Figure 5: Bifurcation diagram for equation 4 as a function of K. n(t) << 1 then substituting into f(n) we get (using Taylor s theorem)

Similar documents
3 Single species models. Reading: Otto & Day (2007) section 4.2.1

Continuous-Time Dynamical Systems: Sketching solution curves and bifurcations

Population Dynamics. Max Flöttmann and Jannis Uhlendorf. June 12, Max Flöttmann and Jannis Uhlendorf () Population Dynamics June 12, / 54

(e) Use Newton s method to find the x coordinate that satisfies this equation, and your graph in part (b) to show that this is an inflection point.

M469, Fall 2010, Practice Problems for the Final

Lecture 3. Dynamical Systems in Continuous Time

Mathematical Modelling in Biology Lecture Notes

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

population size at time t, then in continuous time this assumption translates into the equation for exponential growth dn dt = rn N(0)

Use separation of variables to solve the following differential equations with given initial conditions. y 1 1 y ). y(y 1) = 1

Introduction to Biomathematics. Problem sheet

Systems of Ordinary Differential Equations

THETA-LOGISTIC PREDATOR PREY

Logistic Model with Harvesting

PULSE-SEASONAL HARVESTING VIA NONLINEAR DELAY DIFFERENTIAL EQUATIONS AND APPLICATIONS IN FISHERY MANAGEMENT. Lev V. Idels

MA 777: Topics in Mathematical Biology

Math 3B: Lecture 14. Noah White. February 13, 2016

2 One-dimensional models in discrete time

Mathematical modeling of Fish Resources Harvesting with. Predator at Maximum Sustainable Yield

Optimal Harvesting Models for Fishery Populations

MA 137 Calculus 1 with Life Science Application A First Look at Differential Equations (Section 4.1.2)

3.5 Competition Models: Principle of Competitive Exclusion

1. The growth of a cancerous tumor can be modeled by the Gompertz Law: dn. = an ln ( )

Qualitative analysis of differential equations: Part I

Mathematical Models of Biological Systems

4 Insect outbreak model

For logistic growth, we have

Chapter 4: Growth & Decay. Introduction

Mathematics 22: Lecture 5

GROWTH IN LENGTH: a model for the growth of an individual

ONE DIMENSIONAL FLOWS. Lecture 3: Bifurcations

Mathematical models in life sciences. Lecture notes of a course held by Marco Di Francesco based on the book by J. D. Murray

Homework 2. Due Friday, July We studied the logistic equation in class as a model of population growth. It is given by dn dt = rn 1 N

Chapter 2: Growth & Decay

Chapter 2 Lecture. Density dependent growth and intraspecific competition ~ The Good, The Bad and The Ugly. Spring 2013

Stability Bifurcation Analysis of a Fishery Model with Nonlinear Variation in Market Price

BIOS 3010: ECOLOGY. Dr Stephen Malcolm. Laboratory 6: Lotka-Volterra, the logistic. equation & Isle Royale

Where do differential equations come from?

Optimal control of single species biological population

Workshop on Theoretical Ecology and Global Change March 2009

Today. Introduction to Differential Equations. Linear DE ( y = ky ) Nonlinear DE (e.g. y = y (1-y) ) Qualitative analysis (phase line)

Mathematical Ecology. Christina Kuttler. Sommersemester 2010

Population Ecology & Biosystematics

1 Mathematical models of the population growth

Behaviour of simple population models under ecological processes

F and G have continuous second-order derivatives. Assume Equation (1.1) possesses an equilibrium point (x*,y*) so that

Fundamentals of Dynamical Systems / Discrete-Time Models. Dr. Dylan McNamara people.uncw.edu/ mcnamarad

Physics 127b: Statistical Mechanics. Renormalization Group: 1d Ising Model. Perturbation expansion

Mathematical biology and physiology. 1. The sizes of two populations, one being a predator and the other its prey, are described by the equations

HARVESTING IN A TWO-PREY ONE-PREDATOR FISHERY: A BIOECONOMIC MODEL

CHALMERS, GÖTEBORGS UNIVERSITET. EXAM for COMPUTATIONAL BIOLOGY A. COURSE CODES: FFR 110, FIM740GU, PhD

Basic Concepts. 1.0 renewable, nonrenewable, and environmental resources

INTERPRETING POPULATION DYNAMICS GRAPH

Autonomous Equations and Stability Sections

JMESTN Journal of Multidisciplinary Engineering Science and Technology (JMEST) ISSN: Vol. 2 Issue 4, April

Mathematical Ecology

Population modeling of marine mammal populations

Final Project Descriptions Introduction to Mathematical Biology Professor: Paul J. Atzberger. Project I: Predator-Prey Equations

Lotka Volterra Predator-Prey Model with a Predating Scavenger

Population Changes at a Constant Percentage Rate r Each Time Period

C2 Differential Equations : Computational Modeling and Simulation Instructor: Linwei Wang

The logistic difference equation and the route to chaotic behaviour

Lab 5: Nonlinear Systems

8 Ecosystem stability

Dynamical Systems and Chaos Part II: Biology Applications. Lecture 6: Population dynamics. Ilya Potapov Mathematics Department, TUT Room TD325

Key words and phrases. Bifurcation, Difference Equations, Fixed Points, Predator - Prey System, Stability.

Synchronization and Phase Oscillators

Diffusion equation, flux, diffusion coefficient scaling. Diffusion in fully ionized plasma vs. weakly ionized plasma. n => Coulomb collision frequency

Math 310: Applied Differential Equations Homework 2 Prof. Ricciardi October 8, DUE: October 25, 2010

Pangasius, a fresh water catfish with two barbels.

CHAOS. Verhulst population model

The upper limit for the exponent of Taylor s power law is a consequence of deterministic population growth

8 Autonomous first order ODE

Dynamics on a General Stage Structured n Parallel Food Chains

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

Modeling Population Dynamics: a Graphical Approach

Chapter 9 Population Dynamics, Carrying Capacity, and Conservation Biology

UCI MATH CIRCLE: POPULATION DYNAMICS

Conditional Forecasts

Homework 2 Solutions Math 307 Summer 17

Rosenzweig-MacArthur Model. Considering the Function that Protects a Fixed. Amount of Prey for Population Dynamics

Objective. Single population growth models

The functions in all models depend on two variables: time t and spatial variable x, (x, y) or (x, y, z).

2 Discrete growth models, logistic map (Murray, Chapter 2)

Predator-prey interactions

Models Involving Interactions between Predator and Prey Populations

Functional Response to Predators Holling type II, as a Function Refuge for Preys in Lotka-Volterra Model

Math 2930 Worksheet Introduction to Differential Equations

Semester Project Part 1: Due March 1, 2019

A dynamic reaction model of an inshore-offshore fishery with taxation as a control instrument

Direction fields of differential equations...with SAGE

Mathematical and Computational Methods for the Life Sciences

Population Ecology and the Distribution of Organisms. Essential Knowledge Objectives 2.D.1 (a-c), 4.A.5 (c), 4.A.6 (e)

Ordinary Differential Equations

Interactions. Yuan Gao. Spring Applied Mathematics University of Washington

Lesson 4: Population, Taylor and Runge-Kutta Methods

Characteristics of Fish Populations

8.1 Bifurcations of Equilibria

Continuous Threshold Policy Harvesting in Predator-Prey Models

Homework 4: Solution

Transcription:

Figure 5: Bifurcation diagram for equation 4 as a function of K n(t) << 1 then substituting into f(n) we get (using Taylor s theorem) dn = f(n + n) = f(n ) + f (N )n + higher order terms f (N )n Thus, as with the solution to equation 3 n(t) n 0 e f (N )t We call n 0 a small perturbation. If f (N ) > 0 the perturbation will grow, while if f (N ) < 0 the perturbation will shrink. Hence, the above definition of linear stability. Exponential growth, equation 3, has only one steady state, N = 0. This is (linearly) stable if d > b and unstable if b > d. Logistic growth, equation 4, has two steady states, N = 0 and N = K. f (0) = r and f (K) = r. Thus if r > 0, 0 is unstable and N is stable. Definition: A bifurcation diagram of dn = f b (N) for parameter b is a plot of the position and stability of the steady states of f b (N) as a function of b. Figure 5 shows the bifurcation diagram for equation 4 as a function of K. 8

2 Population dynamics: fishing policy Reading : Britton 1.5 2.1 Harvesting a population with logistic growth In fishing, we want to find the maximum sustainable yield (MSY) that we can take from the population. For example, consider a population that when not fished exhibits logistic growth according to equation 2. We can add a death term to the fish population where each fish is caught at a constant rate E: dn = f(n) = rn(1 N/K) EN (5) where E is the effort put in to catching fish by the fishermen. We define Y (E) = EN to be the fishermen s yield. It is this they aim to maximise. The steady states of 5 are N = 0 and N = K(1 E/r), provided that E < r. The yield is Y (E) = EN = EK(1 E/r) To find the MSY we differentiate with respect to E and find that E M = r/2 is maximal. This gives yield Y M (r/2) = rk/4 This MSY gives a stable fish population, since N = K/2 and f (N ) = r 2rN /K r/2 = r/2 = E M r < 0 We should contrast the MSY with the maximum short term yield, which is simply to take all the fish away from the unfished population. This would give a short term yield of K but leave no fish! 2.2 Crashes in fish stock Consider the following model for a fish population N: dn = rn(1 N/K) EN b(n) 9

Figure 6: Sublinear predation b(n) where r, K and E are as before and b(n) is predation by seals. One possible form for b(n) is as follows b(n) = BN2 A 2 + N 2 where B and A are constants. This form of predation, shown in figure 6 is known as sublinear. For low densities the seals do not focus on the fish, but as the fish population increases the seals will focus on them more and more on catching them. We will return to predation functions in section 7.1 when we look at predator-prey models. The full model for the fish population is then dn = f(n) = rn(1 N/K) EN BN2 A 2 + N 2 (6) This model is much more complex than those we have looked at previously. It has five parameters (with units): r (time 1 ), K (biomass), E (time 1 ), A (biomass) and B (biomass.time 1 ). To simplify the model we can nondimensionalise it. Set, u = N/ ˆN and τ = t/t Note that, d = d dτ dτ = 1 d T dτ 10

Equation 6 becomes ( ˆN du = (r E) T ˆNu 1 r ˆNu ) B ˆN 2 u 2 K(r E) A 2 + ˆN 2 u 2 ( du = (r E)Tu 1 r ˆNu ) 2 B(T/ ˆN)u K(r E) (A 2 / ˆN 2 ) + u 2 Now comes the trick. We can choose ˆN and T, which are dimensionless quantities, to be any values we like. This choice can be motivated by some biological knowledge, or can be quite simply aimed at simplifying the model. Here we simplify the model by choosing ˆN = A, T = A/B. Giving du = su(1 u/q) u2 1 + u 2 (7) where (r E)A K(r E) s = and q = B ra It is best at this point to check that our non-dimensionalisation is correct! For more information on non-dimensionalisation see Edelstein-Keshet, Mathematical Models in Biology, pages 126-128. We can now find the steady states of our simplified model, equation 7 u = 0 or s(1 u /q) = 1 + u 2 This last equation is best studied graphically. Figure 7 shows three possible solutions for the steady states. Still without solving equation 7 we can also determine the stability of the three steady states graphically. This is done in figure 8 by plotting equation 7. We now have enough information to sketch a bifurcation diagram for parameters q and s. We do this in figure 9. The bifurcation diagrams tell us something very important about the effects of fishing: either reducing s or q can result in a sudden crash in the fish population. In terms of our original parameters, an increase in E (fishing effort) corresponds to a decrease in both s and q. Thus a small increase in fishing effort can result in a large drop in fish populations. Furthermore, the reduction in effort required to recover the fish population must be much larger than the increase that caused the crash. 11 u

Figure 7: Three alternative possibilities (depending on the values of s and q) for the steady states of equation 7. 12

Figure 8: Three alternative possibilities (depending on the values of s and q) for the stability of the steady states of equation 7. 13

Figure 9: Sketch of a bifurcation diagram for equation 7. 14