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Lecture Notes in Differential Equations - Bruce E. Shapiro

Lecture Notes in Differential Equations - Bruce E. Shapiro

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281<br />

Example 29.6. Solve t 2 y ′′ + ty ′ + y = 0. The <strong>in</strong>dicial equation is<br />

0 = r(r − 1) + r + 1 = r 2 + 1 =⇒ r = ±i (29.52)<br />

Thus the roots are a complex conjugate pair with real part λ = 0 and<br />

imag<strong>in</strong>ary part µ = 1. Hence the solution is<br />

y = At 0 cos(1 · ln t) + Bt 0 s<strong>in</strong>(1 · ln t) = A cos ln t + B s<strong>in</strong> ln t (29.53)<br />

Summary of Cauchy-Euler Equation<br />

To solve t 2 y ′′ + αty ′ + βy = 0 f<strong>in</strong>d the roots of<br />

r(r − 1) + αr + β = 0 (29.54)<br />

There are three possible case.<br />

1. If the roots are real and dist<strong>in</strong>ct, say r 1 ≠ r 2 , then the solution is<br />

y = C 1 t r1 + C 2 t r2 (29.55)<br />

2. If the roots are real and equal, say r = r 1 = r 2 , then the solution is<br />

y = C 1 t r + C 2 t r ln |t| (29.56)<br />

3. If the roots form a complex conjugate pair r = λ±iµ, where λ, µ ∈ R,<br />

then the solution is<br />

y = C 1 t λ cos(µ ln t) + C 2 t λ s<strong>in</strong>(µ ln t) (29.57)<br />

where, <strong>in</strong> each case, C 1 and C 2 are arbitrary constants (that may be<br />

determ<strong>in</strong>ed by <strong>in</strong>itial conditions).

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