Complex numbers extend the real number system by introducing a solution to the equation x 2 + 1 = 0 x^2 + 1 = 0 x 2 + 1 = 0 . This seemingly abstract idea turns out to be indispensable in pure mathematics, Engineering, and physics, providing powerful tools for analysing rotations, oscillations, and Polynomial equations.
Board Paper Notes AQA Paper 1 Full coverage including transformations w = f ( z ) w = f(z) w = f ( z ) Edexcel FP1/FP2 De Moivre, roots of unity, loci in FP2 OCR (A) Paper 1 De Moivre, exponential form, roots of unity CIE P1 Loci required; exponential form and roots of unity in depth
Definition. A complex number is a number of the form z = a + b i z = a + bi z = a + bi where a , b ∈ R a, b \in \mathbb{R} a , b ∈ R And i i i is defined by the property i 2 = − 1 i^2 = -1 i 2 = − 1 . The set of all complex numbers is denoted C \mathbb{C} C .
We call a a a the real part (written Re ( z ) \operatorname{Re}(z) Re ( z ) ) and b b b the imaginary part (written Im ( z ) \operatorname{Im}(z) Im ( z ) ). Two complex numbers are equal if and only if both their real and imaginary Parts are equal.
Definition. The Argand diagram is a representation of C \mathbb{C} C as a plane, where the Horizontal axis represents Re ( z ) \operatorname{Re}(z) Re ( z ) and the vertical axis represents Im ( z ) \operatorname{Im}(z) Im ( z ) . The complex number z = a + b i z = a + bi z = a + bi is plotted as the point ( a , b ) (a, b) ( a , b ) .
Definition. For z = a + b i ≠ 0 z = a + bi \neq 0 z = a + bi = 0 :
The modulus ∣ z ∣ |z| ∣ z ∣ is defined as ∣ z ∣ = a 2 + b 2 |z| = \sqrt{a^2 + b^2} ∣ z ∣ = a 2 + b 2 . The argument arg ( z ) \arg(z) arg ( z ) is the angle θ \theta θ (measured anticlockwise from the positive real axis) such that tan θ = b a \tan\theta = \dfrac{b}{a} tan θ = a b With − π < θ ≤ π -\pi < \theta \leq \pi − π < θ ≤ π (the principal argument ). z = a + b i = ∣ z ∣ ( cos θ + i sin θ ) = r ( cos θ + i sin θ ) \boxed{z = a + bi = |z|(\cos\theta + i\sin\theta) = r(\cos\theta + i\sin\theta)} z = a + bi = ∣ z ∣ ( cos θ + i sin θ ) = r ( cos θ + i sin θ )
Where r = ∣ z ∣ r = |z| r = ∣ z ∣ and θ = arg ( z ) \theta = \arg(z) θ = arg ( z ) .
For z 1 = a + b i z_1 = a + bi z 1 = a + bi and z 2 = c + d i z_2 = c + di z 2 = c + d i :
Z 1 + z 2 = ( a + c ) + ( b + d ) i Z 1 z 2 = ( a c − b d ) + ( a d + b c ) i z 1 z 2 = z 1 z 2 ‾ ∣ z 2 ∣ 2 = ( a c + b d ) + ( b c − a d ) i c 2 + d 2 \begin{aligned} Z_1 + z_2 &= (a + c) + (b + d)i \\ Z_1 z_2 &= (ac - bd) + (ad + bc)i \\ \frac{z_1}{z_2} &= \frac{z_1 \overline{z_2}}{|z_2|^2} = \frac{(ac + bd) + (bc - ad)i}{c^2 + d^2} \end{aligned} Z 1 + z 2 Z 1 z 2 z 2 z 1 = ( a + c ) + ( b + d ) i = ( a c − b d ) + ( a d + b c ) i = ∣ z 2 ∣ 2 z 1 z 2 = c 2 + d 2 ( a c + b d ) + ( b c − a d ) i Where z 2 ‾ = c − d i \overline{z_2} = c - di z 2 = c − d i is the complex conjugate of z 2 z_2 z 2 .
Caution: warning θ = arctan ( b / a ) \theta = \arctan(b/a) θ = arctan ( b / a ) only gives the correct principal argument when a > 0 a > 0 a > 0 .
Worked Example: Modulus, argument, and polar form Find the modulus, argument, and polar form of z = 1 − 3 i z = 1 - \sqrt{3}\,i z = 1 − 3 i .
∣ z ∣ = 1 2 + ( − 3 ) 2 = 1 + 3 = 2 |z| = \sqrt{1^2 + (-\sqrt{3})^2} = \sqrt{1 + 3} = 2 ∣ z ∣ = 1 2 + ( − 3 ) 2 = 1 + 3 = 2
Since ( a , b ) = ( 1 , − 3 ) (a, b) = (1, -\sqrt{3}) ( a , b ) = ( 1 , − 3 ) lies in the fourth quadrant:
arg ( z ) = arctan ( − 3 1 ) = − π 3 \arg(z) = \arctan\!\left(\frac{-\sqrt{3}}{1}\right) = -\frac{\pi}{3} arg ( z ) = arctan ( 1 − 3 ) = − 3 π
Polar form: z = 2 ( cos ( − π 3 ) + i sin ( − π 3 ) ) z = 2\!\left(\cos\!\left(-\dfrac{\pi}{3}\right) + i\sin\!\left(-\dfrac{\pi}{3}\right)\right) z = 2 ( cos ( − 3 π ) + i sin ( − 3 π ) ) .
Theorem (De Moivre). For any integer n n n and any angle θ \theta θ :
( cos θ + i sin θ ) n = cos ( n θ ) + i sin ( n θ ) \boxed{\left(\cos\theta + i\sin\theta\right)^n = \cos(n\theta) + i\sin(n\theta)} ( cos θ + i sin θ ) n = cos ( n θ ) + i sin ( n θ )
Base case (n = 0 n = 0 n = 0 ): ( cos θ + i sin θ ) 0 = 1 = cos 0 + i sin 0 (\cos\theta + i\sin\theta)^0 = 1 = \cos 0 + i\sin 0 ( cos θ + i sin θ ) 0 = 1 = cos 0 + i sin 0 . ✓
Inductive step. Assume ( cos θ + i sin θ ) k = cos ( k θ ) + i sin ( k θ ) (\cos\theta + i\sin\theta)^k = \cos(k\theta) + i\sin(k\theta) ( cos θ + i sin θ ) k = cos ( k θ ) + i sin ( k θ ) for some k ≥ 0 k \geq 0 k ≥ 0 . Then:
( cos θ + i sin θ ) k + 1 = ( cos θ + i sin θ ) k ⋅ ( cos θ + i sin θ ) = [ cos ( k θ ) + i sin ( k θ ) ] ⋅ [ cos θ + i sin θ ] = cos ( k θ ) cos θ − sin ( k θ ) sin θ + i [ cos ( k θ ) sin θ + sin ( k θ ) cos θ ] = cos ( ( k + 1 ) θ ) + i sin ( ( k + 1 ) θ ) \begin{aligned} (\cos\theta + i\sin\theta)^{k+1} &= (\cos\theta + i\sin\theta)^k \cdot (\cos\theta + i\sin\theta) \\ &= [\cos(k\theta) + i\sin(k\theta)] \cdot [\cos\theta + i\sin\theta] \\ &= \cos(k\theta)\cos\theta - \sin(k\theta)\sin\theta + i\,[\cos(k\theta)\sin\theta + \sin(k\theta)\cos\theta] \\ &= \cos((k+1)\theta) + i\sin((k+1)\theta) \end{aligned} ( cos θ + i sin θ ) k + 1 = ( cos θ + i sin θ ) k ⋅ ( cos θ + i sin θ ) = [ cos ( k θ ) + i sin ( k θ )] ⋅ [ cos θ + i sin θ ] = cos ( k θ ) cos θ − sin ( k θ ) sin θ + i [ cos ( k θ ) sin θ + sin ( k θ ) cos θ ] = cos (( k + 1 ) θ ) + i sin (( k + 1 ) θ ) Using the compound angle identities. ✓
For negative integers, note that 1 cos θ + i sin θ = cos θ − i sin θ = cos ( − θ ) + i sin ( − θ ) \dfrac{1}{\cos\theta + i\sin\theta} = \cos\theta - i\sin\theta = \cos(-\theta) + i\sin(-\theta) cos θ + i sin θ 1 = cos θ − i sin θ = cos ( − θ ) + i sin ( − θ ) So the result follows. □ \square □
Intuition. De Moivre’s theorem says that raising a complex number on the unit circle to the n n n -th power multiplies its angle by n n n . This is because multiplication of complex numbers Adds their arguments: r 1 e i θ 1 ⋅ r 2 e i θ 2 = r 1 r 2 e i ( θ 1 + θ 2 ) r_1 e^{i\theta_1} \cdot r_2 e^{i\theta_2} = r_1 r_2 e^{i(\theta_1 + \theta_2)} r 1 e i θ 1 ⋅ r 2 e i θ 2 = r 1 r 2 e i ( θ 1 + θ 2 ) .
De Moivre’s theorem provides a systematic way to derive multiple-angle identities.
Example. Express cos 3 θ \cos 3\theta cos 3 θ and sin 3 θ \sin 3\theta sin 3 θ in terms of cos θ \cos\theta cos θ and sin θ \sin\theta sin θ .
By De Moivre: cos 3 θ + i sin 3 θ = ( cos θ + i sin θ ) 3 \cos 3\theta + i\sin 3\theta = (\cos\theta + i\sin\theta)^3 cos 3 θ + i sin 3 θ = ( cos θ + i sin θ ) 3 .
Expanding the RHS using the binomial theorem:
( cos θ + i sin θ ) 3 = cos 3 θ + 3 i cos 2 θ sin θ − 3 cos θ sin 2 θ − i sin 3 θ \begin{aligned} (\cos\theta + i\sin\theta)^3 &= \cos^3\theta + 3i\cos^2\theta\sin\theta - 3\cos\theta\sin^2\theta - i\sin^3\theta \end{aligned} ( cos θ + i sin θ ) 3 = cos 3 θ + 3 i cos 2 θ sin θ − 3 cos θ sin 2 θ − i sin 3 θ Equating real and imaginary parts:
cos 3 θ = 4 cos 3 θ − 3 cos θ \boxed{\cos 3\theta = 4\cos^3\theta - 3\cos\theta} cos 3 θ = 4 cos 3 θ − 3 cos θ
sin 3 θ = 3 sin θ − 4 sin 3 θ \boxed{\sin 3\theta = 3\sin\theta - 4\sin^3\theta} sin 3 θ = 3 sin θ − 4 sin 3 θ
To compute z n z^n z n where z = r ( cos θ + i sin θ ) z = r(\cos\theta + i\sin\theta) z = r ( cos θ + i sin θ ) :
z n = r n ( cos ( n θ ) + i sin ( n θ ) ) z^n = r^n\left(\cos(n\theta) + i\sin(n\theta)\right) z n = r n ( cos ( n θ ) + i sin ( n θ ) )
Worked Example: Computing a high power Find ( 1 + i ) 10 (1 + i)^{10} ( 1 + i ) 10 .
First write in polar form: 1 + i = 2 ( cos π 4 + i sin π 4 ) 1 + i = \sqrt{2}\!\left(\cos\frac{\pi}{4} + i\sin\frac{\pi}{4}\right) 1 + i = 2 ( cos 4 π + i sin 4 π ) .
( 1 + i ) 10 = ( 2 ) 10 ( cos 10 π 4 + i sin 10 π 4 ) = 32 ( cos 5 π 2 + i sin 5 π 2 ) = 32 ( cos π 2 + i sin π 2 ) = 32 ( 0 + i ) = 32 i \begin{aligned} (1 + i)^{10} &= \left(\sqrt{2}\right)^{10}\!\left(\cos\frac{10\pi}{4} + i\sin\frac{10\pi}{4}\right) \\ &= 32\!\left(\cos\frac{5\pi}{2} + i\sin\frac{5\pi}{2}\right) \\ &= 32\!\left(\cos\frac{\pi}{2} + i\sin\frac{\pi}{2}\right) \\ &= 32(0 + i) = 32i \end{aligned} ( 1 + i ) 10 = ( 2 ) 10 ( cos 4 10 π + i sin 4 10 π ) = 32 ( cos 2 5 π + i sin 2 5 π ) = 32 ( cos 2 π + i sin 2 π ) = 32 ( 0 + i ) = 32 i Definition. The n n n -th roots of unity are the solutions to the equation z n = 1 z^n = 1 z n = 1 for n ∈ Z + n \in \mathbb{Z}^+ n ∈ Z + .
By De Moivre’s theorem, writing 1 = cos 0 + i sin 0 = cos ( 2 k π ) + i sin ( 2 k π ) 1 = \cos 0 + i\sin 0 = \cos(2k\pi) + i\sin(2k\pi) 1 = cos 0 + i sin 0 = cos ( 2 k π ) + i sin ( 2 k π ) for any integer k k k The n n n distinct solutions are:
z k = cos ( 2 k π n ) + i sin ( 2 k π n ) , k = 0 , 1 , 2 , … , n − 1 \boxed{z_k = \cos\!\left(\frac{2k\pi}{n}\right) + i\sin\!\left(\frac{2k\pi}{n}\right), \quad k = 0, 1, 2, \ldots, n-1} z k = cos ( n 2 k π ) + i sin ( n 2 k π ) , k = 0 , 1 , 2 , … , n − 1
The n n n -th roots of unity lie on the unit circle ∣ z ∣ = 1 |z| = 1 ∣ z ∣ = 1 in the Argand diagram, equally spaced at Angles of 2 π n \dfrac{2\pi}{n} n 2 π radians apart. They form the vertices of a regular n n n -gon Inscribed in the unit circle, with one vertex at z = 1 z = 1 z = 1 .
Since the roots satisfy z n − 1 = 0 z^n - 1 = 0 z n − 1 = 0 The sum of all n n n -th roots of unity is zero:
∑ k = 0 n − 1 z k = 0 \sum_{k=0}^{n-1} z_k = 0 ∑ k = 0 n − 1 z k = 0
This follows from the coefficient of z n − 1 z^{n-1} z n − 1 in z n − 1 = 0 z^n - 1 = 0 z n − 1 = 0 being zero (by Vieta’s formulas). Equivalently, the roots form a geometric series with ratio ω = e 2 π i / n \omega = e^{2\pi i/n} ω = e 2 π i / n and first term 1, Giving:
∑ k = 0 n − 1 ω k = 1 − ω n 1 − ω = 1 − 1 1 − ω = 0 \sum_{k=0}^{n-1} \omega^k = \frac{1 - \omega^n}{1 - \omega} = \frac{1 - 1}{1 - \omega} = 0 ∑ k = 0 n − 1 ω k = 1 − ω 1 − ω n = 1 − ω 1 − 1 = 0
The product of all n n n -th roots of unity is:
∏ k = 0 n − 1 z k = ( − 1 ) n − 1 \prod_{k=0}^{n-1} z_k = (-1)^{n-1} ∏ k = 0 n − 1 z k = ( − 1 ) n − 1
Worked Example: Cube roots of unity Find all cube roots of unity and verify that their sum is zero.
z 3 = 1 ⟹ z k = cos ( 2 k π 3 ) + i sin ( 2 k π 3 ) z^3 = 1 \implies z_k = \cos\!\left(\dfrac{2k\pi}{3}\right) + i\sin\!\left(\dfrac{2k\pi}{3}\right) z 3 = 1 ⟹ z k = cos ( 3 2 k π ) + i sin ( 3 2 k π ) For k = 0 , 1 , 2 k = 0, 1, 2 k = 0 , 1 , 2 .
Z 0 = cos 0 + i sin 0 = 1 Z 1 = cos 2 π 3 + i sin 2 π 3 = − 1 2 + 3 2 i Z 2 = cos 4 π 3 + i sin 4 π 3 = − 1 2 − 3 2 i \begin{aligned} Z_0 &= \cos 0 + i\sin 0 = 1 \\ Z_1 &= \cos\frac{2\pi}{3} + i\sin\frac{2\pi}{3} = -\frac{1}{2} + \frac{\sqrt{3}}{2}\,i \\ Z_2 &= \cos\frac{4\pi}{3} + i\sin\frac{4\pi}{3} = -\frac{1}{2} - \frac{\sqrt{3}}{2}\,i \end{aligned} Z 0 Z 1 Z 2 = cos 0 + i sin 0 = 1 = cos 3 2 π + i sin 3 2 π = − 2 1 + 2 3 i = cos 3 4 π + i sin 3 4 π = − 2 1 − 2 3 i Sum: 1 − 1 2 + 3 2 i − 1 2 − 3 2 i = 0 1 - \dfrac{1}{2} + \dfrac{\sqrt{3}}{2}\,i - \dfrac{1}{2} - \dfrac{\sqrt{3}}{2}\,i = 0 1 − 2 1 + 2 3 i − 2 1 − 2 3 i = 0 . ✓
Product: 1 ⋅ ( − 1 2 + 3 2 i ) ( − 1 2 − 3 2 i ) = 1 ⋅ ( 1 4 + 3 4 ) = 1 = ( − 1 ) 3 − 1 1 \cdot \left(-\dfrac{1}{2} + \dfrac{\sqrt{3}}{2}\,i\right)\left(-\dfrac{1}{2} - \dfrac{\sqrt{3}}{2}\,i\right) = 1 \cdot \left(\dfrac{1}{4} + \dfrac{3}{4}\right) = 1 = (-1)^{3-1} 1 ⋅ ( − 2 1 + 2 3 i ) ( − 2 1 − 2 3 i ) = 1 ⋅ ( 4 1 + 4 3 ) = 1 = ( − 1 ) 3 − 1 . ✓
Definition. The exponential form of a complex number z = r ( cos θ + i sin θ ) z = r(\cos\theta + i\sin\theta) z = r ( cos θ + i sin θ ) is:
z = r e i θ \boxed{z = re^{i\theta}} z = r e i θ
Where e i θ ≡ cos θ + i sin θ e^{i\theta} \equiv \cos\theta + i\sin\theta e i θ ≡ cos θ + i sin θ by Euler’s formula.
The Maclaurin series for e x e^x e x , cos x \cos x cos x And sin x \sin x sin x are:
e x = ∑ n = 0 ∞ x n n ! = 1 + x + x 2 2 ! + x 3 3 ! + x 4 4 ! + ⋯ e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!} = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \cdots e x = ∑ n = 0 ∞ n ! x n = 1 + x + 2 ! x 2 + 3 ! x 3 + 4 ! x 4 + ⋯
cos x = ∑ n = 0 ∞ ( − 1 ) n x 2 n ( 2 n ) ! = 1 − x 2 2 ! + x 4 4 ! − x 6 6 ! + ⋯ \cos x = \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n}}{(2n)!} = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \frac{x^6}{6!} + \cdots cos x = ∑ n = 0 ∞ ( 2 n )! ( − 1 ) n x 2 n = 1 − 2 ! x 2 + 4 ! x 4 − 6 ! x 6 + ⋯
sin x = ∑ n = 0 ∞ ( − 1 ) n x 2 n + 1 ( 2 n + 1 ) ! = x − x 3 3 ! + x 5 5 ! − x 7 7 ! + ⋯ \sin x = \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{(2n+1)!} = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \frac{x^7}{7!} + \cdots sin x = ∑ n = 0 ∞ ( 2 n + 1 )! ( − 1 ) n x 2 n + 1 = x − 3 ! x 3 + 5 ! x 5 − 7 ! x 7 + ⋯
Substituting x = i θ x = i\theta x = i θ into the series for e x e^x e x :
E i θ = 1 + i θ + ( i θ ) 2 2 ! + ( i θ ) 3 3 ! + ( i θ ) 4 4 ! + ( i θ ) 5 5 ! + ⋯ = 1 + i θ + i 2 θ 2 2 ! + i 3 θ 3 3 ! + i 4 θ 4 4 ! + i 5 θ 5 5 ! + ⋯ = 1 + i θ − θ 2 2 ! − i θ 3 3 ! + θ 4 4 ! + i θ 5 5 ! − ⋯ \begin{aligned} E^{i\theta} &= 1 + i\theta + \frac{(i\theta)^2}{2!} + \frac{(i\theta)^3}{3!} + \frac{(i\theta)^4}{4!} + \frac{(i\theta)^5}{5!} + \cdots \\ &= 1 + i\theta + \frac{i^2\theta^2}{2!} + \frac{i^3\theta^3}{3!} + \frac{i^4\theta^4}{4!} + \frac{i^5\theta^5}{5!} + \cdots \\ &= 1 + i\theta - \frac{\theta^2}{2!} - \frac{i\theta^3}{3!} + \frac{\theta^4}{4!} + \frac{i\theta^5}{5!} - \cdots \end{aligned} E i θ = 1 + i θ + 2 ! ( i θ ) 2 + 3 ! ( i θ ) 3 + 4 ! ( i θ ) 4 + 5 ! ( i θ ) 5 + ⋯ = 1 + i θ + 2 ! i 2 θ 2 + 3 ! i 3 θ 3 + 4 ! i 4 θ 4 + 5 ! i 5 θ 5 + ⋯ = 1 + i θ − 2 ! θ 2 − 3 ! i θ 3 + 4 ! θ 4 + 5 ! i θ 5 − ⋯ Using i^2 = -1$$i^3 = -i$$i^4 = 1$$i^5 = i And so on. Grouping real and imaginary parts:
e i θ = ( 1 − θ 2 2 ! + θ 4 4 ! − ⋯ ) ⏟ = cos θ + i ( θ − θ 3 3 ! + θ 5 5 ! − ⋯ ) ⏟ = sin θ e^{i\theta} = \underbrace{\left(1 - \frac{\theta^2}{2!} + \frac{\theta^4}{4!} - \cdots\right)}_{=\,\cos\theta} + i\underbrace{\left(\theta - \frac{\theta^3}{3!} + \frac{\theta^5}{5!} - \cdots\right)}_{=\,\sin\theta} e i θ = = c o s θ ( 1 − 2 ! θ 2 + 4 ! θ 4 − ⋯ ) + i = s i n θ ( θ − 3 ! θ 3 + 5 ! θ 5 − ⋯ )
Therefore e i θ = cos θ + i sin θ e^{i\theta} = \cos\theta + i\sin\theta e i θ = cos θ + i sin θ . □ \square □
Setting θ = π \theta = \pi θ = π :
e i π + 1 = 0 \boxed{e^{i\pi} + 1 = 0} e iπ + 1 = 0
This celebrated identity connects five fundamental constants: e$$i$$\pi$$1 And 0 0 0 .
Intuition. Euler’s identity says that starting at the point 1 1 1 on the real axis and rotating by π \pi π radians (half a turn) on the unit circle lands you at − 1 -1 − 1 . The exponential e i θ e^{i\theta} e i θ Describes a point moving around the unit circle at a rate determined by θ \theta θ .
The standard laws of indices extend :
Z 1 z 2 = r 1 r 2 e i ( θ 1 + θ 2 ) ( a r g u m e n t s a d d ) z 1 z 2 = r 1 r 2 e i ( θ 1 − θ 2 ) ( a r g u m e n t s s u b t r a c t ) Z n = r n e i n θ ( a r g u m e n t m u l t i p l i e s ) \begin{aligned} Z_1 z_2 &= r_1 r_2 \, e^{i(\theta_1 + \theta_2)} & &\mathrm{(arguments add)} \\ \frac{z_1}{z_2} &= \frac{r_1}{r_2} \, e^{i(\theta_1 - \theta_2)} & &\mathrm{(arguments subtract)} \\ Z^n &= r^n e^{in\theta} & &\mathrm{(argument multiplies)} \end{aligned} Z 1 z 2 z 2 z 1 Z n = r 1 r 2 e i ( θ 1 + θ 2 ) = r 2 r 1 e i ( θ 1 − θ 2 ) = r n e in θ ( argumentsadd ) ( argumentssubtract ) ( argumentmultiplies ) Info: info with the cos θ + i sin θ \cos\theta + i\sin\theta cos θ + i sin θ form. All boards require De Moivre’s theorem.
Definition. The locus ∣ z − a ∣ = r |z - a| = r ∣ z − a ∣ = r Where a ∈ C a \in \mathbb{C} a ∈ C and r ∈ R + r \in \mathbb{R}^+ r ∈ R + Is a Circle with centre a a a and radius r r r in the Argand diagram.
∣ z − a ∣ = r ⟺ ( x − α ) 2 + ( y − β ) 2 = r ⟺ ( x − α ) 2 + ( y − β ) 2 = r 2 |z - a| = r \iff \sqrt{(x - \alpha)^2 + (y - \beta)^2} = r \iff (x - \alpha)^2 + (y - \beta)^2 = r^2 ∣ z − a ∣ = r ⟺ ( x − α ) 2 + ( y − β ) 2 = r ⟺ ( x − α ) 2 + ( y − β ) 2 = r 2
Where a = α + β i a = \alpha + \beta i a = α + β i and z = x + y i z = x + yi z = x + y i .
The region ∣ z − a ∣ < r |z - a| < r ∣ z − a ∣ < r is the interior of the circle, and ∣ z − a ∣ > r |z - a| > r ∣ z − a ∣ > r is the exterior .
This locus represents all points equidistant from a a a and b b b Which is the perpendicular bisector Of the line segment joining a a a and b b b .
Definition. The locus arg ( z − a ) = α \arg(z - a) = \alpha arg ( z − a ) = α is a half-line (ray) starting from the point a a a (not including a a a itself) making an angle α \alpha α with the positive real direction.
The region α 1 < arg ( z − a ) < α 2 \alpha_1 < \arg(z - a) < \alpha_2 α 1 < arg ( z − a ) < α 2 is an angular sector (wedge) with vertex at a a a .
Exam questions often require describing a region defined by combining loci, such as:
∣ z − 3 ∣ ≤ 2 |z - 3| \leq 2 ∣ z − 3∣ ≤ 2 and arg ( z ) ≥ π 4 \arg(z) \geq \dfrac{\pi}{4} arg ( z ) ≥ 4 π : the part of a disc in a sector.Regions, be careful about whether boundaries are included (solid line) or excluded (dashed line). Common exam technique: identify the boundary (circle, line, half-line), then determine which side of The boundary is included by testing a point. Worked Example: Describing a locus algebraically A complex number z z z satisfies ∣ z − 2 i ∣ ≤ 3 |z - 2i| \leq 3 ∣ z − 2 i ∣ ≤ 3 and 0 ≤ arg ( z ) ≤ π 2 0 \leq \arg(z) \leq \dfrac{\pi}{2} 0 ≤ arg ( z ) ≤ 2 π . Find the greatest possible value of ∣ z ∣ |z| ∣ z ∣ and the Least possible value of ∣ z ∣ |z| ∣ z ∣ .
The first condition: ∣ z − 2 i ∣ ≤ 3 |z - 2i| \leq 3 ∣ z − 2 i ∣ ≤ 3 is the closed disc of radius 3 centred at 2 i 2i 2 i I.e. At ( 0 , 2 ) (0, 2) ( 0 , 2 ) .
The second condition: 0 ≤ arg ( z ) ≤ π 2 0 \leq \arg(z) \leq \dfrac{\pi}{2} 0 ≤ arg ( z ) ≤ 2 π restricts z z z to the first Quadrant (including axes).
The disc centre ( 0 , 2 ) (0, 2) ( 0 , 2 ) with radius 3 extends from y = − 1 y = -1 y = − 1 to y = 5 y = 5 y = 5 and from x = − 3 x = -3 x = − 3 to x = 3 x = 3 x = 3 .
Greatest ∣ z ∣ |z| ∣ z ∣ : The point in the region farthest from the origin is where the boundary of the Disc intersects the first quadrant boundary furthest from the origin. The disc intersects the Positive y y y -axis at ( 0 , 5 ) (0, 5) ( 0 , 5 ) Giving ∣ z ∣ = 5 |z| = 5 ∣ z ∣ = 5 .
Least ∣ z ∣ |z| ∣ z ∣ : We need the closest point in the region to the origin. The disc boundary is ( x 2 + ( y − 2 ) 2 ) = 9 (x^2 + (y-2)^2) = 9 ( x 2 + ( y − 2 ) 2 ) = 9 . The closest point on this circle to the origin lies along the line from the Origin through the centre ( 0 , 2 ) (0,2) ( 0 , 2 ) Which is the y y y -axis. The point ( 0 , − 1 ) (0, -1) ( 0 , − 1 ) is outside the first Quadrant. Within the first quadrant, the closest point is where the circle meets the x x x -axis: Setting y = 0 y = 0 y = 0 , x 2 + 4 = 9 ⟹ x = 5 x^2 + 4 = 9 \implies x = \sqrt{5} x 2 + 4 = 9 ⟹ x = 5 . So ∣ z ∣ = 5 |z| = \sqrt{5} ∣ z ∣ = 5 .
A complex transformation is a function w = f ( z ) w = f(z) w = f ( z ) that maps points in the z z z -plane (Argand diagram For z z z ) to points in the w w w -plane (Argand diagram for w w w ).
For w = a z + b w = az + b w = a z + b where a , b ∈ C a, b \in \mathbb{C} a , b ∈ C and a ≠ 0 a \neq 0 a = 0 :
Writing a = λ e i α a = \lambda e^{i\alpha} a = λ e i α and b = μ e i β b = \mu e^{i\beta} b = μ e i β :
∣ a ∣ = λ |a| = \lambda ∣ a ∣ = λ produces an enlargement (scale factor λ \lambda λ ) about the origin.arg ( a ) = α \arg(a) = \alpha arg ( a ) = α produces a rotation through angle α \alpha α about the origin.b b b produces a translation by the vector representing b b b .The composition is: enlarge by ∣ a ∣ |a| ∣ a ∣ Rotate by arg ( a ) \arg(a) arg ( a ) Then translate by b b b .
The transformation w = 1 z w = \dfrac{1}{z} w = z 1 maps:
Circles not through the origin to circles. Circles through the origin to straight lines not through the origin. Straight lines through the origin to straight lines through the origin. Straight lines not through the origin to circles through the origin. These are common in exam questions. The general approach is:
Express z z z in terms of w w w : z = f − 1 ( w ) z = f^{-1}(w) z = f − 1 ( w ) . Apply the given condition on z z z (e.g. ∣ z ∣ = 2 |z| = 2 ∣ z ∣ = 2 ) to find the locus of w w w . Critical points. A critical point of a transformation w = f ( z ) w = f(z) w = f ( z ) is a point z 0 z_0 z 0 where f ′ ( z 0 ) = 0 f'(z_0) = 0 f ′ ( z 0 ) = 0 . At a critical point, the mapping is not conformal (angles are not preserved).
Worked Example: Image of a line under inversion Find the image of the line Re ( z ) = 1 \operatorname{Re}(z) = 1 Re ( z ) = 1 under the transformation w = 1 z w = \dfrac{1}{z} w = z 1 .
Let z = x + y i z = x + yi z = x + y i with x = 1 x = 1 x = 1 So z = 1 + y i z = 1 + yi z = 1 + y i and y ∈ R y \in \mathbb{R} y ∈ R .
w = 1 1 + y i = 1 − y i 1 + y 2 = 1 1 + y 2 − y 1 + y 2 i w = \frac{1}{1 + yi} = \frac{1 - yi}{1 + y^2} = \frac{1}{1 + y^2} - \frac{y}{1 + y^2}\,i w = 1 + y i 1 = 1 + y 2 1 − y i = 1 + y 2 1 − 1 + y 2 y i
Let w = u + v i w = u + vi w = u + v i . Then u = 1 1 + y 2 u = \dfrac{1}{1 + y^2} u = 1 + y 2 1 and v = − y 1 + y 2 v = \dfrac{-y}{1 + y^2} v = 1 + y 2 − y .
Note that v = − u y v = -uy v = − u y So y = − v u y = -\dfrac{v}{u} y = − u v (when u ≠ 0 u \neq 0 u = 0 ).
Substituting: u = 1 1 + v 2 / u 2 = u 2 u 2 + v 2 u = \dfrac{1}{1 + v^2/u^2} = \dfrac{u^2}{u^2 + v^2} u = 1 + v 2 / u 2 1 = u 2 + v 2 u 2 Giving u 2 + v 2 = u u^2 + v^2 = u u 2 + v 2 = u I.e.:
u 2 − u + v 2 = 0 ⟹ ( u − 1 2 ) 2 + v 2 = 1 4 u^2 - u + v^2 = 0 \implies \left(u - \frac{1}{2}\right)^2 + v^2 = \frac{1}{4} u 2 − u + v 2 = 0 ⟹ ( u − 2 1 ) 2 + v 2 = 4 1
This is a circle with centre ( 1 2 , 0 ) \left(\dfrac{1}{2}, 0\right) ( 2 1 , 0 ) and radius 1 2 \dfrac{1}{2} 2 1 in the w w w -plane.
Edexcel and OCR cover this topic with less depth. CIE focuses more on loci than on transformations. ( cos θ + i sin θ ) n = cos ( n θ ) + i sin ( n θ ) \boxed{(\cos\theta + i\sin\theta)^n = \cos(n\theta) + i\sin(n\theta)} ( cos θ + i sin θ ) n = cos ( n θ ) + i sin ( n θ )
e i θ = cos θ + i sin θ \boxed{e^{i\theta} = \cos\theta + i\sin\theta} e i θ = cos θ + i sin θ
e i π + 1 = 0 \boxed{e^{i\pi} + 1 = 0} e iπ + 1 = 0
z k = e 2 k π i / n = cos ( 2 k π n ) + i sin ( 2 k π n ) , k = 0 , 1 , … , n − 1 \boxed{z_k = e^{2k\pi i/n} = \cos\!\left(\frac{2k\pi}{n}\right) + i\sin\!\left(\frac{2k\pi}{n}\right), \quad k = 0, 1, \ldots, n-1} z k = e 2 k π i / n = cos ( n 2 k π ) + i sin ( n 2 k π ) , k = 0 , 1 , … , n − 1
∑ k = 0 n − 1 z k = 0 \boxed{\sum_{k=0}^{n-1} z_k = 0} k = 0 ∑ n − 1 z k = 0
∣ z − a ∣ = r ⟺ c i r c l e c e n t r e a r a d i u s r \boxed{|z - a| = r \iff \mathrm{circle centre } a \mathrm{ radius } r} ∣ z − a ∣ = r ⟺ circlecentre a radius r
arg ( z − a ) = α ⟺ h a l f − l i n e f r o m a a t a n g l e α \boxed{\arg(z - a) = \alpha \iff \mathrm{half-line from } a \mathrm{ at angle } \alpha} arg ( z − a ) = α ⟺ half − linefrom a atangle α
Problem 1. Express z = − 3 + i z = -\sqrt{3} + i z = − 3 + i in modulus-argument form and hence find z 5 z^5 z 5 in the form a + b i a + bi a + bi .
Hint Find ∣ z ∣ |z| ∣ z ∣ and arg ( z ) \arg(z) arg ( z ) first. Then apply De Moivre’s theorem.
Answer ∣ z ∣ = 3 + 1 = 2 |z| = \sqrt{3 + 1} = 2 ∣ z ∣ = 3 + 1 = 2 .
The point ( − 3 , 1 ) (-\sqrt{3}, 1) ( − 3 , 1 ) is in the second quadrant. arg ( z ) = π − arctan ( 1 3 ) = π − π 6 = 5 π 6 \arg(z) = \pi - \arctan\!\left(\dfrac{1}{\sqrt{3}}\right) = \pi - \dfrac{\pi}{6} = \dfrac{5\pi}{6} arg ( z ) = π − arctan ( 3 1 ) = π − 6 π = 6 5 π .
z 5 = 2 5 ( cos 25 π 6 + i sin 25 π 6 ) = 32 ( cos π 6 + i sin π 6 ) = 32 ( 3 2 + 1 2 i ) = 16 3 + 16 i z^5 = 2^5\!\left(\cos\frac{25\pi}{6} + i\sin\frac{25\pi}{6}\right) = 32\!\left(\cos\frac{\pi}{6} + i\sin\frac{\pi}{6}\right) = 32\!\left(\frac{\sqrt{3}}{2} + \frac{1}{2}\,i\right) = 16\sqrt{3} + 16i z 5 = 2 5 ( cos 6 25 π + i sin 6 25 π ) = 32 ( cos 6 π + i sin 6 π ) = 32 ( 2 3 + 2 1 i ) = 16 3 + 16 i
Problem 2. Use De Moivre’s theorem to prove that cos 4 θ = 8 cos 4 θ − 8 cos 2 θ + 1 \cos 4\theta = 8\cos^4\theta - 8\cos^2\theta + 1 cos 4 θ = 8 cos 4 θ − 8 cos 2 θ + 1 .
Hint Expand ( cos θ + i sin θ ) 4 (\cos\theta + i\sin\theta)^4 ( cos θ + i sin θ ) 4 using the binomial theorem and equate real parts.
Answer cos 4 θ + i sin 4 θ = ( cos θ + i sin θ ) 4 \cos 4\theta + i\sin 4\theta = (\cos\theta + i\sin\theta)^4 cos 4 θ + i sin 4 θ = ( cos θ + i sin θ ) 4 .
Expanding: cos 4 θ + 4 i cos 3 θ sin θ − 6 cos 2 θ sin 2 θ − 4 i cos θ sin 3 θ + sin 4 θ \cos^4\theta + 4i\cos^3\theta\sin\theta - 6\cos^2\theta\sin^2\theta - 4i\cos\theta\sin^3\theta + \sin^4\theta cos 4 θ + 4 i cos 3 θ sin θ − 6 cos 2 θ sin 2 θ − 4 i cos θ sin 3 θ + sin 4 θ .
Real part: cos 4 θ = cos 4 θ − 6 cos 2 θ sin 2 θ + sin 4 θ \cos 4\theta = \cos^4\theta - 6\cos^2\theta\sin^2\theta + \sin^4\theta cos 4 θ = cos 4 θ − 6 cos 2 θ sin 2 θ + sin 4 θ .
Using sin 2 θ = 1 − cos 2 θ \sin^2\theta = 1 - \cos^2\theta sin 2 θ = 1 − cos 2 θ :
cos 4 θ = cos 4 θ − 6 cos 2 θ ( 1 − cos 2 θ ) + ( 1 − cos 2 θ ) 2 = cos 4 θ − 6 cos 2 θ + 6 cos 4 θ + 1 − 2 cos 2 θ + cos 4 θ = 8 cos 4 θ − 8 cos 2 θ + 1 □ \begin{aligned} \cos 4\theta &= \cos^4\theta - 6\cos^2\theta(1 - \cos^2\theta) + (1 - \cos^2\theta)^2 \\ &= \cos^4\theta - 6\cos^2\theta + 6\cos^4\theta + 1 - 2\cos^2\theta + \cos^4\theta \\ &= 8\cos^4\theta - 8\cos^2\theta + 1 \quad \square \end{aligned} cos 4 θ = cos 4 θ − 6 cos 2 θ ( 1 − cos 2 θ ) + ( 1 − cos 2 θ ) 2 = cos 4 θ − 6 cos 2 θ + 6 cos 4 θ + 1 − 2 cos 2 θ + cos 4 θ = 8 cos 4 θ − 8 cos 2 θ + 1 □ Problem 3. Find all solutions to z 4 = 16 i z^4 = 16i z 4 = 16 i Expressing each in the form a + b i a + bi a + bi .
Hint Write 16 i = 16 e i π / 2 16i = 16e^{i\pi/2} 16 i = 16 e iπ /2 and use the roots formula.
Answer 16 i = 16 ( cos π 2 + i sin π 2 ) 16i = 16\!\left(\cos\dfrac{\pi}{2} + i\sin\dfrac{\pi}{2}\right) 16 i = 16 ( cos 2 π + i sin 2 π ) .
z k = 2 ( cos ( π / 2 + 2 k π 4 ) + i sin ( π / 2 + 2 k π 4 ) ) , k = 0 , 1 , 2 , 3 z_k = 2\!\left(\cos\!\left(\frac{\pi/2 + 2k\pi}{4}\right) + i\sin\!\left(\frac{\pi/2 + 2k\pi}{4}\right)\right), \quad k = 0, 1, 2, 3 z k = 2 ( cos ( 4 π /2 + 2 k π ) + i sin ( 4 π /2 + 2 k π ) ) , k = 0 , 1 , 2 , 3
K = 0 : z 0 = 2 ( cos π 8 + i sin π 8 ) = 2 ( 2 + 2 2 + i 2 − 2 2 ) = 2 + 2 + i 2 − 2 K = 1 : z 1 = 2 ( cos 5 π 8 + i sin 5 π 8 ) = − 2 − 2 + i 2 + 2 K = 2 : z 2 = 2 ( cos 9 π 8 + i sin 9 π 8 ) = − 2 + 2 − i 2 − 2 K = 3 : z 3 = 2 ( cos 13 π 8 + i sin 13 π 8 ) = 2 − 2 − i 2 + 2 \begin{aligned} K = 0:\quad z_0 &= 2\!\left(\cos\frac{\pi}{8} + i\sin\frac{\pi}{8}\right) = 2\!\left(\frac{\sqrt{2+\sqrt{2}}}{2} + i\,\frac{\sqrt{2-\sqrt{2}}}{2}\right) = \sqrt{2+\sqrt{2}} + i\sqrt{2-\sqrt{2}} \\ K = 1:\quad z_1 &= 2\!\left(\cos\frac{5\pi}{8} + i\sin\frac{5\pi}{8}\right) = -\sqrt{2-\sqrt{2}} + i\sqrt{2+\sqrt{2}} \\ K = 2:\quad z_2 &= 2\!\left(\cos\frac{9\pi}{8} + i\sin\frac{9\pi}{8}\right) = -\sqrt{2+\sqrt{2}} - i\sqrt{2-\sqrt{2}} \\ K = 3:\quad z_3 &= 2\!\left(\cos\frac{13\pi}{8} + i\sin\frac{13\pi}{8}\right) = \sqrt{2-\sqrt{2}} - i\sqrt{2+\sqrt{2}} \end{aligned} K = 0 : z 0 K = 1 : z 1 K = 2 : z 2 K = 3 : z 3 = 2 ( cos 8 π + i sin 8 π ) = 2 ( 2 2 + 2 + i 2 2 − 2 ) = 2 + 2 + i 2 − 2 = 2 ( cos 8 5 π + i sin 8 5 π ) = − 2 − 2 + i 2 + 2 = 2 ( cos 8 9 π + i sin 8 9 π ) = − 2 + 2 − i 2 − 2 = 2 ( cos 8 13 π + i sin 8 13 π ) = 2 − 2 − i 2 + 2 Problem 4. The fifth roots of unity are ω 0 , ω 1 , ω 2 , ω 3 , ω 4 \omega^0, \omega^1, \omega^2, \omega^3, \omega^4 ω 0 , ω 1 , ω 2 , ω 3 , ω 4 where ω = e 2 π i / 5 \omega = e^{2\pi i/5} ω = e 2 π i /5 . Show that 1 + ω + ω 2 + ω 3 + ω 4 = 0 1 + \omega + \omega^2 + \omega^3 + \omega^4 = 0 1 + ω + ω 2 + ω 3 + ω 4 = 0 and deduce that cos 2 π 5 + cos 4 π 5 = − 1 2 \cos\dfrac{2\pi}{5} + \cos\dfrac{4\pi}{5} = -\dfrac{1}{2} cos 5 2 π + cos 5 4 π = − 2 1 .
Hint Sum the geometric series. Then separate real and imaginary parts.
Answer The roots satisfy z 5 − 1 = 0 z^5 - 1 = 0 z 5 − 1 = 0 . The coefficient of z 4 z^4 z 4 is 0, so by Vieta’s formulas, ∑ k = 0 4 ω k = 0 \sum_{k=0}^{4} \omega^k = 0 ∑ k = 0 4 ω k = 0 .
Alternatively: ∑ k = 0 4 ω k = 1 − ω 5 1 − ω = 1 − 1 1 − ω = 0 \displaystyle\sum_{k=0}^{4}\omega^k = \frac{1 - \omega^5}{1 - \omega} = \frac{1 - 1}{1 - \omega} = 0 k = 0 ∑ 4 ω k = 1 − ω 1 − ω 5 = 1 − ω 1 − 1 = 0 .
Expanding using ω k = cos 2 k π 5 + i sin 2 k π 5 \omega^k = \cos\frac{2k\pi}{5} + i\sin\frac{2k\pi}{5} ω k = cos 5 2 k π + i sin 5 2 k π :
∑ k = 0 4 ω k = ∑ k = 0 4 cos 2 k π 5 ⏟ r e a l + i ∑ k = 0 4 sin 2 k π 5 ⏟ i m a g i n a r y = 0 \sum_{k=0}^{4}\omega^k = \underbrace{\sum_{k=0}^{4}\cos\frac{2k\pi}{5}}_{\mathrm{real}} + i\underbrace{\sum_{k=0}^{4}\sin\frac{2k\pi}{5}}_{\mathrm{imaginary}} = 0 ∑ k = 0 4 ω k = real k = 0 ∑ 4 cos 5 2 k π + i imaginary k = 0 ∑ 4 sin 5 2 k π = 0
The imaginary part is zero by symmetry (sin θ = − sin ( 2 π − θ ) \sin\theta = -\sin(2\pi - \theta) sin θ = − sin ( 2 π − θ ) ). The real part gives:
1 + cos 2 π 5 + cos 4 π 5 + cos 6 π 5 + cos 8 π 5 = 0 1 + \cos\frac{2\pi}{5} + \cos\frac{4\pi}{5} + \cos\frac{6\pi}{5} + \cos\frac{8\pi}{5} = 0 1 + cos 5 2 π + cos 5 4 π + cos 5 6 π + cos 5 8 π = 0
Since cos 6 π 5 = cos 4 π 5 \cos\frac{6\pi}{5} = \cos\frac{4\pi}{5} cos 5 6 π = cos 5 4 π and cos 8 π 5 = cos 2 π 5 \cos\frac{8\pi}{5} = \cos\frac{2\pi}{5} cos 5 8 π = cos 5 2 π :
1 + 2 cos 2 π 5 + 2 cos 4 π 5 = 0 ⟹ cos 2 π 5 + cos 4 π 5 = − 1 2 □ 1 + 2\cos\frac{2\pi}{5} + 2\cos\frac{4\pi}{5} = 0 \implies \cos\frac{2\pi}{5} + \cos\frac{4\pi}{5} = -\frac{1}{2} \quad \square 1 + 2 cos 5 2 π + 2 cos 5 4 π = 0 ⟹ cos 5 2 π + cos 5 4 π = − 2 1 □
Problem 5. Sketch on separate Argand diagrams the loci given by (a) ∣ z − 1 − i ∣ = ∣ z − 3 + i ∣ |z - 1 - i| = |z - 3 + i| ∣ z − 1 − i ∣ = ∣ z − 3 + i ∣ And (b) arg ( z − 2 ) = π 3 \arg(z - 2) = \dfrac{\pi}{3} arg ( z − 2 ) = 3 π . Find the complex number(s) satisfying both Conditions simultaneously.
Hint Part (a) is a perpendicular bisector. Part (b) is a half-line. Find their intersection.
Answer (a) ∣ z − ( 1 + i ) ∣ = ∣ z − ( 3 − i ) ∣ |z - (1 + i)| = |z - (3 - i)| ∣ z − ( 1 + i ) ∣ = ∣ z − ( 3 − i ) ∣ is the perpendicular bisector of the segment joining ( 1 , 1 ) (1, 1) ( 1 , 1 ) and ( 3 , − 1 ) (3, -1) ( 3 , − 1 ) . The midpoint is ( 2 , 0 ) (2, 0) ( 2 , 0 ) and the slope of the segment is − 1 − 1 3 − 1 = − 1 \dfrac{-1 - 1}{3 - 1} = -1 3 − 1 − 1 − 1 = − 1 So the perpendicular bisector has slope 1 1 1 and equation y = x − 2 y = x - 2 y = x − 2 .
(b) arg ( z − 2 ) = π 3 \arg(z - 2) = \dfrac{\pi}{3} arg ( z − 2 ) = 3 π is a half-line from ( 2 , 0 ) (2, 0) ( 2 , 0 ) at angle π 3 \dfrac{\pi}{3} 3 π to the positive real axis. Its equation is y = 3 ( x − 2 ) y = \sqrt{3}(x - 2) y = 3 ( x − 2 ) for x > 2 x > 2 x > 2 .
Intersection: Setting x − 2 = 3 ( x − 2 ) x - 2 = \sqrt{3}(x - 2) x − 2 = 3 ( x − 2 ) :
( x − 2 ) ( 1 − 3 ) = 0 (x - 2)(1 - \sqrt{3}) = 0 ( x − 2 ) ( 1 − 3 ) = 0 So x = 2 x = 2 x = 2 (gives y = 0 y = 0 y = 0 But the half-line requires x > 2 x > 2 x > 2 ) or 1 = 3 1 = \sqrt{3} 1 = 3 Which is false.
There is no intersection. The half-line from ( 2 , 0 ) (2, 0) ( 2 , 0 ) at angle π / 3 \pi/3 π /3 has slope 3 \sqrt{3} 3 While The perpendicular bisector has slope 1, and they only meet at the point ( 2 , 0 ) (2, 0) ( 2 , 0 ) which is excluded From the half-line.
Answer: No complex number satisfies both conditions simultaneously.
Problem 6. Find the image of the circle ∣ z ∣ = 2 |z| = 2 ∣ z ∣ = 2 under the transformation w = z + 1 z − 1 w = \dfrac{z + 1}{z - 1} w = z − 1 z + 1 .
Hint Express z z z in terms of w w w and substitute ∣ z ∣ = 2 |z| = 2 ∣ z ∣ = 2 .
Answer w = z + 1 z − 1 ⟹ w z − w = z + 1 ⟹ z ( w − 1 ) = w + 1 ⟹ z = w + 1 w − 1 w = \dfrac{z + 1}{z - 1} \implies wz - w = z + 1 \implies z(w - 1) = w + 1 \implies z = \dfrac{w + 1}{w - 1} w = z − 1 z + 1 ⟹ w z − w = z + 1 ⟹ z ( w − 1 ) = w + 1 ⟹ z = w − 1 w + 1 .
Since ∣ z ∣ = 2 |z| = 2 ∣ z ∣ = 2 :
∣ w + 1 w − 1 ∣ = 2 ⟹ ∣ w + 1 ∣ = 2 ∣ w − 1 ∣ \left|\frac{w + 1}{w - 1}\right| = 2 \implies |w + 1| = 2|w - 1| w − 1 w + 1 = 2 ⟹ ∣ w + 1∣ = 2∣ w − 1∣
Let w = u + v i w = u + vi w = u + v i :
( u + 1 ) 2 + v 2 = 2 ( u − 1 ) 2 + v 2 \sqrt{(u+1)^2 + v^2} = 2\sqrt{(u-1)^2 + v^2} ( u + 1 ) 2 + v 2 = 2 ( u − 1 ) 2 + v 2
Squaring: ( u + 1 ) 2 + v 2 = 4 [ ( u − 1 ) 2 + v 2 ] (u+1)^2 + v^2 = 4[(u-1)^2 + v^2] ( u + 1 ) 2 + v 2 = 4 [( u − 1 ) 2 + v 2 ]
u 2 + 2 u + 1 + v 2 = 4 u 2 − 8 u + 4 + 4 v 2 u^2 + 2u + 1 + v^2 = 4u^2 - 8u + 4 + 4v^2 u 2 + 2 u + 1 + v 2 = 4 u 2 − 8 u + 4 + 4 v 2
0 = 3 u 2 − 10 u + 3 + 3 v 2 0 = 3u^2 - 10u + 3 + 3v^2 0 = 3 u 2 − 10 u + 3 + 3 v 2
3 u 2 − 10 u + 3 v 2 + 3 = 0 3u^2 - 10u + 3v^2 + 3 = 0 3 u 2 − 10 u + 3 v 2 + 3 = 0
3 ( u 2 − 10 3 u ) + 3 v 2 = − 3 3\!\left(u^2 - \frac{10}{3}u\right) + 3v^2 = -3 3 ( u 2 − 3 10 u ) + 3 v 2 = − 3
3 ( u − 5 3 ) 2 − 25 3 + 3 v 2 = − 3 3\!\left(u - \frac{5}{3}\right)^2 - \frac{25}{3} + 3v^2 = -3 3 ( u − 3 5 ) 2 − 3 25 + 3 v 2 = − 3
3 ( u − 5 3 ) 2 + 3 v 2 = 16 3 3\!\left(u - \frac{5}{3}\right)^2 + 3v^2 = \frac{16}{3} 3 ( u − 3 5 ) 2 + 3 v 2 = 3 16
( u − 5 3 ) 2 + v 2 = 16 9 \left(u - \frac{5}{3}\right)^2 + v^2 = \frac{16}{9} ( u − 3 5 ) 2 + v 2 = 9 16
This is a circle with centre ( 5 3 , 0 ) \left(\dfrac{5}{3}, 0\right) ( 3 5 , 0 ) and radius 4 3 \dfrac{4}{3} 3 4 in the w w w -plane.
Problem 7. Express ( 1 + i ) 6 ( 1 − i 3 ) 4 \dfrac{(1+i)^6}{(1-i\sqrt{3})^4} ( 1 − i 3 ) 4 ( 1 + i ) 6 in the form a + b i a + bi a + bi .
Hint Write each term in exponential form and use the laws of indices.
Answer 1 + i = 2 e i π / 4 1 + i = \sqrt{2}\,e^{i\pi/4} 1 + i = 2 e iπ /4 and 1 − i 3 = 2 e − i π / 3 1 - i\sqrt{3} = 2\,e^{-i\pi/3} 1 − i 3 = 2 e − iπ /3 .
( 1 + i ) 6 ( 1 − i 3 ) 4 = ( 2 e i π / 4 ) 6 ( 2 e − i π / 3 ) 4 = 8 e 3 π i / 2 16 e − 4 π i / 3 = 1 2 e i ( 3 π / 2 + 4 π / 3 ) \frac{(1+i)^6}{(1-i\sqrt{3})^4} = \frac{(\sqrt{2}\,e^{i\pi/4})^6}{(2\,e^{-i\pi/3})^4} = \frac{8e^{3\pi i/2}}{16\,e^{-4\pi i/3}} = \frac{1}{2}\,e^{i(3\pi/2 + 4\pi/3)} ( 1 − i 3 ) 4 ( 1 + i ) 6 = ( 2 e − iπ /3 ) 4 ( 2 e iπ /4 ) 6 = 16 e − 4 π i /3 8 e 3 π i /2 = 2 1 e i ( 3 π /2 + 4 π /3 )
3 π / 2 + 4 π / 3 = 9 π + 8 π 6 = 17 π 6 = 2 π + 5 π 6 3\pi/2 + 4\pi/3 = \frac{9\pi + 8\pi}{6} = \frac{17\pi}{6} = 2\pi + \frac{5\pi}{6} 3 π /2 + 4 π /3 = 6 9 π + 8 π = 6 17 π = 2 π + 6 5 π
So: 1 2 e 5 π i / 6 = 1 2 ( cos 5 π 6 + i sin 5 π 6 ) = 1 2 ( − 3 2 + 1 2 i ) = − 3 4 + 1 4 i \dfrac{1}{2}\,e^{5\pi i/6} = \dfrac{1}{2}\!\left(\cos\dfrac{5\pi}{6} + i\sin\dfrac{5\pi}{6}\right) = \dfrac{1}{2}\!\left(-\dfrac{\sqrt{3}}{2} + \dfrac{1}{2}\,i\right) = -\dfrac{\sqrt{3}}{4} + \dfrac{1}{4}\,i 2 1 e 5 π i /6 = 2 1 ( cos 6 5 π + i sin 6 5 π ) = 2 1 ( − 2 3 + 2 1 i ) = − 4 3 + 4 1 i
Problem 8. The transformation T T T from the z z z -plane to the w w w -plane is given by w = z 2 w = z^2 w = z 2 . The Region R R R in the z z z -plane is defined by 1 ≤ ∣ z ∣ ≤ 2 1 \leq |z| \leq 2 1 ≤ ∣ z ∣ ≤ 2 and 0 ≤ arg ( z ) ≤ π 4 0 \leq \arg(z) \leq \dfrac{\pi}{4} 0 ≤ arg ( z ) ≤ 4 π . Find and describe the image of R R R under T T T .
Hint Under w = z 2 w = z^2 w = z 2 The modulus squares and the argument doubles.
Answer If z = r e i θ z = re^{i\theta} z = r e i θ Then w = r 2 e 2 i θ w = r^2 e^{2i\theta} w = r 2 e 2 i θ .
Modulus: 1 ≤ r ≤ 2 ⟹ 1 ≤ r 2 ≤ 4 1 \leq r \leq 2 \implies 1 \leq r^2 \leq 4 1 ≤ r ≤ 2 ⟹ 1 ≤ r 2 ≤ 4 So 1 ≤ ∣ w ∣ ≤ 4 1 \leq |w| \leq 4 1 ≤ ∣ w ∣ ≤ 4 . Argument: 0 ≤ θ ≤ π 4 ⟹ 0 ≤ 2 θ ≤ π 2 0 \leq \theta \leq \dfrac{\pi}{4} \implies 0 \leq 2\theta \leq \dfrac{\pi}{2} 0 ≤ θ ≤ 4 π ⟹ 0 ≤ 2 θ ≤ 2 π so 0 ≤ arg ( w ) ≤ π 2 0 \leq \arg(w) \leq \dfrac{\pi}{2} 0 ≤ arg ( w ) ≤ 2 π . The image is the region in the first quadrant of the w w w -plane between the circles ∣ w ∣ = 1 |w| = 1 ∣ w ∣ = 1 and ∣ w ∣ = 4 |w| = 4 ∣ w ∣ = 4 Bounded by the rays arg ( w ) = 0 \arg(w) = 0 arg ( w ) = 0 and arg ( w ) = π 2 \arg(w) = \dfrac{\pi}{2} arg ( w ) = 2 π .
Problem 9. Solve the equation z 3 + z 2 + z + 1 = 0 z^3 + z^2 + z + 1 = 0 z 3 + z 2 + z + 1 = 0 by recognising it as a geometric series, And hence show that cos 2 π 4 + cos 4 π 4 + cos 6 π 4 = − 1 \cos\dfrac{2\pi}{4} + \cos\dfrac{4\pi}{4} + \cos\dfrac{6\pi}{4} = -1 cos 4 2 π + cos 4 4 π + cos 4 6 π = − 1 .
Hint Factor z 3 + z 2 + z + 1 = ( z + 1 ) ( z 2 + 1 ) z^3 + z^2 + z + 1 = (z+1)(z^2+1) z 3 + z 2 + z + 1 = ( z + 1 ) ( z 2 + 1 ) . The roots are the 4th roots of unity excluding z = 1 z = 1 z = 1 .
Answer z 3 + z 2 + z + 1 = z 4 − 1 z − 1 = 0 ⟹ z 4 = 1 z^3 + z^2 + z + 1 = \dfrac{z^4 - 1}{z - 1} = 0 \implies z^4 = 1 z 3 + z 2 + z + 1 = z − 1 z 4 − 1 = 0 ⟹ z 4 = 1 with z ≠ 1 z \neq 1 z = 1 .
The 4th roots of unity are 1 , i , − 1 , − i 1, i, -1, -i 1 , i , − 1 , − i So the solutions are z = i , − 1 , − i z = i, -1, -i z = i , − 1 , − i .
Equivalently, the roots are e k π i / 2 e^{k\pi i/2} e k π i /2 for k = 1 , 2 , 3 k = 1, 2, 3 k = 1 , 2 , 3 .
The sum of roots (by Vieta, coefficient of z 2 z^2 z 2 divided by leading coefficient) is − 1 -1 − 1 :
i + ( − 1 ) + ( − i ) = − 1 ✓ i + (-1) + (-i) = -1 \quad \checkmark i + ( − 1 ) + ( − i ) = − 1 ✓
Now: e i π / 2 + e i π + e 3 i π / 2 = i + ( − 1 ) + ( − i ) = − 1 e^{i\pi/2} + e^{i\pi} + e^{3i\pi/2} = i + (-1) + (-i) = -1 e iπ /2 + e iπ + e 3 iπ /2 = i + ( − 1 ) + ( − i ) = − 1 .
Separating real and imaginary parts: cos π 2 + cos π + cos 3 π 2 = − 1 \cos\dfrac{\pi}{2} + \cos\pi + \cos\dfrac{3\pi}{2} = -1 cos 2 π + cos π + cos 2 3 π = − 1 I.e. 0 − 1 + 0 = − 1 0 - 1 + 0 = -1 0 − 1 + 0 = − 1 . ✓
Alternatively, the claim as stated uses cos 2 π 4 + cos 4 π 4 + cos 6 π 4 = cos π 2 + cos π + cos 3 π 2 = 0 + ( − 1 ) + 0 = − 1 \cos\dfrac{2\pi}{4} + \cos\dfrac{4\pi}{4} + \cos\dfrac{6\pi}{4} = \cos\dfrac{\pi}{2} + \cos\pi + \cos\dfrac{3\pi}{2} = 0 + (-1) + 0 = -1 cos 4 2 π + cos 4 4 π + cos 4 6 π = cos 2 π + cos π + cos 2 3 π = 0 + ( − 1 ) + 0 = − 1 . ✓ □ \square □
Problem 10. (a) Show that 1 e i θ − 1 = − 1 2 − i 2 cot θ 2 \dfrac{1}{e^{i\theta} - 1} = -\dfrac{1}{2} - \dfrac{i}{2}\cot\dfrac{\theta}{2} e i θ − 1 1 = − 2 1 − 2 i cot 2 θ For θ ∉ 2 π Z \theta \notin 2\pi\mathbb{Z} θ ∈ / 2 π Z .
(b) Hence, or otherwise, find ∑ k = 1 n − 1 1 1 − ω k \displaystyle\sum_{k=1}^{n-1}\frac{1}{1 - \omega^k} k = 1 ∑ n − 1 1 − ω k 1 Where ω = e 2 π i / n \omega = e^{2\pi i/n} ω = e 2 π i / n .
Hint For (a), multiply numerator and denominator by the conjugate e − i θ − 1 e^{-i\theta} - 1 e − i θ − 1 and use half-angle Identities. For (b), use the result from (a) with θ = 2 k π / n \theta = 2k\pi/n θ = 2 k π / n .
Answer (a) 1 e i θ − 1 = e − i θ − 1 ( e i θ − 1 ) ( e − i θ − 1 ) = e − i θ − 1 2 − ( e i θ + e − i θ ) = e − i θ − 1 2 − 2 cos θ \dfrac{1}{e^{i\theta} - 1} = \dfrac{e^{-i\theta} - 1}{(e^{i\theta} - 1)(e^{-i\theta} - 1)} = \dfrac{e^{-i\theta} - 1}{2 - (e^{i\theta} + e^{-i\theta})} = \dfrac{e^{-i\theta} - 1}{2 - 2\cos\theta} e i θ − 1 1 = ( e i θ − 1 ) ( e − i θ − 1 ) e − i θ − 1 = 2 − ( e i θ + e − i θ ) e − i θ − 1 = 2 − 2 cos θ e − i θ − 1 .
Numerator: e − i θ − 1 = cos θ − 1 − i sin θ = − 2 sin 2 θ 2 − 2 i sin θ 2 cos θ 2 = − 2 sin θ 2 ( sin θ 2 + i cos θ 2 ) e^{-i\theta} - 1 = \cos\theta - 1 - i\sin\theta = -2\sin^2\dfrac{\theta}{2} - 2i\sin\dfrac{\theta}{2}\cos\dfrac{\theta}{2} = -2\sin\dfrac{\theta}{2}\!\left(\sin\dfrac{\theta}{2} + i\cos\dfrac{\theta}{2}\right) e − i θ − 1 = cos θ − 1 − i sin θ = − 2 sin 2 2 θ − 2 i sin 2 θ cos 2 θ = − 2 sin 2 θ ( sin 2 θ + i cos 2 θ ) .
Denominator: 2 − 2 cos θ = 4 sin 2 θ 2 2 - 2\cos\theta = 4\sin^2\dfrac{\theta}{2} 2 − 2 cos θ = 4 sin 2 2 θ .
1 e i θ − 1 = − 2 sin θ 2 ( sin θ 2 + i cos θ 2 ) 4 sin 2 θ 2 = − sin θ 2 − i cos θ 2 2 sin θ 2 = − 1 2 − i 2 cot θ 2 □ \frac{1}{e^{i\theta} - 1} = \frac{-2\sin\frac{\theta}{2}\!\left(\sin\frac{\theta}{2} + i\cos\frac{\theta}{2}\right)}{4\sin^2\frac{\theta}{2}} = \frac{-\sin\frac{\theta}{2} - i\cos\frac{\theta}{2}}{2\sin\frac{\theta}{2}} = -\frac{1}{2} - \frac{i}{2}\cot\frac{\theta}{2} \quad \square e i θ − 1 1 = 4 s i n 2 2 θ − 2 s i n 2 θ ( s i n 2 θ + i c o s 2 θ ) = 2 s i n 2 θ − s i n 2 θ − i c o s 2 θ = − 2 1 − 2 i cot 2 θ □
(b) Using (a): 1 1 − ω k = − 1 e 2 k π i / n − 1 = 1 2 + i 2 cot k π n \dfrac{1}{1 - \omega^k} = -\dfrac{1}{e^{2k\pi i/n} - 1} = \dfrac{1}{2} + \dfrac{i}{2}\cot\dfrac{k\pi}{n} 1 − ω k 1 = − e 2 k π i / n − 1 1 = 2 1 + 2 i cot n k π .
∑ k = 1 n − 1 1 1 − ω k = ∑ k = 1 n − 1 ( 1 2 + i 2 cot k π n ) = n − 1 2 + i 2 ∑ k = 1 n − 1 cot k π n \sum_{k=1}^{n-1}\frac{1}{1 - \omega^k} = \sum_{k=1}^{n-1}\!\left(\frac{1}{2} + \frac{i}{2}\cot\frac{k\pi}{n}\right) = \frac{n-1}{2} + \frac{i}{2}\sum_{k=1}^{n-1}\cot\frac{k\pi}{n} ∑ k = 1 n − 1 1 − ω k 1 = ∑ k = 1 n − 1 ( 2 1 + 2 i cot n k π ) = 2 n − 1 + 2 i ∑ k = 1 n − 1 cot n k π
The cotangent sum is zero by symmetry: cot k π n = − cot ( n − k ) π n \cot\dfrac{k\pi}{n} = -\cot\dfrac{(n-k)\pi}{n} cot n k π = − cot n ( n − k ) π So terms cancel in pairs.
Therefore: ∑ k = 1 n − 1 1 1 − ω k = n − 1 2 \displaystyle\sum_{k=1}^{n-1}\frac{1}{1 - \omega^k} = \frac{n - 1}{2} k = 1 ∑ n − 1 1 − ω k 1 = 2 n − 1 .
Problem. Express cos 5 θ \cos 5\theta cos 5 θ in terms of cos θ \cos\theta cos θ .
Solution. By de Moivre: ( cos θ + i sin θ ) 5 = cos 5 θ + i sin 5 θ (\cos\theta + i\sin\theta)^5 = \cos 5\theta + i\sin 5\theta ( cos θ + i sin θ ) 5 = cos 5 θ + i sin 5 θ .
Expanding by the binomial theorem:
( cos θ + i sin θ ) 5 = cos 5 θ + 5 i cos 4 θ sin θ − 10 cos 3 θ sin 2 θ − 10 i cos 2 θ sin 3 θ + 5 cos θ sin 4 θ + i sin 5 θ (\cos\theta + i\sin\theta)^5 = \cos^5\theta + 5i\cos^4\theta\sin\theta - 10\cos^3\theta\sin^2\theta - 10i\cos^2\theta\sin^3\theta + 5\cos\theta\sin^4\theta + i\sin^5\theta ( cos θ + i sin θ ) 5 = cos 5 θ + 5 i cos 4 θ sin θ − 10 cos 3 θ sin 2 θ − 10 i cos 2 θ sin 3 θ + 5 cos θ sin 4 θ + i sin 5 θ
Equating real parts:
cos 5 θ = 16 cos 5 θ − 20 cos 3 θ + 5 cos θ \boxed{\cos 5\theta = 16\cos^5\theta - 20\cos^3\theta + 5\cos\theta} cos 5 θ = 16 cos 5 θ − 20 cos 3 θ + 5 cos θ
Problem. Solve z 6 = − 64 z^6 = -64 z 6 = − 64 Giving answers in exponential form.
Solution. − 64 = 64 e i π -64 = 64e^{i\pi} − 64 = 64 e iπ . The 6th roots are:
z k = 64 1 / 6 exp ( i ( π + 2 k π ) 6 ) = 2 exp ( i ( 2 k + 1 ) π 6 ) z_k = 64^{1/6} \exp\!\left(\frac{i(\pi + 2k\pi)}{6}\right) = 2\exp\!\left(\frac{i(2k+1)\pi}{6}\right) z k = 6 4 1/6 exp ( 6 i ( π + 2 k π ) ) = 2 exp ( 6 i ( 2 k + 1 ) π )
For k = 0 , 1 , 2 , 3 , 4 , 5 k = 0, 1, 2, 3, 4, 5 k = 0 , 1 , 2 , 3 , 4 , 5 .
z_0 = 2e^{i\pi/6}$$z_1 = 2e^{i\pi/2}$$z_2 = 2e^{5i\pi/6}$$z_3 = 2e^{7i\pi/6} z_4 = 2e^{3i\pi/2}$$z_5 = 2e^{11i\pi/6} .
These lie on a circle of radius 2, at angles 30 ° , 90 ° , 150 ° , 210 ° , 270 ° , 330 ° 30°, 90°, 150°, 210°, 270°, 330° 30° , 90° , 150° , 210° , 270° , 330° .
Problem. Find the Cartesian equation of the locus ∣ z − 3 − 4 i ∣ = ∣ z + 1 − 2 i ∣ |z - 3 - 4i| = |z + 1 - 2i| ∣ z − 3 − 4 i ∣ = ∣ z + 1 − 2 i ∣ .
Solution. Let z = x + i y z = x + iy z = x + i y .
∣ z − ( 3 + 4 i ) ∣ = ∣ z − ( − 1 + 2 i ) ∣ |z - (3+4i)| = |z - (-1+2i)| ∣ z − ( 3 + 4 i ) ∣ = ∣ z − ( − 1 + 2 i ) ∣
( x − 3 ) 2 + ( y − 4 ) 2 = ( x + 1 ) 2 + ( y − 2 ) 2 \sqrt{(x-3)^2 + (y-4)^2} = \sqrt{(x+1)^2 + (y-2)^2} ( x − 3 ) 2 + ( y − 4 ) 2 = ( x + 1 ) 2 + ( y − 2 ) 2
Squaring: ( x − 3 ) 2 + ( y − 4 ) 2 = ( x + 1 ) 2 + ( y − 2 ) 2 (x-3)^2 + (y-4)^2 = (x+1)^2 + (y-2)^2 ( x − 3 ) 2 + ( y − 4 ) 2 = ( x + 1 ) 2 + ( y − 2 ) 2 .
x 2 − 6 x + 9 + y 2 − 8 y + 16 = x 2 + 2 x + 1 + y 2 − 4 y + 4 x^2 - 6x + 9 + y^2 - 8y + 16 = x^2 + 2x + 1 + y^2 - 4y + 4 x 2 − 6 x + 9 + y 2 − 8 y + 16 = x 2 + 2 x + 1 + y 2 − 4 y + 4
− 8 x − 4 y + 20 = 0 ⟹ 2 x + y = 5 -8x - 4y + 20 = 0 \implies \boxed{2x + y = 5} − 8 x − 4 y + 20 = 0 ⟹ 2 x + y = 5
This is the perpendicular bisector of the segment joining 3 + 4 i 3+4i 3 + 4 i and − 1 + 2 i -1+2i − 1 + 2 i .
Problem. Shade on an Argand diagram the region defined by ∣ z − 2 i ∣ ≤ 3 |z - 2i| \leq 3 ∣ z − 2 i ∣ ≤ 3 and 0 ≤ arg ( z ) ≤ π 4 0 \leq \arg(z) \leq \dfrac{\pi}{4} 0 ≤ arg ( z ) ≤ 4 π .
Solution. ∣ z − 2 i ∣ ≤ 3 |z - 2i| \leq 3 ∣ z − 2 i ∣ ≤ 3 is the closed disc of radius 3 centred at 2 i 2i 2 i (i.e., ( 0 , 2 ) (0, 2) ( 0 , 2 ) ).
0 ≤ arg ( z ) ≤ π 4 0 \leq \arg(z) \leq \dfrac{\pi}{4} 0 ≤ arg ( z ) ≤ 4 π is the sector between the positive real axis and The line y = x y = x y = x (for x ≥ 0 x \geq 0 x ≥ 0 ).
The required region is the intersection: a segment of the disc in the first quadrant between angles 0 0 0 and π / 4 \pi/4 π /4 .
Problem. The transformation T T T maps the complex plane by w = ( 1 + i ) z + 2 i w = (1+i)z + 2i w = ( 1 + i ) z + 2 i . Describe T T T fully And find the image of the line R e ( z ) = 1 \mathrm{Re}(z) = 1 Re ( z ) = 1 .
Solution. w = ( 1 + i ) z + 2 i = 2 e i π / 4 z + 2 i w = (1+i)z + 2i = \sqrt{2}\,e^{i\pi/4}\,z + 2i w = ( 1 + i ) z + 2 i = 2 e iπ /4 z + 2 i .
T T T is an enlargement by scale factor 2 \sqrt{2} 2 Rotation by 45 ° 45° 45° anticlockwise about the origin, Followed by a translation by 2 i 2i 2 i .
For R e ( z ) = 1 \mathrm{Re}(z) = 1 Re ( z ) = 1 : z = 1 + i t z = 1 + it z = 1 + i t . w = ( 1 + i ) ( 1 + i t ) + 2 i = 1 + i t + i − t + 2 i = ( 1 − t ) + i ( 3 + t ) w = (1+i)(1+it) + 2i = 1 + it + i - t + 2i = (1-t) + i(3+t) w = ( 1 + i ) ( 1 + i t ) + 2 i = 1 + i t + i − t + 2 i = ( 1 − t ) + i ( 3 + t ) .
R e ( w ) = 1 − t \mathrm{Re}(w) = 1-t Re ( w ) = 1 − t , I m ( w ) = 3 + t \mathrm{Im}(w) = 3+t Im ( w ) = 3 + t . Eliminating t t t : I m ( w ) = 3 + ( 1 − R e ( w ) ) = 4 − R e ( w ) \mathrm{Im}(w) = 3 + (1 - \mathrm{Re}(w)) = 4 - \mathrm{Re}(w) Im ( w ) = 3 + ( 1 − Re ( w )) = 4 − Re ( w ) .
The image is the line u + v = 4 \boxed{u + v = 4} u + v = 4 (where w = u + i v w = u + iv w = u + i v ).
Problem. Show that ∑ k = 0 n − 1 ω k = 0 \displaystyle\sum_{k=0}^{n-1} \omega^k = 0 k = 0 ∑ n − 1 ω k = 0 where ω = e 2 π i / n \omega = e^{2\pi i/n} ω = e 2 π i / n .
Solution. This is a geometric series with ratio ω ≠ 1 \omega \neq 1 ω = 1 :
∑ k = 0 n − 1 ω k = 1 − ω n 1 − ω = 1 − 1 1 − ω = 0 \sum_{k=0}^{n-1} \omega^k = \frac{1 - \omega^n}{1 - \omega} = \frac{1 - 1}{1 - \omega} = 0 ∑ k = 0 n − 1 ω k = 1 − ω 1 − ω n = 1 − ω 1 − 1 = 0
■ \blacksquare ■
Problem. Show that the product of all n n n -th roots of unity is ( − 1 ) n + 1 (-1)^{n+1} ( − 1 ) n + 1 .
Solution. The n n n -th roots of unity are the roots of z n − 1 = 0 z^n - 1 = 0 z n − 1 = 0 . By Vieta’s formulae, the Product of all roots is ( − 1 ) n × ( − 1 ) = ( − 1 ) n + 1 (-1)^n \times (-1) = (-1)^{n+1} ( − 1 ) n × ( − 1 ) = ( − 1 ) n + 1 .
Alternatively: the roots are 1 , ω , ω 2 , … , ω n − 1 1, \omega, \omega^2, \ldots, \omega^{n-1} 1 , ω , ω 2 , … , ω n − 1 So the product is ω 0 + 1 + 2 + ⋯ + ( n − 1 ) = ω n ( n − 1 ) / 2 = e π i ( n − 1 ) = ( − 1 ) n − 1 = ( − 1 ) n + 1 \omega^{0+1+2+\cdots+(n-1)} = \omega^{n(n-1)/2} = e^{\pi i(n-1)} = (-1)^{n-1} = (-1)^{n+1} ω 0 + 1 + 2 + ⋯ + ( n − 1 ) = ω n ( n − 1 ) /2 = e π i ( n − 1 ) = ( − 1 ) n − 1 = ( − 1 ) n + 1 . ■ \blacksquare ■
| Pitfall | Correct Approach | | ----------------------------------------------------------------- | ------------------------------------------------------------------------------------------------------------ | -------- | --- | --- | --- | --- | --- | --- | ---------------------------------------- | --- | ---- | --- | --- | --- | --- | | Forgetting that arg ( z ) \arg(z) arg ( z ) is measured from the positive real axis | arg ( z ) \arg(z) arg ( z ) is the angle anticlockwise from the positive x x x -axis, range ( − π , π ] (-\pi, \pi] ( − π , π ] or [ 0 , 2 π ) [0, 2\pi) [ 0 , 2 π ) | | Confusing ∣ z − w ∣ | z-w | ∣ z − w ∣ with ∣ z ∣ − ∣ w ∣ | z | - | w | ∣ z ∣ − ∣ w ∣ | ∣ z − w ∣ | z-w | ∣ z − w ∣ is the distance between z z z and w w w ; ∣ z − w ∣ ≠ ∣ z ∣ − ∣ w ∣ | z-w | \neq | z | - | w | ∣ z − w ∣ = ∣ z ∣ − ∣ w ∣ | | Missing roots when solving z n = w z^n = w z n = w | There are always exactly n n n distinct roots; check your k k k values cover 0 0 0 to n − 1 n-1 n − 1 | | Incorrectly applying de Moivre to non-integer powers | De Moivre’s theorem ( cos θ + i sin θ ) n = cos n θ + i sin n θ (\cos\theta + i\sin\theta)^n = \cos n\theta + i\sin n\theta ( cos θ + i sin θ ) n = cos n θ + i sin n θ holds for integer n n n only |
Solve z 4 = 8 ( 1 + i 3 ) z^4 = 8(1 + i\sqrt{3}) z 4 = 8 ( 1 + i 3 ) Giving roots in the form r ( cos θ + i sin θ ) r(\cos\theta + i\sin\theta) r ( cos θ + i sin θ ) .
Solution 8 ( 1 + i 3 ) = 16 e i π / 3 8(1+i\sqrt{3}) = 16e^{i\pi/3} 8 ( 1 + i 3 ) = 16 e iπ /3 .
z k = 2 exp ( i ( π / 3 + 2 k π ) 4 ) z_k = 2\exp\!\left(\dfrac{i(\pi/3 + 2k\pi)}{4}\right) z k = 2 exp ( 4 i ( π /3 + 2 k π ) ) for k = 0 , 1 , 2 , 3 k = 0, 1, 2, 3 k = 0 , 1 , 2 , 3 .
z 0 = 2 ( cos 15 ° + i sin 15 ° ) z_0 = 2(\cos 15° + i\sin 15°) z 0 = 2 ( cos 15° + i sin 15° ) , z 1 = 2 ( cos 105 ° + i sin 105 ° ) z_1 = 2(\cos 105° + i\sin 105°) z 1 = 2 ( cos 105° + i sin 105° ) z 2 = 2 ( cos 195 ° + i sin 195 ° ) z_2 = 2(\cos 195° + i\sin 195°) z 2 = 2 ( cos 195° + i sin 195° ) , z 3 = 2 ( cos 285 ° + i sin 285 ° ) z_3 = 2(\cos 285° + i\sin 285°) z 3 = 2 ( cos 285° + i sin 285° ) .
Prove that cos 4 θ = 3 8 + 1 2 cos 2 θ + 1 8 cos 4 θ \cos^4\theta = \dfrac{3}{8} + \dfrac{1}{2}\cos 2\theta + \dfrac{1}{8}\cos 4\theta cos 4 θ = 8 3 + 2 1 cos 2 θ + 8 1 cos 4 θ .
Solution cos 2 θ = 1 + cos 2 θ 2 \cos^2\theta = \dfrac{1+\cos 2\theta}{2} cos 2 θ = 2 1 + cos 2 θ .
cos 4 θ = ( 1 + cos 2 θ 2 ) 2 = 1 + 2 cos 2 θ + cos 2 2 θ 4 \cos^4\theta = \left(\dfrac{1+\cos 2\theta}{2}\right)^{\!2} = \dfrac{1 + 2\cos 2\theta + \cos^2 2\theta}{4} cos 4 θ = ( 2 1 + cos 2 θ ) 2 = 4 1 + 2 cos 2 θ + cos 2 2 θ .
cos 2 2 θ = 1 + cos 4 θ 2 \cos^2 2\theta = \dfrac{1+\cos 4\theta}{2} cos 2 2 θ = 2 1 + cos 4 θ .
cos 4 θ = 1 4 + cos 2 θ 2 + 1 + cos 4 θ 8 = 3 8 + cos 2 θ 2 + cos 4 θ 8 \cos^4\theta = \dfrac{1}{4} + \dfrac{\cos 2\theta}{2} + \dfrac{1+\cos 4\theta}{8} = \dfrac{3}{8} + \dfrac{\cos 2\theta}{2} + \dfrac{\cos 4\theta}{8} cos 4 θ = 4 1 + 2 cos 2 θ + 8 1 + cos 4 θ = 8 3 + 2 cos 2 θ + 8 cos 4 θ . ■ \blacksquare ■
The complex number z z z satisfies ∣ z − 1 ∣ = ∣ z + 1 ∣ |z-1| = |z+1| ∣ z − 1∣ = ∣ z + 1∣ and ∣ z − 3 i ∣ = 3 |z-3i| = 3 ∣ z − 3 i ∣ = 3 . Find z z z .
Solution ∣ z − 1 ∣ = ∣ z + 1 ∣ |z-1| = |z+1| ∣ z − 1∣ = ∣ z + 1∣ : perpendicular bisector of 1 1 1 and − 1 -1 − 1 Giving R e ( z ) = 0 \mathrm{Re}(z) = 0 Re ( z ) = 0 . So z = i y z = iy z = i y .
∣ z − 3 i ∣ = 3 ⟹ ∣ i y − 3 i ∣ = 3 ⟹ ∣ y − 3 ∣ = 3 ⟹ y − 3 = ± 3 |z-3i| = 3 \implies |iy - 3i| = 3 \implies |y-3| = 3 \implies y - 3 = \pm 3 ∣ z − 3 i ∣ = 3 ⟹ ∣ i y − 3 i ∣ = 3 ⟹ ∣ y − 3∣ = 3 ⟹ y − 3 = ± 3 .
y = 6 y = 6 y = 6 or y = 0 y = 0 y = 0 . So z = 6 i z = 6i z = 6 i or z = 0 z = 0 z = 0 .
Complex eigenvalues of 2×2 matrices correspond to rotation-scaling transformations. See Matrices .
e i x = cos x + i sin x e^{ix} = \cos x + i\sin x e i x = cos x + i sin x connects exponential, trigonometric, and hyperbolic functions. See Hyperbolic Functions .
Argand diagrams and polar form ( r , θ ) (r, \theta) ( r , θ ) connect to polar coordinates. See Polar Coordinates .
| Result | Formula | | ----------------------------- | --------------------------------------------------------- | --- | -------------------------------- | --- | --- | | Modulus | ∣ z ∣ = a 2 + b 2 | z | = \sqrt{a^2+b^2} ∣ z ∣ = a 2 + b 2 for z = a + b i z = a+bi z = a + bi | | Argument | arg ( z ) = arctan ( b / a ) \arg(z) = \arctan(b/a) arg ( z ) = arctan ( b / a ) (adjusting for quadrant) | | Euler’s formula | e i θ = cos θ + i sin θ e^{i\theta} = \cos\theta+i\sin\theta e i θ = cos θ + i sin θ | | De Moivre | ( cos θ + i sin θ ) n = cos n θ + i sin n θ (\cos\theta+i\sin\theta)^n = \cos n\theta+i\sin n\theta ( cos θ + i sin θ ) n = cos n θ + i sin n θ | | n n n -th roots of unity | z k = e 2 π i k / n z_k = e^{2\pi ik/n} z k = e 2 π ik / n , k = 0 , … , n − 1 k = 0, \ldots, n-1 k = 0 , … , n − 1 | | Locus: circle | ∣ z − a ∣ = r | z-a | =r ∣ z − a ∣ = r | | Locus: perpendicular bisector | ∣ z − a ∣ = ∣ z − b ∣ | z-a | = | z-b | ∣ z − a ∣ = ∣ z − b ∣ | | Locus: half-line | arg ( z − a ) = θ \arg(z-a) = \theta arg ( z − a ) = θ |
Solve z 3 = − 8 i z^3 = -8i z 3 = − 8 i Giving roots in Cartesian form.
Solution − 8 i = 8 e − i π / 2 -8i = 8e^{-i\pi/2} − 8 i = 8 e − iπ /2 . Roots: z k = 2 exp ( − i π / 2 + 2 k π i 3 ) z_k = 2\exp\!\left(\dfrac{-i\pi/2 + 2k\pi i}{3}\right) z k = 2 exp ( 3 − iπ /2 + 2 k π i ) For k = 0 , 1 , 2 k=0,1,2 k = 0 , 1 , 2 .
z 0 = 2 e − i π / 6 = 2 ( 3 2 − i 2 ) = 3 − i z_0 = 2e^{-i\pi/6} = 2\!\left(\dfrac{\sqrt{3}}{2} - \dfrac{i}{2}\right) = \sqrt{3}-i z 0 = 2 e − iπ /6 = 2 ( 2 3 − 2 i ) = 3 − i .
z 1 = 2 e i π / 2 = 2 i z_1 = 2e^{i\pi/2} = 2i z 1 = 2 e iπ /2 = 2 i .
z 2 = 2 e 7 i π / 6 = 2 ( − 3 2 − i 2 ) = − 3 − i z_2 = 2e^{7i\pi/6} = 2\!\left(-\dfrac{\sqrt{3}}{2} - \dfrac{i}{2}\right) = -\sqrt{3}-i z 2 = 2 e 7 iπ /6 = 2 ( − 2 3 − 2 i ) = − 3 − i .
z = 3 − i , 2 i , − 3 − i \boxed{z = \sqrt{3}-i,\; 2i,\; -\sqrt{3}-i} z = 3 − i , 2 i , − 3 − i
Prove that ∣ z 1 z 2 ∣ = ∣ z 1 ∣ ∣ z 2 ∣ |z_1 z_2| = |z_1||z_2| ∣ z 1 z 2 ∣ = ∣ z 1 ∣∣ z 2 ∣ for any complex numbers z 1 , z 2 z_1, z_2 z 1 , z 2 .
Solution Let z 1 = r 1 e i θ 1 z_1 = r_1 e^{i\theta_1} z 1 = r 1 e i θ 1 and z 2 = r 2 e i θ 2 z_2 = r_2 e^{i\theta_2} z 2 = r 2 e i θ 2 .
z 1 z 2 = r 1 r 2 e i ( θ 1 + θ 2 ) z_1 z_2 = r_1 r_2 e^{i(\theta_1+\theta_2)} z 1 z 2 = r 1 r 2 e i ( θ 1 + θ 2 ) .
∣ z 1 z 2 ∣ = r 1 r 2 = ∣ z 1 ∣ ∣ z 2 ∣ |z_1 z_2| = r_1 r_2 = |z_1||z_2| ∣ z 1 z 2 ∣ = r 1 r 2 = ∣ z 1 ∣∣ z 2 ∣ . ■ \blacksquare ■
Any non-zero complex number can be written as z = r e i θ z = re^{i\theta} z = r e i θ where r = ∣ z ∣ r = |z| r = ∣ z ∣ and θ = arg ( z ) \theta = \arg(z) θ = arg ( z ) .
This form makes multiplication and division particularly simple:
z 1 z 2 = r 1 r 2 e i ( θ 1 + θ 2 ) z_1 z_2 = r_1 r_2 e^{i(\theta_1+\theta_2)} z 1 z 2 = r 1 r 2 e i ( θ 1 + θ 2 ) z 1 / z 2 = ( r 1 / r 2 ) e i ( θ 1 − θ 2 ) z_1/z_2 = (r_1/r_2) e^{i(\theta_1-\theta_2)} z 1 / z 2 = ( r 1 / r 2 ) e i ( θ 1 − θ 2 ) Setting θ = π \theta = \pi θ = π in Euler’s formula: e i π + 1 = 0 e^{i\pi} + 1 = 0 e iπ + 1 = 0 .
This connects five fundamental constants: e$$i$$\pi$$1 And 0 0 0 .
If P ( z ) P(z) P ( z ) is a polynomial with real coefficients and z = a + b i z = a + bi z = a + bi is a root, then z ˉ = a − b i \bar{z} = a - bi z ˉ = a − bi Is also a root. This is because P ( z ) ‾ = P ( z ˉ ) \overline{P(z)} = P(\bar{z}) P ( z ) = P ( z ˉ ) for real-coefficient polynomials.
Inequality Region ∥ z − a ∥ < r \|z-a\| < r ∥ z − a ∥ < r Interior of circle (open disc) ∥ z − a ∥ ≤ r \|z-a\| \leq r ∥ z − a ∥ ≤ r Closed disc α < arg ( z − a ) < β \alpha < \arg(z-a) < \beta α < arg ( z − a ) < β Sector (angular region) R e ( z ) > k \mathrm{Re}(z) > k Re ( z ) > k Half-plane to the right of x = k x = k x = k I m ( z ) > k \mathrm{Im}(z) > k Im ( z ) > k Half-plane above y = k y = k y = k
From e i θ = cos θ + i sin θ e^{i\theta} = \cos\theta + i\sin\theta e i θ = cos θ + i sin θ and e − i θ = cos θ − i sin θ e^{-i\theta} = \cos\theta - i\sin\theta e − i θ = cos θ − i sin θ :
cos θ = e i θ + e − i θ 2 , sin θ = e i θ − e − i θ 2 i \cos\theta = \frac{e^{i\theta}+e^{-i\theta}}{2}, \qquad \sin\theta = \frac{e^{i\theta}-e^{-i\theta}}{2i} cos θ = 2 e i θ + e − i θ , sin θ = 2 i e i θ − e − i θ
These are essential for deriving trigonometric identities and solving certain integrals.
Express 1 + e i θ 1 − e i θ \dfrac{1+e^{i\theta}}{1-e^{i\theta}} 1 − e i θ 1 + e i θ in the form a + b i a+bi a + bi .
Solution 1 + e i θ 1 − e i θ = e i θ / 2 ( e − i θ / 2 + e i θ / 2 ) e i θ / 2 ( e − i θ / 2 − e i θ / 2 ) = 2 cos ( θ / 2 ) − 2 i sin ( θ / 2 ) = i cos ( θ / 2 ) sin ( θ / 2 ) = i cot ( θ / 2 ) \dfrac{1+e^{i\theta}}{1-e^{i\theta}} = \dfrac{e^{i\theta/2}(e^{-i\theta/2}+e^{i\theta/2})}{e^{i\theta/2}(e^{-i\theta/2}-e^{i\theta/2})} = \dfrac{2\cos(\theta/2)}{-2i\sin(\theta/2)} = \dfrac{i\cos(\theta/2)}{\sin(\theta/2)} = \boxed{i\cot(\theta/2)} 1 − e i θ 1 + e i θ = e i θ /2 ( e − i θ /2 − e i θ /2 ) e i θ /2 ( e − i θ /2 + e i θ /2 ) = − 2 i sin ( θ /2 ) 2 cos ( θ /2 ) = sin ( θ /2 ) i cos ( θ /2 ) = i cot ( θ /2 )
Prove that the sum of the n n n -th roots of unity is zero.
Solution The n n n -th roots of unity are 1 , ω , ω 2 , … , ω n − 1 1, \omega, \omega^2, \ldots, \omega^{n-1} 1 , ω , ω 2 , … , ω n − 1 where ω = e 2 π i / n \omega = e^{2\pi i/n} ω = e 2 π i / n .
This is a geometric series: ∑ k = 0 n − 1 ω k = 1 − ω n 1 − ω = 1 − 1 1 − ω = 0 \displaystyle\sum_{k=0}^{n-1} \omega^k = \frac{1-\omega^n}{1-\omega} = \frac{1-1}{1-\omega} = 0 k = 0 ∑ n − 1 ω k = 1 − ω 1 − ω n = 1 − ω 1 − 1 = 0 . ■ \blacksquare ■
Find all complex numbers z z z such that z z ˉ + z + z ˉ = 3 z\bar{z} + z + \bar{z} = 3 z z ˉ + z + z ˉ = 3 .
Solution Let z = x + i y z = x+iy z = x + i y . Then z ˉ = x − i y \bar{z} = x-iy z ˉ = x − i y and z z ˉ = x 2 + y 2 z\bar{z} = x^2+y^2 z z ˉ = x 2 + y 2 .
x 2 + y 2 + 2 x = 3 ⟹ ( x + 1 ) 2 + y 2 = 4 x^2+y^2 + 2x = 3 \implies (x+1)^2 + y^2 = 4 x 2 + y 2 + 2 x = 3 ⟹ ( x + 1 ) 2 + y 2 = 4 .
This is a circle with centre ( − 1 , 0 ) (-1, 0) ( − 1 , 0 ) and radius 2 2 2 . All complex numbers on this circle satisfy The equation.
Every polynomial of degree n ≥ 1 n \geq 1 n ≥ 1 with complex coefficients has exactly n n n roots (counting Multiplicity) in the complex numbers.
This means: every polynomial can be factored as P ( z ) = a ( z − z 1 ) ( z − z 2 ) ⋯ ( z − z n ) P(z) = a(z - z_1)(z - z_2)\cdots(z - z_n) P ( z ) = a ( z − z 1 ) ( z − z 2 ) ⋯ ( z − z n ) .
Multiplication by r e i θ re^{i\theta} r e i θ represents:
Dilation by scale factor r r r Rotation by angle θ \theta θ anticlockwise This provides a geometric interpretation of all complex arithmetic.
To solve z n = w = r e i ϕ z^n = w = re^{i\phi} z n = w = r e i ϕ :
z k = r 1 / n exp ( i ( ϕ + 2 k π ) n ) for k = 0 , 1 , … , n − 1 z_k = r^{1/n} \exp\!\left(\frac{i(\phi + 2k\pi)}{n}\right) \quad \text{for } k = 0, 1, \ldots, n-1 z k = r 1/ n exp ( n i ( ϕ + 2 k π ) ) for k = 0 , 1 , … , n − 1
The roots lie on a circle of radius r 1 / n r^{1/n} r 1/ n Equally spaced.
e z = e x + i y = e x ( cos y + i sin y ) e^z = e^{x+iy} = e^x(\cos y + i\sin y) e z = e x + i y = e x ( cos y + i sin y ) for z = x + i y z = x + iy z = x + i y .
Key properties:
∣ e z ∣ = e x |e^z| = e^x ∣ e z ∣ = e x arg ( e z ) = y \arg(e^z) = y arg ( e z ) = y (mod 2 π 2\pi 2 π )e z 1 + z 2 = e z 1 e z 2 e^{z_1+z_2} = e^{z_1}e^{z_2} e z 1 + z 2 = e z 1 e z 2 e z ≠ 0 e^z \neq 0 e z = 0 for all z z z e z = 1 ⟺ z = 2 k π i e^z = 1 \iff z = 2k\pi i e z = 1 ⟺ z = 2 k π i for some integer k k k Find all complex numbers z z z such that z 4 = − 16 z^4 = -16 z 4 = − 16 .
Solution − 16 = 16 e i π -16 = 16e^{i\pi} − 16 = 16 e iπ . Roots: z k = 2 exp ( i ( π + 2 k π ) 4 ) z_k = 2\exp\!\left(\dfrac{i(\pi+2k\pi)}{4}\right) z k = 2 exp ( 4 i ( π + 2 k π ) ) for k = 0 , 1 , 2 , 3 k=0,1,2,3 k = 0 , 1 , 2 , 3 .
z_0 = 2e^{i\pi/4} = \sqrt{2}+i\sqrt{2}$$z_1 = 2e^{i3\pi/4} = -\sqrt{2}+i\sqrt{2}
z_2 = 2e^{i5\pi/4} = -\sqrt{2}-i\sqrt{2}$$z_3 = 2e^{i7\pi/4} = \sqrt{2}-i\sqrt{2} .
Prove that for any complex number z z z : z 1 z 2 ‾ = z ˉ 1 ⋅ z ˉ 2 \overline{z_1 z_2} = \bar{z}_1 \cdot \bar{z}_2 z 1 z 2 = z ˉ 1 ⋅ z ˉ 2 .
Solution Let z 1 = a + b i z_1 = a+bi z 1 = a + bi and z 2 = c + d i z_2 = c+di z 2 = c + d i .
z 1 z 2 = ( a c − b d ) + ( a d + b c ) i z_1 z_2 = (ac-bd) + (ad+bc)i z 1 z 2 = ( a c − b d ) + ( a d + b c ) i .
z 1 z 2 ‾ = ( a c − b d ) − ( a d + b c ) i \overline{z_1 z_2} = (ac-bd) - (ad+bc)i z 1 z 2 = ( a c − b d ) − ( a d + b c ) i .
z ˉ 1 ⋅ z ˉ 2 = ( a − b i ) ( c − d i ) = a c − a d i − b c i + b d i 2 = ( a c − b d ) − ( a d + b c ) i \bar{z}_1 \cdot \bar{z}_2 = (a-bi)(c-di) = ac - adi - bci + bdi^2 = (ac-bd) - (ad+bc)i z ˉ 1 ⋅ z ˉ 2 = ( a − bi ) ( c − d i ) = a c − a d i − b c i + b d i 2 = ( a c − b d ) − ( a d + b c ) i .
Equal. ■ \blacksquare ■
The complex numbers z z z and w w w satisfy |z| = 3$$|w| = 4 And ∣ z + w ∣ = 5 |z+w| = 5 ∣ z + w ∣ = 5 . Find ∣ z − w ∣ |z-w| ∣ z − w ∣ .
Solution ∣ z + w ∣ 2 = ∣ z ∣ 2 + ∣ w ∣ 2 + 2 R e ( z w ˉ ) = 9 + 16 + 2 R e ( z w ˉ ) = 25 |z+w|^2 = |z|^2 + |w|^2 + 2\mathrm{Re}(z\bar{w}) = 9+16+2\mathrm{Re}(z\bar{w}) = 25 ∣ z + w ∣ 2 = ∣ z ∣ 2 + ∣ w ∣ 2 + 2 Re ( z w ˉ ) = 9 + 16 + 2 Re ( z w ˉ ) = 25 .
R e ( z w ˉ ) = 0 \mathrm{Re}(z\bar{w}) = 0 Re ( z w ˉ ) = 0 .
∣ z − w ∣ 2 = ∣ z ∣ 2 + ∣ w ∣ 2 − 2 R e ( z w ˉ ) = 9 + 16 − 0 = 25 |z-w|^2 = |z|^2 + |w|^2 - 2\mathrm{Re}(z\bar{w}) = 9+16-0 = 25 ∣ z − w ∣ 2 = ∣ z ∣ 2 + ∣ w ∣ 2 − 2 Re ( z w ˉ ) = 9 + 16 − 0 = 25 .
∣ z − w ∣ = 5 \boxed{|z-w| = 5} ∣ z − w ∣ = 5
The complex logarithm, n n n -th root, and inverse trigonometric functions are all multi-valued. Branch Cuts are used to define single-valued branches (principal values).
The extended complex plane C ^ = C ∪ { ∞ } \hat{\mathbb{C}} = \mathbb{C} \cup \{\infty\} C ^ = C ∪ { ∞ } is topologically a sphere (the Riemann sphere). Stereographic projection maps each point on the sphere (except the north pole) To a unique point in the complex plane.
While complex analysis (Cauchy’s theorem, residue calculus) is beyond A-Level, the fundamental Concepts appear:
Cauchy’s integral formula: f ( a ) = 1 2 π i ∮ C f ( z ) z − a d z f(a) = \dfrac{1}{2\pi i}\displaystyle\oint_C \frac{f(z)}{z-a}\,dz f ( a ) = 2 π i 1 ∮ C z − a f ( z ) d z Residue theorem: ∮ C f ( z ) d z = 2 π i ∑ Res ( f , a k ) \displaystyle\oint_C f(z)\,dz = 2\pi i \sum \text{Res}(f, a_k) ∮ C f ( z ) d z = 2 π i ∑ Res ( f , a k ) These are mentioned for context and further study.
De Moivre’s theorem connects complex numbers to number theory:
Fermat’s theorem on sums of two squares: p ≡ 1 ( m o d 4 ) ⟹ p = a 2 + b 2 p \equiv 1 \pmod 4 \implies p = a^2 + b^2 p ≡ 1 ( mod 4 ) ⟹ p = a 2 + b 2 Wilson’s theorem: ( p − 1 ) ! ≡ − 1 ( m o d p ) (p-1)! \equiv -1 \pmod p ( p − 1 )! ≡ − 1 ( mod p ) for prime p p p Express cos 5 θ + i sin 5 θ \cos 5\theta + i\sin 5\theta cos 5 θ + i sin 5 θ in terms of cos θ \cos\theta cos θ and sin θ \sin\theta sin θ using the binomial Theorem.
Solution ( cos θ + i sin θ ) 5 = cos 5 θ + 5 i cos 4 θ sin θ − 10 cos 3 θ sin 2 θ − 10 i cos 2 θ sin 3 θ + 5 cos θ sin 4 θ + i sin 5 θ (\cos\theta + i\sin\theta)^5 = \cos^5\theta + 5i\cos^4\theta\sin\theta - 10\cos^3\theta\sin^2\theta - 10i\cos^2\theta\sin^3\theta + 5\cos\theta\sin^4\theta + i\sin^5\theta ( cos θ + i sin θ ) 5 = cos 5 θ + 5 i cos 4 θ sin θ − 10 cos 3 θ sin 2 θ − 10 i cos 2 θ sin 3 θ + 5 cos θ sin 4 θ + i sin 5 θ .
Real part: cos 5 θ = cos 5 θ − 10 cos 3 θ sin 2 θ + 5 cos θ sin 4 θ \cos 5\theta = \cos^5\theta - 10\cos^3\theta\sin^2\theta + 5\cos\theta\sin^4\theta cos 5 θ = cos 5 θ − 10 cos 3 θ sin 2 θ + 5 cos θ sin 4 θ .
Using sin 2 θ = 1 − cos 2 θ \sin^2\theta = 1-\cos^2\theta sin 2 θ = 1 − cos 2 θ :
= cos 5 θ − 10 cos 3 θ ( 1 − cos 2 θ ) + 5 cos θ ( 1 − cos 2 θ ) 2 = \cos^5\theta - 10\cos^3\theta(1-\cos^2\theta) + 5\cos\theta(1-\cos^2\theta)^2 = cos 5 θ − 10 cos 3 θ ( 1 − cos 2 θ ) + 5 cos θ ( 1 − cos 2 θ ) 2
= cos 5 θ − 10 cos 3 θ + 10 cos 5 θ + 5 cos θ − 10 cos 3 θ + 5 cos 5 θ = \cos^5\theta - 10\cos^3\theta + 10\cos^5\theta + 5\cos\theta - 10\cos^3\theta + 5\cos^5\theta = cos 5 θ − 10 cos 3 θ + 10 cos 5 θ + 5 cos θ − 10 cos 3 θ + 5 cos 5 θ
= 16 cos 5 θ − 20 cos 3 θ + 5 cos θ = \boxed{16\cos^5\theta - 20\cos^3\theta + 5\cos\theta} = 16 cos 5 θ − 20 cos 3 θ + 5 cos θ .
Prove that ∣ z + w ∣ 2 + ∣ z − w ∣ 2 = 2 ( ∣ z ∣ 2 + ∣ w ∣ 2 ) |z+w|^2 + |z-w|^2 = 2(|z|^2+|w|^2) ∣ z + w ∣ 2 + ∣ z − w ∣ 2 = 2 ( ∣ z ∣ 2 + ∣ w ∣ 2 ) for all complex numbers z , w z, w z , w (the Parallelogram law).
Solution ∣ z + w ∣ 2 + ∣ z − w ∣ 2 = ( z + w ) ( z ˉ + w ˉ ) + ( z − w ) ( z ˉ − w ˉ ) |z+w|^2 + |z-w|^2 = (z+w)(\bar{z}+\bar{w}) + (z-w)(\bar{z}-\bar{w}) ∣ z + w ∣ 2 + ∣ z − w ∣ 2 = ( z + w ) ( z ˉ + w ˉ ) + ( z − w ) ( z ˉ − w ˉ )
= ∣ z ∣ 2 + z w ˉ + w z ˉ + ∣ w ∣ 2 + ∣ z ∣ 2 − z w ˉ − w z ˉ + ∣ w ∣ 2 = 2 ∣ z ∣ 2 + 2 ∣ w ∣ 2 = |z|^2+z\bar{w}+w\bar{z}+|w|^2 + |z|^2-z\bar{w}-w\bar{z}+|w|^2 = 2|z|^2 + 2|w|^2 = ∣ z ∣ 2 + z w ˉ + w z ˉ + ∣ w ∣ 2 + ∣ z ∣ 2 − z w ˉ − w z ˉ + ∣ w ∣ 2 = 2∣ z ∣ 2 + 2∣ w ∣ 2 .
This is the parallelogram law: the sum of squares of the diagonals equals the sum of squares of all Four sides. ■ \blacksquare ■
Further Algebra and Functions — Polynomial roots and factor theorem are extended to the complex domain in this topic.Matrices — Linear transformations in the complex plane can be represented using matrix multiplication.Further Calculus — Integration of complex-valued functions and residue theory build on the algebraic foundations here.Mechanics — Oscillations and wave motion in physics are logically described using complex exponentials.