Exponential Form

A2 · P3 · 2 min

Euler's relation eiθ=cos⁡θ+isin⁡θe^{i\theta} = \cos\theta + i\sin\theta compresses the polar form to z=reiθz = re^{i\theta}. Multiplying and dividing then follow the ordinary index laws, which is the cleanest way to see why arguments add.

The form

Key result
z=reiθmeansz=r(cos⁡θ+isin⁡θ),r=∣z∣, θ=arg⁡z.z = re^{i\theta} \quad\text{means}\quad z = r(\cos\theta + i\sin\theta), \qquad r = |z|,\ \theta = \arg z.

Index laws give:

r1eiθ1⋅r2eiθ2=r1r2ei(θ1+θ2),r1eiθ1r2eiθ2=r1r2ei(θ1−θ2),(reiθ)n=rneinθ.r_1 e^{i\theta_1} \cdot r_2 e^{i\theta_2} = r_1 r_2 e^{i(\theta_1 + \theta_2)}, \qquad \frac{r_1 e^{i\theta_1}}{r_2 e^{i\theta_2}} = \frac{r_1}{r_2}e^{i(\theta_1 - \theta_2)}, \qquad \left(re^{i\theta}\right)^n = r^n e^{in\theta}.

Special values: eiπ=−1e^{i\pi} = -1, eiπ/2=ie^{i\pi/2} = i, e2πi=1e^{2\pi i} = 1. The conjugate of reiθre^{i\theta} is re−iθre^{-i\theta}.

Converting to exponential form

Write 1−i1 - i and −4-4 in the form reiθre^{i\theta}.

Solution

∣1−i∣=2|1 - i| = \sqrt{2}, arg⁡(1−i)=−π4\arg(1 - i) = -\tfrac{\pi}{4}: 2e−iπ/4\sqrt{2}e^{-i\pi/4}.

−4=4eiπ-4 = 4e^{i\pi}.

From exponential to Cartesian

Express 6eiπ/36e^{i\pi/3} and 2e−5iπ/62e^{-5i\pi/6} in the form x+iyx + iy.

Solution

6eiπ/3=6(12+32i)=3+33i6e^{i\pi/3} = 6\left(\tfrac{1}{2} + \tfrac{\sqrt{3}}{2}i\right) = 3 + 3\sqrt{3}i.

2e−5iπ/6=2(−32−12i)=−3−i2e^{-5i\pi/6} = 2\left(-\tfrac{\sqrt{3}}{2} - \tfrac{1}{2}i\right) = -\sqrt{3} - i.

Multiplying and dividing

z=3eiπ/4z = 3e^{i\pi/4} and w=2eiπ/3w = 2e^{i\pi/3}. Find zwzw, zw\dfrac{z}{w} and z4z^4 in exponential form, and z4z^4 in Cartesian form.

Solution

zw=6e7iπ/12zw = 6e^{7i\pi/12}. zw=32e−iπ/12\dfrac{z}{w} = \tfrac{3}{2}e^{-i\pi/12}. z4=81eiπ=−81z^4 = 81e^{i\pi} = -81.

Using the conjugate

Show that z+z∗z + z^* is real and z−z∗z - z^* is purely imaginary using exponential form, for z=reiθz = re^{i\theta}.

Solution

z+z∗=reiθ+re−iθ=r(cos⁡θ+isin⁡θ)+r(cos⁡θ−isin⁡θ)=2rcos⁡θz + z^* = re^{i\theta} + re^{-i\theta} = r(\cos\theta + i\sin\theta) + r(\cos\theta - i\sin\theta) = 2r\cos\theta, real.

z−z∗=2irsin⁡θz - z^* = 2ir\sin\theta, purely imaginary.

Solving an equation in exponential form

Find both square roots of 9eiπ/39e^{i\pi/3}.

Solution

If z=reiϕz = re^{i\phi} then r2e2iϕ=9eiπ/3r^2 e^{2i\phi} = 9e^{i\pi/3}, so r=3r = 3 and 2ϕ=π3+2kπ2\phi = \tfrac{\pi}{3} + 2k\pi, giving ϕ=π6\phi = \tfrac{\pi}{6} or ϕ=π6+π=7π6\phi = \tfrac{\pi}{6} + \pi = \tfrac{7\pi}{6} (principal value −5π6-\tfrac{5\pi}{6}).

z=3eiπ/6z = 3e^{i\pi/6} or z=3e−5iπ/6z = 3e^{-5i\pi/6}; in Cartesian form, ±(332+32i)\pm\left(\tfrac{3\sqrt{3}}{2} + \tfrac{3}{2}i\right).

Watch out

eiθe^{i\theta} has modulus 11 for every real θ\theta: it is a point on the unit circle. Do not confuse eiθe^{i\theta} (a rotation) with eθe^{\theta} (a real number). And the argument in the exponent must be in radians.

Exam tip

Any of the three forms is accepted unless the question specifies. "In the form reiθre^{i\theta}" means give exact rr and θ\theta where possible, e.g. 2e−iπ/4\sqrt{2}e^{-i\pi/4}, and otherwise 3 significant figures for θ\theta.

Practice

Question
  1. Write −1−i3-1 - i\sqrt{3} in the form reiθre^{i\theta}.
  2. Express 4e3iπ/44e^{3i\pi/4} in Cartesian form.
  3. z=2e2iπ/3z = 2e^{2i\pi/3}. Find z3z^3 and 1z\dfrac{1}{z} in exponential form with principal arguments.
  4. Find both square roots of 16eiπ/216e^{i\pi/2} in Cartesian form.
Answers
  1. 2e−2iπ/32e^{-2i\pi/3}.
  2. −22+22i-2\sqrt{2} + 2\sqrt{2}i.
  3. z3=8e2iπ=8e0=8z^3 = 8e^{2i\pi} = 8e^{0} = 8; 1z=12e−2iπ/3\dfrac{1}{z} = \tfrac{1}{2}e^{-2i\pi/3}.
  4. 4eiπ/44e^{i\pi/4} and 4e−3iπ/44e^{-3i\pi/4}: ±(22+22i)\pm(2\sqrt{2} + 2\sqrt{2}i).

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