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Lecture Notes in Differential Equations - Bruce E. Shapiro

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Lesson 20<br />

The Wronskian<br />

We have seen that the sum of any two solutions y 1 , y 2 to<br />

ay ′′ + by ′ + cy = 0 (20.1)<br />

is also a solution, so a natural question becomes the follow<strong>in</strong>g: how many<br />

different solutions do we need to f<strong>in</strong>d to be certa<strong>in</strong> that we have a general<br />

solution? The answer is that every solution of (20.1) is a l<strong>in</strong>ear comb<strong>in</strong>ation<br />

of two l<strong>in</strong>ear <strong>in</strong>dependent solutions. In other words, if y 1<br />

and y 2 are l<strong>in</strong>early <strong>in</strong>dependent (see def<strong>in</strong>ition (15.6)), i.e, there is no<br />

possible comb<strong>in</strong>ation of constants A and B, both nonzero, such that<br />

Ay 1 (t) + By 2 (t) = 0 (20.2)<br />

for all t, and if both y 1 and y 2 are solutions, then every solution of (20.1)<br />

has the form<br />

y = C 1 y 1 (t) + C 2 y 2 (t) (20.3)<br />

We beg<strong>in</strong> by consider<strong>in</strong>g the <strong>in</strong>itial value problem 1<br />

⎫<br />

y ′′ + p(t)y ′ + q(t)y = 0 ⎪⎬<br />

y(t 0 ) = y 0<br />

⎪⎭<br />

y ′ (t 0 ) = y 0<br />

′<br />

(20.4)<br />

Suppose that y 1 (t) and y 2 (t) are both solutions of the homogeneous equation;<br />

then<br />

y(t) = Ay 1 (t) + By 2 (t) (20.5)<br />

1 Eq. (20.1) can be put <strong>in</strong> the same form as (20.4) so long as a ≠ 0, by sett<strong>in</strong>g<br />

p(t) = b/a and q(t) = c/a. However, (20.4) is considerably more general because we are<br />

not requir<strong>in</strong>g the coefficients to be constants.<br />

171

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