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Linear flow on the torus
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Linear flow on the torus : ウィキペディア英語版
Linear flow on the torus
In mathematics, especially in the area of mathematical analysis known as dynamical systems theory, a linear flow on the torus is a flow on the ''n''-dimensional torus
:\mathbb^n = \underbrace_n
which is represented by the following differential equations with respect to the standard angular coordinates (θ1, θ2, ..., θ''n''):
:\frac=\omega_1, \quad \frac=\omega_2,\quad \cdots, \quad \frac=\omega_n.
The solution of these equations can explicitly be expressed as
:\Phi_\omega^t(\theta_1, \theta_2, \dots, \theta_n)=(\theta_1+\omega_1 t, \theta_2+\omega_2 t, \dots, \theta_n+\omega_n t) \mod 2\pi.
If we respesent the torus as R''n''/Z''n'' we see that a starting point is moved by the flow in the direction ω=(ω1, ω2, ..., ω''n'') at constant speed and when it reaches the border of the unitary ''n''-cube it jumps to the opposite face of the cube.
For a linear flow on the torus either all orbits are periodic or all orbits are dense on a subset of the ''n''-torus which is a ''k''-torus. When the components of ω are rationally independent all the orbits are dense on the whole space. This can be easily seen in the two dimensional case: if the two components of ω are rationally independent then the Poincaré section of the flow on an edge of the unit square is an irrational rotation on a circle and therefore its orbits are dense on the circle, as a consequence the orbits of the flow must be dense on the torus.
==See also==

*Completely integrable system
*Ergodic theory
*Quasiperiodic motion

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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