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Titlebook: Chaos; A Program Collection H. J. Korsch,H.-J. Jodl Book 19941st edition Springer-Verlag Berlin Heidelberg 1994 Chaostheorie.Fractals.Frakt

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樓主: solidity
11#
發(fā)表于 2025-3-23 12:55:10 | 只看該作者
12#
發(fā)表于 2025-3-23 16:08:36 | 只看該作者
Other Classes of Crystallizationcause they are discrete, such maps are much simpler to study (both numerically and analytically) than continuous differential equations. In general, the maps can be written as., where . = (..,..., ..) is the state vector of the system — for example, a vector in .-dimensional phase space — and . = (.
13#
發(fā)表于 2025-3-23 21:41:54 | 只看該作者
14#
發(fā)表于 2025-3-23 23:14:13 | 只看該作者
Y. Zhang. In everyday life we feel safer and more comfortable with predictability and determinism: in technically controlled processes, small mechanical forces are expected to cause minor changes; the time-table of trains is hopefully reliable; the motion of the earth and moon around the sun are thought to be regular and stable.
15#
發(fā)表于 2025-3-24 05:15:50 | 只看該作者
Overview and Basic Concepts,. In everyday life we feel safer and more comfortable with predictability and determinism: in technically controlled processes, small mechanical forces are expected to cause minor changes; the time-table of trains is hopefully reliable; the motion of the earth and moon around the sun are thought to be regular and stable.
16#
發(fā)表于 2025-3-24 08:16:34 | 只看該作者
17#
發(fā)表于 2025-3-24 12:10:15 | 只看該作者
18#
發(fā)表于 2025-3-24 17:23:49 | 只看該作者
19#
發(fā)表于 2025-3-24 21:08:35 | 只看該作者
Other Classes of Crystallizationcause they are discrete, such maps are much simpler to study (both numerically and analytically) than continuous differential equations. In general, the maps can be written as., where . = (..,..., ..) is the state vector of the system — for example, a vector in .-dimensional phase space — and . = (..,..., ..) denotes a number of . parameters .
20#
發(fā)表于 2025-3-24 23:41:46 | 只看該作者
Other Classes of Crystallizationtems . where the time derivatives of the canonical coordinates and momenta are given by the partial derivatives of the Hamiltonian. Typically, the right hand side of these equations is a nonlinear function of the variables .. and .. i.e. (12.1) is a nonlinear dynamical system.
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