StarLogo Simulation of Streaming Aggregation. Demonstration of StarLogo Simulation of Streaming. Differentiation & Pattern Formation.
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1 StarLogo Simulation of Streaming Aggregation 1. chemical diffuses 2. if cell is refractory (yellow) 3. then chemical degrades 4. else (it s excitable, colored white) 1. if chemical > movement threshold then take step up chemical gradient 2. else if chemical > relay threshold then produce more chemical (red) become refractory 3. else wait 9/13/04 1 Demonstration of StarLogo Simulation of Streaming Run SlimeStream.slogo 9/13/04 2 Differentiation & Pattern Formation A central problem in development: How do cells differentiate to fulfill different purposes? How do complex systems generate spatial & temporal structure? CAs are natural models of intercellular communication Zebra 9/13/04 photos 2000, S. Cazamine 3 9/13/04 figs. from Cazamine & al.: Self-Org. Biol. Sys. 4 1
2 Vermiculated Rabbit Fish Activation & Inhibition in Pattern Formation Color patterns typically have a characteristic length scale Independent of cell size and animal size Achieved by: short-range activation local uniformity long-range inhibition separation 9/13/04 figs. from Cazamine & al.: Self-Org. Biol. Sys. 5 9/13/04 6 Emergent Hierarchical Structure Interaction Parameters Characteristic length scale Independent of cell size and space size Structures created at intermediate level R 1 and R 2 are the interaction ranges J 1 and J 2 are the interaction strengths 9/13/04 7 9/13/04 8 2
3 CA Activation/Inhibition Model Example (R 1 =1, R 2 =6, J 1 =1, J 2 = 0.1, h=0) Let states s i { 1, +1} and h be a bias parameter and r ij be the distance between cells i and j Then the state update rule is: s i ( t +1)= sign h + J 1 s j () t + J 2 s j () t r ij <R 1 R 1 <r ij <R 2 9/13/04 9 9/13/04 figs. from Bar-Yam 10 Effect of Bias (h = 6, 3, 1; 1, 3, 6) Effect of Interaction Ranges R 2 = 6 R 1 = 1 h = 0 R 2 = 8 R 1 = 1 h = 0 R 2 = 6 R 1 = 1.5 h = 0 R 2 = 6 R 1 = 1.5 h = 3 9/13/04 figs. from Bar-Yam 11 9/13/04 figs. from Bar-Yam 12 3
4 Differential Interaction Ranges How can a system using strictly local interactions discriminate between states at long and short range? E.g. cells in developing organism Can use two different morphogens diffusing at two different rates activator diffuses slowly (short range) inhibitor diffuses rapidly (long range) 9/13/04 13 Digression on Diffusion Simple 2-D diffusion equation: A ( x, y)= c 2 Ax, y Recall the 2-D Laplacian: ( ) 2 Ax, ( y)= 2 Ax, y x 2 ( ) + 2 Ax, ( y) y 2 The Laplacian (like 2 nd derivative) is: positive in a local minimum negative in a local maximum 9/13/04 14 Reaction-Diffusion System diffusion A t = d 2 A A + f A A,I I t = d I 2 I + f I ( A,I) ( ) A = d A 0 2 A t I 0 d I 2 I + f ( A,I ) A f I ( A,I) c = D 2 c + fc (), where c = A I reaction 9/13/04 15 Example: Activation-Inhibition System Let be the logistic sigmoid function Activator A and inhibitor I may diffuse at different rates in x and y directions Cell is on if activator + bias exceeds inhibitor A t = d 2 A Ax x + d 2 A 2 Ay y + k A m 2 A ( A + B I) [ ] I t = d 2 I Ix x + d 2 I 2 Iy y + k I m 2 I ( A + B I) [ ] 9/13/
5 Demonstration of StarLogo Program for Activation/Inhibition Pattern Formation Run Pattern.slogo 9/13/04 17 Abstract Activation/Inhibition Spaces Consider two axes of cultural preference E.g. hair length & interpersonal distance Fictitious example! Suppose there are no objective reasons for preferences Suppose people approve/encourage those with similar preferences Suppose people disapprove/discourage those with different preferences What is the result? 9/13/04 18 Emergent Regions of Acceptable Variation A Key Element of Self-Organization Activation vs. Inhibition Cooperation vs. Competition Amplification vs. Stabilization Growth vs. Limit Positive Feedback vs. Negative Feedback Positive feedback creates Negative feedback shapes 9/13/ /13/
6 Additional Bibliography 1. Kessin, R. H. Dictyostelium: Evolution, Cell Biology, and the Development of Multicellularity. Cambridge, Gerhardt, M., Schuster, H., & Tyson, J. J. A Cellular Automaton Model of Excitable Media Including Curvature and Dispersion, Science 247 (1990): Tyson, J. J., & Keener, J. P. Singular Perturbation Theory of Traveling Waves in Excitable Media (A Review), Physica D 32 (1988): Camazine, S., Deneubourg, J.-L., Franks, N. R., Sneyd, J., Theraulaz, G.,& Bonabeau, E. Self-Organization in Biological Systems. Princeton, Pálsson, E., & Cox, E. C. Origin and Evolution of Circular Waves and Spiral in Dictyostelium discoideum Territories, Proc. Natl. Acad. Sci. USA: 93 (1996): Solé, R., & Goodwin, B. Signs of Life: How Complexity Pervades Biology. Basic Books, /13/04 21 continue to Autonomous Agents 6
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