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Lecture Notes in Differential Equations - Bruce E. Shapiro

Lecture Notes in Differential Equations - Bruce E. Shapiro

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14 LESSON 2. A GEOMETRIC VIEW<br />

Example 2.2. F<strong>in</strong>d and illustrate the one-parameter family of solutions<br />

for the ODE<br />

dy<br />

dt = − t (2.6)<br />

y<br />

Cross multiply<strong>in</strong>g and <strong>in</strong>tegrat<strong>in</strong>g<br />

∫ ∫<br />

ydy = −<br />

tdt (2.7)<br />

1<br />

2 y2 = − 1 2 t2 + C (2.8)<br />

Multiply<strong>in</strong>g through by 2, br<strong>in</strong>g<strong>in</strong>g the t to the left hand side and redef<strong>in</strong><strong>in</strong>g<br />

C ′ = 2C gives us<br />

y 2 + t 2 = C 2 (2.9)<br />

which we (should!) recognize as the equation of a circle of radius C. The<br />

curves for several values of C = 1, 2, . . . is illustrated <strong>in</strong> figure 2.3.<br />

Figure 2.3: One parameter family of solutions for example 2.2.<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

1<br />

2<br />

3<br />

4<br />

5<br />

6<br />

6 5 4 3 2 1 0 1 2 3 4 5 6<br />

Sometimes its not so easy to visualize the trajectories; a tool that gives us<br />

some help here is the direction field. The direction field is a plot of the<br />

slope of the trajectory. We know from the differential equation<br />

dy<br />

dt<br />

= f(t, y) (2.10)

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