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Lecture Notes in Differential Equations - Bruce E. Shapiro

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12 LESSON 2. A GEOMETRIC VIEW<br />

We can plug <strong>in</strong> numbers to get the position of our “particle” at any time<br />

t: At t = 0, y = e 0 = 1; at t = 0.1, y = e ( 0.1) ≈= 1.10517; at t = 0.2,<br />

y = e 0.2 ≈ 1.2214; etc. The correspond<strong>in</strong>g “trajectory” is plotted <strong>in</strong> the<br />

figure 2.1.<br />

Figure 2.1: Solution for example 2.1. Here the y axis gives the particle<br />

position as a function of time (the t or horizontal axis.<br />

1.3<br />

1.2<br />

0.2<br />

(0.2, e )<br />

y<br />

1.1<br />

1.<br />

(0,1)<br />

0.1<br />

(0.1, e )<br />

0.9<br />

0.1 0. 0.1 0.2 0.3<br />

t<br />

S<strong>in</strong>ce the solution of any (solvable 2 ) <strong>in</strong>itial value problem dy/dt = f(t, y),<br />

y(t 0 ) = y 0 is given by some function y = y(t), and because any function<br />

y = y(t) can be <strong>in</strong>terpreted as a trajectory, this tells us that any <strong>in</strong>itial value<br />

problem can be <strong>in</strong>terpreted geometrically <strong>in</strong> terms of a dynamical (mov<strong>in</strong>g<br />

or chang<strong>in</strong>g) system. 3 We say “geometrically” rather than “physically”<br />

because the dynamics may not follow the standard laws of physics (th<strong>in</strong>gs<br />

like F = ma) but <strong>in</strong>stead follow the rules def<strong>in</strong>ed by a differential equation.<br />

The geometric (or dynamic) <strong>in</strong>terpretation of the <strong>in</strong>itial value problem y ′ =<br />

y, y(0) = 1 given <strong>in</strong> the last example is is described by the plot of the<br />

trajectory (curve) of y(t) as a function of t.<br />

2 By solvable we mean any IVP for which a solution exists accord<strong>in</strong>g to the fundamental<br />

existence theorem (theorem 1.5). This does not necessarily mean that we can<br />

actually solve for (f<strong>in</strong>d) an equation for the solution.<br />

3 We will use the word “dynamics” <strong>in</strong> the sense that it is meant <strong>in</strong> mathematics<br />

and not <strong>in</strong> physics. In math a dynamical system is anyth<strong>in</strong>g that is chang<strong>in</strong>g <strong>in</strong><br />

time, hence dynamic. This often (though not always) means that it is governed by<br />

a differential equation. It does not have to follow the rules of Newtonian mechanics.<br />

The term “dynamical system” is frequently bandied about <strong>in</strong> conjunction with chaotic<br />

systems and chaos, but chaotic systems are only one type of dynamics. We will not<br />

study chaotic systems <strong>in</strong> this class but all of the systems we study can be considered<br />

dynamical systems.

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