Proceed to Safety

Gray-Scott Model at F 0.0620, k 0.0630    

These images and movie demonstrate the behavior of the Gray-Scott reaction-diffusion system with σ=Du/Dv=2 and parameters F=0.0620, k=0.0630.

Here a simple symmetrical starting loop grows into a convoluted form while remaining as a single closed loop, much like a Hilbert curve. Multiple loops generally remain separate while growing. As the space is filled, worm tips emerge from bends and lines shift to become more parallel. Most of the structure seen here remains after 1,250,000 tu.

Not shown here, a worm in isolation grows rapidly at the ends into a coral, with tips branching repeatedly and curving back upon themselves.

At F=0.0620, loops grow when k is about 0.0644 or less; above this k value (further east) they shrink to solitons.

Categories: Pearson κ; Wolfram 2-a      (glossary of terms)

                increase F   

decrease k
after 477 tu
after 2,385 tu

15 frames/sec.; each fr. is 159 iter. steps = 79.5 tu; 1800 fr. total (143,100 tu)

increase k
after 8,745 tu after 35,775 tu after 143,100 tu
                decrease F   
(Click on any image to magnify)

In these images:

Wavefronts and other moving objects have decreasing u values (brighter color) on the leading edge of the blue part of the moving object, and increasing u (light pastel color) on the trailing edge. This is true even for very slow-moving objects — thus, you can tell from the coloring what direction things are moving in.

''tu'' is the dimensionless unit of time, and ''lu'' the dimensionless unit of length, implicit in the equations that define the reaction-diffusion model. The grids for these simulations use Δx=1/143 lu and Δt=1/2 tu; the system is 3.2 lu wide. The simulation meets itself at the edges (periodic boundary condition); all images tile seamlessly if used as wallpaper.

Go back to Gray-Scott pattern index

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