Circumference
Circumference is the distance around the outside of a circle, calculated as $\pi$ times the diameter or two times $\pi$ times the radius.
Formula
C = 2\pi r = \pi d
Definition
The circumference is the distance all the way around a circle, the circle's version of perimeter: $C = \pi d$, where $d$ is the diameter, or equivalently $C = 2\pi r$ for radius $r$. The constant ratio $C/d = \pi$ holds for every circle, geometrically defining $\pi$ itself, and this same formula gives the arc length of a full circle; for a partial arc of central angle $\theta$ (in radians), the arc length is $r\theta$, a direct proportional slice of the circumference. As an arc length integral, $$C = \int_0^{2\pi} \sqrt{(r\sin t)^2 + (r\cos t)^2} \, dt = r \cdot 2\pi.$$ In non-Euclidean geometry the formula changes: on a sphere of curvature $K$, $C = 2\pi r_g$ where $r_g$ is the geodesic radius, with correction terms of order $O(r^3)$ for small $r$.
Example
A circle with diameter $10$ cm has circumference $C = 3.14 \times 10 = 31.4$ cm, and a tire with radius $30$ cm travels $C = 2 \times 3.14 \times 30 = 188.4$ cm in one full turn. A circular track with diameter $400$ m has $C = \pi \times 400 = 1256.6$ m per lap, so $10$ laps covers $12{,}566$ m $= 12.57$ km. On a sphere of radius $R$, the circumference of a small circle at geodesic distance $r$ from the pole is $C = 2\pi R \sin(r/R)$, which approaches $2\pi r$ as $r/R \to 0$, recovering the flat result.
Key Insight
No matter how big or small a circle is, its circumference divided by its diameter always equals $\pi$ (about $3.14159$), which is what makes circles special among all shapes. The deviation of circumference from $2\pi r$ in curved space is related to the Gaussian curvature by the Bertrand-Diguet-Puiseux theorem; measuring this deviation is how physicists detect the curvature of spacetime near massive objects.