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The extreme polygons for the self
Chebyshev radius of the boundary

E.V. Nikitenko, Yu.G. Nikonorov Nikitenko Evgeniĭ  Vitalievich
Rubtsovsk Industrial Institute of
Altai State Technical University
after I.I. Polzunov
Rubtsovsk, Traktornaya st., 2/6,
658207, Russia
evnikit@mail.ru Nikonorov Yuriĭ Gennadievich
Southern Mathematical Institute of
the Vladikavkaz Scientific Center of
the Russian Academy of Sciences,
Vladikavkaz, Vatutina st., 53,
362025, Russia
nikonorov2006@mail.ru
Abstract.

The paper is devoted to some extremal problems for convex polygons on the Euclidean plane, related to the concept of self Chebyshev radius for the polygon boundary. We consider a general problem of minimization of the perimeter among all nn-gons with a fixed self Chebyshev radius of the boundary. The main result of the paper is the complete solution of the mentioned problem for n=4n=4: We proved that the quadrilateral of minimum perimeter is a so called magic kite, that verified the corresponding conjecture by Rolf Walter.

2020 Mathematical Subject Classification: 52A10, 52A40, 53A04.

Key words and phrases: approximation by polytopes, convex curve, convex polygon, Chebyshev radius, minimum perimeter, self Chebyshev radius.

1. Introduction and the main result

For a given metric space (X,d)(X,d), we denote by B(x,r)B(x,r) the closed ball with center xx and radius rr. If MM is a nonempty bounded subset of a metric space (X,d)(X,d), then by diam(M)=supx,yMd(x,y)\operatorname{diam}(M)=\sup_{x,y\in M}d(x,y) we denote the diameter of MM, and by

r(M):=inf{a0|xX,MB(x,a)}=infxXsupyMd(x,y)r(M):=\inf\{a\geq 0\,|\,\exists\,x\in X,\,M\subset B(x,a)\}=\inf_{x\in X}\sup_{y\in M}d(x,y)

we denote the Chebyshev radius of MM. A point x0Xx_{0}\in X for which MB(x0,r(M))M\subset B(x_{0},r(M)) is called a Chebyshev center of MM. In general, a Chebyshev center of a set is not unique, and therefore we denote by Z(M)Z(M) the set of all Chebyshev centers of a bounded set MM. The mapping MZ(M)M\mapsto Z(M) is known as the Chebyshev-center map.

Given a nonempty bounded subset MM of XX and a nonempty set YXY\subset X, the relative Chebyshev radius (of the set MM with respect to YY) is defined by the formula

rY(M):=inf{a0|xY,MB(x,a)}=infxYsupyMd(x,y).r_{Y}(M):=\inf\{a\geq 0\,|\,\exists\,x\in Y,\,M\subset B(x,a)\}=\inf_{x\in Y}\sup_{y\in M}d(x,y).

In the case Y=MY=M, we get the definition of the relative Chebyshev radius of MM with respect to MM itself  i.e. the self Chebyshev radius of the set MM:

δ(M):=rM(M)=inf{a0|xM,MB(x,a)}=infxMsupyMd(x,y),\delta(M):=r_{M}(M)=\inf\{a\geq 0\,|\,\exists\,x\in M,\,M\subset B(x,a)\}=\inf\limits_{x\in M}\,\sup\limits_{y\in M}\,d(x,y), (1)

see, e.g., [1], [3, p. 119], and [4].

It is clear that this value depends only on the set MM and the restriction of the metric dd to this set, hence it is an intrinsic characteristic of the (bounded) metric space (M,d|M×M)(M,d|_{M\times M}). It has also the following obvious geometric meaning for compact MM: δ(M)\delta(M) is the smallest radius of a ball having its center in MM and covering MM.

The study of extremal problems for convex curves in the Euclidean plane with a given self Chebyshev radius started with paper [20] by Rolf Walter. In particular, he conjectured that L(Γ)πδ(Γ)L(\Gamma)\geq\pi\cdot\delta(\Gamma) for any closed convex curve Γ\Gamma in the Euclidean plane, where L(Γ)L(\Gamma) is the length of Γ\Gamma and dd is the Euclidean metric. In [20], this conjecture is proved for the case when Γ\Gamma is a convex curve of class C2C^{2} and all curvature centers of Γ\Gamma lie in the interior of Γ\Gamma. It is also shown that the equality L(Γ)=πδ(Γ)L(\Gamma)=\pi\cdot\delta(\Gamma) in this case holds if and only if γ\gamma is of constant width; for sets of constant width the reader is referred to the monograph [17].

It is also proved in [20] that all C2C^{2}-smooth convex curves have good approximations by polygonal chains in terms of the self Chebyshev radius (1). This observation leads to natural extremal problems for convex polygons. In particular, the following result was also proved in [20]. For each triangle PP in the Euclidean plane, one has L(Γ)23δ(Γ)L(\Gamma)\geq 2\sqrt{3}\,\cdot\delta(\Gamma) with equality exactly for equilateral triangles, where Γ\Gamma is the boundary of PP. The proof of this result was simplified by Balestro, Martini, Nikonorova, and one of the present authors in [8], where the authors determined the self Chebyshev radius for the boundary of an arbitrary triangle. Moreover, some related problems were considered in detail in [8]. In particular, the maximal possible perimeter for convex curves and boundaries of convex nn-gons with a given self Chebyshev radius were found.

As the authors of [8] discovered somewhat later, the original problem from [20], which was to prove the inequality L(Γ)πδ(Γ)L(\Gamma)\geq\pi\cdot\delta(\Gamma) for any closed convex curve Γ\Gamma in the Euclidean plane, had already been solved many years ago in paper [11] by K.J. Falconer (the results of that paper were formulated in other terms, without using the self Chebyshev radius). An exposition of the corresponding result can also be found in [17, Theorem 4.3.2]. It should be noted that the following stronger result is also proved in [11]. Instead of convexity, it requires the curve to be rectifiable and instead of the plane it is in n\mathbb{R}^{n}. Let Γ\Gamma be a closed rectifiable curve in n\mathbb{R}^{n} (with the Euclidean metric) such that for every point xx on Γ\Gamma there is a point of Γ\Gamma at distance at least 11 from xx. Then Γ\Gamma has length at least π\pi, this value being attained if and only if Γ\Gamma bounds a plane convex set of constant width 11.

Refer to caption
Figure 1. A magic kite.

This paper is devoted to the proof of Rolf Walter’s conjecture in [20] on quadrilaterals of minimum perimeter among all quadrilaterals with a given self Chebyshev radius of their boundaries that is as follows: L(Γ)4323+3δ(Γ)L(\Gamma)\geq\frac{4}{3}\sqrt{2\sqrt{3}+3}\,\cdot\delta(\Gamma) for any convex quadrilateral P2P\subset\mathbb{R}^{2} with the boundary Γ\Gamma.

Note that this inequality becomes an equality for quadrilaterals PP called magic kites (squares are not extremal in this sense). This definition is taken from [20] and means convex quadrilaterals which are hypothetically extreme with respect to the self Chebyshev radius. Up to similarity, such a quadrilateral could be represented by its vertices, that are as follows (see Fig. 1):

(1,0),(1,0),(0,3323+3),(0,13233).(-1,0),\quad(1,0),\quad\left(0,\frac{\sqrt{3}}{3}\sqrt{2\sqrt{3}+3}\right),\quad\left(0,-\frac{1}{3}\sqrt{2\sqrt{3}-3}\,\right).

The heights drawn from all the vertices to the sides farthest to them have the same length (HiH_{i}, i=1,2,3,4i=1,2,3,4, denotes the bases of the corresponding heights on the sides of the considered quadrilateral), which coincides with the self Chebyshev radius of the boundary Γ\Gamma of this magic kite. Note that two such heights emanate from vertex AA, one such height emanates from vertices BB and DD, while the heights from vertex CC are shorter than the proper Chebyshev radius of the boundary of this polygon.

Note also that we have L(Γ)=85δ(Γ)L(\Gamma_{\square})=\frac{8}{\sqrt{5}}\,\cdot\delta(\Gamma_{\square}), where Γ\Gamma_{\square} is a boundary of a square, and 85>433+23=3.389946\frac{8}{\sqrt{5}}>\frac{4}{3}\sqrt{3+2\sqrt{3}}=3.389946....

Our main result is the following theorem.

Theorem 1.

For any quadrilateral PP with the boundary Γ\Gamma on Euclidean plane, we have the inequality L(Γ)433+23δ(Γ)L(\Gamma)\geq\frac{4}{3}\sqrt{3+2\sqrt{3}}\,\cdot\delta(\Gamma), with equality exactly for magic kites. In other words, a magic kite has the minimal perimeter among all quadrilaterals with a given self Chebyshev radius of their boundaries.

Refer to caption
Figure 2. The transition from a non-convex quadrilateral to a convex one.

If a quadrilateral PP is not convex, then one can easy to find a convex quadrilateral P1P_{1} with the same perimeter and such that the self Chebyshev radius of the boundary of P1P_{1} is not less than the self Chebyshev radius of the boundary of PP. Indeed, if the convex hull of a quadrilateral ABCDABCD is the triangle ABDABD, we can consider the point C1C_{1} that is symmetric to CC with respect the straight line BDBD, see Fig. 2. The quadrilateral ABC1DABC_{1}D is convex and has the same perimeter as ABCDABCD has. For any point M[B,C][C,D]M\in[B,C]\bigcup[C,D], denote by M1M_{1} the point on [B,C1][C1,D][B,C_{1}]\bigcup[C_{1},D] that is symmetric to MM with respect the straight line BDBD. If we take any point L[A,B][A,D]L\in[A,B]\bigcup[A,D], then the distance from LL to M1M_{1} is not less that the distance from LL to MM. This observation implies that the self Chebyshev radius of the boundary of ABCDABCD is not greater than the self Chebyshev radius of the boundary of ABC1DABC_{1}D. Therefore, the above theorem must be proved only for convex quadrilaterals.

We use mainly standard methods of Euclidean geometry and analysis to prove this theorem. Sometimes we have to resort to the help of computer algebra systems. In what follows we repeatedly use some well known properties of convex polygons. As a source on the properties of polygons, one can advise, in particular, books [12, 14, 18]. There is also a special book on the properties of quadrilaterals: [2].

The proof of the main theorem is technically quite difficult. We have to consider many special cases, and in each case we apply different methods. Despite all our attempts to simplify the proofs, we have not succeeded in doing so. We would like to believe that someone will find a shorter and more conceptual reasoning. But while this is not known, we decided to share our version of the proof.

For symbolic and numeric calculations, we used the well-established Maple, a general purpose computer algebra system (CAS). Wherever possible, we have used symbolic calculations. The Maple program provides a wide range of commands for working with symbolic expressions. Numerical calculations were used only where it was not possible to use symbolic calculations effectively and where there was no doubt about the correctness of the approximations (because there is some margin of magnitude with which to compare the result). The precision used was controlled by the Digits global variable, which has a default value of 10. However, it can be set to almost any other value. For more detailed information, see e. g. [16].

The paper is organized as follows. In Section 2 we consider some important information on Chebyshev radii and centers for bounded convex sets in an arbitrary Hilbert space. In Section 3 we prove some important results on self Chebyshev radii and centers for boundaries of convex polygons on the Euclidean plane. In Section 4 we describe a general plan of the study and obtain some auxiliary results. Sections 5, 6, 7, and 8 are devoted to the study of important partial cases of the general problem. We prove our main Theorem 1 on the basis of the results obtained in these sections. In the final section we consider some additional conjectures and outline the prospects for further research on the topic. The list of some important notations and definitions is given at the end of the paper.

The authors are grateful to Endre Makai, Jr., Horst Martini, and Yusuke Sakane for useful discussions and valuable advices. We are also grateful for the advices of both of the anonymous reviewers, whose comments and suggestions allowed us to improve the presentation of this article.

2. Some general results

All propositions in this section can be found in various sources. We give them here in the form we need and provide brief proofs for the sake of completeness.

Let us consider any Hilbert space HH with the inner product (,)(\cdot,\cdot) and the corresponding norm \|\cdot\| (in particular any n\mathbb{R}^{n} with some Euclidean norm). For any set MHM\subset H, the symbols co(M)\operatorname{co}(M), bd(M)\operatorname{bd}(M), and int(M)\operatorname{int}(M) denote respectively the convex hull, the boundary, and the interior of MM.

For given cHc\in H and r0r\geq 0, we consider S(c,r)={xH|xc=r}S(c,r)=\{x\in H\,|\,\|x-c\|=r\}, U(c,r)={xH|xc<r}U(c,r)=\{x\in H\,|\,\|x-c\|<r\}, and B(c,r)={xH|xcr}B(c,r)=\{x\in H\,|\,\|x-c\|\leq r\}, respectively the sphere, the open ball, and the closed ball with the center cc and radius rr. For x,yHx,y\in H, the symbol [x,y][x,y] means the closed interval with the ends xx and yy on the line through xx and yy.

Proposition 1.

Let MM be a non-empty bounded set in HH, and a function t:Ht:H\rightarrow\mathbb{R} such that t(x)=min{r|MB(x,r)}t(x)=\min\{r\,|\,M\subset B(x,r)\}. Then tt is a convex function and there is a real number C>0C>0 such that xCt(x)x+C\|x\|-C\leq t(x)\leq\|x\|+C for all xHx\in H. As a corollary, the function xt(x)x\mapsto t(x) has a unique point of global minimum value in HH.

Proof. Let us consider any x1,x2Hx_{1},x_{2}\in H and any α,β>0\alpha,\beta>0, α+β=1\alpha+\beta=1. Then for every zMz\in M, we have

z(αx1+βx2)=α(zx1)+β(zx2)αzx1+βzx2αt(x1)+βt(x2).\|z-(\alpha x_{1}+\beta x_{2})\|=\|\alpha(z-x_{1})+\beta(z-x_{2})\|\leq\alpha\|z-x_{1}\|+\beta\|z-x_{2}\|\leq\alpha t(x_{1})+\beta t(x_{2}).

Therefore, t(αx1+βx2)αt(x1)+βt(x2)t(\alpha x_{1}+\beta x_{2})\leq\alpha t(x_{1})+\beta t(x_{2}), hence, the function tt is convex. Since MM is bounded, then there is a real number C>0C>0 such that zC\|z\|\leq C for all zMz\in M. Consequently,

xCxzxzx+zx+C\|x\|-C\leq\|x\|-\|z\|\leq\|x-z\|\leq\|x\|+\|z\|\leq\|x\|+C

for every xHx\in H and every zMz\in M. This means that tt is coercive, hence, tt has a point of global minimum value, see e. g. Corollary 11.30 in [9].

Now, we suppose that there are points x2x1x_{2}\neq x_{1}, where tt attains its minimum value, say mtm_{t}. Therefore, MB(x1,mt)M\subset B(x_{1},m_{t}), MB(x2,mt)M\subset B(x_{2},m_{t}), and MB(x1,mt)B(x2,mt)M\subset B(x_{1},m_{t})\cap B(x_{2},m_{t}). It is clear that B(x1,mt)B(x2,mt)B(x1+x22,mt2x2x12/4)B(x_{1},m_{t})\cap B(x_{2},m_{t})\subset B\left(\frac{x_{1}+x_{2}}{2},\sqrt{m_{t}^{2}-\|x_{2}-x_{1}\|^{2}/4}\right). Indeed, for any zB(x1,mt)B(x2,mt)z\in B(x_{1},m_{t})\cap B(x_{2},m_{t}), we have

4z(x1+x2)/22+x2x12=2zx12+2zx224mt2.4\|z-(x_{1}+x_{2})/2\|^{2}+\|x_{2}-x_{1}\|^{2}=2\|z-x_{1}\|^{2}+2\|z-x_{2}\|^{2}\leq 4m_{t}^{2}.

Hence, t(x1+x22)<mtt\left(\frac{x_{1}+x_{2}}{2}\right)<m_{t}, that is impossible.   

Proposition 2.

Let MM be a non-empty convex bounded closed set in HH, and a function t:Ht:H\rightarrow\mathbb{R} such that t(x)=min{r|MB(x,r)}t(x)=\min\{r\,|\,M\subset B(x,r)\}. Then for any yHMy\in H\setminus M, there is a point zbd(M)z\in\operatorname{bd}(M) such that t(z)t(y)t(z)\leq t(y). Moreover, if HH is finite-dimensional, then t(z)<t(y)t(z)<t(y).

Proof. Let zMz\in M be the closest point of MM to the point yy. It is clear that M{xH|xz<xy}M\subset\{x\in H\,|\,\|x-z\|<\|x-y\|\}. Hence if MB(y,r)M\subset B(y,r) for some r>0r>0, then MB(z,r)M\subset B(z,r). It implies that t(z)t(y)t(z)\leq t(y). If HH is finite-dimensional, then MM is compact, hence there is uMu\in M such that uzxz\|u-z\|\geq\|x-z\| for all xMx\in M. Therefore, t(z)=uz<uyt(y)t(z)=\|u-z\|<\|u-y\|\leq t(y).   

For any non-empty bounded closed set MM in HH, a point yHy\in H (yMy\in M) with minimal values of the function xt(x)x\mapsto t(x) on HH (respectively, on MM) is the Chebyshev center (respectively, the self Chebyshev center) for MM. Two above propositions imply

Corollary 1.

Let MM be a non-empty convex bounded closed set in HH, then it has a unique Chebyshev center, which by necessity lies in MM.

Obviously bd(M)\operatorname{bd}(M) has the same Chebyshev center as MM from the above corollary. It is not the case for self Chebyshev centers, of course.

Proposition 3.

Suppose that M1M_{1} and M2M_{2} are convex bounded closed set in HH and M1M2M_{1}\subset M_{2}. If rir_{i} is the self Chebyshev radius of the set bd(Mi)\operatorname{bd}(M_{i}), i=1,2i=1,2, then r1r2r_{1}\leq r_{2}.

Proof. For any ε>0\varepsilon>0, there is a point yεbd(M2)y_{\varepsilon}\in\operatorname{bd}(M_{2}) such that bd(M2)M2B(yε,r2+ε)\operatorname{bd}(M_{2})\subset M_{2}\subset B(y_{\varepsilon},r_{2}+\varepsilon). Since M1M2M_{1}\subset M_{2}, we have bd(M1)M1M2B(yε,r2+ε)\operatorname{bd}(M_{1})\subset M_{1}\subset M_{2}\subset B(y_{\varepsilon},r_{2}+\varepsilon). If yεbd(M1)y_{\varepsilon}\in\operatorname{bd}(M_{1}), then we put zε:=yεz_{\varepsilon}:=y_{\varepsilon}. Now, suppose that yεbd(M1)y_{\varepsilon}\not\in\operatorname{bd}(M_{1}) and consider the function t1:Ht_{1}:H\rightarrow\mathbb{R} such that t1(x)=min{r|M1B(x,r)}t_{1}(x)=\min\{r\,|\,M_{1}\subset B(x,r)\}. We see that t1(yε)r2+εt_{1}(y_{\varepsilon})\leq r_{2}+\varepsilon. By Proposition 2, there is zεbd(M1)z_{\varepsilon}\in\operatorname{bd}(M_{1}) such that t1(zε)t1(yε)t_{1}(z_{\varepsilon})\leq t_{1}(y_{\varepsilon}). In both cases we have t1(zε)t1(yε)r2+εt_{1}(z_{\varepsilon})\leq t_{1}(y_{\varepsilon})\leq r_{2}+\varepsilon. Since ε>0\varepsilon>0 could be as small as we want, we get r1=inf{t1(z)|zbd(M2)}r2r_{1}=\inf\{t_{1}(z)\,|\,z\in\operatorname{bd}(M_{2})\}\leq r_{2}.   

Remark 1.

Let us consider one more proof of Proposition 3 (we put Γ1=bd(M1)\Gamma_{1}=\operatorname{bd}(M_{1}) and Γ2=bd(M2)\Gamma_{2}=\operatorname{bd}(M_{2})). We know that δ(Γ2)=infxΓ2min{r|Γ2M2B(x,r)}\delta(\Gamma_{2})=\inf\limits_{x\in\Gamma_{2}}\min\{r\,|\,\Gamma_{2}\subset M_{2}\subset B(x,r)\}, Γ1M1M2\Gamma_{1}\subset M_{1}\subset M_{2}, and for any xΓ2x\in\Gamma_{2} there is uΓ1u\in\Gamma_{1} such that min{r|Γ1B(u,r)}min{r|Γ1B(x,r)}\min\{r\,|\,\Gamma_{1}\subset B(u,r)\}\leq\min\{r\,|\,\Gamma_{1}\subset B(x,r)\} by Proposition 2. Therefore,

δ(Γ1)=infuΓ1min{r|Γ1B(u,r)}infxΓ2min{r|Γ1B(x,r)}δ(Γ2),\delta(\Gamma_{1})=\inf\limits_{u\in\Gamma_{1}}\min\{r\,|\,\Gamma_{1}\subset B(u,r)\}\leq\inf\limits_{x\in\Gamma_{2}}\min\{r\,|\,\Gamma_{1}\subset B(x,r)\}\leq\delta(\Gamma_{2}),

that proves the proposition. It should be noted that Proposition 3 holds for non-convex M2M_{2}, but the proof is too complicated for non-convex case.

3. Some auxiliary results for boundaries of convex polygons

In what follows, the symbol A\|A\| means the cardinality of a given set AA. We identify the Euclidean plane with 2\mathbb{R}^{2} supplied with the standard Euclidean metric dd, where d(x,y)=(x1y1)2+(x2y2)2d(x,y)=\sqrt{(x_{1}-y_{1})^{2}+(x_{2}-y_{2})^{2}}.

We call Γ\Gamma a convex curve if it is the boundary of some convex compact set in the Euclidean plane 2\mathbb{R}^{2}. Important examples of convex curves are convex closed polygonal chains, i.e. boundaries of convex polygons. A polygon PP is called an nn-gon if it has exactly nn vertices. For n=2n=2 we get line segments. The perimeter L(P)L(P) of any 22-gon is defined as the double length of the line segment PP. Such definition is justified, since it leads to the continuity of the perimeter as a functional on the set of convex polygons with respect to the Hausdorff distance.

Let Γ2\Gamma\subset\mathbb{R}^{2} be a compact set (in particular, a convex curve). We define the function μ:Γ\mu:\Gamma\rightarrow\mathbb{R} as follows:

μ(x)=maxyΓd(x,y).\mu(x)=\max\limits_{y\in\Gamma}d(x,y). (2)

For any polygon PP and any given point xPx\in P, maxyPd(x,y)\max\limits_{y\in P}d(x,y) is achieved at a vertex of PP (see, e.g., Lemma 4.1 in [20]), i.e., μ(x)\mu(x) is equal to the maximal distance from xx to vertices of PP. Note also that the diameter diam(P)=maxx,yPd(x,y)\operatorname{diam}(P)=\max\limits_{x,y\in P}d(x,y) of a polygon PP always connects two vertices.

The following property (monotonicity of the perimeter) of convex curves is well known (see, e.g., [10, §7]).

Proposition 4.

If a convex curve Γ1\Gamma_{1} is inside another convex curve Γ2\Gamma_{2} in the Euclidean plane, then the length of Γ1\Gamma_{1} is less than or equal to the length of Γ2\Gamma_{2}, and equality holds if and only if Γ1=Γ2\Gamma_{1}=\Gamma_{2}.

The following simple result is very useful.

Proposition 5 ([8]).

Let Γ\Gamma be a convex curve in 2\mathbb{R}^{2} such that Γ\Gamma contains the line segment [p,q][p,q] with the property Γ{x2|d(x,o)12d(p,q)}\Gamma\subset\left\{x\in\mathbb{R}^{2}\,|\,d(x,o)\leq\frac{1}{2}d(p,q)\right\}, where oo is the midpoint of [p,q][p,q]. Then δ(Γ)=12d(p,q)=μ(o)\delta(\Gamma)=\frac{1}{2}d(p,q)=\mu(o). Moreover, oo is a unique self Chebyshev center for Γ\Gamma.

Let us consider n4n\geq 4 and let Γ\Gamma be a boundary of a convex nn-gon PP. We will show how to estimate δ(Γ)\delta(\Gamma). Let us denote AiA_{i}, 1in1\leq i\leq n, consecutive vertices of a polygonal line Γ\Gamma (vertices of the polygon PP), assuming that indices are taken modn\!\!\!\mod n. The direction of traversing the curve Γ\Gamma in the direction A1,A2,,A_{1},A_{2},..., is called positive, and the opposite direction to it is called negative.

For a given point AΓA\in\Gamma, we consider the set

(A)={BΓd(A,B)=μ(A)},{\mathcal{F}}(A)=\{B\in\Gamma\,\mid\,d(A,B)=\mu(A)\}, (3)

see (2). It is clear that (A){\mathcal{F}}(A) contains only vertices of Γ\Gamma.

Refer to caption

a)

Refer to caption

b)

Figure 3. a) N(A)N(A) for an interior point of [Ai,Ai+1][A_{i},A_{i+1}]; b) N(A)N(A) for a vertex A=AiA=A_{i}.

For a given point AΓA\in\Gamma, we denote by T+(A)T_{+}(A) (respectively, T(A)T_{-}(A)) the limit limBAABd(A,B)\lim\limits_{B\to A}\frac{\overrightarrow{AB}}{d(A,B)}, where the points BΓB\in\Gamma tend to AA via the negative (respectively, the positive) direction. These vectors have length 11 and are called one-sided tangent vectors at the point AA. If AA is an interior point of some segment [Ai,Ai+1][A_{i},A_{i+1}], then T+(A)=T(A)T_{+}(A)=-T_{-}(A).


For a given point A[Ai,Ai+1]ΓA\in[A_{i},A_{i+1}]\subset\Gamma we put N(A):=[Ai,Ai+1]N(A):=[A_{i},A_{i+1}] if AA is in the interior of the segment [Ai,Ai+1][A_{i},A_{i+1}] and N(A):=[Ai1,Ai][Ai,Ai+1]N(A):=[A_{i-1},A_{i}]\cup[A_{i},A_{i+1}] if A=AiA=A_{i} for some ini\in\mathbb{Z}_{n}, see Fig. 3.

Proposition 6.

In the above notations, for a given point AΓA\in\Gamma, the following conditions are equivalent:

1) The function μ\mu (see (2)) attains its minimal value on the set N(A)N(A) at the point AA;

2) The point AA is the point of local minimum of the function μ:Γ\mu:\Gamma\rightarrow\mathbb{R};

3) For any vector v{T+(A),T(A)}\vec{v}\in\{T_{+}(A),T_{-}(A)\}, there is a point B(A)ΓB\in{\mathcal{F}}(A)\subset\Gamma such that (v,AB)0(\vec{v},\overrightarrow{AB})\leq 0.

Proof. Obviously, 1) implies 2). Let us prove 2)3)2)\Rightarrow 3). Suppose that 2) holds but 3) does not hold. Choose a vector v{T+(A),T(A)}\vec{v}\in\{T_{+}(A),T_{-}(A)\}, such that (v,AB)>0(\vec{v},\overrightarrow{AB})>0 for any B(A)B\in{\mathcal{F}}(A), and consider the points A(ε)=A+εvΓA(\varepsilon)=A+\varepsilon\vec{v}\in\Gamma. Since (v,AB)>0(\vec{v},\overrightarrow{AB})>0, then d(A(ε),B)<d(A,B)=μ(A)d(A(\varepsilon),B)<d(A,B)=\mu(A) for sufficiently small ε>0\varepsilon>0. If CC is any vertex of PP that is not in (A){\mathcal{F}}(A), then d(A,C)<μ(A)d(A,C)<\mu(A), hence, d(A(ε),C)<μ(A)d(A(\varepsilon),C)<\mu(A) for sufficiently small ε>0\varepsilon>0. Therefore, d(A(ε),D)<μ(A)d(A(\varepsilon),D)<\mu(A) for any vertex DD of PP, that implies μ(A(ε))<μ(A)\mu(A(\varepsilon))<\mu(A) for sufficiently small ε>0\varepsilon>0. Hence, we get the contradiction with the condition 2) and, therefore, 2) implies 3).

Now, let us prove 3)1)3)\Rightarrow 1). We suppose that 3) holds. Let us choose any vector v{T+(A),T(A)}\vec{v}\in\{T_{+}(A),T_{-}(A)\} and consider the point A(ε)=A+εvA(\varepsilon)=A+\varepsilon\vec{v} for any ε>0\varepsilon>0. By the condition 3), there is B(A)ΓB\in{\mathcal{F}}(A)\subset\Gamma such that (v,AB)0(\vec{v},\overrightarrow{AB})\leq 0. It implies d(A(ε),B)>d(A,B)=μ(A)d(A(\varepsilon),B)>d(A,B)=\mu(A). Hence, μ(A(ε))d(A(ε),B)>μ(A)\mu(A(\varepsilon))\geq d(A(\varepsilon),B)>\mu(A) for all ε>0\varepsilon>0. Since we can take both T+(A)T_{+}(A) and T(A)T_{-}(A) as v\vec{v}, we get that AA is the minimal value point of μ\mu on the set N(A)N(A), hence, the condition 1) holds.   

Remark 2.

This proposition also follows from Proposition 1. Indeed, the restriction of a convex function to any line segment is also a convex function. For every convex function, any point of local minimum is also a point of global minimum.

Using the equivalence of conditions 1) and 3) in the previous proposition, we obtain the following

Corollary 2.

If the angle at the vertex AiA_{i} of the nn-gon PP is less than π/2\pi/2, then AiA_{i} is not a minimal value point of the function μ\mu on the set N(Ai)=[Ai1,Ai][Ai,Ai+1]N(A_{i})=[A_{i-1},A_{i}]\cup[A_{i},A_{i+1}].

For a given point AΓA\in\Gamma we have d(A,Ai)=d(A,Aj)d(A,A_{i})=d(A,A_{j}) if and only if AA is on the perpendicular bisector of AiA_{i} and AjA_{j}. Hence, we have only finite numbers of points AΓA\in\Gamma such that the set (A){\mathcal{F}}(A) has more that one point. Proposition 6 implies

Corollary 3.

Suppose that the point AΓA\in\Gamma is such that the set (A){\mathcal{F}}(A) has only one point. If AA is the local minimum point of the function μ\mu, then AA is an interior point of some segment [Ai,Ai+1][A_{i},A_{i+1}] and AiAi+1\overrightarrow{A_{i}A_{i+1}} is orthogonal to AB\overrightarrow{AB}, where {B}=(A)\{B\}={\mathcal{F}}(A).

Proposition 7.

For a given nn-gon PP with Γ=bd(P)\Gamma=\operatorname{bd}(P), we consider the set

Glocmin={xΓ|x is a local minimum point of the function μ}.G_{\operatorname{locmin}}=\{x\in\Gamma\,|\,x\mbox{ is a local minimum point of the function }\mu\}.

If there is ini\in\mathbb{Z}_{n} such that AiGlocminA_{i}\in G_{\operatorname{locmin}} and μ(Ai)=max{d(Ai,Ai1),d(Ai,Ai+1)}\mu(A_{i})=\max\left\{d(A_{i},A_{i-1}),d(A_{i},A_{i+1})\right\}, then L(Γ)(2+2)δ(Γ)L(\Gamma)\geq(2+\sqrt{2})\cdot\delta(\Gamma).

Proof. By Corollary 3 we see that the set (Ai){\mathcal{F}}(A_{i}) has at least two elements. Let us consider the set J={jn|AjF(Ai)}={jn|d(Ai,Aj)=μ(Ai)}J=\{j\in\mathbb{Z}_{n}\,|\,A_{j}\in F(A_{i})\}=\{j\in\mathbb{Z}_{n}\,|\,d(A_{i},A_{j})=\mu(A_{i})\}.

Now, we suppose that for every k,lJk,l\in J we have AkAiAl<π/2\angle A_{k}A_{i}A_{l}<\pi/2. Let us fix jJj\in J such that j=i1j=i-1 or j=i+1j=i+1 (it is possible by the assumptions) and consider the points Ai(ε)=εAj+(1ε)AiΓA_{i}(\varepsilon)=\varepsilon A_{j}+(1-\varepsilon)A_{i}\in\Gamma for ε(0,1)\varepsilon\in(0,1). It is easy to see that

d(Ai(ε),Ak)<d(Ai,Ak)=μ(Ai)d(A_{i}(\varepsilon),A_{k})<d(A_{i},A_{k})=\mu(A_{i})

for all kJk\in J and for sufficiently small ε>0\varepsilon>0 (due to the inequality AjAiAk<π/2\angle A_{j}A_{i}A_{k}<\pi/2). Moreover, for all knJk\in\mathbb{Z}_{n}\setminus J, kik\neq i, we have d(Ai(ε),Ak)<μ(Ai)d(A_{i}(\varepsilon),A_{k})<\mu(A_{i}) for sufficiently small ε>0\varepsilon>0 (due to the inequality d(Ai,Ak)<μ(Ai)d(A_{i},A_{k})<\mu(A_{i})). So we have μ(Ai(ε))<μ(Ai)\mu(A_{i}(\varepsilon))<\mu(A_{i}) for all sufficiently small ε>0\varepsilon>0, that is contradicts to AiGlocminA_{i}\in G_{\operatorname{locmin}}.

Therefore, there are k,lJk,l\in J such that AkAiAlπ/2\angle A_{k}A_{i}A_{l}\geq\pi/2. It means that PP contains the triangle AkAiAl\triangle A_{k}A_{i}A_{l}, which has the perimeter at least (2+2)δ(Γ)(2+\sqrt{2})\cdot\delta(\Gamma) (we have this minimal value for AkAiAl=π/2\angle A_{k}A_{i}A_{l}=\pi/2). Hence, L(Γ)(2+2)δ(Γ)L(\Gamma)\geq(2+\sqrt{2})\cdot\delta(\Gamma).   

In what follows, we call an nn-gon PP extremal if it has the smallest perimeter among all convex nn-gons whose boundaries have a given value of the self Chebyshev radius (1) (i. e. L(Γ)/δ(Γ)L(\Gamma)/\delta(\Gamma) has a minimal possible value, where Γ=bd(P)\Gamma=\operatorname{bd}(P)).

Remark 3.

The existence of an extremal nn-gon for every n3n\geq 3 can be proved using a limiting argument. The limit polygon cannot be an mm-gon with m<nm<n, since for any mm-gon we can easily construct an nn-gon with the same self Chebyshev radius for its boundary and with a bigger perimeter. Indeed, it suffices to replace one side of a given mm-gon to a suitable almost straight polygonal chain of nm+1n-m+1 line segments.

The self Chebyshev radius δ(Γ)\delta(\Gamma) of Γ\Gamma coincides with the minimal value of the function μ\mu (see (2)).

For fixed nn-gon PP with Γ=bd(P)\Gamma=\operatorname{bd}(P), we consider the function t:2t:\mathbb{R}^{2}\rightarrow\mathbb{R} such that

t(x)=min{r|ΓB(x,r)}.t(x)=\min\{r\,|\,\Gamma\subset B(x,r)\}. (4)

We know that this function is convex with an unique point of the global minimum x0x_{0} (Proposition 1). The point x0x_{0} is the Chebyshev center of Γ\Gamma (and PP), t(x0)t(x_{0}) is the Chebyshev radius rΓr_{\Gamma} of Γ\Gamma (and PP). We know also that x0Px_{0}\in P by Corollary 1.

Since the function tt is convex, for any r>rΓr>r_{\Gamma}, the set Ur:={x2|t(x)r}U_{r}:=\{x\in\mathbb{R}^{2}\,|\,t(x)\leq r\} is a convex set, and Lr:={x2|t(x)=r}L_{r}:=\{x\in\mathbb{R}^{2}\,|\,t(x)=r\} is a closed convex curve.

Lemma 1.

For every r>rΓr>r_{\Gamma}, the convex curve LrL_{r} is the union of finite circular arcs of radius rr with the center at some vertices of Γ\Gamma. A common point of two arcs with different centers AiA_{i} and AjA_{j} is on the same distance from these two points.

Proof. If xLrx\in L_{r}, then ΓB(x,r)\Gamma\subset B(x,r) and there is a point zΓz\in\Gamma such that d(x,z)=rd(x,z)=r. Obviously, zz is a vertex of Γ\Gamma (and PP). Since we have only finite number of the vertices, we get the lemma.   

It is clear that

δ(Γ)=min{r[rΓ,)|ΓLr}.\delta(\Gamma)=\min\{r\in[r_{\Gamma},\infty)\,|\,\Gamma\cap L_{r}\neq\emptyset\}. (5)

Hence, we have Uδ(Γ)PU_{\delta(\Gamma)}\subset P and

Gmin:=Lδ(Γ)Γ=Uδ(Γ)Γ.G_{\min}:=L_{\delta(\Gamma)}\cap\Gamma=U_{\delta(\Gamma)}\cap\Gamma\neq\emptyset. (6)

If zGminz\in G_{\min} and zz is a smooth point of Lδ(Γ)L_{\delta(\Gamma)}, then zz is necessarily in the interior of some segment [Ai,Ai+1]Γ[A_{i},A_{i+1}]\subset\Gamma. If zGminz\in G_{\min} and zz is a non-smooth point (an intersection point of two circular arcs with different centers) of Lδ(Γ)L_{\delta(\Gamma)}, then zz could be some vertex AiA_{i} (in this case Ai1AiAi+1π/2\angle A_{i-1}A_{i}A_{i+1}\geq\pi/2 by Corollary 2).

It is clear that the set Gmin[Ai,Ai+1]G_{\min}\cap[A_{i},A_{i+1}] is either empty or has exactly one point for any line segment [Ai,Ai+1]Γ[A_{i},A_{i+1}]\subset\Gamma.

Let us suppose that PP is extremal. Fix the vertex AiA_{i} and consider two variations of Γ\Gamma: Γε+\Gamma_{\varepsilon}^{+} and Γε\Gamma_{\varepsilon}^{-}, where ε(0,1)\varepsilon\in(0,1). This polygonal lines have the same vertices AjA_{j} as Γ\Gamma has with one exception: instead of AiA_{i} we take respectively Ai+(ε)=εAi+1+(1ε)AiA_{i}^{+}({\varepsilon})=\varepsilon A_{i+1}+(1-\varepsilon)A_{i} and Ai(ε)=εAi1+(1ε)AiA_{i}^{-}({\varepsilon})=\varepsilon A_{i-1}+(1-\varepsilon)A_{i}. Since Ai+(ε)[Ai,Ai+1]A_{i}^{+}({\varepsilon})\in[A_{i},A_{i+1}] and Ai(ε)[Ai1,Ai]A_{i}^{-}({\varepsilon})\in[A_{i-1},A_{i}], then L(Γε+)<L(Γ)L(\Gamma_{\varepsilon}^{+})<L(\Gamma) and L(Γε)<L(Γ)L(\Gamma_{\varepsilon}^{-})<L(\Gamma) for all ε(0,1)\varepsilon\in(0,1). Since PP is extremal, then δ(Γε+)<δ(Γ)\delta(\Gamma_{\varepsilon}^{+})<\delta(\Gamma) and δ(Γε)<δ(Γ)\delta(\Gamma_{\varepsilon}^{-})<\delta(\Gamma) (by Proposition 3 we know that δ(Γε+)δ(Γ)\delta(\Gamma_{\varepsilon}^{+})\leq\delta(\Gamma) and δ(Γε)δ(Γ)\delta(\Gamma_{\varepsilon}^{-})\leq\delta(\Gamma)).

Now, we deal with the variation Γε\Gamma_{\varepsilon}^{-}. There is a point zεΓεz_{\varepsilon}\in\Gamma_{\varepsilon}^{-} such that d(zε,x)δ(Γε)d(z_{\varepsilon},x)\leq\delta(\Gamma_{\varepsilon}^{-}) for any xΓεx\in\Gamma_{\varepsilon}^{-}, in particular, for all vertices AjA_{j}, jij\neq i. Moreover, d(zε,Ai(ε))δ(Γε)d(z_{\varepsilon},A_{i}^{-}({\varepsilon}))\leq\delta(\Gamma_{\varepsilon}^{-}). If we can choose ε\varepsilon arbitrarily close to zero and such that zε[Ai(ε),Ai+1]z_{\varepsilon}\in[A_{i}^{-}({\varepsilon}),A_{i+1}], then we get that [Ai,Ai+1]Gmin[A_{i},A_{i+1}]\cap G_{\min}\neq\emptyset.

If zε[Ai(ε),Ai+1]z_{\varepsilon}\not\in[A_{i}^{-}({\varepsilon}),A_{i+1}], then zεΓz_{\varepsilon}\in\Gamma, hence, d(zε,Ai)>δ(Γε)d(z_{\varepsilon},A_{i})>\delta(\Gamma_{\varepsilon}^{-}) (otherwise δ(Γε)δ(Γ)\delta(\Gamma_{\varepsilon}^{-})\geq\delta(\Gamma)). If we can choose ε\varepsilon arbitrarily close to zero and such that zεΓz_{\varepsilon}\in\Gamma, then we get some zGminz\in G_{\min} such that d(z,Ai)=δ(Γ)d(z,A_{i})=\delta(\Gamma). Indeed, if zεzz_{\varepsilon}\to z as ε0\varepsilon\to 0, then d(zε,Ai(ε))δ(Γε)<d(zε,Ai)d(z_{\varepsilon},A_{i}^{-}({\varepsilon}))\leq\delta(\Gamma_{\varepsilon}^{-})<d(z_{\varepsilon},A_{i}), Ai(ε)AiA_{i}^{-}({\varepsilon})\to A_{i} and δ(Γε)δ(Γ)\delta(\Gamma_{\varepsilon}^{-})\to\delta(\Gamma) as ε0\varepsilon\to 0.

The variation Γε+\Gamma_{\varepsilon}^{+} could be considered similarly. Hence we get the following

Proposition 8.

Suppose that an nn-gon PP is extremal. If [Ai,Ai+1]Gmin=[A_{i},A_{i+1}]\cap G_{\min}=\emptyset for some ini\in\mathbb{Z}_{n}, then there are points z1,z2Gminz_{1},z_{2}\in G_{\min} such that d(z1,Ai)=d(z2,Ai+1)=δ(Γ)d(z_{1},A_{i})=d(z_{2},A_{i+1})=\delta(\Gamma).

4. A plan how to find extremal quadrilaterals and some preliminary considerations

The main idea is to determine all extremal 44-gons PP and to prove that this set coincides with magic kites. We use the notations from the previous sections.

Since 2+2=3.414213>4323+3=3.3899462+\sqrt{2}=3.414213...>\frac{4}{3}\sqrt{2\sqrt{3}+3}=3.389946..., then we get the following simple consequence of Corollary 3 and Proposition 7.

Corollary 4.

If there is i4i\in\mathbb{Z}_{4} such that AiGminA_{i}\in G_{\min}, then L(Γ)(2+2)δ(Γ)L(\Gamma)\geq(2+\sqrt{2})\cdot\delta(\Gamma). Consequently, for any extremal 44-gon PP, we have AiGminA_{i}\not\in G_{\min} for all i4i\in\mathbb{Z}_{4}.

Proposition 9.

Suppose that a quadrilateral PP is extremal. If AGminA\in G_{\min} and A[Ai,Ai+1]A\in[A_{i},A_{i+1}], then Ai,Ai+1(A)A_{i},A_{i+1}\not\in{\mathcal{F}}(A). In particular, (A){Ai+2,Ai+3}{\mathcal{F}}(A)\subset\{A_{i+2},A_{i+3}\}.

Proof. By Corollary 4 we see that A{Ai,Ai+1}A\not\in\{A_{i},A_{i+1}\}. Suppose that Ai(A)A_{i}\in{\mathcal{F}}(A), i. e. d(A,Ai)=δ(Γ)d(A,A_{i})=\delta(\Gamma). By Proposition 6, for the vector v=1AAiAAi{T+(A),T(A)}\vec{v}=\frac{1}{\|\overrightarrow{AA_{i}}\|}\overrightarrow{AA_{i}}\in\{T_{+}(A),T_{-}(A)\}, there is a point B(A)ΓB\in{\mathcal{F}}(A)\subset\Gamma such that (v,AB)0(\vec{v},\overrightarrow{AB})\leq 0. Hence, AiABπ/2\angle A_{i}AB\geq\pi/2 and d(A,Ai)=d(A,B)=δ(Γ)d(A,A_{i})=d(A,B)=\delta(\Gamma). Since the triangle AiABA_{i}AB is a subset of the quadrilateral PP and has the perimeter (2+2)δ(Γ)\geq(2+\sqrt{2})\cdot\delta(\Gamma), then L(Γ)(2+2)δ(Γ)L(\Gamma)\geq(2+\sqrt{2})\cdot\delta(\Gamma). This means that PP is not extremal. Therefore, Ai(A)A_{i}\not\in{\mathcal{F}}(A). Similar arguments proves Ai+1(A)A_{i+1}\not\in{\mathcal{F}}(A).   

We are going to prove that L(Γ)4323+3δ(Γ)L(\Gamma)\geq\frac{4}{3}\sqrt{2\sqrt{3}+3}\,\cdot\delta(\Gamma) for any extremal quadrilateral PP. For this goal, we consider some auxiliary problems.

Refer to caption

a)

​​​​​ Refer to caption b) Refer to caption c) Refer to caption d) Refer to caption e) Refer to caption f) Refer to caption g)

Figure 4. a) Case 2.1, b) Case 2.2, c) Case 2.3, d) Case 3.1, e) Case 3.2, f) Case 3.3, g) Case 3.4.

Denote by Gmin\|G_{\min}\| the number of points in the set GminG_{\min}, or, in other words, the number of self Chebyshev centers for Γ\Gamma (see (6)). For any i4i\in\mathbb{Z}_{4}, the set Gmin[Ai,Ai+1]G_{\min}\cap[A_{i},A_{i+1}] is either empty or has exactly one point.

We denote the elements of GminG_{\min} by capital roman letter (sometimes with indices). The possible subcases depends not only of cardinality of GminG_{\min} but also on how many elements of the set GminG_{\min} satisfy the conditions ()2\|{\mathcal{F}}(\,\cdot\,)\|\geq 2 and ()=1\|{\mathcal{F}}(\,\cdot\,)\|=1 (see (3)) and the relative position of these points.

In what follows, a self Chebyshev center xΓx\in\Gamma is called simple if (x)=1\|{\mathcal{F}}(x)\|=1 and non-simple if (x)2\|{\mathcal{F}}(x)\|\geq 2.

On the other hand, GminG_{\min}\neq\emptyset and, therefore, 1Gmin41\leq\|G_{\min}\|\leq 4. Moreover, GminG_{\min} does not contain any vertex of Γ\Gamma by Corollary 4. We distinguish four cases according to the value of Gmin\|G_{\min}\|. Case kk is the case when Gmin=k\|G_{\min}\|=k, k=1,2,3,4k=1,2,3,4.

5. Case 1

Proposition 10.

Case 1 does not provide extremal quadrilaterals.

Proof. Suppose that Gmin=1\|G_{\min}\|=1 and Gmin={B}G_{\min}=\{B\}, where BB is an interior point of the segment (say) [A1,A2][A_{1},A_{2}]. Hence, [A2,A3]Gmin=[A3,A4]Gmin=[A4,A1]Gmin=[A_{2},A_{3}]\cap G_{\min}=[A_{3},A_{4}]\cap G_{\min}=[A_{4},A_{1}]\cap G_{\min}=\emptyset and A1,A2,A3,A4F(B)A_{1},A_{2},A_{3},A_{4}\in F(B) by Proposition 8. In particular, d(A1,A2)=d(A1,B)+d(A2,B)=2δ(Γ)d(A_{1},A_{2})=d(A_{1},B)+d(A_{2},B)=2\delta(\Gamma). By the triangle inequality we have also that d(A2,A3)+d(A3,A4)+d(A4,A1)d(A1,A2)=2δ(Γ)d(A_{2},A_{3})+d(A_{3},A_{4})+d(A_{4},A_{1})\geq d(A_{1},A_{2})=2\delta(\Gamma). Therefore, L(Γ)4δ(Γ)L(\Gamma)\geq 4\delta(\Gamma). Obviously, 4>4323+3=3.3899464>\frac{4}{3}\sqrt{2\sqrt{3}+3}=3.389946.... Therefore, Case 1 does not provide an extremal quadrilateral.   

Refer to caption
Figure 5. The ellipse and the circle for the quadrilateral ABCDABCD.
Remark 4.

Recall that we use the term ‘‘extremal’’ in this paper only for polygons with minimal perimeter among all polygons with a given self Chebyshev radius of the boundary. It should be noted that the polygon with maximal perimeter among all polygons with a given self Chebyshev radius of the boundary was determined in [8, Theorem 4]. The boundary of such a polygon has only one self Chebyshev center. For n=4n=4, such a polygon is a half of a regular 66-gon.

In the following three sections, we will consider Cases 2, 3, and 4 in turn. For all this cases, it is reasonable to consider separately some subcases. In Fig. 4, we show all the essential subcases of Cases 2 and 3.

The following auxiliary result is very useful.

Lemma 2.

Let ABCDABCD be a quadrilateral with δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD))=1 for the self Chebyshev radius of its boundary. Suppose that there is a point HGmin[A,B]H\in G_{\min}\cap[A,B] such that (H)={C,D}{\mathcal{F}}(H)=\{C,D\} and AHD<π/2\angle AHD<\pi/2. If, moreover, [A,D]Gmin=[A,D]\cap G_{\min}=\emptyset (respectively, Gmin[A,B][B,C]G_{\min}\subset[A,B]\cup[B,C]) and D(H)D\not\in{\mathcal{F}}(H^{\prime}) for any HGmin{H}H^{\prime}\in G_{\min}\setminus\{H\}, then either HDCHDA\angle HDC\leq\angle HDA (respectively, HDC=HDA\angle HDC=\angle HDA) or there exists a point DD^{\prime} arbitrarily close to the point DD, such that δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD^{\prime}))=1 and L(bd(ABCD))<L(bd(ABCD))L(\operatorname{bd}(ABCD^{\prime}))<L(\operatorname{bd}(ABCD)).

Proof. At first, we consider the case [A,D]Gmin=[A,D]\cap G_{\min}=\emptyset. Let us suppose that HDC>HDA\angle HDC>\angle HDA. We consider an ellipse \mathcal{E} with the foci at the points AA and CC, that contains the point DD (see Fig. 5). Let 𝒮\mathcal{S} be a circle of radius 11 centered at the point HH. Recall that C,D𝒮C,D\in\mathcal{S}.

Let l1l_{1} be the tangent line to the ellipse \mathcal{E} at the point DD and l2l_{2} the tangent line to the circle 𝒮\mathcal{S} at the point DD. Note that l2DHl_{2}\bot DH. Since HDC>HDA\angle HDC>\angle HDA, then the angle between the tangent l2l_{2} and the segment DCDC is less than the angle between the tangent l2l_{2} and the segment DADA.

By a well known property of the ellipse, the angle between the tangent l1l_{1} and the line segment [D,C][D,C] is equal to the angle between the tangent l1l_{1} and the the segment [D,A][D,A]. Therefore, the arc of a circle 𝒮\mathcal{S} between the points DD and CC is such that any its point DDD^{\prime}\neq D, that is sufficiently close to the point DD, lies inside the ellipse \mathcal{E}. Therefore, we have d(A,D)+d(D,C)<d(A,D)+d(D,C)d(A,D^{\prime})+d(D^{\prime},C)<d(A,D)+d(D,C) for such a point DD^{\prime} according to another one well known property of the ellipse. Hence, L(bd(ABCD))<L(bd(ABCD))L(\operatorname{bd}(ABCD^{\prime}))<L(\operatorname{bd}(ABCD)). It is easy to see that the self Chebyshev radius of the boundary of the quadrilateral ABCDABCD^{\prime} is 11 if DD^{\prime} is sufficiently close to DD.

In the case Gmin[A,B][B,C]G_{\min}\subset[A,B]\cup[B,C] we can repeat the above arguments with one addition. In this case, we can take also the point DD^{\prime} outside the arc between DD and CC (but sufficiently close to DD). Since [C,D]Gmin=[C,D]\cap G_{\min}=\emptyset, then such a variation of the quadrilateral ABCDABCD does not decrease the value of the self Chebyshev radius of the boundary. On the other hand, if HDC<HDA\angle HDC<\angle HDA, such a variation decreases the perimeter. Therefore, either HDC=HDA\angle HDC=\angle HDA or there exists a point DD^{\prime} arbitrarily close to the point DD, such that δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD^{\prime}))=1 and L(bd(ABCD))<L(bd(ABCD))L(\operatorname{bd}(ABCD^{\prime}))<L(\operatorname{bd}(ABCD)).   

We obviously get the following important corollary.

Refer to caption
Figure 6. Lemma 3.
Corollary 5.

If the quadrilateral ABCDABCD is extremal in the assumptions of Lemma 2, then CDHADH\angle CDH\leq\angle ADH (respectively, CDH=ADH\angle CDH=\angle ADH).

The following lemma is important for further considerations.

Lemma 3.

Let OF1EF2OF_{1}EF_{2} be a quadrilateral such that d(O,E)=d(O,F1)=1d(O,E)=d(O,F_{1})=1, d(O,F2)1d(O,F_{2})\leq 1, OF1E=OEF1=OEF2=:βπ/4\angle OF_{1}E=\angle OEF_{1}=\angle OEF_{2}=:\beta\geq\pi/4 and β<π/2\beta<\pi/2. We consider an ellipse \mathcal{E} with the foci at the points F1F_{1} and F2F_{2}, that contains the point EE. Let 𝒮\mathcal{S} be a circle of radius 11 centered at the point OO. If d(E,F2)>13d(E,F1)d(E,F_{2})>\frac{1}{3}d(E,F_{1}) then all points EEE^{\prime}\neq E on the circle 𝒮\mathcal{S} sufficiently close to the point EE lie inside the ellipse \mathcal{E}.

Proof. In a suitable Cartesian coordinate system, the points we need have the following coordinates:

O=(0,0),E=(1,0),F1=(cos(α),sin(α)),F2=(lcos(α)+1l,lsin(α)),O=(0,0),\quad E=(1,0),\quad F_{1}=\bigl{(}\cos(\alpha),\sin(\alpha)\bigr{)},\quad F_{2}=\bigl{(}l\cos(\alpha)+1-l,-l\sin(\alpha)\bigr{)},

where α:=π2β\alpha:=\pi-2\beta (see Fig. 6). Let us consider the equation of the ellipse \mathcal{E}:

f(x,y):=d((x,y),F1)+d((x,y),F2)d(E,F1)d(E,F2)=0.f(x,y):=d\bigl{(}(x,y),F_{1}\bigr{)}+d\bigl{(}(x,y),F_{2}\bigr{)}-d(E,F_{1})-d(E,F_{2})=0.

By direct computations, we get

f(cos(t),sin(t))=2(1cos(t))g(t),f\bigl{(}\cos(t),\sin(t)\bigr{)}=2\bigl{(}1-\cos(t)\bigr{)}\cdot g(t),

where g(t)=(1+l)(3l1)(1cos(α))(1l2)sin(α)t+o(t)g(t)=-(1+l)(3l-1)\bigl{(}1-\cos(\alpha)\bigr{)}-(1-l^{2})\sin(\alpha)t+o(t) as t0t\rightarrow 0. Therefore, l>1/3l>1/3 (that is equivalent to d(E,F2)>13d(E,F1)d(E,F_{2})>\frac{1}{3}\,d(E,F_{1})) implies g(t)<0g(t)<0 for tt sufficiently close to 0.   

6. Case 2

Suppose that Gmin=2\|G_{\min}\|=2. Our general assumptions are as follows. Let ABCDABCD be a quadrilateral with Gmin=2\|G_{\min}\|=2 and with δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD))=1 for the self Chebyshev radius of its boundary. We consider the set

Gmin={xbd(ABCD)|μ(x)=1}={H1,H2},G_{\min}=\{x\in\operatorname{bd}(ABCD)\leavevmode\nobreak\ |\leavevmode\nobreak\ \mu(x)=1\}=\{H_{1},H_{2}\},

where both points H1H_{1} and H2H_{2} are interior points of some sides of ABCDABCD, see (6). In other words, uGminu\in G_{\min} if and only if (u)={ybd(ABCD)|d(u,y)=1}\mathcal{F}(u)=\{y\in\operatorname{bd}(ABCD)\leavevmode\nobreak\ |\leavevmode\nobreak\ d(u,y)=1\}.

We consider several subcases according to Fig. 4.

6.1. Case 2.1

Without loss of generality, we may suppose that GG is an interior point of [A,D][A,D], EE is an interior point of [A,B][A,B] such that DE[A,B]DE\perp[A,B], and δ(bd(ABCD))=d(G,B)=d(G,C)=d(E,D)=1\delta(\operatorname{bd}(ABCD))=d(G,B)=d(G,C)=d(E,D)=1 (see Fig. 7). Moreover, we have DGCπ/2\angle DGC\leq\pi/2 and BGAπ/2\angle BGA\leq\pi/2 by Proposition 6.

Let us suppose that the quadrilateral ABCDABCD is extremal. Then we have GCD=GCB\angle GCD=\angle GCB by Corollary 5. Let us introduce the following notation: β:=GBC\beta:=\angle GBC, φ=ADE\varphi=\angle ADE, ψ=GBA\psi=\angle GBA.

If βπ/4\beta\leq\pi/4, then CGBπ/2\angle CGB\geq\pi/2 and we obtain the following simple estimate for the perimeter: L(bd(CGB))2+2L(\operatorname{bd}(CGB))\geq 2+\sqrt{2}. Hence, we have L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}, that is impossible for an extremal quadrilateral. Therefore, β>π/4\beta>\pi/4.

Refer to caption
Figure 7. Case 2.1.

Since AGB=π/2(ψφ)π/2\angle AGB=\pi/2-(\psi-\varphi)\leq\pi/2, then ψφ0\psi\geq\varphi\geq 0. It is easy to see that EDC=3π/23βψ\angle EDC=3\pi/2-3\beta-\psi. Hence GDC=φ+EDC=3π/23β(ψφ)π/2\angle GDC=\varphi+\angle EDC=3\pi/2-3\beta-(\psi-\varphi)\geq\pi/2. It implies βπ/3(ψφ)/3π/3\beta\leq\pi/3-(\psi-\varphi)/3\leq\pi/3.

It is important that d(C,D)13d(B,C)d(C,D)\leq\frac{1}{3}d(B,C) (otherwise the quadrilateral ABCDABCD is not extremal by Lemma 3). Since d(B,C)=2cos(β)d(B,C)=2\cos(\beta), we get d(C,D)=2lcos(β)d(C,D)=2l\cos(\beta), where l(0,1/3]l\in(0,1/3].

If β[π/4,π/3]\beta\in[\pi/4,\pi/3] and l[0,1/3]l\in[0,1/3], then 4cos2(β)24\cos^{2}(\beta)\leq 2 and l(1l)2/9l(1-l)\leq 2/9. These inequalities imply 4cos2(β)l(1l)4/94\cos^{2}(\beta)l(1-l)\leq 4/9 and, consequently,

d(G,D)=14cos2(β)l(1l)53d(G,D)=\sqrt{1-4\cos^{2}(\beta)\cdot l(1-l)}\geq\frac{\sqrt{5}}{3}

On the other hand, d(G,D)=1sin(ψ)cos(φ)d(G,D)=\frac{1-\sin(\psi)}{\cos(\varphi)}. Hence, 1sin(ψ)53cos(φ)1-\sin(\psi)\geq\frac{\sqrt{5}}{3}\cos(\varphi) or, equivalently, 53cos(φ)+sin(ψ)1\frac{\sqrt{5}}{3}\cos(\varphi)+\sin(\psi)\leq 1. We have sin(φ)sin(ψ)\sin(\varphi)\leq\sin(\psi) and cos(φ)cos(ψ)\cos(\varphi)\geq\cos(\psi) due to 0φψ0\leq\varphi\leq\psi. It implies that φ\varphi and ψ\psi both satisfy the inequality 53cos(t)+sin(t)1\frac{\sqrt{5}}{3}\cos(t)+\sin(t)\leq 1, which solutions for t[0,π/2]t\in[0,\pi/2] are as follows: t[0,t0]t\in[0,t_{0}], where t0=arcsin(2/7)t_{0}=\arcsin(2/7). Therefore, 0φψt0<π/100\leq\varphi\leq\psi\leq t_{0}<\pi/10.

Put θ:=ψφ\theta:=\psi-\varphi. It is easy to see that DGC=πβGDC=2β+θπ/2\angle DGC=\pi-\beta-\angle GDC=2\beta+\theta-\pi/2. The equations (the low of sines for CDG\triangle CDG)

d(G,D)sin(β)=1sin(3π23βθ)=2lcos(β)sin(2β+θπ/2)\frac{d(G,D)}{\sin(\beta)}=\frac{1}{\sin(\frac{3\pi}{2}-3\beta-\theta)}=\frac{2l\cos(\beta)}{\sin(2\beta+\theta-\pi/2)}

imply 2lcos(β)=cos(2β+θ)cos(3β+θ)2l\cos(\beta)=\frac{\cos(2\beta+\theta)}{\cos(3\beta+\theta)} or, equivalently,

l=cos(2β+θ)2cos(3β+θ)cos(β)=:f(β,θ).l=\frac{\cos(2\beta+\theta)}{2\cos(3\beta+\theta)\cos(\beta)}=:f(\beta,\theta).

It is easy to check that

fθ(β,θ)=sin(β)2cos2(3β+θ)cos(β)>0,\frac{\partial f}{\partial\theta}(\beta,\theta)=\frac{\sin(\beta)}{2\cos^{2}(3\beta+\theta)\cos(\beta)}>0,

for β[π/4,π/3]\beta\in[\pi/4,\pi/3] and θ[0,π/10]\theta\in[0,\pi/10]. Hence 13lcos(2β)2cos(3β)cos(β)=cos(2β)cos(2β)+cos(4β)\frac{1}{3}\geq l\geq\frac{\cos(2\beta)}{2\cos(3\beta)\cos(\beta)}=\frac{\cos(2\beta)}{\cos(2\beta)+\cos(4\beta)}. It implies cos(4β)2cos(2β)\cos(4\beta)\leq 2\cos(2\beta). We get 2η22η102\eta^{2}-2\eta-1\leq 0 for η:=cos(2β)\eta:=\cos(2\beta). The solution of this inequality is η[132,0]\eta\in\left[\frac{1-\sqrt{3}}{2},0\right]. Therefore, β(π/4,β0]\beta\in(\pi/4,\beta_{0}], where β0=π212arccos(132)\beta_{0}=\frac{\pi}{2}-\frac{1}{2}\arccos\left(\frac{1-\sqrt{3}}{2}\right).

Now we are going to show that the inequality d2(E,C)1d^{2}(E,C)\leq 1 does not hold for β(π/4,β0]\beta\in(\pi/4,\beta_{0}] (hence, EGminE\not\in G_{\min}, and we get a contradiction). If we suppose that d2(E,C)1d^{2}(E,C)\leq 1, then EDC<π/2\angle EDC<\pi/2 and, consequently, 3β+ψ>π3\beta+\psi>\pi. In particular, ψ>π3β0=ψ0\psi>\pi-3\beta_{0}=\psi_{0} and sin(3β+ψ)<0\sin(3\beta+\psi)<0. On the other hand,

d(B,C)sin(EBC)+d(C,D)cos(EDC)=2cos(β)(sin(β+ψ)lsin(3β+ψ))=1d(B,C)\cdot\sin(\angle EBC)+d(C,D)\cdot\cos(\angle EDC)=2\cos(\beta)\bigl{(}\sin(\beta+\psi)-l\sin(3\beta+\psi)\bigr{)}=1

i.e.

lsin(3β+ψ)=12cos(β)sin(β+ψ)=:F(β,ψ).-l\sin(3\beta+\psi)=\frac{1}{2\cos(\beta)}-\sin(\beta+\psi)=:F(\beta,\psi).

Therefore, sin(3β+ψ)<0\sin(3\beta+\psi)<0 if and only if F(β,ψ)>0F(\beta,\psi)>0. It is easy to check that

Fβ(β,ψ)=sin(β)2cos2(β)cos(β+ψ)>sin(β)2cos2(β)cos(β)=sin(β)2cos3(β)2cos2(β)>0\frac{\partial F}{\partial\beta}(\beta,\psi)=\frac{\sin(\beta)}{2\cos^{2}(\beta)}-\cos(\beta+\psi)>\frac{\sin(\beta)}{2\cos^{2}(\beta)}-\cos(\beta)=\frac{\sin(\beta)-2\cos^{3}(\beta)}{2\cos^{2}(\beta)}>0

for β(π/4,β0]\beta\in(\pi/4,\beta_{0}]. Thus, the function F(β,ψ)F(\beta,\psi) is strictly increasing with respect to the variable β\beta for any ψ(ψ0,π/10]\psi\in(\psi_{0},\pi/10]. Further, it is easy to see that

Fψ(β,ψ)=cos(β+ψ)<0\frac{\partial F}{\partial\psi}(\beta,\psi)=-\cos(\beta+\psi)<0

for ψ(ψ0,π/10]\psi\in(\psi_{0},\pi/10]. Thus, the function F(β,ψ)F(\beta,\psi) is strictly decreasing with respect to the variable ψ\psi for any β(π/4,β0]\beta\in(\pi/4,\beta_{0}].

Refer to caption
Figure 8. Case 2.2.

Therefore, F(β0,ψ0)>F(β,ψ)F(\beta_{0},\psi_{0})>F(\beta,\psi). Now, it is easy to check that F(β0,ψ0)<0F(\beta_{0},\psi_{0})<0. Indeed,

12cos(β0)sin(β0+ψ0)=123sin(12arccos(312))=0.047891316<0.1-2\cos(\beta_{0})\sin(\beta_{0}+\psi_{0})=1-\sqrt{2\sqrt{3}}\sin\left(\frac{1}{2}\arccos\left(\frac{\sqrt{3}-1}{2}\right)\right)=-0.047891316...<0.

Consequently, F(β,ψ)<0F(\beta,\psi)<0 and we get a contradiction. Hence, Case 2.1 does not provide extremal quadrilaterals.

6.2. Case 2.2

Let us suppose that the quadrilateral under consideration is extremal. Assume, for definiteness, that H1H_{1} is an interior point of [A,B][A,B], H2H_{2} is an interior point of [A,D][A,D] and δ(bd(ABCD))=d(H1,C)=d(H1,D)=d(H2,B)=d(H2,C)=1\delta(\operatorname{bd}(ABCD))=d(H_{1},C)=d(H_{1},D)=d(H_{2},B)=d(H_{2},C)=1 (see Fig. 8).

Then Gmin[B,C]=G_{\min}\cap[B,C]=\emptyset and Gmin[D,C]=G_{\min}\cap[D,C]=\emptyset. By Corollary 5 we have DCH1BCH1\angle DCH_{1}\leq\angle BCH_{1} and BCH2DCH2\angle BCH_{2}\leq\angle DCH_{2}, respectively. However, DCH2<DCH1\angle DCH_{2}<\angle DCH_{1} and BCH1<BCH2\angle BCH_{1}<\angle BCH_{2}. This contradiction shows that our assumption (that ABCDABCD is extremal) is wrong.

6.3. Case 2.3

Let us suppose that the quadrilateral under consideration is extremal. Assume for definiteness that H1H_{1} is an interior point of [A,B][A,B], H2H_{2} is an interior point of [C,D][C,D], and δ(bd(ABCD))=d(H1,C)=d(H1,D)=d(H2,A)=d(H2,B)=1\delta(\operatorname{bd}(ABCD))=d(H_{1},C)=d(H_{1},D)=d(H_{2},A)=d(H_{2},B)=1 (see the left panel of Fig. 9). Without loss of generality, we may suppose that CDAπ/2\angle CDA\leq\pi/2.

We know that DH1Aπ/2\angle DH_{1}A\leq\pi/2. Suppose at first that DH1A<π/2\angle DH_{1}A<\pi/2. Then we have the inequality H1DCH1DA\angle H_{1}DC\leq\angle H_{1}DA (for an extremal quadrilateral) by Corollary 5. Since H1DC+H1DA=CDAπ/2\angle H_{1}DC+\angle H_{1}DA=\angle CDA\leq\pi/2, we get H1DC=H1CDπ/4\angle H_{1}DC=\angle H_{1}CD\leq\pi/4, then DH1Cπ/2\angle DH_{1}C\geq\pi/2 and we obtain the following simple estimate for the perimeter: L(bd(DCH1))2+2L(\operatorname{bd}(DCH_{1}))\geq 2+\sqrt{2}. Hence, we have L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}, that is impossible for an extremal quadrilateral.

Now, let us suppose that DH1A=π/2\angle DH_{1}A=\pi/2. It implies DAB=DAH1<π/2\angle DAB=\angle DAH_{1}<\pi/2 and we can repeat the above arguments changing the points A,B,C,D,H1,H2A,B,C,D,H_{1},H_{2} to the points C,D,A,B,H2,H1C,D,A,B,H_{2},H_{1}, respectively. Hence, if AH2D<π/2\angle AH_{2}D<\pi/2 we again get L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2} by Corollary 5.

Therefore, the remaining case, called Case 2.3a, is AH2D=π/2\angle AH_{2}D=\pi/2 that (together with DH1A=π/2\angle DH_{1}A=\pi/2) implies CDA=BAD\angle CDA=\angle BAD.

Thus ABCDABCD is an isosceles trapezoid with the bases DADA and CBCB (see the right panel of Fig. 9). Put α:=CDA=BAD(0,π/2)\alpha:=\angle CDA=\angle BAD\in\left(0,\pi/2\right). It is easy to see that H2AD=H1DA=π/2α\angle H_{2}AD=\angle H_{1}DA=\pi/2-\alpha and

H2AB=H2BA=H1DC=H1CD=α(π2α)=2απ2.\angle H_{2}AB=\angle H_{2}BA=\angle H_{1}DC=\angle H_{1}CD=\alpha-\left(\frac{\pi}{2}-\alpha\right)=2\alpha-\frac{\pi}{2}\,.

In particular, α>π/4\alpha>{\pi}/{4}.

Refer to caption

a)

Refer to caption

b)

Figure 9. a) Case 2.3; b) Case 2.3a.

Since the straight line H2L1H_{2}L_{1} is orthogonal to the straight line ABAB, then BH2L1=AH2L1=π/2(2απ/2)=π2α\angle BH_{2}L_{1}=\angle AH_{2}L_{1}={\pi}/{2}-\left(2\alpha-{\pi}/{2}\right)=\pi-2\alpha. Therefore, d(A,L1)=sin(π2α)=sin(2α)d(A,L_{1})=\sin(\pi-2\alpha)=\sin(2\alpha) and d(A,B)=d(D,C)=2sin(2α)d(A,B)=d(D,C)=2\sin(2\alpha).

Since the straight line BM1BM_{1} is orthogonal to the straight line ADAD, we get

d(A,M1)\displaystyle d(A,M_{1}) =\displaystyle= d(A,B)cos(α)=2sin(2α)cos(α)=4sin(α)cos2(α),\displaystyle d(A,B)\cos(\alpha)=2\sin(2\alpha)\cos(\alpha)=4\sin(\alpha)\cos^{2}(\alpha),
d(B,M1)\displaystyle d(B,M_{1}) =\displaystyle= d(A,B)sin(α)=2sin(2α)sin(α)=4sin2(α)cos(α).\displaystyle d(A,B)\sin(\alpha)=2\sin(2\alpha)\sin(\alpha)=4\sin^{2}(\alpha)\cos(\alpha).

From d(A,M1)<12d(A,D)d(A,M_{1})<\frac{1}{2}d(A,D), we get 4sin(α)cos2(α)<12sin(α)4\sin(\alpha)\cos^{2}(\alpha)<\frac{1}{2\sin(\alpha)} or sin2(2α)<1/2\sin^{2}(2\alpha)<1/2. Therefore, sin(2α)<12\sin(2\alpha)<\frac{1}{\sqrt{2}}. Solving this inequality and taking into account that π/2<2α<π\pi/2<2\alpha<\pi, we get α(3π/8,π/2)\alpha\in\left(3\pi/8,\pi/2\right).

Let OO be the midpoint of the line segment [D,A][D,A]. Then

d2(O,B)=d2(O,C)=d2(O,M1)+d2(B,M1)d^{2}(O,B)=d^{2}(O,C)=d^{2}(O,M_{1})+d^{2}(B,M_{1})
=(12sin(α)4sin(α)cos(α))2+16sin4(α)cos2(α)=\left(\frac{1}{2\sin(\alpha)}-4\sin(\alpha)\cos(\alpha)\right)^{2}+16\sin^{4}(\alpha)\cos^{2}(\alpha)
=14sin2(α)4cos2(α)+16sin2(α)cos2(α)=:h(α).=\frac{1}{4\sin^{2}(\alpha)}-4\cos^{2}(\alpha)+16\sin^{2}(\alpha)\cos^{2}(\alpha)=:h(\alpha).

It is easy to check that the function h(α)h(\alpha) is strictly decreasing for α(3π/8,π/2)\alpha\in\left(3\pi/8,\pi/2\right) and takes the value h(α)1h(\alpha)\geq 1 for α[3π/8,α0]\alpha\in\left[3\pi/8,\alpha_{0}\right], where α0=arccos(624)\alpha_{0}=\arccos\left(\frac{\sqrt{6}-\sqrt{2}}{4}\right). It follows from the following facts: h(α0)=1h(\alpha_{0})=1, h(α)=sin(2α)(16cos(2α)4+1(1cos(2α))2)h^{\prime}(\alpha)=-\sin(2\alpha)\left(-16\cos(2\alpha)-4+\frac{1}{(1-\cos(2\alpha))^{2}}\right), cos(2α)>1/2-\cos(2\alpha)>1/\sqrt{2} and sin(2α)>0\sin(2\alpha)>0 for α(3π/8,π/2)\alpha\in\left(3\pi/8,\pi/2\right).

Consider the perimeter

L(bd(ABCD))=2sin(α)8sin(α)cos2(α)+8sin(α)cos(α)=:g(α).L\bigl{(}\operatorname{bd}(ABCD)\bigr{)}=\frac{2}{\sin(\alpha)}-8\sin(\alpha)\cos^{2}(\alpha)+8\sin(\alpha)\cos(\alpha)=:g(\alpha).

It is easy to see that the function g(α)g(\alpha) is strictly decreasing for α[3π/8,α0]\alpha\in\left[3\pi/8,\alpha_{0}\right]. Indeed, g(α)=8f(cos(α))2cos(α)sin2(α)g^{\prime}(\alpha)=-8f\bigl{(}\cos(\alpha)\bigr{)}-2\frac{\cos(\alpha)}{\sin^{2}(\alpha)}, where f(t)=12t+2t23t3f(t)=1-2t+2t^{2}-3t^{3}. It is easy to check that the maximal value of f(t)f(t) for t[cos(α0),cos(3π/8)]t\in[\cos(\alpha_{0}),\cos(3\pi/8)] is f(cos(3π/8))=0.1098679896f\bigl{(}\cos(3\pi/8)\bigr{)}=-0.1098679896... Hence, g(α)<2cos(α)sin2(α)<0g^{\prime}(\alpha)<-2\frac{\cos(\alpha)}{\sin^{2}(\alpha)}<0 on the segment [3π/8,α0]\left[3\pi/8,\alpha_{0}\right].

Therefore, g(α)g(\alpha) achieves its minimal value on [3π/8,α0]\left[3\pi/8,\alpha_{0}\right] exactly at the point α=α0\alpha=\alpha_{0}. This minimal value is

g(arccos(624))=3(62)2+2=3.55291.g\left(\arccos\left(\frac{\sqrt{6}-\sqrt{2}}{4}\right)\right)=\frac{3(\sqrt{6}-\sqrt{2})}{2}+2=3.55291....

Therefore, the quadrilateral ABCDABCD is not extremal.

7. Case 3

In this section we deal with the case Gmin=3\|G_{\min}\|=3, i. e. bd(ABCD)\operatorname{bd}(ABCD) has three self Chebyshev centers. We consider several subcases according to Fig. 4.

7.1. Case 3.1

Let us suppose that Gmin=3\|G_{\min}\|=3 and Gmin={H1,H2,G}G_{\min}=\{H_{1},H_{2},G\}. Without loss of generality, we may suppose that H1H_{1} is an interior point of [B,C][B,C], H2H_{2} is an interior point of [A,D][A,D], GG is an interior point of [A,B][A,B] such that d(A,G)d(B,G)d(A,G)\leq d(B,G), and δ(bd(ABCD))=d(H1,A)=d(H2,B)=d(G,D)=d(G,C)=1\delta(\operatorname{bd}(ABCD))=d(H_{1},A)=d(H_{2},B)=d(G,D)=d(G,C)=1. It is clear that AH1AH_{1} is orthogonal to [B,C][B,C] and BH2BH_{2} is orthogonal to [A,D][A,D]. Moreover, AGDπ/2\angle AGD\leq\pi/2 and BGCπ/2\angle BGC\leq\pi/2 by Proposition 6. We put α:=DAB=CBA\alpha:=\angle DAB=\angle CBA.

Lemma 4.

In the conditions as above, we get απ/3\alpha\geq\pi/3. If, in addition, d(B,G)1d(B,G)\geq 1, then L(bd(ABCD))2+2L\bigl{(}\operatorname{bd}(ABCD)\bigr{)}\geq 2+\sqrt{2}.

Proof. Let us consider the quadrilateral ABCDABCD as a subset of the isosceles triangle ABEABE (see the left panel of Fig. 10). We put x=d(A,G)x=d(A,G), y=d(G,B)y=d(G,B), where xyx\leq y.

Since ADBπ/2\angle ADB\leq\pi/2, then we get ADGπ/2\angle ADG\leq\pi/2 and GDEπ/2\angle GDE\geq\pi/2. Since AGDπ/2\angle AGD\leq\pi/2 and d(A,G)d(B,G)d(A,G)\leq d(B,G), then there is a point D[D,E]D^{\prime}\in[D,E], such that the straight line DGD^{\prime}G is orthogonal to the straight line ABAB. The inequality GDEπ/2\angle GDE\geq\pi/2 implies d(G,D)d(G,D)=1d(G,D^{\prime})\geq d(G,D)=1. Since cos(α)sin(α)=d(A,G)d(G,D)d(A,G)=x\frac{\cos(\alpha)}{\sin(\alpha)}=\frac{d(A,G)}{d(G,D^{\prime})}\leq d(A,G)=x, then we get xcos(α)sin(α)x\geq\frac{\cos(\alpha)}{\sin(\alpha)}.

On the other hand, d(A,B)=x+y=1sin(α)d(A,B)=x+y=\frac{1}{\sin(\alpha)}, hence x12sin(α)x\leq\frac{1}{2\sin(\alpha)}. Therefore,

cos(α)sin(α)x12sin(α).\frac{\cos(\alpha)}{\sin(\alpha)}\leq x\leq\frac{1}{2\sin(\alpha)}.

Hence, we get cos(α)1/2\cos(\alpha)\leq 1/2 or, equivalently, απ/3\alpha\geq\pi/3.

Now, if d(B,G)1d(B,G)\geq 1, then the perimeter of the triangle BGDBGD is as least 2+22+\sqrt{2}. Indeed, it easily follows from the relations d(G,D)=1d(G,D)=1, d(G,B)1d(G,B)\geq 1, and BGDπ/2\angle BGD\geq\pi/2. Since quadrilateral ABCDABCD contains the triangle BGDBGD, then L(Γ)2+2L(\Gamma)\geq 2+\sqrt{2}.   

Refer to caption

a)

Refer to caption

b)

Figure 10. a) Case 3.1; b) Case 3.1a.

Now we consider, the following class 𝒫spec\mathcal{P}_{\operatorname{spec}} of quadrilaterals: a quadrilateral ABCDABCD is in 𝒫spec\mathcal{P}_{\operatorname{spec}} if and only if the following conditions hold: α:=DAB=CBA[π/3,π/2)\alpha:=\angle DAB=\angle CBA\in[\pi/3,\pi/2) and there are H1[B,C]H_{1}\in[B,C], H2[A,D]H_{2}\in[A,D], and G[A,B]G\in[A,B] such that d(H1,A)=d(H2,B)=d(G,D)=d(G,C)=1d(H_{1},A)=d(H_{2},B)=d(G,D)=d(G,C)=1, d(A,G)d(B,G)1d(A,G)\leq d(B,G)\leq 1, AH1[B,C]AH_{1}\perp[B,C], BH2[A,D]BH_{2}\perp[A,D], AGDπ/2\angle AGD\leq\pi/2, BGCπ/2\angle BGC\leq\pi/2.

Lemma 4 implies that any quadrilateral in Case 3.1 with d(G,B)1d(G,B)\leq 1 is in the class 𝒫spec\mathcal{P}_{\operatorname{spec}}. Now, it suffices to prove the following

Proposition 11.

For any quadrilateral P=ABCDP=ABCD in the class 𝒫spec\mathcal{P}_{\operatorname{spec}}, we have δ(Γ)1\delta(\Gamma)\leq 1 and L(Γ)2+2L(\Gamma)\geq 2+\sqrt{2}. In particular, there is no extremal quadrilateral in 𝒫spec\mathcal{P}_{\operatorname{spec}}.

Proof. Since the distances from the points A,B,C,DA,B,C,D to GG is at most 11, then δ(Γ)1\delta(\Gamma)\leq 1. Let us prove that L(Γ)2+2L(\Gamma)\geq 2+\sqrt{2}. We put x:=d(A,G)x:=d(A,G), y:=d(G,B)y:=d(G,B), β:=DGA\beta:=\angle DGA, and γ:=CGB\gamma:=\angle CGB. We have xyx\leq y by our assumptions. Note that d(A,B)=x+y=1sin(α)d(A,B)=x+y=\frac{1}{\sin(\alpha)}, hence, x12sin(α)x\leq\frac{1}{2\sin(\alpha)}. It is easy to see also that xcos(α)sin(α)x\geq\frac{\cos(\alpha)}{\sin(\alpha)} (see e.g. the proof of Lemma 4)

Let us consider EE, the intersection point of the straight lines ADAD and BCBC (the quadrilateral ABCDABCD is a subset of the isosceles triangle ABEABE), see the left panel of Fig. 10.

Since d(D,G)=d(C,G)=1d(D,G)=d(C,G)=1, then we have GDC=GCD=β+γ2\angle GDC=\angle GCD=\frac{\beta+\gamma}{2} and d(C,D)=2cos(β+γ2)d(C,D)=2\cos\left(\frac{\beta+\gamma}{2}\right). The equalities d(A,D)sin(β)=1sin(α)\frac{d(A,D)}{\sin(\beta)}=\frac{1}{\sin(\alpha)} and d(B,C)sin(γ)=1sin(α)\frac{d(B,C)}{\sin(\gamma)}=\frac{1}{\sin(\alpha)} imply d(A,D)+d(B,C)=sin(β)+sin(γ)sin(α)d(A,D)+d(B,C)=\frac{\sin(\beta)+\sin(\gamma)}{\sin(\alpha)}. Therefore, we get

L(Γ)=d(A,B)+d(B,C)+d(C,D)+d(D,A)=1sin(α)+sin(β)+sin(γ)sin(α)+2cos(β+γ2).L(\Gamma)=d(A,B)+d(B,C)+d(C,D)+d(D,A)=\frac{1}{\sin(\alpha)}+\frac{\sin(\beta)+\sin(\gamma)}{\sin(\alpha)}+2\cos\left(\frac{\beta+\gamma}{2}\right).

The equalities xsin(α+β)=1sin(α)\frac{x}{\sin(\alpha+\beta)}=\frac{1}{\sin(\alpha)} and ysin(α+γ)=1sin(α)\frac{y}{\sin(\alpha+\gamma)}=\frac{1}{\sin(\alpha)} imply x=sin(α+β)sin(α)x=\frac{\sin(\alpha+\beta)}{\sin(\alpha)} and y=sin(α+γ)sin(α)y=\frac{\sin(\alpha+\gamma)}{\sin(\alpha)}, respectively. Since x+y=1sin(α)x+y=\frac{1}{\sin(\alpha)}, then we get sin(α+β)+sin(α+γ)=1\sin(\alpha+\beta)+\sin(\alpha+\gamma)=1.

Now, we introduce new variables tt and ss such that t:=β+γ2t:=\frac{\beta+\gamma}{2} and s:=βγ2s:=\frac{\beta-\gamma}{2}. We get

sin(β)+sin(γ)=2sin(β+γ2)cos(βγ2)=2sin(t)cos(s).\sin(\beta)+\sin(\gamma)=2\sin\left(\frac{\beta+\gamma}{2}\right)\cos\left(\frac{\beta-\gamma}{2}\right)=2\sin(t)\cos(s).

The equation

1=sin(α+β)+sin(α+γ)=2sin(α+β+γ2)cos(βγ2)=2sin(α+t)cos(s),1=\sin(\alpha+\beta)+\sin(\alpha+\gamma)=2\sin\left(\alpha+\frac{\beta+\gamma}{2}\right)\cos\left(\frac{\beta-\gamma}{2}\right)=2\sin(\alpha+t)\cos(s),

implies cos(s)=12sin(α+t)\cos(s)=\frac{1}{2\sin(\alpha+t)}. Therefore, we get

L(Γ)\displaystyle L(\Gamma) =\displaystyle= 1sin(α)+sin(β)+sin(γ)sin(α)+2cos(β+γ2)\displaystyle\frac{1}{\sin(\alpha)}+\frac{\sin(\beta)+\sin(\gamma)}{\sin(\alpha)}+2\cos\left(\frac{\beta+\gamma}{2}\right)
=\displaystyle= 1sin(α)+sin(t)sin(α)sin(α+t)+2cos(t)=:F(α,t).\displaystyle\frac{1}{\sin(\alpha)}+\frac{\sin(t)}{\sin(\alpha)\sin(\alpha+t)}+2\cos(t)=:F(\alpha,t).

We will now find useful upper and lower bounds for the value tt. The equation xsin(α+β)=1sin(α)\frac{x}{\sin(\alpha+\beta)}=\frac{1}{\sin(\alpha)} implies sin(α+β)=xsin(α)\sin(\alpha+\beta)=x\sin(\alpha) and παβ=arcsin(xsin(α))\pi-\alpha-\beta=\arcsin(x\sin(\alpha)), that could be rewritten as

β=παarcsin(xsin(α)).\beta=\pi-\alpha-\arcsin\bigl{(}x\sin(\alpha)\bigr{)}.

Similarly, we get

γ=παarcsin(ysin(α))=παarcsin(1xsin(α)).\gamma=\pi-\alpha-\arcsin(y\sin(\alpha))=\pi-\alpha-\arcsin\bigl{(}1-x\sin(\alpha)\bigr{)}.

The above equality obviously implies

t=β+γ2=πα12arcsin(xsin(α))12arcsin(1xsin(α))=:u(x).t=\frac{\beta+\gamma}{2}=\pi-\alpha-\frac{1}{2}\arcsin(x\sin(\alpha))-\frac{1}{2}\arcsin\bigl{(}1-x\sin(\alpha)\bigr{)}=:u(x).

It is easy to check that

u(x)=sin(α)2(arcsin(1xsin(α))arcsin(xsin(α))).u^{\prime}(x)=\frac{\sin(\alpha)}{2}\Bigl{(}\arcsin^{\prime}\bigl{(}1-x\sin(\alpha)\bigr{)}-\arcsin^{\prime}\bigl{(}x\sin(\alpha)\bigr{)}\Bigr{)}.

Therefore, u(x)0u^{\prime}(x)\geq 0 if and only if 1xsin(α)xsin(α)>01-x\sin(\alpha)\geq x\sin(\alpha)>0 or, equivalently, 0<x12sin(α)0<x\leq\frac{1}{2\sin(\alpha)}.

Since cos(α)sin(α)x12sin(α),\frac{\cos(\alpha)}{\sin(\alpha)}\leq x\leq\frac{1}{2\sin(\alpha)}, we will find the value of the function uu at the boundary points:

u(12sin(α))\displaystyle u\left(\frac{1}{2\sin(\alpha)}\right) =\displaystyle= παarcsin(12)=5π6α.\displaystyle\pi-\alpha-\arcsin\left(\frac{1}{2}\right)=\frac{5\pi}{6}-\alpha.
u(cos(α)sin(α))\displaystyle u\left(\frac{\cos(\alpha)}{\sin(\alpha)}\right) =\displaystyle= πα12arcsin(cos(α))12arcsin(1cos(α))\displaystyle\pi-\alpha-\frac{1}{2}\arcsin\bigl{(}\cos(\alpha)\bigr{)}-\frac{1}{2}\arcsin\bigl{(}1-\cos(\alpha)\bigr{)}
=\displaystyle= 34π12α+12arcsin(cos(α)1)=:l(α).\displaystyle\frac{3}{4}\pi-\frac{1}{2}\alpha+\frac{1}{2}\arcsin\bigl{(}\cos(\alpha)-1\bigr{)}=:l(\alpha).

Therefore, l(α)t56παl(\alpha)\leq t\leq\frac{5}{6}\pi-\alpha for a given α[π/3,π/2]\alpha\in[\pi/3,\pi/2]. Now, we will prove that the minimal value of F(α,t)F(\alpha,t) on the set

S:={(α,t)|π3απ2,l(α)t5π6α}S:=\left\{(\alpha,t)\,\left|\,\,\frac{\pi}{3}\leq\alpha\leq\frac{\pi}{2},\,l(\alpha)\leq t\leq\frac{5\pi}{6}-\alpha\right.\right\} (7)

is 2+22+\sqrt{2}. It will be suffices to prove the proposition.

It is easy to see that l(α)=12(1+sin(α)1(cos(α)1)2)<0l^{\prime}(\alpha)=-\frac{1}{2}\left(1+\frac{\sin(\alpha)}{\sqrt{1-(\cos(\alpha)-1)^{2}}}\right)<0 for α[0,π2)\alpha\in[0,\frac{\pi}{2}). Therefore, the function ll is strictly decreasing on the interval [0,π2][0,\frac{\pi}{2}], l(0)=3π/4l(0)=3\pi/4, l(π/2)=π/4l(\pi/2)=\pi/4. By direct computations, we get

Fα(α,t)\displaystyle\frac{\partial F}{\partial\alpha}(\alpha,t) =\displaystyle\!\!\!\!=\!\!\!\! cos(α)sin2(α)sin(t)cos(α)sin2(α)sin(α+t)sin(t)cos(α+t)sin(α)sin2(α+t)\displaystyle-\frac{\cos(\alpha)}{\sin^{2}(\alpha)}-\frac{\sin(t)\cos(\alpha)}{\sin^{2}(\alpha)\sin(\alpha+t)}-\frac{\sin(t)\cos(\alpha+t)}{\sin(\alpha)\sin^{2}(\alpha+t)}
=\displaystyle\!\!\!\!=\!\!\!\! cos(α)+1sin2(α)sin2(α+t)(cos2(α+t)cos(α))\displaystyle\frac{\cos(\alpha)+1}{\sin^{2}(\alpha)\sin^{2}(\alpha+t)}\bigl{(}\cos^{2}(\alpha+t)-\cos(\alpha)\bigr{)}
=\displaystyle\!\!\!\!=\!\!\!\! cos(α)+1sin2(α)sin2(α+t)(2sin2(α2)sin2(α+t))\displaystyle\frac{\cos(\alpha)+1}{\sin^{2}(\alpha)\sin^{2}(\alpha+t)}\left(2\sin^{2}\left(\frac{\alpha}{2}\right)-\sin^{2}(\alpha+t)\right)
=\displaystyle\!\!\!\!=\!\!\!\! cos(α)+1sin2(α)sin2(α+t)(2sin(α2)+sin(α+t))(2sin(α2)sin(α+t)).\displaystyle\frac{\cos(\alpha)+1}{\sin^{2}(\alpha)\sin^{2}(\alpha+t)}\left(\sqrt{2}\sin\left(\frac{\alpha}{2}\right)+\sin(\alpha+t)\right)\left(\sqrt{2}\sin\left(\frac{\alpha}{2}\right)-\sin(\alpha+t)\right).

The derivative Fα(α,t)\frac{\partial F}{\partial\alpha}(\alpha,t) has the same sign as the expression (2sin(α2)sin(α+t))\left(\sqrt{2}\sin\left(\frac{\alpha}{2}\right)-\sin(\alpha+t)\right). Solving equation 2sin(α/2)=sin(α+t)\sqrt{2}\sin\left(\alpha/2\right)=\sin(\alpha+t) with respect to tt, we obtain

t=παarcsin(2sin(α/2)).t=\pi-\alpha-\arcsin\left(\sqrt{2}\sin\bigl{(}\alpha/2\bigr{)}\right).

It is easy to show that the graph of this function does not intersect a two-dimensional connected set SS (see (7)). Since 2sin(π/4)sin(π/2+π/4)=222>0\sqrt{2}\sin\left(\pi/4\right)-\sin\left(\pi/2+\pi/4\right)=\frac{2-\sqrt{2}}{2}>0, then we get Fα(π/2,π/4)>0\frac{\partial F}{\partial\alpha}(\pi/2,\pi/4)>0. Thus, the function F(α,t)F(\alpha,t) is strictly increasing with respect to the variable α\alpha for any t[l(α),5π/6α]t\in\left[l(\alpha),5\pi/6-\alpha\right].

Therefore, the function F(α,t)F(\alpha,t) achieves its minimum value on SS at one of the points of the curve t=l(α)t=l(\alpha), that corresponds to the following configuration, which will be called Case 3.1a (see the right panel of Fig. 10): d(A,H1)=d(B,H2)=d(D,G)=d(C,G)=1d(A,H_{1})=d(B,H_{2})=d(D,G)=d(C,G)=1, AGD=π/2\angle AGD=\pi/2. Now we are going to find the explicit expression for F(α,l(α))F(\alpha,l(\alpha)), α[π/3,π/2)\alpha\in[\pi/3,\pi/2).

We have d(A,B)=d(A,D)=1sin(α)d(A,B)=d(A,D)=\frac{1}{\sin(\alpha)}, d(A,G)=cos(α)sin(α)d(A,G)=\frac{\cos(\alpha)}{\sin(\alpha)} and d(G,B)=1cos(α)sin(α)d(G,B)=\frac{1-\cos(\alpha)}{\sin(\alpha)} for t=l(α)t=l(\alpha). Let GDC=GCD=β\angle GDC=\angle GCD=\beta. Since DGCπ/2\angle DGC\leq\pi/2, we have β[π/4,π/2]\beta\in\left[\pi/4,\pi/2\right]. It is clear that CGB=π/2(π2β)=2βπ/2\angle CGB=\pi/2-(\pi-2\beta)=2\beta-\pi/2. The equations

d(B,C)sin(2βπ/2)=d(B,C)cos(2β)=d(C,G)sin(α)=1sin(α)\frac{d(B,C)}{\sin(2\beta-\pi/2)}=\frac{d(B,C)}{-\cos(2\beta)}=\frac{d(C,G)}{\sin(\alpha)}=\frac{1}{\sin(\alpha)}

imply d(B,C)=cos(2β)sin(α)d(B,C)=-\frac{\cos(2\beta)}{\sin(\alpha)}. Since d(C,D)=2cos(β)d(C,D)=2\cos(\beta), then we have

F(α,l(α))=d(A,B)+d(B,C)+d(C,D)+d(D,A)=2cos(2β)sin(α)+2cos(β).F(\alpha,l(\alpha))=d(A,B)+d(B,C)+d(C,D)+d(D,A)=\frac{2-\cos(2\beta)}{\sin(\alpha)}+2\cos(\beta).

It is clear that GCB=π(2βπ/2+α)=3π/2(α+2β)\angle GCB=\pi-\left(2\beta-\pi/2+\alpha\right)=3\pi/2-(\alpha+2\beta). Since GCB[0,π/2]\angle GCB\in[0,\pi/2], then α+2β[π,3π/2]\alpha+2\beta\in\left[\pi,3\pi/2\right]. The equations

d(C,G)sin(α)=1sin(α)=d(G,B)sin(GCB)=d(G,B)cos(α+2βπ)=1cos(α)sin(α)cos(α+2βπ)\frac{d(C,G)}{\sin(\alpha)}=\frac{1}{\sin(\alpha)}=\frac{d(G,B)}{\sin(\angle GCB)}=\frac{d(G,B)}{\cos(\alpha+2\beta-\pi)}=\frac{1-\cos(\alpha)}{\sin(\alpha)\cos(\alpha+2\beta-\pi)}

imply cos(α+2βπ)=1cos(α)\cos(\alpha+2\beta-\pi)=1-\cos(\alpha). Therefore, 2β=πα+arccos(1cos(α))2\beta=\pi-\alpha+\arccos\bigl{(}1-\cos(\alpha)\bigr{)} and, consequently,

cos(2β)=cos(αarccos(1cos(α)))=cos2(α)cos(α)2cos(α)cos2(α)sin(α).\cos(2\beta)=-\cos\bigl{(}\alpha-\arccos(1-\cos(\alpha))\bigr{)}=\cos^{2}(\alpha)-\cos(\alpha)-\sqrt{2\cos(\alpha)-\cos^{2}(\alpha)}\sin(\alpha).

Since cos(β)=1+cos(2β)2\cos(\beta)=\sqrt{\frac{1+\cos(2\beta)}{2}}, then we get

F(α,l(α))\displaystyle F(\alpha,l(\alpha)) =\displaystyle= 2+cos(α)cos2(α)sin(α)+2cos(α)cos2(α)\displaystyle\frac{2+\cos(\alpha)-\cos^{2}(\alpha)}{\sin(\alpha)}+\sqrt{2\cos(\alpha)-\cos^{2}(\alpha)}
+2+2cos2(α)2cos(α)22cos(α)cos2(α)sin(α)=:g(α).\displaystyle+\sqrt{2+2\cos^{2}(\alpha)-2\cos(\alpha)-2\sqrt{2\cos(\alpha)-\cos^{2}(\alpha)}\sin(\alpha)}=:g(\alpha).

By direct computations we get that the function g(α)g(\alpha) achieves its maximal value on [π/3,π/2]\left[\pi/3,\pi/2\right] at the point α=arccos(t0)=1.416644291\alpha=\arccos(t_{0})=1.416644291..., where t0t_{0} is the root of the polynomial f(t)=16t7120t6+346t5485t4+348t3118t2+18t1f(t)=16t^{7}-120t^{6}+346t^{5}-485t^{4}+348t^{3}-118t^{2}+18t-1 on the interval [0.15,0.16][0.15,0.16]. This maximal value is

g(arccos(t0))=3.51731.g\bigl{(}\arccos(t_{0})\bigr{)}=3.51731....

By direct computations we get also that the function g(α)g(\alpha) achieves its minimal value on [π/3,π/2]\left[\pi/3,\pi/2\right] exactly at the point α=π/2\alpha=\pi/2. This minimal value is g(π/2)=2+2g\left(\pi/2\right)=2+\sqrt{2}. Therefore, F(α,t)F(α,l(α))=g(α)g(π/2)=2+2F(\alpha,t)\geq F(\alpha,l(\alpha))=g(\alpha)\geq g(\pi/2)=2+\sqrt{2} for all (a,t)S(a,t)\in S. The proposition is proved.   

Remark 5.

Note that minimal value of F(α,t)F(\alpha,t) on SS is achieved at the point (α,t)=(π/2,l(π/2))=(π/2,π/4)(\alpha,t)=(\pi/2,l(\pi/2))=(\pi/2,\pi/4), that corresponds to a degenerate quadrilateral ABCDABCD, where B=CB=C, d(A,B)=d(A,D)=1d(A,B)=d(A,D)=1, and BAD=π/2\angle BAD=\pi/2. The self Chebyshev radius of the boundary of this degenerate quadrilateral (in fact, a triangle) is 1/2<11/\sqrt{2}<1.

7.2. Case 3.2

Without loss of generality, we may suppose that Gmin={E,G,F}G_{\min}=\{E,G,F\} (see Fig. 11), where EE is an interior point of [A,B][A,B], FF is an interior point of [B,C][B,C], GG is an interior point of [A,D][A,D] such that d(A,G)d(D,G)d(A,G)\leq d(D,G), and δ(bd(ABCD))=d(E,D)=d(F,A)=d(G,B)=d(G,C)=1\delta(\operatorname{bd}(ABCD))=d(E,D)=d(F,A)=d(G,B)=d(G,C)=1. It is clear that DEDE is orthogonal to [A,B][A,B] and AFAF is orthogonal to [B,C][B,C]. Moreover, AGBπ/2\angle AGB\leq\pi/2 and DGCπ/2\angle DGC\leq\pi/2 by Proposition 6.

Now we are going to show that this case is impossible.

Remark 6.

It should be noted that it does not matter for the arguments below whether there is a fourth self Chebyshev center for bd(ABCD)\operatorname{bd}(ABCD) or not. Therefore, we can use this arguments also for some quadrilaterals with four self Chebyshev centers.

Refer to caption

a)

Refer to caption

b)

Figure 11. a) Case 3.2a; b) Case 3.2b.

We put GCB=GBC=:φ\angle GCB=\angle GBC=:\varphi, BAD=:α\angle BAD=:\alpha and BAF=:β\angle BAF=:\beta (see the left panel of Fig. 11). Let FF^{\prime} is an interior point of [A,D][A,D] such that the straight line FFFF^{\prime} is orthogonal to the straight line [A,D][A,D].

Since d(A,D)=1/sin(α)d(A,D)=1/\sin(\alpha) and d(A,F)=d(A,F)cos(αβ)=cos(αβ)d(A,F^{\prime})=d(A,F)\cos(\alpha-\beta)=\cos(\alpha-\beta), then we have d(F,D)=d(A,D)d(A,F)=1/sin(α)cos(αβ)d(F^{\prime},D)=d(A,D)-d(A,F^{\prime})=1/\sin(\alpha)-\cos(\alpha-\beta). It is clear that d(F,F)=d(A,F)sin(αβ)=sin(αβ)d(F^{\prime},F)=d(A,F)\sin(\alpha-\beta)=\sin(\alpha-\beta). Therefore, we get

d2(F,D)=d2(F,D)+d2(F,F)=(1sin(α)cos(αβ))2+sin2(αβ)d^{2}(F,D)=d^{2}(F^{\prime},D)+d^{2}(F^{\prime},F)=\left(\frac{1}{\sin(\alpha)}-\cos(\alpha-\beta)\right)^{2}+\sin^{2}(\alpha-\beta)
=1sin2(α)2cos(αβ)sin(α)+1=12cos(αβ)sin(α)sin2(α)+1.=\frac{1}{\sin^{2}(\alpha)}-\frac{2\cos(\alpha-\beta)}{\sin(\alpha)}+1=\frac{1-2\cos(\alpha-\beta)\sin(\alpha)}{\sin^{2}(\alpha)}+1.

Hence, d2(F,D)1d^{2}(F,D)\leq 1 if and only if 2cos(αβ)sin(α)12\cos(\alpha-\beta)\sin(\alpha)\geq 1.

Since AGBπ/2\angle AGB\leq\pi/2, there is a point B[A,G]B^{\prime}\in[A,G], such that the straight line BBB^{\prime}B is orthogonal to the straight line ADAD (see the right panel of Fig. 11). It is easy to see that BBG=ABFABBGBC=π/2β(π/2α)φ=αβφ\angle B^{\prime}BG=\angle ABF-\angle ABB^{\prime}-\angle GBC=\pi/2-\beta-(\pi/2-\alpha)-\varphi=\alpha-\beta-\varphi. Hence, BGA=π/2(αβφ)\angle BGA=\pi/2-(\alpha-\beta-\varphi).

The equations

d(B,G)sin(α)=1sin(α)=d(A,B)sin(BGA)=1cos(β)cos(αβφ)\frac{d(B,G)}{\sin(\alpha)}=\frac{1}{\sin(\alpha)}=\frac{d(A,B)}{\sin(\angle BGA)}=\frac{1}{\cos(\beta)\cos(\alpha-\beta-\varphi)}

imply cos(αβφ)=sin(α)/cos(β)\cos(\alpha-\beta-\varphi)=\sin(\alpha)/\cos(\beta). Therefore, φ=αβarccos(sin(α)cos(β))\varphi=\alpha-\beta-\arccos\left(\frac{\sin(\alpha)}{\cos(\beta)}\right) and, consequently,

cos(φ)=cos(αβ)sin(α)cos(β)+sin(αβ)sin(arccos(sin(α)cos(β)))\cos(\varphi)=\cos(\alpha-\beta)\frac{\sin(\alpha)}{\cos(\beta)}+\sin(\alpha-\beta)\sin\left(\arccos\left(\frac{\sin(\alpha)}{\cos(\beta)}\right)\right)
=1cos(β)(cos(αβ)sin(α)+sin(αβ)cos2(β)sin2(α)).=\frac{1}{\cos(\beta)}(\cos(\alpha-\beta)\sin(\alpha)+\sin(\alpha-\beta)\sqrt{\cos^{2}(\beta)-\sin^{2}(\alpha)}).

Let CC^{\prime} is an interior point of [A,B][A,B] such that the straight line CCCC^{\prime} is orthogonal to the straight line ABAB (see the right panel of Fig. 11). The equations

d(B,C)=2cos(φ)=d(C,C)sin(π/2β)=d(C,C)cos(β)d(B,C)=2\cos(\varphi)=\frac{d(C,C^{\prime})}{\sin(\pi/2-\beta)}=\frac{d(C,C^{\prime})}{\cos(\beta)}

imply d(C,C)=2cos(φ)cos(β)d(C,C^{\prime})=2\cos(\varphi)\cos(\beta).

It is easy to see that d(B,C)=d(B,C)cos(π/2β)=2cos(φ)sin(β)d(B,C^{\prime})=d(B,C)\cos(\pi/2-\beta)=2\cos(\varphi)\sin(\beta), d(A,E)=cot(α)d(A,E)=\cot(\alpha) and d(A,B)=1cos(β)d(A,B)=\frac{1}{\cos(\beta)}. Hence,

d(E,C)=d(A,B)d(A,E)d(B,C)=1cos(β)cot(α)2cos(φ)sin(β).d(E,C^{\prime})=d(A,B)-d(A,E)-d(B,C^{\prime})=\frac{1}{\cos(\beta)}-\cot(\alpha)-2\cos(\varphi)\sin(\beta).

Therefore, we get

d2(E,C)=d2(E,C)+d2(C,C)d^{2}(E,C)=d^{2}(E,C^{\prime})+d^{2}(C,C^{\prime})
=(1cos(β)cot(α)2cos(φ)sin(β))2+4cos2(φ)cos2(β).=\left(\frac{1}{\cos(\beta)}-\cot(\alpha)-2\cos(\varphi)\sin(\beta)\right)^{2}+4\cos^{2}(\varphi)\cos^{2}(\beta).

Let us now show that the inequalities d2(F,D)1d^{2}(F,D)\leq 1 and d2(E,C)1d^{2}(E,C)\leq 1 cannot hold simultaneously. For this goal, we prove the following simple result.

Lemma 5.

Let MM be a topological space and X,YX,Y are closed subsets of MM. Let the following conditions be satisfied:

  • YY be a connected set;

  • bd(X)Y=\operatorname{bd}(X)\cap Y=\emptyset;

  • There exists xYx\in Y such that xXx\notin X.

Then XY=X\cap Y=\emptyset.

Proof. Let X1=Xbd(X)X_{1}=X{\setminus}\operatorname{bd}(X) and X2=MXX_{2}=M{\setminus}X. It is clear that YX1X2Y\subset X_{1}\cup X_{2} and X1,X2X_{1},X_{2} are open and disjoint sets. As YY is a connected set, we have YX1Y\subset X_{1} or YX2Y\subset X_{2}. By the third property, YX1Y\subset X_{1} is impossible. Hence, YX2Y\subset X_{2} and XY=X\cap Y=\emptyset.   

Let YY the connected set of solutions (α,β)[0,π/2]2(\alpha,\beta)\in[0,\pi/2]^{2} to the inequality d2(F,D)1d^{2}(F,D)\leq 1 (i.e. 2cos(αβ)sin(α)12\cos(\alpha-\beta)\sin(\alpha)\geq 1) and XX the set of solutions to the inequality d2(E,C)1d^{2}(E,C)\leq 1. If 2cos(αβ)sin(α)=12\cos(\alpha-\beta)\sin(\alpha)=1 then β=arccos(12sin(α))+α\beta=-\arccos\left(\frac{1}{2\sin(\alpha)}\right)+\alpha and

d2(C,C)=(4sin2(α)1sin2(α)cos(arccos(12sin(α))+α)2sin2(α)+1)2>1.d^{2}(C,C^{\prime})=\left(\sqrt{\frac{4\sin^{2}(\alpha)-1}{\sin^{2}(\alpha)}}\sqrt{\cos\left(-\arccos\left(\frac{1}{2\sin(\alpha)}\right)+\alpha\right)^{2}-\sin^{2}(\alpha)}+1\right)^{2}>1.

Hence, d2(E,C)>1d^{2}(E,C)>1 and bd(X)Y=\operatorname{bd}(X)\cap Y=\emptyset. It is easy to see that xYx\in Y and xXx\notin X for the point x=(π/4,π/4)x=(\pi/4,\pi/4). Therefore, the inequalities d2(F,D)1d^{2}(F,D)\leq 1 and d2(E,C)1d^{2}(E,C)\leq 1 cannot hold simultaneously. Hence, the case under consideration is impossible.

7.3. Case 3.3

Suppose that Gmin=3\|G_{\min}\|=3 and Gmin={E,G,H}G_{\min}=\{E,G,H\} (see Fig. 12). Without loss of generality, we may suppose that EE is an interior point of [A,B][A,B], GG is an interior point of [A,D][A,D], HH is an interior point of [C,D][C,D], and δ(bd(ABCD))=d(E,D)=d(G,B)=d(G,C)=d(H,A)=d(H,B)=1\delta(\operatorname{bd}(ABCD))=d(E,D)=d(G,B)=d(G,C)=d(H,A)=d(H,B)=1. It is clear that EDED is orthogonal to [A,B][A,B]. Moreover, AGBπ/2\angle AGB\leq\pi/2 and DGCπ/2\angle DGC\leq\pi/2, AHDπ/2\angle AHD\leq\pi/2 and BHCπ/2\angle BHC\leq\pi/2 by Proposition 6.

Refer to caption
Figure 12. Case 3.3.

Let us consider the quadrilateral ABCDABCD as a subset of the triangle ATDATD (see Fig. 12). We put α:=BAD\alpha:=\angle BAD, β:=HAB=HBA\beta:=\angle HAB=\angle HBA, and γ:=ATD\gamma:=\angle ATD. Since BAD>HAB\angle BAD>\angle HAB and HBA>ATD\angle HBA>\angle ATD, we get α>β>γ>0\alpha>\beta>\gamma>0.

Since β+γ=HAT+HTA=AHDπ/2\beta+\gamma=\angle HAT+\angle HTA=\angle AHD\leq\pi/2, we get γπ/2β\gamma\leq\pi/2-\beta and cot(γ)cot(π/2β)=tan(β)\cot(\gamma)\geq\cot(\pi/2-\beta)=\tan(\beta). It is clear that d(A,D)sinADTd(A,D)\cdot\sin\angle ADT, the distance from the point AA to the straight line DTDT, is at most d(A,H)=1=d(D,E)=d(A,D)sinBADd(A,H)=1=d(D,E)=d(A,D)\sin\angle BAD. Therefore, sinADT=sin(παγ)=sin(α+γ)sin(α)=sinBAD\sin\angle ADT=\sin(\pi-\alpha-\gamma)=\sin(\alpha+\gamma)\leq\sin(\alpha)=\sin\angle BAD. It implies that α+γ>π/2\alpha+\gamma>\pi/2 and π(α+γ)α\pi-(\alpha+\gamma)\leq\alpha. Hence, we get 2απγπ(π/2β)=π/2+β2\alpha\geq\pi-\gamma\geq\pi-(\pi/2-\beta)=\pi/2+\beta and

αβ/2+π/4.\alpha\geq\beta/2+\pi/4. (8)

Let HH^{\prime} be the midpoint of [A,B][A,B]. Since triangles THHTH^{\prime}H and TEDTED are similar, then we have d(T,H)d(E,T)=d(H,H)d(E,D)=sin(β)\frac{d(T,H^{\prime})}{d(E,T)}=\frac{d(H,H^{\prime})}{d(E,D)}=\sin(\beta). Hence d(T,H)=sin(β)cot(γ)d(T,H^{\prime})=\sin(\beta)\cot(\gamma). Further on,

d(E,H)=d(T,E)d(T,H)=cot(γ)sin(β)cot(γ)=(1sin(β))cot(γ),d(E,H^{\prime})=d(T,E)-d(T,H^{\prime})=\cot(\gamma)-\sin(\beta)\cot(\gamma)=\bigl{(}1-\sin(\beta)\bigr{)}\cot(\gamma),

and

d(E,A)=d(A,H)d(E,H)=cos(β)(1sin(β))cot(γ).d(E,A)=d(A,H^{\prime})-d(E,H^{\prime})=\cos(\beta)-\bigl{(}1-\sin(\beta)\bigr{)}\cot(\gamma).

Moreover, we get cot(α)=d(E,A)d(E,D)=cos(β)(1sin(β))cot(γ)\cot(\alpha)=\frac{d(E,A)}{d(E,D)}=\cos(\beta)-\bigl{(}1-\sin(\beta)\bigr{)}\cot(\gamma), which implies

γ=arccot(cos(β)cot(α)1sin(β)).\gamma=\mathop{\rm arccot}\nolimits\left(\frac{\cos(\beta)-\cot(\alpha)}{1-\sin(\beta)}\right). (9)

From the triangle ABGABG we have

d(A,B)sin(AGB)=d(A,G)sin(ABG)=d(B,G)sin(BAG)=1sin(α)=d(A,D)\frac{d(A,B)}{\sin(\angle AGB)}=\frac{d(A,G)}{\sin(\angle ABG)}=\frac{d(B,G)}{\sin(\angle BAG)}=\frac{1}{\sin(\alpha)}=d(A,D)

and, consequently, 2cos(β)sin(α)=sin(AGB)12\cos(\beta)\sin(\alpha)=\sin(\angle AGB)\leq 1 and

d(A,G)sin(α)=sin(ABG)=sin(α+arcsin(2sin(α)cos(β))).d(A,G)\cdot\sin(\alpha)=\sin(\angle ABG)=\sin\bigl{(}\alpha+\arcsin(2\sin(\alpha)\cos(\beta))\bigr{)}.

Then we get

βarccos(12sin(α)),\beta\geq\arccos\left(\frac{1}{2\sin(\alpha)}\right), (10)
d(G,D)=d(A,D)d(A,G)=(1sin(α+arcsin(2sin(α)cos(β))))(sin(α))1.d(G,D)=d(A,D)-d(A,G)=\Bigl{(}1-\sin\bigl{(}\alpha+\arcsin(2\sin(\alpha)\cos(\beta))\bigr{)}\Bigr{)}\cdot\bigl{(}\sin(\alpha)\bigr{)}^{-1}.

Let us consider θ:=GCD\theta:=\angle GCD and p:=1sin(α+arcsin(2sin(α)cos(β)))p:=1-\sin\bigl{(}\alpha+\arcsin(2\sin(\alpha)\cos(\beta))\bigr{)}. It is clear that CGD=π(παγ)θ=α+γθ\angle CGD=\pi-(\pi-\alpha-\gamma)-\theta=\alpha+\gamma-\theta. From the triangle DCGDCG we get equalities

d(G,D)sin(θ)=d(D,C)sin(α+γθ)=d(G,C)sin(GDC)=1sin(α+γ)\frac{d(G,D)}{\sin(\theta)}=\frac{d(D,C)}{\sin(\alpha+\gamma-\theta)}=\frac{d(G,C)}{\sin(\angle GDC)}=\frac{1}{\sin(\alpha+\gamma)}

imply

sin(θ)=sin(α+γ)d(G,D)=sin(α+γ)sin(α)pandd(D,C)=sin(α+γθ)sin(α+γ).\sin(\theta)=\sin(\alpha+\gamma)\cdot d(G,D)=\frac{\sin(\alpha+\gamma)}{\sin(\alpha)}\cdot p\quad\mbox{and}\quad d(D,C)=\frac{\sin(\alpha+\gamma-\theta)}{\sin(\alpha+\gamma)}\,.

It is clear that BGC=πAGBCGD=παγ+θarcsin(2sin(α)cos(β))\angle BGC=\pi-\angle AGB-\angle CGD=\pi-\alpha-\gamma+\theta-\arcsin(2\sin(\alpha)\cos(\beta)). This implies

d(B,C)=2sin(BGC2)=2cos(α+γθ+arcsin(2sin(α)cos(β))2).d(B,C)=2\sin\left(\frac{\angle BGC}{2}\right)=2\cos\left(\frac{\alpha+\gamma-\theta+\arcsin(2\sin(\alpha)\cos(\beta))}{2}\right).

Therefore, we get the following expression for the perimeter of the quadrilateral ABCDABCD:

L(bd(ABCD))=d(A,B)+d(A,D)+d(D,C)+d(B,C)\displaystyle L\bigl{(}\operatorname{bd}(ABCD)\bigr{)}=d(A,B)+d(A,D)+d(D,C)+d(B,C)
=2cos(β)+1sin(α)+sin(α+γθ)sin(α+γ)+2cos(α+γθ+arcsin(2sin(α)cos(β))2).\displaystyle=2\cos(\beta)+\frac{1}{\sin(\alpha)}+\frac{\sin(\alpha+\gamma-\theta)}{\sin(\alpha+\gamma)}+2\cos\left(\frac{\alpha+\gamma-\theta+\arcsin(2\sin(\alpha)\cos(\beta))}{2}\right).

We can explicitly express γ\gamma and θ\theta in terms of α\alpha and β\beta from (9) and the equality

sin(θ)\displaystyle\sin(\theta) =\displaystyle= sin(α+γ)sin(α)p=sin(α+γ)sin(α)(1sin(α+arcsin(2sin(α)cos(β)))).\displaystyle\frac{\sin(\alpha+\gamma)}{\sin(\alpha)}\cdot p=\frac{\sin(\alpha+\gamma)}{\sin(\alpha)}\Bigl{(}1-\sin\bigl{(}\alpha+\arcsin(2\sin(\alpha)\cos(\beta))\bigr{)}\Bigr{)}.

Now we going to obtain some estimation on possible values of α\alpha and β\beta. Note that

cot(α)\displaystyle\cot(\alpha) =cos(β)(1sin(β))cot(γ)cos(β)(1sin(β))tan(β)=1sin(β)cos(β)\displaystyle=\cos(\beta)-\bigl{(}1-\sin(\beta)\bigr{)}\cot(\gamma)\leq\cos(\beta)-\bigl{(}1-\sin(\beta)\bigr{)}\tan(\beta)=\frac{1-\sin(\beta)}{\cos(\beta)}

due to cot(γ)cot(π/2β)=tan(β)\cot(\gamma)\geq\cot(\pi/2-\beta)=\tan(\beta). Note also that cot2(α)=1sin2(α)14cos2(β)1\cot^{2}(\alpha)=\frac{1}{\sin^{2}(\alpha)}-1\geq 4\cos^{2}(\beta)-1 (due to 2sin(α)cos(β)12\sin(\alpha)\cos(\beta)\leq 1), therefore we have (1sin(β))2cos2(β)(4cos2(β)1)(1-\sin(\beta))^{2}\geq\cos^{2}(\beta)\bigl{(}4\cos^{2}(\beta)-1\bigr{)} or, dividing by 1sin(β)>01-\sin(\beta)>0,

1+2sin(β)2sin2(β)2sin3(β)0.1+2\sin(\beta)-2\sin^{2}(\beta)-2\sin^{3}(\beta)\leq 0.

Hence, sin(β)y0=0.8546376797\sin(\beta)\geq y_{0}=0.8546376797... and βarcsin(y0)=1.024852629\beta\geq\arcsin(y_{0})=1.024852629..., where y0y_{0} is a unique root of the polynomial 2y3+2y22y12y^{3}+2y^{2}-2y-1 on [0,1][0,1]. Therefore, we get that α[α0,π/2]\alpha\in[\alpha_{0},\pi/2] and β[β0,π/2]\beta\in[\beta_{0},\pi/2], where α0=arcsin(y0)/2+π/4=1.29782448\alpha_{0}=\arcsin(y_{0})/2+\pi/4=1.29782448..., β0=arcsin(y0)=1.024852629\beta_{0}=\arcsin(y_{0})=1.024852629....

Now we will find additional important restrictions on the values of α\alpha, β\beta. We are going to prove that any possible pair (α,β)(\alpha,\beta) should lie in the following set:

Ω={(α,β)|π/2αβ/2+π/4,π/3βarccos(12sin(α))}.\Omega=\left\{(\alpha,\beta)\,\,\left|\,\,\pi/2\geq\alpha\geq\beta/2+\pi/4,\,\,\pi/3\geq\beta\geq\arccos\left(\frac{1}{2\sin(\alpha)}\right)\right.\right\}. (11)

It is easy to check that Ω\Omega is bounded by the straight lines L1={(α,β)|α=β/2+π/4}L_{1}=\left\{(\alpha,\beta)\,|\,\alpha=\beta/2+\pi/4\right\}, β=π/3\beta=\pi/3, and by the curve

L2={(α,β)| 2sin(α)cos(β)=1,π/2αβarcsin(y0)}.L_{2}=\left\{(\alpha,\beta)\,|\,2\sin(\alpha)\cos(\beta)=1,\,\,\pi/2\geq\alpha\geq\beta\geq\arcsin(y_{0})\right\}.

The above argument implies that the point M:=(α0,β0)M:=(\alpha_{0},\beta_{0}) lies in the intersection of L1L_{1} and L2L_{2}. It is easy to check also that L1L2={M}L_{1}\cap L_{2}=\{M\}.

Recall that we have obtained the inequalities αβ/2+π/4\alpha\geq\beta/2+\pi/4 and 2sin(α)cos(β)12\sin(\alpha)\cos(\beta)\leq 1. Hence it suffices to prove that βπ/3\beta\leq\pi/3. In any case, all possible pairs (α,β)(\alpha,\beta) lie in the set

Π={(α,β)|π/2αβ/2+π/4,π/2βarccos(12sin(α))}.\Pi=\left\{(\alpha,\beta)\,\,\left|\,\,\pi/2\geq\alpha\geq\beta/2+\pi/4,\,\,\pi/2\geq\beta\geq\arccos\left(\frac{1}{2\sin(\alpha)}\right)\right.\right\}. (12)

Note that the straight line L1L_{1} passes through the points (π/2,π/2)(\pi/2,\pi/2), hence we can omit the restriction βπ/2\beta\leq\pi/2 from the formal point of view.

Let us consider the point CC^{\prime} on [C,T][C,T] such that d(E,C)=1d(E,C^{\prime})=1 (recall that d(E,C)1d(E,C)\leq 1 and γ<π/4\gamma<\pi/4, hence, d(E,T)>d(E,D)=1d(E,T)>d(E,D)=1). Note that d(E,C)d(E,C)d(E,C)\leq d(E,C^{\prime}) holds if and only if d(D,C)d(D,C)d(D,C)\leq d(D,C^{\prime}) or, equivalently, d(G,C)1d(G,C^{\prime})\geq 1. We can rewrite the latter inequality using the law of cosines the triangle GDCGDC^{\prime}. It is clear that d(D,C)=2sin(γ)d(D,C^{\prime})=2\sin(\gamma) (recall that d(E,C)=d(E,D)=1d(E,C^{\prime})=d(E,D)=1 and EDC=π/2γ\angle EDC^{\prime}=\pi/2-\gamma). Therefore,

d(D,C)2+2d(G,D)d(D,C)cos(α+γ)+d(G,D)2=d(G,C)21,d(D,C^{\prime})^{2}+2d(G,D)d(D,C^{\prime})\cos(\alpha+\gamma)+d(G,D)^{2}=d(G,C^{\prime})^{2}\geq 1,

which can be rewritten (d(G,D)sin(α)=p=1sin(α+arcsin(2sin(α)cos(β))))\Bigl{(}d(G,D)\cdot\sin(\alpha)=p=1-\sin\bigl{(}\alpha+\arcsin(2\sin(\alpha)\cos(\beta))\bigr{)}\Bigr{)} as

4sin2(γ)+4sin(γ)cos(α+γ)sin(α)p+p2sin2(α)1.4\sin^{2}(\gamma)+\frac{4\sin(\gamma)\cos(\alpha+\gamma)}{\sin(\alpha)}\,p+\frac{p^{2}}{\sin^{2}(\alpha)}\geq 1.

Now, we define the function

Refer to caption
Figure 13. The curvilinear triangle MNR.
F(α,β):=4sin2(γ)+4sin(γ)cos(α+γ)sin(α)p+p2sin2(α)1,F(\alpha,\beta):=4\sin^{2}(\gamma)+\frac{4\sin(\gamma)\cos(\alpha+\gamma)}{\sin(\alpha)}\,p+\frac{p^{2}}{\sin^{2}(\alpha)}-1, (13)

where

p=1sin(α+arcsin(2sin(α)cos(β))),γ=arccot(cos(β)cot(α)1sin(β)),p=1-\sin\bigl{(}\alpha+\arcsin(2\sin(\alpha)\cos(\beta))\bigr{)},\quad\gamma=\mathop{\rm arccot}\nolimits\left(\frac{\cos(\beta)-\cot(\alpha)}{1-\sin(\beta)}\right),

and the set

L3={(α,β)Π|F(α,β)=0}.L_{3}=\left\{(\alpha,\beta)\in\Pi\,|\,F(\alpha,\beta)=0\right\}.

Now we will find the intersection point N=(α1,β1)N=(\alpha_{1},\beta_{1}) of the curve L1L_{1} and the set L3L_{3}. Substituting α=β/2+π/4\alpha=\beta/2+\pi/4 into (13)\eqref{eq.ec}, we easily get that β1=π/3\beta_{1}=\pi/3 and, consequently, α1=π/6+π/4=5π/12\alpha_{1}=\pi/6+\pi/4=5\pi/12.

Now we will find the intersection of the curve L2L_{2} and the set L3L_{3}. Substituting cos(β)=12sin(α)\cos(\beta)=\frac{1}{2\sin(\alpha)} and sin(β)=4sin2(α)12sin(α)\sin(\beta)=\frac{\sqrt{4\sin^{2}(\alpha)-1}}{2\sin(\alpha)} into (13)\eqref{eq.ec} we get

sin(α)34cos2(α)(2cos(α)+3)+4cos3(α)+8cos2(α)5cos(α)5(cos(α)cos2(α))1sin2(α)(sin(α)34cos2(α)+cos(α)2+cos(α)2)=0.\frac{\sin(\alpha)\sqrt{3-4\cos^{2}(\alpha)}\Bigl{(}2\cos(\alpha)+3\Bigr{)}+4\cos^{3}(\alpha)+8\cos^{2}(\alpha)-5\cos(\alpha)-5}{\Bigl{(}\cos(\alpha)-\cos^{2}(\alpha)\Bigr{)}^{-1}\sin^{2}(\alpha)\Bigl{(}\sin(\alpha)\sqrt{3-4\cos^{2}(\alpha)}+\cos(\alpha)^{2}+\cos(\alpha)-2\Bigr{)}}=0.
Refer to caption
Refer to caption
Figure 14. The perimeter LL of ABCDABCD over MNR.

Hence, either α=π/2\alpha=\pi/2 or

2(12cos2(α))(4cos3(α)+4cos2(α)7cos(α)+1)=0.2\bigl{(}1-2\cos^{2}(\alpha)\bigr{)}\Bigl{(}4\cos^{3}(\alpha)+4\cos^{2}(\alpha)-7\cos(\alpha)+1\Bigr{)}=0.

By direct computations, we get that α=α2:=arccos(t)=1.4103331\alpha=\alpha_{2}:=\arccos(t^{\prime})=1.4103331..., where t=0.1597754t^{\prime}=0.1597754... is a unique root of the polynomial f(t)=4t3+4t27t+1=0f(t)=4t^{3}+4t^{2}-7t+1=0 on the interval (0,0.2)(0,0.2). Consequently, we obtain the intersection points Q=(α2,β2)Q=(\alpha_{2},\beta_{2}), where β2=arccos(12sin(α2))=1.039667597\beta_{2}=\arccos\left(\frac{1}{2\sin(\alpha_{2})}\right)=1.039667597..., and R=(π/2,π/3)R=(\pi/2,\pi/3).

If we consider h(α):=F(α,π/3)h(\alpha):=F(\alpha,\pi/3) for α[α1=5π/12,π/2]\alpha\in[\alpha_{1}=5\pi/12,\pi/2], then h(α1)=h(π/2)=0h(\alpha_{1})=h(\pi/2)=0 and h(α)<0h(\alpha)<0 for α(α1,π/2)\alpha\in(\alpha_{1},\pi/2). Let us suppose that there exist (α,β)Π(\alpha^{\prime},\beta^{\prime})\in\Pi such that F(α,β)0F(\alpha^{\prime},\beta^{\prime})\geq 0 and β>π/3\beta^{\prime}>\pi/3. Then, by the continuity, there exists (α′′,β′′)Π(\alpha^{\prime\prime},\beta^{\prime\prime})\in\Pi such that F(α′′,β′′)=0F(\alpha^{\prime\prime},\beta^{\prime\prime})=0 and β′′>π/3\beta^{\prime\prime}>\pi/3. Without loss of generality, we can fix such a point (α′′,β′′)(\alpha^{\prime\prime},\beta^{\prime\prime}) with the maximal possible value of β′′\beta^{\prime\prime}. Its clear that αF(α′′,β′′)=0\frac{\partial}{\partial\alpha}F(\alpha^{\prime\prime},\beta^{\prime\prime})=0. On the other hand, the system

F(α′′,β′′)=αF(α′′,β′′)=0F(\alpha^{\prime\prime},\beta^{\prime\prime})=\frac{\partial}{\partial\alpha}F(\alpha^{\prime\prime},\beta^{\prime\prime})=0 (14)

has no solution in Π\Pi with βπ/3\beta\geq\pi/3. Since we have αβ/2+π/4\alpha\geq\beta/2+\pi/4 by (8), hence, we need to check only (α,β)[5π/12,π/2]×[π/3,π/2](\alpha,\beta)\in[5\pi/12,\pi/2]\times[\pi/3,\pi/2]. By numerical calculations (one can use commands Maximize and Minimize for the Optimization package in Maple) we get that the maximal value of αF(α,β)\frac{\partial}{\partial\alpha}F(\alpha,\beta) for (α,β)[5π/12,π/2]×[11/10,π/2](\alpha,\beta)\in[5\pi/12,\pi/2]\times[11/10,\pi/2] is 1.09119149<0-1.09119149...<0. On the other hand, the minimal value of F(α,β)F(\alpha,\beta) for (α,β)[5π/12,π/2]×[π/3,6/5](\alpha,\beta)\in[5\pi/12,\pi/2]\times[\pi/3,6/5] is 0.79177743>00.79177743...>0. Since 6/5>11/106/5>11/10, we obtain that system (14) has no solution for (α,β)[5π/12,π/2]×[π/3,π/2](\alpha,\beta)\in[5\pi/12,\pi/2]\times[\pi/3,\pi/2].

Therefore, for all possible pair (α,β)Π(\alpha,\beta)\in\Pi we have βπ/3\beta\leq\pi/3. Thus we have constructed the (curvilinear) triangle

MNR={(α,β)|αβ/2+π/4,π/3βarccos(12sin(α))},MNR=\left\{(\alpha,\beta)\,\,\left|\,\,\alpha\geq\beta/2+\pi/4,\,\,\pi/3\geq\beta\geq\arccos\left(\frac{1}{2\sin(\alpha)}\right)\right.\right\}, (15)

where NRNR is the straight line β=π/3\beta=\pi/3 (see Fig. 13).

By numerical calculations we get also that the minimum value of the value β\beta on the set L3ΠL_{3}\cap\Pi is β3=1.034584325\beta_{3}=1.034584325..., that corresponds to α3=1.34546261\alpha_{3}=1.34546261... (see the point P=(α3,β3)P=(\alpha_{3},\beta_{3}) at Fig. 13, this point gives a unique solution of (14) in Π\Pi).

Now, we consider only pair (α,β)(\alpha,\beta) from the curvilinear triangle MNRMNR, since this inclusion follows from the equality δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD))=1.

The results of numerical calculations show that the perimeter L(bd(ABCD))L(\operatorname{bd}(ABCD)) (on the curvilinear triangle MNRMNR) achieves its minimal value provided that AGB=AHD=π/2\angle AGB=\angle AHD=\pi/2, see Fig. 14. This minimal value is L(bd(ABCD))=3.503591801L(\operatorname{bd}(ABCD))=3.503591801.... Hence, the quadrilateral ABCDABCD is not extremal.

Remark 7.

It should be noted that in Сase 3.3, in contrast to Сase 3.2, there are real quadrilaterals with all the necessary properties, therefore, a lower estimate for the value of the perimeter is required.

Remark 8.

In Case 3.3 we ended the discussion with a reference to numerical calculations. This is sufficient, since the minimum value of the perimeter in this case is separated from the hypothetical minimum value (obtained for magic kites) by a distance greater than 1/101/10. It is clear that instead of referring to numerical calculations, one can carry out perimeter estimates (with some margin), using only symbolic calculations (the function being minimized is analytic and has good properties). But this will take additional space in the paper, although it is in fact some technical point. The same remark is valid for the following Case 3.4.

7.4. Case 3.4

Without loss of generality, we may suppose that Gmin={E,G,F}G_{\min}=\{E,G,F\}, where EE is an interior point of [A,B][A,B], GG is an interior point of [B,C][B,C], FF is an interior point of [A,D][A,D], and δ(bd(ABCD))=d(E,D)=d(E,C)=d(G,A)=d(G,D)=d(F,B)=d(F,C)=1\delta(\operatorname{bd}(ABCD))=d(E,D)=d(E,C)=d(G,A)=d(G,D)=d(F,B)=d(F,C)=1 (see Fig. 15). Moreover, AGBπ/2\angle AGB\leq\pi/2, AFBπ/2\angle AFB\leq\pi/2 and AEDπ/2\angle AED\leq\pi/2 by Proposition 6.

Refer to caption
Figure 15. Case 3.4.

Let us consider a slightly more general case in a suitable system of Cartesian coordinates. We take the coordinates as follows: E=(0,0)E=(0,0), C=(cos(α),sin(α))C=(\cos(\alpha),\sin(\alpha)), D=(cos(α),sin(α))D=(-\cos(\alpha),\sin(\alpha)), where α(0,π/2)\alpha\in(0,\pi/2). Let kk be a number such that the equation of the straight line ABAB is y=kxy=kx. Without loss of generality, we may suppose that k0k\geq 0. Then A=(x1,kx1)A=(x_{1},kx_{1}), B=(x2,kx2)B=(x_{2},kx_{2}) and x1<0<x2x_{1}<0<x_{2}.

If απ/4\alpha\leq\pi/4, then DECπ/2\angle DEC\geq\pi/2 and we obtain the following simple estimate for the perimeter: L(bd(DEC))2+2L(\operatorname{bd}(DEC))\geq 2+\sqrt{2}. Hence, we have L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}, that is impossible for an extremal quadrilateral. Thus, απ/4\alpha\geq\pi/4.

Since DEBπ/2\angle DEB\geq\pi/2 then (ED,EB)0(\overrightarrow{ED},\overrightarrow{EB})\leq 0. It implies cos(α)x2+sin(α)kx20-\cos(\alpha)x_{2}+\sin(\alpha)kx_{2}\leq 0 or, equivalently, kcos(α)sin(α)=cot(α)k\leq\frac{\cos(\alpha)}{\sin(\alpha)}=\cot(\alpha). Therefore, 0kcot(α)0\leq k\leq\cot(\alpha).

It is easy to see that

L(bd(ABCD))=d(A,B)+d(B,C)+d(C,D)+d(D,A)=(x2x1)1+k2+2cos(α)L(\operatorname{bd}(ABCD))=d(A,B)+d(B,C)+d(C,D)+d(D,A)=(x_{2}-x_{1})\sqrt{1+k^{2}}+2\cos(\alpha)
+(x2cos(α))2+(kx2sin(α))2+(x1+cos(α))2+(kx1sin(α))2.+\sqrt{(x_{2}-\cos(\alpha))^{2}+(kx_{2}-\sin(\alpha))^{2}}+\sqrt{(x_{1}+\cos(\alpha))^{2}+(kx_{1}-\sin(\alpha))^{2}}.

In particular, L(bd(ABCD))x2x1=|x2x1|L(\operatorname{bd}(ABCD))\geq x_{2}-x_{1}=|x_{2}-x_{1}|. Since GG is a point of [B,C][B,C] and FF is a point of [A,D][A,D], there are t[0,1]t\in[0,1] and s[0,1]s\in[0,1] such that

F\displaystyle F =\displaystyle= (tx1(1t)cos(α),tkx1+(1t)sin(α)),\displaystyle\bigl{(}tx_{1}-(1-t)\cos(\alpha),\,tkx_{1}+(1-t)\sin(\alpha)\bigr{)},
G\displaystyle G =\displaystyle= (sx2+(1s)cos(α),skx2+(1s)sin(α)).\displaystyle\bigl{(}sx_{2}+(1-s)\cos(\alpha),\,skx_{2}+(1-s)\sin(\alpha)\bigr{)}.

Let FF^{\prime} be the midpoint of [B,C][B,C] and GG^{\prime} be the midpoint of [A,D][A,D]. Then

G=12(x1cos(α),kx1+sin(α)),F=12(x2+cos(α),kx2+sin(α)).G^{\prime}=\frac{1}{2}\bigl{(}x_{1}-\cos(\alpha),kx_{1}+\sin(\alpha)\bigr{)},\quad F^{\prime}=\frac{1}{2}\bigl{(}x_{2}+\cos(\alpha),kx_{2}+\sin(\alpha)\bigr{)}.

Since the straight line GGG^{\prime}G (FFF^{\prime}F) is orthogonal to the straight line ADAD (respectively, BCBC) then

(GG,AD)=0and(FF,BC)=0.(\overrightarrow{G^{\prime}G},\overrightarrow{AD})=0\quad\text{and}\quad(\overrightarrow{F^{\prime}F},\overrightarrow{BC})=0.

Solving these linear equations with respect to ss and tt, we get some explicit expressions

s=g(x1,x2,k,α),t=f(x1,x2,k,α).s=g(x_{1},x_{2},k,\alpha),\quad t=f(x_{1},x_{2},k,\alpha).

Since d(G,D)=d(G,A)=1d(G,D)=d(G,A)=1 and d(F,C)=d(F,B)=1d(F,C)=d(F,B)=1, we have the equations

d(G,D)=1,d(F,C)=1,d(G,D)=1,\quad d(F,C)=1,

with respect to x1,x2,k,αx_{1},x_{2},k,\alpha. Thus, here we have four variables and two constraints, that is, roughly speaking, two degrees of freedom. Recall also that x1<0<x2x_{1}<0<x_{2}, α[π/4,π/2)\alpha\in[\pi/4,\pi/2), 0kcot(α)0\leq k\leq\cot(\alpha), moreover, s=g(x1,x2,k,α),t=f(x1,x2,k,α)[0,1]s=g(x_{1},x_{2},k,\alpha),t=f(x_{1},x_{2},k,\alpha)\in[0,1], and we can assume that |x2x1|2+2|x_{2}-x_{1}|\leq 2+\sqrt{2} (otherwise the perimeter of ABCDABCD is at least 2+22+\sqrt{2}, and ABCDABCD is not extremal).

The results of numerical calculations show that the perimeter L(bd(ABCD))L\bigl{(}\operatorname{bd}(ABCD)\bigr{)} for the quadrilaterals under consideration reaches its minimal value exactly for AED=AFB=π/2\angle AED=\angle AFB=\pi/2. This minimal value is L(bd(ABCD))=3.510690988L(\operatorname{bd}(ABCD))=3.510690988.... Hence, the quadrilateral ABCDABCD is not extremal.

8. Case 4

Let us suppose that Gmin=4\|G_{\min}\|=4 and Gmin={E,F,G,H}G_{\min}=\{E,F,G,H\}. Without loss of generality we may suppose that E[A,D]E\in[A,D], F[A,B]F\in[A,B], G[B,C]G\in[B,C] and H[C,D]H\in[C,D]. In all subsaces of this case we have only one degree of freedom.

Recall that a self Chebyshev center xx for bd(ABCD)\operatorname{bd}(ABCD) is simple if (x)=1\|{\mathcal{F}}(x)\|=1 and non-simple if (x)2\|{\mathcal{F}}(x)\|\geq 2 (see (3)).

Refer to caption

a)

Refer to caption

b)

Figure 16. a) Two straight lines; b) A ‘‘thin’’ quadrilateral.

Now, we are going to study a special case that we will call Case 4.0.

8.1. Case 4.0.

We consider a quadrilateral ABCDABCD with δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD))=1 and Gmin=4\|G_{\min}\|=4, such that there are two opposite sides of ABCDABCD with non-simple self Chebyshev centers of bd(ABCD)\operatorname{bd}(ABCD). We will prove that such a quadrilateral can not be extremal. In other words, the following proposition holds.

Proposition 12.

Suppose that a quadrilateral ABCDABCD with δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD))=1 is extremal and Gmin=4\|G_{\min}\|=4. Then there are no two opposite sides of ABCDABCD such that each of them has a non-simple self Chebyshev center of bd(ABCD)\operatorname{bd}(ABCD).

To prove this result, we need some lemmas.

Lemma 6.

Let l1,l2l_{1},l_{2} are straight lines with points A1l1A_{1}\in l_{1}, A2l2A_{2}\in l_{2}, A1l2A^{\prime}_{1}\in l_{2}, A2l1A^{\prime}_{2}\in l_{1} that A1A1l2A_{1}A^{\prime}_{1}\perp l_{2}, A2A2l1A_{2}A^{\prime}_{2}\perp l_{1} and d(A1,A1)=d(A2,A2)d(A_{1},A^{\prime}_{1})=d(A_{2},A^{\prime}_{2}) (see the left panel of Fig. 16). If [A1,A1][A2,A2]=[A_{1},A^{\prime}_{1}]\cap[A_{2},A^{\prime}_{2}]=\emptyset then A1A1A2A2A_{1}A^{\prime}_{1}A_{2}A^{\prime}_{2} is rectangle, otherwise A1A2A1A2A_{1}A_{2}A^{\prime}_{1}A^{\prime}_{2} is isosceles trapezoid.

Proof. The triangle A1A1A2A_{1}A^{\prime}_{1}A_{2} is congruent to triangle A2A2A1A_{2}A^{\prime}_{2}A_{1} in the common hypotenuse ([A1,A2][A_{1},A_{2}]) and legs (d(A1,A1)=d(A2,A2))(d(A_{1},A^{\prime}_{1})=d(A_{2},A^{\prime}_{2})). Hence A2A1A2=A1A2A1\angle A_{2}A_{1}A^{\prime}_{2}=\angle A_{1}A_{2}A^{\prime}_{1}. It implies that if [A1,A1][A2,A2]=[A_{1},A^{\prime}_{1}]\cap[A_{2},A^{\prime}_{2}]=\emptyset then A1A1A2A2A_{1}A^{\prime}_{1}A_{2}A^{\prime}_{2} is rectangle, otherwise A1A2A1A2A_{1}A_{2}A^{\prime}_{1}A^{\prime}_{2} is isosceles trapezoid.   

Lemma 7.

Let ABCDABCD be a quadrilateral with δ(bd(ABCD))=1\delta(\operatorname{bd}(ABCD))=1 for the self Chebyshev radius of its boundary. If d(A,B)12d(A,B)\leq\frac{1}{\sqrt{2}} and d(C,D)12d(C,D)\leq\frac{1}{\sqrt{2}} then either L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2} or Gmin[A,D]=G_{\min}\cap[A,D]=\emptyset and Gmin[B,C]=G_{\min}\cap[B,C]=\emptyset.

Proof. Suppose that EGmin[A,D]E\in G_{\min}\cap[A,D]. If (E)=1\|{\mathcal{F}}(E)\|=1 then (E)={B}{\mathcal{F}}(E)=\{B\} or (E)={C}{\mathcal{F}}(E)=\{C\}. Hence d(B,E)=1d(B,E)=1 and BE[A,D]BE\perp[A,D] or d(C,E)=1d(C,E)=1 and CE[A,D]CE\perp[A,D]. But this is not possible because 12d(A,B)d(B,E)=1\frac{1}{\sqrt{2}}\geq d(A,B)\geq d(B,E)=1 or 12d(C,D)d(C,E)=1\frac{1}{\sqrt{2}}\geq d(C,D)\geq d(C,E)=1. Thus, (E)=2\|{\mathcal{F}}(E)\|=2 and (E)={B,C}{\mathcal{F}}(E)=\{B,C\} (see the right panel Fig. 16).

Let us consider the perpendiculars from the points A,E,DA,E,D to the straight line BCBC. Denote by A,E,DBCA^{\prime},E^{\prime},D^{\prime}\in BC the foots of these perpendiculars, respectively. Since d(A,A)d(A,B)12d(A,A^{\prime})\leq d(A,B)\leq\frac{1}{\sqrt{2}} and d(D,D)d(D,C)12d(D,D^{\prime})\leq d(D,C)\leq\frac{1}{\sqrt{2}} then d(E,E)max{d(A,A),d(D,D)}12d(E,E^{\prime})\leq\max\{d(A,A^{\prime}),d(D,D^{\prime})\}\leq\frac{1}{\sqrt{2}}. It implies d(B,E)=d(C,E)=1d2(E,E)12d(B,E^{\prime})=d(C,E^{\prime})=\sqrt{1-d^{2}(E,E^{\prime})}\geq\frac{1}{\sqrt{2}}. Therefore, L(bd(ABCD))>L(bd(BEC))2+2L(\operatorname{bd}(ABCD))>L(\operatorname{bd}(BEC))\geq 2+\sqrt{2}.

The same arguments show that Gmin[B,C]G_{\min}\cap[B,C]\neq\emptyset also implies L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}.   

The assertion of the following lemma is well known and belongs to folklore. At one time it was proposed as an Olympiad problem in mathematics (see [12, 1997 Olympiad, Level C, Problem 2]).

Lemma 8.

Among quadrilaterals ABCDABCD with given diagonal lengths and the angle θ\theta between them, a parallelogram has the smallest perimeter.

Refer to caption

a)

Refer to caption

b)

Figure 17. a) The proof of Lemma 8; b) The proof of Proposition 12.

Proof. We present the proof for completeness. Let us translate the quadrilateral ABCDABCD by vector ACAC (see the left panel Fig. 17). We get the quadrilateral ABCDA^{\prime}B^{\prime}C^{\prime}D^{\prime}, where A=CA^{\prime}=C and the quadrilateral BBDDBB^{\prime}D^{\prime}D is a parallelogram.

Let the points A0,B0,C0A_{0},B_{0},C_{0} and D0D_{0} are midpoints of [B,D],[B,B],[BD][B,D],[B,B^{\prime}],[B^{\prime}D^{\prime}] and [D,D][D^{\prime},D], respectively. It is easy to see that the quadrilateral A0,B0,C0,D0A_{0},B_{0},C_{0},D_{0} is a parallelogram. Moreover, the sum of the lengths of the diagonals and the angle between them of which are equal to the sum of the lengths of the diagonals and the angle between them of the quadrilateral ABCDABCD.

By the triangle inequality d(B,C)+d(C,D)d(B,D)d(B,C)+d(C,D^{\prime})\geq d(B,D^{\prime}) and d(B,C)+d(C,D)d(B,D)d(B^{\prime},C)+d(C,D)\geq d(B^{\prime},D). Adding up these inequalities we get L(bd(ABCD))d(B,D)+d(B,D)=L(bd(A0B0C0D0))L(\operatorname{bd}(ABCD))\geq d(B,D^{\prime})+d(B^{\prime},D)=L(\operatorname{bd}(A_{0}B_{0}C_{0}D_{0})) what was required to be shown.   

Lemma 8 obviously implies the following result.

Corollary 6.

We have L(bd(ABCD))22sin(θ/2+π/4)L\bigl{(}\operatorname{bd}(ABCD)\bigr{)}\geq 2\sqrt{2}\cdot\sin(\theta/2+\pi/4) for any quadrilateral ABCDABCD with given diagonal lengths d(A,C)=d(B,D)=1d(A,C)=d(B,D)=1 and the angle θ\theta between them.

Proof of Proposition 12. Let us suppose the contrary. Without loss of generality, we may suppose that there are at least two non-simple self Chebyshev centers FF and EE, where FF is an interior point of [A,B][A,B], EE is an interior point of [C,D][C,D], while δ(bd(ABCD))=d(F,D)=d(F,C)=d(E,A)=d(E,B)=1\delta(\operatorname{bd}(ABCD))=d(F,D)=d(F,C)=d(E,A)=d(E,B)=1 (see the right panel Fig. 17).

By Corollary 6 we have

L(bd(BCEF))2f(θ1)andL(bd(ADEF))2f(θ2),L(\operatorname{bd}(BCEF))\geq 2f(\theta_{1})\quad\mbox{and}\quad L(\operatorname{bd}(ADEF))\geq 2f(\theta_{2}),

where f(θ):=cos(θ/2)+sin(θ/2)f(\theta):=\cos\bigl{(}\theta/2\bigr{)}+\sin\bigl{(}\theta/2\bigr{)}. Therefore, we get

L(bd(ABCD))=L(bd(BCEF))+L(bd(ADEF))d(E,F)2(f(θ1)+f(θ2))1.L(\operatorname{bd}(ABCD))=L(\operatorname{bd}(BCEF))+L(\operatorname{bd}(ADEF))-d(E,F)\geq 2(f(\theta_{1})+f(\theta_{2}))-1.

Let us consider φ1:=BEA\varphi_{1}:=\angle BEA and φ2:=CFD\varphi_{2}:=\angle CFD. It is easy to see that θ1+θ2=φ1+φ2\theta_{1}+\theta_{2}=\varphi_{1}+\varphi_{2}. Moreover, φ1/2=arcsin(d(A,B)/2)\varphi_{1}/2=\arcsin(d(A,B)/2) and φ2/2=arcsin(d(C,D)/2)\varphi_{2}/2=\arcsin(d(C,D)/2). Thus, we have

d(A,B)2+d(C,D)2=sin(φ1/2)+sin(φ2/2)φ1+φ22=θ1+θ22\frac{d(A,B)}{2}+\frac{d(C,D)}{2}=\sin(\varphi_{1}/2)+\sin(\varphi_{2}/2)\leq\frac{\varphi_{1}+\varphi_{2}}{2}=\frac{\theta_{1}+\theta_{2}}{2}

or d(A,B)+d(C,D)θ1+θ2d(A,B)+d(C,D)\leq\theta_{1}+\theta_{2}.

Suppose that d(A,B)+d(C,D)12d(A,B)+d(C,D)\geq\frac{1}{\sqrt{2}}. It implies θ1+θ212\theta_{1}+\theta_{2}\geq\frac{1}{\sqrt{2}}. Consider the function F(θ1,θ2):=f(θ1)+f(θ2)F(\theta_{1},\theta_{2}):=f(\theta_{1})+f(\theta_{2}) on the set

S:={(θ1,θ2)|  0θ1,θ2π2,θ1+θ212}.S:=\left\{(\theta_{1},\theta_{2})\,\left|\,\,0\leq\theta_{1},\theta_{2}\leq\frac{\pi}{2},\,\theta_{1}+\theta_{2}\geq\frac{1}{\sqrt{2}}\right.\right\}. (16)

Since f(θ)=2sin(θ/2+π/4)=12cos(θ/2+π/4)>0f^{\prime}(\theta)=\sqrt{2}\sin^{\prime}(\theta/2+\pi/4)=\frac{1}{\sqrt{2}}\cos(\theta/2+\pi/4)>0 for θ[0,π/2)\theta\in[0,\pi/2) then the function f(θ)f(\theta) is strictly increasing at a given interval. On the other hand f′′(θ)=12cos(θ/2+π/4)=122sin(θ/2+π/4)<0f^{\prime\prime}(\theta)=\frac{1}{\sqrt{2}}\cos^{\prime}(\theta/2+\pi/4)=-\frac{1}{2\sqrt{2}}\sin(\theta/2+\pi/4)<0 for θ[0,π/2]\theta\in[0,\pi/2]. Thus, the minimum of the function F(θ1,θ2)F(\theta_{1},\theta_{2}) is possible only at three points: (0,1/2)(0,1/\sqrt{2}), (1/2,0)(1/\sqrt{2},0) and (1/2,1/2)(1/\sqrt{2},1/\sqrt{2}). By direct computations we get

F(0,1/2)=F(1/2,0)=2.2843,F(1/2,1/2)=2.5687.F(0,1/\sqrt{2})=F(1/\sqrt{2},0)=2.2843...,\quad F(1/\sqrt{2},1/\sqrt{2})=2.5687....

Hence, L(bd(ABCD))2F(θ1,θ2)1=3.5686L(\operatorname{bd}(ABCD))\geq 2F(\theta_{1},\theta_{2})-1=3.5686... and the quadrilateral ABCDABCD is not extremal.

Therefore, d(A,B)+d(C,D)12d(A,B)+d(C,D)\leq\frac{1}{\sqrt{2}}, that implies d(A,B)12d(A,B)\leq\frac{1}{\sqrt{2}} and d(C,D)12d(C,D)\leq\frac{1}{\sqrt{2}}. By Lemma 7, we get L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}, hence, ABCDABCD is not extremal.   


According to Proposition 12, any extremal quadrilateral ABCDABCD with Gmin=4\|G_{\min}\|=4 has at least 22 simple self Chebyshev centers on some adjacent sides (otherwise there are a pair of opposite sides with non-simple centers, which is impossible due to the mentioned proposition). Fix a pair of such simple self Chebyshev centers, EE and FF.

There are three possible cases:

  • They have one and the same farthest vertex;

  • They have different farthest vertices that are adjacent;

  • They have different farthest vertices that are not adjacent.

We shall call this three possibilities as Cases 4.1, 4.2, and 4.3 respectively.

Refer to caption

a)

Refer to caption

b)

Figure 18. a) Case 4.1; b) Case 4.1a.

8.2. Case 4.1

Let us consider a quadrilateral ABCDABCD with δ(bd(ABCD))=d(A,H)=d(A,G)=1\delta(\operatorname{bd}(ABCD))=d(A,H)=d(A,G)=1 and AH[C,D]AH\perp[C,D], AG[B,C]AG\perp[B,C] (see the left panel Fig. 18).

If BADπ/2\angle BAD\geq\pi/2, then L(bd(ABD))2+2L(\operatorname{bd}(ABD))\geq 2+\sqrt{2}. Hence, we have L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}, that is impossible for an extremal quadrilateral. Thus, BAD<π/2\angle BAD<\pi/2.

If d(C,F)=1d(C,F)=1 and CF[A,B]CF\perp[A,B] then HAFCHAFC is rectangle and d(H,F)>d(C,F)=1d(H,F)>d(C,F)=1. Therefore, HH and FF are not self Chebyshev centers. Hence CFCF is not orthogonal to [A,B][A,B] as well as CECE is not orthogonal to [A,D][A,D].

If EE is a simple and FF is not simple (or vice versa, FF is a simple and EE is not simple) self Chebyshev centers respectively, then the case is impossible (see Remark 6 for Case 3.2).

Let us consider the case when EE and FF are not simple self Chebyshev centers, i. e. δ(bd(ABCD))=d(D,F)=d(C,F)=d(C,E)=d(B,E)=d(H,A)=d(G,A)=1\delta(\operatorname{bd}(ABCD))=d(D,F)=d(C,F)=d(C,E)=d(B,E)=d(H,A)=d(G,A)=1 (see the right panel of Fig. 18). Moreover, DFAπ/2\angle DFA\leq\pi/2 and BEAπ/2\angle BEA\leq\pi/2 by Proposition 6. We show that this case is also impossible.

We put α:=DAH\alpha:=\angle DAH, β:=BAG\beta:=\angle BAG, and γ:=HAC=GAC\gamma:=\angle HAC=\angle GAC. It is clear that α<γ\alpha<\gamma and β<γ\beta<\gamma. From the triangle HABHAB we have HAB=β+2γ<π/3\angle HAB=\beta+2\gamma<\pi/3. Similarly, GAD=α+2γ<π/3\angle GAD=\alpha+2\gamma<\pi/3. It implies α+γ<π/4\alpha+\gamma<\pi/4.

From tan(α+γ)=tan(α)+tan(γ)1tan(α)tan(γ)<tan(π/4)=1\tan(\alpha+\gamma)=\frac{\tan(\alpha)+\tan(\gamma)}{1-\tan(\alpha)\tan(\gamma)}<\tan(\pi/4)=1, we get tan(α)+tan(γ)<1\tan(\alpha)+\tan(\gamma)<1, i.e. d(C,D)<1d(C,D)<1. Hence, FDC>π/3\angle FDC>\pi/3.

Since DAF=α+HAB<α+π/3\angle DAF=\alpha+\angle HAB<\alpha+\pi/3 and ADF=ADHFDC<π/2απ/3\angle ADF=\angle ADH-\angle FDC<\pi/2-\alpha-\pi/3, then DAF+ADF<π/2\angle DAF+\angle ADF<\pi/2. Consequently, DFA=πDAFADF>π/2\angle DFA=\pi-\angle DAF-\angle ADF>\pi/2 and we get a contradiction.

Refer to caption
Figure 19. Case 4.1b.

We suppose now that EE and FF are simple self Chebyshev centers. Hence BE[A,D]BE\perp[A,D] and DF[A,B]DF\perp[A,B] (see Fig. 19).

It is clear that the triangles DFADFA and AHDAHD, and respectively, BEABEA and AGBAGB are congruent. It implies CDA=DAB=ABC:=α\angle CDA=\angle DAB=\angle ABC:=\alpha and the triangles DFADFA and BEABEA are congruent. Hence d(A,B)=d(A,D)d(A,B)=d(A,D) and d(B,C)=d(C,D)d(B,C)=d(C,D).

It is clear that FDC=ADCADF=α(π/2α)=2απ/2\angle FDC=\angle ADC-\angle ADF=\alpha-(\pi/2-\alpha)=2\alpha-\pi/2. Hence BCD=2π(π/2+α+2απ/2)=2π3α\angle BCD=2\pi-(\pi/2+\alpha+2\alpha-\pi/2)=2\pi-3\alpha. Since the triangles AHCAHC and AGCAGC are congruent then ACD=ACB=π32α\angle ACD=\angle ACB=\pi-\frac{3}{2}\alpha. It implies d(C,H)=cot(π3α/2)=cot(3α/2)=d(C,G)d(C,H)=\cot(\pi-3\alpha/2)=-\cot(3\alpha/2)=d(C,G) and d(D,H)=d(B,G)=cot(α)d(D,H)=d(B,G)=\cot(\alpha).

Therefore, we get

L(bd(ABCD))=2sin(α)+2cot(α)2cot(3α2)=:f(α).L\bigl{(}\operatorname{bd}(ABCD)\bigr{)}=\frac{2}{\sin(\alpha)}+2\cot(\alpha)-2\cot\left(\frac{3\alpha}{2}\right)=:f(\alpha).

Since π3α/2<π/2\pi-3\alpha/2<\pi/2 then 3α>π3\alpha>\pi, i.e. α>π/3\alpha>\pi/3.

By direct computations, we obtain

f(α)\displaystyle f^{\prime}(\alpha) =\displaystyle\!\!\!\!=\!\!\!\! 12cos(α)sin2(α)2cos2(α)sin2(α)+3cos2(3α2)sin2(3α2)\displaystyle 1-\frac{2\cos(\alpha)}{\sin^{2}(\alpha)}-\frac{2\cos^{2}(\alpha)}{\sin^{2}(\alpha)}+\frac{3\cos^{2}(\frac{3\alpha}{2})}{\sin^{2}(\frac{3\alpha}{2})}
=\displaystyle\!\!\!\!=\!\!\!\! 1sin2(α)sin2(3α2)(sin2(3α2)(13cos2(α)2cos(α))+3cos2(3α2)sin2(α))\displaystyle\frac{1}{\sin^{2}(\alpha)\sin^{2}(\frac{3\alpha}{2})}\left(\sin^{2}\left(\frac{3\alpha}{2}\right)\left(1-3\cos^{2}(\alpha)-2\cos(\alpha)\right)+3\cos^{2}\left(\frac{3\alpha}{2}\right)\sin^{2}(\alpha)\right)
=\displaystyle\!\!\!\!=\!\!\!\! 2sin2(3α2)(8cos4(α2)4cos2(α2)1).\displaystyle-\frac{2}{\sin^{2}(\frac{3\alpha}{2})}\left(8\cos^{4}\left(\frac{\alpha}{2}\right)-4\cos^{2}\left(\frac{\alpha}{2}\right)-1\right).

Solving the equation 8cos4(α2)4cos2(α2)1=08\cos^{4}\left(\frac{\alpha}{2}\right)-4\cos^{2}\left(\frac{\alpha}{2}\right)-1=0 with respect to α\alpha, we obtain

α0=2arccos(121+3).\alpha_{0}=2\arccos\left(\frac{1}{2}\sqrt{1+\sqrt{3}}\right).

It is easy to check that f(α)f(\alpha) achieves its minimal value on (π/3,π/2)(\pi/3,\pi/2) exactly at the point α0\alpha_{0}. This minimal value is

f(2arccos(121+3))=433+23=3.389946f\left(2\arccos\left(\frac{1}{2}\sqrt{1+\sqrt{3}}\right)\right)=\frac{4}{3}\sqrt{3+2\sqrt{3}}=3.389946...

Therefore, if a quadrilateral ABCDABCD is extremal, then it is a magic kite.

8.3. Case 4.2

Let us consider a quadrilateral ABCDABCD with δ(bd(ABCD))=d(A,H)=d(B,E)=1\delta(\operatorname{bd}(ABCD))=d(A,H)=d(B,E)=1 and AH[D,C]AH\perp[D,C], BE[A,D]BE\perp[A,D] (see the left panel Fig. 20).

If d(D,G)=1d(D,G)=1 and DG[B,C]DG\perp[B,C] then EBGDEBGD is rectangle and d(E,G)>d(D,G)=1d(E,G)>d(D,G)=1. Therefore, EE and GG are not self Chebyshev centers. Hence DG⟂̸[B,C]DG\not\perp[B,C] and CF⟂̸[A,B]CF\not\perp[A,B].

If d(D,F)=d(C,F)=1d(D,F)=d(C,F)=1 then this case is impossible (see Remark 6 for Case 3.2).

Now, we consider the case when DF[A,B]DF\perp[A,B] and d(A,G)=d(D,G)=1d(A,G)=d(D,G)=1 (see the right panel Fig. 20). We put α:=BAD=ADC<π/2\alpha:=\angle BAD=\angle ADC<\pi/2, γ:=EBC<π/2\gamma:=\angle EBC<\pi/2 and denote by GG^{\prime} the midpoint of [A,D][A,D].

If AGDπ2\angle AGD\geq\frac{\pi}{2}, then L(bd(AGD))2+2L(\operatorname{bd}(AGD))\geq 2+\sqrt{2}. Hence, we have L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}, that is impossible for an extremal quadrilateral. Thus, AGD<π2\angle AGD<\frac{\pi}{2}. It implies that α>GAD>π4\alpha>\angle GAD>\frac{\pi}{4}.

Refer to caption

a)

Refer to caption

b)

Figure 20. a) Case 4.2; b) Case 4.2a.

It is easy to see that d(A,E)=cot(α)d(A,E)=\cot(\alpha) and d(A,G)=12d(A,D)=12sin(α)d(A,G^{\prime})=\frac{1}{2}d(A,D)=\frac{1}{2\sin(\alpha)}. Hence d(E,G)=12sin(α)cot(α)=12cos(α)2sin(α)d(E,G^{\prime})=\frac{1}{2\sin(\alpha)}-\cot(\alpha)=\frac{1-2\cos(\alpha)}{2\sin(\alpha)} and d(G,G)=1d2(A,G)=114sin2αd(G,G^{\prime})=\sqrt{1-d^{2}(A,G^{\prime})}=\sqrt{1-\frac{1}{4\sin^{2}{\alpha}}}.

From cot(γ)d(E,G)+d(G,G)=d(E,B)=1\cot(\gamma)d(E,G^{\prime})+d(G,G^{\prime})=d(E,B)=1 we get

cot(γ)(12cos(α))+4sin2(α)1=2sin(α),\cot(\gamma)(1-2\cos(\alpha))+\sqrt{4\sin^{2}(\alpha)-1}=2\sin(\alpha),

or, equivalently,

γ=arctan(12cos(α)2sin(α)4sin2(α)1).\gamma=\arctan\left(\frac{1-2\cos(\alpha)}{2\sin(\alpha)-\sqrt{4\sin^{2}(\alpha)-1}}\right).

Since BAH=BADDAH=α(π/2α)=2απ/2\angle BAH=\angle BAD-\angle DAH=\alpha-(\pi/2-\alpha)=2\alpha-\pi/2 then from the triangle BAHBAH we have

1+1sin2(α)2sin(α)cos(2απ/2)=1+1sin2(α)4cos(α)=d2(B,H)1.1+\frac{1}{\sin^{2}(\alpha)}-\frac{2}{\sin(\alpha)}\cos(2\alpha-\pi/2)=1+\frac{1}{\sin^{2}(\alpha)}-4\cos(\alpha)=d^{2}(B,H)\leq 1.

It implies 14sin2(α)cos(α)1\leq 4\sin^{2}(\alpha)\cos(\alpha). On the other hand since GAB=αGAG\angle GAB=\alpha-\angle G^{\prime}AG we get

AGB=πγ(π/2α)α+GAG=π/2γ+GAGπ/2.\angle AGB=\pi-\gamma-(\pi/2-\alpha)-\alpha+\angle G^{\prime}AG=\pi/2-\gamma+\angle G^{\prime}AG\leq\pi/2.

Thus, γGAG=arctan(d(G,G)d(A,G))=arctan(4sin2(α)1)\gamma\geq\angle G^{\prime}AG=\arctan\left(\frac{d(G,G^{\prime})}{d(A,G)}\right)=\arctan(4\sin^{2}(\alpha)-1) or, substituting the found expression for γ\gamma, we get

12cos(α)2sin(α)4sin2(α)14sin2(α)1,\frac{1-2\cos(\alpha)}{2\sin(\alpha)-\sqrt{4\sin^{2}(\alpha)-1}}\geq 4\sin^{2}(\alpha)-1,

which can be rewritten as 14sin2(α)cos(α)1\geq 4\sin^{2}(\alpha)\cos(\alpha).

Solving equation 1=4sin2(α)cos(α)1=4\sin^{2}(\alpha)\cos(\alpha) with respect to α(π/4,π/2)\alpha\in(\pi/4,\pi/2), we obtain α0=arccos(t0)=1.297824478\alpha_{0}=\arccos(t_{0})=1.297824478..., where t0=0.2695944364t_{0}=0.2695944364... is the root of the polynomial f(t)=4t34t+1f(t)=4t^{3}-4t+1 on the interval [0.2, 0.3][0.2,\,0.3]. By direct computations, we get γ0=1.024852628\gamma_{0}=1.024852628... and AGB=π/2\angle AGB=\pi/2. Hence d(C,D)=d(B,C)d(C,D)=d(B,C).

It is easy to see that ACB=π(π/2α)γα/2=π/2+α/2γ\angle ACB=\pi-(\pi/2-\alpha)-\gamma-\alpha/2=\pi/2+\alpha/2-\gamma. The equalities

d(B,C)sin(α/2)=d(A,B)sin(ACB)=1sin(α)sin(π/2γ+α/2)=1sin(α)cos(γα/2),\frac{d(B,C)}{\sin(\alpha/2)}=\frac{d(A,B)}{\sin(\angle ACB)}=\frac{1}{\sin(\alpha)\sin(\pi/2-\gamma+\alpha/2)}=\frac{1}{\sin(\alpha)\cos(\gamma-\alpha/2)},

imply

d(B,C)=12cos(α/2)cos(γα/2)=1cos(γ)+cos(αγ).d(B,C)=\frac{1}{2\cos(\alpha/2)\cos(\gamma-\alpha/2)}=\frac{1}{\cos(\gamma)+\cos(\alpha-\gamma)}.

Therefore, by direct computations, we get

L(bd(ABCD))=2d(A,B)+2d(B,C))=2sin(α0)+2cos(γ0)+cos(α0γ0)=3.426L(\operatorname{bd}(ABCD))=2d(A,B)+2d(B,C))=\frac{2}{\sin(\alpha_{0})}+\frac{2}{\cos(\gamma_{0})+\cos(\alpha_{0}-\gamma_{0})}=3.426...

Hence, the quadrilateral ABCDABCD is not extremal.

Refer to caption

a)

Refer to caption

b)

Figure 21. a) Case 4.3; b) Case 4.3a.

8.4. Case 4.3

Let us consider a quadrilateral ABCDABCD with δ(bd(ABCD))=d(D,F)=d(B,E)=1\delta(\operatorname{bd}(ABCD))=d(D,F)=d(B,E)=1 and DF[A,B]DF\perp[A,B], BE[A,D]BE\perp[A,D] (see the left panel Fig. 21).

If d(D,G)=1d(D,G)=1 and DG[B,C]DG\perp[B,C] then EBGDEBGD is rectangle and d(E,G)>d(D,G)=1d(E,G)>d(D,G)=1. Consequently, EE and GG is not self Chebyshev centers. Therefore, DGDG not [B,C]\perp[B,C] and CFCF not [A,B]\perp[A,B].

Now, we suppose that d(A,H)=d(B,H)=1d(A,H)=d(B,H)=1 and d(A,G)=d(D,G)=1d(A,G)=d(D,G)=1 (see the right panel Fig. 21). It is easy to see that d(A,B)=d(A,D)d(A,B)=d(A,D) and d(B,C)=d(C,D)d(B,C)=d(C,D). We put α:=BAD<π/2\alpha:=\angle BAD<\pi/2, γ:=EBC<π/2\gamma:=\angle EBC<\pi/2 and denote by GG^{\prime} be the midpoint of [A,D][A,D].

If AGDπ2\angle AGD\geq\frac{\pi}{2}, then L(bd(AGD))2+2L(\operatorname{bd}(AGD))\geq 2+\sqrt{2}. Hence, we have L(bd(ABCD))>2+2L(\operatorname{bd}(ABCD))>2+\sqrt{2}, that is impossible for an extremal quadrilateral. Thus, AGD<π2\angle AGD<\frac{\pi}{2}. It implies that α>GAD>π4\alpha>\angle GAD>\frac{\pi}{4}.

Repeating the reasoning similar to the previous case we get 14sin2(α)cos(α)1\geq 4\sin^{2}(\alpha)\cos(\alpha). Solving this inequality for α(π/4,π/2)\alpha\in(\pi/4,\pi/2), we obtain α(α0,π/2)\alpha\in(\alpha_{0},\pi/2) and α0=arccos(t0)=1.297824478\alpha_{0}=\arccos(t_{0})=1.297824478..., where t0=0.2695944364t_{0}=0.2695944364... is a unique root of the polynomial 4t34t+14t^{3}-4t+1 on the interval [0.2,0.3][0.2\,,0.3].

Also similar to the previous case, we get

L(bd(ABCD))=2d(A,B)+2d(B,C)=2sin(α)+2cos(γ)+cos(αγ).L(\operatorname{bd}(ABCD))=2d(A,B)+2d(B,C)=\frac{2}{\sin(\alpha)}+\frac{2}{\cos(\gamma)+\cos(\alpha-\gamma)}.

The results of numerical calculations show that the perimeter L(bd(ABCD))L\bigl{(}\operatorname{bd}(ABCD)\bigr{)} for the quadrilaterals under consideration reaches its minimal value exactly for AGB=AHD=π/2\angle AGB=\angle AHD=\pi/2 or α=α0=1.297824478\alpha=\alpha_{0}=1.297824478... and γ0=1.024852628\gamma_{0}=1.024852628.... This minimal value is L(bd(ABCD))=3.426L(\operatorname{bd}(ABCD))=3.426.... Hence, the quadrilateral ABCDABCD is not extremal.

It should be noted, that we found a quadralateral that can be extremal only in Case 4.1. Since at least one extremal quadrilateral does exist, we conclude that it is a magic kite from Case 4.1 and from the conjecture by Rolf Walter. This argument finished the proof of Theorem 1.

9. Computations and further conjectures

The search for possible extremal polygons for small values of nn was undertaken by E.V. Nikitenko. His experiments led to the conjecture that for odd nn, any extremal polygon is a regular nn-gon (this is the case for n=3n=3). On the other hand, for even values of nn, regular nn-gons are not extremal in the above sense. The type of an extremal polygon (quite possibly) depends on the power of the number 22 with which it enters to nn as a multiplier. See Fig. 22 for hypothetical extreme polygons for n=6n=6 and n=10n=10. The calculation of the characteristics of these polygons (in particular, these polygons are equilateral), as well as numerous computer experiments, lead to the following conjectures:

Refer to caption

a)

Refer to caption

b)

Figure 22. Extreme nn-gon candidates for: a) n=6n=6; b) n=10n=10. In both cases, the green and red polygons are regular, and are negative homothets of each other.
Conjecture 1.

For any convex 66-gon PP in the Euclidean plane, one has

L(Γ)12(23)δ(Γ),L(\Gamma)\geq 12\left(2-\sqrt{3}\leavevmode\nobreak\ \right)\cdot\delta(\Gamma),

where Γ\Gamma is the boundary of PP.

Conjecture 2.

For any convex 1010-gon PP in the Euclidean plane, one has

L(Γ)20(1+55+25)δ(Γ),L(\Gamma)\geq 20\left(1+\sqrt{5}-\sqrt{5+2\sqrt{5}}\leavevmode\nobreak\ \right)\cdot\delta(\Gamma),

where Γ\Gamma is the boundary of PP.

It should be noted that there are several extremal problems for polygons, with a similar behavior of the solution with respect to the number of sides nn. We recall two well-known problems of such kind.

Two classical isodiametric problems for polygons are to determine the maximal area and maximal perimeter of an nn-gon with unit diameter. Important results in the study of these two problems were obtained by K. Reinhardt in [19].

One of the main his results is the following [19, Theorem 1, P. 252]: Let nn be an odd number, n3n\geq 3; then the regular nn-gon has maximal area among all simple nn-gons of diameter dd.

For even n6n\geq 6 this is not true. For n=4n=4 it is true, but the square is not a unique solution: The diagonals of the square can be slightly shifted relative to each other, leaving them orthogonal.

It should be noted that a nn-gon of the maximum area among nn-gons with diameter dd is unique if nn is an odd number [19, P. 259].

The second main result by K. Reinhardt is the following [19, Theorem 2, P. 252]: Let nn be an integer that is not a degree of 22, n3n\geq 3. Then, among the convex nn-gons with diameter dd, the maximum perimeter is achieved if and only if a nn-gon is equilateral and inscribed in a Reulaux polygon of diameter dd so that the vertices of the Reulaux polygon are also the vertices of the nn-gon (such polygons are called Reinhardt polygons).

Moreover, this maximum perimeter coincides with the perimeter of the regular 2n2n-gon of diameter dd, as E. Makai, J. noticed (a private conversation). Indeed, if PnP_{n} is such a nn-gon, then the diameter of the polygon 12(PnPn)\frac{1}{2}(P_{n}-P_{n}) (this is the central symmetral of PnP_{n}, that have the same perimeter as PnP_{n} has) is also equal to dd, 12(PnPn)\frac{1}{2}(P_{n}-P_{n}) is inscribed into a circle of diameter dd, and has 2n\leq 2n sides. So, this perimeter is no more than the perimeter of the regular 2n2n-gon incribed into this circle (that can obtained via the above procedure from a regular nn-gon of diameter dd).

We also note that for any simple n3n\geq 3, there is only one nn-gon of the maximum perimeter among nn-gons with diameter dd [19, P. 263].

The largest areas of a hexagon and an octagon, resp., of unit diameter were given by R. Graham [13], and by C. Audet, P. Hansen, F. Messine, J. Xiong [7]. The largest perimeter of an octagon of unit diameter was given in C. Audet, P. Hansen, F. Messine [5]. The cases of higher even numbers, and higher powers of 22 seem to be open. See also [15] for more recent results on the topic.

C. Audet, P. Hansen, and F. Messine showed that the value 12ncot(π2n)\frac{1}{2n}\cot\left(\frac{\pi}{2n}\right) is an upper bound for the width of any nn-sided polygon with unit perimeter. This bound is reached when nn is not a power of 22, and the corresponding optimal solutions are the regular polygons when nn is odd and clipped regular Reuleaux polygons when nn is even but not a power of 22 [6].

We hope that these analogies will be useful in further research and will help to find an approach to the conjectures formulated above.

For the convenience of readers, here we provide the list of some important notations and definitions used in the paper (for each object, the page of the paper on which it is introduced is indicated).

  • For a given set MM in a given metric space (X,d)(X,d), the following concepts are defined on the Page 1: the Chebyshev radius, a Chebyshev center, the relative Chebyshev radius (with respect to a given non-empty subset in XX), the self Chebyshev radius.

  • Quadrilaterals called magic kites are defined on Page 1.

  • For a given compact set Γ2\Gamma\subset\mathbb{R}^{2} (in particular, a convex curve), the function μ:Γ\mu:\Gamma\rightarrow\mathbb{R} is defined by (2) on Page 2.

  • For a given point AΓA\in\Gamma, where Γ\Gamma is the boundary of a fixed nn-gon PP, the notations T+(A)T_{+}(A), T(A)T_{-}(A), and N(A)N(A) are introduced on Page 3, and (A)\mathcal{F}(A) is defined by (3) on the same page.

  • GlocminG_{\operatorname{locmin}}, the set of local minimum points of the function μ\mu, is introduced on Page 7.

  • The definition of extremal nn-gon PP is given on Page 7, see also Remark 4 on Page 4.

  • For the boundary Γ\Gamma of a fixed nn-gon PP, the function t:2t:\mathbb{R}^{2}\rightarrow\mathbb{R} is define by (4) on Page 4. On the same page, the sets UrU_{r} and LrL_{r} are defined for any r>0r>0, and GminG_{\min}, the set of self Chebyshev centers for Γ\Gamma, is introduced by (6).

  • On Page 4, the notation Gmin\|G_{\min}\| is introduced for the number of points in the set GminG_{\min}, or, in other words, the number of self Chebyshev centers for Γ\Gamma.

  • Simple and non-simple self Chebyshev centers for Γ\Gamma are defined on Page 4.

  • A special class of quadrilaterals 𝒫spec\mathcal{P}_{\operatorname{spec}} is introduced on Page 10.

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