BCSSS

International Encyclopedia of Systems and Cybernetics

2nd Edition, as published by Charles François 2004 Presented by the Bertalanffy Center for the Study of Systems Science Vienna for public access.

About

The International Encyclopedia of Systems and Cybernetics was first edited and published by the system scientist Charles François in 1997. The online version that is provided here was based on the 2nd edition in 2004. It was uploaded and gifted to the center by ASC president Michael Lissack in 2019; the BCSSS purchased the rights for the re-publication of this volume in 200?. In 2018, the original editor expressed his wish to pass on the stewardship over the maintenance and further development of the encyclopedia to the Bertalanffy Center. In the future, the BCSSS seeks to further develop the encyclopedia by open collaboration within the systems sciences. Until the center has found and been able to implement an adequate technical solution for this, the static website is made accessible for the benefit of public scholarship and education.

A B C D E F G H I J K L M N O P Q R S T U V W Y Z

LIAPOUNOV EXPONENT 2)5)

The exponent of the function e established by LIAPOUNOV.

LIAPOUNOV's exponents express the rate of separation or convergence of a dynamic system's trajectories. "And if either of these numbers is positive, indicating a positive rate of separation of the initial points in a given direction, we say that the system is chaotic" (J. CASTI, 1990, p.100).

"A negative exponent means limit cycles and at least a somewhat regular behavior. A positive exponent means chaos"(C. ZIMMER, 2000, p.84)

J. GLEICK explains: "The Lyapunov exponents in a system provide a way of measuring the conflicting effects of stretching, contracting and folding in the phase space of an attractor. They give a picture of all the properties of a system that lead to stability or instability. An exponent greater than zero means stretching – nearby points would separate. An exponent smaller than zero means contraction… For a fixed-point attractor, all the Lyapunov exponents are negative, since the direction of pull is inward toward the final steady state. An attractor in the form of a periodic orbit has one exponent of exactly zero and other exponents… negative. A strange attractor… has… at least one positive Lyapunov exponent" (1987, p.252).

In I. PRIGOGINE and I. STENGERS words: "A behavior is chaotic if trajectories starting from points as close as wanted in the phase space, move away from each other in time in an exponential way. The distance between any two points belonging to such trajectories grows thus in proportion to a function e, in which, positive by definition for chaotic systems is Lyapunov's exponent and Lyapunov's time… After an evolution time long in relation to Lyapunov's time, the knowledge that we possessed from the initial state of the system has lost its relevance and does not permit us anymore to determine its trajectory" (1992, p.77).

Thus, when is positive, it defines irreversibility in time, in conformity with the 2nd. Law of thermodynamics.

Categories

  • 1) General information
  • 2) Methodology or model
  • 3) Epistemology, ontology and semantics
  • 4) Human sciences
  • 5) Discipline oriented

Publisher

Bertalanffy Center for the Study of Systems Science(2020).

To cite this page, please use the following information:

Bertalanffy Center for the Study of Systems Science (2020). Title of the entry. In Charles François (Ed.), International Encyclopedia of Systems and Cybernetics (2). Retrieved from www.systemspedia.org/[full/url]


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