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Tight bounds on the maximal perimeter of convex equilateral small polygons

Christian Bingane Department of Mathematics and Industrial Engineering, Polytechnique Montreal, Montreal, Quebec, Canada, H3C 3A7. Emails: christian.bingane@polymtl.ca, charles.audet@polymtl.ca    Charles Audet11footnotemark: 1
Abstract

A small polygon is a polygon that has diameter one. The maximal perimeter of a convex equilateral small polygon with n=2sn=2^{s} sides is not known when s4s\geq 4. In this paper, we construct a family of convex equilateral small nn-gons, n=2sn=2^{s} and s4s\geq 4, and show that their perimeters are within O(1/n4)O(1/n^{4}) of the maximal perimeter and exceed the previously best known values from the literature. In particular, for the first open case n=16n=16, our result proves that Mossinghoff’s equilateral hexadecagon is suboptimal.

Keywords

Planar geometry, equilateral polygons, isodiametric problem, maximal perimeter

1 Introduction

The diameter of a polygon is the largest distance between any pair of its vertices. A polygon is called small if its diameter equals one. We recall that an equilateral polygon is a polygon that has all sides of the same length and a regular polygon is an equilateral polygon whose interior angles are equal. For an integer n3n\geq 3, the problem of finding the maximal perimeter of a convex small nn-gon was investigated by Reinhardt [1] in 1922, Vincze [2] in 1950, and Datta [3] in 1997. They proved that for n3n\geq 3

  • the value 2nsinπ2n2n\sin\frac{\pi}{2n} is an upper bound on the perimeter of any convex small nn-gon;

  • the regular small nn-gon is an optimal solution only when nn is odd;

  • there are finitely many optimal solutions [4, 5, 6] when nn has an odd factor and these solutions are all equilateral.

When nn is a power of 22, the maximal perimeter problem is solved for n=4n=4 and n=8n=8. The case n=4n=4 was solved by Tamvakis [7] in 1987 and the case n=8n=8 by Audet, Hansen, and Messine [8] in 2007. Both optimal 44-gon and 88-gon, shown respectively in Figure 1b and Figure 3d, are not equilateral. For n=2sn=2^{s} with integer s4s\geq 4, exact solutions in the maximal perimeter problem appear to be presently out of reach. However, tight lower bounds may be obtained analytically. Recently, Bingane [9, 10] constructed a family of convex non-equilateral small nn-gons, for n=2sn=2^{s} with s4s\geq 4, and proved that the perimeters obtained cannot be improved for large nn by more than π9/(8n8)\pi^{9}/(8n^{8}).

The diameter graph of a polygon is the graph with the vertices of the polygon, and an edge between two vertices exists only if the distance between these vertices equals the diameter. Figure 1, Figure 2, and Figure 3 represent diameter graphs of some convex small polygons. The solid lines illustrate pairs of vertices which are unit distance apart. Vincze [2] studied the problem of finding the minimal diameter of a convex polygon with unit-length sides. This problem is equivalent to the equilateral case of the maximal perimeter problem. He showed that a necessary condition of a convex equilateral small polygon to have maximal perimeter is that each vertex should have an opposite vertex at a distance equal to the diameter. It is easy to see that for n=4n=4, the maximal perimeter of a convex equilateral small 44-gon is only attained by the regular 44-gon. Vincze also described a convex equilateral small 88-gon, shown in Figure 3b, with longer perimeter than that of the regular 88-gon. In 2004, Audet, Hansen, Messine, and Perron [11] used both geometrical arguments and methods of global optimization to determine the unique convex equilateral small 88-gon with the longest perimeter, illustrated in Figure 3c.

For n=2sn=2^{s} with integer s4s\geq 4, the equilateral case of the maximal perimeter problem remains unsolved and, as in the general case, exact solutions appear to be presently out of reach. In 2008, Mossinghoff [12] constructed a family of convex equilateral small nn-gons, for n=2sn=2^{s} with s4s\geq 4, whose perimeters differ from the upper bound 2nsinπ2n2n\sin\frac{\pi}{2n} by just O(1/n4)O(1/n^{4}). By contrast, the perimeter of a regular small nn-gon differs by O(1/n2)O(1/n^{2}) when n4n\geq 4 is even. In the present paper, we propose tighter lower bounds on the maximal perimeter of convex equilateral small nn-gons when n=2sn=2^{s} and integer s4s\geq 4 by a constructive approach. Thus, our main result is the following:

Theorem 1.

Suppose n=2sn=2^{s} with integer s4s\geq 4. Let L¯n:=2nsinπ2n\overline{L}_{n}:=2n\sin\frac{\pi}{2n} denote an upper bound on the perimeter L(𝙿n)L(\mathtt{P}_{n}) of a convex small nn-gon 𝙿n\mathtt{P}_{n}. Let 𝙼n\mathtt{M}_{n} denote the convex equilateral small nn-gon constructed by Mossinghoff [12]. Then there exists a convex equilateral small nn-gon 𝙰n\mathtt{A}_{n} such that

L¯nL(𝙰n)=π4n4+O(1n5)\overline{L}_{n}-L(\mathtt{A}_{n})=\frac{\pi^{4}}{n^{4}}+O\left(\frac{1}{n^{5}}\right)

and

L(𝙰n)L(𝙼n)=2π4n4+O(1n5)>0.L(\mathtt{A}_{n})-L(\mathtt{M}_{n})=\frac{2\pi^{4}}{n^{4}}+O\left(\frac{1}{n^{5}}\right)>0.

In addition, we show that the resulting polygons for n=32n=32 and n=64n=64 are not optimal by providing two convex equilateral small polygons with longer perimeters.

The remainder of this paper is organized as follows. Section 2 recalls principal results on the maximal perimeter of convex small polygons. Section 3 considers the polygons 𝙰n\mathtt{A}_{n} and shows that they satisfy Theorem 1. Section 4 shows that the polygons 𝙰32\mathtt{A}_{32} and 𝙰64\mathtt{A}_{64} are not optimal by constructing a 3232-gon and a 6464-gon with larger perimeters. Concluding remarks are presented in Section 5.

(a) (𝚁4,2.828427)(\mathtt{R}_{4},2.828427)
(b) (𝚃4,3.035276)(\mathtt{T}_{4},3.035276)
Figure 1: Two convex small 44-gons (𝙿4,L(𝙿4))(\mathtt{P}_{4},L(\mathtt{P}_{4})): (a) Regular 44-gon; (b) Tamvakis 44-gon [7]
(a) (𝚁6,3)(\mathtt{R}_{6},3)
(b) (𝚁3,6,3.105829)(\mathtt{R}_{3,6},3.105829)
Figure 2: Two convex equilateral small 66-gons (𝙿6,L(𝙿6))(\mathtt{P}_{6},L(\mathtt{P}_{6})): (a) Regular 66-gon; (b) Reinhardt 66-gon [1]
(a) (𝚁8,3.061467)(\mathtt{R}_{8},3.061467)
(b) (𝚅8,3.090369)(\mathtt{V}_{8},3.090369)
(c) (𝙷8,3.095609)(\mathtt{H}_{8},3.095609)
(d) (𝙱8,3.121147)(\mathtt{B}_{8}^{*},3.121147)
Figure 3: Four convex small 88-gons (𝙿8,L(𝙿8))(\mathtt{P}_{8},L(\mathtt{P}_{8})): (a) Regular 88-gon; (b) Vincze 88-gon [2]; (c) Optimal equilateral 88-gon [11]; (d) Optimal non-equilateral 88-gon [8]

2 Perimeters of convex equilateral small polygons

Let L(𝙿)L(\mathtt{P}) denote the perimeter of a polygon 𝙿\mathtt{P}. For a given integer n3n\geq 3, let 𝚁n\mathtt{R}_{n} denote the regular small nn-gon. We have

L(𝚁n)={2nsinπ2nif n is odd,nsinπnif n is even.L(\mathtt{R}_{n})=\begin{cases}2n\sin\frac{\pi}{2n}&\text{if $n$ is odd,}\\ n\sin\frac{\pi}{n}&\text{if $n$ is even.}\\ \end{cases}

When nn has an odd factor mm, consider the family of convex equilateral small nn-gons constructed as follows:

  1. 1.

    Transform the regular small mm-gon 𝚁m\mathtt{R}_{m} into a Reuleaux mm-gon by replacing each edge by a circle’s arc passing through its end vertices and centered at the opposite vertex;

  2. 2.

    Add at regular intervals n/m1n/m-1 vertices within each arc;

  3. 3.

    Take the convex hull of all vertices.

These nn-gons are denoted 𝚁m,n\mathtt{R}_{m,n} and L(𝚁m,n)=2nsinπ2nL(\mathtt{R}_{m,n})=2n\sin\frac{\pi}{2n}. The 66-gon 𝚁3,6\mathtt{R}_{3,6} is illustrated in Figure 2b.

Theorem 2 (Reinhardt [1], Vincze [2], Datta [3]).

For all n3n\geq 3, let LnL_{n}^{*} denote the maximal perimeter among all convex small nn-gons, n\ell_{n}^{*} the maximal perimeter among all equilateral ones, and L¯n:=2nsinπ2n\overline{L}_{n}:=2n\sin\frac{\pi}{2n}.

  • When nn has an odd factor mm, n=Ln=L¯n\ell_{n}^{*}=L_{n}^{*}=\overline{L}_{n} is achieved by finitely many equilateral nn-gons [4, 5, 6], including 𝚁m,n\mathtt{R}_{m,n}. The optimal nn-gon 𝚁m,n\mathtt{R}_{m,n} is unique if mm is prime and n/m2n/m\leq 2.

  • When n=2sn=2^{s} with s2s\geq 2, L(𝚁n)<Ln<L¯nL(\mathtt{R}_{n})<L_{n}^{*}<\overline{L}_{n}.

When n=2sn=2^{s}, both LnL_{n}^{*} and n\ell_{n}^{*} are only known for s3s\leq 3. Tamvakis [7] found that L4=2+62L_{4}^{*}=2+\sqrt{6}-\sqrt{2}, and this value is only achieved by 𝚃4\mathtt{T}_{4}, represented in Figure 1b. Audet, Hansen, and Messine [8] proved that L8=3.121147L_{8}^{*}=3.121147\dots, and this value is only achieved by 𝙱8\mathtt{B}_{8}^{*}, represented in Figure 3d. For the equilateral quadrilateral, it is easy to see that 4=L(𝚁4)=22\ell_{4}^{*}=L(\mathtt{R}_{4})=2\sqrt{2}. Audet, Hansen, Messine and Perron [11] studied the equilateral octagon and determined that 8=3.095609>L(𝚁8)=422\ell_{8}^{*}=3.095609\ldots>L(\mathtt{R}_{8})=4\sqrt{2-\sqrt{2}}, and this value is only achieved by 𝙷8\mathtt{H}_{8}, represented in Figure 3c. If u:=82/64u:={\ell_{8}^{*}}^{2}/64 denotes the square of the sides length of 𝙷8\mathtt{H}_{8}, we can show that uu is the unique root of the polynomial equation

2u618u5+57u478u3+46u212u+1=02u^{6}-18u^{5}+57u^{4}-78u^{3}+46u^{2}-12u+1=0

that belongs to (sin2(π/8),4sin2(π/16))(\sin^{2}(\pi/8),4\sin^{2}(\pi/16)). Note that the following inequalities are strict: 4<L4\ell_{4}^{*}<L_{4}^{*} and 8<L8\ell_{8}^{*}<L_{8}^{*}.

For n=2sn=2^{s} with s4s\geq 4, exact solutions of the maximal perimeter problem appear to be presently out of reach. However, tight lower bounds may be obtained analytically. Recently, Bingane [9, 10] proved that, for n=2sn=2^{s} with s4s\geq 4,

Ln2nsinπ2ncos(12arctan(tan2πntanπn)12arcsin(sin(2π/n)sin(π/n)4sin2(π/n)+cos(4π/n))),L_{n}^{*}\geq 2n\sin\frac{\pi}{2n}\cos\left(\frac{1}{2}\arctan\left(\tan\frac{2\pi}{n}\tan\frac{\pi}{n}\right)-\frac{1}{2}\arcsin\left(\frac{\sin(2\pi/n)\sin(\pi/n)}{\sqrt{4\sin^{2}(\pi/n)+\cos(4\pi/n)}}\right)\right),

which implies

L¯nLnπ98n8+O(1n10).\overline{L}_{n}-L_{n}^{*}\leq\frac{\pi^{9}}{8n^{8}}+O\left(\frac{1}{n^{10}}\right).

On the other hand, Mossinghoff [12] constructed a family of convex equilateral small nn-gons 𝙼n\mathtt{M}_{n}, illustrated in Figure 4, such that

L¯nL(𝙼n)=3π4n4+O(1n5)\overline{L}_{n}-L(\mathtt{M}_{n})=\frac{3\pi^{4}}{n^{4}}+O\left(\frac{1}{n^{5}}\right)

and

L(𝙼n)L(𝚁n)=π38n2+O(1n4)>0L(\mathtt{M}_{n})-L(\mathtt{R}_{n})=\frac{\pi^{3}}{8n^{2}}+O\left(\frac{1}{n^{4}}\right)>0

for n=2sn=2^{s} with s4s\geq 4. The next section proposes tighter lower bounds for n\ell_{n}^{*}.

(a) (𝙼16,3.134707)(\mathtt{M}_{16},3.134707)
(b) (𝙼32,3.140134)(\mathtt{M}_{32},3.140134)
Figure 4: Mossinghoff polygons (𝙼n,L(𝙼n))(\mathtt{M}_{n},L(\mathtt{M}_{n})): (a) Hexadecagon 𝙼16\mathtt{M}_{16}; (b) Triacontadigon 𝙼32\mathtt{M}_{32}

3 Proof of Theorem 1

Cartesian coordinates are used to describe an nn-gon 𝙿n\mathtt{P}_{n}: a vertex 𝚟i\mathtt{v}_{i}, i=0,1,,n1i=0,1,\ldots,n-1, is positioned at abscissa xix_{i} and ordinate yiy_{i}. Sums or differences of the indices of the coordinates are taken modulo nn. Placing the vertex 𝚟0\mathtt{v}_{0} at the origin, we set x0=y0=0x_{0}=y_{0}=0. We also assume that the nn-gon 𝙿n\mathtt{P}_{n} is in the half-plane y0y\geq 0 and the vertices 𝚟i\mathtt{v}_{i}, i=1,2,,n1i=1,2,\ldots,n-1, are arranged in a counterclockwise order as illustrated in Figure 5, i.e., xiyi+1yixi+1x_{i}y_{i+1}\geq y_{i}x_{i+1} for all i=1,2,,n2i=1,2,\ldots,n-2.

The nn-gon 𝙿n\mathtt{P}_{n} is small if maxi,j𝚟i𝚟j=1\max_{i,j}\|\mathtt{v}_{i}-\mathtt{v}_{j}\|=1. It is equilateral if 𝚟i𝚟i1=c\|\mathtt{v}_{i}-\mathtt{v}_{i-1}\|=c for all i=1,2,,ni=1,2,\ldots,n. Imposing that the determinants of the 2×22\times 2 matrices satisfy

σi:=|xixi1xi+1xi1yiyi1yi+1yi1|0\sigma_{i}:=\begin{vmatrix}x_{i}-x_{i-1}&x_{i+1}-x_{i-1}\\ y_{i}-y_{i-1}&y_{i+1}-y_{i-1}\end{vmatrix}\geq 0

for all i=1,2,,n1i=1,2,\ldots,n-1 ensures the convexity of the nn-gon.

𝚟0(0,0)\mathtt{v}_{0}(0,0)𝚟1(x1,y1)\mathtt{v}_{1}(x_{1},y_{1})𝚟2(x2,y2)\mathtt{v}_{2}(x_{2},y_{2})𝚟3(x3,y3)\mathtt{v}_{3}(x_{3},y_{3})𝚟4(x4,y4)\mathtt{v}_{4}(x_{4},y_{4})𝚟5(x5,y5)\mathtt{v}_{5}(x_{5},y_{5})𝚟6(x6,y6)\mathtt{v}_{6}(x_{6},y_{6})𝚟7(x7,y7)\mathtt{v}_{7}(x_{7},y_{7})xxyy
Figure 5: Definition of variables: Case of n=8n=8 vertices

For any n=2sn=2^{s} where s4s\geq 4 is an integer, we introduce a convex equilateral small nn-gon called 𝙰n\mathtt{A}_{n} and constructed as follows. Its diameter graph has the edge 𝚟0𝚟n2\mathtt{v}_{0}-\mathtt{v}_{\frac{n}{2}} as axis of symmetry and can be described by the (3n/81)(3n/8-1)-length half-path 𝚟0𝚟n21𝚟3n4+1𝚟n4\mathtt{v}_{0}-\mathtt{v}_{\frac{n}{2}-1}-\ldots-\mathtt{v}_{\frac{3n}{4}+1}-\mathtt{v}_{\frac{n}{4}} and the pendant edges 𝚟0𝚟n2\mathtt{v}_{0}-\mathtt{v}_{\frac{n}{2}}, 𝚟4k1𝚟4k1+n2\mathtt{v}_{4k-1}-\mathtt{v}_{4k-1+\frac{n}{2}}, k=1,2,,n/8k=1,2,\ldots,n/8. The polygons 𝙰16\mathtt{A}_{16} and 𝙰32\mathtt{A}_{32} are shown in Figure 6. They are symmetrical with respect to the vertical diameter.

(a) (𝙰16,3.135288)(\mathtt{A}_{16},3.135288)
(b) (𝙰32,3.140246)(\mathtt{A}_{32},3.140246)
Figure 6: Polygons (𝙰n,L(𝙰n))(\mathtt{A}_{n},L(\mathtt{A}_{n})) defined in Theorem 1: (a) Hexadecagon 𝙰16\mathtt{A}_{16}; (b) Triacontadigon 𝙰32\mathtt{A}_{32}

Place the vertex 𝚟n2\mathtt{v}_{\frac{n}{2}} at (0,1)(0,1) in the plane. Let t=𝚟n2𝚟0𝚟n21(0,π/n)t=\angle\mathtt{v}_{\frac{n}{2}}\mathtt{v}_{0}\mathtt{v}_{\frac{n}{2}-1}\in(0,\pi/n). This implies that the sides length of 𝙰n\mathtt{A}_{n} is 2sin(t/2)2\sin(t/2). Since 𝙰n\mathtt{A}_{n} is equilateral and symmetric, we have from the half-path 𝚟0𝚟n4\mathtt{v}_{0}-\ldots-\mathtt{v}_{\frac{n}{4}},

x3n4+1\displaystyle x_{\frac{3n}{4}+1} =sintk=1n/81(1)k1(sin(4k1)tsin4kt+sin(4k+1)t)\displaystyle=\sin t-\sum_{k=1}^{n/8-1}(-1)^{k-1}(\sin(4k-1)t-\sin 4kt+\sin(4k+1)t)
=sint(2cost1)(sin2t+sin(n/22)t)2cos2t\displaystyle=\sin t-\frac{(2\cos t-1)(\sin 2t+\sin(n/2-2)t)}{2\cos 2t} =xn41,\displaystyle=-x_{\frac{n}{4}-1},
xn4\displaystyle x_{\frac{n}{4}} =x3n4+1+sin(n/21)t\displaystyle=x_{\frac{3n}{4}+1}+\sin(n/2-1)t =x3n4,\displaystyle=-x_{\frac{3n}{4}},
y3n4+1\displaystyle y_{\frac{3n}{4}+1} =costk=1n/81(1)k1(cos(4k1)tcos4kt+cos(4k+1)t)\displaystyle=\cos t-\sum_{k=1}^{n/8-1}(-1)^{k-1}(\cos(4k-1)t-\cos 4kt+\cos(4k+1)t)
=cost(2cost1)(cos2t+cos(n/22)t)2cos2t\displaystyle=\cos t-\frac{(2\cos t-1)(\cos 2t+\cos(n/2-2)t)}{2\cos 2t} =yn41,\displaystyle=y_{\frac{n}{4}-1},
yn4\displaystyle y_{\frac{n}{4}} =y3n4+1+cos(n/21)t\displaystyle=y_{\frac{3n}{4}+1}+\cos(n/2-1)t =y3n4.\displaystyle=y_{\frac{3n}{4}}.

Finally, the angle tt is chosen so that 𝚟3n4+1𝚟3n4=2sin(t/2)\|\mathtt{v}_{\frac{3n}{4}+1}-\mathtt{v}_{\frac{3n}{4}}\|=2\sin(t/2), i.e.,

(2x3n4+1+sin(n/21)t)2+cos2(n/21)t=4sin2(t/2).(2x_{\frac{3n}{4}+1}+\sin(n/2-1)t)^{2}+\cos^{2}(n/2-1)t=4\sin^{2}(t/2).

An asymptotic analysis produces that, for large nn, this equation has a solution t0(n)t_{0}(n) satisfying

t0(n)=πnπ4n5+π5n611π66n7+35π712n8+O(1n9).t_{0}(n)=\frac{\pi}{n}-\frac{\pi^{4}}{n^{5}}+\frac{\pi^{5}}{n^{6}}-\frac{11\pi^{6}}{6n^{7}}+\frac{35\pi^{7}}{12n^{8}}+O\left(\frac{1}{n^{9}}\right).

By setting t=t0(n)t=t_{0}(n), the perimeter of 𝙰n\mathtt{A}_{n} is

L(𝙰n)\displaystyle L(\mathtt{A}_{n}) =2nsint0(n)2=2nsin(π2nπ42n5+O(1n6))\displaystyle=2n\sin\frac{t_{0}(n)}{2}=2n\sin\left(\frac{\pi}{2n}-\frac{\pi^{4}}{2n^{5}}+O\left(\frac{1}{n^{6}}\right)\right)
=ππ324n2+(π51920π4)1n4+π5n5(π7322560+41π624)1n6+O(1n7)\displaystyle=\pi-\frac{\pi^{3}}{24n^{2}}+\left(\frac{\pi^{5}}{1920}-\pi^{4}\right)\frac{1}{n^{4}}+\frac{\pi^{5}}{n^{5}}-\left(\frac{\pi^{7}}{322560}+\frac{41\pi^{6}}{24}\right)\frac{1}{n^{6}}+O\left(\frac{1}{n^{7}}\right)

and

L¯nL(𝙰n)=π4n4π5n5+O(1n6).\overline{L}_{n}-L(\mathtt{A}_{n})=\frac{\pi^{4}}{n^{4}}-\frac{\pi^{5}}{n^{5}}+O\left(\frac{1}{n^{6}}\right).

Since the polygon 𝙼n\mathtt{M}_{n} proposed by Mossinghoff [12] satisfies

L(𝙼n)=ππ324n2+(π519203π4)1n4+9π5n5(π7322560+9π68)1n6+O(1n7),L(\mathtt{M}_{n})=\pi-\frac{\pi^{3}}{24n^{2}}+\left(\frac{\pi^{5}}{1920}-3\pi^{4}\right)\frac{1}{n^{4}}+\frac{9\pi^{5}}{n^{5}}-\left(\frac{\pi^{7}}{322560}+\frac{9\pi^{6}}{8}\right)\frac{1}{n^{6}}+O\left(\frac{1}{n^{7}}\right),

it follows that

L(𝙰n)L(𝙼n)=2π4n48π5n57π612n6+O(1n7).L(\mathtt{A}_{n})-L(\mathtt{M}_{n})=\frac{2\pi^{4}}{n^{4}}-\frac{8\pi^{5}}{n^{5}}-\frac{7\pi^{6}}{12n^{6}}+O\left(\frac{1}{n^{7}}\right).

To verify that 𝙰n\mathtt{A}_{n} is small, we calculate

𝚟n4𝚟3n4=2xn4=1π3n37π54n5+O(1n7)<1.\|\mathtt{v}_{\frac{n}{4}}-\mathtt{v}_{\frac{3n}{4}}\|=2x_{\frac{n}{4}}=1-\frac{\pi^{3}}{n^{3}}-\frac{7\pi^{5}}{4n^{5}}+O\left(\frac{1}{n^{7}}\right)<1.

To test that 𝙰n\mathtt{A}_{n} is convex, we compute

σn4=2π3n3π4n4+O(1n5)>0.\sigma_{\frac{n}{4}}=\frac{2\pi^{3}}{n^{3}}-\frac{\pi^{4}}{n^{4}}+O\left(\frac{1}{n^{5}}\right)>0.

This completes the proof of Theorem 1.∎

All polygons presented in this work and in [13, 14] were implemented as a package: OPTIGON [15], which is freely available on GitHub. In OPTIGON, we provide Julia and MATLAB functions that give the coordinates of the vertices. One can also find an algorithm developed in [16] to find an estimate of the maximal area of a small nn-gon when n6n\geq 6 is even.

Table 1 shows the perimeters of 𝙰n\mathtt{A}_{n}, along with the upper bounds L¯n\overline{L}_{n}, the perimeters of the regular polygons 𝚁n\mathtt{R}_{n} and Mossinghoff polygons 𝙼n\mathtt{M}_{n}. When n=2sn=2^{s} and s4s\geq 4, 𝙰n\mathtt{A}_{n} provides a tighter lower bound on the maximal perimeter n\ell_{n}^{*} compared to the best prior convex equilateral small nn-gon 𝙼n\mathtt{M}_{n}. As nn increases, it is not surprising that the fraction L(𝙰n)L(𝙼n)L¯nL(𝙼n)\frac{L(\mathtt{A}_{n})-L(\mathtt{M}_{n})}{\overline{L}_{n}-L(\mathtt{M}_{n})} of the length of the interval [L(𝙼n),L¯n][L(\mathtt{M}_{n}),\overline{L}_{n}] containing L(𝙰n)L(\mathtt{A}_{n}) approaches 23\frac{2}{3} since L(𝙰n)L(𝙼n)2π4n4L(\mathtt{A}_{n})-L(\mathtt{M}_{n})\sim\frac{2\pi^{4}}{n^{4}} and L¯nL(𝙼n)3π4n4\overline{L}_{n}-L(\mathtt{M}_{n})\sim\frac{3\pi^{4}}{n^{4}} for large nn.

Table 1: Perimeters of 𝙰n\mathtt{A}_{n}
nn L(𝚁n)L(\mathtt{R}_{n}) L(𝙼n)L(\mathtt{M}_{n}) L(𝙰n)L(\mathtt{A}_{n}) L¯n\overline{L}_{n} L(𝙰n)L(𝙼n)L¯nL(𝙼n)\frac{L(\mathtt{A}_{n})-L(\mathtt{M}_{n})}{\overline{L}_{n}-L(\mathtt{M}_{n})}
16 3.1214451523 3.1347065475 3.1352878881 3.1365484905 0.3156
32 3.1365484905 3.1401338091 3.1402460942 3.1403311570 0.5690
64 3.1403311570 3.1412623836 3.1412717079 3.1412772509 0.6272
128 3.1412772509 3.1415127924 3.1415134468 3.1415138011 0.6487
256 3.1415138011 3.1415728748 3.1415729180 3.1415729404 0.6589

4 Improved triacontadigon and hexacontatetragon

It is natural to ask if the polygon constructed 𝙰n\mathtt{A}_{n} might be optimal for some nn. Using constructive arguments, Proposition 1 and Proposition 2 show that 𝙰32\mathtt{A}_{32} and 𝙰64\mathtt{A}_{64} are suboptimal.

Proposition 1.

There exists a convex equilateral small 3232-gon whose perimeter exceeds that of 𝙰32\mathtt{A}_{32}.

Proof.

Consider the 3232-gon 𝚉32\mathtt{Z}_{32}, illustrated in Figure 7a. Its diameter graph has the edge 𝚟0𝚟16\mathtt{v}_{0}-\mathtt{v}_{16} as axis of symmetry and can be described by the 44-length half-path 𝚟0𝚟11𝚟24𝚟10𝚟23\mathtt{v}_{0}-\mathtt{v}_{11}-\mathtt{v}_{24}-\mathtt{v}_{10}-\mathtt{v}_{23} and the pendant edges 𝚟0𝚟15,,𝚟0𝚟12\mathtt{v}_{0}-\mathtt{v}_{15},\ldots,\mathtt{v}_{0}-\mathtt{v}_{12}, 𝚟11𝚟31,,𝚟11𝚟25\mathtt{v}_{11}-\mathtt{v}_{31},\ldots,\mathtt{v}_{11}-\mathtt{v}_{25}.

Place the vertex 𝚟0\mathtt{v}_{0} at (0,0)(0,0) in the plane, and the vertex 𝚟16\mathtt{v}_{16} at (0,1)(0,1). Let t=𝚟16𝚟0𝚟15(0,π/32)t=\angle\mathtt{v}_{16}\mathtt{v}_{0}\mathtt{v}_{15}\in(0,\pi/32). We have, from the half-path 𝚟0𝚟23\mathtt{v}_{0}-\ldots-\mathtt{v}_{23},

x10\displaystyle x_{10} =sin5tsin13t+sin14t\displaystyle=\sin 5t-\sin 13t+\sin 14t =x22,\displaystyle=-x_{22}, y10\displaystyle y_{10} =cos5tcos13t+cos14t\displaystyle=\cos 5t-\cos 13t+\cos 14t =y11,\displaystyle=y_{11},
x23\displaystyle x_{23} =x10sin15t\displaystyle=x_{10}-\sin 15t =x9,\displaystyle=-x_{9}, y23\displaystyle y_{23} =y10cos15t\displaystyle=y_{10}-\cos 15t =y9.\displaystyle=y_{9}.

Finally, tt is chosen so that 𝚟10𝚟9=2sin(t/2)\|\mathtt{v}_{10}-\mathtt{v}_{9}\|=2\sin(t/2), i.e.,

(2(sin5tsin13t+sin14t)sin15t)2+cos215t=4sin2(t/2).(2(\sin 5t-\sin 13t+\sin 14t)-\sin 15t)^{2}+\cos^{2}15t=4\sin^{2}(t/2).

We obtain t=0.0981744286t=0.0981744286\ldots and L(𝚉32)=64sin(t/2)=3.1403202339>L(𝙰32)L(\mathtt{Z}_{32})=64\sin(t/2)=3.1403202339\ldots>L(\mathtt{A}_{32}). One can verify that 𝚉32\mathtt{Z}_{32} is small and convex. ∎

Proposition 2.

There exists a convex equilateral small 6464-gon whose perimeter exceeds that of 𝙰64\mathtt{A}_{64}.

Proof.

Consider the 6464-gon 𝚉64\mathtt{Z}_{64}, illustrated in Figure 7b. Its diameter graph has the edge 𝚟0𝚟32\mathtt{v}_{0}-\mathtt{v}_{32} as axis of symmetry and can be described by the 2323-length half-path 𝚟0𝚟31𝚟63𝚟30𝚟61𝚟29𝚟60𝚟28𝚟58𝚟27𝚟57𝚟26𝚟56𝚟25𝚟55𝚟24𝚟54𝚟23𝚟53𝚟21𝚟52𝚟19𝚟51𝚟16\mathtt{v}_{0}-\mathtt{v}_{31}-\mathtt{v}_{63}-\mathtt{v}_{30}-\mathtt{v}_{61}-\mathtt{v}_{29}-\mathtt{v}_{60}-\mathtt{v}_{28}-\mathtt{v}_{58}-\mathtt{v}_{27}-\mathtt{v}_{57}-\mathtt{v}_{26}-\mathtt{v}_{56}-\mathtt{v}_{25}-\mathtt{v}_{55}-\mathtt{v}_{24}-\mathtt{v}_{54}-\mathtt{v}_{23}-\mathtt{v}_{53}-\mathtt{v}_{21}-\mathtt{v}_{52}-\mathtt{v}_{19}-\mathtt{v}_{51}-\mathtt{v}_{16}, the pendant edges 𝚟30𝚟62\mathtt{v}_{30}-\mathtt{v}_{62}, 𝚟28𝚟59\mathtt{v}_{28}-\mathtt{v}_{59}, 𝚟53𝚟22\mathtt{v}_{53}-\mathtt{v}_{22}, 𝚟52𝚟20\mathtt{v}_{52}-\mathtt{v}_{20}, 𝚟51𝚟18\mathtt{v}_{51}-\mathtt{v}_{18}, 𝚟51𝚟17\mathtt{v}_{51}-\mathtt{v}_{17}, and the 44-length path 𝚟15𝚟50𝚟14𝚟49\mathtt{v}_{15}-\mathtt{v}_{50}-\mathtt{v}_{14}-\mathtt{v}_{49}.

Place the vertex 𝚟0\mathtt{v}_{0} at (0,0)(0,0) in the plane, and the vertex 𝚟32\mathtt{v}_{32} at (0,1)(0,1). Let t=𝚟32𝚟0𝚟31(0,π/64)t=\angle\mathtt{v}_{32}\mathtt{v}_{0}\mathtt{v}_{31}\in(0,\pi/64). We have, from the half-path 𝚟0𝚟31\mathtt{v}_{0}-\ldots-\mathtt{v}_{31},

x51\displaystyle x_{51} =sintsin2t+sin3tsin5t+sin6tsin7t+sin8t\displaystyle=\sin t-\sin 2t+\sin 3t-\sin 5t+\sin 6t-\sin 7t+\sin 8t
k=1020(1)ksinkt+sin22tsin23t+sin25tsin26t\displaystyle-\sum_{k=10}^{20}(-1)^{k}\sin kt+\sin 22t-\sin 23t+\sin 25t-\sin 26t =x13,\displaystyle=-x_{13},
y51\displaystyle y_{51} =costcos2t+cos3tcos5t+cos6tcos7t+cos8t\displaystyle=\cos t-\cos 2t+\cos 3t-\cos 5t+\cos 6t-\cos 7t+\cos 8t
k=1020(1)kcoskt+cos22tcos23t+cos25tcos26t\displaystyle-\sum_{k=10}^{20}(-1)^{k}\cos kt+\cos 22t-\cos 23t+\cos 25t-\cos 26t =y13,\displaystyle=y_{13},
x16\displaystyle x_{16} =x51+sin29t\displaystyle=x_{51}+\sin 29t =x48,\displaystyle=-x_{48},
y16\displaystyle y_{16} =y51+cos29t\displaystyle=y_{51}+\cos 29t =y48,\displaystyle=y_{48},

and, from the path 𝚟15𝚟49\mathtt{v}_{15}-\ldots-\mathtt{v}_{49},

x50\displaystyle x_{50} =1/2\displaystyle=-1/2 =x14,\displaystyle=-x_{14}, y50\displaystyle y_{50} =y\displaystyle=y =y14,\displaystyle=y_{14},
x15\displaystyle x_{15} =x50+cost\displaystyle=x_{50}+\cos t =x49,\displaystyle=-x_{49}, y15\displaystyle y_{15} =y50+sint\displaystyle=y_{50}+\sin t =y49.\displaystyle=y_{49}.

Finally, tt and yy are chosen so that 𝚟51𝚟50=𝚟16𝚟15=2sin(t/2)\|\mathtt{v}_{51}-\mathtt{v}_{50}\|=\|\mathtt{v}_{16}-\mathtt{v}_{15}\|=2\sin(t/2). We obtain t=0.0490873533t=0.0490873533\ldots and L(𝚉64)=128sin(t/2)=3.1412752155>L(𝙰64)L(\mathtt{Z}_{64})=128\sin(t/2)=3.1412752155\ldots>L(\mathtt{A}_{64}). One can verify that 𝚉64\mathtt{Z}_{64} is small and convex. ∎

Polygons 𝚉32\mathtt{Z}_{32} and 𝚉64\mathtt{Z}_{64} offer a significant improvement to the lower bound of the optimal value. We note that

32L(𝚉32)\displaystyle\ell_{32}^{*}-L(\mathtt{Z}_{32}) <L¯32L(𝚉32)=1.09×105<L¯32L(𝙰32)=8.50×105,\displaystyle<\overline{L}_{32}-L(\mathtt{Z}_{32})=1.09\ldots\times 10^{-5}<\overline{L}_{32}-L(\mathtt{A}_{32})=8.50\ldots\times 10^{-5},
64L(𝚉64)\displaystyle\ell_{64}^{*}-L(\mathtt{Z}_{64}) <L¯64L(𝚉64)=2.03×106<L¯64L(𝙰64)=5.54×106.\displaystyle<\overline{L}_{64}-L(\mathtt{Z}_{64})=2.03\ldots\times 10^{-6}<\overline{L}_{64}-L(\mathtt{A}_{64})=5.54\ldots\times 10^{-6}.

Also, the fractions

L(𝚉32)L(𝙰32)L¯32L(𝙰32)\displaystyle\frac{L(\mathtt{Z}_{32})-L(\mathtt{A}_{32})}{\overline{L}_{32}-L(\mathtt{A}_{32})} =0.8715,\displaystyle=0.8715\ldots,
L(𝚉64)L(𝙰64)L¯64L(𝙰64)\displaystyle\frac{L(\mathtt{Z}_{64})-L(\mathtt{A}_{64})}{\overline{L}_{64}-L(\mathtt{A}_{64})} =0.6327\displaystyle=0.6327\ldots

indicate that the perimeters of the improved polygons are quite close to the maximal perimeter. This suggests that it is possible that another family of convex equilateral small polygons might produce an improvement to Theorem 1.

(a) (𝚉32,3.140320)(\mathtt{Z}_{32},3.140320)
(b) (𝚉64,3.141275)(\mathtt{Z}_{64},3.141275)
Figure 7: Improved convex equilateral small nn-gons (𝚉n,L(𝚉n))(\mathtt{Z}_{n},L(\mathtt{Z}_{n})): (a) Triacontadigon 𝚉32\mathtt{Z}_{32} with larger perimeter than 𝙰32\mathtt{A}_{32}; (b) Hexacontatetragon 𝚉64\mathtt{Z}_{64} with larger perimeter than 𝙰64\mathtt{A}_{64}

5 Conclusion

Lower bounds on the maximal perimeter of convex equilateral small nn-gons were provided when nn is a power of 22 and these bounds are tighter than the previous ones from the literature. For any n=2sn=2^{s} with integer s4s\geq 4, we constructed a convex equilateral small nn-gon 𝙰n\mathtt{A}_{n} whose perimeter is within π4/n4+O(1/n5)\pi^{4}/n^{4}+O(1/n^{5}) of the optimal value. For n=32n=32 and n=64n=64, we propose solutions with even larger perimeters.

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