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Lecture Notes in Differential Equations - Bruce E. Shapiro

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209<br />

Example 24.3. Solve the <strong>in</strong>itial value problem<br />

⎫<br />

t 2 y ′′ − 2y = 2t⎪⎬<br />

y(1) = 0<br />

⎪⎭<br />

y ′ (1) = 1<br />

(24.41)<br />

given the observation that y = t 2 is a homogeneous solution.<br />

First, we f<strong>in</strong>d a second homogeneous solution us<strong>in</strong>g reduction of order. By<br />

Abel’s formula, s<strong>in</strong>ce there is no y ′ term, the Wronskian is a constant:<br />

W (t) = e − ∫ 0dt = C (24.42)<br />

A direct calculation of the Wronskian gives<br />

W (t) =<br />

∣ t2 y 2<br />

2t y 2<br />

′ ∣ = t2 y 2 ′ − 2ty 2 (24.43)<br />

Sett<strong>in</strong>g the two expressions for the Wronskian equal to one another gives<br />

t 2 y ′ − 2ty = C (24.44)<br />

where we have omitted the subscript. This is a first order l<strong>in</strong>ear equation<br />

<strong>in</strong> y;putt<strong>in</strong>g it <strong>in</strong>to standard form,<br />

y ′ − 2 t y = C t 2 (24.45)<br />

An <strong>in</strong>tegrat<strong>in</strong>g factor is µ = e ∫ (−2/t)dt = e −2 ln t = t −2 , hence<br />

Integrat<strong>in</strong>g both sides of the equation over t,<br />

Multiply<strong>in</strong>g through by t 2 ,<br />

d y<br />

dt t 2 = Ct−4 (24.46)<br />

y<br />

t 2 = −C 3 t−3 + C 1 (24.47)<br />

y = C 1 t 2 + C 2<br />

t<br />

(24.48)<br />

where C 2 = C/ − 3. S<strong>in</strong>ce y 1 = t 2 , we conclude that y 2 = 1/t. This gives<br />

us the entire homogeneous solution.

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