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Convex pentagons and concave octagons that can form
rotationally symmetric tilings

Teruhisa SUGIMOTO1),2)
Abstract

In this study, the properties of convex pentagons that can form rotationally symmetric edge-to-edge tilings are discussed. Because the rotationally symmetric tilings are formed by concave octagons that are generated by two convex pentagons connected through a line symmetry, they are considered to be equivalent to rotationally symmetric tilings with concave octagons. In addition, under certain circumstances, tiling-like patterns with a regular polygonal hole at the center can be formed using these convex pentagons.

1) The Interdisciplinary Institute of Science, Technology and Art

2) Japan Tessellation Design Association

E-mail: [email protected]

Keywords: pentagon, octagon, tiling, rotational symmetry, monohedral, spiral

1 Introduction

In this study, as shown in Figure 1(a), let us label the vertices (interior angles) of the convex pentagon AA, BB, CC, DD, and EE, and its edges aa, bb, cc, dd, and ee in a fixed manner. A convex pentagonal tile111 A tiling (or tessellation) of the plane is a collection of sets that are called tiles, which covers a plane without gaps and overlaps, except for the boundaries of the tiles. The term “tile” refers to a topological disk, whose boundary is a simple closed curve. If all the tiles in a tiling are of the same size and shape, then the tiling is monohedral [3, 14]. In this study, a polygon that admits a monohedral tiling is called a polygonal tile [10, 9, 11]. Note that, in monohedral tiling, it admits the use of reflected tiles. that satisfies the conditions “A+B+C=360,C=2D,a=b=c=dA+B+C=360^{\circ},\;C=2D,\;a=b=c=d” belongs to the Type 1 family222 To date, fifteen families of convex pentagonal tiles, each of them referred to as a “Type,” are known [3, 10, 14]. For example, if the sum of three consecutive angles in a convex pentagonal tile is 360360^{\circ}, the pentagonal tile belongs to the Type 1 family. Convex pentagonal tiles belonging to some families also exist. Known convex pentagonal tiles can form periodic tiling. In May 2017, Michaël Rao declared that the complete list of Types of convex pentagonal tiles had been obtained (i.e., they have only the known 15 families), but it does not seem to be fixed as of March 2020 [14]. [3, 9, 10, 14]. The tile is called “C11-T1A” in [13] and its geometric properties are shown. Because this convex pentagon has four equal-length edges, its interior can be divided into a triangle BDE and two isosceles triangles ABE and BCD as shown in Figure 1(b). Given the foregoing properties, the relational expression of the interior angle of each vertex of C11-T1A can be rewritten as follows:

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Figure. 1: Nomenclature for vertices and edges of a convex pentagon, three triangles in the convex pentagonal tile C11-T1a, and the Octa-unit
Refer to caption
Figure. 2: Examples of variations of Type 1 tilings by C11-T1A
{A=1802B3,C=180B3,D=90B6,E=90+B6,\left\{{\begin{array}[]{l}A=180^{\circ}-\dfrac{2B}{3},\\ C=180^{\circ}-\dfrac{B}{3},\\ D=90^{\circ}-\dfrac{B}{6},\\ E=90^{\circ}+\dfrac{B}{6},\\ \end{array}}\right. (1)

where 0<B<1800^{\circ}<B<180^{\circ}. From the relationship between the five interior angles, the vertex concentrations that are always valid in tilings are “A+B+C=360, 2E+C=360, 2D+A+B=360, 2D+2E=360A+B+C=360^{\circ},\;2E+C=360^{\circ},\;2D+A+B=360^{\circ},\;2D+2E=360^{\circ}.” If a=b=c=d=1a=b=c=d=1, then the edge length of ee can be expressed as follows:

e=2sin(B2).e=2\sin\left({\frac{B}{2}}\right).

As shown in Figure 2, C11-T1A can form the representative tiling of Type 1 or variations of Type 1 tilings (i.e., tilings whose vertices are formed only by the relations of A+B+C=360A+B+C=360^{\circ} and D+E=180D+E=180^{\circ}). The edge ee of C11-T1A is the only edge of different length. As shown in Figure 1(c), an equilateral concave octagon formed by two convex pentagons, connected through a line symmetry whose axis is edge ee, is referred to as the Octa-unit. C11-T1A can form tilings that are not contained in the variations of Type 1 tilings, as shown in Figure 3, by using Octa-units. That is, C11-T1A can also form tilings by freely combining Octa-units with different directions in one direction [5, 13]

In this study, we introduce the convex pentagon C11-T1A that can generate countless numbers of rotationally symmetric tilings. Because the Octa-unit of C11-T1A is used in these rotationally symmetric tilings, it is considered similar to the concave octagons that can generate countless rotationally symmetric tilings.

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Figure. 3: Examples of tilings with Octa-units of C11-T1A

2 Rotationally symmetric tilings

In [5], there are figures of four-fold, five-fold, six-fold, and ten-fold rotationally symmetric edge-to-edge333 A tiling by convex polygons is edge-to-edge if any two convex polygons in a tiling are either disjoint or share one vertex or an entire edge in common. Then other case is non-edge-to-edge [3, 9, 10]. tilings using convex pentagonal tiles (or tiles that can be regarded as concave octagons). In [5], there are multiple types of edge-to-edge tilings with six-fold rotational symmetry by an equilateral convex pentagon, including Hirschhorn and Hunt’s types [4]. The convex pentagons forming these rotationally symmetric edge-to-edge tilings corresponded to C11-T1A.

By using the relational expression of the interior angles of (1), the conditions of pentagonal tile C11-T1A that can form nn-fold rotationally symmetric edge-to-edge tilings are expressed in (2).

{A=180240n,B=360n,C=180120n,D=9060n,E=90+60n,a=b=c=d,\left\{{\begin{array}[]{l}A=180^{\circ}-\dfrac{240^{\circ}}{n},\\ B=\dfrac{360^{\circ}}{n},\\ C=180^{\circ}-\dfrac{120^{\circ}}{n},\\ D=90^{\circ}-\dfrac{60^{\circ}}{n},\\ E=90^{\circ}+\dfrac{60^{\circ}}{n},\\ a=b=c=d,\\ \end{array}}\right. (2)

where nn is an integer greater than or equal to three, because 0<B<1800^{\circ}<B<180^{\circ}.

Table 1 presents some of the relationships between the interior angles of convex pentagons satisfying (2) that can form the nn-fold rotationally symmetric edge-to-edge tilings. (For n=313n=3\!-\!13, tilings with convex pentagonal tiles are drawn. For further details, Figures 515.) Given that n=6n=6, the convex pentagonal tile that satisfies (2) is an equilateral convex pentagon, and can form several different six-fold rotationally symmetric edge-to-edge tilings [4, 5, 13, 14]. The tiling in Figure 8 is one of the six-fold rotationally symmetric edge-to-edge tilings by the equilateral convex pentagon that Hirschhorn and Hunt presented [4]. Note that the nn-fold rotationally symmetric edge-to-edge tilings by convex pentagonal tiles satisfying (2) have CnC_{n} symmetry444CnC_{n}” is based on the Schoenflies notation for symmetry in a two-dimensional point group [15, 16]. “CnC_{n}” represents an nn-fold rotation axis without reflection. The notation for symmetry is based on that presented in [6]. because they have rotational symmetry, but no axis of reflection symmetry.

Table 1: Interior angles of convex pentagons satisfying (2) that can form the nn-fold rotationally symmetric edge-to-edge tilings
nn Value of interior angle (degree) Edge length of ee Figure number
A B C D E
3 100100 120120 140140 7070 110110 1.732 5
4 120120 9090 150150 7575 105105 1.414 6
5 132132 7272 156156 7878 102102 1.176 7
6 140140 6060 160160 8080 100100 1 8
7 145.71145.71 51.4351.43 162.86162.86 81.4381.43 98.5798.57 0.868 9
8 150150 4545 165165 82.582.5 97.597.5 0.765 10
9 153.33153.33 4040 166.67166.67 83.3383.33 96.6796.67 0.684 11
10 156156 3636 168168 8484 9696 0.618 12
11 158.18158.18 32.7332.73 169.09169.09 84.5584.55 95.4595.45 0.563 13
12 160160 3030 170170 8585 9595 0.518 14
13 161.54161.54 27.6927.69 170.77170.77 85.3885.38 94.6294.62 0.479 15
14 162.86162.86 25.7125.71 171.43171.43 85.7185.71 94.2994.29 0.445
15 164164 2424 172172 8686 9494 0.416
16 165165 22.522.5 172.5172.5 86.2586.25 93.7593.75 0.390
17 165.88165.88 21.1821.18 172.94172.94 86.4786.47 93.5393.53 0.367
18 166.67166.67 2020 173.33173.33 86.6786.67 93.3393.33 0.347
... ... ... ... ...
Refer to caption
Figure. 4: Formation methods of rotationally symmetric edge-to-edge tiling and of rotationally symmetric tiling with a regular mm-gonal hole at the center using C11-T1A

Here, the formation of rotationally symmetric edge-to-edge tiling with convex pentagonal tiles is briefly explained. First, as shown in STEP 1 in Figure 4, create a unit connecting the Octa-units that are generated by convex pentagons satisfying (2) in one direction so that A+B+C=360A+B+C=360^{\circ}. The Octa-units can then be assembled in such a way as to increase the number of pieces from one to two to three, and so on, in order. Then, copy the two units in STEP 1. In STEP 2, first, rotate one of the two copied units by 120n\frac{120^{\circ}}{n}, with respect to the original (see STEP 2 of Figure 4, wherein the axis of \scriptsize2⃝\scriptsize2⃝ has a rotation of 120n\frac{120^{\circ}}{n} with respect to the axis of \scriptsize1⃝\scriptsize1⃝), and connect it to the original to get the following results: 2E+C=3602E+C=360^{\circ}, 2D+A+B=3602D+A+B=360^{\circ}, and A+B+C=360A+B+C=360^{\circ}, as expressed in STEP 2 of Figure 4. Next, rotate the remaining unit by 240n\frac{240^{\circ}}{n}, with respect to the original (see STEP 2 of Figure 4, wherein the axis of \scriptsize3⃝\scriptsize3⃝ has a rotation of 240n\frac{240^{\circ}}{n} with respect to the axis of \scriptsize1⃝\scriptsize1⃝), and connect it in the same way as the one previously made to make a unit like that in STEP 2 in Figure 4. Next, copy the unit in STEP 2. Subsequently, take the unit from STEP 2 and rotate it by the value of the interior angle of vertex BB. When the original unit and the rotated unit are arranged as shown in STEP 3 (Rotationally symmetric tiling) in Figure 4, 2n\frac{2}{n} parts in the nn-fold rotationally symmetric tiling can be formed. Then, by repeating this process as many times as necessary, an nn-fold rotationally symmetric edge-to-edge tiling with convex pentagonal tiles can be formed.

Klaassen [6] presented the convex pentagonal tiles that can generate countless rotationally symmetric edge-to-edge tilings; however, the pentagon tilings were non-edge-to-edge. On the other hand, it was shown that the convex pentagonal tiles satisfying (2) can generate countless rotationally symmetric edge-to-edge tilings. Although the corresponding theorem and proof are not presented, similar to how it was in [6], it will still be understood that countless rotationally symmetric tilings can be generated by the foregoing explanations and methods.

3 Rotationally symmetric tilings (tiling-like patterns) with a regular polygonal hole at the center

In [5], there are figures of rotationally symmetric tiling-like patterns with a hole in the center of a regular heptagon, 10-gon, 12-gon, or 18-gon formed using convex pentagons (or elements that can be regarded as concave octagons). The regular 18-gonal hole can be filled with convex pentagons, but the other holes cannot be filled with convex pentagons. Note that the tiling-like patterns are not considered tilings due to the presence of a gap, but are simply called tilings in this study. The convex pentagons forming these rotationally symmetric tilings with a regular mm-gonal hole corresponded to C11-T1A.

By using the relational expression of the interior angles of (1), the conditions of pentagonal tile C11-T1A that can form rotationally symmetric tilings with a regular mm-gonal hole are expressed in (3).

{A=180720m,B=1080m,C=180360m,D=90180m,E=90+180m,a=b=c=d,\left\{{\begin{array}[]{l}A=180^{\circ}-\dfrac{720^{\circ}}{m},\\ B=\dfrac{1080^{\circ}}{m},\\ C=180^{\circ}-\dfrac{360^{\circ}}{m},\\ D=90^{\circ}-\dfrac{180^{\circ}}{m},\\ E=90^{\circ}+\dfrac{180^{\circ}}{m},\\ a=b=c=d,\\ \end{array}}\right. (3)

where mm is an integer greater than or equal to seven, because 0<B<1800^{\circ}<B<180^{\circ}. Note that, because “180360m180^{\circ}-\frac{360^{\circ}}{m}” corresponds to one interior angle of a regular mm-gon, the value of “A+BA+B” in (3) is equal to the outer angle (180+360m180^{\circ}+\frac{360^{\circ}}{m}) of one vertex of a regular mm-gon.

Table 2 presents some of the relationships between the interior angles of convex pentagons satisfying (3) that can form the rotationally symmetric tilings with a regular mm-gonal hole at the center. (For m=710,12,14,15,18,21,24,27m=7\!-\!10,12,14,15,18,21,24,27, tilings with a regular mm-gonal hole at the center formed by convex pentagons are drawn. For further details, Figures 1826.) If these elements are considered to be convex pentagons, the connection is edge-to-edge. These tilings with a regular mm-gonal hole with DmD_{m} symmetry555DmD_{m}” is based on the Schoenflies notation for symmetry in a two-dimensional point group [15, 16]. “DmD_{m}” represents an mm-fold rotation axis with mm reflection symmetry axes. at the center have CmC_{m} symmetry. If convex pentagons satisfying (3) have mm that is divisible by three, they are also convex pentagonal tiles that satisfy (2).

Table 2: Interior angles of convex pentagons satisfying (3) that can form the rotationally symmetric tilings with a regular mm-gonal hole at the center
nn Value of interior angle (degree) Edge length of ee nn of Table 1 Figure number
A B C D E
7 77.1477.14 154.29154.29 128.57128.57 64.2964.29 115.71115.71 1.950 16
8 9090 135135 135135 67.567.5 112.5112.5 1.848 17
9 100100 120120 140140 7070 110110 1.732 3 18
10 108108 108108 144144 7272 108108 1.618 19
11 114.55114.55 98.1898.18 147.27147.27 73.6473.64 106.36106.36 1.511
12 120120 9090 150150 7575 105105 1.414 4 20
13 124.62124.62 83.0883.08 152.31152.31 76.1576.15 103.85103.85 1.326
14 128.57128.57 77.1477.14 154.29154.29 77.1477.14 102.86102.86 1.247 21
15 132132 7272 156156 7878 102102 1.176 5 22
16 135135 67.567.5 157.5157.5 78.7578.75 101.25101.25 1.111
17 137.65137.65 63.5363.53 158.82158.82 79.4179.41 100.59100.59 1.053
18 140140 6060 160160 8080 100100 1 6 23
19 142.11142.11 56.8456.84 161.05161.05 80.5380.53 99.4799.47 0.952
20 144144 5454 162162 8181 9999 0.908
21 145.71145.71 51.4351.43 162.86162.86 81.4381.43 98.5798.57 0.868 7 25
22 147.27147.27 49.0949.09 163.64163.64 81.8281.82 98.1898.18 0.831
23 148.70148.70 46.9646.96 164.35164.35 82.1782.17 97.8397.83 0.797
24 150150 4545 165165 82.582.5 97.597.5 0.765 8 26
25 151.2151.2 43.243.2 165.6165.6 82.882.8 97.297.2 0.736
26 152.31152.31 41.5441.54 166.15166.15 83.0883.08 96.9296.92 0.709
27 153.33153.33 4040 166.67166.67 83.3383.33 96.6796.67 0.684 9 27
... ... ... ... ...

Rotationally symmetric tilings with a regular mm-gonal hole at the center can be made in almost the same way as the nn-fold rotationally symmetric edge-to-edge tiling (i.e., the manner of creation follows the same steps up to STEP 2 of Figure 4). The part with three edges AB, at the center of the unit made in STEP 2 of Figure 4, corresponds to the contour of a regular mm-gon. Therefore, copy the unit in STEP 2, take the unit from STEP 2 and rotate it by the value of the interior angle of vertex BB. When the original unit and the rotated unit are arranged as shown in STEP 3 (Tiling with a regular mm-gonal hole) in Figure 4, 6m\frac{6}{m} parts of a regular mm-gon can be formed. Then, by repeating this process as many times as necessary, a rotationally symmetric tiling with a regular mm-gonal hole at the center can be formed.

As shown in Table 2 and Figure 23, the convex pentagonal tile that satisfies (3), where m=18m=18, is an equilateral convex pentagon. As such, the regular 18-gonal hole can be filled with equilateral convex pentagons. The pentagonal arrangement pattern in the regular 18-gon is unique; however, the regular 18-gon can be reversed; therefore, two patterns can be used in the hole (see Figure 23). The tiling in Figure 24 is one of the six-fold rotationally symmetric edge-to-edge tilings with equilateral convex pentagons that Hirschhorn and Hunt present in [4]. In addition, the tiling in Figure 23 is that of Hirschhorn [7]. In [5], there are figures of tilings corresponding to Figures 8, 23, and 24, with the one corresponding to Figure 24 labeled as Hirschhorn’s rosette. These tilings with a regular 18-gonal hole that is filled with equilateral convex pentagons have C6C_{6} symmetry. In Pegg’s research [2], they stated there exists the tiling of Figure 8, using the equilateral convex pentagon, and that there are also other interesting tilings, such as that with the “crystal-like” structure. Note that in Pegg’s research [2], there are non-monohedral tilings created using convex and concave pentagons.

As described above, the tiling of m=10m=10 in Table 2 (see Figure 19) is listed in Iliev’s research [5], however, the value of the interior angle of the convex pentagon was erroneous, as well as in Smith’s research [8]. It is shown that the convex pentagon of m=10m=10 in Table 2 is the same as the convex pentagonal tile belonging to both the Type 1 and Type 2 families, and that it can form various tilings [1, 5, 8]. In [1] and [8], there are also tilings with a regular pentagonal hole at the center using this convex pentagon of m=10m=10 in Table 2. Moreover, it is interesting to note that the ring-shaped layer forming the periphery can be reversed in [8].

4 Spiral tilings

Klaassen [6] also showed the viewpoint of rotationally symmetric tilings with convex pentagons as a spiral structure. A similar spiral structure can be found in the rotationally symmetric edge-to-edge tilings with convex pentagons of C11-T1A. Figure 28 pertains to the case where n=5n=5, which makes the spiral structure easier to understand. From this spiral structure, the difference between the rotationally symmetric tilings with convex pentagons in [6] and the rotationally symmetric edge-to-edge tilings with C11-T1A other than the edge-to-edge property will be determinable.

Here, let us pay attention to the convex pentagon of m=8m=8 in Table 2. This convex pentagon has the property of B=C=135B=C=135^{\circ}. From this property, the convex pentagon of m=8m=8 in Table 2 can form spiral tilings666 It is difficult to determine what the spiral tiling is. There are some discussions, such as those in [7]. The tiling shown in Figure 28 can be regarded as a spiral, however, it has a radial structure extending from the center. Thus, we feel that it is more straightforward to regard it as a rotationally symmetric tiling. On the other hand, because the tiling of Figure 29 does not have a radial structure extending from the center or singularity point, we feel that it is a spiral rather than a rotationally symmetric tiling. with two-fold rotational symmetry, as shown in Figure 29(a). This convex pentagonal tile belongs to both the Type 1 and Type 7 families [3, 10, 9, 11, 14].

After finding the tiling in Figure 29(a), we found that, in “(6) Central block ‘wraparound’ ” of [1], Bailey presented the spiral tilings with two-fold rotational symmetry by the convex pentagon corresponding to the case of m=10m=10 in Table 2. The spiral tiling is the same as that in Figure 30(a). Furthermore, from [1], we found that it is possible to form tilings that keep the spiral structure and extend in one direction only, as shown in Figures 30(b), 30(c), and 30(d). Then, we determined that the convex pentagon of m=8m=8 in Table 2 can also form tilings that keep the spiral structure and extend in one direction (see Figures 29(b), 29(c), and 29(d)).

The convex pentagon of m=14m=14 in Table 2 has B=D=3π777.14B=D=\frac{3\pi}{7}\approx 77.14^{\circ}, and belongs to both the Type 1 and Type 2 families. Similar to the convex pentagons of m=8,10m=8,10 in Table 2, the convex pentagon of m=14m=14 in Table 2 can also form the spiral tiling with two-fold rotational symmetry (see Figure 31(a)) and tilings that keep the spiral structure and extend in one direction (see Figures 31(b), 31(c), and 31(d)). For all convex pentagons of m=8,10,14m=8,10,14 in Table 2, it is also possible to remove one spiral structure and to extend the belts wherein the Octa-units are arranged (see Figure 32).

It should be noted that the spiral tiling with a regular pentagonal hole at the center is shown in [8] using the convex pentagon corresponding to m=10m=10 in Table 2.

5 Conclusions

The existence of convex pentagonal tiles that can generate countless number of rotationally symmetric edge-to-edge tilings is not well-known. As mentioned above, Klaassen presented a case where tilings are not edge-to-edge. From [5], we determined that the convex pentagon called C11-T1A in [13] had this property. In [5], Iliev presented the tilings corresponding to n=4,5,6,10n=4,5,6,10 in Table 1 and m=7,10,12,18m=7,10,12,18 in Table 2. It may have been inferred by Iliev that there are countless rotationally symmetric tilings similar to those; however, there seems to be no clarification on the matter. In particular, there is no description of the concrete properties (tile conditions), such as the convex pentagon of C11-T1A, as shown in this study.

It was previously recognized that the convex pentagon belonging to both the Type 1 and Type 7 families (i.e., convex pentagon corresponding to m=8m=8 in Table 2) can generate various albeit limited tilings. However, in reality, we noticed that it is possible to generate more tilings. Among them are other rotational symmetric tilings and spiral tilings. We will introduce them in a different article [12] .


Acknowledgments. The author would like to thank Yoshiaki ARAKI of Japan Tessellation Design Association, for information of Bailey’s site, etc. and comments.

References

Refer to caption
Figure. 5: Three-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 6: Four-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 7: Five-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 8: Six-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 9: Seven-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 10: Eight-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 11: Nine-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 12: 10-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 13: 11-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 14: 12-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 15: 13-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 16: Rotationally symmetric tiling with C7C_{7} symmetry with a regular convex heptagonal hole at the center by a convex pentagon
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Figure. 17: Rotationally symmetric tiling with C8C_{8} symmetry with a regular convex octagonal hole at the center by a convex pentagon
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Figure. 18: Rotationally symmetric tiling with C9C_{9} symmetry with a regular convex nonagonal hole at the center by a convex pentagon
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Figure. 19: Rotationally symmetric tiling with C10C_{10} symmetry with a regular convex 10-gonal hole at the center by a convex pentagon
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Figure. 20: Rotationally symmetric tiling with C12C_{12} symmetry with a regular convex 12-gonal hole at the center by a convex pentagon
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Figure. 21: Rotationally symmetric tiling with C14C_{14} symmetry with a regular convex 14-gonal hole at the center by a convex pentagon
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Figure. 22: Rotationally symmetric tiling with C15C_{15} symmetry with a regular convex 15-gonal hole at the center by a convex pentagon
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Figure. 23: Rotationally symmetric tiling with a regular convex 18-gon at the center by an equilateral convex pentagon
Refer to caption
Figure. 24: Hirschhorn and Hunt’s rotationally symmetric tiling with a regular convex 18-gon at the center by an equilateral convex pentagon
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Figure. 25: Rotationally symmetric tiling with C21C_{21} symmetry with a regular convex 21-gonal hole at the center by a convex pentagon
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Figure. 26: Rotationally symmetric tiling with C24C_{24} symmetry with a regular convex 24-gonal hole at the center by a convex pentagon
Refer to caption
Figure. 27: Rotationally symmetric tiling with C27C_{27} symmetry with a regular convex 27-gonal hole at the center by a convex pentagon
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Figure. 28: Spiral structure of five-fold rotationally symmetric edge-to-edge tiling by a convex pentagon
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Figure. 29: Spiral tilings with two-fold rotational symmetry by a convex pentagon of m=8m=8 in Table 2
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Figure. 30: Spiral tilings with two-fold rotational symmetry by a convex pentagon of m=10m=10 in Table 2
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Figure. 31: Spiral tilings with two-fold rotational symmetry by a convex pentagon of m=14m=14 in Table 2
Refer to caption
Figure. 32: Tilings that removed one spiral structure and extend the belts of Octa-units using convex pentagons of m=8,10,14m=8,10,14 in Table 2