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
2jExercise on 12.5
Ifz 1 =^
(π4)
andz 2 =^(
−π
3)
evaluatez 1
z 2in polar and Cartesian form.Answer
z 1
z 2
=^(
7 π
12)
=( 1 −√
3 )
2√
2+(√
3 + 1 )
2√
2j12.6 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)ejp(^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