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Lecture Notes in Differential Equations - Bruce E. Shapiro

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248 LESSON 27. HIGHER ORDER EQUATIONS<br />

where m<strong>in</strong>(m ij ) is the m<strong>in</strong>or of the ij th element. Differentiat<strong>in</strong>g,<br />

dM<br />

dt<br />

n+1<br />

∑<br />

n+1<br />

∑<br />

= (−1) 1+i m ′ 1i m<strong>in</strong>(m 1i ) + (−1) 1+i d<br />

m 1i<br />

dt m<strong>in</strong>(m 1i) (27.170)<br />

i=1<br />

i=1<br />

The first sum is d(M,1). S<strong>in</strong>ce (27.166) is true for any n × n matrix, we<br />

can apply it to m<strong>in</strong>(m 1i ) <strong>in</strong> the second sum.<br />

dM<br />

dt<br />

= d(M, 1) + ∑ n+1<br />

i=1 (−1)1+i m 1i<br />

∑ n<br />

j=1 d(m<strong>in</strong>(m 1i), j)<br />

(27.171)<br />

which completes the <strong>in</strong>ductive proof of the lemma.<br />

Proof. (Abel’s Formula)<br />

(n = 2). Suppose y 1 and y 2 are solutions of (27.165). Their Wronskian is<br />

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

W (t) = y 1 y ′ 2 − y 2 y ′ 1 (27.172)<br />

W ′ (x) = y 1 y ′′<br />

2 + y ′ 1y ′ 2 − y ′ 2y ′ 1 − y 2 y ′′<br />

1 = y 1 y ′′<br />

2 − y 2 y ′′<br />

1 (27.173)<br />

S<strong>in</strong>ce L 2 y 1 = L 2 y 2 = 0,<br />

Hence<br />

y ′′<br />

1 = −p(t)y ′ 1 − q(t)y 1 (27.174)<br />

y ′′<br />

2 = −p(t)y ′ 2 − q(t)y 2 (27.175)<br />

W ′ (t) = y 1 (−p(t)y 2 ′ − q(t)y 2 ) − y 2 (−p(t)y 1 ′ − q(t)y 1 )<br />

= −p(t)(y 1 y 2 ′ − y 2 y 1)<br />

′<br />

= −p(t)W (t)<br />

Rearrang<strong>in</strong>g and <strong>in</strong>tegrat<strong>in</strong>g gives W (t) = C exp [ − ∫ p(t)dt ] .<br />

General Case. The Wronskian is<br />

W [y 1 , ..., y n ](t) =<br />

∣<br />

y 1 · · · y n<br />

.<br />

.<br />

y (n−1)<br />

1 · · · y n<br />

(n−1) ∣<br />

(27.176)<br />

(27.177)

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