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Lecture Notes in Differential Equations - Bruce E. Shapiro

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141<br />

The general solution to<br />

is given by<br />

y =<br />

ay ′′ + by ′ + cy = 0 (16.60)<br />

{<br />

Ae r1t + Be r2t r 1 ≠ r 2 (dist<strong>in</strong>ct roots)<br />

(A + Bt)e rt r = r 1 = r 2 (repeated root)<br />

(16.61)<br />

where r 1 and r 2 are roots of the characteristic equation ar 2 + br + c = 0.<br />

Example 16.4. Solve the <strong>in</strong>itial value problem<br />

⎫<br />

y ′′ − 6y ′ + 8y = 0⎪⎬<br />

y(0) = 1<br />

⎪⎭<br />

y ′ (0) = 1<br />

(16.62)<br />

The characteristic equation is<br />

0 = r 2 − 6r + 8 = (r − 4)(r − 2) (16.63)<br />

The roots are r = 2 and r = 4, hence<br />

y = Ae 2t + Be 4t (16.64)<br />

From the first <strong>in</strong>itial condition,<br />

1 = A + B (16.65)<br />

Differentiat<strong>in</strong>g (16.64)<br />

y ′ = 2Ae 2t + 4Be 4t (16.66)<br />

From the second <strong>in</strong>itial condition<br />

1 = 2A + 4B (16.67)<br />

From (16.65), B = 1 − A, hence<br />

hence<br />

1 = 2A + 4(1 − A) = 4 − 2A =⇒ 2A = 3 =⇒ A = 3 2<br />

B = 1 − A = 1 − 3 2 = −1 2<br />

(16.68)<br />

(16.69)<br />

The solution to the IVP is<br />

y = 3 2 e2t − 1 2 e4t (16.70)

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