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Introduction to the Modeling and Analysis of Complex Systems

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8.2. BIFURCATIONS IN 1-D CONTINUOUS-TIME MODELS 139output (asymp<strong>to</strong>tic state in this case) not only on <strong>the</strong> input (parameter r in this case) butalso on its his<strong>to</strong>ry. To underst<strong>and</strong> what this means, imagine that you are slowly changingr from -1 upward. Initially, <strong>the</strong> system’s state stays at <strong>the</strong> stable equilibrium at <strong>the</strong> bot<strong>to</strong>m<strong>of</strong> <strong>the</strong> diagram, which continues until you reach a critical threshold at r ≈ 0.4. As soon asyou cross this threshold, <strong>the</strong> system’s state suddenly jumps up <strong>to</strong> ano<strong>the</strong>r stable equilibriumpoint at <strong>the</strong> <strong>to</strong>p <strong>of</strong> <strong>the</strong> diagram. Such a sudden jump in <strong>the</strong> system’s state is <strong>of</strong>tencalled a catastrophe. You get upset, <strong>and</strong> try <strong>to</strong> bring <strong>the</strong> system’s state back <strong>to</strong> whereit was, by reducing r. However, counter <strong>to</strong> your expectation, <strong>the</strong> system’s state remainshigh even after you reduce r below 0.4. This is hysteresis; <strong>the</strong> system’s asymp<strong>to</strong>tic statedepends not just on r, but also on where its state was in <strong>the</strong> immediate past. In o<strong>the</strong>rwords, <strong>the</strong> system’s state works as a memory <strong>of</strong> its his<strong>to</strong>ry. In order <strong>to</strong> bring <strong>the</strong> system’sstate back down <strong>to</strong> <strong>the</strong> original value, you have <strong>to</strong> spend extra effort <strong>to</strong> reduce r all <strong>the</strong>way below ano<strong>the</strong>r critical threshold, r ≈ −0.4.Such hysteresis could be useful; every bit (binary digit) <strong>of</strong> computer memory has thiskind <strong>of</strong> bifurcation dynamics, which is why we can s<strong>to</strong>re information in it. But in o<strong>the</strong>r contexts,hysteresis could be devastating—if an ecosystem’s state has this property (manystudies indicate it does), it takes a huge amount <strong>of</strong> effort <strong>and</strong> resources <strong>to</strong> revert a desertedecosystem back <strong>to</strong> a habitat with vegetation, for example.Exercise 8.1 Conduct a bifurcation analysis <strong>of</strong> <strong>the</strong> following dynamical systemwith parameter r:dxdt= rx(x + 1) − x (8.17)Find <strong>the</strong> critical threshold <strong>of</strong> r at which a bifurcation occurs. Draw a bifurcationdiagram <strong>and</strong> determine what kind <strong>of</strong> bifurcation it is.Exercise 8.2 Assume that two companies, A <strong>and</strong> B, are competing against eacho<strong>the</strong>r for <strong>the</strong> market share in a local region. Let x <strong>and</strong> y be <strong>the</strong> market share <strong>of</strong>A <strong>and</strong> B, respectively. Assuming that <strong>the</strong>re are no o<strong>the</strong>r third-party competi<strong>to</strong>rs,x + y = 1 (100%), <strong>and</strong> <strong>the</strong>refore this system can be unders<strong>to</strong>od as a one-variablesystem. The growth/decay <strong>of</strong> A’s market share can thus be modeled asdx= ax(1 − x)(x − y), (8.18)dtwhere x is <strong>the</strong> current market share <strong>of</strong> A, 1 − x is <strong>the</strong> size <strong>of</strong> <strong>the</strong> available potentialcus<strong>to</strong>mer base, <strong>and</strong> x − y is <strong>the</strong> relative competitive edge <strong>of</strong> A, which can be

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