[2.7] How are maps related to flows (differential equations)? Every differential equation gives rise to a map, the time one map, defined b y advancing the flow one unit of time. This map may or may not be useful. If the differential equation contains a term or terms periodic in time, then t he time T map (where T is the period) is very useful--it is an example of a Poincar□ section. The time T map in a system with periodic terms is also ca lled a stroboscopic map, since we are effectively looking at the location in phase space with a stroboscope tuned to the period T. This map is useful be cause it permits us to dispense with time as a phase space coordinate: the r emaining coordinates describe the state completely so long as we agree to co nsider the same instant within every period. In autonomous systems (no time-dependent terms in the equations), it may als o be possible to define a Poincar□ section and again reduce the phase space dimension by one. Here the Poincar□ section is defined not by a fixed time interval, but by successive times when an orbit crosses a fixed surface in phase space. (Surface here means a manifold of dimension one less than the p hase space dimension). However, not every flow has a global Poincar□ section (e.g. any flow with a n equilibrium point), which would need to be transverse to every possible or bit. Maps arising from stroboscopic sampling or Poincar□ section of a flow are n ecessarily invertible, because the flow has a unique solution through any po int in phase space--the solution is unique both forward and backward in time . However, noninvertible maps can be relevant to differential equations: Poi ncar□ maps are sometimes very well approximated by noninvertible maps. For example, the Henon map (x,y) -> (-y-a+x^2,bx) with small |b| is close to the logistic map, x -> -a+x^2. It is often (though not always) possible to go backwards, from an invertible map to a differential equation having the map as its Poincar□ map. This is called a suspension of the map. One can also do this procedure approximatel y for maps that are close to the identity, giving a flow that approximates t he map to some order. This is extremely useful in bifurcation theory. Note that any numerical solution procedure for a differential initial value problem which uses discrete time steps in the approximation is effectively a map. This is not a trivial observation; it helps explain for example why a continuous-time system which should not exhibit chaos may have numerical sol utions which do--see [2.15]. -- 在细雨的午後 书页里悉哩哩地传来 " 周期3 = ? " 然而我知道 当我正在日耳曼深处的黑森林 继续发掘海森堡未曾做过的梦时 康德的诺言早已远离......... 远来的传教士静静地看着山涧不断反覆叠代自己的 过去 现在 和 未来 於是仅以 一颗量子浑沌 一本符号动力学 祝那发生在周一下午的新生 --

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