An implementation of the Lorenz dynamical system,
which describes the motion of a possible particle, which will
neither converge to a steady state, nor diverge to infinity;
but rather stay in a bounded but 'chaotically' defined
region, i.e., an attractor.
Usage
lorenzattractor(numsteps, dt, sigma, r, b)
Value
It returns a matrix with the 3 dimensions of the Lorenz
Arguments
numsteps
The number of simulated points
dt
System parameter
sigma
System parameter
r
System parameter
b
System parameter
Author
Moreno I. Coco (moreno.cocoi@gmail.com)
References
Lorenz, Edward Norton (1963). Deterministic nonperiodic flow.
Journal of the Atmospheric Sciences 20(2) 130-141.