A number of length 1 and its reciprocal
Take z with |z| = 1 and argument , so . By De Moivre’s theorem with n = −1, . The cosine of is and the sine of is , so .
So when |z| = 1, the reciprocal is the conjugate of z. Check by multiplying: .
Add them, subtract them
With |z| = 1, add z and : . The imaginary parts cancel. Subtract instead: . The real parts cancel.
So and , whenever |z| = 1.
For example, z = 0.6 + 0.8i has , with and . Then , , and .
z = 0.6 + 0.8i has length 1, and , dashed, is its mirror image in the real axis. Laid tip to tail, the 0.8 up and the 0.8 down cancel, and the sum lands on the real axis at .
Every power
With |z| = 1, De Moivre gives and . Adding and subtracting as before: and , for every whole number n.
For z = 0.6 + 0.8i: and , so . And .
A power of as multiple angles
With |z| = 1, , so . By the binomial theorem, .
Pair each power with its reciprocal: . The left side is , so , and .
Check at : , and .
This turns a power of into cosines of single angles, which is the form an integral of needs.
Sines the same way
With |z| = 1, . Cube it: .
The left side is . Dividing both sides by −8i: . Check at : , and .
Only when |z| = 1
Off the unit circle the identities fail. has |z| = 2. Its reciprocal is at −60°, which is , so , about 1.25 + 1.299i. That is not real, and not 2cos 60° = 1.
The reciprocal is the mirror image of z only when |z| = 1. Otherwise its length is 1/|z|, and the imaginary parts no longer cancel.
The usual mistakes
Changing both signs for . is −z, half a turn away; with |z| = 1, turns the angle back to , which changes only the sign of the imaginary part.
Giving for . That is the difference; adding cancels the imaginary parts and leaves .
Cubing the cosine instead of the angle. , not : De Moivre multiplies the angle.
Forgetting the 2. It is that equals , so is , not .
A middle coefficient of 1. The middle terms of are 3z and , so , not .
How much darker the corner of a photo is
The application below takes , so |z| = 1, and expands the fourth power with coefficients 1, 4, 6, 4, 1: , which is . Its angle is in radians: is 30°.
Worked example: How Much Darker the Corner of a Photo Is: The Cosine-Fourth Law Written in Multiple Angles
Question In a camera, light reaching the image at an angle θ to the axis of the lens is dimmed by the cosine-fourth law: its brightness is cos4θ times the brightness at the center. (a) Taking z = cosθ + i sinθ, show that cos4θ = 18(cos 4θ + 4cos 2θ + 3). (b) What fraction of the center's brightness reaches a point of the image at π6 to the axis? Work it from the formula in (a).
1.Adding zn = cos nθ + i sin nθ and 1zn = cos nθ − i sin nθ gives zn + 1zn = 2cos nθ; with n = 1, z + 1z = 2cosθ.
The brightness cos4θ falls from 1 on the axis. With z = cosθ + i sinθ, z + 1z = 2cosθ. 2.By the binomial theorem, (2cosθ)4 = (z + 1z)4 = z4 + 4z2 + 6 + 4z2 + 1z4.
The fourth power of z + 1z has binomial coefficients 1, 4, 6, 4, 1. 3.Pair each power with its reciprocal: (z4 + 1z4) + 4(z2 + 1z2) + 6 = 2cos 4θ + 8cos 2θ + 6.
Each power of z paired with its reciprocal is twice a cosine: zn + 1zn = 2cos nθ. 4.(a) So 16cos4θ = 2cos 4θ + 8cos 2θ + 6; dividing by 16, cos4θ = 18(cos 4θ + 4cos 2θ + 3).
(a) Dividing by 16: the green dots, worked from the new formula, lie on the curve of cos4θ. 5.(b) At θ = π6: 18(cos 2π3 + 4cos π3 + 3) = 18(−12 + 2 + 3) = 916, so 916 of the brightness, about 56%, reaches that point. Check: cos π6 = √32, and (√32)4 = 916.
(b) At π6 to the axis the image gets 916 of the brightness at the center.
Answer: (a) cos4θ = 18(cos 4θ + 4cos 2θ + 3); (b) 916 of the center's brightness
Common mistakes
- Writing cos4θ = (z + 1z)4 and forgetting the 2. It is 2cosθ that equals z + 1z, so the expansion gives 16cos4θ, and the division by 16 is what brings the 18.
- Taking the middle term of (z + 1z)4 as 4 instead of 6. The binomial coefficients for a fourth power are 1, 4, 6, 4, 1, and the middle term is 6z2 × 1z2 = 6.