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Lecture Notes in Differential Equations - Bruce E. Shapiro

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181<br />

The method of reduction of order is more generally valid then for equations<br />

with constant coefficient which we already know how to solve. It is usually<br />

more practical to repeat the derivation rather than us<strong>in</strong>g equation (21.14),<br />

which is difficult to memorize.<br />

Example 21.2. F<strong>in</strong>d a second solution to<br />

us<strong>in</strong>g the observation that y 1 = t is a solution.<br />

We look for a solution of the form<br />

Differentiat<strong>in</strong>g,<br />

y ′′ + ty ′ − y = 0 (21.21)<br />

y 2 = y 1 u = tu (21.22)<br />

Hence from (21.21)<br />

y 2 ′ = tu ′ + u (21.23)<br />

y 2 ′′ = tu ′′ + 2u ′ (21.24)<br />

tu ′′ + 2u ′ + t 2 u ′ + tu − tu = 0 (21.25)<br />

tu ′′ + 2u ′ + t 2 u ′ = 0 (21.26)<br />

tz ′ + (2 + t 2 )z = 0 (21.27)<br />

where z = u ′ . Rearrang<strong>in</strong>g and separat<strong>in</strong>g variables <strong>in</strong> z,<br />

∫ 1<br />

z<br />

1 dz + t2<br />

= −2 = − 2 z dt t t − t (21.28)<br />

∫ ∫<br />

dz 2<br />

dt dt = − t dt − tdt (21.29)<br />

ln z = −2 ln t − 1 2 t2 (21.30)<br />

z = 1 t 2 e−t2 /2<br />

(21.31)<br />

Therefore<br />

or<br />

du<br />

dt = 1 /2<br />

t 2 e−t2 (21.32)<br />

∫<br />

u(t) = t −2 e −t2 /2 dt (21.33)<br />

Thus a second solution is<br />

∫<br />

y 2 = tu = t<br />

t −2 e −t2 /2 dt (21.34)

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