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  2. Rössler attractor - Wikipedia

    en.wikipedia.org/wiki/Rössler_attractor

    The Rössler attractor Rössler attractor as a stereogram with =, =, = The Rössler attractor (/ ˈ r ɒ s l ər /) is the attractor for the Rössler system, a system of three non-linear ordinary differential equations originally studied by Otto Rössler in the 1970s.

  3. Takens's theorem - Wikipedia

    en.wikipedia.org/wiki/Takens's_theorem

    Rössler attractor reconstructed by Takens' theorem, using different delay lengths. Orbits around the attractor have a period between 5.2 and 6.2. In the study of dynamical systems, a delay embedding theorem gives the conditions under which a chaotic dynamical system can be reconstructed from a sequence of observations of the state of that system.

  4. Attractor - Wikipedia

    en.wikipedia.org/wiki/Attractor

    The phase space is the horizontal complex plane; the vertical axis measures the frequency with which points in the complex plane are visited. The point in the complex plane directly below the peak frequency is the fixed point attractor. A fixed point of a function or transformation is a point that is mapped to itself by the function or ...

  5. Duffing equation - Wikipedia

    en.wikipedia.org/wiki/Duffing_equation

    The frequency response of this oscillator describes the amplitude of steady state response of the equation (i.e. ()) at a given frequency of excitation . For a linear oscillator with β = 0 , {\displaystyle \beta =0,} the frequency response is also linear.

  6. Lorenz system - Wikipedia

    en.wikipedia.org/wiki/Lorenz_system

    A sample solution in the Lorenz attractor when ρ = 28, σ = 10, and β = ⁠ 8 / 3 ⁠. The Lorenz system is a system of ordinary differential equations first studied by mathematician and meteorologist Edward Lorenz.

  7. Logistic map - Wikipedia

    en.wikipedia.org/wiki/Logistic_map

    The attractive fixed points and periodic points mentioned above are also members of the attractor family. The structure of the Feigenbaum attractor is the same as that of a fractal figure called the Cantor set. The number of points that compose the Feigenbaum attractor is infinite and their cardinality is equal to the real numbers.

  8. Phase portrait - Wikipedia

    en.wikipedia.org/wiki/Phase_portrait

    An attractor is a stable point which is also called a "sink". The repeller is considered as an unstable point, which is also known as a "source". A phase portrait graph of a dynamical system depicts the system's trajectories (with arrows) and stable steady states (with dots) and unstable steady states (with circles) in a phase space.

  9. Floris Takens - Wikipedia

    en.wikipedia.org/wiki/Floris_Takens

    Floris Takens (12 November 1940 – 20 June 2010) [1] was a Dutch mathematician known for contributions to the theory of chaotic dynamical systems.. Together with David Ruelle, he predicted that fluid turbulence could develop through a strange attractor, a term they coined, as opposed to the then-prevailing theory of accretion of modes.