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Logistic Equation: Growth Population Dynamics

Logistic Equation Lab Script: Growth Population Dynamics. An Interdisciplinary Lab Script for Math, Physics and Non Linear Dynamic Courses.

Instructions

To the Instructor

Theory

The growth population dynamics of a colony of a single species in a controlled environment (a lab) can be modeled by ecologists in terms of the Logistic equation (1 - 4),

Pn + 1 = cPn(1 - Pn)

where

Pn = percentage of a limiting population L that is alive at generation n. By definition, 0 < P < 1.
Pn + 1 percentage of the limiting population L that is alive at another generation n + 1
c = growth population constant; depends upon several parameters such as amount of food, temperature, and the like. It is usually defined by the ecologist between 0 < 4.

This is an idealized model for growth population without external influences. The species under investigation could be a colony of formosan subterranean termites, potatoe weevils, or fire ants -the exact nature of the colony is irrelevant.

The limiting population that is alive (L) is governed, for example, by the physical size of the laboratory or colony in which the species is confined; After all, there can be no more of the species alive than can physically fit into the laboratory (1 - 4). Thus if Pn = 1/2 = 0.5, the exact population is PnL = L/2 at generation n. If there is no species present (initial population P0 = 0) or if the lab is completely full (P0 = 1), then there is no species present during the ensuing generations. Furthermore, if P0 is small, the population tends to increase, whereas if P0 is large, the population tends to decrease, as expected. From the numerical dynamics standpoint the exact value of L is inmaterial; what is important is the fraction of survival species, Pn, and how this fraction changes between generations.

However, assuming that the ecologist can count accurately the population of the species during each generation, can he or she use this knowledge to predict in advance the population of future generations? How small changes in the initial conditions (small changes in growth rates and initial population values) affect the outcome of the experiment (prediction of future populations)?

Enters Chaos Theory. The study where a dynamical behavior changes as a condition is varied is called bifurcation theory. Chaos Theory pretends to describe why small changes on initial conditions (e.g., P = 0.50, P = 0.51; c = 3.70, c = 3.71) produce unpredictable behaviors. Understanding when and why these unpredictable behaviors occur should enable an ecologist to develop better growth population models or experimental conditions suitable for replication and modeling. Under chaotic conditions growth population (or the outcome of any experiment, for that matter) cannot be predicted (1 - 4).

Notes

Possible Experiments

  1. Math, Physics and Non Linear Dynamics: Numerical Analysis of Attractors and Basins of Attractions for the Logistic Equation.
  2. Biology, Pest Integrated Management and Environmental: Growth Population Models for Formosan Subterranean Termites, Cockroaches and Fire Ants.

Suggested Exercises

Find similarities and differences for three different growth population models in which c = 3, L = 30,000, n = 50 and

  1. P0 is 0, 0.5, and 1, respectively.
  2. P0 is any three values between 0 < P0 < 1.
  3. P0 < 0, P0 > 1 or P0 = 2c? In each case, what is the enviromental significance of the result?

An ecologist is interested in studying a single species present in a residential neighborhood whose growth population is known to oscillate every 4 generations. The species affect other species and the neighborhood real estate property value. He examines four possible growth population models using P0 = 0.5, L = 20,000, and n = 100 at three different growth rates; i.e., c = 1.5, c = 3.2 and c = 3.5

  1. Compare the growth population dynamics in each case.
  2. Which of the three is a suitable working model and why?
  3. Suggest a working model that experience chaos, thus is not suitable for modeling the ecologist's case study.

References

  1. An Introduction to Chaotic Dynamical Systems; Robert L. Devaney, Addison, 1988.
  2. Chaos and Fractals; Robert L. Devaney and Linda Keen, Editors, American Mathematical Society, 1989.
  3. Chaos, Fractals and Dynamics; Robert L. Devaney, Addison, 1990.
  4. A First Course in Chaotic Dynamical Systems; Robert L. Devaney, Addison, 1992.

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