The Central Idea

A nonzero complex number

\[ z=a+bi \]

determines a point \((a,b)\) in the complex plane. The same point can be described by its distance \(r\) from the origin and an angle \(\theta\) from the positive real axis.

\[ a=r\cos\theta, \qquad b=r\sin\theta. \]

Therefore,

\[ \boxed{z=r(\cos\theta+i\sin\theta)}. \]

This is the polar, or trigonometric, form of a complex number.

The Modulus

For

\[ z=a+bi, \]

the distance from the origin is

\[ \boxed{|z|=\sqrt{a^2+b^2}}. \]

In polar notation this distance is written \(r\), so

\[ \boxed{r=|z|}. \]

The Argument

The angle from the positive real axis to the vector representing \(z\) is called an argument of \(z\).

\[ \theta=\arg z. \]

When \(a\neq0\), the angle satisfies

\[ \tan\theta=\frac{b}{a}. \]

The quadrant of \((a,b)\) must be considered when selecting the correct angle.

The Argument Is Not Unique

A complete rotation changes an angle by \(2\pi\) without changing its direction. Therefore, if \(\theta\) is one argument of \(z\), then

\[ \boxed{\theta+2\pi k,\qquad k\in\mathbb{Z}} \]

is also an argument.

The Principal Argument

A common convention chooses one standard argument called the principal argument, written \(\operatorname{Arg}(z)\), with

\[ \boxed{-\pi<\operatorname{Arg}(z)\le\pi}. \]

Other conventions are possible, so the interval should always be stated or understood from context.

The Special Case \(z=0\)

The complex number \(0\) has modulus \(0\), but it has no defined argument. The zero vector has no direction, so formulas involving \(\arg z\) normally assume \(z\neq0\).

Converting Rectangular Form to Polar Form

For \(z=a+bi\), first calculate

\[ r=\sqrt{a^2+b^2}. \]

Then determine an angle \(\theta\) satisfying

\[ \cos\theta=\frac{a}{r}, \qquad \sin\theta=\frac{b}{r}. \]

Finally write

\[ \boxed{z=r(\cos\theta+i\sin\theta)}. \]

Example: Convert \(1+i\) to Polar Form

The modulus is

\[ r=\sqrt{1^2+1^2}=\sqrt2. \]

The point \((1,1)\) lies at angle

\[ \theta=\frac{\pi}{4}. \]

Therefore,

\[ \boxed{ 1+i=\sqrt2\left(\cos\frac{\pi}{4}+i\sin\frac{\pi}{4}\right) }. \]

Example: Quadrant Matters

Convert

\[ z=-1+\sqrt3\,i \]

to polar form. The modulus is

\[ r=\sqrt{(-1)^2+(\sqrt3)^2}=2. \]

The reference angle is \(\pi/3\), but the point lies in Quadrant II, so the principal argument is

\[ \theta=\frac{2\pi}{3}. \]

Thus,

\[ \boxed{ -1+\sqrt3\,i = 2\left(\cos\frac{2\pi}{3}+i\sin\frac{2\pi}{3}\right) }. \]

Converting Polar Form to Rectangular Form

Starting with

\[ z=r(\cos\theta+i\sin\theta), \]

distribute \(r\):

\[ z=r\cos\theta+i(r\sin\theta). \]

Therefore,

\[ \boxed{a=r\cos\theta,\qquad b=r\sin\theta}. \]

Example: Convert Polar Form to Rectangular Form

Convert

\[ 6\left(\cos\frac{\pi}{6}+i\sin\frac{\pi}{6}\right). \]

Since

\[ \cos\frac{\pi}{6}=\frac{\sqrt3}{2}, \qquad \sin\frac{\pi}{6}=\frac12, \]

we get

\[ z=6\left(\frac{\sqrt3}{2}\right)+6i\left(\frac12\right). \]

Therefore,

\[ \boxed{z=3\sqrt3+3i}. \]

Multiplying Complex Numbers in Polar Form

Let

\[ z_1=r_1(\cos\theta_1+i\sin\theta_1) \]

and

\[ z_2=r_2(\cos\theta_2+i\sin\theta_2). \]

Using the trigonometric angle-addition identities,

\[ \boxed{ z_1z_2 = r_1r_2 \left[ \cos(\theta_1+\theta_2) + i\sin(\theta_1+\theta_2) \right] }. \]

The Geometry of Complex Multiplication

The multiplication rule says:

  1. multiply the moduli;
  2. add the arguments.
\[ \boxed{|z_1z_2|=|z_1||z_2|} \]

and

\[ \boxed{\arg(z_1z_2)=\arg z_1+\arg z_2\pmod{2\pi}}. \]

Complex multiplication is therefore a combination of scaling and rotation.

Example: Multiplication in Polar Form

Let

\[ z_1=2\left(\cos\frac{\pi}{6}+i\sin\frac{\pi}{6}\right) \]

and

\[ z_2=3\left(\cos\frac{\pi}{4}+i\sin\frac{\pi}{4}\right). \]

Multiply the moduli:

\[ 2\cdot3=6. \]

Add the angles:

\[ \frac{\pi}{6}+\frac{\pi}{4}=\frac{5\pi}{12}. \]

Therefore,

\[ \boxed{ z_1z_2 = 6\left(\cos\frac{5\pi}{12}+i\sin\frac{5\pi}{12}\right) }. \]

Dividing Complex Numbers in Polar Form

For \(z_2\neq0\),

\[ \boxed{ \frac{z_1}{z_2} = \frac{r_1}{r_2} \left[ \cos(\theta_1-\theta_2) + i\sin(\theta_1-\theta_2) \right] }. \]

Division divides moduli and subtracts arguments.

Example: Division in Polar Form

Compute

\[ \frac{ 8\left(\cos\frac{3\pi}{4}+i\sin\frac{3\pi}{4}\right) }{ 2\left(\cos\frac{\pi}{6}+i\sin\frac{\pi}{6}\right) }. \]

Divide the moduli:

\[ \frac82=4. \]

Subtract the arguments:

\[ \frac{3\pi}{4}-\frac{\pi}{6}=\frac{7\pi}{12}. \]

Therefore,

\[ \boxed{ 4\left(\cos\frac{7\pi}{12}+i\sin\frac{7\pi}{12}\right) }. \]

De Moivre's Formula

Repeated multiplication leads to a convenient rule for integer powers. If

\[ z=r(\cos\theta+i\sin\theta), \]

then for an integer \(n\),

\[ \boxed{ z^n = r^n(\cos n\theta+i\sin n\theta) }. \]

This is De Moivre's formula.

Example: Using De Moivre's Formula

Compute

\[ \left[ 2\left(\cos\frac{\pi}{3}+i\sin\frac{\pi}{3}\right) \right]^4. \]

Raise the modulus to the fourth power:

\[ 2^4=16. \]

Multiply the argument by \(4\):

\[ 4\cdot\frac{\pi}{3}=\frac{4\pi}{3}. \]

Therefore,

\[ \boxed{ 16\left(\cos\frac{4\pi}{3}+i\sin\frac{4\pi}{3}\right) }. \]

Roots of a Complex Number

Suppose

\[ w^n=z \]

and write

\[ z=r(\cos\theta+i\sin\theta). \]

The \(n\) distinct roots are

\[ \boxed{ w_k = r^{1/n} \left[ \cos\left(\frac{\theta+2\pi k}{n}\right) + i\sin\left(\frac{\theta+2\pi k}{n}\right) \right] } \]

for

\[ k=0,1,\ldots,n-1. \]

The Geometry of Complex Roots

All \(n\)th roots of a nonzero complex number have modulus

\[ r^{1/n}. \]

Their arguments differ by

\[ \frac{2\pi}{n}. \]

Therefore, the roots are equally spaced around a circle centered at the origin.

The \(n\)th Roots of Unity

The equation

\[ z^n=1 \]

has the roots

\[ \boxed{ z_k = \cos\left(\frac{2\pi k}{n}\right) + i\sin\left(\frac{2\pi k}{n}\right) } \]

for \(k=0,1,\ldots,n-1\). They lie at the vertices of a regular \(n\)-gon on the unit circle.

Example: Cube Roots of Unity

The equation

\[ z^3=1 \]

gives the angles

\[ 0, \qquad \frac{2\pi}{3}, \qquad \frac{4\pi}{3}. \]

Therefore, the roots are

\[ \boxed{1}, \] \[ \boxed{-\frac12+\frac{\sqrt3}{2}i}, \] \[ \boxed{-\frac12-\frac{\sqrt3}{2}i}. \]

The Complex Exponential

The exponential function extends naturally to complex inputs. The central identity is

\[ \boxed{e^{i\theta}=\cos\theta+i\sin\theta}. \]

This is Euler's formula. It links exponential functions, trigonometry, and rotation in the complex plane.

Special Values from Euler's Formula

At \(\theta=0\),

\[ e^{0i}=1. \]

At \(\theta=\frac{\pi}{2}\),

\[ e^{i\pi/2}=i. \]

At \(\theta=\pi\),

\[ e^{i\pi}=-1. \]

Euler's Identity

Since

\[ e^{i\pi}=-1, \]

we obtain

\[ \boxed{e^{i\pi}+1=0}. \]

This single equation connects \(e\), \(i\), \(\pi\), \(1\), and \(0\).

Exponential Form of a Complex Number

Combining polar form with Euler's formula gives

\[ z=r(\cos\theta+i\sin\theta) =re^{i\theta}. \]

Therefore,

\[ \boxed{z=re^{i\theta}}. \]

This is the exponential form of a nonzero complex number.

Example: Write \(1+i\) in Exponential Form

We know

\[ |1+i|=\sqrt2 \]

and

\[ \arg(1+i)=\frac{\pi}{4}. \]

Therefore,

\[ \boxed{1+i=\sqrt2\,e^{i\pi/4}}. \]

Multiplication in Exponential Form

If

\[ z_1=r_1e^{i\theta_1} \]

and

\[ z_2=r_2e^{i\theta_2}, \]

then ordinary exponent rules give

\[ \boxed{z_1z_2=r_1r_2e^{i(\theta_1+\theta_2)}}. \]

Division in Exponential Form

For \(z_2\neq0\),

\[ \boxed{ \frac{z_1}{z_2} = \frac{r_1}{r_2}e^{i(\theta_1-\theta_2)} }. \]

Powers in Exponential Form

If

\[ z=re^{i\theta}, \]

then

\[ \boxed{z^n=r^ne^{in\theta}}. \]

Applying Euler's formula recovers De Moivre's formula immediately.

The Unit Circle in Exponential Form

Every complex number of modulus \(1\) can be written as

\[ \boxed{e^{i\theta}}. \]

As \(\theta\) varies, \(e^{i\theta}\) traces the unit circle.

Rotation by Multiplication with \(e^{i\phi}\)

Let

\[ z=re^{i\theta}. \]

Multiplication by \(e^{i\phi}\) gives

\[ e^{i\phi}z=re^{i(\theta+\phi)}. \]

The modulus remains unchanged while the argument increases by \(\phi\). Therefore,

\[ \boxed{z\mapsto e^{i\phi}z} \]

rotates the plane counterclockwise by angle \(\phi\) about the origin.

Scaling and Rotation Together

Let

\[ w=\rho e^{i\phi}. \]

Multiplying

\[ z=re^{i\theta} \]

by \(w\) gives

\[ wz=\rho r e^{i(\phi+\theta)}. \]

Thus multiplication by \(w\):

Conjugation in Exponential Form

If

\[ z=re^{i\theta}, \]

then

\[ \boxed{\overline{z}=re^{-i\theta}}. \]

Reversing the sign of the angle reflects the point across the real axis.

Reciprocals in Exponential Form

For \(z=re^{i\theta}\neq0\),

\[ \boxed{\frac1z=\frac1r e^{-i\theta}}. \]

The reciprocal inverts the modulus and reverses the argument.

The Negative Real Axis

If \(r>0\), then the negative real number \(-r\) has principal argument \(\pi\). Therefore,

\[ \boxed{-r=re^{i\pi}}. \]

All equivalent arguments are

\[ \pi+2\pi k, \qquad k\in\mathbb{Z}. \]

Exponential Form Is Not Unique

Since

\[ e^{i(\theta+2\pi k)}=e^{i\theta}, \]

a nonzero complex number has infinitely many exponential representations:

\[ \boxed{z=re^{i(\theta+2\pi k)},\qquad k\in\mathbb{Z}}. \]

A Preview of the Complex Logarithm

For a nonzero complex number

\[ z=re^{i\theta}, \]

expressions of the form

\[ \ln r+i\theta \]

naturally arise when solving for an exponent. Because \(\theta\) can differ by multiples of \(2\pi\), the complex logarithm is naturally multivalued. Later lessons will treat branches and principal values carefully.

Why Exponential Form Is Useful

Rectangular form is usually most efficient for addition and subtraction. Polar or exponential form is usually most efficient for:

Connection to Oscillation and Signals

Euler's formula gives

\[ e^{i\omega t}=\cos(\omega t)+i\sin(\omega t). \]

A complex exponential therefore packages sine and cosine into one expression. This representation appears throughout differential equations, Fourier analysis, electrical engineering, wave models, communications, and signal processing.

A First Look at Phasors

A sinusoidal expression such as

\[ A\cos(\omega t+\phi) \]

can be viewed as the real part of

\[ Ae^{i(\omega t+\phi)}. \]

This rotating complex representation separates amplitude and phase from repetitive trigonometric calculations. It is the basic idea behind phasor methods.

Common Error: Ignoring the Quadrant

Using

\[ \theta=\arctan\left(\frac{b}{a}\right) \]

without checking the signs of \(a\) and \(b\) can produce the wrong angle. For example, \(-1+i\) lies in Quadrant II, so its principal argument is

\[ \boxed{\frac{3\pi}{4}}, \]

not \(-\frac{\pi}{4}\).

Common Error: Mixing Degrees and Radians

Complex analysis normally uses radians. For example,

\[ 90^\circ=\frac{\pi}{2}. \]

When using a calculator, confirm the angle mode before interpreting an inverse-trigonometric result.

Common Error: Treating the Argument as Unique

If \(\theta\) is an argument, then

\[ \theta+2\pi k \]

is also an argument for every integer \(k\). Only the principal argument is chosen as one conventional representative.

Common Error: Finding Only One Root

An equation such as

\[ w^n=z \]

has \(n\) distinct roots when \(z\neq0\). Omitting the \(2\pi k\) term from the root formula usually causes the remaining roots to be missed.

Common Error: Applying the Wrong Operations

In polar form, multiplication means:

Division means:

A Reliable Procedure: Rectangular to Polar Form

  1. Identify \(a=\operatorname{Re}(z)\) and \(b=\operatorname{Im}(z)\).
  2. Compute \(r=\sqrt{a^2+b^2}\).
  3. Find a reference angle.
  4. Use the quadrant to determine the correct argument.
  5. Write \(z=r(\cos\theta+i\sin\theta)\).
  6. When useful, rewrite it as \(z=re^{i\theta}\).
  7. Check using \(a=r\cos\theta\) and \(b=r\sin\theta\).

A Reliable Procedure: Polar Operations

  1. Write each nonzero number as \(re^{i\theta}\).
  2. For multiplication, multiply moduli and add arguments.
  3. For division, divide moduli and subtract arguments.
  4. For powers, raise the modulus and multiply the argument.
  5. For \(n\)th roots, take the \(n\)th root of the modulus.
  6. Use \((\theta+2\pi k)/n\) to generate every root argument.
  7. Convert back to rectangular form only when useful.

Worked Example: Rectangular, Polar, and Exponential Forms

Let

\[ z=-\sqrt3+i. \]

The modulus is

\[ r=\sqrt{3+1}=2. \]

The point lies in Quadrant II with reference angle \(\pi/6\), so

\[ \theta=\frac{5\pi}{6}. \]

Polar form:

\[ \boxed{ z=2\left(\cos\frac{5\pi}{6}+i\sin\frac{5\pi}{6}\right) }. \]

Exponential form:

\[ \boxed{z=2e^{i5\pi/6}}. \]

Worked Example: Product by Exponential Form

Let

\[ z_1=2e^{i\pi/3} \]

and

\[ z_2=5e^{-i\pi/6}. \]

Then

\[ z_1z_2 = 10e^{i(\pi/3-\pi/6)} = 10e^{i\pi/6}. \]

Therefore,

\[ \boxed{z_1z_2=10e^{i\pi/6}}. \]

In rectangular form,

\[ \boxed{z_1z_2=5\sqrt3+5i}. \]

Worked Example: Find All Fourth Roots of \(16\)

Write

\[ 16=16e^{i2\pi k}. \]

The fourth-root modulus is

\[ 16^{1/4}=2. \]

The root arguments are

\[ \frac{2\pi k}{4}=\frac{\pi k}{2}, \qquad k=0,1,2,3. \]

Therefore, the roots are

\[ \boxed{2,\quad2i,\quad-2,\quad-2i}. \]

Practice 1: Convert to Polar Form

Write

\[ z=\sqrt3+i \]

in polar form.

Practice 2: Convert to Exponential Form

Write

\[ z=-2i \]

in exponential form using the principal argument.

Practice 3: Convert to Rectangular Form

Convert

\[ 4e^{i\pi/3} \]

to rectangular form.

Practice 4: Multiply

Compute

\[ \left(3e^{i\pi/4}\right)\left(2e^{i\pi/6}\right). \]

Practice 5: Divide

Compute

\[ \frac{12e^{i5\pi/6}}{3e^{i\pi/3}}. \]

Practice 6: Power

Use De Moivre's formula to compute

\[ \left[ 2\left(\cos\frac{\pi}{4}+i\sin\frac{\pi}{4}\right) \right]^3. \]

Practice 7: Roots of Unity

Find all solutions of

\[ z^4=1. \]

Practice 8: General Arguments

Give all arguments of

\[ z=-1-i. \]

Practice 9: Rotation

If

\[ z=3-2i, \]

find the result of rotating \(z\) counterclockwise by \(\pi/2\) using complex multiplication.

Practice 10: Find All Cube Roots

Find all solutions of

\[ w^3=8. \]

Practice Answers

Practice 1

The modulus is

\[ r=2, \]

and the argument is \(\pi/6\). Therefore,

\[ \boxed{ \sqrt3+i = 2\left(\cos\frac{\pi}{6}+i\sin\frac{\pi}{6}\right) }. \]

Practice 2

The modulus is \(2\), and the principal argument is \(-\pi/2\). Therefore,

\[ \boxed{-2i=2e^{-i\pi/2}}. \]

Practice 3

\[ 4e^{i\pi/3} = 4\left(\frac12+i\frac{\sqrt3}{2}\right). \]

Therefore,

\[ \boxed{2+2\sqrt3\,i}. \]

Practice 4

\[ \boxed{6e^{i5\pi/12}}. \]

Practice 5

\[ \frac{12e^{i5\pi/6}}{3e^{i\pi/3}} = 4e^{i\pi/2}. \]

Therefore,

\[ \boxed{4i}. \]

Practice 6

\[ 2^3=8 \]

and

\[ 3\cdot\frac{\pi}{4}=\frac{3\pi}{4}. \]

Therefore,

\[ \boxed{ 8\left(\cos\frac{3\pi}{4}+i\sin\frac{3\pi}{4}\right) }. \]

In rectangular form,

\[ \boxed{-4\sqrt2+4\sqrt2\,i}. \]

Practice 7

The fourth roots of unity are

\[ \boxed{1,\quad i,\quad-1,\quad-i}. \]

Practice 8

The principal argument is \(-3\pi/4\). Therefore, all arguments are

\[ \boxed{-\frac{3\pi}{4}+2\pi k,\qquad k\in\mathbb{Z}}. \]

Practice 9

A counterclockwise rotation by \(\pi/2\) is multiplication by \(i\):

\[ i(3-2i)=3i-2i^2=2+3i. \]

Therefore,

\[ \boxed{2+3i}. \]

Practice 10

The cube-root modulus is \(2\), and the arguments are

\[ 0, \qquad \frac{2\pi}{3}, \qquad \frac{4\pi}{3}. \]

Therefore,

\[ \boxed{2,\quad-1+\sqrt3\,i,\quad-1-\sqrt3\,i}. \]

Checking Strategies

Connections to Earlier Mathematics

What to Remember

For

\[ z=a+bi\neq0, \]

the modulus is

\[ \boxed{r=|z|=\sqrt{a^2+b^2}}. \]

Polar form is

\[ \boxed{z=r(\cos\theta+i\sin\theta)}. \]

Euler's formula is

\[ \boxed{e^{i\theta}=\cos\theta+i\sin\theta}. \]

Exponential form is

\[ \boxed{z=re^{i\theta}}. \]

In this form,

\[ \boxed{ (r_1e^{i\theta_1})(r_2e^{i\theta_2}) = r_1r_2e^{i(\theta_1+\theta_2)} } \]

and

\[ \boxed{ \frac{r_1e^{i\theta_1}}{r_2e^{i\theta_2}} = \frac{r_1}{r_2}e^{i(\theta_1-\theta_2)} }. \]

The central geometric rule is: complex multiplication multiplies scale and adds rotation.

Where We Go Next

We now have three complementary representations of a complex number: rectangular form \(a+bi\), polar form \(r(\cos\theta+i\sin\theta)\), and exponential form \(re^{i\theta}\).

The next lesson, Complex Functions, uses these representations to study mappings from the complex plane to itself. We will examine how functions transform points, regions, magnitude, direction, and geometric structure before moving into complex limits and continuity.