2 Revision of the exponential form of a complex number

Recall that a complex number in Cartesian form which is written as

z = a +  i b ,

where a and b are real numbers and  i 2 = 1 , can be written in polar form as

z = r ( cos θ +  i sin θ )

where r = z = a 2 + b 2 and θ , the argument or phase of z , is such that

a = r cos θ b = r sin θ .

A more concise version of the polar form of z can be obtained by defining a complex exponential quantity e  i θ by Euler’s relation

e  i θ cos θ +  i sin θ

The polar angle θ is normally expressed in radians . Replacing  i by  i we obtain the alternative form

e  i θ cos θ  i sin θ

Task!

Write down in cos θ ± i sin θ form and also in Cartesian form

  1. e  i π 6
  2. e  i π 6 .

Use Euler’s relation:

We have, by definition,

  1. e  i π 6 = cos π 6 +  i sin π 6 = 3 2 + 1 2  i
  2. e  i π 6 = cos π 6  i sin π 6 = 3 2 1 2  i
Task!

Write down

  1. cos π 6    
  2. sin π 6    in terms of e  i π 6 and e  i π 6 .

We have, adding the two results from the previous task

e  i π 6 + e  i π 6 = 2 cos π 6  or cos π 6 = 1 2 e  i π 6 + e  i π 6

Similarly, subtracting the two results,

e  i π 6 e  i π 6 = 2  i sin π 6  or sin π 6 = 1 2  i e  i π 6 e  i π 6

(Don’t forget the factor  i in this latter case.)

Clearly, similar calculations could be carried out for any angle θ . The general results are summarised in the following Key Point.

Key Point 8

Euler’s Relations

e i θ cos θ + i sin θ , e i θ cos θ i sin θ cos θ 1 2 e  i θ + e  i θ sin θ 1 2  i e  i θ e  i θ

Using these results we can redraft an expression of the form

a n cos n θ + b n sin n θ

in terms of complex exponentials.

(This expression, with θ = ω 0 t , is of course the n th harmonic of a trigonometric Fourier series.)

Task!

Using the results from the Key Point 8 (with n θ instead of θ ) rewrite

a n cos n θ + b n sin n θ

in complex exponential form.

First substitute for cos n θ and sin n θ with exponential expressions using Key Point 8:

We have

a n cos n θ = a n 2 e  i n θ + e  i n θ b n sin n θ = b n 2  i e  i n θ e  i n θ

so

a n cos n θ + b n sin n θ = a n 2 e  i n θ + e  i n θ + b n 2  i e  i n θ e  i n θ

Now collect the terms in e  i n θ and in e  i n θ and use the fact that 1 i = i :

We get

1 2 a n + b n  i e  i n θ + 1 2 a n b n  i e  i n θ

or, since 1  i =  i  i 2 =  i 1 2 ( a n  i b n ) e  i n θ + 1 2 ( a n +  i b n ) e  i n θ .

Now write this expression in more concise form by defining

c n = 1 2 ( a n  i b n )   which has complex conjugate   c n = 1 2 ( a n +  i b n ) .

Write the concise complex exponential expression for a n cos n θ + b n sin n θ :

a n cos n θ + b n sin n θ = c n e  i n θ + c n e  i n θ

Clearly, we can now rewrite the trigonometric Fourier series

a 0 2 + n = 1 ( a n cos n ω 0 t + b n sin n ω 0 t ) as a 0 2 + n = 1 c n e  i n ω 0 t + c n e  i n ω 0 t (3)

A neater, and particularly concise, form of this expression can be obtained as follows:

Firstly write a 0 2 = c 0 (which is consistent with the general definition of c n since b 0 = 0 ).

The second term in the summation

n = 1 c n e  i n ω 0 t = c 1 e  i ω 0 t + c 2 e 2  i ω 0 t +

can be written, if we define c n = c n = 1 2 ( a n +  i b n ) , as

c 1 e  i ω 0 t + c 2 e 2  i ω 0 t + c 3 e 3  i ω 0 t + = n = 1 c n e  i n ω 0 t

Hence (3) can be written c 0 + n = 1 c n e  i n ω 0 t + n = 1 c n e  i n ω 0 t  or in the very concise form n = c n e  i n ω 0 t .

The complex Fourier coefficients c n can be readily obtained as follows using (1) and (2) for a n , b n .

Firstly

c 0 = a 0 2 = 1 T T 2 T 2 f ( t ) d t (4)

For n = 1 , 2 , 3 , we have

c n = 1 2 ( a n  i b n ) = 1 T T 2 T 2 f ( t ) ( cos n ω 0 t  i sin n ω 0 t ) d t  i.e. c n = 1 T T 2 T 2 f ( t ) e  i n ω 0 t d t (5)

Also for n = 1 , 2 , 3 , we have

c n = c n = 1 2 ( a n +  i b n ) = 1 T T 2 T 2 f ( t ) e  i n ω 0 t d t

This last expression is equivalent to stating that for n = 1 , 2 , 3 ,

c n = 1 T T 2 T 2 f ( t ) e  i n ω 0 t d t (6)

The three equations (4), (5), (6) can thus all be contained in the one expression

c n = 1 T T 2 T 2 f ( t ) e  i n ω 0 t d t  for n = 0 , ± 1 , ± 2 , ± 3 ,

The results of this discussion are summarised in the following Key Point.

Key Point 9

Fourier Series in Complex Form

A function f ( t ) of period T has a complex Fourier series

f ( t ) = n = c n e  i n ω 0 t  where c n = 1 T T 2 T 2 f ( t ) e  i n ω 0 t d t

For the special case T = 2 π , so that ω 0 = 1 , these formulae become particularly simple:

f ( t ) = n = c n e  i n t c n = 1 2 π π π f ( t ) e  i n t d t .