try
←

The Exponential Form of a Complex Number

Practice this lesson in the app →

The series for e to the is exactly plus

The exponential series, fed an imaginary number

The Maclaurin series for is , and it adds up to for every real number x. Its terms use only multiplying and adding, which work for complex numbers too, so the same series gives a meaning to e raised to an imaginary power.

Substitute , where is real:

The powers of i sort the terms

The powers of i repeat every four: , , , , and then again. So , , and .

The series becomes The even powers have no i and the odd powers have one, so collect them separately: .

Cosine and sine

The bracket without i is the Maclaurin series for , and the bracket with i is the series for . So .

From here on the angle is in RADIANS. The series and hold only for in radians, so does too. A half turn is radians, so 30° is , 60° is , 90° is and 180° is .

Check at , which is 1 radian, about 57.3°. The first four terms of each bracket give and , and , .

realimaginary

The terms of the series for at , laid head to tail: 1, then i, then , then , then . Each turns a quarter turn from the one before, and from the third on each is shorter; their total closes on the point , on the dashed unit circle.

A point on the unit circle

The length of is , and its argument is . So is the point on the unit circle at angle from the positive real axis.

The quarter turns: , , , and . Written another way, . A full turn returns to the start: .

is the point at 60°: .

realimaginary

Five values of on the unit circle: 1 at , at , i at , −1 at and −i at .

Every complex number as re

A complex number with modulus r and argument is , and the bracket is . So z = re: r is the distance from the origin, and , in radians, is the direction.

, which is . 1 + i has modulus and argument , so . , its argument below the axis.

On the axes: , , and . Arguments are taken in , the radian form of .

Lengths multiply, angles add

Index laws add powers: . So . The lengths multiply and the angles add, the rule for multiplying complex numbers met in polar form.

. In parts, and , and .

Dividing subtracts the angles: . The conjugate of re is re. And De Moivre’s theorem is the index law in.

The usual mistakes

Moving r into the exponent. is not : the second has length 1 and angle .

Dropping the i. is a real number, about 5.70; it is the i in the exponent that makes an angle.

Giving . is half a turn, so ; a full turn, , is 1.

Adding the lengths, or multiplying the exponents. is , not or .

Putting degrees in the exponent. is not : it is the point at 60 radians, about −0.952 − 0.305i.

Four loudspeakers slightly out of step

In the application below, the phasors 1, , and are 1 at 0°, 30°, 60° and 90°. Their sum is the sum drawn in Summing a Series with De Moivre at : , which has length about 3.35 and argument , or 45°.

The Complex Plane · Four Loudspeakers Slightly Out of Step: The Loudness and Phase of the Combined Tone

QuestionFour loudspeakers play the same tone, each with amplitude 1 unit. At a listener, the phase of each wave is π6 radians ahead of the one before, so the four waves are the phasors 1, eiπ/6, e2iπ/6 and e3iπ/6, and the combined tone is their sum S. (a) Find the amplitude of the combined tone, |S|, to 3 significant figures. (b) Find its phase, arg S, measured from the first speaker's wave.

  1. 1.With w = eiπ/6 the sum is S = 1 + w + w2 + w3, a geometric series of four terms, so S = w4 − 1w − 1 = e2iπ/3 − 1eiπ/6 − 1.

    ReIm1234S = 1 + w + w2+ w3= (w4− 1)/(w − 1)
    The four waves are arrows of length 1, each turned π6 from the last; the combined tone is their sum, head to tail.
  2. 2.Take out half the angle: eiα − 1 = eiα/2(eiα/2 − e−iα/2) = eiα/2 × 2i sinα2. So the top is eiπ/3 × 2i sinπ3 and the bottom is eiπ/12 × 2i sinπ12.

    ReIm1234S = 1 + w + w2+ w3= (w4− 1)/(w − 1)eia− 1 = eia/2× 2i sin(a/2)
    Taking out half the angle writes eiα − 1 as eiα/2 × 2i sinα2.
  3. 3.Dividing, the 2i cancels and the exponentials divide by subtracting their angles: S = ei(π3 − π12) × sin(π/3)sin(π/12) = eiπ/4 × sin(π/3)sin(π/12).

    ReIm1234S = 1 + w + w2+ w3= (w4− 1)/(w − 1)eia− 1 = eia/2× 2i sin(a/2)S = ei pi/4× sin(pi/3)/sin(pi/12)
    The 2i cancels, and the exponentials divide by subtracting their angles, π3 − π12 = π4.
  4. 4.(a) The amplitude is |S| = sin(π/3)sin(π/12) = 0.86600.2588 ≈ 3.35 units, a little less than the 4 units the speakers would give in step.

    ReIm1234size 3.35S = 1 + w + w2+ w3= (w4− 1)/(w − 1)eia− 1 = eia/2× 2i sin(a/2)S = ei pi/4× sin(pi/3)/sin(pi/12)size of S = 0.866/0.259 = 3.35
    (a) The combined amplitude is 3.35 units, the length of the gold arrow.
  5. 5.(b) The phase is arg S = π4, halfway between the first wave and the last. Check by adding the four directly: the real parts are 1 + 0.866 + 0.5 + 0 = 2.366 and the imaginary parts 0 + 0.5 + 0.866 + 1 = 2.366. The two parts are equal, so the angle is π4, and √2.3662 + 2.3662 = 3.35.

    ReIm1234size 3.35pi/4S = 1 + w + w2+ w3= (w4− 1)/(w − 1)eia− 1 = eia/2× 2i sin(a/2)S = ei pi/4× sin(pi/3)/sin(pi/12)size of S = 0.866/0.259 = 3.35arg S = pi/4
    (b) Its phase is π4 ahead of the first speaker's wave.

Answer: (a) |S| = sin(π/3)sin(π/12) ≈ 3.35 units; (b) arg S = π4 radians ahead of the first wave

Watch out for

  • Adding the amplitudes to get 4 units. The waves are not in step, so the phasors point in different directions and add as arrows, head to tail; the arrows' total length is 4, but the sum reaches only 3.35.
  • Using w3 on the top of the formula because the last term is w3. A geometric series of n terms sums to wn − 1w − 1, and here there are four terms, from w0 to w3, so the top is w4 − 1.

Your turn

1.Write in exponential form. 

as re
Practice The Exponential Form of a Complex Number in the app