The most important formula connecting exponential and trigonometric functions. Derived by substituting iθ into the Taylor series of eˣ and separating real and imaginary parts. The special case θ = π gives Euler's identity: e^(iπ) + 1 = 0.
Derivation
Three functions — ex, cosθ, sinθ — look entirely unrelated when first encountered. Euler's formula reveals they are the same object, viewed from different angles.
The Taylor Series of ex
For any real number x:
ex=1+x+2!x2+3!x3+4!x4+5!x5+⋯
This series converges for all x∈R. We now ask: what happens if we substitute x=iθ, where θ is real?
Substituting x=iθ
eiθ=1+iθ+2!(iθ)2+3!(iθ)3+4!(iθ)4+5!(iθ)5+⋯
Each power of iθ simplifies using the cycle i1=i,i2=−1,i3=−i,i4=1:
These two series are exactly the Taylor expansions of cosθ and sinθ:
cosθ=1−2!θ2+4!θ4−⋯sinθ=θ−3!θ3+5!θ5−⋯
Therefore:
eiθ=cosθ+isinθ
Euler's Identity
Setting θ=π:
eiπ=cosπ+isinπ=−1+0=−1eiπ+1=0
Five fundamental constants — e, i, π, 1, 0 — in a single equation. This is not a coincidence or a trick. It is the direct consequence of the series expansion above.
What the Formula Is Really Saying
Writing z=eiθ means ∣z∣=1 and arg(z)=θ. The exponential eiθ is simply the point on the unit circle at angle θ. As θ increases from 0 to 2π, eiθ traces the unit circle exactly once anticlockwise.
This is why multiplying any complex number reiϕ by eiα rotates it by α — you are adding angles in the exponent.