Lotka Volterra Model with Time Delay

Size: px
Start display at page:

Download "Lotka Volterra Model with Time Delay"

Transcription

1 International Journal of Mathematics Research. ISSN Volume 6, Number (4), pp. 5- International Research Publication House Lotka Volterra Model with Time Dela Tapas Kumar Sinha and Sachinandan Chanda Computer Centre, North Eastern Hill Universit, Shillong 793 Department of Mathematics, Shillong Poltechnic, Shillong 793 Abstract We model the Lotka-Volterra equations with a time dela. For this model we derive the conditions for the existence of stead state conditions, asmptotic stabilit.. Introduction Time dela is inherent in the predator-pre sstems. Both the predator and pre require their own times to grow from birth to maturit and from maturit to death. If the time spans for predator and pre are greatl different it will lead to instabilit in the predator pre sstem. Using a time dela of a predator pre sstem we derive the conditions for temporal stabilit of a predator pre sstem following the techniques given in []. Predator pre models with time dela (or lag) have been studied b a number of authors [] [8]. Time dela can induces instabilit, oscillations and bifurcation and in some cases switching of stabilities. However most authors have used a single time dela to characterize the predator pre sstem. Here we have associated unique delas with both predator and pre.. Time Dela Equations for Predator-Pre The lotka Volterra equations with time dela are given b d t t tt () dt t d t tt dt () Here t, t are dela times for predator and pre respectivel. On substituting

2 6 Tapas Kumar Sinha & Sachinandan Chanda we obtain t t t e A and t e A (3) t t t A te (4) ( ) Ae t t (5) tt Here A, A correspond to the predator, pre population at time t =. t and For solutions of t to exist, we must have, from equations (4) and (5), that tt Ae tt Ae (6) From equation (6), we get t t t a b e (7) a Where b AA (8) Note that we have defined a as the time dela (which is defined in terms of a ) has to be positive. In absence of dela cos t t ba b then the equation (7) becomes t t P, t ab e (9) Suppose that i ( > ) is a purel imaginar root of equation (9).It suffices to seek solution.putting i in (9) and separating real parts and imaginar parts, we get b cos t t () a Sin t t () Eliminating t t from Equations () & (),we get

3 Lotka Volterra Model with Time Dela 7 4 U a b b () Let be the determinant of equation (3),we get a b 4b If a b 4b,then there is no positive solution of. If a b b positive solution of 4 or if and given b a b,then there ma be a ba (3) If b, then there is one positive solution of given b ba (taking onl positive sign) (4) Thus From equation (), we get t t From equation (), we get a sin (5) cos t t a (6) cos t Equation (6) determines the sign of cos t t t must lie. From equation (5), we get and the quadrant in which sin a n ; n,,, 3,... n (7) Where t t (8)

4 8 Tapas Kumar Sinha & Sachinandan Chanda Where is given b equation (4) and where second quadrant according to the sign of cos t t sin a is chosen in the first or 3. Stabilit Analsis To analze the change of behavior of the stabilit of the stead state E with respect to t,we examine the sign of d d,where i. d If,then the sstem is unstable for some values of. d d If,then is the sstem stable for some values of. d Differentiating equation () with respect to t,we get d e d ae Hence d 4 i cos isin d at i i a cos isin (9) Using (5) & (6) in (9) and simplifing, we get a aa a 4a 4 d Re d at i aa a () Since and d, Re at ever root. dt at i Therefore ever time a root crosses the imaginar axis with increasing t it crosses from left to right, stabilit of the zero solution is lost at,where a sin () and stabilit persists for all.

5 Lotka Volterra Model with Time Dela 9 4. Conclusion We have derived the stabilit criteria for a delaed predator pre sstem. Note that is the composite dela as given b (9). Criteria for stabilit is given in (). For the case A or A one finds that. In the opposite limit where A, A A A are ver large one obtains Note that in both limits if,. AA Here is the rate of growth of predator and is the rate of death of pre. In other words in this limit there is no possibilit of an predator pre oscillations. References [] N.C. Majee and A. B. Ro Temporal dnamics of a two-neuron continuous network model with time dela Appl. Math,. Modelling,(997), [] T. K. Kar and A. Ghorai, Dnamic behavior of a delaed predator-pre model with harvesting, Applied Mathematics and Computation, () [3] Chao-Pao Ho, Yuei-Liang Ou The Influence of Time Dela on Local Stabilit for a Predator-Pre Sstem, Tunghai Science Vol. 4: 47 6 Jul, [4] M.A. Haque, A Predator Pre Model with Discrete Time Dela Considering Different Growth Function of Pre, Advances in Applied Mathematical Biosciences, Number (), pp. -6 [5] Peter J. Wangersk and W. J. Cunningham, Time Lag in Pre-Predator Population Models, Ecolog, (957) [6] Roger arditi, Jean-marie abillon, Jorge vieira da silva, The Effect of a Time- Dela in a Predator-Pre Model Mathematical biosciences (977) 33, 7- [7] T. K. Kar, Selective harvesting in a predator-pre fisher with time dela, Mathematical and Computer Modelling, (3) [8] A. Martin and S. Ruan, Predator-pre models with dela and pre harvesting, Journal of Mathematical Biolog, ()

6 Tapas Kumar Sinha & Sachinandan Chanda

Control Schemes to Reduce Risk of Extinction in the Lotka-Volterra Predator-Prey Model

Control Schemes to Reduce Risk of Extinction in the Lotka-Volterra Predator-Prey Model Journal of Applied Mathematics and Phsics, 2014, 2, 644-652 Published Online June 2014 in SciRes. http://www.scirp.org/journal/jamp http://d.doi.org/10.4236/jamp.2014.27071 Control Schemes to Reduce Risk

More information

Nonlinear Systems Examples Sheet: Solutions

Nonlinear Systems Examples Sheet: Solutions Nonlinear Sstems Eamples Sheet: Solutions Mark Cannon, Michaelmas Term 7 Equilibrium points. (a). Solving ẋ =sin 4 3 =for gives =as an equilibrium point. This is the onl equilibrium because there is onl

More information

7.7 LOTKA-VOLTERRA M ODELS

7.7 LOTKA-VOLTERRA M ODELS 77 LOTKA-VOLTERRA M ODELS sstems, such as the undamped pendulum, enabled us to draw the phase plane for this sstem and view it globall In that case we were able to understand the motions for all initial

More information

The Hopf Bifurcation Theorem: Abstract. Introduction. Transversality condition; the eigenvalues cross the imginary axis with non-zero speed

The Hopf Bifurcation Theorem: Abstract. Introduction. Transversality condition; the eigenvalues cross the imginary axis with non-zero speed Supercritical and Subcritical Hopf Bifurcations in Non Linear Maps Tarini Kumar Dutta, Department of Mathematics, Gauhati Universit Pramila Kumari Prajapati, Department of Mathematics, Gauhati Universit

More information

Dynamics in Delay Cournot Duopoly

Dynamics in Delay Cournot Duopoly Dnamics in Dela Cournot Duopol Akio Matsumoto Chuo Universit Ferenc Szidarovszk Universit of Arizona Hirouki Yoshida Nihon Universit Abstract Dnamic linear oligopolies are eamined with continuous time

More information

Interspecific Segregation and Phase Transition in a Lattice Ecosystem with Intraspecific Competition

Interspecific Segregation and Phase Transition in a Lattice Ecosystem with Intraspecific Competition Interspecific Segregation and Phase Transition in a Lattice Ecosstem with Intraspecific Competition K. Tainaka a, M. Kushida a, Y. Ito a and J. Yoshimura a,b,c a Department of Sstems Engineering, Shizuoka

More information

ARTICLE IN PRESS. Nonlinear Analysis: Real World Applications. Contents lists available at ScienceDirect

ARTICLE IN PRESS. Nonlinear Analysis: Real World Applications. Contents lists available at ScienceDirect Nonlinear Analsis: Real World Applications ( Contents lists available at ScienceDirect Nonlinear Analsis: Real World Applications journal homepage: www.elsevier.com/locate/nonrwa Qualitative analsis of

More information

520 Chapter 9. Nonlinear Differential Equations and Stability. dt =

520 Chapter 9. Nonlinear Differential Equations and Stability. dt = 5 Chapter 9. Nonlinear Differential Equations and Stabilit dt L dθ. g cos θ cos α Wh was the negative square root chosen in the last equation? (b) If T is the natural period of oscillation, derive the

More information

10 Back to planar nonlinear systems

10 Back to planar nonlinear systems 10 Back to planar nonlinear sstems 10.1 Near the equilibria Recall that I started talking about the Lotka Volterra model as a motivation to stud sstems of two first order autonomous equations of the form

More information

Systems of Differential Equations

Systems of Differential Equations WWW Problems and Solutions 5.1 Chapter 5 Sstems of Differential Equations Section 5.1 First-Order Sstems www Problem 1. (From Scalar ODEs to Sstems). Solve each linear ODE; construct and solve an equivalent

More information

NUMERICAL SIMULATION DYNAMICAL MODEL OF THREE-SPECIES FOOD CHAIN WITH LOTKA-VOLTERRA LINEAR FUNCTIONAL RESPONSE

NUMERICAL SIMULATION DYNAMICAL MODEL OF THREE-SPECIES FOOD CHAIN WITH LOTKA-VOLTERRA LINEAR FUNCTIONAL RESPONSE Journal of Sustainability Science and Management Volume 6 Number 1, June 2011: 44-50 ISSN: 1823-8556 Universiti Malaysia Terengganu Publisher NUMERICAL SIMULATION DYNAMICAL MODEL OF THREE-SPECIES FOOD

More information

Today. Qualitative analysis examples.

Today. Qualitative analysis examples. Toda Qualitative analsis examples. = -(-1)(+1) What are the stead states of this equation? Draw the slope fields for this equation. = -(-1)(+1) What are the stead states of this equation? Draw the slope

More information

Chapter 8 Equilibria in Nonlinear Systems

Chapter 8 Equilibria in Nonlinear Systems Chapter 8 Equilibria in Nonlinear Sstems Recall linearization for Nonlinear dnamical sstems in R n : X 0 = F (X) : if X 0 is an equilibrium, i.e., F (X 0 ) = 0; then its linearization is U 0 = AU; A =

More information

A Review of Complex Numbers Ilya Pollak ECE 301 Signals and Systems Section 2, Fall 2010 Purdue University

A Review of Complex Numbers Ilya Pollak ECE 301 Signals and Systems Section 2, Fall 2010 Purdue University A Review of Complex Numbers la Pollak ECE 30 Signals and Sstems Section, Fall 00 Purdue Universit A complex number is represented in the form z = x + j, where x and are real numbers satisfing the usual

More information

Complex dynamical behaviour of Disease Spread in a Plant- Herbivore System with Allee Effect

Complex dynamical behaviour of Disease Spread in a Plant- Herbivore System with Allee Effect IOSR Journal of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue 6 Ver. III (Nov. - Dec. 5), PP 74-83 www.iosrjournals.org Complex dnamical behaviour of Disease Spread in a Plant- Herbivore

More information

* τσ σκ. Supporting Text. A. Stability Analysis of System 2

* τσ σκ. Supporting Text. A. Stability Analysis of System 2 Supporting Tet A. Stabilit Analsis of Sstem In this Appendi, we stud the stabilit of the equilibria of sstem. If we redefine the sstem as, T when -, then there are at most three equilibria: E,, E κ -,,

More information

Analysis of a Prey-Predator System with Modified Transmission Function

Analysis of a Prey-Predator System with Modified Transmission Function Research Paper American Journal of Engineering Research (AJER) e-issn : 2320-0847 p-issn : 2320-0936 Volume-3, Issue-9, pp-194-202 www.ajer.org Open Access Analysis of a Prey-Predator System with Modified

More information

Curriculum: MechEng, UC Berkeley

Curriculum: MechEng, UC Berkeley Curriculum: MechEng, UC Berkele ME 132, 3-units, required, 2 nd or 3 rd ear students Prerequisites: Programming and Scientific computing (E7); Linear Algebra and ODEs (Math 54) Emphasis: mathematics of

More information

Heteroclinic Bifurcation and Multistability in a Ratio-dependent Predator-Prey System with Michaelis-Menten Type Harvesting Rate

Heteroclinic Bifurcation and Multistability in a Ratio-dependent Predator-Prey System with Michaelis-Menten Type Harvesting Rate Proceedings of the World Congress on ngineering Vol I WC Jul 4-6 London U.K. Heteroclinic Bifurcation and Multistabilit in a Ratio-dependent Predator-Pre Sstem with Michaelis-Menten Tpe Harvesting Rate

More information

Chaos Control and Synchronization of a Fractional-order Autonomous System

Chaos Control and Synchronization of a Fractional-order Autonomous System Chaos Control and Snchronization of a Fractional-order Autonomous Sstem WANG HONGWU Tianjin Universit, School of Management Weijin Street 9, 37 Tianjin Tianjin Universit of Science and Technolog College

More information

Two Dimensional Linear Systems of ODEs

Two Dimensional Linear Systems of ODEs 34 CHAPTER 3 Two Dimensional Linear Sstems of ODEs A first-der, autonomous, homogeneous linear sstem of two ODEs has the fm x t ax + b, t cx + d where a, b, c, d are real constants The matrix fm is 31

More information

Bifurcation and Stability Analysis of a Prey-predator System with a Reserved Area

Bifurcation and Stability Analysis of a Prey-predator System with a Reserved Area ISSN 746-733, England, UK World Journal of Modelling and Simulation Vol. 8 ( No. 4, pp. 85-9 Bifurcation and Stability Analysis of a Prey-predator System with a Reserved Area Debasis Mukherjee Department

More information

BIFURCATION AND SPATIAL PATTERN FORMATION IN SPREADING OF DISEASE WITH INCUBATION PERIOD IN A PHYTOPLANKTON DYNAMICS

BIFURCATION AND SPATIAL PATTERN FORMATION IN SPREADING OF DISEASE WITH INCUBATION PERIOD IN A PHYTOPLANKTON DYNAMICS Electronic Journal of Differential Equations, Vol. 212 (212), No. 21, pp. 1 12. ISSN: 172-6691. URL: http://ejde.math.tstate.edu or http://ejde.math.unt.edu ftp ejde.math.tstate.edu BIFURCATION AND SPATIAL

More information

Global dynamics and bifurcation of a tri-trophic food chain model

Global dynamics and bifurcation of a tri-trophic food chain model ISSN 746-7, England, UK World Journal of Modelling and Simulation Vol. 8 ) No., pp. 66-8 Global dnamics and bifurcation of a tri-trophic food chain model Tapan Kumar Kar, Abhijit Ghorai, Ashim Batabal

More information

2D-Volterra-Lotka Modeling For 2 Species

2D-Volterra-Lotka Modeling For 2 Species Majalat Al-Ulum Al-Insaniya wat - Tatbiqiya 2D-Volterra-Lotka Modeling For 2 Species Alhashmi Darah 1 University of Almergeb Department of Mathematics Faculty of Science Zliten Libya. Abstract The purpose

More information

A PREY-PREDATOR MODEL WITH HOLLING II FUNCTIONAL RESPONSE AND THE CARRYING CAPACITY OF PREDATOR DEPENDING ON ITS PREY

A PREY-PREDATOR MODEL WITH HOLLING II FUNCTIONAL RESPONSE AND THE CARRYING CAPACITY OF PREDATOR DEPENDING ON ITS PREY Journal of Applied Analsis and Computation Volume 8, Number 5, October 218, 1464 1474 Website:http://jaac-online.com/ DOI:1.11948/218.1464 A PREY-PREDATOR MODEL WITH HOLLING II FUNCTIONAL RESPONSE AND

More information

C. Non-linear Difference and Differential Equations: Linearization and Phase Diagram Technique

C. Non-linear Difference and Differential Equations: Linearization and Phase Diagram Technique C. Non-linear Difference and Differential Equations: Linearization and Phase Diaram Technique So far we have discussed methods of solvin linear difference and differential equations. Let us now discuss

More information

GALLOPING OF SMALL ASPECT RATIO SQUARE CYLINDER

GALLOPING OF SMALL ASPECT RATIO SQUARE CYLINDER OL. NO. JANUARY 5 ISSN 89-668 6-5 Asian Research Publishing Network (ARPN). All rights reserved. GALLOPING OF SMALL ASPET RATIO SQUARE YLINDER A. N. Rabinin and. D. Lusin Facult of Mathematics and Mechanics

More information

Dynamics Analysis of Anti-predator Model on Intermediate Predator With Ratio Dependent Functional Responses

Dynamics Analysis of Anti-predator Model on Intermediate Predator With Ratio Dependent Functional Responses Journal of Physics: Conference Series PAPER OPEN ACCESS Dynamics Analysis of Anti-predator Model on Intermediate Predator With Ratio Dependent Functional Responses To cite this article: D Savitri 2018

More information

Two Limit Cycles in a Two-Species Reaction

Two Limit Cycles in a Two-Species Reaction Two Limit Ccles in a Two-Species Reaction Brigita Ferčec 1 Ilona Nag Valer Romanovski 3 Gábor Szederkéni 4 and János Tóth 5 The Facult of Energ Technolog Krško 1 Center for Applied Mathematics and Theoretical

More information

3.5 Competition Models: Principle of Competitive Exclusion

3.5 Competition Models: Principle of Competitive Exclusion 94 3. Models for Interacting Populations different dimensional parameter changes. For example, doubling the carrying capacity K is exactly equivalent to halving the predator response parameter D. The dimensionless

More information

Hopf Bifurcation and Control of Lorenz 84 System

Hopf Bifurcation and Control of Lorenz 84 System ISSN 79-3889 print), 79-3897 online) International Journal of Nonlinear Science Vol.63) No.,pp.5-3 Hopf Bifurcation and Control of Loren 8 Sstem Xuedi Wang, Kaihua Shi, Yang Zhou Nonlinear Scientific Research

More information

THE most studied topics in theoretical ecology is the

THE most studied topics in theoretical ecology is the Engineering Letters :3 EL 3_5 Stabilit Nonlinear Oscillations Bifurcation in a Dela-Induced Predator-Pre Sstem with Harvesting Debaldev Jana Swapan Charabort Nadulal Bairagi Abstract A harvested predator-pre

More information

Study on Nonlinear Vibration and Crack Fault of Rotor-bearing-seal Coupling System

Study on Nonlinear Vibration and Crack Fault of Rotor-bearing-seal Coupling System Sensors & Transducers 04 b IFSA Publishing S. L. http://www.sensorsportal.com Stud on Nonlinear Vibration and Crack Fault of Rotor-bearing-seal Coupling Sstem Yuegang LUO Songhe ZHANG Bin WU Wanlei WANG

More information

Vector Fields. Field (II) Field (V)

Vector Fields. Field (II) Field (V) Math 1a Vector Fields 1. Match the following vector fields to the pictures, below. Eplain our reasoning. (Notice that in some of the pictures all of the vectors have been uniforml scaled so that the picture

More information

Research concerning the evaluation of the connection forces in the joints of the sucker rod pumping units mechanism

Research concerning the evaluation of the connection forces in the joints of the sucker rod pumping units mechanism IOP Conference Series: Materials Science and Engineering PAPER OPEN ACCESS Research concerning the evaluation of the connection forces in the oints of the sucker rod pumping units mechanism To cite this

More information

THE UNIVERSITY OF MICHIGAN. Timing Analysis of Domino Logic

THE UNIVERSITY OF MICHIGAN. Timing Analysis of Domino Logic Timing Analsis of Domino Logic b David Van Campenhout, Trevor Mudge and Karem Sakallah CSE-T-296-96 THE UNIVESITY O MICHIGAN Computer Science and Engineering Division Department of Electrical Engineering

More information

Research Article Bifurcations in Van der Pol-Like Systems

Research Article Bifurcations in Van der Pol-Like Systems Mathematical Problems in Engineering Volume 3, Article ID 3843, 8 pages http://d.doi.org/.55/3/3843 Research Article Bifurcations in Van der Pol-Like Sstems Orhan Ozgur Abar,, Ilknur Kusbezi Abar, 3 and

More information

New approach to study the van der Pol equation for large damping

New approach to study the van der Pol equation for large damping Electronic Journal of Qualitative Theor of Differential Equations 2018, No. 8, 1 10; https://doi.org/10.1422/ejqtde.2018.1.8 www.math.u-szeged.hu/ejqtde/ New approach to stud the van der Pol equation for

More information

Submarine sand ripples formation in a viscous fluid: 2D and 3D linear stability analysis

Submarine sand ripples formation in a viscous fluid: 2D and 3D linear stability analysis Marine Sandwave and River Dune Dnamics 1 & April 4 - Enschede, the Netherlands Submarine sand ripples formation in a viscous fluid: D and 3D linear stabilit analsis V. Langlois (1) and A. Valance (1) Groupe

More information

Affine transformations

Affine transformations Reading Optional reading: Affine transformations Brian Curless CSE 557 Autumn 207 Angel and Shreiner: 3., 3.7-3. Marschner and Shirle: 2.3, 2.4.-2.4.4, 6..-6..4, 6.2., 6.3 Further reading: Angel, the rest

More information

Lotka Volterra Predator-Prey Model with a Predating Scavenger

Lotka Volterra Predator-Prey Model with a Predating Scavenger Lotka Volterra Predator-Prey Model with a Predating Scavenger Monica Pescitelli Georgia College December 13, 2013 Abstract The classic Lotka Volterra equations are used to model the population dynamics

More information

n n. ( t) ( ) = = Ay ( ) a y

n n. ( t) ( ) = = Ay ( ) a y Sstems of ODE Example of sstem with ODE: = a+ a = a + a In general for a sstem of n ODE = a + a + + a n = a + a + + a n = a + a + + a n n n nn n n n Differentiation of matrix: ( t) ( t) t t = = t t ( t)

More information

NONLINEAR DYNAMICS AND CHAOS. Numerical integration. Stability analysis

NONLINEAR DYNAMICS AND CHAOS. Numerical integration. Stability analysis LECTURE 3: FLOWS NONLINEAR DYNAMICS AND CHAOS Patrick E McSharr Sstems Analsis, Modelling & Prediction Group www.eng.o.ac.uk/samp patrick@mcsharr.net Tel: +44 83 74 Numerical integration Stabilit analsis

More information

Simulation and Experimental Validation of Chaotic Behavior of Airflow in a Ventilated Room

Simulation and Experimental Validation of Chaotic Behavior of Airflow in a Ventilated Room Simulation and Eperimental Validation of Chaotic Behavior of Airflow in a Ventilated Room Jos van Schijndel, Assistant Professor Eindhoven Universit of Technolog, Netherlands KEYWORDS: Airflow, chaos,

More information

Physics of Tsunamis. This is an article from my home page: Ole Witt-Hansen 2011 (2016)

Physics of Tsunamis. This is an article from my home page:   Ole Witt-Hansen 2011 (2016) Phsics of Tsunamis This is an article from m home page: www.olewitthansen.dk Ole Witt-Hansen 11 (16) Contents 1. Constructing a differential equation for the Tsunami wave...1. The velocit of propagation

More information

MULTI-SCROLL CHAOTIC AND HYPERCHAOTIC ATTRACTORS GENERATED FROM CHEN SYSTEM

MULTI-SCROLL CHAOTIC AND HYPERCHAOTIC ATTRACTORS GENERATED FROM CHEN SYSTEM International Journal of Bifurcation and Chaos, Vol. 22, No. 2 (212) 133 ( pages) c World Scientific Publishing Compan DOI: 1.1142/S21812741332 MULTI-SCROLL CHAOTIC AND HYPERCHAOTIC ATTRACTORS GENERATED

More information

Stability analysis of a prey-predator model with a reserved area

Stability analysis of a prey-predator model with a reserved area Available online at www.pelagiaresearchlibrary.com Advances in Applied Science Research, 4, 5(3):93-3 ISSN: 976-86 CODEN (USA): AASRFC Stability analysis of a prey-predator model with a reserved area Neelima

More information

Ordinary Differential Equations

Ordinary Differential Equations Instructor: José Antonio Agapito Ruiz UCSC Summer Session II, 00 Math Ordinar Differential Equations Final Solution This report does not contain full answers to all questions of the final. Instead, ou

More information

Functions of One Variable Basics

Functions of One Variable Basics Functions of One Variable Basics Function Notation: = f() Variables and are placeholders for unknowns» We will cover functions of man variables during one of the in-residence QSW lectures. = independent

More information

Stability Analysis And Maximum Profit Of Logistic Population Model With Time Delay And Constant Effort Of Harvesting

Stability Analysis And Maximum Profit Of Logistic Population Model With Time Delay And Constant Effort Of Harvesting Jurnal Vol 3, Matematika, No, 9-8, Juli Statistika 006 & Komputasi Vol No Juli 006 9-8, Juli 006 9 Stability Analysis And Maximum Profit Of Logistic Population Model With Time Delay And Constant Effort

More information

ON THE STABILITY OF SOLUTIONS OF A CERTAIN GENERAL THIRD ORDER NON LINEAR ORDINARY DIFFERENTIAL EQUATION

ON THE STABILITY OF SOLUTIONS OF A CERTAIN GENERAL THIRD ORDER NON LINEAR ORDINARY DIFFERENTIAL EQUATION Vol.2, No.5, pp.23-28, December 214 Published b European Centre for Research Training and Development UK (www.eajournals.org) ON THE STABILITY OF SOLUTIONS OF A CERTAIN GENERAL THIRD ORDER NON LINEAR ORDINARY

More information

3 First order nonlinear equations

3 First order nonlinear equations Separable equations 3 First order nonlinear equations d f dx = where f(x,) is not (in general) a linear function of. ( x, ) The equation is autonomous if there is no explicit dependence on the independent

More information

THETA-LOGISTIC PREDATOR PREY

THETA-LOGISTIC PREDATOR PREY THETA-LOGISTIC PREDATOR PREY What are the assumptions of this model? 1.) Functional responses are non-linear. Functional response refers to a change in the rate of exploitation of prey by an individual

More information

14 Periodic phenomena in nature and limit cycles

14 Periodic phenomena in nature and limit cycles 14 Periodic phenomena in nature and limit cycles 14.1 Periodic phenomena in nature As it was discussed while I talked about the Lotka Volterra model, a great deal of natural phenomena show periodic behavior.

More information

Local Phase Portrait of Nonlinear Systems Near Equilibria

Local Phase Portrait of Nonlinear Systems Near Equilibria Local Phase Portrait of Nonlinear Sstems Near Equilibria [1] Consider 1 = 6 1 1 3 1, = 3 1. ( ) (a) Find all equilibrium solutions of the sstem ( ). (b) For each equilibrium point, give the linear approimating

More information

A New Closed-loop Identification Method of a Hammerstein-type System with a Pure Time Delay

A New Closed-loop Identification Method of a Hammerstein-type System with a Pure Time Delay A New Closed-loop Identification Method of a Hammerstein-tpe Sstem with a Pure Time Dela Edin Drljević a, Branislava Peruničić b, Željko Jurić c, Member of IEEE Abstract A procedure for the closed-loop

More information

Dynamical Analysis of a Harvested Predator-prey. Model with Ratio-dependent Response Function. and Prey Refuge

Dynamical Analysis of a Harvested Predator-prey. Model with Ratio-dependent Response Function. and Prey Refuge Applied Mathematical Sciences, Vol. 8, 214, no. 11, 527-537 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/12988/ams.214.4275 Dynamical Analysis of a Harvested Predator-prey Model with Ratio-dependent

More information

STABILITY AND NEIMARK-SACKER BIFURCATION OF A SEMI-DISCRETE POPULATION MODEL

STABILITY AND NEIMARK-SACKER BIFURCATION OF A SEMI-DISCRETE POPULATION MODEL Journal of Applied Analsis and Computation Website:http://jaac-online.com/ Volume 4, Number 4, November 14 pp. 419 45 STABILITY AND NEIMARK-SACKER BIFURCATION OF A SEMI-DISCRETE POPULATION MODEL Cheng

More information

FIRST- AND SECOND-ORDER IVPS The problem given in (1) is also called an nth-order initial-value problem. For example, Solve: Solve:

FIRST- AND SECOND-ORDER IVPS The problem given in (1) is also called an nth-order initial-value problem. For example, Solve: Solve: .2 INITIAL-VALUE PROBLEMS 3.2 INITIAL-VALUE PROBLEMS REVIEW MATERIAL Normal form of a DE Solution of a DE Famil of solutions INTRODUCTION We are often interested in problems in which we seek a solution

More information

Modeling the Immune System W9. Ordinary Differential Equations as Macroscopic Modeling Tool

Modeling the Immune System W9. Ordinary Differential Equations as Macroscopic Modeling Tool Modeling the Immune System W9 Ordinary Differential Equations as Macroscopic Modeling Tool 1 Lecture Notes for ODE Models We use the lecture notes Theoretical Fysiology 2006 by Rob de Boer, U. Utrecht

More information

Systems of Linear Equations: Solving by Graphing

Systems of Linear Equations: Solving by Graphing 8.1 Sstems of Linear Equations: Solving b Graphing 8.1 OBJECTIVE 1. Find the solution(s) for a set of linear equations b graphing NOTE There is no other ordered pair that satisfies both equations. From

More information

Introduction to Differential Equations. National Chiao Tung University Chun-Jen Tsai 9/14/2011

Introduction to Differential Equations. National Chiao Tung University Chun-Jen Tsai 9/14/2011 Introduction to Differential Equations National Chiao Tung Universit Chun-Jen Tsai 9/14/011 Differential Equations Definition: An equation containing the derivatives of one or more dependent variables,

More information

AN EXTENSION OF THE ANTOCI-DEI-GALEOTTI EVOLUTIONARY MODEL FOR ENVIRONMENT PROTECTION THROUGH FINANCIAL INSTRUMENTS

AN EXTENSION OF THE ANTOCI-DEI-GALEOTTI EVOLUTIONARY MODEL FOR ENVIRONMENT PROTECTION THROUGH FINANCIAL INSTRUMENTS ISSN 1974-4110 WP-EMS Working Papers Series in Economics, Mathematics and Statistics AN EXTENSION OF THE ANTOCI-DEI-GALEOTTI EVOLUTIONARY MODEL FOR ENVIRONMENT PROTECTION THROUGH FINANCIAL INSTRUMENTS

More information

Math 2930 Worksheet Equilibria and Stability

Math 2930 Worksheet Equilibria and Stability Math 2930 Worksheet Equilibria and Stabilit Week 3 September 7, 2017 Question 1. (a) Let C be the temperature (in Fahrenheit) of a cup of coffee that is cooling off to room temperature. Which of the following

More information

Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum.

Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum. Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum. These equations greatl facilitate the solution of man problems in which

More information

Mathematics 309 Conic sections and their applicationsn. Chapter 2. Quadric figures. ai,j x i x j + b i x i + c =0. 1. Coordinate changes

Mathematics 309 Conic sections and their applicationsn. Chapter 2. Quadric figures. ai,j x i x j + b i x i + c =0. 1. Coordinate changes Mathematics 309 Conic sections and their applicationsn Chapter 2. Quadric figures In this chapter want to outline quickl how to decide what figure associated in 2D and 3D to quadratic equations look like.

More information

Modelling biological oscillations

Modelling biological oscillations Modelling biological oscillations Shan He School for Computational Science University of Birmingham Module 06-23836: Computational Modelling with MATLAB Outline Outline of Topics Van der Pol equation Van

More information

Math 323 Exam 2 - Practice Problem Solutions. 2. Given the vectors a = 1,2,0, b = 1,0,2, and c = 0,1,1, compute the following:

Math 323 Exam 2 - Practice Problem Solutions. 2. Given the vectors a = 1,2,0, b = 1,0,2, and c = 0,1,1, compute the following: Math 323 Eam 2 - Practice Problem Solutions 1. Given the vectors a = 2,, 1, b = 3, 2,4, and c = 1, 4,, compute the following: (a) A unit vector in the direction of c. u = c c = 1, 4, 1 4 =,, 1+16+ 17 17

More information

Stability of Limit Cycles in Hybrid Systems

Stability of Limit Cycles in Hybrid Systems Proceedings of the 34th Hawaii International Conference on Sstem Sciences - 21 Stabilit of Limit Ccles in Hbrid Sstems Ian A. Hiskens Department of Electrical and Computer Engineering Universit of Illinois

More information

Subband Coding and Wavelets. National Chiao Tung University Chun-Jen Tsai 12/04/2014

Subband Coding and Wavelets. National Chiao Tung University Chun-Jen Tsai 12/04/2014 Subband Coding and Wavelets National Chiao Tung Universit Chun-Jen Tsai /4/4 Concept of Subband Coding In transform coding, we use N (or N N) samples as the data transform unit Transform coefficients are

More information

Symmetry Breaking and Turbulence in Perturbed Plane Couette Flow

Symmetry Breaking and Turbulence in Perturbed Plane Couette Flow Theoret. Comput. Fluid Dnamics (2002) 16: 91 97 Digital Object Identifier (DOI) 10.1007/s00162-002-0064- Theoretical and Computational Fluid Dnamics Smmetr Breaking and Turbulence in Perturbed Plane Couette

More information

Not for reproduction

Not for reproduction ROTATION OF AES For a discussion of conic sections, see Review of Conic Sections In precalculus or calculus ou ma have studied conic sections with equations of the form A C D E F Here we show that the

More information

ESAIM: M2AN Modélisation Mathématique et Analyse Numérique M2AN, Vol. 37, N o 2, 2003, pp DOI: /m2an:

ESAIM: M2AN Modélisation Mathématique et Analyse Numérique M2AN, Vol. 37, N o 2, 2003, pp DOI: /m2an: Mathematical Modelling and Numerical Analysis ESAIM: M2AN Modélisation Mathématique et Analyse Numérique M2AN, Vol. 37, N o 2, 2003, pp. 339 344 DOI: 10.1051/m2an:2003029 PERSISTENCE AND BIFURCATION ANALYSIS

More information

Chapter 13. Overview. The Quadratic Formula. Overview. The Quadratic Formula. The Quadratic Formula. Lewinter & Widulski 1. The Quadratic Formula

Chapter 13. Overview. The Quadratic Formula. Overview. The Quadratic Formula. The Quadratic Formula. Lewinter & Widulski 1. The Quadratic Formula Chapter 13 Overview Some More Math Before You Go The Quadratic Formula The iscriminant Multiplication of Binomials F.O.I.L. Factoring Zero factor propert Graphing Parabolas The Ais of Smmetr, Verte and

More information

Lecture 1a. Complex numbers, phasors and vectors. Introduction. Complex numbers. 1a.1

Lecture 1a. Complex numbers, phasors and vectors. Introduction. Complex numbers. 1a.1 1a.1 Lecture 1a Comple numbers, phasors and vectors Introduction This course will require ou to appl several concepts ou learned in our undergraduate math courses. In some cases, such as comple numbers

More information

( 7, 3) means x = 7 and y = 3. ( 7, 3) works in both equations so. Section 5 1: Solving a System of Linear Equations by Graphing

( 7, 3) means x = 7 and y = 3. ( 7, 3) works in both equations so. Section 5 1: Solving a System of Linear Equations by Graphing Section 5 : Solving a Sstem of Linear Equations b Graphing What is a sstem of Linear Equations? A sstem of linear equations is a list of two or more linear equations that each represents the graph of a

More information

Department of Mathematical and Statistical Sciences University of Alberta

Department of Mathematical and Statistical Sciences University of Alberta MATH 4 (R) Winter 8 Intermediate Calculus I Solutions to Problem Set #5 Completion Date: Frida Februar 5, 8 Department of Mathematical and Statistical Sciences Universit of Alberta Question. [Sec.., #

More information

Fluid Mechanics II. Newton s second law applied to a control volume

Fluid Mechanics II. Newton s second law applied to a control volume Fluid Mechanics II Stead flow momentum equation Newton s second law applied to a control volume Fluids, either in a static or dnamic motion state, impose forces on immersed bodies and confining boundaries.

More information

Extra Credit Solutions Math 181, Fall 2018 Instructor: Dr. Doreen De Leon

Extra Credit Solutions Math 181, Fall 2018 Instructor: Dr. Doreen De Leon Extra Credit Solutions Math 181, Fall 018 Instrutor: Dr. Doreen De Leon 1. In eah problem below, the given sstem is an almost linear sstem at eah of its equilibrium points. For eah, (i Find the (real equilibrium

More information

STABILITY ANALYSIS OF DELAY DIFFERENTIAL EQUATIONS WITH TWO DISCRETE DELAYS

STABILITY ANALYSIS OF DELAY DIFFERENTIAL EQUATIONS WITH TWO DISCRETE DELAYS CANADIAN APPLIED MATHEMATICS QUARTERLY Volume 20, Number 4, Winter 2012 STABILITY ANALYSIS OF DELAY DIFFERENTIAL EQUATIONS WITH TWO DISCRETE DELAYS XIHUI LIN AND HAO WANG ABSTRACT. We use an algebraic

More information

12.1 Systems of Linear equations: Substitution and Elimination

12.1 Systems of Linear equations: Substitution and Elimination . Sstems of Linear equations: Substitution and Elimination Sstems of two linear equations in two variables A sstem of equations is a collection of two or more equations. A solution of a sstem in two variables

More information

A Discrete Numerical Scheme of Modified Leslie-Gower With Harvesting Model

A Discrete Numerical Scheme of Modified Leslie-Gower With Harvesting Model CAUCHY Jurnal Matematika Murni dan Aplikasi Volume 5(2) (2018), Pages 42-47 p-issn: 2086-0382; e-issn: 2477-3344 A Discrete Numerical Scheme of Modified Leslie-Gower With Harvesting Model Riski Nur Istiqomah

More information

HSML Honors or AP Calculus Course Preparedness Test

HSML Honors or AP Calculus Course Preparedness Test HSML Honors or AP Calculus Course Preparedness Test High School Math Live wants parents to be well informed. We want our student to be placed in the appropriate course so that the will be successful and

More information

Solving Differential Equations with Simulink

Solving Differential Equations with Simulink Solving Differential Equation with Simulink Dr. R. L. Herman UNC Wilmington, Wilmington, NC March, 206 Solving ODE with Simulink, ICTCM 206 R. L. Herman Mar, 206 /9 Outline Simulink 2 Solution of ODE 3

More information

Math 128A Spring 2003 Week 12 Solutions

Math 128A Spring 2003 Week 12 Solutions Math 128A Spring 2003 Week 12 Solutions Burden & Faires 5.9: 1b, 2b, 3, 5, 6, 7 Burden & Faires 5.10: 4, 5, 8 Burden & Faires 5.11: 1c, 2, 5, 6, 8 Burden & Faires 5.9. Higher-Order Equations and Systems

More information

Algebra II Notes Unit Six: Polynomials Syllabus Objectives: 6.2 The student will simplify polynomial expressions.

Algebra II Notes Unit Six: Polynomials Syllabus Objectives: 6.2 The student will simplify polynomial expressions. Algebra II Notes Unit Si: Polnomials Sllabus Objectives: 6. The student will simplif polnomial epressions. Review: Properties of Eponents (Allow students to come up with these on their own.) Let a and

More information

Numerical Solution of a Fractional-Order Predator-Prey Model with Prey Refuge and Additional Food for Predator

Numerical Solution of a Fractional-Order Predator-Prey Model with Prey Refuge and Additional Food for Predator 66 Numerical Solution of a Fractional-Order Predator-Prey Model with Prey Refuge Additional Food for Predator Rio Satriyantara, Agus Suryanto *, Noor Hidayat Department of Mathematics, Faculty of Mathematics

More information

LOTKA-VOLTERRA SYSTEMS WITH DELAY

LOTKA-VOLTERRA SYSTEMS WITH DELAY 870 1994 133-140 133 LOTKA-VOLTERRA SYSTEMS WITH DELAY Zhengyi LU and Yasuhiro TAKEUCHI Department of Applied Mathematics, Faculty of Engineering, Shizuoka University, Hamamatsu 432, JAPAN ABSTRACT Sufftcient

More information

SPATIALLY EXPLICIT POPULATION MODELS

SPATIALLY EXPLICIT POPULATION MODELS SPATIALLY EXPLICIT POPULATION MODELS During the last decade, ecologists and particularl mathematical ecologists have focused on different approaches to the problem of spatial distribution of species. When

More information

Geometry and Honors Geometry Summer Review Packet 2014

Geometry and Honors Geometry Summer Review Packet 2014 Geometr and Honors Geometr Summer Review Packet 04 This will not be graded. It is for our benefit onl. The problems in this packet are designed to help ou review topics from previous mathematics courses

More information

Coordinate geometry. + bx + c. Vertical asymptote. Sketch graphs of hyperbolas (including asymptotic behaviour) from the general

Coordinate geometry. + bx + c. Vertical asymptote. Sketch graphs of hyperbolas (including asymptotic behaviour) from the general A Sketch graphs of = a m b n c where m = or and n = or B Reciprocal graphs C Graphs of circles and ellipses D Graphs of hperbolas E Partial fractions F Sketch graphs using partial fractions Coordinate

More information

MATRIX TRANSFORMATIONS

MATRIX TRANSFORMATIONS CHAPTER 5. MATRIX TRANSFORMATIONS INSTITIÚID TEICNEOLAÍOCHTA CHEATHARLACH INSTITUTE OF TECHNOLOGY CARLOW MATRIX TRANSFORMATIONS Matri Transformations Definition Let A and B be sets. A function f : A B

More information

Ordinary Differential Equations n

Ordinary Differential Equations n Numerical Analsis MTH63 Ordinar Differential Equations Introduction Talor Series Euler Method Runge-Kutta Method Predictor Corrector Method Introduction Man problems in science and engineering when formulated

More information

LESSON #42 - INVERSES OF FUNCTIONS AND FUNCTION NOTATION PART 2 COMMON CORE ALGEBRA II

LESSON #42 - INVERSES OF FUNCTIONS AND FUNCTION NOTATION PART 2 COMMON CORE ALGEBRA II LESSON #4 - INVERSES OF FUNCTIONS AND FUNCTION NOTATION PART COMMON CORE ALGEBRA II You will recall from unit 1 that in order to find the inverse of a function, ou must switch and and solve for. Also,

More information

ME 321: FLUID MECHANICS-I

ME 321: FLUID MECHANICS-I 6/07/08 ME 3: LUID MECHANI-I Dr. A.B.M. Toufique Hasan Professor Department of Mechanical Engineering Bangladesh Universit of Engineering & Technolog (BUET), Dhaka Lecture- 4/07/08 Momentum Principle teacher.buet.ac.bd/toufiquehasan/

More information

115.3 Assignment #9 Solutions

115.3 Assignment #9 Solutions 115. Assignment #9 Solutions-1 115. Assignment #9 Solutions 8.1-12 Solve the differential equation d dx = 2(1 ), where 0 = 2 for x 0 = 0. d 1 = 2dx d 1 = 2dx ln 1 =2x + C Find C b inserting the Initial

More information

Development of an Extended Operational States Observer of a Power Assist Wheelchair

Development of an Extended Operational States Observer of a Power Assist Wheelchair Development of an Extended Operational States Observer of a Power Assist Wheelchair Sehoon Oh Institute of Industrial Science Universit of Toko 4-6-, Komaba, Meguro, Toko, 53-855 Japan sehoon@horilab.iis.u-toko.ac.jp

More information

Feedback Optimal Control for Inverted Pendulum Problem by Using the Generating Function Technique

Feedback Optimal Control for Inverted Pendulum Problem by Using the Generating Function Technique (IJACSA) International Journal o Advanced Computer Science Applications Vol. 5 No. 11 14 Feedback Optimal Control or Inverted Pendulum Problem b Using the Generating Function echnique Han R. Dwidar Astronom

More information

Law of Sines, Law of Cosines, Heron s Formula:

Law of Sines, Law of Cosines, Heron s Formula: PreAP Math Analsis nd Semester Review Law of Sines, Law of Cosines, Heron s Formula:. Determine how man solutions the triangle has and eplain our reasoning. (FIND YOUR FLOW CHART) a. A = 4, a = 4 ards,

More information