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Introduction to the Modeling and Analysis of Complex Systems

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114 CHAPTER 7. CONTINUOUS-TIME MODELS II: ANALYSIS2.52.01.51.00.50.00.0 0.5 1.0 1.5 2.0 2.5Figure 7.1: Phase space drawn with Code 7.1.as “walls” that separate <strong>the</strong> phase space in<strong>to</strong> multiple contiguous regions. Inside eachregion, <strong>the</strong> signs <strong>of</strong> <strong>the</strong> time derivatives never change (if <strong>the</strong>y did, <strong>the</strong>y would be caughtin a nullcline), so just sampling one point in each region gives you a rough picture <strong>of</strong> how<strong>the</strong> phase space looks.Let’s learn how this analytical process works with <strong>the</strong> following Lotka-Volterra model:dx= ax − bxydt(7.13)dy= −cy + dxydt(7.14)x ≥ 0, y ≥ 0, a > 0, b > 0, c > 0, d > 0 (7.15)First, find <strong>the</strong> nullclines. This is a two-dimensional system with two time derivatives, so<strong>the</strong>re must be two sets <strong>of</strong> nullclines; one set is derived from dx/dt = 0, <strong>and</strong> ano<strong>the</strong>r set isderived from dy/dt = 0. They can be obtained by solving each <strong>of</strong> <strong>the</strong> following equations:0 = ax − bxy (7.16)0 = −cy + dxy (7.17)

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