A Closer Look at Jamnitzer's Polyhedra
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BY S. RAMASESHAN Number of Diffaent Kinds of Planes Permitted By
BY S. RAMASESHAN (From thy Department ef Physics, Indian Institute of Science, Bangalore) Received for publication June 20, 1916 (Communicated by Sir C. V. Raman, ~t.,F. R.s., N.L.) number of diffaent kinds of planes permitted by the law of rational indices to appear as faces on a crystal is practically unlimited. The number of "forms " actually observed, however, is limited and there is a decided preference for a few amongst them. This is one of the most striking facts of geometric crystallography and its explanation is obviously of importance. Pierre Curie (1885) stressed the role played by the surface energy of the faces in determining the " forms " of the crystal. According to him, the different faces of a crystal have different surface energies and the form of the crystal as a whole is determined by the condition that the total surface energy of the crystal should be a minimum. According to W. Gibbs (1877), on the other hand, it is the velocity of growth in different directions which is the determining factor, while the surface energy of the crystal plays a subordi- nate role and is only effective in the case of crystals of submicroscopic size, We have little direct knowledge as to how diamond is actually formed in nature. It is necessary, therefore, to rely upon the indications furnished by the observed forms of the crystals. One of the most remarkable facts about diamond is the curvature of the faces which is a very common and marked feature. This is particularly noticeable in the case of the diamonds found in the State of Panna in Central India. -
Arxiv:1705.01294V1
Branes and Polytopes Luca Romano email address: [email protected] ABSTRACT We investigate the hierarchies of half-supersymmetric branes in maximal supergravity theories. By studying the action of the Weyl group of the U-duality group of maximal supergravities we discover a set of universal algebraic rules describing the number of independent 1/2-BPS p-branes, rank by rank, in any dimension. We show that these relations describe the symmetries of certain families of uniform polytopes. This induces a correspondence between half-supersymmetric branes and vertices of opportune uniform polytopes. We show that half-supersymmetric 0-, 1- and 2-branes are in correspondence with the vertices of the k21, 2k1 and 1k2 families of uniform polytopes, respectively, while 3-branes correspond to the vertices of the rectified version of the 2k1 family. For 4-branes and higher rank solutions we find a general behavior. The interpretation of half- supersymmetric solutions as vertices of uniform polytopes reveals some intriguing aspects. One of the most relevant is a triality relation between 0-, 1- and 2-branes. arXiv:1705.01294v1 [hep-th] 3 May 2017 Contents Introduction 2 1 Coxeter Group and Weyl Group 3 1.1 WeylGroup........................................ 6 2 Branes in E11 7 3 Algebraic Structures Behind Half-Supersymmetric Branes 12 4 Branes ad Polytopes 15 Conclusions 27 A Polytopes 30 B Petrie Polygons 30 1 Introduction Since their discovery branes gained a prominent role in the analysis of M-theories and du- alities [1]. One of the most important class of branes consists in Dirichlet branes, or D-branes. D-branes appear in string theory as boundary terms for open strings with mixed Dirichlet-Neumann boundary conditions and, due to their tension, scaling with a negative power of the string cou- pling constant, they are non-perturbative objects [2]. -
The Crystal Forms of Diamond and Their Significance
THE CRYSTAL FORMS OF DIAMOND AND THEIR SIGNIFICANCE BY SIR C. V. RAMAN AND S. RAMASESHAN (From the Department of Physics, Indian Institute of Science, Bangalore) Received for publication, June 4, 1946 CONTENTS 1. Introductory Statement. 2. General Descriptive Characters. 3~ Some Theoretical Considerations. 4. Geometric Preliminaries. 5. The Configuration of the Edges. 6. The Crystal Symmetry of Diamond. 7. Classification of the Crystal Forros. 8. The Haidinger Diamond. 9. The Triangular Twins. 10. Some Descriptive Notes. 11. The Allo- tropic Modifications of Diamond. 12. Summary. References. Plates. 1. ~NTRODUCTORY STATEMENT THE" crystallography of diamond presents problems of peculiar interest and difficulty. The material as found is usually in the form of complete crystals bounded on all sides by their natural faces, but strangely enough, these faces generally exhibit a marked curvature. The diamonds found in the State of Panna in Central India, for example, are invariably of this kind. Other diamondsJas for example a group of specimens recently acquired for our studies ffom Hyderabad (Deccan)--show both plane and curved faces in combination. Even those diamonds which at first sight seem to resemble the standard forms of geometric crystallography, such as the rhombic dodeca- hedron or the octahedron, are found on scrutiny to exhibit features which preclude such an identification. This is the case, for example, witb. the South African diamonds presented to us for the purpose of these studŸ by the De Beers Mining Corporation of Kimberley. From these facts it is evident that the crystallography of diamond stands in a class by itself apart from that of other substances and needs to be approached from a distinctive stand- point. -
Uniform Panoploid Tetracombs
Uniform Panoploid Tetracombs George Olshevsky TETRACOMB is a four-dimensional tessellation. In any tessellation, the honeycells, which are the n-dimensional polytopes that tessellate the space, Amust by definition adjoin precisely along their facets, that is, their ( n!1)- dimensional elements, so that each facet belongs to exactly two honeycells. In the case of tetracombs, the honeycells are four-dimensional polytopes, or polychora, and their facets are polyhedra. For a tessellation to be uniform, the honeycells must all be uniform polytopes, and the vertices must be transitive on the symmetry group of the tessellation. Loosely speaking, therefore, the vertices must be “surrounded all alike” by the honeycells that meet there. If a tessellation is such that every point of its space not on a boundary between honeycells lies in the interior of exactly one honeycell, then it is panoploid. If one or more points of the space not on a boundary between honeycells lie inside more than one honeycell, the tessellation is polyploid. Tessellations may also be constructed that have “holes,” that is, regions that lie inside none of the honeycells; such tessellations are called holeycombs. It is possible for a polyploid tessellation to also be a holeycomb, but not for a panoploid tessellation, which must fill the entire space exactly once. Polyploid tessellations are also called starcombs or star-tessellations. Holeycombs usually arise when (n!1)-dimensional tessellations are themselves permitted to be honeycells; these take up the otherwise free facets that bound the “holes,” so that all the facets continue to belong to two honeycells. In this essay, as per its title, we are concerned with just the uniform panoploid tetracombs. -
Convex Polytopes and Tilings with Few Flag Orbits
Convex Polytopes and Tilings with Few Flag Orbits by Nicholas Matteo B.A. in Mathematics, Miami University M.A. in Mathematics, Miami University A dissertation submitted to The Faculty of the College of Science of Northeastern University in partial fulfillment of the requirements for the degree of Doctor of Philosophy April 14, 2015 Dissertation directed by Egon Schulte Professor of Mathematics Abstract of Dissertation The amount of symmetry possessed by a convex polytope, or a tiling by convex polytopes, is reflected by the number of orbits of its flags under the action of the Euclidean isometries preserving the polytope. The convex polytopes with only one flag orbit have been classified since the work of Schläfli in the 19th century. In this dissertation, convex polytopes with up to three flag orbits are classified. Two-orbit convex polytopes exist only in two or three dimensions, and the only ones whose combinatorial automorphism group is also two-orbit are the cuboctahedron, the icosidodecahedron, the rhombic dodecahedron, and the rhombic triacontahedron. Two-orbit face-to-face tilings by convex polytopes exist on E1, E2, and E3; the only ones which are also combinatorially two-orbit are the trihexagonal plane tiling, the rhombille plane tiling, the tetrahedral-octahedral honeycomb, and the rhombic dodecahedral honeycomb. Moreover, any combinatorially two-orbit convex polytope or tiling is isomorphic to one on the above list. Three-orbit convex polytopes exist in two through eight dimensions. There are infinitely many in three dimensions, including prisms over regular polygons, truncated Platonic solids, and their dual bipyramids and Kleetopes. There are infinitely many in four dimensions, comprising the rectified regular 4-polytopes, the p; p-duoprisms, the bitruncated 4-simplex, the bitruncated 24-cell, and their duals. -
[ENTRY POLYHEDRA] Authors: Oliver Knill: December 2000 Source: Translated Into This Format from Data Given In
ENTRY POLYHEDRA [ENTRY POLYHEDRA] Authors: Oliver Knill: December 2000 Source: Translated into this format from data given in http://netlib.bell-labs.com/netlib tetrahedron The [tetrahedron] is a polyhedron with 4 vertices and 4 faces. The dual polyhedron is called tetrahedron. cube The [cube] is a polyhedron with 8 vertices and 6 faces. The dual polyhedron is called octahedron. hexahedron The [hexahedron] is a polyhedron with 8 vertices and 6 faces. The dual polyhedron is called octahedron. octahedron The [octahedron] is a polyhedron with 6 vertices and 8 faces. The dual polyhedron is called cube. dodecahedron The [dodecahedron] is a polyhedron with 20 vertices and 12 faces. The dual polyhedron is called icosahedron. icosahedron The [icosahedron] is a polyhedron with 12 vertices and 20 faces. The dual polyhedron is called dodecahedron. small stellated dodecahedron The [small stellated dodecahedron] is a polyhedron with 12 vertices and 12 faces. The dual polyhedron is called great dodecahedron. great dodecahedron The [great dodecahedron] is a polyhedron with 12 vertices and 12 faces. The dual polyhedron is called small stellated dodecahedron. great stellated dodecahedron The [great stellated dodecahedron] is a polyhedron with 20 vertices and 12 faces. The dual polyhedron is called great icosahedron. great icosahedron The [great icosahedron] is a polyhedron with 12 vertices and 20 faces. The dual polyhedron is called great stellated dodecahedron. truncated tetrahedron The [truncated tetrahedron] is a polyhedron with 12 vertices and 8 faces. The dual polyhedron is called triakis tetrahedron. cuboctahedron The [cuboctahedron] is a polyhedron with 12 vertices and 14 faces. The dual polyhedron is called rhombic dodecahedron. -
A General Method for Building Topological Models of Polyhedra
Bridges 2017 Conference Proceedings A General Method for Building Topological Models of Polyhedra Mircea Draghicescu ITSPHUN LLC [email protected] Abstract We show how to build 3D topological models of arbitrary convex polyhedra by connecting same-shape pieces. We also show that many well-known tensegrity structures can be obtained as particular instances of this method. We illustrate the method with examples of models made of a variety of materials. Introduction We focus here on building, in a modular fashion, “topological” polyhedra models that preserve the con- nectivity properties between the vertices, faces, and edges, but not the spatial characteristics such as length and angles. We show that all convex polyhedra can be modeled using a single type of construction element (representing a polyhedron edge) and a single type of connection between these elements.1 In the remainder of the paper we introduce the construction elements, describe the models that can be built with them, and then show how these elements can be replaced with simpler, linear shapes that generate both woven-style models and tensegrity structures. In the last section we show how to modify the construction elements to bring the built objects closer to the modeled polyhedra. George Hart pioneered modular constructions using multiple copies of a single shape (see for example [2]); many of his amazing creations fit into the paradigm described here. The sculptures described in [4] can also be derived from our method. Some of the ideas presented here were first introduced in [1]. A Construction Element with Four Connection Points We restrict the presentation to convex polyhedra; to avoid repetition, “polyhedron” will mean from now on “convex polyhedron”. -
Visualizing the Polychora with Hyperbolic Patchwork
Bridges 2017 Conference Proceedings Crooked Houses: Visualizing the Polychora with Hyperbolic Patchwork Taneli Luotoniemi Dept. of Art, School of Arts, Design and Architecture, Aalto University Hämeentie 135 C, 00560 Helsinki, FINLAND [email protected] Abstract This paper presents kinetic models based on the 4-dimensional regular polytopes. The sequential ‘flattening’ is realized through the use of hyperbolic patchwork surfaces, which portray the bitruncated versions of the polychora. As pedagogical tools, these models offer a hands-on experience of 4D geometry. Introduction Four-dimensional space (hyperspace, 4-space) is the result of adding an extra spatial dimension perpendicular to our three dimensions of length, height and width. The research on its properties is made possible by generalizing the geometric principles acquired by studying more familiar spaces of lower dimensions. Originated in philosophy and mathematically formulated in geometry, the concept has roused interpretations in mysticism, in theoretical physics, in fiction and in visual arts. Lately the availability of digital visualization technologies has given artists a chance to study higher space with a greater fidelity to the precise geometry of the concept. Because the fourth dimension of space cannot be directly portrayed in our physical world, the focus of many inquiries into the subject has been on the challenge of developing a visual understanding of 4-dimensional reality. Luckily, just as 3-dimensional structures can be drawn, unfolded, sliced, photographed or otherwise projected onto a 2-dimensional medium like paper or a computer screen, these graphical techniques can be generalized to produce 3D models of 4-dimensional structures described by mathematicians. The precise subject matter of these visualizations is usually the family of regular polychora – 4-dimensional counterparts of the Platonic solids. -
Spectral Realizations of Graphs
SPECTRAL REALIZATIONS OF GRAPHS B. D. S. \DON" MCCONNELL 1. Introduction 2 The boundary of the regular hexagon in R and the vertex-and-edge skeleton of the regular tetrahe- 3 dron in R , as geometric realizations of the combinatorial 6-cycle and complete graph on 4 vertices, exhibit a significant property: Each automorphism of the graph induces a \rigid" isometry of the figure. We call such a figure harmonious.1 Figure 1. A pair of harmonious graph realizations (assuming the latter in 3D). Harmonious realizations can have considerable value as aids to the intuitive understanding of the graph's structure, but such realizations are generally elusive. This note explains and explores a proposition that provides a straightforward way to generate an entire family of harmonious realizations of any graph: A matrix whose rows form an orthogonal basis of an eigenspace of a graph's adjacency matrix has columns that serve as coordinate vectors of the vertices of an harmonious realization of the graph. This is a (projection of a) spectral realization. The hundreds of diagrams in Section 42 illustrate that spectral realizations of graphs with a high degree of symmetry can have great visual appeal. Or, not: they may exist in arbitrarily-high- dimensional spaces, or they may appear as an uninspiring jumble of points in one-dimensional space. In most cases, they collapse vertices and even edges into single points, and are therefore only very rarely faithful. Nevertheless, spectral realizations can often provide useful starting points for visualization efforts. (A basic Mathematica recipe for computing (projected) spectral realizations appears at the end of Section 3.) Not every harmonious realization of a graph is spectral. -
A Frustrated, Centred Tetrakis Hexahedron†
ChemComm View Article Online COMMUNICATION View Journal | View Issue [Fe15]: a frustrated, centred tetrakis hexahedron† a a a b Cite this: Chem. Commun., 2021, Daniel J. Cutler, Mukesh K. Singh, Gary S. Nichol, Marco Evangelisti, c d a 57, 8925 Ju¨rgen Schnack, * Leroy Cronin * and Euan K. Brechin * Received 20th July 2021, Accepted 9th August 2021 DOI: 10.1039/d1cc03919a rsc.li/chemcomm The combination of two different FeIII salts in a solvothermal anomalous magnetisation behaviour in an applied magnetic reaction with triethanolamine results in the formation of a high field.8 III symmetry [Fe15] cluster whose structure conforms to a centred, One synthetic methodology proven to enable the construc- tetrakis hexahedron. tion of such species is hydro/solvothermal synthesis, which Creative Commons Attribution 3.0 Unported Licence. typically exploits superheating reaction solutions under auto- Homometallic compounds of FeIII have played a central role in the genous pressure.9 In the chemistry of polynuclear cluster history of molecular magnetism, proving key to the development compounds of paramagnetic transition metal ions, the tem- and understanding of an array of physical properties. For exam- perature regimes employed (which are typically below 250 1C) ple, the study of oxo-bridged [Fe2] dimers allowed the develop- can lead to enhanced solubility, reduced solvent viscosity and ment of detailed magneto-structural correlations that can increased reagent diffusion. The result is often the synthesis of be translated to larger species,1 antiferromagnetically coupled metastable kinetic products of high symmetry, with slow cool- [Fe6–12] ferric wheels revealed interesting quantum size effects ing enabling pristine crystal growth directly from the reaction 2 10 manifested in stepped magnetisation, [Fe17/19] was an early mixture. -
One Shape to Make Them All
Bridges Finland Conference Proceedings Dual Models: One Shape to Make Them All Mircea Draghicescu ITSPHUN LLC [email protected] Abstract We show how a potentially infinite number of 3D decorative objects can be built by connecting copies of a single geometric element made of a flexible material. Each object is an approximate model of a compound of some polyhe- dron and its dual. We present the underlying geometry and show a few such constructs. The geometric element used in the constructions can be made from a variety of materials and can have many shapes that give different artistic effects. In the workshop, we will build a few models that the participants can take home. Introduction Wireframe models of polyhedra can be built by connecting linear elements that represent polyhedral edges. We describe here a different modeling method where each atomic construction element represents not an edge, but a pair of edges, one belonging to some polyhedron P and the other one to P 0, the dual of P ; the resulting object is a model of the compound of P and P 0. Using the same number of construction elements as the number of edges of P and P 0, the model of the compound exhibits a richer structure and, due to the additional connections, is stronger than the models of P and P 0 alone. The model has at least the symmetry of P and P 0, and can have a higher symmetry if P is self-dual. The construction process challenges the maker to think simultaneously of both P and P 0 and can be used as a teaching aid in the study of polyhedra and duality. -
A Small Closed Convex Projective 4-Manifold Via Dehn Filling Gye-Seon Lee, Ludovic Marquis, Stefano Riolo
A small closed convex projective 4-manifold via Dehn filling Gye-Seon Lee, Ludovic Marquis, Stefano Riolo To cite this version: Gye-Seon Lee, Ludovic Marquis, Stefano Riolo. A small closed convex projective 4-manifold via Dehn filling. 2021. hal-02334154v3 HAL Id: hal-02334154 https://hal.archives-ouvertes.fr/hal-02334154v3 Preprint submitted on 9 Apr 2021 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. A SMALL CLOSED CONVEX PROJECTIVE 4-MANIFOLD VIA DEHN FILLING GYE-SEON LEE, LUDOVIC MARQUIS, AND STEFANO RIOLO ABSTRACT. In order to obtain a closed orientable convex projective four-manifold with small positive Euler characteristic, we build an explicit example of convex projective Dehn filling of a cusped hyperbolic four-manifold through a continuous path of projective cone- manifolds. 1. INTRODUCTION Convex projective manifolds form an interesting class of aspherical manifolds, includ- ing complete hyperbolic manifolds. We refer to [Ben08, Mar14, CLM18] and [Mar18] for surveys on convex projective manifolds and hyperbolic 4-manifolds, respectively. This class of geometric manifolds has been studied notably in the context of deformations of geometric structures on manifolds or orbifolds (see the survey [CLM18] and the refer- ences therein), or for its link to dynamical systems through the notion of Anosov repre- sentation [Ben04, DGK18, DGK17] (see [Lab06, GW12] for the notion of Anosov repre- sentation).