Exploring Noble Polyhedra with the Program Stella4d
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Avenues for Polyhedral Research
Avenues for Polyhedral Research by Magnus J. Wenninger In the epilogue of my book Polyhedron Models I alluded Topologie Structurale #5, 1980 Structural Topology #5,1980 to an avenue for polyhedral research along which I myself have continued to journey, involving Ar- chimedean stellations and duals (Wenninger 1971). By way of introduction to what follows here it may be noted that the five regular convex polyhedra belong to a larger set known as uniform’ polyhedra. Their stellated forms are derived from the process of extending their R&urn6 facial planes while preserving symmetry. In particular the tetrahedron and the hexahedron have no stellated forms. The octahedron has one, the dodecahedron Cet article est le sommaire d’une etude et de three and the icosahedron a total of fifty eight (Coxeter recherches faites par I’auteur depuis une dizaine 1951). The octahedral stellation is a compound of two d’annees, impliquant les polyedres archimediens Abstract tetrahedra, classified as a uniform compound. The &oil& et les duals. La presentation en est faite a three dodecahedral stellations are non-convex regular partir d’un passe historique, et les travaux This article is a summary of investigations and solids and belong to the set of uniform polyhedra. Only d’auteurs recents sont brievement rappel& pour study done by the author over the past ten years, one icosahedral stellation is a non-convex regular la place importante qu’ils occupent dans I’etude involving Archimedean stellations and duals. The polyhedron and hence also a uniform polyhedron, but des formes polyedriques. L’auteur enonce une presentation is set into its historical background, several other icosahedral stellations are uniform com- regle &n&ale par laquelle on peut t,rouver un and the works of recent authors are briefly sket- pounds, namely the compound of five octahedra, five dual a partir de n’importe quel polyedre uniforme ched for their place in the continuing study of tetrahedra and ten tetrahedra. -
Framing Cyclic Revolutionary Emergence of Opposing Symbols of Identity Eppur Si Muove: Biomimetic Embedding of N-Tuple Helices in Spherical Polyhedra - /
Alternative view of segmented documents via Kairos 23 October 2017 | Draft Framing Cyclic Revolutionary Emergence of Opposing Symbols of Identity Eppur si muove: Biomimetic embedding of N-tuple helices in spherical polyhedra - / - Introduction Symbolic stars vs Strategic pillars; Polyhedra vs Helices; Logic vs Comprehension? Dynamic bonding patterns in n-tuple helices engendering n-fold rotating symbols Embedding the triple helix in a spherical octahedron Embedding the quadruple helix in a spherical cube Embedding the quintuple helix in a spherical dodecahedron and a Pentagramma Mirificum Embedding six-fold, eight-fold and ten-fold helices in appropriately encircled polyhedra Embedding twelve-fold, eleven-fold, nine-fold and seven-fold helices in appropriately encircled polyhedra Neglected recognition of logical patterns -- especially of opposition Dynamic relationship between polyhedra engendered by circles -- variously implying forms of unity Symbol rotation as dynamic essential to engaging with value-inversion References Introduction The contrast to the geocentric model of the solar system was framed by the Italian mathematician, physicist and philosopher Galileo Galilei (1564-1642). His much-cited phrase, " And yet it moves" (E pur si muove or Eppur si muove) was allegedly pronounced in 1633 when he was forced to recant his claims that the Earth moves around the immovable Sun rather than the converse -- known as the Galileo affair. Such a shift in perspective might usefully inspire the recognition that the stasis attributed so widely to logos and other much-valued cultural and heraldic symbols obscures the manner in which they imply a fundamental cognitive dynamic. Cultural symbols fundamental to the identity of a group might then be understood as variously moving and transforming in ways which currently elude comprehension. -
Temperature-Tuned Faceting and Shape-Changes in Liquid Alkane Droplets
Published in Langmuir 33, 1305 (2017) Temperature-tuned faceting and shape-changes in liquid alkane droplets Shani Guttman,† Zvi Sapir,†,¶ Benjamin M. Ocko,‡ Moshe Deutsch,† and Eli Sloutskin∗,† Physics Dept. and Institute of Nanotechnology, Bar-Ilan University, Ramat-Gan 5290002, Israel, and NSLS-II, Brookhaven National Laboratory, Upton NY 11973, USA E-mail: [email protected] Abstract Recent extensive studies reveal that surfactant-stabilized spherical alkane emulsion droplets spontaneously adopt polyhedral shapes upon cooling below a temperature Td, while still remaining liquid. Further cooling induces growth of tails and spontaneous droplet splitting. Two mechanisms were offered to account for these intriguing effects. One assigns the effects to the formation of an intra-droplet frame of tubules, consist- ing of crystalline rotator phases with cylindrically curved lattice planes. The second assigns the sphere-to-polyhedron transition to the buckling of defects in a crystalline interfacial monolayer, known to form in these systems at some Ts > Td. The buck- ling reduces the extensional energy of the crystalline monolayer’s defects, unavoidably formed when wrapping a spherical droplet by a hexagonally-packed interfacial mono- layer. The tail growth, shape changes, and droplet splitting were assigned to the ∗To whom correspondence should be addressed †Physics Dept. and Institute of Nanotechnology, Bar-Ilan University, Ramat-Gan 5290002, Israel ‡NSLS-II, Brookhaven National Laboratory, Upton NY 11973, USA ¶Present address: Intel (Israel) Ltd., Kiryat Gat, Israel 1 vanishing of the surface tension, γ. Here we present temperature-dependent γ(T ), optical microscopy measurements, and interfacial entropy determinations, for several alkane/surfactant combinations. We demonstrate the advantages and accuracy of the in-situ γ(T ) measurements, done simultaneously with the microscopy measurements on the same droplet. -
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. -
Order in Space
Order in space A.K. van der Vegt VSSD Other textbooks on mathematics, published by VSSD Mathematical Systems Theory, G. Olsder and J.W. van der Woude, x + 210 pp. See http://www.vssd.nl/hlf/a003.htm Numerical Methods in Scientific Computing, J. van Kan, A. Segal and F. Vermolen, xii + 279 pp. See http://www.vssd.nl/hlf/a002.htm By the author of Order in space: From Plastics to Polymers, A.K. van der Vegt, 268 pp. See http://www.vssd.nl/hlf/m028.htm © VSSD Edition on the internet, 2001 Printed edition 2006 Published by: VSSD Leeghwaterstraat 42, 2628 CA Delft, The Netherlands tel. +31 15 27 82124, telefax +31 15 27 87585, e-mail: [email protected] internet: http://www.vssd.nl/hlf URL about this book: http://www.vssd.nl/hlf/a017.htm A collection of digital pictures and/or an electronic version can be made available for lecturers who adopt this book. Please send a request by e-mail to [email protected] All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, electronic, mechanical, photo-copying, recording, or otherwise, without the prior written permission of the publisher. NUR 918 ISBN-10: 90-71301-61-3 ISBN-13: 978-90-71301-61-2 Keywords: geometry 3 PREFACE This book deals with a very old subject. Many centuries ago some people were already fascinated by polyhedra, and they spent much time in investigating regular spatial structures. In the terminology of polyhedra we, therefore, meet the names of Archimedes, Pythagoras, Plato, Kepler etc. -
Assembly of One-Patch Colloids Into Clusters Via Emulsion Droplet Evaporation
materials Article Assembly of One-Patch Colloids into Clusters via Emulsion Droplet Evaporation Hai Pham Van 1,2, Andrea Fortini 3 and Matthias Schmidt 1,* 1 Theoretische Physik II, Physikalisches Institut, Universität Bayreuth, Universitätsstraße 30, D-95440 Bayreuth, Germany 2 Department of Physics, Hanoi National University of Education, 136 Xuanthuy, Hanoi 100000, Vietnam; [email protected] 3 Department of Physics, University of Surrey, Guildford GU2 7XH, UK; [email protected] * Correspondence: [email protected]; Tel.: +49-921-55-3313 Academic Editors: Andrei V. Petukhov and Gert Jan Vroege Received: 23 February 2017; Accepted: 27 March 2017; Published: 29 March 2017 Abstract: We study the cluster structures of one-patch colloidal particles generated by droplet evaporation using Monte Carlo simulations. The addition of anisotropic patch–patch interaction between the colloids produces different cluster configurations. We find a well-defined category of sphere packing structures that minimize the second moment of mass distribution when the attractive surface coverage of the colloids c is larger than 0.3. For c < 0.3, the uniqueness of the packing structures is lost, and several different isomers are found. A further decrease of c below 0.2 leads to formation of many isomeric structures with less dense packings. Our results could provide an explanation of the occurrence of uncommon cluster configurations in the literature observed experimentally through evaporation-driven assembly. Keywords: one-patch colloid; Janus colloid; cluster; emulsion-assisted assembly; Pickering effect 1. Introduction Packings of colloidal particles in regular structures are of great interest in colloid science. One particular class of such packings is formed by colloidal clusters which can be regarded as colloidal analogues to small molecules, i.e., “colloidal molecules” [1,2]. -
DETECTION of FACES in WIRE-FRAME POLYHEDRA Interactive Modelling of Uniform Polyhedra
DETECTION OF FACES IN WIRE-FRAME POLYHEDRA Interactive Modelling of Uniform Polyhedra Hidetoshi Nonaka Hokkaido University, N14W9, Sapporo, 060 0814, Japan Keywords: Uniform polyhedron, polyhedral graph, simulated elasticity, interactive computing, recreational mathematics. Abstract: This paper presents an interactive modelling system of uniform polyhedra including regular polyhedra, semi-regular polyhedra, and intersected concave polyhedra. In our system, user can virtually “make” and “handle” them interactively. The coordinate of vertices are computed without the knowledge of faces, solids, or metric information, but only with the isomorphic graph structure. After forming a wire-frame polyhedron, the faces are detected semi-automatically through user-computer interaction. This system can be applied to recreational mathematics, computer assisted education of the graph theory, and so on. 1 INTRODUCTION 2 UNIFORM POLYHEDRA This paper presents an interactive modelling system 2.1 Platonic Solids of uniform polyhedra using simulated elasticity. Uniform polyhedra include five regular polyhedra Five Platonic solids are listed in Table 1. The (Platonic solids), thirteen semi-regular polyhedra symbol Pmn indicates that the number of faces (Archimedean solids), and four regular concave gathering around a vertex is n, and each face is m- polyhedra (Kepler-Poinsot solids). Alan Holden is describing in his writing, “The best way to learn sided regular polygon. about these objects is to make them, next best to handle them (Holden, 1971).” Traditionally, these Table 1: The list of Platonic solids. objects are made based on the shapes of faces or Symbol Polyhedron Vertices Edges Faces solids. Development figures and a set of regular polygons cut from card boards can be used to P33 Tetrahedron 4 6 4 assemble them. -
Bridges Conference Proceedings Guidelines Word
Bridges 2019 Conference Proceedings Helixation Rinus Roelofs Lansinkweg 28, Hengelo, the Netherlands; [email protected] Abstract In the list of names of the regular and semi-regular polyhedra we find many names that refer to a process. Examples are ‘truncated’ cube and ‘stellated’ dodecahedron. And Luca Pacioli named some of his polyhedral objects ‘elevations’. This kind of name-giving makes it easier to understand these polyhedra. We can imagine the model as a result of a transformation. And nowadays we are able to visualize this process by using the technique of animation. Here I will to introduce ‘helixation’ as a process to get a better understanding of the Poinsot polyhedra. In this paper I will limit myself to uniform polyhedra. Introduction Most of the Archimedean solids can be derived by cutting away parts of a Platonic solid. This operation , with which we can generate most of the semi-regular solids, is called truncation. Figure 1: Truncation of the cube. We can truncate the vertices of a polyhedron until the original faces of the polyhedron become regular again. In Figure 1 this process is shown starting with a cube. In the third object in the row, the vertices are truncated in such a way that the square faces of the cube are transformed to regular octagons. The resulting object is the Archimedean solid, the truncated cube. We can continue the process until we reach the fifth object in the row, which again is an Archimedean solid, the cuboctahedron. The whole process or can be represented as an animation. Also elevation and stellation can be described as processes. -
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. -
Regulating the Distortion Degree of the Square Antiprism Coordination
Electronic Supplementary Material (ESI) for CrystEngComm. This journal is © The Royal Society of Chemistry 2021 Electronic Supplementary Information (ESI) for CrystEngComm Regulating the Distortion Degree of the Square Antiprism Coordination Geometry in the Dy-Na Single Ion Magnets Hui-Sheng Wang,*a Ke Zhang,a Jia Wang,b Zhaobo Hu,b You Song,*b Zaichao Zhang,c and Zhi-Quan Pana aSchool of Chemistry and Environmental Engineering, Key Laboratory of Green Chemical Process of Ministry of Education, Key Laboratory of Novel Reactor and Green Chemical Technology of Hubei Province, Wuhan Institute of Technology, Wuhan 430205, P. R. China. bState Key Laboratory of Coordinate Chemistry, Nanjing National Laboratory of Microstructures, School of Chemistry and Chemical Engineering, Nanjing University, Nanjing 210023, P. R. China. cJiangsu Key Laboratory for the Chemistry of Low-dimensional Materials, School of Chemistry and Chemical Engineering, Huaiyin Normal University, P. R. China. *Email: [email protected] (H.-S. W.). *Email: [email protected] (Y. S.) -S1- Contents Table S1. Crystal data and structure refinement parameters for complexes 1-2. Table S2. Selected bond lengths (Å) and angles (°) for 1. Table S3. Selected bond lengths (Å) and angles (°) for 2. Table S4. The possible geometries of octa-coordination metal centers and Deviation parameters from each ideal polyhedron for Dy in complex 1. Table S5. The possible geometries of octa-coordination metal centers and Deviation parameters from each ideal polyhedron for Dy in complex 2. Table S6. The details for parameters involved in SAP geometry for 1 and 2. Table S7. Best fitted parameters obtained for the extended Debye model with ac susceptibility data from SQUID magnetometer of compound 1 under a 1000 Oe dc applied field. -
This Is a Set of Activities Using Both Isosceles and Equilateral Triangles
This is a set of activities using both Isosceles and Equilateral Triangles. 3D tasks Technical information This pack includes 25 Equilateral Triangles and 25 Isosceles Triangles. You will also need a small tube of Copydex. If you are new to making models with Copydex we suggest you start by watching www.atm.org.uk/Using-ATM-MATs Different polyhedra to make Kit A: 4 Equilateral Triangle MATs. Place one triangle on your desk and join the other three triangles to its three sides, symmetrically. Now add glue to one edge of each of the three added triangles so that all can be joined into a polyhedron This is your first polyhedron. Kit B: 3 Isosceles triangles and 1 equilateral triangle Kit C: 4 Isosceles triangles Kit D: 6 Equilateral Triangles Kit E: 6 Isosceles Triangles Kit F: 3 Equilateral and 3 Isosceles Triangles. (are there different possible polyhedra this time?) Kit G: 8 Equilateral Triangles. One possibility is a Regular Octahedron, but is there more than one Octahedron? Kit H: 4 Equilateral and 4 Isosceles Triangles (are there different possible polyhedra this time?) Kit I: 2 Equilateral Triangles and 6 Isosceles Triangles Kit J: Go back to the Regular Octahedron (from Kit G) and add a Regular Tetrahedron to one of its faces, then add another … until four have been added. Keep track (in a table) of how many faces and vertices the Regular Octahedron and the next four polyhedra have. Hint: if you spaced the added Tetrahedra equally around the Octahedron you will find a bigger version of a previously made solid.