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Lorenz attractor : ウィキペディア英語版
Lorenz system

The Lorenz system is a system of ordinary differential equations (the Lorenz equations, note it is not Lorentz) first studied by Edward Lorenz. It is notable for having chaotic solutions for certain parameter values and initial conditions. In particular, the Lorenz attractor is a set of chaotic solutions of the Lorenz system which, when plotted, resemble a butterfly or figure eight.
==Overview==
In 1963, Edward Lorenz developed a simplified mathematical model for atmospheric convection. The model is a system of three ordinary differential equations now known as the Lorenz equations:
: \begin
\frac &= \sigma (y - x), \\
\frac &= x (\rho - z) - y, \\
\frac &= x y - \beta z.
\end
Here x, y, and z make up the system state, t is time, and \sigma, \rho, \beta are the system parameters. The Lorenz equations also arise in simplified models for lasers, dynamos, thermosyphons, brushless DC motors, electric circuits, chemical reactions and forward osmosis.
From a technical standpoint, the Lorenz system is nonlinear, three-dimensional and deterministic. The Lorenz equations have been the subject of hundreds of research articles, and at least one book-length study.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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