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Introduction to the Modeling and Analysis of Complex Systems

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7.2. PHASE SPACE VISUALIZATION 115The first equation givesx = 0, or y = a b . (7.18)These are two straight lines, which constitute one set <strong>of</strong> nullclines for dx/dt = 0 (i.e., youcould call each line a single nullcline). In <strong>the</strong> meantime, <strong>the</strong> second one givesy = 0, or x = c d . (7.19)Again, <strong>the</strong>se two lines constitute ano<strong>the</strong>r set <strong>of</strong> nullclines for dy/dt = 0. These results canbe visualized manually as shown in Fig. 7.2. Equilibrium points exist where <strong>the</strong> two sets<strong>of</strong> nullclines intersect.yNullclines fordx/dt = 0a/bEquilibriumpointsNullclines fordy/dt = 00 c/dxFigure 7.2: Drawing a phase space (1): Adding nullclines.Everywhere on <strong>the</strong> first set <strong>of</strong> nullclines, dx/dt is zero, i.e., <strong>the</strong>re is no “horizontal”movement in <strong>the</strong> system’s state. This means that all local trajec<strong>to</strong>ries on <strong>and</strong> near thosenullclines must be flowing vertically. Similarly, everywhere on <strong>the</strong> second set <strong>of</strong> nullclines,dy/dt is zero, <strong>the</strong>refore <strong>the</strong>re is no “vertical” movement <strong>and</strong> all <strong>the</strong> local trajec<strong>to</strong>ries flowhorizontally. These facts can be indicated in <strong>the</strong> phase space by adding tiny line segmentson<strong>to</strong> each nullcline (Fig. 7.3).

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