Powered By Blogger

Sunday, December 8, 2019

Random convex polygons III

As I mentioned in one of my earlier posts, the early work of Renyi and Sulanke on  random  planar polygons   was available only in German.    This consists of three separate articles published over a couple of years.     Now, courtesy of the efforts  of  Manfred Weis,   English   translations are available to  the non-German-reading audience. What follows is the third in this series of articles.


Z. Wahrscheinlichkeitstheorie verw. Geb. 9, 146-157 (1968)


Random Convex Polygons in a Ring-shaped Region

by

A. Rényi and R. Sulanke


Received June 2nd 1967

 1. Introduction

Let $K$ be a non-degenerated, finite convex region of the Euclidean plane and $B$ an arbitrary convex region that is contained in the interior of $K$. We chose $n$ random lines $g_1,\,\ldots,\,g_n$ that intersect $K$ but not $B$.

The $g_i$ shall be independent; their distribution shall be the Euclidean invariant line measure $\mu$ with density $dg$ (W. Blaschke $[1]$, § 2). By $H_i$ we denote the closed halfplane defined by $g_i$ that contains $B$. Then

$$(1.1)\quad\Pi_n=\cap_{i=1}^nH_i$$

is a random convex polygon that contains $B$ and is uniquely defined by the $g_i$. By $X_n$ we denote the number of corners of $\Pi_n$. We want to determine the asymptotic behavior of the mathematical expectation of the number of corners of $X_n$ under various assumptions on $B$.

In § 2 we establish the formulas for the probabilities that are to be investigated and derive some simple estimates that will be applied in §§ 3-5. Further we show that the probability for $\Pi_n$ not being closed, as well as the probability that $\Pi_n$ isn't contained in $K$ is of the order $O(\gamma^n)\ (0\lt\gamma\lt 1)$ tends to zero. In § 3 we consider the case that $B$ degenerates to a point and prove $E(X_n)\to\frac{\pi^2}{2}$ for $n\to+\infty$.

In the case that $B$ has a smooth boundary of limited curvature it holds true that $E(X_n)\sim \mathrm{const}.\,n^{1/3}$(theorem 4.  § 4); if finally $B$ is a convex $r$-gon ($r\geqq2$; $r=2$ means that $B$ degenerates to a line segment ), that yields $E(X_n)\sim\frac{2}{3}r\,\log\,n$ (theorem 5,  § 5). The order of magnitude with which $E(X_n)$ tends to infinity with $n$ in the last two cases therefore complies with the corresponding orders of magnitude for the case of the corners of the convex hull of $n$ points that are randomly chosen in $B$ (A. Rényi, R. Sulanke $[2]$).

We would like to warmly thank Mr. L. Berg for some hints to the calculations in § 5.

The result of § 3 may be interpreted as follows: We consider a system of $n$ random linear inequalities $a_kx+b_ky\leqq c_k$ ($k =1,\,2,\,\ldots,\,n$). The word "random" shall mean that the distribution of the lines $a_kx+b_ky=c_k$, that are independent from each other and that all shall hit the region $K$, is determined by the invariant line-measure and the point $B(x=0, y=0)\in K$ satisfies all inequalities.  Let $X_n$ be the smallest number with the following property: There are $X_n$ of the inequalities such that every point $(x,y)$, that satisfies these $X_n$ inequalities, even satisfies all $n$ inequalities. Our result says that for $n\to\infty$ the expected value of the minimal number $X_n$ of the "critical" inequalities approaches $\pi^2/2$. Therefore one can expect that the solutionto a problem from linear programming with two unknowns and arbitrarily large number of linear inequalities with random data requires on average only a rather small number of steps when following one of the known procedures.  So naturally the problem comes up, to treat the analogous task for an arbitrary number of unknowns ( that is for the intersection of random halfspaces of a $k$-dimensional space, $k=3\,,4\,\ldots$). That task was solved recently by Mr. Wolfgang M. Schmidt, when he proved that the average minimal number of "critical" inequalities, also in the $k$-dimensional case ($k=3,\,4,\,\ldots$) approaches a finite value $\lambda_k$ that only depends on $k$; but his prove only yields the existence of the numbers $\lambda_k$ and not their exact value. From the  theorem of Mr. Wolfgang M. Schmidt follows the existence of the limit distribution of $X_n$  for the two-dimensional case that we consider. We hope to return to the explicit determination of that limit distribution in another work.



2. Basic formulas and simple estimations

Let $S_{ij}=g_i\cap g_j\ (i\ne j)$. The point $S_{ij}$ exists with probability 1.

If we now set $\varepsilon_{ij}=1$ if $S_{ij}$ is a corner of $\Pi_n$ and $\varepsilon_{ij}=0$ else, then it holds true that

$$(2.1)\quad X_n=\sum_{1\leqq i\lt j\leqq}\varepsilon_{ij}.$$

Let $W\,(n)$ be the probability for $S_{12}$ being a corner of $\Pi_n$. For reasons of symmetry the mathematical expectation turns out to be

$$(2.2)\quad E(X_n)=\binom{n}{2}\,W\,(n).$$

We first want to derive a general formula for $W\,(n)$. The point $S=S_{12}$ is a corner of $\Pi_n$ exactly if none of the lines $g_3,\,\ldots,\,g_n$ hits the convex hull $B_S$ of $B\cup S$. Let $l$ be the circumference of $K$, $b$ the one of $B$ and $l_S$ the one of $B_S$. According to Crofton's formula for convex regions (W. Blaschke $[1]$, § 3, (60))

$$(2.3)\quad \int_{g\,\cap K\ne\emptyset}dg=l$$

yields for the case $S\in K$

$$(2.4)\quad P\left(g_3\,\cap B_S\ne\emptyset\right)=\frac{l-l_S}{l-b}.$$

We decompose $W\,(n)$ into the two probabilities

$$(2.5)\quad W\,(n) = W_1(n)+W_2(n),$$

$$ (2.6)\quad W_1(n) = P\left(S\  \mathrm{corner\ of}\ \Pi_n,\, S\in K\right),$$

$$ (2.7)\quad W_1(n) = P\left(S\  \mathrm{corner\ of}\ \Pi_n,\, S\notin K\right).$$

It holds true that

$$(2.8)\quad W_1=\frac{1}{(l-b)^n}\iint_{g_1\,\cap\,g_2\,\cap \,K\ne\emptyset,\ (g_1\,\cup \,g_2)\cap B=\emptyset}(l-l_S)^{n-2}dg_1\,dg_2.$$

For $W_2(n)$ we give an estimation from which it will follow that $W_2(n)$ will be neglegible compared to $W_1(n)$. If $\mu$ denotes the line-measure then that yields

$$(2.9)\quad W_2\,(n)=\frac{1}{(l-b^n)}\iint_Df(S)^{n-2}dg_1\,dg_2$$

with $f(S)=\mu(g:\,g\,\cap\,B_S=\emptyset,\ g\,\cap\,K\ne\emptyset)$.  Integration is over the region $D$ of all line-pairs $g_1,\,g_2$ with $g_1\cap\,K\ne\emptyset,\,g_2\,\cap\,K\ne\emptyset,\,g_1\,\cap\,g_2\,\cap\,K=\emptyset,\,(g_1\,\cup\,g_2)\,\cap\,B=\emptyset$. In order to estimate $f(S)$ we chose a boundary point $R$ of $K$ that lies in $B_S$; then $B_R\subset B_S$ and consequently

$$(2,10)\quad f(S)\leqq f(R)=l-l_R=(l-b)-(l_R-b).$$





By cutting off from $B_R$ by means of an appropriate support-line (i.e. tangent to the boundary) and isosceles triangle (fig. 1) we get

$$(2.11)\quad l_R-b\geqq 2a-c=2a\left(1-\sin\frac{\varphi}{2}\right).$$

If $r$ denotes the distance of the boundaries of $B$ and $K$, then obviously $a\geqq r\gt 0$; further we have, if $\varphi$ is the angle under which $B$ is seen from a boundary point of $K$, $0\leqq\varphi\leqq\varphi_0\le\pi$; because lies completely inside the inner of $K$. So it holds true that

$$(2.12)\quad l-l_b\geqq l_R-b\geqq2r\left(1-\sin\frac{\varphi_0}{2}\right)=\varepsilon\gt 0.$$

From $(2.10)$ and $(2.12)$ follows

$$(2.13)\quad\frac{f(S)}{l-b}\leqq\frac{l-b-\varepsilon}{l-b}=\gamma\ \text{with}\ 0\lt\gamma\lt 1,$$

where $\gamma$ only depends on $B$ and $K$. We get

$$(2.14)\quad W_2(n)=\frac{\gamma^{n-2}}{(l-b)^2}\iint_{\begin{matrix}g_1\,\cap\,K\ne \emptyset,\,g_2\,\cap\,K\ne\emptyset \\ g_1\,\cap\,g_2\,\cap\,K=\emptyset \end{matrix}}dg_1\,dg_2.$$

After a formula of Crofton (W.Blaschke, $[1]$, § 7 ) one gets for the integral $(2.14)$

$$(2.15)\quad\iint\,dg_1\,dg_2 =l^2-2\,\pi\,F$$

where $F$ is the area of $K$. It follows

$$(2.16)\quad W_2(n)=O(\gamma^n)\quad\mathrm{with}\quad 0\lt\gamma\lt1 \,.$$

If the region $B$ degenerates to a point, one gets $(2.16)$ by an even simpler estimation. The thoughts show in general that the portion of line-pairs $g_1,\,g_2$, whose intersection point $S$ lies outside a fixed convex neighborhood $U$ of $B$, is of the order of magnitude $O(\gamma^n)$ where $\gamma$ with $0\lt\gamma\lt 1$ of course depends on the neighborhood $U$.

Theorem 1.  Let $B$ be a ( possibly degenrate ) convex region and $K$ a convex neighborhood of $B$. The probability for a corner of $\Pi_n$ to lie outside of $K$  satisfies  the relation

$$(2.17)\quad P(\,\mathrm{corner}\ \mathrm{of}\ \Pi_n\notin K )=O(\gamma^n)\quad(0\lt\gamma\lt 1)$$

where $\gamma$ is a constant depending on $K$ and $B$.

It remains to evaluate $(2.8)$. To this end we carry out, after W. Blaschke $[1]$, § 6, (89), the substitution

$$(2.18)\quad dg_1\,dg_2=\left|\sin(\varphi_1-\varphi_2)\right|\,d\varphi_1\,d\varphi_2\,dS\,;$$

here $\varphi_1$, $\varphi_2$ are the angles of $g_1$, resp. $g_2$ with a given fixed direction and, $dS$ the density of the intersection point $S=g_1\cap\,g_2$. Because

$$(2.19)\quad\int_0^\alpha\int_0^\alpha\left|\sin(\varphi_1-\varphi_2)\right|\,d\varphi_1\,d\varphi_2\,dS=2(\alpha-\sin\,\alpha)$$

we get, because we have to integrate over $\psi_1\leqq\varphi_1,\,\varphi_2\leqq\psi_2$,

$$(2.20)\quad W_1(n)=\frac{2}{(l-b)^2}\int_{S\in K\setminus B}\left(1-\frac{l_S-b}{l-b}\right)^{n-2}\left(\alpha(S)-\sin\alpha(S)\right)\,dS\,;$$

here $\alpha=\psi_2-\psi_1=\pi-\omega$ and $\omega$ is the angle under which $B$ is seen from $S$ ($fig.\ 2$). The evaluation of the integral under various preconditions on $B$ is carried out in §§ 3-5.

$$fig.\ 2$$

Before that, we investigate the probability for $\Pi_n$ not being closed. It could be suspected that the  polygon $\Pi_n$ doesn't enclose region $B$ also for larger $n$, i.e. isn't finite. That will happen particularly if $B$ comes close to the boundary of $K$ only at one side. Of course the probability that $\Pi_n$ isn't closed tends for $n\to\infty$ towards zero. We now want to estimate the order of magnitude of this convergence.

Let $\varphi_i$ be the angle of the normals of $g_i$, that are directed away from $B$, with a fixed direction. By $\psi_i$ we denote the ordered sample of the $\varphi_i$, i.e. the $\psi_i$ as well as the $\varphi_i$ are ordered according to magnitude: $0\leqq\psi_1\leqq\psi_2\leqq\cdots\leqq\psi_n\le 2\pi$. Let $\delta_i=\psi_i-\psi_{i-1}$ ($i=1,\,\ldots,\,n$), where  $\psi_0=\psi_n-2\pi$ shall be set. The polygon is not closed exactly if one of the angles $\delta_i\geqq\pi$ is. Consequently we first have to calculate the distribution function of the angle $\varphi$ under the condition $g\,\cap\,K\ne\emptyset,\  g\,\cap\,B=\emptyset$. If $p_0(\varphi)$ is the support function of $B$ and $p_1(\varphi)$ the one of  $K$, then it follows for $0\leqq x\leqq2\pi$

$$(2.21)\quad P(\varphi\leqq x)=\frac{1}{l-b}\int_0^x\int_{p_0(\varphi)}^{p_1(\varphi)}dp\,d\varphi=\frac{1}{l-b}\int_0^x\left(p_1(\varphi)-p_0(\varphi)\right)\,d\varphi\,.$$

This implies: If $p_1(\varphi)-p_0(\varphi)=r$ is constant, i.e. $K$is the outer parallel region at distance $r$ from $B$, then $\varphi$ is equally distributed on the unit circle and it holds true that

$$(2.22)\quad l-b=2\pi r$$

In this case the density of $\varphi$

$$(2.23)\quad f(\varphi)=\frac{p_1(\varphi)-p_(\varphi)}{l-b}$$

is constantly equal to $\frac{1}{2\pi}$; The probability for $\delta_i\geqq\pi$ is equal to the probability that $n-1$ angles $\psi_1,\,\ldots,\,\psi_{i-1},\,\psi_{i+1},\,\ldots,\,\psi_n$ lie between $\psi_i$ and $\psi_i+\pi$, i.e. equal to $2^{-(n-1)}$. As all possibilities $\delta_i\geqq\pi$ are mutually exclusive and equally likely, this yields (c.f. $[3]$)

$$(2.24)\quad P\,(\Pi_n\ \mathrm{not}\ \mathrm{closed})=\frac{n}{2^{n-1}}$$

(if $K$ is a parallel region of $B$).

In the general case it again holds true that

$$(2.25)\quad P\,(\Pi_n\ \mathrm{not}\ \mathrm{closed})=n\int_0^{2\pi}f(\varphi)\left(\int_{\varphi}^{\varphi+\pi}f(\Theta)\,d\Theta\right)^{n-1}d\varphi\,.$$

Now obviously

$$(2.26)\quad f(\varphi)=\frac{p_1(\varphi)-p_0(\varphi)}{l-b}\geqq c\gt0$$

therefore

$$(2.27)\quad \int_{\varphi}^{\varphi+\pi}f(\Theta)\,d\Theta\leqq 1-\pi\,c$$

where

$$(2.28)\quad \pi\,c\lt\int_0^{2\pi}f(\Theta)\,d\Theta=1$$

holds true. From $(2.25) and $(2.27)$ follows

Theorem 2. If $K$ is a parallel region of $B$ then  the probability that $\Pi_n$ is not closed is governed by relation $(2.24)$. If $B$ is contained in the inner of $K$, then for this probability in the general case it results in

$$(2.29)\quad P(\Pi_n\ \mathrm{not}\ \mathrm{closed})\leqq n\gamma^{n-1}$$

where $\gamma\,(0\lt\gamma\lt1)$ is a constant that depends on $B$ and $K$.



3. Random polygons around a point

Let $B=O\,\in\,K$ be a fixed point. Then $b=0$ and $l_S=2\left|\,O\,S\,\right|$ is equal to twice the length of the line segment $O\,S$. from $(2.28)$ follows

$$(3.1)\quad W_1=\frac{1}{l^2}\iint_{g_1\,\cap\,g_2\,\cap\,K\ne\emptyset}\left(1-\frac{2\left|\,O\,S\,\right|}{l}\right)^{n-2}dg_1\,dg_2$$

The condition $g_i\,\cap\,O=\emptyset$ need not be taken into consideration because the set of all through a point has measure zero. From $(2.20)$ follows, because in our case $\alpha=\pi$:

 $$(3.2)\quad W_1(n)=\frac{2\pi}{l^2}\int_{S\in K}\left(1-\frac{2\left|\,O\,S\,\right|}{l}\right)^{n-2}dS\,.$$

Let $0\lt r\lt\,l/2,\ r$ fixed. Then obviously

$$(3.3)\quad \frac{2\pi}{l^2}\int_{\begin{matrix}S\in K\\ \left|\,O\,S\,\right|\gt r\end{matrix}}\left(1-\frac{2\left|\,O\,S\,\right|}{l}\right)^{n-2}dS = O(\alpha^n),\quad 0\lt\alpha \lt1,$$

where $\alpha=1-(2r)/l$ has to be set. If $K_r$ denotes the circle of radius $r$ around $O,\ K_r\subset K$, it follows that

$$(3.4)\quad W_1(n)=\frac{2\pi}{l^2}\int_{S\in K_r}\left(1-\frac{2\left|\,O\,S\,\right|}{l}\right)^{n-2}dS + O(\alpha^n)$$

with $0\lt\alpha\lt1$. For polar coordinates $\varrho,\ \Theta$ we have $dS=\varrho\,d\varrho\,d\Theta$ and by a simple calculation we get

$$(3.5)\quad E(X_n)=\frac{n(n-1)}{2}W\,(n)=\frac{\pi^2}{2}+O(\gamma^n)\quad \mathrm{with}\quad 0\lt\gamma\lt 1\,.$$

Theorem 3. The mathmatical expectation of the number $X_n$ of corners of a random convex polygon $\Pi_n$ around a point $O$ of a convex set $K$ satisfies the relation $(3.5)$.



4. Ringshaped areal around a smooth region

Concerning $B$ we now assume that the boundary curve is convex and sufficiently often continuously differentiable. Formula $(2.20)$ has to be evaluated under that precondition. In order to estimate the values $\alpha(S)$ and $l_S-b$ we first chose appropriate coordinates $t,\,s$. On the boundary $\mathscr{B}$ of $B$ we introduce the arclength $s$ as the parameter. We orient $\mathscr{B}$ counterclockwise. Let $x=f\,(s),\ y=g\,(s)$  be the equation of $\mathscr{B},\ \mathfrak{t}=\lbrace f'(s),\,g'(s)\rbrace$ the tangential vector and $\mathfrak{n}=\lbrace g',\,-f'\rbrace$ the outer normal vector; the primes denote derivation with respect to $s$. It is then $[\mathfrak{n},\,\mathfrak{t}]=1$ for the determinant of $\mathfrak{n},\,\mathfrak{t}$. The normals

$$(4.1)\quad \frac{\partial(x,\,y)}{\partial(t,\,s)}=1+t\,k(s)\gt 0\quad\mathrm{for}\quad t\gt-\frac{1}{k(s)}\,;$$

here $k(s)\,\geqq\,0$ denotes the curvature of $\mathscr{B}$ in the point $S$. For $dS$ follows

$$(4.3)\quad dS=(1+t\,k(s))\,dt\,ds\,.$$

We now consider a fixed point $Y_0$ of $\mathscr{B}$, for example $s_0=0$, and draw from an outer point $S$ on the normal through $Y_0$ the tangents to $\mathscr{B}$, which shall touch $\mathscr{B}$ in the points $Y\,(\sigma_\alpha),\ \alpha=1,\,2$  (fig. 3). For calculating approximate expressions for the values $\sigma_\alpha$ and $\tau_\alpha=\left|Y_\alpha\,S\right|$ as a function of $t$, we express the curve $\mathscr{B}$ with respect to the accompanying bipod (i.e. in its local Frenet frame) $\mathfrak{n},\ \mathfrak{t}$ in point $Y_0$:

$$\quad\quad\mathfrak{x}=\mathfrak{t}\left(s-\frac{k^2}{3!}s^3-\frac{3k\,k'}{4!}+O(s^5)\right)$$
$$(4.4)$$
$$\quad\quad-\mathfrak{n}\left(\frac{k}{2!}s^2+\frac{k'}{3!}s^3+(k''-k^3)\frac{s^4}{4!}+O(s^5)\right)\,.$$

For the intersection point $S$ of the tangent at $\mathscr{B}$ in point $Y\,(\sigma_\alpha)$ with the normal through $Y_0$ we have to evaluate the relation

$$(4.5)\quad\mathfrak{\sigma}+\tau\,\mathfrak{x}'(\sigma)'=t\mathfrak{n}$$

If we take for $\tau$ an expansion

$$(4.6)\quad\tau=A\,\sigma+B\,\sigma^2+C\,\sigma^3+D\,\sigma^4+O(\sigma^5)$$

and enter it into $(4.5)$, we get, after partitioning into the components related to $\mathfrak{t}$, $\mathfrak{n}$, two scalar equations. From the $\mathfrak{t}$-component follows

$$(4.7)\quad \tau=-\sigma-\frac{k^2}{3}\sigma^3-\frac{3}{8}k\,k'\sigma^4+O(\sigma^5)\,.$$

By comparing the coefficients of the $\mathfrak{n}$-component one gets, when taking into account $(4.7)$:

$$(4.8)\quad t=\frac{k}{2}\sigma^2+\frac{k'}{3}\sigma^3+(3k''+5\,k^3)\,\frac{\sigma^4}{4!}+O(\sigma^5)\,.$$

If we now set $t=u^2$ then an ansatz analog to $\sigma=\sigma(u)$ in $(4.8)$:

$$(4.9)\quad\sigma_{1,\,2}(u)=\pm\sqrt{\frac{2}{k}}u-\frac{2}{3}\frac{k'}{k^2}u2\pm\frac{1}{3}\sqrt{\frac{k}{2}}\left(\frac{10}{3}\frac{k'^2}{k^4}\,-\,\frac{3}{2}\frac{k''}{k^3}-\frac{5}{2}\right)u^3+O(u^4)\,.$$

That expansion makes the precondition $k\gt0$ for $\mathscr{B}$ necessary; the boundary of $B$ must not contain a line-point (Translator's Note: I guess that "Streckpunkt" means a point where the curvature vanishes) and most of all no line segment. The two signs correspond to the two tangents from $S$ to $\mathscr{B}$. Now we can evaluate the integral $(2.20)$, taking into account $(4.3)$. Accounting for the signs of the calculated lengths (fig. 3) it hold true according to $(4.7)$ that:

$$(4.10)\quad l_S-b=(\tau_2+\sigma_2)-(\tau_1-\sigma_1)=\frac{k^2}{3}(\sigma_1^3-\sigma_2^3)+\frac{3}{8}k\,k'\,(\sigma_1^4-\sigma_2^4)+O(\sigma^5)\,.$$

Because of $(4.9)$ we get

$$(4.11)\quad l_S-b=\frac{4}{3}\sqrt{2\,k}\,u^3+O(u^5)\,.$$

For $\alpha-\sin\,\alpha$ we get because of

$$(4.12)\quad\alpha(s,t)=\int_{\sigma_2}^{\sigma_1}k(\sigma)\,d\sigma$$

and taking into account $(4.9)$

$$(4.13)\quad\alpha-\sin\,\alpha=\frac{1}{3!}\left(2\sqrt{2\,k}\,u\right)^3+O(u^4)\,.$$

The integral $(2.20)$ that shall be estimated becomes, because $u=t^{1/2}$, after inserting the obtained expressions $(4.3),\ (4.11),\ (4.13)$

$$W_1(n)=\frac{2}{(l-b)^2}\int_0^b\int_0^{h(s)}\left(1-\frac{4\sqrt{2\,k}\,t^{3/2}}{3\,(l-b)}+O(t^{5/2})\right)^{n-2}\left(\frac{8}{3!}\left(\sqrt{2\,k\,t}\right)^3+O(t^2)\right)(1+tk)\,dt\,ds\,.$$

If we now substitute

$$(4.14)\quad t=\left(\frac{3\,(l-b)}{4\sqrt{2\,k}}\frac{x}{n}\right)^{2/3}$$

that yields after some rearranging

$$(4.15)\quad W_1(n)=2\left(\frac{2}{3\,(l-b)} \right)^{1/3}\int_0^bk^{2/3}\int_0^\infty\left(1-\frac{x}{n}\right)^n\frac{x^{2/3}}{n^{5/3}}\,dx\,ds+O\left(\frac{1}{n^2}\right)\,.$$

From this follows

Theorem 4. Let $B$ be a convexr finite region with smooth boundary, whose curvature $k=k(s)$ is positive and finite. $B$ be in the inner of a convex set $K$; $l$ and $b$ be the circumference of $K$, resp. $B$. For the mathematical expectation of the number of corners of a random convex polygon* $\Pi_n$ around $B$  it then holds true that

$$(4.16)\quad E(X_n)=\left[\left(\frac{2}{3\,(l-b)}\right)^{1/3}\Gamma\left(\frac{5}{3}\right)\int_0^bk^{2/3}\,ds\right]n^{1/3}+O(1)\,.$$

Consequently the order of magnitude of the number of corners is the same as in the case of the convex hull of $n$ points that are randomly chosen in $B$ (cf A.\,Rényi, R.\, Sulanke $[2]$), the factors are however significantly different.



5. Ringshaped areal around a convex polygon

Let $B$ now be a convex $r$-gon. According to theorem 1 the random polygon $\Pi_n$ lies with high probability in an arbitrary, fixed convex  surrounding $U$ of $B$; $U$ shall be selected in a way that all intersection points of non-adjacent sides of $B$ are located outside of $U$. The ring-shaped areal $U\,\setminus\,B$, for which the integral $(2.20)$ must be evaluated is partitioned by the sides of $B$ into $r$ corner-regions $E_i$ and $r$ side-regions $T_i$ (fig. 4), in which we carry out the integration separately.

$T$ be one of the side-regions with corners $A,\,A'$ at a side of length $2\,c=\left|\,A\,A'\,\right|$ . For $S\in T$ it holds true that

$$(5.1)\quad l_S-b=\left|\,S\,A\,\right|+\left|\,S\,A'\,\right|-\left|\,A\,A'\,\right|=2\,(a-c)\ ,$$

where a is the semi-major axis of the ellipse with focal points $A,\ A'$ through the point $S$. As coordinates of $S$ we chose $a$ and the distance $x$ of the projection of $S$ onto the major axis of the ellipse from its center. For the area-element $dS$ we obtain in these coordinates

$$(5.2)\quad dS=\frac{a^4-c^2x^2}{a^2\sqrt{(a^2-c^2)(a^2-x^2)}}\,dx\,da\,.$$

For the angle $\alpha$ that is inserted into $(2.20)$ the outer angles of the triangle $A\,A'\,S$ in $S_i$, one calculates

$$(5.3)\quad\sin\,\alpha=\frac{2\,a\,c\sqrt{(a^2-c^2)(a^2-x^2)}}{a^4-c^2x^2}=f(x,\,a)\,.$$

We now replace the region $T$ with a section of the half-circle over $A,\,A'$ that is adjacent to $A\,A'$ and lies in $U$ and in which $\alpha\leqq\pi/2$n; we will later estimate the error that is generated by this. The is determined by $f=1$; for $x,\,a$ we get the integration-region

$$(5.4)\quad c\leqq a\leqq\delta c,\quad\left|x\right|\leqq\frac{a}{c}\sqrt{2\,c^2-a^2}\,,$$

here $\delta\ (1\lt\delta\leqq\sqrt{2})$ is a number that is chosen in a way that the  circle-segment lies in $U$. According to $(2.20)$ the integral

$$(5.5)\quad W=\frac{8\,c}{(l-b)^2}\int_c^{\delta\,c}\int_0^{(a/c)\sqrt{2\,c^2-a^2}}\left(1-\frac{2\,(a-c)}{l-b}\right)^{n-2}\left(\frac{\mathrm{arc}\sin\,f\ -\ f}{a\,f}\right)\,dx\,da$$

has to be calculated first. To that end we develop the inner integral

$$(5.6)\quad F(a) =\int_0^{(a/c)\sqrt{2\,c^2-a^2}}\frac{1}{f}(\mathrm{arc}\sin\,f\ -\ f)\,dx$$

according to powers of $a-c$ and set

$$(5.7)\quad\frac{1}{f}(\mathrm{arc}\sin\,f\ -\ f)=\frac{1}{6}f^2+R$$

The integral over the first part yields

$$(5.8)\quad\frac{1}{6}\int_0^{(a/c)\sqrt{2\,c^2-a^2}}f^2dx=-\frac{a^4-c^4}{6\,a^2c}\log(a-c)+O(a-c)\,.$$

For the rest $R$ we show

$$(5.9)\quad\int_0^{(a/c)\sqrt{2\,c^2-a^2}}R\,dx=O(a-c)\,.$$

It holds true that, if

$$\quad\mathrm{arc}\sin\,\xi=\sum_{v=0}^\infty c_v\xi^{2v+1}$$

is set,

$$(5.10)\quad 0\lt R=\sum_{v=2}^\infty c_vf^{2v}\leqq f^4\sum_{v=2}^\infty c_v=f^4\left(\frac{\pi}{2}-\frac{7}{6}\right)\,.$$

Therefore it suffices to prove

$$\quad\int_0^{(a/c)\sqrt{2\,c^2-a^2}}f^4dx=(a-c)\,,$$

that is,

$$(5.11)\quad\int_0^{(a/c)\sqrt{2\,c^2-a^2}}\frac{(a^2-c^2)^2}{(a^4-c^2\,x^2)^4}dx=O\left(\frac{1}{a-c}\right)\,.$$

Now, because $0\leqq x\leqq c\leqq a$

$$(5.12)\quad\frac{(a-x)^2}{16\,a^2\,(a^2-c\,x)^4}\leqq\frac{(a^2-x^2)^2}{(a^4-c^2\,x^2)^4}\leqq\frac{4\,(a-x)^2}{a^6\,(a^2-c\,x)^4}\,.$$

Therefore it remains to show

$$(5.13)\quad\int_0^{(a/c)\sqrt{2\,c^2-a^2}}\frac{(a^2-x^2)^2}{(a^2-c\,x)^4}dx=O\left(\frac{1}{a-c}\right)$$

One easily obtains that relationeasily via the substitution $a^2-c\,x=t$ and some simple estimations. From $(5.6)-(5.9)$ we get

$$(5.14)\quad F(a)=-\frac{a^4-c^4}{6\,a^2\,c}\log\,(a-c)+O(a-c)\,.$$

According to $(5.5)$ it therefore holds true that

$$(5.15)\quad=\frac{-4}{3\,(l-b)^2}\int_0^{\delta c}\left(1-\frac{2\,(a-c)}{(l-b)}\right)^{n-2}\left(\frac{a^4-c^4}{a^3}\log\,(a-c)+O(a-c)\right)\,da\,.$$

The substitution

$$\quad\frac{2\,(a-c)}{l-b}=\frac{Z}{n-2}$$

yields after some simple calculations because of

$$(5.16)\quad\int_c^{\delta c}\left(1-\frac{2\,(a-c)}{(l-b)}\right)^{n-2}\cdot\, O(a-c)\,da=O\left(\frac{1}{n^2}\right)$$

the relation

$$(5.17)\quad W=\frac{4}{3\,n\,(n-1)}\log\,(n-2)+O\left(\frac{1}{n^2}\right)\,.$$

When replacing the side-region $T$ with a half-circle section, we have either integrated a region that is bound by the line of the neighboring side and a circular arc, too much (fig. 5 a) or too little (fig. 5 b).

We show that the errors that are generated by this are of the order of magnitude $O(1/n^2)$. Let

$$(5.18)\quad x(a)=c+(a-c)\,\gamma+O\left((a-c)^2\right)$$

be a representation of the neighboring side. The error in the first case (fig. 5 a) then is

$$(5.19)\quad\Delta=q\int_c^{\delta c}\left(1-\frac{2\,(a-c)}{(l-b)}\right)^{n-2}\frac{1}{a^2\,\sqrt{a^2-c^2}}\int_{x(a)}^{(a/c)\sqrt{2\,c^2-a^2}}(\alpha-\sin\,\alpha)\frac{a^4-c^2\,x^2}{\sqrt{a^2-x^2}}\,dx\,da\,;$$

here $q$ denotes a constant. Because of $(5.16)$ it suffices to show that

$$(5.20)\quad I(a)=\int_{x(a)}^{(a/c)\sqrt{2\,c^2-a^2}}(\alpha-\sin\,\alpha)\frac{a^4-c^2\,x^2}{\sqrt{a^2-x^2}}dx=O\left((a-c)^{3/2}\right)$$

holds. Now $\alpha-\sin\,\alpha$ is bound, so that it suffices to prove

$$(5.21)\quad\int_{x(a)}^{(a/c)\sqrt{2\,c^2-a^2}}\frac{a^4-c^2\,x^2}{\sqrt{a^2-x^2}}dx=O\left((a-c)^{3/2}\right)$$

For the indefinite integral

$$(5.22)\quad Q(x)=\int\frac{a^4-c^2\,x^2}{\sqrt{a^2-x^2}}dx=\frac{c^2\,x}{2}\sqrt{a^2-x^2}-a^2\,\left(a^2-\frac{c^2}{2}\right)\,\mathrm{arc}\cos\,\frac{x}{a}$$

we get, because $\mathrm{arc}\cos\frac{x}{a}=\mathrm{arc}\sin\frac{1}{a}\sqrt{a^2-x^2}$ the series expansion

$$(5.23)\quad Q(x)=\frac{1}{2}\sqrt{a^2-x^2}\,(c^2x-a^3+a(c^2-a^2)+O(a^2-x^2))\,.$$

Substituting the lower bound $x=x(a)$ according to $(5.18)$ immediately yields

$$(5.24)\quad Q(x(a))=O\left((a-c)^{3/2}\right)$$

But the same also holds for the upper bound, because the expression that is to be substituted also is of the form $(5.18)$, of course with a different constant $\gamma$. Quite analogously one also estimates the second error (fig. 5 b). Thus we may replace in $(5.17)$ the half-circle section with the side-region $T$ and alltogether get

$$(5.25)\quad W\,(T)=\frac{4}{3\,n\,(n-1)}\log\,n+O\left(\frac{1}{n^2}\right)\,.$$

This formula is also valid if $B$ degenerates to a line-segment.

Now we consider the corner-region $E=E_i$ at the corner $A_i$ of $B$. We now introduce, as in $(5.2)$, semi-elliptic coordinates; only the basis is now the line-segment $A_{i-1}\,A_{i+1}$, whose length will again be denoted by $2\,c$. With

$$\quad d=\frac{1}{2}(\left|A_{i-1}A_i\right|+\left|A_i A_{i+1}\right|)$$

we have for the difference of distance

$$(5.26)\quad l_S-b=2\,(a-d)\,.$$

Therefore, according to $(2.20)$ and $(5.2)$, for the corresponding probablity

$$(5.27)\quad W\,(E)=\frac{2}{(l-b)^2}\int_d^{a_0}\left(1-\frac{2\,(a-d)}{(l-b)}\right)^{n-2}\int_{x_1(a)}^{x_2(a)}(\alpha-\sin\,\alpha)\frac{a^4-c^2\,x^2}{a^2\sqrt{(a^2-c^2)(a^2-x^2)}}\,dx\,da\,.$$

Here $x_1(a),\ x_2(a)$ denote the $x$-coordinates of the intersection point of the ellipse that belongs to $a$ with the elongations of the sides that are adjacent to $A_i$ beyond $A_i$. As we only consider a sufficiently small surrounding of $B$, it holds true that

$$\quad\left|x\right|\leqq\max\left(\left|x_1(a)\right|,\,\left|x_1(a)\right|\right)\lt a,\quad c\lt d\leqq a\,.$$

From the mean value theorem follows, because of the boudedness and continuity of the integrand,

$$(5.28)\quad \int_{x_1(a)}^{x_2(a)}(\alpha-\sin\,\alpha)\frac{a^4-c^2\,x^2}{a^2\sqrt{(a^2-c^2)(a^2-x^2)}}dx=M(a)\,(x_2(a)-x_1(a))\,,$$

where $M(a)$ remains bounded for all $a$ from the range under consideration: $\left|\,M(a)\,\right|\leqq M_0\,.$

For $a=d$ it holds $x_1(d)=x_2(d)$. The functions  $x_i(a)$ are sufficiently often differentiable in location $d$. It follows

$$(5.29)\quad x_2(a)-x_1(a)=h_0(a-d)+O\left((a-d)^2\right)\,,$$

where $h_0$ is a certain constant. If one inserts $(5.28),\ (5.29)$ into $(5.27)$, then according to $(5.16)$ follows immediately

$$(5.30)\quad W\,(E)=O\left(\frac{1}{n^2}\right)\,.$$

Because of theorem 1, $(5.25)$ and $(5.30)$ we get the following

Theorem 5.  Let $B$ a convex $r$-gon, $r\geqq2$, that lies in the inner of $K$.For the mathematical expectation of the number of corners $X_n$ of a random polygon $\Pi_n$ it holds true that

$$\quad E(X_n)=\frac{2\,r}{3}\,\log n+O(1)\,.$$

The principal term of this formula matches the corresponding principal term of theorem 1of our work $[2]$ on the convex hull of random points that lie in a polygon.



References

1. Blaschke, W.: Vorlesungen über Integralgeometrie. 3. Aufl. Berlin: VEB Deutscher Verlag der Wissenschaften 1955.

2. Rényi, A., u. R. Sulanke: Über die konvexe Hülle von $n$ zufällig gewählten Punkten. Z. Wahrscheinlichkeitstheorie verw. Geb. 2, 75-84 (1963).

3. Stevens, W.L.: Solution to a geometrical problem in probability. Ann. Eugenics 9, 315-320 (1939.

   Dr. R. Sulanke
   Mathematisches Institut der
   Humboldt-Universität
   Berlin

   Prof. Dr. A. Rényi
   Mathematisches Institut der Ungarischen
   Akademie der Wissenschaften
   Reáltonada u. 13-15
   Budapest V, Ungarn

No comments: