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Introduction to the Modeling and Analysis of Complex Systems

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100 CHAPTER 6. CONTINUOUS-TIME MODELS I: MODELING6.2 Classifications <strong>of</strong> Model EquationsDistinctions between linear <strong>and</strong> nonlinear systems as well as au<strong>to</strong>nomous <strong>and</strong> non-au<strong>to</strong>nomoussystems, which we discussed in Section 4.2, still apply <strong>to</strong> continuous-time models. But<strong>the</strong> distinction between first-order <strong>and</strong> higher-order systems are slightly different, as follows.First-order system A differential equation that involves first-order derivatives <strong>of</strong> statevariables ( dxdt ) only.Higher-order system A differential equation that involves higher-order derivatives <strong>of</strong>state variables ( d2 xdt , d3 x2 dt , etc.).3Luckily, <strong>the</strong> following is still <strong>the</strong> case for continuous-time models as well:Non-au<strong>to</strong>nomous, higher-order differential equations can always be converted in<strong>to</strong>au<strong>to</strong>nomous, first-order forms by introducing additional state variables.Here is an example:d 2 θdt = − g sin θ (6.3)2 LThis equation describes <strong>the</strong> swinging motion <strong>of</strong> a simple pendulum, which you might haveseen in an intro <strong>to</strong> physics course. θ is <strong>the</strong> angular position <strong>of</strong> <strong>the</strong> pendulum, g is <strong>the</strong>gravitational acceleration, <strong>and</strong> L is <strong>the</strong> length <strong>of</strong> <strong>the</strong> string that ties <strong>the</strong> weight <strong>to</strong> <strong>the</strong>pivot. This equation is obviously nonlinear <strong>and</strong> second-order. While we can’t remove<strong>the</strong> nonlinearity from <strong>the</strong> model, we can convert <strong>the</strong> equation <strong>to</strong> a first-order form, byintroducing <strong>the</strong> following additional variable:ω = dθdt(6.4)Using this, <strong>the</strong> left h<strong>and</strong> side <strong>of</strong> Eq. (6.3) can be written as dω/dt, <strong>and</strong> <strong>the</strong>refore, <strong>the</strong>equation can be turned in<strong>to</strong> <strong>the</strong> following first-order form:dθdt = ω (6.5)dωdt = − g sin θL(6.6)

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