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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 135clear that <strong>the</strong> system’s state is converging <strong>to</strong> <strong>the</strong> stable equilibrium point while it is repellingfrom <strong>the</strong> unstable one. If you do <strong>the</strong> same for several different values <strong>of</strong> r, youobtain Fig. 8.2, which shows how <strong>to</strong> interpret this diagram.Figure 8.2: How <strong>to</strong> interpret a bifurcation diagram. Each vertical slice <strong>of</strong> <strong>the</strong> diagramdepicts a phase space <strong>of</strong> <strong>the</strong> system for a particular parameter value.There are o<strong>the</strong>r types <strong>of</strong> bifurcations. A transcritical bifurcation is a bifurcation whereone equilibrium point “passes through” ano<strong>the</strong>r, exchanging <strong>the</strong>ir stabilities. For example:dxdt = rx − x2 (8.8)This dynamical system always has <strong>the</strong> following two equilibrium pointsx eq = 0, r, (8.9)with <strong>the</strong> exception that <strong>the</strong>y collide when r = 0, which is when <strong>the</strong>y swap <strong>the</strong>ir stabilities.Its bifurcation diagram is shown in Fig. 8.3.Ano<strong>the</strong>r one is a pitchfork bifurcation, where an equilibrium point splits in<strong>to</strong> three. Two<strong>of</strong> <strong>the</strong>se (<strong>the</strong> outermost two) have <strong>the</strong> same stability as <strong>the</strong> original equilibrium point,while <strong>the</strong> one between <strong>the</strong>m has a stability opposite <strong>to</strong> <strong>the</strong> original one’s stability. Thereare two types <strong>of</strong> pitchfork bifurcations. A supercritical pitchfork bifurcation makes a stable

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