De Moivre's Theorem

De Moivre's Theorem provides a formula for computing powers of complex numbers in polar form.

For an integral index n, the theorem states:

(cosθ+isinθ)n=cos(nθ)+isin(nθ)(\cos\theta + i\sin\theta)^n = \cos(n\theta) + i\sin(n\theta)

In Euler's form, this is simply (eiθ)n=einθ(e^{i\theta})^n = e^{in\theta}. The theorem also holds for rational indices, which is the basis for finding roots.

n-th Roots of a Complex Number

To find the n-th roots of a complex number z=r(cosθ+isinθ)z = r(\cos\theta + i\sin\theta), we solve the equation wn=zw^n = z. The n distinct roots are given by:

wk=r1/n[cos(θ+2kπn)+isin(θ+2kπn)]w_k = r^{1/n} \left[ \cos\left(\frac{\theta + 2k\pi}{n}\right) + i\sin\left(\frac{\theta + 2k\pi}{n}\right) \right]

where k=0,1,2,...,n1k = 0, 1, 2, ..., n-1.

Geometrically, the n-th roots of a complex number lie on the vertices of a regular n-sided polygon inscribed in a circle of radius r1/nr^{1/n}.

n-th Roots of Unity

The n-th roots of unity are the solutions to the equation zn=1z^n=1. Since 1=cos(0)+isin(0)1 = \cos(0) + i\sin(0), the n roots are:

zk=cos(2kπn)+isin(2kπn)=ei(2kπ/n)z_k = \cos\left(\frac{2k\pi}{n}\right) + i\sin\left(\frac{2k\pi}{n}\right) = e^{i(2k\pi/n)}

for k=0,1,2,...,n1k=0, 1, 2, ..., n-1. These roots are often written as 1,ω,ω2,...,ωn11, \omega, \omega^2, ..., \omega^{n-1}, where ω=ei(2π/n)\omega = e^{i(2\pi/n)}.

Properties of n-th Roots of Unity:

  • They form a Geometric Progression.
  • Sum of the roots is 0: 1+ω+ω2+...+ωn1=01 + \omega + \omega^2 + ... + \omega^{n-1} = 0.
  • Product of the roots is (1)n1(-1)^{n-1}.

Cube Roots of Unity (z3=1z^3=1):

This is a special and very important case. The three cube roots of unity are:

  • 11
  • ω=12+i32=ei(2π/3)\omega = -\frac{1}{2} + i\frac{\sqrt{3}}{2} = e^{i(2\pi/3)}
  • ω2=12i32=ei(4π/3)\omega^2 = -\frac{1}{2} - i\frac{\sqrt{3}}{2} = e^{i(4\pi/3)}

Properties of Cube Roots of Unity:

  • 1+ω+ω2=01 + \omega + \omega^2 = 0
  • ω3=1\omega^3 = 1

Example 1: Using De Moivre's Theorem

Question: Simplify (1+i)8(1+i)^8.

Solution: First, convert 1+i1+i to polar form. r=1+i=12+12=2r = |1+i| = \sqrt{1^2+1^2} = \sqrt{2}. θ=arg(1+i)=π/4\theta = \arg(1+i) = \pi/4. So, 1+i=2(cos(π/4)+isin(π/4))1+i = \sqrt{2}(\cos(\pi/4) + i\sin(\pi/4)). Now, apply De Moivre's Theorem:

(1+i)8=[2(cos(π/4)+isin(π/4))]8(1+i)^8 = [\sqrt{2}(\cos(\pi/4) + i\sin(\pi/4))]^8

=(2)8(cos(8π/4)+isin(8π/4))= (\sqrt{2})^8 (\cos(8 \cdot \pi/4) + i\sin(8 \cdot \pi/4))

=16(cos(2π)+isin(2π))=16(1+0i)=16= 16 (\cos(2\pi) + i\sin(2\pi)) = 16(1 + 0i) = 16

Example 2: Finding n-th Roots

Question: Find the cube roots of 8i8i.

Solution: First, write 8i8i in polar form. z=0+8iz = 0+8i. r=8i=8r = |8i| = 8. The argument θ=π/2\theta = \pi/2. So, 8i=8(cos(π/2)+isin(π/2))8i = 8(\cos(\pi/2) + i\sin(\pi/2)). The cube roots are given by:

wk=81/3[cos(π/2+2kπ3)+isin(π/2+2kπ3)]w_k = 8^{1/3} \left[ \cos\left(\frac{\pi/2 + 2k\pi}{3}\right) + i\sin\left(\frac{\pi/2 + 2k\pi}{3}\right) \right]

for k=0,1,2k=0, 1, 2.

  • For k=0: w0=2(cos(π/6)+isin(π/6))=2(32+i12)=3+iw_0 = 2(\cos(\pi/6) + i\sin(\pi/6)) = 2(\frac{\sqrt{3}}{2} + i\frac{1}{2}) = \sqrt{3}+i.
  • For k=1: w1=2(cos(5π/6)+isin(5π/6))=2(32+i12)=3+iw_1 = 2(\cos(5\pi/6) + i\sin(5\pi/6)) = 2(-\frac{\sqrt{3}}{2} + i\frac{1}{2}) = -\sqrt{3}+i.
  • For k=2: w2=2(cos(9π/6)+isin(9π/6))=2(cos(3π/2)+isin(3π/2))=2(0i)=2iw_2 = 2(\cos(9\pi/6) + i\sin(9\pi/6)) = 2(\cos(3\pi/2) + i\sin(3\pi/2)) = 2(0 - i) = -2i.

Example 3: Using Properties of Cube Roots of Unity

Question: If ω\omega is a complex cube root of unity, find the value of (1ω+ω2)5(1 - \omega + \omega^2)^5.

Solution: We know the property 1+ω+ω2=01 + \omega + \omega^2 = 0. From this, we can write 1+ω2=ω1 + \omega^2 = -\omega. Substitute this into the expression:

(1ω+ω2)5=((1+ω2)ω)5=(ωω)5=(2ω)5(1 - \omega + \omega^2)^5 = ((1+\omega^2) - \omega)^5 = (-\omega - \omega)^5 = (-2\omega)^5

=(2)5(ω)5=32ω5= (-2)^5 (\omega)^5 = -32 \omega^5

Since ω3=1\omega^3 = 1, we can simplify ω5=ω3ω2=1ω2=ω2\omega^5 = \omega^3 \cdot \omega^2 = 1 \cdot \omega^2 = \omega^2. So the final value is 32ω2-32\omega^2.