Home Download Help Forum Resources Extensions FAQ NetLogo Publications Contact Us Donate Models: Library Community Modeling Commons Beginners Interactive NetLogo Dictionary (BIND) NetLogo Dictionary User Manuals: Web Printable Chinese Czech Farsi / Persian Japanese Spanish

NetLogo User Community Models(back to the NetLogo User Community Models)
WHAT IS IT?
This is a model of a 2D cellular automaton where each cell's state can take a real value between 0 and 1 and the stateupdating rule consists of a coupled chaotic map (in this case the logistic map). Each cell 'reads' its own state and the state of each of its four neighbours and updates its state accordingly. The result is an everchanging aperiodic spatiotemporal pattern with large clusters of cells with states near each other; moreover, the global pattern emerges from a random initial condition, showing a more organized structure.
HOW IT WORKS
Each cell starts by being in a random state between 0 and 1, and it updates its state at each time step by applying the following rules:
 "Read your current state (si(t));
si(t+1) = A [wi si(t) + (1  wi) sa(t)] [1  (wi si(t) + (1  wi) sa(t))]
where, wi is a coefficient between 0 and 1, and represents the weight that a cell gives to its own current state when determining its new state (and 1  wi is the weight each cell gives to its neighbours). In the current model we set wi to be equal to 0.5.
If we take A = 4 we get the well known logistic map's chaotic dynamics, for A < 4 we get different types of dynamics, from fixed points to periodic dynamics.
HOW TO USE IT
There are two items on the interface tab, one is a slider rule for the A parameter, you can set it to different values than 4 and see what type of dynamic you get from there, the other is a 'turnon neighbours/shutoff neighbours button', it allows you to see the results in the dynamics without any neighbour interaction and the dynamics with neighbour interaction. If you start with the neighbours button in the off position and turn it on latter you can see the effects of the coupling on the pattern. You can also see the graph of the series of the states of a patch previously chosen, to get the feeling of how the global network of cells affects a given local cell.
THINGS TO NOTICE
Start the model with neighbour coupling on, and notice how an organized pattern emerges from a previously disorganized one.
Notice also the differences in the local dynamics and in the global pattern from the uncoupled to the coupled case.
THINGS TO TRY
Do try:
 Different values for the parameter A, to see the different dynamics, and try to start with very low values increasing the parameter progressively to higher values to see the bifurcation structure;
Notice also that each cell has a state defined by real numbers between 0 and 1, and the grey colours you see are the result of multiplying the cells' state by 10, if you multiply by 100, for instance, you get a multicoloured pattern. Try to change the code and multiply the cell's state by 100 or even 1000, and try to identify the patterns in these different colour schemes (note that if you multiply the cells' state by 100 or 1000 you are actually enhancing what might be called the "resolution" with which you observe the system, and, thus you are really seeing more and more details and more and more differences).
EXTENDING THE MODEL
You could try to change the weights that a given cell attributes to itself and its neighbours, different neighbourhood structure, different nonlinear maps.
One thing that might be interesting to try would be to set the following colour scheme: if the patch state is above a given state (for instance 0.5) set the colour blue, else, set the colour green, you can proceed in this manner with more and more fine partitions of the unit interval to see how the different cells visit the different subintervals of a given partition of the unit interval.
CREDITS AND REFERENCES
Some references on deterministic chaos and spatiotemporal complexity:
BlancTalon, Jacques and Deniau, Laurent., PCA and CA: a statistical approach for deterministic machines, Complexity International, Vol. 2, 1995
BlancTalon, Jacques, Effective Computation of 2D Coupled Map Lattices, Complexity International, Vol.6, 1998
Deane, Deane, J.H.B. and Jefferies, D.J., The Behaviour of Coupled Map Chains, Complexity International, Vol.3, 1996
Cvitanovic, P., Universality in Chaos, 2nd Edition, Bristol: Institute of Physics Publishing, 1993
Gottlieb, H.P.W., Properties of Some Generalised Logistic Maps with Fractional Exponents, Complexity International, Vol. 2, 1995
Gulick, Denny, Encounters With Chaos, McGrawHill, 1992
Kaplan, Daniel, Glass, Leon, Understanding Nonlinear Dynamics, SpringerVerlag, New York, 1995
Shibata, Tatsuo, Chawanya, Tsuyoshi, Kaneko, Kunihiko, Noiseless Collective Motion out of Noisy Chaos, obtained from website http://arxiv.org/pdf/chaodyn/9812007
Stogratz, Steven H., Nonlinear Dynamics and Chaos, Perseus Books, 1994
Web site for Complexity International:

(back to the NetLogo User Community Models)