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Lecture Notes in Differential Equations - Bruce E. Shapiro

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168 LESSON 19. METHOD OF UNDETERMINED COEFFICIENTS<br />

The second <strong>in</strong>itial condition is y ′ (0) = −1 so that<br />

− 1 = 2C 2 (19.58)<br />

hence<br />

y = − 1 2 s<strong>in</strong> 2t + 3 t s<strong>in</strong> 2t (19.59)<br />

4<br />

Example 19.5. Solve the <strong>in</strong>itial value problem<br />

⎫<br />

y ′′ − y = t + e 2t ⎪⎬<br />

y(0) = 0<br />

⎪⎭<br />

y ′ (0) = 1<br />

(19.60)<br />

The characteristic equation is r 2 − 1 = 0 so that<br />

y H = C 1 e t + C 2 e −t (19.61)<br />

For a particular solution we try a l<strong>in</strong>ear comb<strong>in</strong>ation of particular solutions<br />

for each of the two forc<strong>in</strong>g functions,<br />

Substitut<strong>in</strong>g <strong>in</strong>to the differential equation,<br />

y P = At + B + Ce 2t (19.62)<br />

y ′ P = A + 2Ce 2t (19.63)<br />

y ′′<br />

P = 4Ce 2t (19.64)<br />

4Ce 2t − At − B − Ce 2t = t + e 2t (19.65)<br />

3Ce 2t − At − B = t + e 2t (19.66)<br />

A = −1 (19.67)<br />

B = 0 (19.68)<br />

C = 1 3<br />

(19.69)<br />

Hence<br />

y = C 1 e t + C 2 e −t − t + 1 3 e2t (19.70)<br />

From the first <strong>in</strong>itial condition, y(0) = 0,<br />

0 = C 1 + C 2 + 1 3<br />

(19.71)<br />

From the second <strong>in</strong>itial condition y ′ (0) = 1,<br />

1 = C 1 − C 2 + 2 3<br />

(19.72)

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