# Probability of random sphere lying inside the unit ball

Let $$n\geq2$$. Let $$B\subseteq\mathbb{R}^n$$ be the unit ball. Randomly choose $$n+1$$ points of $$B$$ (uniformly and independently). Then (almost surely) there will be a unique hypersphere $$S$$ passing through all $$n+1$$ points.

What is the probability that $$S\subseteq B$$?

When $$n=2$$, the probability seems to be exactly $$40\%$$.

• In the $n=2$ case, after choosing two of the points, the set of good possibilities for the third point is a disjoint union of two lunes. I think this generalizes to higher dimensions as well. Feb 22, 2020 at 2:53
• Just to make sure I understand. If I take three random points $(x_1,y_1), (x_2,y_2),(x_3,y_3)$ all such $x^2+y^2<1$ there is a nearly $40$% chance that these three points lie in some circle completely contained in $x^2+y^2<1$? Feb 22, 2020 at 23:55
• @Mason yes, there seems to be exactly a 40% chance that those three points lie on some circle inside $x^2+y^2<1$. Feb 23, 2020 at 1:01
• @Mason: Note that you wrote "in" whereas Thomas Browning wrote "on". The question says "passing through", so Thomas Browning's interpretation is the correct one. Feb 23, 2020 at 16:31
• @joriki. Thanks. Yes. I understand. If we take 'in' to mean the interior of a circle the problem is trivialized and this happens 100% of the time. Feb 23, 2020 at 20:56

I’ll do this for $$n=2$$ first, where the calculation is more tangible, and then build on that for the general case.

Parameterize the three points $$(x_i,y_i)$$ by the centre $$(x,y)$$ of the circle passing through them, the radius $$r$$ of that circle and three angles $$\phi_i$$, so that $$(x_i,y_i)=(x,y)+r(\cos\phi_i,\sin\phi_i)$$. The Jacobian is

$$\begin{eqnarray} \frac{\partial(x_1,y_1,x_2,y_2,x_3,y_3)}{\partial(x,y,r,\phi_1,\phi_2,\phi_3)} &=& \left|\matrix{ 1&0&1&0&1&0\\ 0&1&0&1&0&1\\ \cos\phi_1&\sin\phi_1&\cos\phi_2&\sin\phi_2&\cos\phi_3&\sin\phi_3\\ -r\sin\phi_1&r\cos\phi_1&0&0&0&0\\ 0&0&-r\sin\phi_2&r\cos\phi_2&0&0\\ 0&0&0&0&-r\sin\phi_3&r\cos\phi_3\\ }\right|\;. \end{eqnarray}$$

The last three rows, which reflect how the coordinates change with the angular variables, are mutually orthogonal. Their orthogonal complement is spanned by the three vectors that reflect how the three points change with the radial variable. We can transform the matrix accordingly, multiplying by an orthogonal matrix with determinant $$1$$:

$$\begin{eqnarray} \pmatrix{ 1&0&1&0&1&0\\ 0&1&0&1&0&1\\ \cos\phi_1&\sin\phi_1&\cos\phi_2&\sin\phi_2&\cos\phi_3&\sin\phi_3\\ -r\sin\phi_1&r\cos\phi_1&0&0&0&0\\ 0&0&-r\sin\phi_2&r\cos\phi_2&0&0\\ 0&0&0&0&-r\sin\phi_3&r\cos\phi_3\\ } \\[10pt] \times\pmatrix{ \cos\phi_1&0&0&-\sin\phi_1&0&0\\ \sin\phi&0&0&\cos\phi_1&0&0\\ 0&\cos\phi_2&0&0&-\sin\phi_2&0\\ 0&\sin\phi_2&0&0&\cos\phi_2&0\\ 0&0&\cos\phi_3&0&0&-\sin\phi_3\\ 0&0&\sin\phi_3&0&0&\cos\phi_3 } \\[10pt] = \pmatrix{ \cos\phi_1&\cos\phi_2&\cos\phi_3&-\sin\phi_1&-\sin\phi_2&-\sin\phi_3\\ \sin\phi_1&\sin\phi_2&\sin\phi_3&\cos\phi_1&\cos\phi_2&\cos\phi_3\\ 1&1&1&0&0&0\\ 0&0&0&r&0&0\\ 0&0&0&0&r&0\\ 0&0&0&0&0&r }\;. \end{eqnarray}$$

Thus

$$\frac{\partial(x_1,y_1,x_2,y_2,x_3,y_3)}{\partial(x,y,r,\phi_1,\phi_2,\phi_3)}=r^3\left| \matrix{ \cos\phi_1&\cos\phi_2&\cos\phi_3\\ \sin\phi_1&\sin\phi_2&\sin\phi_3\\ 1&1&1 } \right|\;.$$

This determinant is twice the area of the triangle formed by the three radial unit vectors $$(\cos\phi_i,\sin\phi_i)$$. We want

$$\begin{eqnarray} P(\text{circle in unit disk}) &=& \frac1{\pi^3}\iiint_\limits{\sqrt{x^2+y^2}+r\lt1}\mathrm dx\mathrm dy\mathrm dr\int_0^{2\pi}\!\int_0^{2\pi}\!\int_0^{2\pi}\mathrm d\phi_1\mathrm d\phi_2\mathrm d\phi_3\frac{\partial(x_1,y_1,x_2,y_2,x_3,y_3)}{\partial(x,y,r,\phi_1,\phi_2,\phi_3)} \\ &=& \frac2{\pi^2}\iint_\limits{\rho+r\lt1}\rho\mathrm d\rho\mathrm dr\int_0^{2\pi}\!\int_0^{2\pi}\!\int_0^{2\pi}\mathrm d\phi_1\mathrm d\phi_2\mathrm d\phi_3\frac{\partial(x_1,y_1,x_2,y_2,x_3,y_3)}{\partial(x,y,r,\phi_1,\phi_2,\phi_3)} \\ &=& \frac1{\pi^2}\int_0^1(1-r)^2\mathrm dr\int_0^{2\pi}\!\int_0^{2\pi}\!\int_0^{2\pi}\mathrm d\phi_1\mathrm d\phi_2\mathrm d\phi_3\frac{\partial(x_1,y_1,x_2,y_2,x_3,y_3)}{\partial(x,y,r,\phi_1,\phi_2,\phi_3)} \\\\ &=& \frac1{\pi^2}\int_0^1(1-r)^2r^3\mathrm dr\int_0^{2\pi}\!\int_0^{2\pi}\!\int_0^{2\pi}\mathrm d\phi_1\mathrm d\phi_2\mathrm d\phi_3\left| \matrix{ \cos\phi_1&\cos\phi_2&\cos\phi_3\\ \sin\phi_1&\sin\phi_2&\sin\phi_3\\ 1&1&1 } \right|\\ \\ &=& \frac1{60\pi^2}\int_0^{2\pi}\!\int_0^{2\pi}\!\int_0^{2\pi}\mathrm d\phi_1\mathrm d\phi_2\mathrm d\phi_3\left| \matrix{ \cos\phi_1&\cos\phi_2&\cos\phi_3\\ \sin\phi_1&\sin\phi_2&\sin\phi_3\\ 1&1&1 } \right|\;. \end{eqnarray}$$

The integral is $$(2\pi)^3$$ times twice the average area of a triangle formed by three points independently uniformly distributed on the unit circle, which is $$\frac3{2\pi}$$ (see e.g. MathWorld). Thus

$$P(\text{circle in unit disk})=\frac1{60\pi^2}\cdot(2\pi)^3\cdot2\cdot\frac3{2\pi}=\frac25\;,$$

Now let’s generalize this for arbitrary $$n$$. We have $$n+1$$ points in $$n$$ dimensions, and thus $$n(n+1)$$ degrees of freedom. We parametrize them by the centre ($$n$$ coordinates), the radius ($$1$$ coordinate) and $$n-1$$ angular variables for each point ($$(n+1)(n-1)=n^2-1$$ coordinates). Differentiating with respect to the $$n^2-1$$ angular variables yields $$n^2-1$$ mutually orthogonal direction vectors with magnitude $$r$$ (corresponding to the last $$2^2-1=3$$ rows above). Transforming to separate the space spanned by these vectors and its orthogonal complement yields the Jacobian

$$\left|\matrix{ \vec u_1&\cdots&\vec u_{n+1}\\ 1&\cdots&1 }\right|\;,$$

where $$\vec u_k$$ is the radial unit vector for the $$k$$-th point. This is $$n!$$ times the volume of the simplex formed by these $$n+1$$ unit vectors. Thus, if we denote the surface area of the $$n$$-sphere by $$S_n$$, the volume of the $$n$$-ball by $$V_n$$ and $$n!$$ times the average volume spanned by $$n+1$$ points independently uniformly distributed on the $$(n-1)$$-sphere by $$T_n$$, we have

$$\begin{eqnarray} P(\text{n-sphere in unit n-ball}) &=& \frac{S_{n-1}}{V_n^{n+1}}\iint_\limits{\rho+r\lt1}\mathrm d\rho\mathrm dr\rho^{n-1}r^{n^2-1}\int\mathrm d\Omega^{n+1}\left|\matrix{ \vec u_1&\cdots&\vec u_{n+1}\\ 1&\cdots&1 }\right| \\ &=& \frac{S_{n-1}}{nV_n^{n+1}}\int_0^1\mathrm dr(1-r)^nr^{n^2-1}\int\mathrm d\Omega^{n+1}\left|\matrix{ \vec u_1&\cdots&\vec u_{n+1}\\ 1&\cdots&1 }\right| \\ &=& \frac{S_{n-1}^{n+2}}{nV_n^{n+1}}B\left(n+1,n^2\right)T_n\;, \end{eqnarray}$$

where

$$B(x,y)=\frac{\Gamma(x)\Gamma(y)}{\Gamma(x+y)}$$

is the beta function.

The volume and surface area are given by (see e.g. Wikipedia)

$$V_n=\frac{\pi^{\frac n2}}{\Gamma\left(\frac n2+1\right)}$$

and

$$S_{n-1}=nV_n\;,$$

$$T_n=\Xi\left(\frac{n^2}2\right)\Xi\left(\frac n2\right)^{-n}\prod_{l=1}^{n-1}\Xi\left(\frac l2\right)$$

with

$$\Xi(n):=\frac{\Gamma\left(n+\frac12\right)}{\Gamma(n)}\;.$$

Thus

$$\begin{eqnarray} P(\text{n-sphere in unit n-ball}) &=& \frac{S_{n-1}^{n+2}}{nV_n^{n+1}}B\left(n+1,n^2\right)T_n \\ &=& n^{n+1}\pi^\frac n2\frac{\Gamma\left(n^2\right)\Gamma(n+1)}{\Gamma\left(\frac n2+1\right)\Gamma\left(n^2+n+1\right)}\Xi\left(\frac{n^2}2\right)\Xi\left(\frac n2\right)^{-n}\prod_{l=1}^{n-1}\Xi\left(\frac l2\right)\;. \end{eqnarray}$$

For $$n=2$$ we can recover the above result,

$$P(\text{circle in unit disk})=2^3\pi\frac{\Gamma(4)\Gamma(3)}{\Gamma(2)\Gamma(7)}\frac{\Xi(2)\Xi\left(\frac12\right)}{\Xi(1)\Xi(1)}=\frac25\;,$$

and for $$n=3$$ we obtain

$$P(\text{sphere in unit ball})=3^4\pi^\frac32\frac{\Gamma(9)\Gamma(4)}{\Gamma\left(\frac52\right)\Gamma(13)}\frac{\Xi\left(\frac92\right)\Xi\left(\frac12\right)\Xi(1)}{\Xi\left(\frac32\right)\Xi\left(\frac32\right)\Xi\left(\frac32\right)}=\frac{24\pi^2}{1925}\approx0.123\;.$$

• Lovely! Last night I figured out your change of variables in 2 dimensions but higher dimensions looked too messy. I'll read through this closely when I have time. Also, your value for $n=3$ agrees with my experimental results. Feb 24, 2020 at 17:35
• Here's a nicer way to write the final answer: $2\cdot n^{n-2}\pi^{(n-1)/2}\frac{n^2!\,n!}{(n^2+n)!}\Xi(n^2/2)\Xi(n/2)^{-n}$. Feb 24, 2020 at 19:44
• When $n$ is even, I think this simplifies to $2^n\binom{n^2}{n^2/2}\binom{n^2+n}{n}^{-1}\binom{n}{n/2}^{-n}$. Feb 24, 2020 at 19:59
• When $n$ is odd, I think this simplifies to $2^nn^{n-2}\pi^{n-1}\binom{n-1}{(n-1)/2}^n\binom{n^2+n}{n}^{-1}\binom{n^2-1}{(n^2-1)/2}^{-1}$. Feb 24, 2020 at 21:14