(S.Xiao)

AMS SubjectClassifications:35B35,35K51

Chinese Library Classifications:0193.26

主站蜘蛛池模板: 少妇人妻无码首页| 99在线视频免费| 亚洲天堂网2014| 国产在线第二页| 小蝌蚪亚洲精品国产| 99久久精品免费观看国产| а∨天堂一区中文字幕| 在线免费亚洲无码视频| 日韩黄色精品| 国产高清国内精品福利| 波多野结衣久久高清免费| 日韩无码视频网站| julia中文字幕久久亚洲| 视频一本大道香蕉久在线播放| 麻豆国产在线观看一区二区| 99热这里只有成人精品国产| 国产成人亚洲综合a∨婷婷| 国产亚洲美日韩AV中文字幕无码成人| 亚洲一区二区精品无码久久久| 日韩福利视频导航| 乱系列中文字幕在线视频| 精品無碼一區在線觀看 | 91精品国产一区| 亚洲中文字幕久久无码精品A| 中文字幕在线看视频一区二区三区| 亚洲福利视频一区二区| 色婷婷在线播放| 国产美女一级毛片| 久久这里只有精品23| 亚洲国产综合精品一区| 国产原创演绎剧情有字幕的| 久久黄色毛片| 91精品国产91欠久久久久| 久久婷婷国产综合尤物精品| 亚洲国产精品久久久久秋霞影院| 一本大道香蕉久中文在线播放| 98精品全国免费观看视频| 国产福利免费在线观看| 亚洲中久无码永久在线观看软件| 国产在线日本| 国产91久久久久久| 免费一看一级毛片| 亚洲黄色视频在线观看一区| WWW丫丫国产成人精品| 任我操在线视频| 久久一级电影| 在线观看欧美精品二区| 91小视频在线| 亚洲人成影院午夜网站| 日韩麻豆小视频| 国产一区二区免费播放| 日韩大乳视频中文字幕| 久久久久久久久亚洲精品| 亚洲最黄视频| AV无码一区二区三区四区| 久久香蕉国产线看观看式| 亚洲一级毛片在线观| 国产麻豆91网在线看| 亚洲三级电影在线播放 | 91精品福利自产拍在线观看| 26uuu国产精品视频| 91成人免费观看在线观看| 国产成人亚洲毛片| 国产乱人激情H在线观看| 永久免费AⅤ无码网站在线观看| 国产美女丝袜高潮| 亚洲色无码专线精品观看| 特级毛片免费视频| 亚洲日本在线免费观看| 欧美另类第一页| 中文字幕资源站| 亚洲一区二区三区国产精品| 久草视频中文| 四虎免费视频网站| 国产精品无码影视久久久久久久 | 亚洲欧美人成人让影院| 亚洲成网777777国产精品| 成人国产精品2021| 国产在线专区| 国产成人8x视频一区二区| 亚洲精品男人天堂| 无码精品国产dvd在线观看9久|