Lecture Notes in Differential Equations - Bruce E. Shapiro

Lecture Notes in Differential Equations - Bruce E. Shapiro Lecture Notes in Differential Equations - Bruce E. Shapiro

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156 LESSON 18. COMPLEX ROOTS line from the origin to the point (x, y). Hence x cos θ = √ x2 + y = x 2 |z| y sin θ = √ x2 + y = y 2 |z| Therefore (18.27) (18.28) z = x + iy (18.29) ( x = |z| |z| + i y ) (18.30) |z| = |z|(cos θ + i sin θ) (18.31) = |z|e iθ (18.32) This form is called the polar form of the complex number. Roots of Polynomials 1. If z = x + iy is the root of a polynomial, then z = x − iy is also a root. 2. Every polynomial of order n has precisely n complex roots. 3. Every odd-ordered polynomial of order n has at least one real root: the number of real roots is either 1, or 3, or 5, ..., or n; the remaining roots are complex conjugate pairs. 4. An even-ordered polynomial of order n has either zero, or 2, or 4, or 6, or ... n real real roots; all of the remaining roots are complex conjugate pairs. Theorem 18.5. Every complex number z has precisely n unique n th roots. Proof. Write z in polar form. z = re iθ = re iθ+2kπ = re iθ e 2kπ , k = 0, 1, 2, . . . (18.33) where r and θ are real numbers. Take the n th root: n√ z = z 1/n = ( re iθ+2kπ) 1/n (18.34) (18.35) = r 1/n e i(θ+2kπ)/n (18.36) ( = n√ r cos θ + 2kπ + i sin θ + 2kπ ) (18.37) n n

157 For k = 0, 1, 2, . . . , n − 1 the right hand side produces unique results. But for k ≥ n, the results start to repeat: k = n gives the same angle as k = 0; k = n + 1 gives the same angle as k = 1; and so on. Hence there are precisely n unique numbers. Example 18.3. Find the three cube roots of 27. To find the cube roots we repeat the proof! 27 = 27 + (0)i = 27e (i)(0) = 27e (i)(0+2π) = 27e 2kπi (18.38) 3√ 27 = 27 1/3 (e 2kπi ) 1/3 (18.39) = 3e 2kπi/3 (18.40) For k = 0 this gives 3√ 27 = 3 (18.41) For k = 1 this gives 3√ 27 = 3e 2πi/3 = 3 For k = 2 this gives 3√ 27 = 3e 4πi/3 = 3 ( cos 2π 3 + i sin 2π ) = − 3 3 2 + i3√ 3 2 ( cos 4π 3 + i sin 4π ) = − 3 3 2 − i3√ 3 2 (18.42) (18.43) Using k = 3 will give us the first result, and so forth, so these are all the possible answers. Theorem 18.6. If the roots of ar 2 + br + c = 0 (18.44) are a complex conjugate pair } r 1 = µ + iω r 2 = µ − iω (18.45) where µ, ω ∈ R and ω ≠ 0, (this will occur when b 2 < 4ac), then the solution of the homogeneous second order linear ordinary differential equation with constant coefficients Ly = ay ′′ + by ′ + cy = 0 (18.46) is given by y H = C 1 e r1t + C 2 e r2t (18.47) = e µt (A cos ωt + B sin ωt) (18.48)

156 LESSON 18. COMPLEX ROOTS<br />

l<strong>in</strong>e from the orig<strong>in</strong> to the po<strong>in</strong>t (x, y). Hence<br />

x<br />

cos θ = √<br />

x2 + y = x<br />

2 |z|<br />

y<br />

s<strong>in</strong> θ = √<br />

x2 + y = y<br />

2 |z|<br />

Therefore<br />

(18.27)<br />

(18.28)<br />

z = x + iy (18.29)<br />

( x<br />

= |z|<br />

|z| + i y )<br />

(18.30)<br />

|z|<br />

= |z|(cos θ + i s<strong>in</strong> θ) (18.31)<br />

= |z|e iθ (18.32)<br />

This form is called the polar form of the complex number.<br />

Roots of Polynomials<br />

1. If z = x + iy is the root of a polynomial, then z = x − iy is also a<br />

root.<br />

2. Every polynomial of order n has precisely n complex roots.<br />

3. Every odd-ordered polynomial of order n has at least one real root:<br />

the number of real roots is either 1, or 3, or 5, ..., or n; the rema<strong>in</strong><strong>in</strong>g<br />

roots are complex conjugate pairs.<br />

4. An even-ordered polynomial of order n has either zero, or 2, or 4,<br />

or 6, or ... n real real roots; all of the rema<strong>in</strong><strong>in</strong>g roots are complex<br />

conjugate pairs.<br />

Theorem 18.5. Every complex number z has precisely n unique n th roots.<br />

Proof. Write z <strong>in</strong> polar form.<br />

z = re iθ = re iθ+2kπ = re iθ e 2kπ , k = 0, 1, 2, . . . (18.33)<br />

where r and θ are real numbers. Take the n th root:<br />

n√ z = z<br />

1/n<br />

= ( re iθ+2kπ) 1/n<br />

(18.34)<br />

(18.35)<br />

= r 1/n e i(θ+2kπ)/n (18.36)<br />

(<br />

= n√ r cos θ + 2kπ + i s<strong>in</strong> θ + 2kπ )<br />

(18.37)<br />

n<br />

n

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