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LATENT REFERENCES / TAG2

Chaos Theory and the Lorenz Equations

This reference note belongs to Tag2 in Latent References, an archive curated by Keigo Yoshida. Its archive region is Chaos theory · Lorenz equations. The note preserves its source text and links so that readers can trace the material behind the 3D map.

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Tag2
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Chaos theory · Lorenz equations

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Chaos theory (Japanese reading: kaosu riron; English: chaos theory; German: Chaosforschung; French: théorie du chaos) studies phenomena displaying complex behavior found in some dynamical systems, considered unpredictable because of numerical errors. Also called chaotic dynamics. Unpredictable here by no means means random. Although its behavior follows deterministic laws, solutions cannot be obtained by integration, so numerical analysis must be used to learn its future (and past) behavior. However, sensitivity to initial values requires information of infinite precision at a given time, and errors arising during numerical analysis (inevitably, because computers cannot handle infinitely many digits) also amplify the discrepancy between obtained values and true values. It means prediction is therefore practically impossible. The Lorenz equations are nonlinear ordinary differential equations first studied by mathematician and meteorologist Edward Lorenz. They attract attention for having chaotic solutions for particular parameter values and initial conditions. In particular, the set of chaotic solutions of the Lorenz equations is called the Lorenz attractor. Often used to explain the so-called butterfly effect, the sensitivity to initial values of deterministic simultaneous ordinary differential equations was met with surprise and sparked research into chaos. https://scrapbox.io/files/65a5eadf6fa05f00239856d6.png Solution trajectories of the chaotic Lorenz equations.

Source updated 2024-01-16 · Snapshot 2026-10-08

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