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Lecture Notes in Differential Equations - Bruce E. Shapiro

Lecture Notes in Differential Equations - Bruce E. Shapiro

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376 LESSON 34. CRITICAL POINTS<br />

The <strong>in</strong>itial conditions for (34.11) give<br />

hence the solution is<br />

The trajectory is the unit circle because<br />

0 = A cos 0 + B s<strong>in</strong> 0 = A (34.18)<br />

1 = −A s<strong>in</strong> 0 + B cos 0 = B (34.19)<br />

y = s<strong>in</strong> t (34.20)<br />

x = cos t (34.21)<br />

x 2 + y 2 = 1 (34.22)<br />

for all t, and the solution is the set of all po<strong>in</strong>ts start<strong>in</strong>g at an angle of 0<br />

from the x axis.<br />

The <strong>in</strong>itial conditions for (34.13), on the other hand, give<br />

add<strong>in</strong>g the two equations<br />

√ √<br />

2 2<br />

0 = A<br />

2 + B √<br />

2<br />

√<br />

2 2<br />

1 = −A<br />

2 + B 2<br />

(34.23)<br />

(34.24)<br />

1 = 2B<br />

√<br />

2<br />

2 = B√ 2 =⇒ B = 1 √<br />

2<br />

=<br />

√<br />

2<br />

2<br />

(34.25)<br />

hence<br />

which gives a solution of<br />

√<br />

2<br />

A = −B = −<br />

2<br />

(34.26)<br />

√ √<br />

2 2<br />

y = −<br />

2 cos t + s<strong>in</strong> t (34.27)<br />

√ √<br />

2<br />

2 2<br />

x =<br />

2 s<strong>in</strong> t + cos t (34.28)<br />

2

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