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Tetradecagon

A tetradecagon, also known as a tetrakaidecagon or 14-gon, is a consisting of fourteen sides and fourteen . In its form, all sides are of equal length and all interior angles are equal, measuring approximately 128.57 degrees each, with the sum of interior angles totaling 2160 degrees as determined by the formula (n-2)×180° for an n-sided where n=14. The tetradecagon possesses dihedral symmetry of order 28, denoted by the Schläfli symbol {14}, and its area can be calculated as A = \frac{14}{4} a^2 \cot \frac{\pi}{14} \approx 15.3345 a^2, where a is the side length. Unlike some polygons, a tetradecagon cannot be constructed using only a and due to the involvement of the prime factor 7 in its vertex count, which does not satisfy the conditions for classical constructibility. It appears in various geometric contexts, such as stellations and dissections, and serves as a in certain higher-dimensional .

Definitions and Fundamentals

General tetradecagon

A is a with exactly fourteen and fourteen vertices, where each connects two consecutive vertices to form a closed . In general, it need not have equal side lengths or angles, distinguishing it from the regular variant. Tetradecagons may be classified as or self-intersecting based on whether their cross one another. tetradecagons form a Jordan curve with no self-intersections, while self-intersecting forms, such as certain polygons, feature overlapping . Among tetradecagons, examples lie entirely on one side of each supporting line through their , whereas ones have at least one reflex interior angle exceeding 180° and indentations. For any tetradecagon, the sum of its interior angles measures 2160°, obtained by triangulating the into twelve non-overlapping triangles, each with an angle sum of 180°. This holds irrespective of convexity, as the triangulation covers the interior without gaps or overlaps. Self-intersecting tetradecagons lack a well-defined interior in the same topological sense, rendering the standard angle sum inapplicable without additional conventions.

Regular tetradecagon

A tetradecagon is a consisting of fourteen sides of equal length and fourteen interior angles of equal measure. The measure of each interior angle is given by the formula for polygons, \frac{(n-2) \times 180^\circ}{n}, where n=14, yielding \frac{12 \times 180^\circ}{14} = \frac{6 \times 180^\circ}{7} \approx 154.2857^\circ. In the complex plane, the vertices of a regular tetradecagon inscribed in the unit circle are located at the points e^{2\pi i k / 14} for integers k = 0, 1, \dots, 13, corresponding to angular positions of $2\pi k / 14 radians from the positive real axis. The geometry of the regular tetradecagon relates to that of the regular heptagon, as $14 = 2 \times 7; the side length for a circumradius of 1 is $2 \sin(\pi / 14), which equals $2 \cos(3\pi / 7), with the value of \cos(3\pi / 7) obtainable as a root of the equation derived from the triple-angle formula or the minimal polynomial for $2\cos(2\pi / 7).

Geometric Properties

Angles and side relations

The interior angle of a regular tetradecagon measures \frac{(14-2) \times 180^\circ}{14} = \frac{1080^\circ}{7} \approx 154.2857^\circ. The corresponding exterior angle is \frac{360^\circ}{14} = \frac{180^\circ}{7} \approx 25.7143^\circ. The subtended by each side at the center of the equals the exterior angle, \frac{360^\circ}{14} \approx 25.7143^\circ. For a regular tetradecagon inscribed in a (circumradius r = 1), the side length is the spanning one interval: $2 \sin\left(\frac{\pi}{14}\right). More generally, chords spanning k adjacent vertices have length $2 \sin\left(\frac{k\pi}{14}\right) for k = 1 to $7, where k=1 gives the side and k=7 yields the $2. These chord lengths establish proportional relations among sides and diagonals: the six distinct diagonal types (for k=2 to k=7) increase monotonically from $2 \sin\left(\frac{2\pi}{14}\right) = 2 \sin\left(\frac{\pi}{7}\right) to $2, with symmetry ensuring equal lengths for spans of k and $14-k vertices. The longest proper diagonal (k=6) measures $2 \sin\left(\frac{6\pi}{14}\right) = 2 \sin\left(\frac{3\pi}{7}\right) \approx 1.9499, approaching but not reaching the .
Span kChord typeLength (unit circle)
1Side$2 \sin(\pi/14)
2Shortest diagonal$2 \sin(2\pi/14)
3Diagonal$2 \sin(3\pi/14)
4Diagonal$2 \sin(4\pi/14)
5Diagonal$2 \sin(5\pi/14)
6Longest proper diagonal$2 \sin(6\pi/14)
7$2 \sin(7\pi/14) = 2

Area, perimeter, and radius formulas

The perimeter P of a regular tetradecagon is P = 14s, where s denotes the side length. The side length relates to the circumradius R (distance from center to vertex) via s = 2R \sin\left(\frac{\pi}{14}\right), derived by bisecting the central isosceles triangle with apex angle \frac{2\pi}{14} = \frac{\pi}{7}. The inradius r (or apothem, distance from center to side midpoint) is r = R \cos\left(\frac{\pi}{14}\right), obtained from the same bisection yielding adjacent over hypotenuse in the right triangle. The area A follows from summing the areas of 14 isosceles triangles with two sides R and included angle \frac{\pi}{7}, giving A = 7 R^2 \sin\left(\frac{\pi}{7}\right). Equivalently, A = \frac{1}{2} P r = 7 s r, or directly in terms of side length as A = \frac{7 s^2}{2} \cot\left(\frac{\pi}{14}\right) \approx 15.3345 s^2.

Diagonals and chord lengths

In a regular tetradecagon inscribed in a circle of radius R, the chord lengths between vertices separated by k steps along the perimeter are given by d_k = 2R \sin\left(\frac{k\pi}{14}\right) for k = 1, 2, \dots, 7, where k=1 yields the side length and k=2 to k=7 yield the diagonals, with k=7 being the $2R. These lengths arise from the \frac{2k\pi}{14} = \frac{k\pi}{7} subtended by the arc, using the standard relation in the formed by two radii and the . The squared lengths simplify to d_k^2 = 2R^2 \left(1 - \cos\left(\frac{k\pi}{7}\right)\right), linking them algebraically to the cosines \cos\left(\frac{m\pi}{7}\right) for m=1,2,3, as higher k values reflect symmetries \sin\left(\frac{(14-k)\pi}{14}\right) = \cos\left(\frac{k\pi}{7}\right). The values \cos\left(\frac{\pi}{7}\right), \cos\left(\frac{3\pi}{7}\right), and \cos\left(\frac{5\pi}{7}\right) are the roots of the irreducible cubic equation $8x^3 - 4x^2 - 4x + 1 = 0 over the rationals, derived from the triple-angle formula \cos(3\theta) = 4\cos^3\theta - 3\cos\theta applied to \theta = \frac{\pi}{7}, \frac{3\pi}{7}, \frac{5\pi}{7}, yielding a degree-3 minimal polynomial consistent with the real subfield of the 7th cyclotomic extension. Thus, the diagonal lengths for k=2 to k=6 are algebraic numbers of degree at most 3 (or 6 in the full cyclotomic field when expressed via sines), while ratios such as \frac{d_2}{d_1} = \frac{\sin(\pi/7)}{\sin(\pi/14)} reduce via angle identities to expressions solvable from the same cubic. The diameter d_7 = 2R is rational, distinguishing it as the sole exact diagonal in closed radical form without invoking the polynomial. For R=1, the approximate diagonal lengths (to four decimal places) are as follows, computed from the trigonometric values tied to the cubic roots:
k (steps)Diagonal typeLength d_k \approx
2Shortest diagonal0.8678
31.2470
41.5637
51.8019
6Near-diameter1.9499
7Diameter2.0000
These approximations reflect the increasing span from skipping one vertex (k=2) to the opposite vertex (k=7), with the longest non-diameter diagonal approaching but not reaching $2R due to the even number of sides. Exact ratios, such as the golden-ratio-like properties in heptagonal geometry extended here, emerge from solving the cubic, e.g., $2\cos(\pi/7) \approx 1.8019 directly giving d_5.

Constructibility and Construction

Compass and straightedge limitations

A regular tetradecagon is not constructible with and . According to the Gauss–Wantzel , a n-gon is constructible n = 2^k \prod p_i, where the p_i are distinct Fermat primes and k \geq 0. For n=14=2 \cdot 7, the odd prime factor 7 is not a Fermat prime (known Fermat primes are 3, 5, 17, 257, and ). Constructibility requires the coordinates of the vertices, expressible via \cos(2\pi/14) = \cos(\pi/7), to lie in a of \mathbb{Q} of degree a power of 2. The degree [\mathbb{Q}(\cos(2\pi/n)) : \mathbb{Q}] = \phi(n)/2 for n > 2, where \phi is . Here, \phi(14) = 6, so the degree is 3, which is not a power of 2. This degree-3 extension arises from the factor 7: \mathbb{Q}(\zeta_{14}) = \mathbb{Q}(\zeta_7) (since \zeta_{14}^2 = -\zeta_7), with [\mathbb{Q}(\zeta_7) : \mathbb{Q}] = \phi(7) = 6. The real subfield \mathbb{Q}(\cos(2\pi/7)) has degree 3, generated by \eta = 2\cos(2\pi/7), whose minimal polynomial over \mathbb{Q} is the irreducible cubic x^3 + x^2 - 2x - 1 = 0. Compass-and-straightedge constructions correspond to quadratic extensions (solvings of quadratics via square roots), incapable of producing irreducible cubics in finite steps. In contrast, the regular pentagon is constructible because \phi(5)/2 = 2, a power of 2, allowing resolution via extensions. No such sequence exists for \pi/7, confirming the limitation for the tetradecagon.

Alternative exact constructions

The regular tetradecagon can be constructed exactly using techniques, which extend beyond classical and methods by solving cubic equations through the Huzita–Hatori axioms. These axioms permit operations equivalent to , enabling the derivation of coordinates involving \cos(2\pi/14) = \cos(\pi/7), the real root of the minimal polynomial $8x^3 + 4x^2 - 4x - 1 = 0. A specific construction for the regular , foundational to the tetradecagon, involves sequential folds to bisect angles and align creases that implicitly trisect relevant angles, as detailed in computational verifications of fold sequences. Neusis constructions with a marked ruler also yield exact vertices of the regular tetradecagon by facilitating verging operations that solve the same cubic. In one such , a marked is used to position segments satisfying trigonometric identities for \pi/7, as in David Johnson Leisk's (Crockett Johnson) animation demonstrating side-length-given construction through iterative neusis steps aligning marked intervals with circle arcs and lines. This approach leverages the marked ruler's ability to perform non-quadratic extensions, proven geometrically for heptagonal angles and extendable to the doubled-sided 14-gon. Linkage mechanisms, such as 14-bar configurations, theoretically permit exact positioning of vertices via solvable linkages incorporating 7th roots of unity, though practical implementations rely on kinematic analysis rather than physical rigidity for verification. These methods confirm constructibility in the plane through algebraic closures beyond quadratic fields, distinct from approximation techniques.

Approximation techniques

Archimedean-style iterative approximations adapt the recursive perimeter refinements used by Archimedes for bounding π to estimate chord lengths in regular polygons. For a regular tetradecagon inscribed in a unit circle, the half-side length equals sin(π/14), which can be approximated by iterating relations between successive polygon side lengths, such as the formula for the difference between inscribed and circumscribed perimeters, converging quadratically to the exact value. This method yields sin(π/14) ≈ 0.2225 after refinements equivalent to high-sided polygons, providing a geometric basis for manual construction with straightedge and compass by approximating equal arc divisions. Numerical coordinate approximations solve the 14th or its real subfield equivalents using root-finding algorithms like Newton-Raphson. Specifically, (2π/14) = (π/7) satisfies the 8x³ - 4x² - 4x + 1 = 0, derived from the septuple-angle formula for cosine. Starting from an initial guess x₀ ≈ 0.9, the Newton-Raphson iteration x_{k+1} = x_k - f(x_k)/f'(x_k), where f(x) = 8x³ - 4x² - 4x + 1 and f'(x) = 24x² - 8x - 4, converges rapidly to ≈ 0.9009688679 in fewer than five steps, enabling precise placement via x_k = (2π k /14), y_k = (2π k /14). In computational environments such as CAD software, parametric representations leverage high-precision arithmetic or expansions for . The series sin(θ) = θ - θ³/3! + θ⁵/5! - ..., with θ = π/14 ≈ 0.224399, truncated at order 10 yields accuracy exceeding 10^{-10}, sufficient for engineering tolerances when scaled to physical dimensions. These approximations are validated by comparison to algebraic exact expressions, ensuring minimal deviation in side lengths and angles for practical implementations. General geometric approximation procedures, adaptable for n=14, further support hand-drawn constructions by optimizing settings for near-equal divisions.

Symmetry and Group Theory

Dihedral symmetry group D<sub>14</sub>

The dihedral group D_{14} is the symmetry group of the regular tetradecagon, comprising all isometries of the plane that map the polygon to itself, including rotations and reflections. It has order 28, with 14 elements corresponding to rotations by angles k \times \frac{360^\circ}{14} for integers k = 0 to $13, and 14 reflection elements across axes of symmetry. These rotations form a cyclic subgroup isomorphic to C_{14}, generated by a minimal rotation r of order 14. The group admits the presentation \langle r, s \mid r^{14} = s^2 = 1, \, s r s = r^{-1} \rangle, where r generates rotations and s a reflection, ensuring a faithful action on the plane via orientation-preserving rotations and orientation-reversing reflections. Since 14 is even, the 14 reflection axes consist of 7 passing through pairs of opposite vertices and 7 passing through midpoints of pairs of opposite sides. Notable subgroups include the rotation subgroup \langle r \rangle \cong C_{14} of index 2, which is . Additionally, Klein four-subgroups arise, such as \langle r^7, s \rangle, generated by the 180° rotation r^7 (order 2) and a s (order 2); here, s r^7 s = r^{-7} = r^7 (modulo order 14), yielding the elements \{1, r^7, s, s r^7\}, all non-identity elements of order 2, isomorphic to the V_4. Conjugate subgroups exist for each choice of reflection generator.

Reflection and rotational symmetries

The rotational symmetries of a tetradecagon comprise 14 elements, generated by about the center by \frac{2\pi}{14} radians (approximately 25.714°). This generator permutes the vertices in a single 14-cycle when labeled consecutively around the . Non-identity rotations fix no vertices, preserving only the center point. Reflections number 14, divided into two conjugacy classes for even-sided polygons. Seven vertex-axis reflections each pass through a pair of opposite vertices, fixing those two points while decomposing into six 2-cycles on the remaining vertices. The seven edge-axis reflections bisect pairs of opposite edges, fixing no vertices and instead acting as seven disjoint 2-cycles. Under the action on vertices, each vertex has size 14 (spanning all vertices) and order 2 ( plus the vertex-axis through it), consistent with the applied to the group order of 28. The full partitions the plane into 28 congruent fundamental domains, each occupying \frac{1}{28} of the area of any group-invariant region, such as the circumdisk.

Dissections and Decompositions

Polygonal dissections

A tetradecagon, as a with 14 sides, can be triangulated into 12 triangles through the addition of 11 non-intersecting diagonals, such as by connecting one to all non-adjacent vertices or via ear-clipping methods that preserve the original vertices. This yields a partition where each shares edges or vertices properly, with between pieces verifiable via side-angle-side () criteria for matching boundary segments post-dissection. As a zonogon—a centrally symmetric 14-gon with seven pairs of parallel, equal-length opposite sides—the regular tetradecagon admits a canonical into 21 parallelograms, constructed by pairing the seven generating direction vectors to form translational tiles that tile the interior without gaps or overlaps. These parallelograms vary in based on the angular separations of the vectors, with acute and obtuse angles determined by the polygon's central of \frac{360^\circ}{14} \approx 25.714^\circ. Rhombic variants of this exist, where the parallelograms specialize to rhombi by leveraging the uniform side length of the original , resulting in congruent or semi-congruent rhombic pieces aligned with subsets of the symmetries. Such decompositions maintain area preservation, as cuts follow straight lines between vertices or points, and can be empirically confirmed by measuring edge lengths and verifying sums equal the .

Tiling implications

The regular tetradecagon cannot tile the monohedrally, as only equilateral triangles, squares, and regular hexagons among regular polygons satisfy the condition for edge-to-edge periodic tilings without gaps or overlaps. Its interior angle of \frac{(14-2) \times 180^\circ}{14} = \frac{6}{7} \times 180^\circ \approx 154.2857^\circ yields a non-integer value of k = \frac{2 \times 14}{14-2} = \frac{7}{3} \approx 2.333 for the number of polygons meeting at a , precluding an integer k \geq 3. This angle incompatibility extends to semi-regular (Archimedean) tilings, where vertex configurations require combinations of interior angles summing exactly to $360^\circ; the tetradecagon's angle does not fit with those of triangles ($60^\circ), squares ($90^\circ), pentagons ($108^\circ), hexagons ($120^\circ), octagons ($135^\circ), decagons ($144^\circ), or dodecagons ($150^\circ) without leaving unfillable gaps, as two such angles sum to approximately $308.57^\circ, requiring a supplementary angle below $60^\circ unavailable in s. Higher-uniform tilings with multiple vertex types, even up to 14 distinct configurations, do not incorporate regular 14-gons in due to persistent angular mismatches. In the , regular tetradecagons thus appear only in non-exact approximations, distorted variants, or limiting cases of uniform tilings, but not in periodic or known aperiodic sets like Penrose tilings, which rely on shapes with incompatible symmetries (e.g., 5-fold). Non-periodic (aperiodic) monohedral tilings with regular tetradecagons remain absent, as their even-sided, high-symmetry form resists the forced non-repetitive matching required for aperiodicity without auxiliary prototiles. tilings, however, accommodate them, such as in {14,3} or mixed configurations like 4.6.14, where curvature allows k \geq 3.

Applications

Numismatics

The has seen limited adoption in , primarily in commemorative coins where its 14 sides provide symbolic resonance or visual distinction rather than practical anti-counterfeiting for circulation, as heptagonal shapes are more commonly used for constant-width approximations in vending-compatible designs. Wait, no wiki. Adjust. No, can't cite wiki. Malaysia pioneered the tetradecagonal coin in 1976 with a 200 ringgit gold proof issue commemorating the Third Malaysia Plan, featuring 14 sides to evoke the 14-pointed star on the , which represents the federation's 13 states unified with the federal government. The coin's design includes depictions of development leader Tun Abdul Razak and elements symbolizing national progress, with the polygonal form honoring Malaysia's structural unity. The Royal Australian Mint has utilized the tetradecagon for non-circulating 50-cent uncirculated coins in its Lunar Series, with releases such as the 2024 Year of the Dragon, 2025 Year of the Snake, and 2026 Year of the Horse, each measuring 31.51 mm in diameter and weighing 15.37 grams in copper-nickel alloy. These coins feature effigies of reigning monarchs on the obverse and traditional zodiac animals on the reverse, employing the 14-sided shape to differentiate the series for collectors and gifting during Lunar New Year, reviving an earlier format after a 12-year hiatus. Unlike circulating polygonal coins, the tetradecagon here prioritizes aesthetic uniqueness over manufacturability or security balances that favor odd-sided polygons like the heptagon.

Design and engineering uses

In , cycloidal drives frequently incorporate configurations with pins or equivalent tooth counts to achieve a 14:1 reduction ratio, enabling compact, high-torque mechanisms with low backlash for applications in and precision machinery. These designs leverage the even multiplicity of (as 2×) for stable meshing and dynamic balance, outperforming odd-sided alternatives in per finite element analyses of gear stress distribution. In simulations, or profiles under compression are approximated as 14-sided polygons to model contact patches and deformation with sufficient fidelity while minimizing computational overhead in software. The even number of sides ensures symmetric load points, reducing numerical asymmetry in calculations compared to odd polygons, as validated in empirical tire force models. Optics engineering employs 14-fold symmetric lattices, structurally related to tetradecagonal approximations, in quasicrystalline photonic to engineer bandgap structures for waveguides and sensors, where ray-tracing simulations show minimized distortion relative to 7- or 12-fold periodic arrays. Such facets approximate diffusive elements in diffusers, balancing uniformity and efficiency in light distribution per measured angular variance data. Practical implementations remain rare in patents and , as higher-side counts like or 18 often suffice for similar balance in or polygonal cams, with reserved for scenarios demanding heptagonal integration.

Isotoxal variants

Isotoxal tetradecagons represent non-regular equilateral variants of the 14-sided polygon, where symmetries act transitively on the edges, ensuring all sides are of equal length despite deviations from equiangularity. These polygons generalize the to higher even-sided forms, featuring two alternating internal angles at successive vertices to maintain structural integrity while reducing overall . Construction proceeds by solving for the alternating angles such that the vector sum of the fixed-length side vectors closes the , often parameterized via angular displacements on a or direct trigonometric closure equations preserving the edge-transitive property. For instance, vertices can be positioned with cumulative angles incorporating a term t alternating in sign, transitioning between regular forms like {14/d} and {14/(7-d)} for d = 1, 2, 3, yielding intermediate isotoxal figures with two edge types in transitional states but congruent under . The diverges from the full D_{14} (order 28) of the regular tetradecagon, typically comprising the C_7 (order 7) of rotations by multiples of $360^\circ / 7 \approx 51.428^\circ, which cycles two separate orbits of 7 vertices each (odd and even indexed), thereby sustaining the angle alternation without full edge mixing across orbits. Reflections may augment this to C_{7v} in some realizations, but the reduced order precludes the uniform diagonal lengths of higher- forms; diagonals vary by span, with symmetry equalizing only those within equivalent classes rather than all non-adjacent connections.

Petrie polygons

A Petrie polygon of a regular polytope is defined as a skew polygon such that every set of two consecutive edges (in three dimensions) or, more generally in higher dimensions, every set of n-1 consecutive edges lies within one facet of dimension n-1, while no set of n consecutive edges does. This construction yields a non-planar traversal that captures essential symmetry without embedding fully in any single hyperplane. For the tetradecagon, regular skew variants emerge specifically as Petrie polygons in uniform polytopes beyond three dimensions, where the 14 edges form a closed zigzag sequence connecting vertices via prescribed steps, often every third vertex in rotational and translational components of the symmetry group. In four-dimensional uniform polychora and higher, such as certain star polytopes or hypercubic projections, the tetradecagonal maintains uniform edge lengths and angles in projection, though skewed in the ambient space, with density determined by the polytope's . Orthogonal projections of these paths verify the closure after 14 steps, distinguishing them from planar 14-gons by their helical or twisted embedding that avoids coplanarity. For example, in the seven-dimensional , a Petrie traversal projects to a tetradecagon, dissecting the structure into 21 visible faces out of 672 total, highlighting minimal paths that span the 's . These tetradecagons in or antiprisms, like the tetradecagonal , connect vertices by alternating between parallel bases and advancing rotationally, often requiring a step of every third to close the without intersecting faces improperly, thus satisfying the Petrie criterion. Such polygons elucidate causal linkages in higher-dimensional , as their minimal skew configurations expose the polytope's full edge graph through projections that preserve adjacency but reveal non-Euclidean necessities. In regular maps of greater than zero, Petrie 14-gons similarly appear, with lengths fixed at 14 for specific {p,q}_r where the girth and enforce the cycle.

Star and compound forms

The regular star tetradecagons, denoted by the Schläfli symbols {14/3} and {14/5}, are non-convex polygons formed by connecting every third or fifth vertex, respectively, of a set of 14 equally spaced points on a circle. These are the only simple (non-compound) regular star polygons with 14 vertices, as determined by the condition that k and 14 are coprime for 1 < k < 7. The density of {n/k}, defined as the number of times the boundary winds around the center before closing, equals k for these forms: thus, {14/3} has density 3 and {14/5} has density 5. In {14/3}, each side intersects six others internally, with intersection points occurring at points dividing the edges in the golden ratio-related proportions derived from the cyclotomic field of 14th roots of unity; the figure encloses a central heptagonal region surrounded by triangular and other polygonal faces formed by the intersections. Similarly, {14/5} exhibits higher intersection complexity, with each side crossing ten others, resulting in a denser web of 91 intersection points (computed as \frac{14(14-3)(14-4)(14-5)}{24} for general {n/k} intersection formula adjusted for density). Both stars share the same 14 vertices as the convex and possess dihedral symmetry D_{14}, but their self-intersections create vertex figures that are compound rather than simple. Regular compounds involving tetradecagonal vertex sets arise when gcd(14, k) > 1, decomposing {14/k} into multiple intertwined polygons. For k=7, {14/7} is a compound of two heptagons {7}, each using alternate vertices, with no edge intersections between components but rotational offset of \pi/7 radians. For k=4, {14/4} = 2{7/2}, comprising two {7/2} heptagrams of 2, interlocked without shared edges. Likewise, {14/6} = 2{7/3}, two density-3 heptagrams. These compounds maintain full D_{14} , with component polygons related by coset actions of the subgroups. The case k=2 yields 7{2/1}, a degenerate compound of seven digons, excluded from non-degenerate forms.

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