Euler's Formula
Also known as: Euler's identity (θ = π case) · Complex exponential · Phasor relation
Multiplying by e^{iθ} rotates the complex plane by angle θ. The exponential of an imaginary number is a point on the unit circle, decomposing naturally into cosine (real) and sine (imaginary) parts.
A rotating phasor of unit length sweeps the complex plane. Dashed projections drop to the real axis (cosθ, orange) and imaginary axis (sinθ, green), while side bars track those projections as the angle advances — the unit circle generating sine and cosine.
Equivalent forms
Five fundamental constants — 0, 1, e, i, π — bound into one identity, and every rotation, oscillation, and AC circuit secretly runs on it.
Unit systems
Where it holds
Dimensional analysis
Euler published the formula in his 1748 Introductio, uniting the exponential, trigonometric, and imaginary worlds. The special case e^{iπ}+1=0 — linking e, i, π, 1 and 0 — is routinely voted the most beautiful equation in mathematics.
How can raising a number to an imaginary power make it spin? Euler's formula says exponential growth and circular motion are the same act, seen from different sides.
Spin the angle θ and watch e^{iθ} ride the unit circle while its shadow traces cosθ and its height traces sinθ.
- Phasors in AC circuit analysis and signal processing
- Fourier analysis basis functions)
- Quantum mechanics wavefunctions and time evolution
- Rotations in computer graphics and control theory
- grows like a normal exponential — it has constant magnitude 1; only its phase changes.
- i is 'imaginary' so it isn't physical — it is just a rotation operator and is everywhere in engineering.
- Euler's identity is a coincidence — it's a direct consequence of the series definitions.
Limiting cases
What if…
e^{a+bi} = e^a(cos b + i sin b): the real part scales the magnitude, the imaginary part rotates the phase.
You get — counter-rotating phasors add to a real oscillation, the heart of Fourier analysis.
Evaluate e^{iπ/3}
- \theta:
Why i·i = −1, geometrically
- i:
- Each i is a rotation
- Two of them make a rotation
- rotation of