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Lecture Notes in Differential Equations - Bruce E. Shapiro

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235<br />

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

− 2K |t − t 0 | ≤ ln |u(t)/u(t 0 )| ≤ 2K |t − t 0 | (27.59)<br />

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

|u 0 (t)| e −2K|t−t0| ≤ |u(t)| ≤ |u 0 (t)| e 2K|t−t0| (27.60)<br />

By equation (27.39) this last statement is equivalent to the desired result,<br />

which is the fundamental <strong>in</strong>equality.<br />

Proof. (Theorem 27.3) By the previous theorem, each term <strong>in</strong> the sum is a<br />

solution of L n y = 0, and hence by the superposition pr<strong>in</strong>ciple, (27.23) is a<br />

solution.<br />

To prove that it is the general solution we must show that every solution<br />

of L n y = 0 has the form (27.23).<br />

Suppose that u(t) is a solution that does not have the form given by (27.23),<br />

i.e., it is not a l<strong>in</strong>ear comb<strong>in</strong>ation of the y ij = e rit t j .<br />

Renumber the y ij to have a s<strong>in</strong>gle <strong>in</strong>dex y 1 , ..., y n , and let u 0 = u(t 0 ), u 1 =<br />

u ′ (t 0 ), ..., u n−1 = u (n−1) (t o ). Then u(t) is a solution of some <strong>in</strong>itial value<br />

problem<br />

L n y = 0, y(t 0 ) = u 0 , y ′ (t 0 ) = u 1 , ..., y (n−1) (t 0 ) = u n−1 (27.61)<br />

and by uniqueness it must be the only solution of (27.61). Let<br />

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

v = c 1 y 1 + c 2 y 2 + · · · + c n y n (27.62)<br />

v ′ = c 1 y ′ 1 + c 2 y ′ 2 + · · · + c n y ′ n (27.63)<br />

We ask whether there is a solution c 1 , c 2 , ..., c n to the system<br />

v(t 0 ) = c 1 y 1 (t 0 ) + c 2 y 2 (t 0 ) + · · · + c n y n (t 0 ) = u 0 (27.64)<br />

If the matrix<br />

⎛<br />

M = ⎜<br />

⎝<br />

⎞<br />

y 1 (t 0 ) y 2 (t 0 ) · · · y n (t 0 )<br />

y 1(t ′ 0 ) y 2(t ′ 0 ) y n(t ′ 0 )<br />

.<br />

.<br />

.. ⎟ . ⎠<br />

y (n−1)<br />

1 (t 0 ) y (n−1)<br />

2 (t 0 ) y n (n−1) (t 0 )<br />

(27.65)

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