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Lecture Notes in Differential Equations - Bruce E. Shapiro

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138 LESSON 16. LINEAR EQS. W/ CONST. COEFFICENTS<br />

When a root is repeated, the square root is zero, hence<br />

r = − b<br />

2a<br />

(16.33)<br />

Rearrang<strong>in</strong>g gives<br />

2ar + b = 0 (16.34)<br />

whenever r is a repeated root. Substitut<strong>in</strong>g equation (16.34) <strong>in</strong>to equation<br />

(16.31) gives L(te rt ) = 0.<br />

Example 16.3. We can use theorem (16.4) to f<strong>in</strong>d two solutions of the<br />

homogeneous l<strong>in</strong>ear differential equation<br />

The characteristic equation is<br />

y ′′ − 7y ′ + 12y = 0 (16.35)<br />

r 2 − 7r + 12 = 0 (16.36)<br />

Factor<strong>in</strong>g gives<br />

(r − 3)(r − 4) = 0 (16.37)<br />

S<strong>in</strong>ce the roots are r = 3 and r = 4, two solutions of the differential equation<br />

(16.35) are<br />

Thus for any real numbers A and B,<br />

is also a solution.<br />

y H1 = e 3t (16.38)<br />

y H2 = e 4t (16.39)<br />

y = Ae 3t + Be 4t (16.40)<br />

Because equation (16.14) <strong>in</strong>volves a second-order derivative the solution<br />

will <strong>in</strong> general <strong>in</strong>clude two constants of <strong>in</strong>tegration rather than the s<strong>in</strong>gle<br />

arbitrary constant that we had when we were solv<strong>in</strong>g first order equations.<br />

These <strong>in</strong>itial conditions are expressed as the values of both the function<br />

and its derivative at the same po<strong>in</strong>t, e.g.,<br />

}<br />

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

y ′ (t 0 ) = y 1<br />

(16.41)

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