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Introduction to the Modeling and Analysis of Complex Systems

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Chapter 14Continuous Field Models II: <strong>Analysis</strong>14.1 Finding Equilibrium StatesOne nice thing about PDE-based continuous field models is that, unlike CA models, everythingis still written in smooth differential equations so we may be able <strong>to</strong> conductsystematic ma<strong>the</strong>matical analysis <strong>to</strong> investigate <strong>the</strong>ir dynamics (especially <strong>the</strong>ir stabilityor instability) using <strong>the</strong> same techniques as those we learned for non-spatial dynamicalsystems in Chapter 7.The first step is, as always, <strong>to</strong> find <strong>the</strong> system’s equilibrium states. Note that this is nolonger about equilibrium “points,” because <strong>the</strong> system’s state now has spatial extensions.In this case, <strong>the</strong> equilibrium state <strong>of</strong> an au<strong>to</strong>nomous continuous field model(∂f∂t = F f, ∂f )∂x , ∂2 f∂x , . . . (14.1)2is given as a static spatial function f eq (x), which satisfies(0 = F f eq , ∂f )eq∂x , ∂2 f eq∂x , . . . . (14.2)2For example, let’s obtain <strong>the</strong> equilibrium state <strong>of</strong> a diffusion equation in a 1-D spacewith a simple sinusoidal source/sink term:∂c∂t = D∇2 c + sin x (−π ≤ x ≤ π) (14.3)The source/sink term sin x means that <strong>the</strong> “stuff” is being produced where 0 < x ≤ π,while it is being drained where −π ≤ x < 0. Ma<strong>the</strong>matically speaking, this is still a nonau<strong>to</strong>nomoussystem because <strong>the</strong> independent variable x appears explicitly on <strong>the</strong> right269

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