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Lecture Notes in Differential Equations - Bruce E. Shapiro

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157<br />

For k = 0, 1, 2, . . . , n − 1 the right hand side produces unique results. But<br />

for k ≥ n, the results start to repeat: k = n gives the same angle as k = 0;<br />

k = n + 1 gives the same angle as k = 1; and so on. Hence there are<br />

precisely n unique numbers.<br />

Example 18.3. F<strong>in</strong>d the three cube roots of 27.<br />

To f<strong>in</strong>d the cube roots we repeat the proof!<br />

27 = 27 + (0)i = 27e (i)(0) = 27e (i)(0+2π) = 27e 2kπi (18.38)<br />

3√<br />

27 = 27 1/3 (e 2kπi ) 1/3 (18.39)<br />

= 3e 2kπi/3 (18.40)<br />

For k = 0 this gives<br />

3√<br />

27 = 3 (18.41)<br />

For k = 1 this gives<br />

3√<br />

27 = 3e 2πi/3 = 3<br />

For k = 2 this gives<br />

3√<br />

27 = 3e 4πi/3 = 3<br />

(<br />

cos 2π 3 + i s<strong>in</strong> 2π )<br />

= − 3 3 2 + i3√ 3<br />

2<br />

(<br />

cos 4π 3 + i s<strong>in</strong> 4π )<br />

= − 3 3 2 − i3√ 3<br />

2<br />

(18.42)<br />

(18.43)<br />

Us<strong>in</strong>g k = 3 will give us the first result, and so forth, so these are all the<br />

possible answers.<br />

Theorem 18.6. If the roots of<br />

ar 2 + br + c = 0 (18.44)<br />

are a complex conjugate pair<br />

}<br />

r 1 = µ + iω<br />

r 2 = µ − iω<br />

(18.45)<br />

where µ, ω ∈ R and ω ≠ 0, (this will occur when b 2 < 4ac), then the solution<br />

of the homogeneous second order l<strong>in</strong>ear ord<strong>in</strong>ary differential equation with<br />

constant coefficients<br />

Ly = ay ′′ + by ′ + cy = 0 (18.46)<br />

is given by<br />

y H = C 1 e r1t + C 2 e r2t (18.47)<br />

= e µt (A cos ωt + B s<strong>in</strong> ωt) (18.48)

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