๐Ÿงฎ Brain Teaser
Probability
The Thick Coin
2026-06-03
โœ๏ธŽ

The Thick Coin

A fair coin is tossed in such a way that it lands uniformly at random on any face โ€” heads, tails, or edge. How thick should the coin be (as a fraction of its diameter) so that the probability of landing on edge is exactly 13\frac{1}{3}?

More precisely: model the coin as a right circular cylinder with radius rr and thickness tt. Inscribe it in a sphere of radius RR (centered at the coin's center). A random direction is chosen uniformly on the sphere; the coin lands on edge if the radius in that direction hits the curved band (the edge), and on a face otherwise.

Find t/2rt/2r (the ratio of thickness to diameter).

geometric probabilityspherezone areaArchimedes3D geometry

Answer: The Thick Coin

Key Idea / Intuition

The beautiful insight is a classical theorem from solid geometry: the surface area of a spherical zone depends only on its height, not on where it sits on the sphere. So the probability of landing on edge equals the fraction of the sphere's surface covered by the "equatorial band" โ€” which is simply proportional to the height of that band. Setting this fraction to 1/31/3 is then a clean geometric calculation using the Pythagorean theorem.


Formal Proof / Solution

Setup. Inscribe the coin (a cylinder of radius rr, thickness tt) in a sphere of radius RR. The center of the sphere coincides with the center of the coin. A random point on the sphere is chosen uniformly; if the radius to that point hits the curved side of the cylinder, the coin lands on edge.

Archimedes' Hat-Box Theorem (Zone Area). For a sphere of radius RR, the area of a spherical zone of height hh (the region between two parallel planes) is: Azone=2ฯ€Rh.A_{\text{zone}} = 2\pi R h. This is independent of where the zone sits โ€” only the height matters.

Geometry. The edge band corresponds to the zone of height h=th = t (the thickness). The total surface area of the sphere is 4ฯ€R24\pi R^2. So: P(edge)=2ฯ€Rt4ฯ€R2=t2R.P(\text{edge}) = \frac{2\pi R t}{4\pi R^2} = \frac{t}{2R}.

Finding RR in terms of rr and tt. The corners of the cylinder touch the inscribed sphere. By the Pythagorean theorem: R2=r2+(t2)2.R^2 = r^2 + \left(\frac{t}{2}\right)^2.

Setting P(edge)=13P(\text{edge}) = \frac{1}{3}. We need: t2R=13โ€…โ€ŠโŸนโ€…โ€Št=2R3.\frac{t}{2R} = \frac{1}{3} \implies t = \frac{2R}{3}.

Substituting into R2=r2+(t/2)2R^2 = r^2 + (t/2)^2: R2=r2+R29โ€…โ€ŠโŸนโ€…โ€Š8R29=r2โ€…โ€ŠโŸนโ€…โ€ŠR=3r22.R^2 = r^2 + \frac{R^2}{9} \implies \frac{8R^2}{9} = r^2 \implies R = \frac{3r}{2\sqrt{2}}.

Then: t=2R3=23โ‹…3r22=r2.t = \frac{2R}{3} = \frac{2}{3} \cdot \frac{3r}{2\sqrt{2}} = \frac{r}{\sqrt{2}}.

The ratio of thickness to diameter: t2r=122=24โ‰ˆ0.354.\frac{t}{2r} = \frac{1}{2\sqrt{2}} = \frac{\sqrt{2}}{4} \approx 0.354.

Conclusion. The coin should be about 35.4% as thick as its diameter to have a 13\frac{1}{3} chance of landing on edge. This is the answer von Neumann reportedly computed in his head in 20 seconds.

Sanity check: If t=0t = 0 (flat disk), P(edge)=0P(\text{edge}) = 0. If tโ†’โˆžt \to \infty (long cylinder), P(edge)โ†’1P(\text{edge}) \to 1. The formula t/2R=1/3t/2R = 1/3 interpolates cleanly between these extremes. โœ“

Source: Fifty Challenging Problems in Probability with Solutions, Frederick Mosteller, Problem 38

Type: ProbabilitySource: Fifty Challenging Problems in Probability with Solutions, Frederick Mosteller, Problem 38Edit on GitHub โ†—