This nonlinear system with specific initial conditions is solved
numerically and the resulting trajectory is shown through a 3 dimensional animation.
[www.3d-meier.de...]
Initial condition 1: (1. ,1., 1.05)
Initial condition 2: (1.05,1., 1. )
"When the parameters a = 36 and b = 3 are fixed while parameter c varies, one can observe that the attractor generated by this system is similar to the Lorenz attractor for c in (12.7 -17.0), has a transitory shape when 'c' is between 18.0 to 22.0, and then becomes similar to Chen’s attractor when 'c' is in range of 23.0 - 28.5"
Reference: A NEW CHAOTIC ATTRACTOR COINED JINHU LÜ, GUANRONG CHEN
International Journal of Bifurcation and Chaos, Vol. 12, No. 3 (2002) 659-661
lsc.amss.ac.cn/...
In 1963, Lorenz reported the first chaotic attractor in a three-dimensional autonomous system [Sparrow, 1982].
Since Lorenz found the first chaotic attractor in a smooth three-dimensional autonomous system, later chaotic attractors were developed, for example the Rossler system, the Sprott system, the Chen system, the Lu system, the generalized Lorenz system family, and the hyperbolic type of the generalized Lorenz canonical form. Here one of such attractor is shown in this video.
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#ChenCelikovsky|#ChaoticSystem #ButterflyEffect| thinkeccel
27 сен 2024