Dynamic behaviors of a nonlinear amensalism model

Abstract A nonlinear amensalism model of the form dN1dt=r1N1(1−(N1P1)α1−u(N2P1)α2),dN2dt=r2N2(1−(N2P2)α3), $$\begin{aligned} &\frac{dN_{1}}{dt}= r_{1}N_{1} \biggl(1- \biggl( \frac{N_{1}}{P_{1}} \biggr)^{\alpha _{1}}-u \biggl(\frac{N_{2}}{P_{1}} \biggr)^{\alpha_{2}} \biggr), \\ &\frac{dN_{2}}...

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Main Author: Runxin Wu
Format: Article
Language:English
Published: SpringerOpen 2018-05-01
Series:Advances in Difference Equations
Subjects:
Online Access:http://link.springer.com/article/10.1186/s13662-018-1624-9
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author Runxin Wu
author_facet Runxin Wu
author_sort Runxin Wu
collection DOAJ
description Abstract A nonlinear amensalism model of the form dN1dt=r1N1(1−(N1P1)α1−u(N2P1)α2),dN2dt=r2N2(1−(N2P2)α3), $$\begin{aligned} &\frac{dN_{1}}{dt}= r_{1}N_{1} \biggl(1- \biggl( \frac{N_{1}}{P_{1}} \biggr)^{\alpha _{1}}-u \biggl(\frac{N_{2}}{P_{1}} \biggr)^{\alpha_{2}} \biggr), \\ &\frac{dN_{2}}{dt}= r_{2}N_{2} \biggl(1- \biggl( \frac{N_{2}}{P_{2}} \biggr)^{\alpha_{3}} \biggr), \end{aligned}$$ where ri,Pi,u,i=1,2,α1,α2,α3 $r_{i}, P_{i}, u, i=1, 2, \alpha_{1}, \alpha_{2}, \alpha_{3}$ are all positive constants, is proposed and studied in this paper. The dynamic behaviors of the system are determined by the sign of the term 1−u(P2P1)α2 $1-u (\frac{P_{2}}{P_{1}} )^{\alpha_{2}} $. If 1−u(P2P1)α2>0 $1-u (\frac {P_{2}}{P_{1}} )^{\alpha_{2}}>0$, then the unique positive equilibrium D(N1∗,N2∗) $D(N_{1}^{*},N_{2}^{*})$ is globally attractive, if 1−u(P2P1)α2<0 $1-u (\frac{P_{2}}{P_{1}} )^{\alpha_{2}}<0$, then the boundary equilibrium C(0,P2) $C(0, P_{2})$ is globally attractive. Our results supplement and complement the main results of Xiong, Wang, and Zhang (Advances in Applied Mathematics 5(2):255–261, 2016).
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spelling doaj.art-0848e0106e00440fa89326c1259099df2022-12-22T01:47:38ZengSpringerOpenAdvances in Difference Equations1687-18472018-05-012018111310.1186/s13662-018-1624-9Dynamic behaviors of a nonlinear amensalism modelRunxin Wu0Mathematics and Physics Institute, Fujian University of TechnologyAbstract A nonlinear amensalism model of the form dN1dt=r1N1(1−(N1P1)α1−u(N2P1)α2),dN2dt=r2N2(1−(N2P2)α3), $$\begin{aligned} &\frac{dN_{1}}{dt}= r_{1}N_{1} \biggl(1- \biggl( \frac{N_{1}}{P_{1}} \biggr)^{\alpha _{1}}-u \biggl(\frac{N_{2}}{P_{1}} \biggr)^{\alpha_{2}} \biggr), \\ &\frac{dN_{2}}{dt}= r_{2}N_{2} \biggl(1- \biggl( \frac{N_{2}}{P_{2}} \biggr)^{\alpha_{3}} \biggr), \end{aligned}$$ where ri,Pi,u,i=1,2,α1,α2,α3 $r_{i}, P_{i}, u, i=1, 2, \alpha_{1}, \alpha_{2}, \alpha_{3}$ are all positive constants, is proposed and studied in this paper. The dynamic behaviors of the system are determined by the sign of the term 1−u(P2P1)α2 $1-u (\frac{P_{2}}{P_{1}} )^{\alpha_{2}} $. If 1−u(P2P1)α2>0 $1-u (\frac {P_{2}}{P_{1}} )^{\alpha_{2}}>0$, then the unique positive equilibrium D(N1∗,N2∗) $D(N_{1}^{*},N_{2}^{*})$ is globally attractive, if 1−u(P2P1)α2<0 $1-u (\frac{P_{2}}{P_{1}} )^{\alpha_{2}}<0$, then the boundary equilibrium C(0,P2) $C(0, P_{2})$ is globally attractive. Our results supplement and complement the main results of Xiong, Wang, and Zhang (Advances in Applied Mathematics 5(2):255–261, 2016).http://link.springer.com/article/10.1186/s13662-018-1624-9Amensalism modelDifferential inequality theoryGlobal stability
spellingShingle Runxin Wu
Dynamic behaviors of a nonlinear amensalism model
Advances in Difference Equations
Amensalism model
Differential inequality theory
Global stability
title Dynamic behaviors of a nonlinear amensalism model
title_full Dynamic behaviors of a nonlinear amensalism model
title_fullStr Dynamic behaviors of a nonlinear amensalism model
title_full_unstemmed Dynamic behaviors of a nonlinear amensalism model
title_short Dynamic behaviors of a nonlinear amensalism model
title_sort dynamic behaviors of a nonlinear amensalism model
topic Amensalism model
Differential inequality theory
Global stability
url http://link.springer.com/article/10.1186/s13662-018-1624-9
work_keys_str_mv AT runxinwu dynamicbehaviorsofanonlinearamensalismmodel