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Lecture Notes in Differential Equations - Bruce E. Shapiro

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210 LESSON 24. VARIATION OF PARAMETERS<br />

Next, we need to f<strong>in</strong>d a particular solution; we can do this us<strong>in</strong>g the variation<br />

of parameters formula. S<strong>in</strong>ce a(t) = t 2 and f(t) = 2t, we have<br />

∫<br />

∫<br />

y2 (t)f(t)<br />

y P = −y 1 (t)<br />

a(t)W (t) dt + y y1 (t)f(t)<br />

2(t)<br />

dt (24.49)<br />

a(t)W (t)<br />

We previously had W = C; but here we need an exact value. To get<br />

the exact value of C, we calculate the Wronsk<strong>in</strong>a from the now-known<br />

homogeneous solutions,<br />

C = W =<br />

∣ y ∣ ∣<br />

1 y 2<br />

∣∣∣ y 1 ′ y 2<br />

′ ∣ = t 2 1/t ∣∣∣<br />

2t −1/t 2 = −3 (24.50)<br />

Us<strong>in</strong>g y 1 = t 2 , y 2 = 1/t, f(t) = 2t, and a(t) = t 2 ,<br />

∫<br />

y P = −t 2 2t<br />

t · t 2 · −3 dt + 1 ∫<br />

t2 · 2t<br />

t t 2 dt (24.51)<br />

· −3<br />

∫<br />

= 2t2 t −2 dt − 2 ∫<br />

tdt (24.52)<br />

3<br />

3t<br />

= 2t2<br />

3 · −1 − 2 t 3t · t2 (24.53)<br />

2<br />

= − 2t<br />

3 − t = −t (24.54)<br />

3<br />

Hence y P = −t and therefore<br />

y = y H + y P = C 1 t 2 + C 2 t − 1 t<br />

(24.55)<br />

From the first <strong>in</strong>itial condition we have 0 = C 1 + C 2 − 1 or<br />

To use the second condition we need the derivative,<br />

C 1 + C 2 = 1. (24.56)<br />

y ′ = 2C 1 t − C 2<br />

t 2 − 1 (24.57)<br />

hence the second condition gives 1 = 2C 1 − C 2 − 1 or<br />

2C 1 − C 2 = 2. (24.58)<br />

Solv<strong>in</strong>g for C 1 and C 2 gives C 1 = 1, hence C 2 = 0, so that the complete<br />

solution of the <strong>in</strong>itial value problem is<br />

y = t 2 − 1 t<br />

(24.59)

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