Hans Jürgen Korsch, Hans-Jörg Jodl, Timo Hartmann's Chaos: A Program Collection for the PC, Third Edition PDF
By Hans Jürgen Korsch, Hans-Jörg Jodl, Timo Hartmann
ISBN-10: 3540748660
ISBN-13: 9783540748663
This new version strives another time to supply readers with a operating wisdom of chaos conception and dynamical platforms via parallel introductory factors within the e-book and interplay with carefully-selected courses provided at the accompanying diskette. The courses allow readers, specially advanced-undergraduate scholars in physics, engineering, and math, to take on appropriate actual platforms speedy on their desktops, with no distraction from algorithmic info. For the 3rd version of Chaos: A application assortment for the computer, all the past twelve courses is polished and rewritten in C++ (both home windows and Linux types are included). a brand new application treats kicked structures, an enormous classification of two-dimensional difficulties, that's brought in bankruptcy thirteen. each one bankruptcy follows the constitution: theoretical heritage; numerical concepts; interplay with this system; desktop experiments; actual experiments and empirical proof; reference. Interacting with the various numerical experiments have confirmed to assist readers to get to grips with this interesting subject or even to benefit from the event.
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Extra info for Chaos: A Program Collection for the PC, Third Edition
Example text
Exactly at the crossing we have neutral stability and the iterates trace out an elliptic orbit. — For a negative real part, the iterates spiral and oscillate simultaneously. In addition, the behavior can be sensitively dependent on the phase of the eigenvalues at the crossing point of the unit circle. 4 Special Topics 41 orbit, which slowly contracts (inside the stability region) or expands (outside the stability region). The interested reader can investigate these bifurcations numerically in some of the computer experiments described below (most directly for the two-dimensional maps studied in Chap.
Such an attracting periodic solution is called a ‘limit cycle’ . 30), various limit cycles may coexist. This is explored in more detail in Chap. 8. In addition, the period of the limit cycle may be entirely determined by intrinsic properties of the system, and not by any external driving function. Other simple attractors are two-dimensional tori embedded in phase space and supporting a limiting quasiperiodic oscillation characterized by two frequencies. When a parameter of the systems is varied slowly, the attracting limit points and limit cycles also change, while remaining structurally similar.
In addition, the period of the limit cycle may be entirely determined by intrinsic properties of the system, and not by any external driving function. Other simple attractors are two-dimensional tori embedded in phase space and supporting a limiting quasiperiodic oscillation characterized by two frequencies. When a parameter of the systems is varied slowly, the attracting limit points and limit cycles also change, while remaining structurally similar. , change their character, split into pairs, disappear, etc.
Chaos: A Program Collection for the PC, Third Edition by Hans Jürgen Korsch, Hans-Jörg Jodl, Timo Hartmann
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