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Steady State, Oscillation, and Chaos in Population Dynamics

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Modeling Dynamic Biological Systems

Part of the book series: Modeling Dynamic Systems ((MDS))

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Abstract

Let us return to the simple population models of Chapter 2, in the absence of randomness, and explore the behavior of a simple deterministic model as a parameter value gets pushed outside the realm that is typically considered in these models. Denote the size of the population in time period t as N(t) and the net change in the population size during that period as ΔN. The exogenous parameter influencing the net flow is R. The net flow ΔN updates the stock N:

$$ \Delta {\text{N = N(t + DT) - N(t)}}{\text{.}} $$
(1)

And then so slight, so delicate is death That there’s but the end of a leaf’s fall A moment of no consequence at all. Mark Swann, as quoted by Alfred Lotka, 1956, The Elements of Physical Biology, Dover, NY, p. 376

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Notes

  1. For a full discussion of this and other versions of chaos, see R.V. Jenson, Classical Chaos, American Scientist, 75:168–181, 1987.

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  2. S. Kaufman, The Origins of Order: Self Organization and Selection in Evolution, New York: Oxford University Press, 1993.

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© 1997 Springer Science+Business Media New York

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Ruth, M., Hannon, B. (1997). Steady State, Oscillation, and Chaos in Population Dynamics. In: Modeling Dynamic Biological Systems. Modeling Dynamic Systems. Springer, New York, NY. https://doi.org/10.1007/978-1-4612-0651-4_4

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  • DOI: https://doi.org/10.1007/978-1-4612-0651-4_4

  • Publisher Name: Springer, New York, NY

  • Print ISBN: 978-1-4612-6856-7

  • Online ISBN: 978-1-4612-0651-4

  • eBook Packages: Springer Book Archive

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