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| These equations were first studied by Edward Lorenz in the early 1960's. | |||
| The applet to the right shows the "Lorenz attractor" being created by taking randomly distributed points and following their evolution under the Lorenz equations. Newly introduced points are red, they turn blue as they "age". |
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| Lorenz considered the relatively harmless looking coupled non-linear differential equations. dy/dt = rx - y- xz dz/dt = xy - bz One commonly used set of constants is s = 10, b = 8 / 3, r = 28; this produces the "Lorenz attractor" shown in the applet above. If it were not for the two non-linear terms (xz in the second equation and xy in the third), the complete set of solutions would be expressible using at most one natural frequency. Lorenz found solutions that are nonperiodic; they cannot be represented using any finite number of frequencies. These solutions are also sensitively dependent on initial conditions, which means that for all practical purposes, prediction of the state of the system is limited to relatively short times. Moreover, regardless of the initial conditions, all solutions are attracted to the same strange attractor, which resembles a surface with two wings; it is, in fact, a fractal.
These pages are hosted by Mathematical Sciences Institute, ANU, and maintained by Brian Davies . e-mail
to Brian.Davies@anu.edu.au
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