The Logistic Equation Robert M. Hayes 2003.

Slides:



Advertisements
Similar presentations
The Logistic Equation Robert M. Hayes Overview §Historical ContextHistorical Context §Summary of Relevant ModelsSummary of Relevant Models §Logistic.
Advertisements

Population fluctuations Topics for this class: n Population fluctuations in nature can result from changing environment, i.e., extrinsic environmental.
Normalizing and Redistributing Variables Chapter 7 of Data Preparation for Data Mining Markus Koskela.
Lesson 9-5 Logistic Equations. Logistic Equation We assume P(t) is constrained by limited resources so : Logistic differential equation for population.
DIFFERENTIAL EQUATIONS 9. We have looked at a variety of models for the growth of a single species that lives alone in an environment.
1) Consider the differential equation
Boyce/DiPrima 9th ed, Ch 2.5: Autonomous Equations and Population Dynamics Elementary Differential Equations and Boundary Value Problems, 9th edition,
Exploring Exponential Growth and Decay Models
Computational Biology, Part 17 Biochemical Kinetics I Robert F. Murphy Copyright  1996, All rights reserved.
7 INVERSE FUNCTIONS.
CHAPTER 52 POPULATION ECOLOGY Copyright © 2002 Pearson Education, Inc., publishing as Benjamin Cummings Section C: Population Growth 1.The exponential.
9. 1 Modeling with Differential Equations Spring 2010 Math 2644 Ayona Chatterjee.
Logarithmic and Exponential Functions
9 DIFFERENTIAL EQUATIONS.
Section 3.5 Exponential and Logarithmic Models. Important Vocabulary Bell-shaped curve The graph of a Gaussian model. Logistic curve A model for describing.
Population Modeling Mathematical Biology Lecture 2 James A. Glazier (Partially Based on Brittain Chapter 1)
1 GEM2505M Frederick H. Willeboordse Taming Chaos.
Lesson 17 – Introducing and Applying Base e. IBHL1 Math - Santowski 10/1/20151 IBHL1 - Santowski.
APPLICATIONS OF DIFFERENTIATION 4. Many applications of calculus depend on our ability to deduce facts about a function f from information concerning.
Ch 9.5: Predator-Prey Systems In Section 9.4 we discussed a model of two species that interact by competing for a common food supply or other natural resource.
SECOND LAW OF POPULATIONS: Population growth cannot go on forever - P. Turchin 2001 (Oikos 94:17-26) !?
Computational Biology, Part 15 Biochemical Kinetics I Robert F. Murphy Copyright  1996, 1999, 2000, All rights reserved.
In Sections 2.2 and 2.4, we investigated infinite limits and vertical asymptotes.  There, we let x approach a number.  The result was that the values.
DIFFERENTIAL EQUATIONS 9. Perhaps the most important of all the applications of calculus is to differential equations. DIFFERENTIAL EQUATIONS.
Differential Equations 7. Modeling with Differential Equations 7.1.
Jochen Triesch, UC San Diego, 1 Motivation: natural processes unfold over time: swinging of a pendulum decay of radioactive.
The simplest model of population growth is dy/dt = ky, according to which populations grow exponentially. This may be true over short periods of time,
1 6. Mean, Variance, Moments and Characteristic Functions For a r.v X, its p.d.f represents complete information about it, and for any Borel set B on the.
Exploring Exponential Growth and Decay Models Acc. Coordinate Algebra / Geometry A Day 57.
Ecology 2b- Population Growth & Limiting Factors.
Population Models Modeling and Simulation I-2012.
1 6. Mean, Variance, Moments and Characteristic Functions For a r.v X, its p.d.f represents complete information about it, and for any Borel set B on the.
Copyright © Cengage Learning. All rights reserved.
5.2 Polynomial & Linear Factors Learning goals graph functions expressed symbolically and show key features of the graph, by hand in simple cases and using.
2.6 Limits at Infinity: Horizontal Asymptotes LIMITS AND DERIVATIVES In this section, we: Let x become arbitrarily large (positive or negative) and see.
Copyright © Cengage Learning. All rights reserved. 9 Differential Equations.
AiS Challenge Summer Teacher Institute 2003 Richard Allen Modeling Populations: an introduction.
Logistic Equations Sect. 8-6.
Splash Screen.
Exponential Functions
7 INVERSE FUNCTIONS.
Lesson 18 - Solving & Applying Exponential Equations Using Logarithms
Exploring Exponential Growth and Decay Models
Graphing.
Splash Screen.
§ 4.4 The Natural Logarithm Function.
Exponential Functions
Populations.
Population Ecology Chapter 45.
Ways to Evaluate Limits:
Warm-Up: Exponential Functions lesson
Exploring Exponential Growth and Decay Models
3.3 Constrained Growth.
Exponential Functions and Graphs
Exploring Exponential Growth and Decay Models
Clicker Question 1 What is the general solution to the DE dy / dx = x(1+ y2)? A. y = arctan(x2 / 2) + C B. y = arctan(x2 / 2 + C) C. y = tan(x2 / 2)
Copyright © Cengage Learning. All rights reserved.
MATH 175: NUMERICAL ANALYSIS II
Determine all of the real zeros of f (x) = 2x 5 – 72x 3 by factoring.
Population Ecology Notes
Relationship Notes: Graphs
Differential Equations
Population Modeling Mathematical Biology Lecture 2 James A. Glazier
Chapter 14 Interactions in Ecosystems
Population Fluctuation Notes
Module 3.3 Constrained Growth
CHAPTER 52 POPULATION ECOLOGY Section C: Population Growth
Eva Arnold, Dr. Monika Neda
Presentation transcript:

The Logistic Equation Robert M. Hayes 2003

Overview Historical Context Summary of Relevant Models Logistic Difference Growth Model Linear Growth The Logistic Equation

Historical Context The starting point for population growth models is The Principle of Population, published in 1798 by Thomas R. Malthus (1766-1834). In it he presented his theories of human population growth and relationships between over-population and misery. The model he used is now called the exponential model of population growth.  In 1846, Pierre Francois Verhulst, a Belgian scientist, proposed that population growth depends not only on the population size but also on the effect of a “carrying capacity” that would limit growth. His formula is now called the "logistic model" or the Verhulst model.

Recent Developments Most recently, the logistic equation has been used as part of exploration of what is called "chaos theory". Most of this work was collected for the first time by Robert May in a classic article published in Nature in June of 1976. Robert May started his career as a physicist but then did his post-doctoral work in applied mathematics. He became very interested in the mathematical explanations of what enables competing species to coexist and then in the mathematics behind populations growth.

Summary of Relevant Models Logistic growth models are derived from the exponential models by multiplying the respective factors r and (1+r) in the exponential models by (K – pt)/K. Note that the two models for exponential growth are identical but the two for logistic growth are different. The linear growth model is important both in itself and as a part of the logistic models.

Logistic Difference Growth Model The logistic difference growth model will be considered in two contexts: The Incremental Context, in which growth takes place at discrete points in time The Continuous Context

The Incremental Context - I Verhulst modified the exponential growth model to reflect the effect of a maximum for the size of the population. He denoted the carrying capacity as K and multiplied the ratio r in the difference exponential model by the factor (K - pt)/K to represent the effect of the maximum limit: (1) pt+1 = pt + ((K – pt)/K)*r*pt   Equivalently, (2) pt+1 – pt = ((K – pt)/K)*r*pt

The Incremental Context - II Equation (2) will be called the logistic difference equation. The term "difference" emphasizes that the left hand side of the equation is the difference between successive values. The following chart illustrates logistic difference growth, assuming a carrying capacity K = 1000, a growth rate r = 0.3, and a starting population p0 = 1. At the start, with a small value of population, the factor (K – pt)/K will be very close to one, and the growth will be nearly exponential. As the population value grows and gets closer to K, the factor will limit the population growth.

Illustrative Logistic Difference Growth As this shows, the curve produced by the logistic difference equation is S-shaped. Initially there is an exponential growth phase, but as growth gets closer to the carrying capacity (more or less at time step 37 in this case), the growth slows down and the population asymptotically approaches capacity.

The Continuous Context The differential counterpart to equation (6) is given by (3) dp = r*p(t)*(K – p(t))/K dt There is a closed solution to this equation: (4) p(t) = K/(1 + ((K – p(0))/p(0))*e-r*t)

Linear Growth Note that, qualitatively, there are three main sections of the logistic curve. The first has exponential growth and the third has asymptotic growth to the limit. But between those two is the third segment, in which the growth is virtually linear.

The Logistic Equation Turning from the to the logistic population model to the "logistic equation": (7) pt+1 = ((K – pt)/K)*(1 + r)*pt = ((K – pt)/K)*s*pt, where s = 1 + r.   This equation exhibits fascinating behavior depending on the value of s = (1+r). We will illustrate the behavior with different values of s.

Some simple mathematical properties First, though, there are two simple mathematical properties that will be of importance. To identify them, simplify the equation by letting pt = p and pt+1 = f(p) The fixed points for f(p) occur when f(p) = p, and that is either when p = 0 or when p = K – K/s = K*(s - 1)/s The maximum value for pt occurs when the derivative of equation (10) is set to zero: (8) d f(p)/dp = s*(1 – 2*p/K) = 0, which can occur only if s = 0 (which is the minimum) or when p = K/2. At that value, pmax = s*K/4. Since pmax  K, s  4.

Decline to Zero (0 < s < 1) When the value of s is between 0 and 1 (r  0) , the population will eventually decrease to zero. This is illustrated in the following graph, with K = 1000 and an initial population p0 = 500 individuals:

Normal Growth (1 < s < 3) - I When the value of s is between 1 and 3, the population will increase towards a stable value. The following graph illustrates with three values of s (in each case, K = 1000 and p0 = 1.00):

Normal Growth (1 < s < 3) - II Recall that the fixed points for f(p) occur at K*(1 – 1/s). For these three values of s, the fixed points therefore are at 200, 500, and 636. The three cases show very different speeds towards achieving their stable values. One more thing to notice is that when the value of s is larger than 2.4, the equation shows an oscillation which is larger as it gets closer to 3.0, but in all cases the oscillation dies down and the population value settles down to its steady value.

Normal Growth (1 < s < 3) - III One very interesting aspect of the logistic equation is that the long-term value of the population will be the same regardless of where it starts:

Multiple Stable Values (3 < s < 3.7) - I When s reaches the value of 3, the population oscillates between two steady values, and at 3.4495 the population switches among four values! This effect continues, with oscillation among eight values when s = 3.56, sixteen values when s = 3.596, etc. Note that for s > 3, there is truly a spectacular rate of growth—more than tripling in each time period. It is therefore not surprising that there should be a rebound as the population bounces against its upper limit and then recovers rapidly only to rebound again. The following charts show three graphs of this behavior:

At s = 3. 00, the oscillation is among two values and at 3 At s = 3.00, the oscillation is among two values and at 3.55, among four values.

At s = 3.56, the oscillation is among eight values:

Chaos (3.7 < s < 4) When s reaches a value of 3.7, the population jumps in what appears to be a random, unpredictable way, and it behaves so until s reaches a value 4.0. While this behavior looks random, it really isn't. This phenomenon has been called "chaos“, first used to describe this phenomenon by James A. Yorke and Tien Yien Li in their classic paper "Period Three Implies Chaos" [American Mathematical Monthly 82, no. 10, pp. 985-992, 1975] The following graph uses a value of r = 3.75.

An example of Chaos

Another example of Chaos

Solutions to the Logistic Equation There are only three values of s for which there are closed form solutions to the logistic equation. To simplify, let K = 1, so that f(p) = s*p*(1 – p) For s = 4, f(pn) = (1 – cos(2n*g))/2, where g = cos-1(1 – 2 p0) For s = 2,  f(pn) = (1 – exp(2n*g), where exp(x) = ex and g = log(1 – 2*p0) For s = – 2,  f(pn) = 1/2 – cos( + (-2)n*g), where

THE END