Great dodecicosacron: Difference between revisions
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== Proportions== |
== Proportions== |
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Each face has two angles of <math>\arccos(\frac{3}{4}+\frac{1}{20}\sqrt{5})\approx 30.480\,324\,565\,36^{\circ}</math> and two angles of <math>\arccos(-\frac{5}{12}+\frac{1}{4}\sqrt{5})\approx 81.816\,127\,508\,183^{\circ}</math>. The diagonals of each antiparallelogram intersect at an angle of <math>\arccos(\frac{5}{12}-\frac{1}{60}\sqrt{5})\approx 67.703\,547\,926\,46^{\circ}</math>. The [[dihedral angle]] equals <math>\arccos(\frac{-44+3\sqrt{5}}{61})\approx 127.686\,523\,427\,48^{\circ}</math>. The ratio between the lengths of the long edges and the short ones equals <math>\frac{1} |
Each face has two angles of <math>\arccos(\frac{3}{4}+\frac{1}{20}\sqrt{5})\approx 30.480\,324\,565\,36^{\circ}</math> and two angles of <math>\arccos(-\frac{5}{12}+\frac{1}{4}\sqrt{5})\approx 81.816\,127\,508\,183^{\circ}</math>. The diagonals of each antiparallelogram intersect at an angle of <math>\arccos(\frac{5}{12}-\frac{1}{60}\sqrt{5})\approx 67.703\,547\,926\,46^{\circ}</math>. The [[dihedral angle]] equals <math>\arccos(\frac{-44+3\sqrt{5}}{61})\approx 127.686\,523\,427\,48^{\circ}</math>. The ratio between the lengths of the long edges and the short ones equals <math>\frac{1}{2}+\frac{1}{2}\sqrt{5}</math>, which is the [[golden ratio]]. Part of each face lies inside the solid, hence is invisible in solid models. |
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==References== |
==References== |
Revision as of 11:27, 15 July 2020
Great dodecicosacron | |
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Type | Star polyhedron |
Face | |
Elements | F = 60, E = 120 V = 32 (χ = −28) |
Symmetry group | Ih, [5,3], *532 |
Index references | DU63 |
dual polyhedron | Great dodecicosahedron |
In geometry, the great dodecicosacron (or great dipteral trisicosahedron) is the dual of the great dodecicosahedron (U63). It has 60 intersecting bow-tie-shaped faces.
Proportions
Each face has two angles of and two angles of . The diagonals of each antiparallelogram intersect at an angle of . The dihedral angle equals . The ratio between the lengths of the long edges and the short ones equals , which is the golden ratio. Part of each face lies inside the solid, hence is invisible in solid models.
References
- Wenninger, Magnus (1983), Dual Models, Cambridge University Press, ISBN 978-0-521-54325-5, MR 0730208