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Lecture Notes in Differential Equations - Bruce E. Shapiro

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284 LESSON 30. THE METHOD OF FROBENIUS<br />

Example 30.1. Attempt to f<strong>in</strong>d a series solution for equation (30.5).<br />

Follow<strong>in</strong>g our usual procedure we let y = ∑ ∞<br />

0 c kt k , differentiate twice, and<br />

substitute the results <strong>in</strong>to the differential equation, lead<strong>in</strong>g to<br />

∑<br />

∞ ∞∑<br />

∞∑<br />

0 = t 2 c k k(k − 1)t k−2 + t c k kt k−1 + c k t k (30.7)<br />

k=0<br />

k=0<br />

k=0<br />

k=0<br />

k=0<br />

∞∑<br />

∞∑<br />

∞∑<br />

= c k k(k − 1)t k + c k kt k + c k t k (30.8)<br />

=<br />

=<br />

k=0<br />

∞∑<br />

c k (k(k − 1) + k + 1)t k (30.9)<br />

k=0<br />

∞∑<br />

c k (k 2 + 1)t k (30.10)<br />

k=0<br />

By l<strong>in</strong>ear <strong>in</strong>dependence,<br />

c k (k 2 + 1) = 0 (30.11)<br />

for all k. But s<strong>in</strong>ce k 2 + 1 is a positive <strong>in</strong>teger, this means c k = 0 for all<br />

values of k. Hence the only series solution is the trivial one, y = 0.<br />

Before one is tempted to conclude that there is no non-trivial solution to<br />

equation (30.5), consider the follow<strong>in</strong>g example.<br />

Example 30.2. Use the substitution x = ln t to f<strong>in</strong>d a solution to (30.5).<br />

By the cha<strong>in</strong> rule<br />

y ′ = dy<br />

dx<br />

Differentiat<strong>in</strong>g a second time,<br />

y ′′ = d ( 1<br />

dt t<br />

)<br />

dy<br />

dx<br />

= − 1 t 2 dy<br />

dx + 1 t<br />

=− 1 t 2 dy<br />

dx + 1 t<br />

dx<br />

dt = 1 dy<br />

t dx<br />

( )<br />

d dy<br />

dt dx<br />

( dy<br />

dx<br />

d<br />

dx<br />

) dx<br />

dt<br />

Substitut<strong>in</strong>g (30.12) and (30.16) <strong>in</strong>to (30.5) gives<br />

(30.12)<br />

(30.13)<br />

(30.14)<br />

(30.15)<br />

=− 1 t 2 dy<br />

dx + 1 t 2 d 2 y<br />

dx 2 (30.16)<br />

d 2 y<br />

dx 2 + y = 0 (30.17)

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