Tying the Knot: Applications of Topology to Chemistry
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Chirality in the Plane
Chirality in the plane Christian G. B¨ohmer1 and Yongjo Lee2 and Patrizio Neff3 October 15, 2019 Abstract It is well-known that many three-dimensional chiral material models become non-chiral when reduced to two dimensions. Chiral properties of the two-dimensional model can then be restored by adding appropriate two-dimensional chiral terms. In this paper we show how to construct a three-dimensional chiral energy function which can achieve two-dimensional chirality induced already by a chiral three-dimensional model. The key ingredient to this approach is the consideration of a nonlinear chiral energy containing only rotational parts. After formulating an appropriate energy functional, we study the equations of motion and find explicit soliton solutions displaying two-dimensional chiral properties. Keywords: chiral materials, planar models, Cosserat continuum, isotropy, hemitropy, centro- symmetry AMS 2010 subject classification: 74J35, 74A35, 74J30, 74A30 1 Introduction 1.1 Background A group of geometric symmetries which keeps at least one point fixed is called a point group. A point group in d-dimensional Euclidean space is a subgroup of the orthogonal group O(d). Naturally this leads to the distinction of rotations and improper rotations. Centrosymmetry corresponds to a point group which contains an inversion centre as one of its symmetry elements. Chiral symmetry is one example of non-centrosymmetry which is characterised by the fact that a geometric figure cannot be mapped into its mirror image by an element of the Euclidean group, proper rotations SO(d) and translations. This non-superimposability (or chirality) to its mirror image is best illustrated by the left and right hands: there is no way to map the left hand onto the right by simply rotating the left hand in the plane. -
Chirality and Projective Linear Groups
DISCRETE MATHEMATICS Discrete Mathematics 131 (1994) 221-261 Chirality and projective linear groups Egon Schultea,l, Asia IviC Weissb**,’ “Depurtment qf Mathematics, Northeastern Uniwrsity, Boston, MA 02115, USA bDepartment qf Mathematics and Statistics, York University, North York, Ontario, M3JIP3, Camda Received 24 October 1991; revised 14 September 1992 Abstract In recent years the term ‘chiral’ has been used for geometric and combinatorial figures which are symmetrical by rotation but not by reflection. The correspondence of groups and polytopes is used to construct infinite series of chiral and regular polytopes whose facets or vertex-figures are chiral or regular toroidal maps. In particular, the groups PSL,(Z,) are used to construct chiral polytopes, while PSL,(Z,[I]) and PSL,(Z,[w]) are used to construct regular polytopes. 1. Introduction Abstract polytopes are combinatorial structures that generalize the classical poly- topes. We are particularly interested in those that possess a high degree of symmetry. In this section, we briefly outline some definitions and basic results from the theory of abstract polytopes. For details we refer to [9,22,25,27]. An (abstract) polytope 9 ofrank n, or an n-polytope, is a partially ordered set with a strictly monotone rank function rank( .) with range { - 1, 0, . , n}. The elements of 9 with rankj are called j-faces of 8. The maximal chains (totally ordered subsets) of .P are calledJags. We require that 6P have a smallest (- 1)-face F_ 1, a greatest n-face F,, and that each flag contains exactly n+2 faces. Furthermore, we require that .Y be strongly flag-connected and that .P have the following homogeneity property: when- ever F<G, rank(F)=j- 1 and rank(G)=j+l, then there are exactly two j-faces H with FcH-cG. -
Intuitive Chemical Topology Concepts. / In
1 Intuitive Chemical Topology Concepts Eugene V. Babaev Moscow State University, Moscow 119899, RUSSIA 1. Introduction During last two decades, chemistry underwent a strong influence from nonroutine mathematical methods. Chemical applications of graph theory [1–10], topology [11–18], and related fields of fundamental mathematics [21–27] are growing rapidly. This trend may indicate the birth of a novel interdisciplinary field, mathematical chemistry, imperceptibly flourishing on the border of chemistry and pure mathematics. The term “chemical topology” (the title of this volume) has become frequent in papers, books, and scientific conferences. Similarly, the term molecular topology (differing in its sense from molecular geometry) has become frequently used, although there may exist diverse viewpoints on the meaning of this concept. The key difference between topology and geometry is that in geometry the concepts of distances and angles are important, whereas in topology they are not. Instead, the essential topological properties are connectedness and continuity. Chemical structural formulas are good examples of topological models of molecules: the pattern of connectivity between atoms is essential, whereas the interatomic distances and angles are less important and may be neglected. A colloquial definition of topology is “rubber” geometry. Indeed, one may consider a topological object made of an ideal elastic material, so that any deformation (like stretching or distortion) retains points of this elastic object “close enough” one to another. In contrast, cutting separates previously close points, and any joining of parts makes points “closer” one to another. Such a continuous transformation of an object without cutting and joining any parts is called homeomorphism. (The term should not be confused with homomorphism.) The study of properties that are invariant to homeomorphic transformations is the fundamental goal of topology. -
From Chemical Topology to Molecular Machines Nobel Lecture, December 8, 2016 by Jean-Pierre Sauvage University of Strasbourg, Strasbourg, France
From Chemical Topology to Molecular Machines Nobel Lecture, December 8, 2016 by Jean-Pierre Sauvage University of Strasbourg, Strasbourg, France. o a large extent, the eld of “molecular machines” started aer several groups T were able to prepare reasonably easily interlocking ring compounds (named catenanes for compounds consisting of interlocking rings and rotaxanes for rings threaded by molecular laments or axes). Important families of molecular machines not belonging to the interlocking world were also designed, prepared and studied but, for most of them, their elaboration was more recent than that of catenanes or rotaxanes. Since the creation of interlocking ring molecules is so important in relation to the molecular machinery area, we will start with this aspect of our work. e second part will naturally be devoted to the dynamic properties of such systems and to the compounds for which motions can be directed in a controlled manner from the outside, i.e., molecular machines. We will restrict our discussion to a very limited number of examples which we con- sider particularly representative of the eld. CHEMICAL TOPOLOGY Generally speaking, chemical topology refers to molecules whose graph (i.e., their representation based on atoms and bonds) is non-planar [1–2]. A planar graph cannot be represented in a plane or on a sheet of paper without crossing points. In topology, the object can be distorted as much as one likes but its topo- logical properties are not modied as long as no cleavage occurs [3]. In other 111 112 The Nobel Prizes words, a circle and an ellipse are topologically identical. -
Chiral Icosahedral Hinge Elastegrity's Geometry of Motion
Chiral Icosahedral Hinge Elastegrity’s Geometry of Motion Eleftherios Pavlides, PhD AIA Roger Williams University1, Peter Fauci, Roger Williams University [email protected] 401 662 7521 Introduction Hinge Elastegrity, Definitions and Transformations Presented at G4G12 2a. 2 pairs 2b. 3 orthogonal H H 3.b 2 hypotenuse elastic of moving isosceles triangle faces hinges link each of 2 triangles for each of 8 irregular tetrahedra frame each tetrahedra 3c. isosceles leg elastic of 6 gates 3.a 4 free isosceles legss hinging pairs of right Fig.1 (left) edges per gate (6 gates) triangles forming 6-strut s 12 springs 24-cable Fig.2 Chiral Icosahedral nodal Hinge elastegrity rigid & Fig.3 Chiral Icosahedral tensegrity moving parts Hinge elastegrity rigid & hinges & gate edges The object that gave rise to the math in this paper is “hinge elastegrities”, a class of structures that originally arose from two Bauhaus exercises assigned at the Yale School of Architecture in the 1970’s and investigated in a series of art projects. The key new object obtained in 1982 involved cutting slits into folded pieces of paper and weaving them into 8 irregular tetrahedra, each with 3 isosceles right-triangle faces outlining an equilateral face fig.2b The 8 tetrahedra are suspended with 12 pairs of moving isosceles-right-triangles, congruent to the tetrahedral face right triangles fig.2a giving rise to an icosahedral shape (not necessarily regular) fig.2. Each pair of right triangles is attached to each other with an elastic hinge, along one of its isosceles legs fig.2a that act as springs. -
Symmetry and Chirality in Discrete Structures
Symmetry and chirality in discrete structures Marston Conder University of Auckland, New Zealamd UW Math Day, Seattle, March 2013 Where is New Zealand? What is New Zealand famous for? • Great place to live (South Pacific) • Multi-cultural (European, Maori/Polynesian, Asian ...) • Beautiful scenery (beaches, volcanoes, lakes, mountains) • Kiwis (strange little birds), kiwi fruit (strange little fruit) • Dairy produce (milk, butter, cheese, etc.) • Film sites (Lord of the Rings, The Hobbit, Narnia, etc.) • Rugby football • Extreme sports (bungy-jumping, white-water rafting, etc.) What is symmetry? Symmetry can mean many different things, such as balance, uniform proportion, harmony, or congruence Generally, an object has symmetry if it can be transformed in way that leaves it looking the same as it did originally. Symmetry can be reflective: ... or rotational: ... or translational: ... or a combination of these types Examples of these kinds of symmetry abound in nature ... but have also been manufactured by human fascination and enterprise e.g. the Platonic solids (c. 360BC) or earlier ... the `Neolithic Scots' (c. 2000BC) ... as publicised by Atiyah and Sutcliffe (2003) ... but unfortunately a hoax! The claim that the Scots knew about these five regular solids over 1000 years before Plato was based on the above five `Scottish stones' at the Ashmolean Museum in Oxford | but one has 14 faces, and none of them is an icosahedron [See John Baez's website for the full story] Tilings at the Alhambra Palace { on its walls, floors, ceilings, and even some of the furniture { amazingly exhibit all of the 17 \wallpaper symmetries" (in two dimensions) [Rafael P´erezG´omezand Jos´eMara Montesinos, 1980s] Symmetry can induce strength and stability: .. -
On the Study of Chirality of Knots Through Polynomial Invariants
Treball final de grau GRAU DE MATEMÀTIQUES Facultat de Matemàtiques i Informàtica Universitat de Barcelona KNOT THEORY: On the study of chirality of knots through polynomial invariants Autor: Sergi Justiniano Claramunt Director: Dr. Javier José Gutiérrez Marín Realitzat a: Departament de Matemàtiques i Informàtica Barcelona, January 18, 2019 Contents Abstract ii Introduction iii 1 Mathematical bases 1 1.1 Definition of a knot . .1 1.2 Equivalence of knots . .4 1.3 Knot projections and diagrams . .6 1.4 Reidemeister moves . .8 1.5 Invariants . .9 1.6 Symmetries, properties and generation of knots . 11 1.7 Tangles and Conway notation . 12 2 Jones Polynomial 15 2.1 Introduction . 15 2.2 Rules of bracket polynomial . 16 2.3 Writhe and invariance of Jones polynomial . 18 2.4 Main theorems and applications . 22 3 HOMFLY and Kauffman polynomials on chirality detection 25 3.1 HOMFLY polynomial . 25 3.2 Kauffman polynomial . 28 3.3 Testing chirality . 31 4 Conclusions 33 Bibliography 35 i Abstract In this project we introduce the theory of knots and specialize in the compu- tation of the knot polynomials. After presenting the Jones polynomial, its two two-variable generalizations are also introduced: the Kauffman and HOMFLY polynomial. Then we study the ability of these polynomials on detecting chirality, obtaining a knot not detected chiral by the HOMFLY polynomial, but detected chiral by the Kauffman polynomial. Introduction The main idea of this project is to give a clear and short introduction to the theory of knots and in particular the utility of knot polynomials on detecting chirality of knots. -
Chirality: the Handedness of Molecules
06 Chirality: The Handedness of Molecules Tartaric acid is found in grapes and other fruits, both free and as its salts (see Section 6.4B). Inset: A model of tartaric acid. (© fatihhoca/iStockphoto) KEY QUESTIONS 6.1 What Are Stereoisomers? 6.9 What Is the Significance of Chirality in the 6.2 What Are Enantiomers? Biological World? 6.3 How Do We Designate the Configuration of a 6.10 How Can Enantiomers Be Resolved? Stereocenter? HOW TO 6.4 What Is the 2n Rule? 6.1 How to Draw Enantiomers 6.5 How Do We Describe the Chirality of 6.2 How to Determine the R & S Configuration Cyclic Molecules with Two Stereocenters? without Rotating the Molecule 6.6 How Do We Describe the Chirality 6.3 How to Determine Whether Two Compounds Are of Molecules with Three or More the Same, Enantiomers, or Diastereomers without Stereocenters? the Need to Spatially Manipulate the Molecule 6.7 What Are the Properties of Stereoisomers? 6.8 How Is Chirality Detected in the CHEMICAL CONNECTIONS Laboratory? 6A Chiral Drugs IN THIS CHAPTER, we will explore the relationships between three-dimensional ob- jects and their mirror images. When you look in a mirror, you see a reflection, or mirror Mirror image The reflection image, of yourself. Now, suppose your mirror image becomes a three-dimensional object. of an object in a mirror. 167 168 CHAPTER 6 Chirality: The Handedness of Molecules We could then ask, “What is the relationship between you and your mirror image?” By relationship, we mean “Can your reflection be superposed on the original ‘you’ in such a way that every detail of the reflection corresponds exactly to the original?” The answer is that you and your mirror image are not superposable. -
Topological Analysis of Electron Density
Jyväskylä Summer School on Charge Density August 2007 Topological Analysis of Electron Density Louis J Farrugia Jyväskylä Summer School on Charge Density August 2007 What is topological analysis ? A method of obtaining chemically significant information from th e electron density ρ (rho ) ρ is a quantum -mechanical observable , and may also be obtained from experiment “It seems to me that experimental study of the scattered radiati on, in particular from light atoms, should get more attention, since in this way it should be possible to determine the arrangement of the electrons in the atoms.” P. Debye, Ann. Phys. (1915) 48 , 809. Jyväskylä Summer School on Charge Density August 2007 Why analyse the charge density ? The traditional way of approaching the theoretical basis of chem istry is though the wavefunction and the molecular orbitals obtained through (approximate) solutions to the Schr ödinger wave equation HHΨΨ == EE ΨΨ The Hohenberg -Kohn theorem confirmed that the density, ρ(r), is the fundamental property that characterises the ground state of a sy stem - once ρ(r) is known, the energy of the system is uniquely defined, and from there a diverse range of molecular properties can, in princ iple, be deduced. Thus a knowledge of ρ(r) opens the door to understanding of all the key challenges of chemistry. ρ is a quantum -mechanical observable. 9 P. Hohenberg, W. Kohn Phys. Rev. 1964 , 136 , B864. Jyväskylä Summer School on Charge Density August 2007 Can we ever observe orbitals ? Simply not ever possible - see E. Scerri (2000) J. Chem. Ed. 77 , 1492 . However ?? - see J. -
Controlling the Shape and Chirality of an Eight- Crossing Molecular Knot
Controlling the Shape and Chirality of an Eight- crossing Molecular Knot John P. Carpenter,‡ Charlie T. McTernan,‡ Jake L. Greenfield, Roy Lavendomme, Tanya K. Ronson and Jonathan R. Nitschke* 1Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge, CB2 1EW, UK ‡ these authors contributed equally *e-mail: [email protected] Abstract The knotting of biomolecules impacts their function, and enables them to carry out new tasks. Likewise, complex topologies underpin the operation of many synthetic molecular machines. The ability to generate and control more complex knotted architectures is essential to endow these machines with more advanced functions. Here we report the synthesis of a molecular knot with eight crossing points, consisting of a single organic loop woven about six templating metal centres, via one-pot self-assembly from a simple pair of dialdehyde and diamine subcomponents and a single metal salt. The structure and topology of the knot were established by NMR spectroscopy, mass spectrometry and X-ray crystallography. Upon demetallation, the purely organic strand relaxes into a symmetric conformation, whilst retaining the topology of the original knot. This knot is topologically chiral, and may be synthesised diastereoselectively through the use of an enantiopure diamine building block. 1 Knots are one of the oldest technologies, having been used for thousands of years to transform the properties of the materials in which they are tied.1 At the molecular level, knots are found in biology in proteins and DNA,2,3 -
Mathematical Chemistry! Is It? and If So, What Is It?
Mathematical Chemistry! Is It? And if so, What Is It? Douglas J. Klein Abstract: Mathematical chemistry entailing the development of novel mathe- matics for chemical applications is argued to exist, and to manifest an extreme- ly diverse range of applications. Yet further it is argued to have a substantial history of well over a century, though the field has perhaps only attained a de- gree of recognition with a formal widely accepted naming in the last few dec- ades. The evidence here for the broad range and long history is by way of nu- merous briefly noted example sub-areas. That mathematical chemistry was on- ly recently formally recognized is seemingly the result of its having been somewhat disguised for a period of time – sometimes because it was viewed as just an unnamed part of physical chemistry, and sometimes because the rather frequent applications in other chemical areas were not always viewed as math- ematical (often involving somewhat ‘non-numerical’ mathematics). Mathemat- ical chemistry’s relation to and distinction from computational chemistry & theoretical chemistry is further briefly addressed. Keywords : mathematical chemistry, physical chemistry, computational chemistry, theoretical chemistry. 1. Introduction Chemistry is a rich and complex science, exhibiting a diversity of reproduci- ble and precisely describable predictions. Many predictions are quantitative numerical predictions and also many are of a qualitative (non-numerical) nature, though both are susceptible to sophisticated mathematical formaliza- tion. As such, it should naturally be anticipated that there is a ‘mathematical chemistry’, rather likely with multiple roots and with multiple aims. Mathe- matical chemistry should focus on mathematically novel ideas and concepts adapted or developed for use in chemistry (this view being much in parallel with that for other similarly named mathematical fields, in physics, or in biology, or in sociology, etc. -
Assembled Molecular Face-Rotating Polyhedra to Transfer Chirality from Two to Three Dimensions
ARTICLE Received 28 Dec 2015 | Accepted 6 Jul 2016 | Published 24 Aug 2016 DOI: 10.1038/ncomms12469 OPEN Assembled molecular face-rotating polyhedra to transfer chirality from two to three dimensions Xinchang Wang1,*, Yu Wang1,2,*, Huayan Yang1,2, Hongxun Fang1, Ruixue Chen1,2, Yibin Sun1,2, Nanfeng Zheng1,2, Kai Tan1, Xin Lu1,2, Zhongqun Tian1,2 & Xiaoyu Cao1,2 In nature, protein subunits on the capsids of many icosahedral viruses form rotational patterns, and mathematicians also incorporate asymmetric patterns into faces of polyhedra. Chemists have constructed molecular polyhedra with vacant or highly symmetric faces, but very little is known about constructing polyhedra with asymmetric faces. Here we report a strategy to embellish a C3h truxene unit with rotational patterns into the faces of an octahedron, forming chiral octahedra that exhibit the largest molar ellipticity ever reported, to the best of our knowledge. The directionalities of the facial rotations can be controlled by vertices to achieve identical rotational directionality on each face, resembling the homo-directionality of virus capsids. Investigations of the kinetics and mechanism reveal that non-covalent interaction among the faces is essential to the facial homo-directionality. 1 State Key Laboratory of Physical Chemistry of Solid Surfaces and College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, China. 2 Collaborative Innovation Centre of Chemistry for Energy Materials, Xiamen University, Xiamen 361005, China. * These authors contributed equally to this work. Correspondence and requests for materials should be addressed to X.C. (email: [email protected]). NATURE COMMUNICATIONS | 7:12469 | DOI: 10.1038/ncomms12469 | www.nature.com/naturecommunications 1 ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/ncomms12469 otifs in architecture, mathematics and nature have daltons (calculated M.W.: 3196.31), corresponding to a [4 þ 6] inspired chemists to create their molecular composition (Fig.