which we can check directly
√
3 −j
1 −
√
3 j
=
(
√
3 −j)( 1 +
√
3 j)
12 +(
√
3 )^2
=
2
√
3 + 2 j
4
=
√
3
2
+
1
2
j
Exercise on 12.5
Ifz 1 =^
(π
4
)
andz 2 =^
(
−
π
3
)
evaluate
z 1
z 2
in polar and Cartesian form.
Answer
z 1
z 2
=^
(
7 π
12
)
=
( 1 −
√
3 )
2
√
2
+
(
√
3 + 1 )
2
√
2
j
12.6 Exponential form of a complex number
Having explained the usefulness of the polar form in multiplication and division of complex
numbers, I will now introduce a result that is as pretty as it is powerful:
ejθ≡cosθ+jsinθ=^ (θ)
Remember that this result is unchanged ifθis replaced byθ+ 2 kπwherekis an integer.
This result forejθwas first stated explicitly by the Swiss mathematician Leonard Euler
(1707 – 83) in 1748 – not so long ago really. It is known, along with countless other results,
asEuler’s formula. It can be proved by expanding the left-hand side in series, gathering
together real and imaginary parts after usingj^2 =−1 and summing the resulting series to
cosθand sinθ(see Reinforcement Exercise 18).
Problem 12.10
By taking particular values forqshow that
(i)ej^0 =ej^2 p= 1 (ii)ejp=− 1 (iii)ej
p
(^2) =j
(i)ej^0 =cos 0+jsin 0=1 and similarlyej^2 π=cos 2π+jsin 2π= 1
(ii)ejπ=cosπ+jsinπ=− 1
(iii)ej
π
(^2) =cos
π
2
+jsin
π
2
= 0 +j 1 =j
It can be shown thatejθobeys all the usual indices laws:
ejxejy=ej(x+y)– from multiplication in polar form
ejx
ejy
=ej(x−y)– from division in polar form
(ejx)y=ejxy– from an extension of Q2, Exercise 12.4