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5.6 Argument of a complex number
Let z = x + iy be a non{zero complex number, r = jzj =
p
x2 + y2. Then
we have x = r cos µ; y = r sin µ, where µ is the angle made by z with the
positive x{axis. So µ is unique up to addition of a multiple of 2¼ radians.
DEFINITION 5.6.1 (Argument) Any number µ satisfying the above
pair of equations is called an argument of z and is denoted by arg z. The
particular argument of z lying in the range ¡¼ < µ · ¼ is called the principal
argument of z and is denoted by Arg z (see Figure 5.5).
We have z = r cos µ + ir sin µ = r(cos µ + i sin µ) and this representation
of z is called the polar representation or modulus{argument form of z.
EXAMPLE 5.6.1 Arg 1 = 0, Arg (¡1) = ¼, Arg i = ¼
2 , Arg (¡i) = ¡¼
2 .
We note that y=x = tan µ if x 6= 0, so µ is determined by this equation up
to a multiple of ¼. In fact
Arg z = tan¡1 y
x
+ k¼;
104 CHAPTER 5. COMPLEX NUMBERS
¾ -
6
?
½
½
½
½>
x
r y
z
µ
Figure 5.5: The argument of z: arg z = µ.
where k = 0 if x > 0; k = 1 if x < 0; y > 0; k = ¡1 if x < 0; y < 0.
To determine Arg z graphically, it is simplest to draw the triangle formed
by the points 0; x; z on the complex plane, mark in the positive acute angle
® between the rays 0; x and 0; z and determine Arg z geometrically, using
the fact that ® = tan¡1(jyj=jxj), as in the following examples:
EXAMPLE 5.6.2 Determine the principal argument of z for the followig
complex numbers:
z = 4 + 3i; ¡4 + 3i; ¡4 ¡ 3i; 4 ¡ 3i:
Solution. Referring to Figure 5.6, we see that Arg z has the values
®; ¼ ¡ ®; ¡¼ + ®; ¡®;
where ® = tan¡1 3
4 .
An important property of the argument of a complex number states that
the sum of the arguments of two non{zero complex numbers is an argument
of their product:
THEOREM 5.6.1 If µ1 and µ2 are arguments of z1 and z2, then µ1 + µ2
is an argument of z1z2.
Proof. Let z1 and z2 have polar representations z1 = r1(cos µ1 + i sin µ1)
and z2 = r2(cos µ2 + i sin µ2). Then
z1z2 = r1(cos µ1 + i sin µ1)r2(cos µ2 + i sin µ2)
= r1r2(cos µ1 cos µ2 ¡ sin µ1 sin µ2 + i(cos µ1 sin µ2 + sin µ1 cos µ2))
= r1r2(cos (µ1 + µ2) + i sin (µ1 + µ2));
5.6. ARGUMENT OF A COMPLEX NUMBER 105
¾ -
6
?
x
y
4 + 3i
½®
½
½
½>
¾ -
6
?
x
y
¡4 + 3i
®Z
Z
Z
Z}
¾ -
6
?
x
y
¡4 ¡ 3i
®½
½
½
½=
¾ -
6
?
x
y
4 ¡ 3i
Z®
Z
Z
Z~
Figure 5.6: Argument examples.
which is the polar representation of z1z2, as r1r2 = jz1jjz2j = jz1z2j. Hence
µ1 + µ2 is an argument of z1z2.
An easy induction gives the following generalization to a product of n
complex numbers:
COROLLARY 5.6.1 If µ1; : : : ; µn are arguments for z1; : : : ; zn respectively,
then µ1 + ¢ ¢ ¢ + µn is an argument for z1 ¢ ¢ ¢ zn.
Taking µ1 = ¢ ¢ ¢ = µn = µ in the previous corollary gives
COROLLARY 5.6.2 If µ is an argument of z, then nµ is an argument for
zn.
THEOREM 5.6.2 If µ is an argument of the non{zero complex number
z, then ¡µ is an argument of z¡1.
Proof. Let µ be an argument of z. Then z = r(cos µ+i sin µ), where r = jzj.
Hence
z¡1 = r¡1(cos µ + i sin µ)¡1
= r¡1(cos µ ¡ i sin µ)
= r¡1(cos(¡µ) + i sin(¡µ)):
106 CHAPTER 5. COMPLEX NUMBERS
Now r¡1 = jzj¡1 = jz¡1j, so ¡µ is an argument of z¡1.
COROLLARY 5.6.3 If µ1 and µ2 are arguments of z1 and z2, then µ1¡µ2
is an argument of z1=z2.
In terms of principal arguments, we have the following equations:
(i) Arg (z1z2) = Arg z1+Arg z2 + 2k1¼,
(ii) Arg (z¡1) = ¡Arg z + 2k2¼,
(iii) Arg (z1=z2) = Arg z1¡Arg z2 + 2k3¼,
(iv) Arg (z1 ¢ ¢ ¢ zn) = Arg z1 + ¢ ¢ ¢ +Arg zn + 2k4¼,
(v) Arg (zn) = n Arg z + 2k5¼,
where k1; k2; k3; k4; k5 are integers.
In numerical examples, we can write (i), for example, as
Arg (z1z2) ´ Arg z1 + Arg z2:
EXAMPLE 5.6.3 Find the modulus and principal argument of
z =
Ãp3 + i
1 + i
!17
and hence express z in modulus{argument form.
Solution. jzj = jp3 + ij17
j1 + ij17 =
217
(p2)17
= 217=2.
Arg z ´ 17Arg
Ãp3 + i
1 + i
!
= 17(Arg (p3 + i) ¡ Arg (1 + i))
= 17
³¼
6 ¡
¼
4
´
= ¡17¼
12
:
Hence Arg z =
¡
¡17¼
12
¢
+ 2k¼, where k is an integer. We see that k = 1 and
hence Arg z = 7¼
12 . Consequently z = 217=2
¡
cos 7¼
12 + i sin 7¼
12
¢
.
DEFINITION 5.6.2 If µ is a real number, then we de¯ne eiµ by
eiµ = cos µ + i sin µ:
More generally, if z = x + iy, then we de¯ne ez by
ez = exeiy:
5.7. DE MOIVRE'S THEOREM 107
For example,
e
i¼
2 = i; ei¼ = ¡1; e¡i¼
2 = ¡i:
The following properties of the complex exponential function are left as
exercises:
THEOREM 5.6.3 (i) ez1ez2 = ez1+z2 ,
(ii) ez1 ¢ ¢ ¢ ezn = ez1+¢¢¢+zn,
(iii) ez 6= 0,
(iv) (ez)¡1 = e¡z,
(v) ez1=ez2 = ez1¡z2 ,
(vi) ez = ez.
THEOREM 5.6.4 The equation
ez = 1
has the complete solution z = 2k¼i; k 2 Z.
Proof. First we observe that
e2k¼i = cos (2k¼) + i sin (2k¼) = 1:
Conversely, suppose ez = 1; z = x + iy. Then ex(cos y + i sin y) = 1. Hence
ex cos y = 1 and ex sin y = 0. Hence sin y = 0 and so y = n¼; n 2 Z. Then
ex cos (n¼) = 1, so ex(¡1)n = 1, from which follows (¡1)n = 1 as ex > 0.
Hence n = 2k; k 2 Z and ex = 1. Hence x = 0 and z = 2k¼i.
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