1.5  The Unit Circle and Polar Form

Addition in C is addition of arrows in the plane: (a,b)+(c,d)=(a+c,b+d) puts the second arrow at the tip of the first. Multiplication has a picture too, and Section 1.2 already holds half of it: the modulus of a product is the product of the moduli (Theorem 1.2.2 (d)). The other half is about angles, and angles need the functions cosine and sine, which this volume does not construct. This section first proves everything about directions that needs no angle at all, then states exactly five facts about cosine and sine that it borrows, and from those five builds the polar form of a complex number and the rule “multiply the lengths, add the angles”.

1.5.1. Length and direction

Every non-zero complex number should be a length times a direction. The length is the modulus. The directions are the complex numbers of length 1, and they deserve a name.

The unit circle is the set of complex numbers at distance 1 from 0.

We write T:={u∈C:|u|=1} for the unit circle. For u=x+yi with x,y∈R, the condition |u|=1 says x2+y2=1, that is, x2+y2=1: both sides of the first equation are non-negative, so it holds exactly when the squares agree (Number Systems: From N to R, Proposition 2.3.5 (g)). So T is the circle of radius 1 about 0 in the plane. It contains 1, −1, i and −i, and also 35+45i, since 925+1625=1. It does not contain 1+i, whose modulus is 2≠1.

The next proposition collects what the multiplication of C does on T. None of it uses an angle.

Proposition 1.5.1 (The Unit Circle)
  • (a) 1∈T. If u,v∈T, then uv∈T. If u∈T, then u≠0 and u−1=u―∈T.
  • (b) For every z∈C with z≠0 there is exactly one pair (r,u) with r∈R, r>0, u∈T and z=ru, namely r=|z| and u=z/|z|.
  • (c) For z∈C with z≠0: 1/z=z― if and only if |z|=1.

Idea. Every part is a statement about moduli, so each follows from the rules of Section 1.2: moduli multiply, uu―=|u|2, and only 0 has modulus 0. For (b), divide z by its length; for the uniqueness, take moduli of z=ru.

Proof.

Part (b) is the picture we wanted: z=|z|⋅u, a length times a direction, and both factors are forced. Part (a) says that the directions are closed under multiplication and inversion and contain 1; Algebraic Preliminaries, Chapter 2 calls a set with these properties, under an associative product, a group, and T is one of its first examples. Part (c) is a practical test: on the unit circle, and only there, dividing by z is the same as conjugating.

Quick check. Write z=3+4i as ru with r>0 and u∈T. What is 1/u?

Solution. By Proposition 1.5.1 (b), r=|3+4i|=5 and u=35+45i. By (a), 1/u=u―=35−45i. Check: (35+45i)(35−45i)=925+1625=1.

So far a direction is a point u of T, and multiplying two directions gives a third. What we cannot yet say is how much a direction turns the plane. For that we need to measure positions on the circle by a real number, an angle, so that multiplying directions adds angles. That is a job for cosine and sine.

1.5.2. What this volume borrows about cosine and sine

An angle should be a real number θ that walks around the circle: a point (cos⁡θ,sin⁡θ) on T, moving as θ moves, returning to its start after a full turn of length 2π. Defining such functions needs limits of functions, by power series or by integrals. This volume develops no limits of functions, so it does not define cosine and sine. Analysis on the Real Line, Chapter 10 does: there cos and sin are defined by power series, π is defined as twice the least positive zero of cos, and the facts below are proved. Its R is a complete ordered field, so by Number Systems: From N to R, Theorem 6.3.1 it is our R, up to the one order-preserving field isomorphism; the functions and the number carry over along it.

We write 2πZ:={2πk:k∈Z}, the integer multiples of 2π in R.

Axiom 1.5.2 (What This Volume Borrows about Cosine and Sine)

There are functions cos,sin:R→R and a real number π>0 with the following properties. They are assumed here and proved in Analysis on the Real Line, Chapter 10.

  • (T1) cos2⁡θ+sin2⁡θ=1 for every θ∈R.
  • (T2) For all θ,φ∈R, cos⁡(θ+φ)=cos⁡θcos⁡φ−sin⁡θsin⁡φ,sin⁡(θ+φ)=sin⁡θcos⁡φ+cos⁡θsin⁡φ.
  • (T3) For θ∈R: cos⁡θ=1 if and only if θ∈2πZ.
  • (T4) For every (x,y)∈R2 with x2+y2=1 there is θ∈R with cos⁡θ=x and sin⁡θ=y.
  • (T5) sin⁡θ>0 whenever 0<θ<π.

In words: (T1) puts the point (cos⁡θ,sin⁡θ) on the unit circle; (T2) is the pair of addition formulas; (T3) says that the cosine reaches 1 exactly at the multiples of a full turn; (T4) says that every point of the circle is reached; (T5) says that during the first half turn the point stays in the upper half plane.

This box is where the chapter borrows. Like Logic and Proof, Axiom 4.2.1, which Logic and Proof assumed and Number Systems: From N to R, Chapter 1 proved, it is a statement assumed in one volume and proved in another. Nothing in Sections 1.1–1.4, and nothing in this section above the box, uses it. From here on we use these five facts about cos, sin and π and no others: no value such as cos⁡(π/3)=12, no periodicity, no picture of a graph. Whatever else we need, we derive, and each proof that uses one of the facts names it by its number. Two consequences come at once.

  • cos⁡0=1, by (T3), since 0=2π⋅0∈2πZ. Then (T1) gives sin2⁡0=1−1=0, so sin⁡0=0, because a non-zero real number has a positive square (Number Systems: From N to R, Proposition 2.3.5 (e)).
  • cos⁡(2πk)=1 and sin⁡(2πk)=0 for every k∈Z, by (T3) and then (T1) in the same way.

Warning. The five facts are about cos, sin and π only. A school fact such as sin⁡(π/6)=12 is not among them, and a proof in this volume may not quote it: Example (Special Angles) below derives the few values we use. Nor do the facts say that cos and sin are “periodic with period 2π” as functions; that is true, and derivable from (T2) and (T3), but no proof here needs it.

1.5.3. Polar form

With angles available, we can name the point of T at angle θ.

eiθ is the point of the unit circle at angle θ.

Definition 1.5.1 (Polar Form)

For θ∈R we write eiθ:=cos⁡θ+isin⁡θ. Let z∈C with z≠0. A polar form of z is an expression z=reiθ with r∈R, r>0, and θ∈R. Then θ is an argument of z.

In words: the first line is an abbreviation, not an exponential. This volume has no exponential function, the letter e on its own means nothing here, and the only rule of exponents we will use for eiθ is the one proved below (Theorem 1.5.3 (a)). Analysis on the Real Line, Chapter 10 shows that eiθ is indeed the value of the complex exponential function at iθ; the notation anticipates that, and the linear algebra volumes write their roots of unity with it. The exponent may be written in any form equal to iθ with θ real, and the symbol then means eiθ: for example e−iθ=ei(−θ), e2πi=ei⋅2π, einθ=ei(nθ) and e−2πi=ei(−2π). This is unambiguous, because the real number θ is determined by iθ (it is its imaginary part). The second part asks for a positive real r and allows any real θ.

The point eiθ lies on T. Indeed |eiθ|=cos2⁡θ+sin2⁡θ=1=1, by Definition 1.2.1 and (T1). So reiθ is a length r times a direction, as in Proposition 1.5.1 (b), and that proposition gives r=|z| for every polar form of z.

Examples.

  • ei0=cos⁡0+isin⁡0=1, by the consequences of the box. So 1=1⋅ei0 and 5=5ei0 are polar forms.
  • e2πi=cos⁡2π+isin⁡2π=1, by the second consequence with k=1. So 1=1⋅e2πi as well: 0 and 2π are both arguments of 1, and they differ, since π>0.
  • The number 0 has no polar form, since |reiθ|=r>0.

A non-example by minimal change. Allow r<0: then −1=(−1)⋅ei0 looks like a polar form of −1 with argument 0. The clause that fails is r>0, and it matters: with negative r allowed, the length could no longer be read off as |z|, and 1=1⋅ei0 and −1=(−1)ei0 would share the argument 0. We will see in Example (Special Angles) that −1=1⋅eiπ is a genuine polar form.

The examples already show why the definition says an argument: 1=ei0=e2πi. How much freedom there is, exactly, is part (b) of Proposition 1.5.4 below. First, the reason for the notation: these numbers multiply the way exponentials do.

Theorem 1.5.3 (Multiplication in Polar Form)
  • (a) eiθeiφ=ei(θ+φ) for all θ,φ∈R.
  • (b) ei0=1, and (eiθ)−1=e−iθ=eiθ― for every θ∈R.
  • (c) If r,s∈R with r,s>0 and θ,φ∈R, then (reiθ)(seiφ)=rsei(θ+φ), and this is a polar form of the product.

Idea. Multiply out (cos⁡θ+isin⁡θ)(cos⁡φ+isin⁡φ) with the rule of Definition 1.1.1: the real and imaginary parts that appear are exactly the right-hand sides of the addition formulas (T2). The rest is bookkeeping with inverses and moduli.

Proof.

  • (a) By the multiplication rule of Definition 1.1.1, eiθeiφ=(cos⁡θcos⁡φ−sin⁡θsin⁡φ)+(cos⁡θsin⁡φ+sin⁡θcos⁡φ)i=cos⁡(θ+φ)+isin⁡(θ+φ), where the second equality is (T2), with the two products in the imaginary part reordered by commutativity in R. The right-hand side is ei(θ+φ).

  • (b) ei0=1 was shown in the first example above. By (a) with φ=−θ, eiθe−iθ=ei0=1, so e−iθ is the inverse of eiθ, by uniqueness of inverses in the field C (Theorem 1.2.4, Number Systems: From N to R, Lemma 4.1.1 (a)). Since eiθ∈T, its inverse is also its conjugate (Proposition 1.5.1 (a)).

  • (c) By Proposition 1.1.2 (commutativity and associativity of ⋅), (reiθ)(seiφ)=(rs)(eiθeiφ), and (a) turns this into rsei(θ+φ). Here rs>0 by Number Systems: From N to R, Proposition 2.3.5 (c) (multiply 0<r by s>0), so this is a polar form.

In words: to multiply two complex numbers, multiply their moduli and add their arguments. This is the chapter’s third named move, multiply moduli, add angles. Multiplying by a fixed w=seiφ therefore turns the plane about 0 by the angle φ and stretches it by the factor s. The picture shows z, w and zw for |z|=1.5, |w|=1.2, and arguments of 20∘ and 50∘ (a full turn being 360∘, that is, 2π).

Diagram. Labels: operatorname Re, operatorname Im, z, w, zw, small 20^circ, small 50^circ, small 1

The arrow for zw has length 1.5×1.2=1.8 and makes the angle 20∘+50∘=70∘ with the positive real axis: it is the arrow for z, turned by the argument of w and stretched by the modulus of w. The small arc marks the argument of z, the large arc the extra turn by the argument of w, and the dashed arc is part of the unit circle, where the numbers eiθ live.

Now the freedom in the argument. Every non-zero number has a polar form, and its arguments are determined up to a whole number of full turns.

Proposition 1.5.4 (Existence and Uniqueness of Polar Form)
  • (a) Every z∈C with z≠0 has a polar form, and every polar form z=reiθ has r=|z|.
  • (b) For r,s∈R with r,s>0 and θ,φ∈R, reiθ=seiφ⟺r=s and θ−φ∈2πZ.

Proof.

  • (a) By Proposition 1.5.1 (b), z=|z|⋅u with u=x+yi∈T, so x2+y2=1. By (T4) there is θ∈R with cos⁡θ=x and sin⁡θ=y, that is, u=eiθ. Hence z=|z|eiθ, with |z|>0. Conversely, if z=reiθ is a polar form, then eiθ∈T, and the uniqueness in Proposition 1.5.1 (b) gives r=|z|.

  • (b) Suppose first that reiθ=seiφ. The number reiθ is non-zero: r≠0, eiθ∈T is non-zero (Proposition 1.5.1 (a)), and a product of non-zero elements of the field C is non-zero (Theorem 1.2.4, Number Systems: From N to R, Lemma 4.1.1 (d)). So both sides are polar forms of the same non-zero number, and r=s by (a). Multiplying by r−1 gives eiθ=eiφ. In the other direction, if r=s, the two sides are equal exactly when eiθ=eiφ. So it remains to show that eiθ=eiφ if and only if θ−φ∈2πZ.

Multiplying by e−iφ, and back by eiφ, shows that eiθ=eiφ holds if and only if eiθe−iφ=eiφe−iφ, that is, by Theorem 1.5.3 (a) and (b), if and only if ei(θ−φ)=1. Comparing real and imaginary parts, this says cos⁡(θ−φ)=1 and sin⁡(θ−φ)=0. The second condition follows from the first: by (T1), cos⁡(θ−φ)=1 gives sin2⁡(θ−φ)=0, hence sin⁡(θ−φ)=0 (Number Systems: From N to R, Proposition 2.3.5 (e)). So eiθ=eiφ if and only if cos⁡(θ−φ)=1, and by (T3) that holds if and only if θ−φ∈2πZ.

Existence came from (T4), and uniqueness from (T3), with (T1) helping and (T2) entering through Theorem 1.5.3. “Comparing arguments” therefore always means comparing them up to a multiple of 2π, and the next warning is the trap this sets.

Warning. From eiθ=eiφ one may not conclude θ=φ: ei0=e2πi=1, and 0≠2π. Only θ−φ∈2πZ follows (Proposition 1.5.4 (b)). Forgetting this loses solutions as soon as an equation is solved for an angle; Section 1.6 meets an equation where it would lose all but one of them.

1.5.4. Powers

Repeating Theorem 1.5.3 gives powers. The powers zn are those of the recursion z0=1, zn+1=znz (Proposition 1.1.3).

Theorem 1.5.5 (De Moivre’s Formula)

For every θ∈R and every n∈N, (eiθ)n=einθ,that is,(cos⁡θ+isin⁡θ)n=cos⁡nθ+isin⁡nθ. Consequently (reiθ)n=rneinθ for every real r>0, and this is a polar form.

Idea. A power is a repeated product, and each new factor eiθ adds θ to the argument, by Theorem 1.5.3 (a). So induction on n, along the recursion zn+1=znz.

Proof. We use Logic and Proof, Axiom 4.2.1 on n, read on N=ω through Number Systems: From N to R, Corollary 1.7.3 (b); here nθ is the product in R of n⋅1R and θ (Number Systems: From N to R, Definition 4.2.1 (a)). For n=0, the left side is (eiθ)0=1 by the recursion, and the right side is ei0=1 by Theorem 1.5.3 (b). Suppose (eiθ)n=einθ for some n∈N. Then (eiθ)n+1=(eiθ)neiθ=einθeiθ=ei(nθ+θ)=ei(n+1)θ, by the recursion, the induction hypothesis, Theorem 1.5.3 (a), and (n+1)⋅1R=n⋅1R+1R (Number Systems: From N to R, Definition 4.2.1 (a)) with distributivity in R. This proves the formula for every n∈N.

For the consequence, Proposition 1.1.3 (c) gives (reiθ)n=rn(eiθ)n=rneinθ. The power rn is the same whether it is computed in R or in C, by the remark after Proposition 1.1.3 in Section 1.1, and rn>0 because a product of positive reals is positive (Number Systems: From N to R, Proposition 2.3.5 (c); induction on n, with r0=1>0).

For a negative exponent, Exercise C1 below defines z−n locally and proves the matching formula; nothing in the text uses it.

The five borrowed facts give no particular value of cos or sin except at multiples of 2π. Every other value this chapter uses is derived next, from (T1)–(T5) and the algebra of Sections 1.1–1.4.

Example (Special Angles)

Show, using only (T1)–(T5) and the results proved so far, that eiπ=−1,eiπ/2=i,eiπ/3=12+32i,eiπ/6=32+12i,eiπ/4=12+12i.

Solution. Each value is found the same way: a power of the unknown point is a point we already know, and (T5) chooses between the candidates. Since π>0, each of π/2, π/3, π/4, π/6 lies strictly between 0 and π, so (T5) gives Imeiθ=sin⁡θ>0 for each of them.

  • (i) eiπ=−1. Let u:=eiπ. By Theorem 1.5.5, u2=e2πi=1, so (u−1)(u+1)=u2−1=0, and since C has no zero divisors (Theorem 1.2.4, Number Systems: From N to R, Lemma 4.1.1 (d)), u=1 or u=−1. Suppose u=1. Then cos⁡π=1, so π=2πk for some k∈Z by (T3); dividing by π≠0 gives 1=2k in R, an equation between images of integers. The embedding of Z into R, through Q (Number Systems: From N to R, Proposition 2.4.4) and κ (Number Systems: From N to R, Theorem 5.6.3), is injective and preserves + and ⋅, so 1=2k holds in Z. But 1=2⋅0+1 is odd, and an odd integer is not of the form 2k (Number Systems: From N to R, Corollary 3.1.3 (a)). So u≠1, and eiπ=−1.

  • (ii) eiπ/2=i. Let u:=eiπ/2. By Theorem 1.5.3 (a), u2=eiπ=−1=i2, so (u−i)(u+i)=0 and u=±i. Since Imu>0 and Im(−i)=−1<0, u=i.

  • (iii) eiπ/3=12+32i. Let u:=eiπ/3. By Theorem 1.5.5, u3=eiπ=−1. Multiplying out shows (u+1)(u2−u+1)=u3+1=0. Now u≠−1, since Imu>0; so u2−u+1=0. By Corollary 1.4.2 with a=1, b=−1, c=1, and d:=3i, a square root of b2−4ac=−3 (indeed (3i)2=3i2=−3), u=1+3i2oru=1−3i2. Since Imu>0, u=12+32i.

  • (iv) eiπ/6=32+12i. Since π/6=π/2+(−π/3), Theorem 1.5.3 (a) and (b) give eiπ/6=eiπ/2e−iπ/3=i⋅eiπ/3―=i(12−32i)=32+12i, by (ii) and (iii).

  • (v) eiπ/4=12+12i. Let u:=eiπ/4. By Theorem 1.5.3 (a) and (ii), u2=eiπ/2=i. The formula of Proposition 1.4.1 for z=i (so a=0, b=1, r=|i|=1) gives the square root w=1/2+1/2i, and 1/2=1/2, since both are non-negative and square to 12. By Proposition 1.4.1 (b), u=w or u=−w, and Imu>0 rules out −w. So u=w.

Comparing real and imaginary parts turns these into values of cos and sin:

θ 0 π/6 π/4 π/3 π/2 π
cos⁡θ 1 3/2 1/2 1/2 0 −1
sin⁡θ 0 1/2 1/2 3/2 1 0

These are the familiar values, now proved from the five facts.

Two special cases of the rotation picture are worth isolating. Multiplying by i=eiπ/2 turns the plane by a quarter turn, counterclockwise; two quarter turns make a half turn, and this is the picture behind i2=−1=eiπ. And multiplying by e−iθ=eiθ― undoes the turn by θ (Theorem 1.5.3 (b)).

Powers that are tedious to expand become one line in polar form.

Example (A Power via Polar Form)

Compute (3+i)6.

Solution. We have 3+i=2(32+12i)=2eiπ/6, by Example (Special Angles) (iv). By Theorem 1.5.5 and Example (Special Angles) (i), (3+i)6=26ei⋅6π/6=64eiπ=−64. By hand: (3+i)2=3+23i−1=2+23i=2(1+3i), and (1+3i)3=(1+3i)(−2+23i)=−2−6=−8, so (3+i)6=(2(1+3i))3=8⋅(−8)=−64 (Proposition 1.1.3 (b), (c)), the same answer.

Quick check. Use polar form to compute (1+i)8, and check the answer with (1+i)2=2i.

Solution. By Example (Special Angles) (v), 1+i=2(12+12i)=2eiπ/4. By Theorem 1.5.5, (1+i)8=(2)8ei⋅8π/4=16e2πi=16, since (2)8=((2)2)4=24=16 and e2πi=1. Check: (1+i)8=((1+i)2)4=(2i)4=16i4=16, by Proposition 1.1.3 (b), (c).

1.5.5. Exercises

A. Check your understanding

Exercise (A1)
  • (a) Give a polar form of −2 and of 3i.
  • (b) True or false: if eiθ=eiφ, then θ=φ. Justify your answer.
  • (c) In Proposition 1.5.4, which of the borrowed facts (T1)–(T5) gives the existence of a polar form, and which gives the uniqueness of the argument up to 2πZ?
  • (d) Which results of Sections 1.1–1.5 use none of the borrowed facts? Is Proposition 1.5.1 among them?

Solution.

  • (a) −2=2eiπ and 3i=3eiπ/2, by Example (Special Angles) (i) and (ii); the moduli 2 and 3 are positive, as a polar form requires. (Any π+2πk, respectively π/2+2πk, with k∈Z, is also an argument, by Proposition 1.5.4 (b).)

  • (b) False. ei0=1=e2πi, but 0≠2π since π>0. What is true is θ−φ∈2πZ (Proposition 1.5.4 (b)).

  • (c) Existence: (T4), which provides an angle for the point z/|z| of T. Uniqueness: (T3), which turns cos⁡(θ−φ)=1 into θ−φ∈2πZ; (T1) is used alongside it, to see that sin⁡(θ−φ)=0 follows from cos⁡(θ−φ)=1, and (T2) enters through Theorem 1.5.3, which turns eiθ=eiφ into ei(θ−φ)=1.

  • (d) Everything in Sections 1.1–1.4, and the part of this section before Axiom 1.5.2; after the box, only Exercise C2, which is set up to avoid them. In particular Proposition 1.5.1 uses none of them: its proof uses only the modulus rules of Section 1.2, the field properties of C, and order facts about R from Number Systems: From N to R.

B. Practice

Exercise (B1)

Compute (1−3i)6.

Solution. We have 1−3i=2(12−32i)=2eiπ/3―=2e−iπ/3, by Example (Special Angles) (iii) and Theorem 1.5.3 (b). By Theorem 1.5.5, (1−3i)6=26e−6iπ/3=64e−2πi=64, since −2π=2π⋅(−1)∈2πZ, so cos⁡(−2π)=1 and sin⁡(−2π)=0 by (T3) and (T1), and e−2πi=1.

Exercise (B2: Symmetries of Cosine and Sine)

Prove that for every θ∈R: cos⁡(−θ)=cos⁡θ,sin⁡(−θ)=−sin⁡θ,cos⁡(θ+π)=−cos⁡θ,sin⁡(θ+π)=−sin⁡θ,cos⁡θ=sin⁡(θ+π/2).

Hint: write each left side as a part of some eiψ, and compute that eiψ with Theorem 1.5.3.

Solution. By Theorem 1.5.3 (b), e−iθ=eiθ―, that is, cos⁡(−θ)+isin⁡(−θ)=cos⁡θ−isin⁡θ. Comparing real and imaginary parts gives cos⁡(−θ)=cos⁡θ and sin⁡(−θ)=−sin⁡θ.

By Theorem 1.5.3 (a) and Example (Special Angles) (i), ei(θ+π)=eiθeiπ=−eiθ, that is, cos⁡(θ+π)+isin⁡(θ+π)=−cos⁡θ−isin⁡θ. Comparing parts gives the next two identities.

By Theorem 1.5.3 (a) and Example (Special Angles) (ii), ei(θ+π/2)=ieiθ=icos⁡θ−sin⁡θ. Comparing imaginary parts gives sin⁡(θ+π/2)=cos⁡θ. (Comparing real parts gives, in addition, cos⁡(θ+π/2)=−sin⁡θ.)

Exercise (B3)

Let θ∈R. Show that |eiθ−1|2=2−2cos⁡θ. Hence show again that eiθ=1 if and only if cos⁡θ=1.

Solution. Let u:=eiθ, so uu―=|u|2=1. Squaring the modulus, by Theorem 1.2.2 (a)–(c), |u−1|2=(u−1)(u−1)―=(u−1)(u―−1)=uu―−(u+u―)+1=2−2Reu, and Reu=cos⁡θ. Hence |u−1|2=2−2cos⁡θ.

Now u=1 if and only if |u−1|=0 (Theorem 1.2.2 (e)), if and only if |u−1|2=0 (a real number is 0 exactly when its square is: 02=0 by Number Systems: From N to R, Proposition 2.3.2 (b), and a non-zero square is positive by Number Systems: From N to R, Proposition 2.3.5 (e)), if and only if 2−2cos⁡θ=0, that is, cos⁡θ=1.

C. Going deeper

Exercise (C1: Triple Angles and Negative Powers)
  • (a) Prove that cos⁡3θ=4cos3⁡θ−3cos⁡θ and sin⁡3θ=3sin⁡θ−4sin3⁡θ for every θ∈R.
  • (b) For z∈C with z≠0 and n∈N, put z−n:=(z−1)n (a definition local to this exercise). Show that (eiθ)−n=e−inθ.

Solution.

  • (a) Write c:=cos⁡θ and s:=sin⁡θ. By Theorem 1.5.5, cos⁡3θ+isin⁡3θ=(c+is)3. Now (c+is)2=(c2−s2)+2csi, and (c+is)3=((c2−s2)+2csi)(c+is)=(c3−3cs2)+(3c2s−s3)i. Comparing real parts and using s2=1−c2 (T1), cos⁡3θ=c3−3c(1−c2)=4c3−3c. Comparing imaginary parts and using c2=1−s2, sin⁡3θ=3(1−s2)s−s3=3s−4s3.

  • (b) By Theorem 1.5.3 (b), (eiθ)−1=e−iθ=ei(−θ). By Theorem 1.5.5 applied to −θ, (eiθ)−n=(ei(−θ))n=ein(−θ)=e−inθ.

Nothing in this chapter uses negative powers of complex numbers; the definition in (b) is for practice only.

Exercise (C2: Points on the Circle without Angles)

For t∈R put ut:=1+it1−it.

  • (a) Show that ut is defined, that ut∈T, and that ut≠−1.
  • (b) Show that every u∈T with u≠−1 equals ut for exactly one t∈R, namely t=Imu/(1+Reu).
  • (c) Compute u1/2 in the form a+bi.

Use none of the borrowed facts (T1)–(T5).

Solution (Hint 1). For (b), on the unit circle the conjugate is the inverse: u―=1/u.

Solution (Hint 2). Clearing the denominator, u=ut is equivalent to u−1=it(u+1), and u+1≠0, so t is determined; it remains to show that (u−1)/(i(u+1)) is real.

Solution.

  • (a) The real part of 1−it is 1, so 1−it≠0 and the quotient is defined. The numbers 1+it and 1−it are conjugate, so they have the same modulus (Theorem 1.2.2 (d)), which is non-zero. From ut(1−it)=1+it and Theorem 1.2.2 (d), |ut||1−it|=|1+it|=|1−it|, and canceling the non-zero real number |1−it| gives |ut|=1. If ut=−1, then 1+it=−(1−it)=−1+it, so 1=−1, which is false. So ut≠−1.

  • (b) Let u∈T with u≠−1, and let t∈R. Since 1−it≠0, the equation u=ut is equivalent to u(1−it)=1+it, that is, to u−1=it(u+1). Since i(u+1)≠0, this holds if and only if t=t0, where t0:=(u−1)/(i(u+1))∈C. So at most one real t has ut=u, and one does exactly when t0 is real. Using uu―=1, (u−1)(u―+1)=uu―+u−u―−1=u−u―=2iImu, where u−u―=2iImu by Definition 1.2.1 (with u=a+bi, (a+bi)−(a−bi)=2bi); and (u+1)(u―+1)=|u+1|2=2+2Reu, by Theorem 1.2.2 (a), (c). This is a positive real number, since u+1≠0. Multiplying numerator and denominator of (u−1)/(u+1) by u―+1=u+1―≠0, t0=1i⋅2iImu2+2Reu=Imu1+Reu, a real number. So exactly one t∈R has ut=u, namely t0.

  • (c) Multiplying numerator and denominator by the conjugate 1+12i of the denominator, u1/2=(1+12i)21+14=34+i54=35+45i. Check against (b): Imu/(1+Reu)=45/85=12.

So the map t↦ut is a bijection from R onto T∖{−1}, and it was found with no angle. For rational t, the point ut has rational coordinates: the computation in (c) with t in place of 12 gives ut=((1−t2)+2ti)/(1+t2), and t=1/2 gives the point (3/5,4/5) behind the right triangle with sides 3, 4, 5.

Marking scheme. (10 points) - 2: 1−it≠0 with a reason, and |ut|=1 from the equal moduli of conjugates. - 1: ut≠−1. - 2: u=ut rewritten as a linear equation in t, with u+1≠0 used to solve it uniquely. - 3: shows that the unique solution is real and equals Imu/(1+Reu), with 1+Reu≠0 justified (for example by multiplying by u+1― and using uu―=1, with 2+2Reu>0). - Second route (coordinates u=x+yi, x2+y2=1): the two lines above (5 points) become 2 for splitting u−1=it(u+1) into x−1=−ty and y=t(1+x), showing x≠−1 (otherwise u=−1) and so t=y/(1+x) is forced; and 3 for checking that this t satisfies x−1=−ty, using x2+y2=1. - 2: (c) computed and checked. Fatal errors (0 for the step): writing u=eiθ and using a half-angle formula (borrowed facts, and values not derived here); dividing by 1+Reu without showing it is non-zero.