Crystallography I

Total Page:16

File Type:pdf, Size:1020Kb

Crystallography I X-Ray Crystallography: Producing Crystals Feb 17-19, 2014 X-Ray Crystallography • Method to determine the ATOMIC structure of a molecule • The most widely used technique for determine structures of biological molecules • Can also be used to determine small molecules • Most entries in the PDB were determined by X-ray crystallography • NMR depends on interactions between nuclei X-Rays interacts with electrons. X-Ray • Why X-rays?? • X-rays are part of the EM spectrum • Atomic resolution - the position of two bonded atoms can be distinguished • Typical covalent bond is about 0.12 nm or 1.2x10-10m • 1x10-10 m is called an Angstrom (Å) • Limit of resolution of any optical method is defined by half the wavelength of the incident radiation • This is a consequence of the wave like properties of light • wavelength of visible light (400 to 800nm) therefore it can resolve objects to about 200nm (many cellular organelles) • For atomic resolution 0.12nm x2=0.24nm • This falls into the range of X-rays. • NO LENS for X-rays Light Microscope vs X-Ray Diffraction Light Microscopy X-ray Diffraction Sample X-rays X-ray source There is no lens for X-rays Crystals • X-rays weakly interact with matter • Crystals serve two purposes • High concentration • Order • Crystals are solids that are exact repeats • Comparison of crystalline quartz and glass - same molecule but quartz is an ordered crystal and glass is amorphous solid • Crystals are composed of repeating units - translational and rotational symmetry operators relate molecules to each other • Biological molecules are composed of chiral molecules. • Chirality limits the types of symmetry that can be used to describe a crystal • No mirror planes or points of symmetry Growing Crystals • There is no straightforward way to grow crystals • Protein crystals are a solid but do contain a lot of solvent - Most have 30-70% solvent • Large amounts of purified material • Empirical process that requires careful observation Growing Crystals II • Molecules come out of solution when its concentration exceeds it intrinsic solubility • Intrinsic solubility is related to the properties of the molecule (ie basic, acidic, hydrophobic, etc) and conditions (ie salt concentrations, pH, temperature) • Make a supersaturated solution and slowly precipitate the molecule in an orderly fashion • Methods • Remove excess solvent • This method is done for many small molecules • Not so useful for proteins since there may be other additives (salt, detergent, etc) • Decrease the solubility of molecule • This is accomplished by increasing or decreasing ionic strength of the solution or the addition of a molecule to dehydrate the protein (PEG) Crystal Growth in Theory Crystal Growth in Practice Past and Present Technology Definitions •Unit Cell - Repeating unit that builds the crystal •Asymmetric unit - the smallest portion of a crystal structure to which symmetry operations can be applied in order to generate the complete unit cell •A crystal asymmetric unit may contain •one biological assembly •a portion of a biological assembly •multiple biological assemblies •Symmetry operations - most common to crystals of biological macromolecules are rotations, translations and screw axes Bravais Lattice Unit cell defined by cell edges A, B, C with angles α,β,γ angle between A and B is γ; B and C is α; A and C is β Triclinic Monoclinic A≠B≠C A≠B≠C α≠β≠γ not 90° α,γ= 90° β anything but 90° Orthorhombic A≠B≠C α, β, γ= 90° Hexagonal Rhombohedral Tetragonal A=A≠C A=B=C A=A≠C α, β = 90° α=β=γ≠90° α, β, γ= 90° γ=120° Cubic A=B=C α=β=γ=90° Symbols to Denote Symmetry Into the page Along the page ⟶ ⇀ 2-fold 2-fold screw axis 2-fold 2-fold screw axis 3-fold 3-fold screw axis 4-fold 4-fold screw axis Two-Fold Axes of Rotation Three-Fold Axes of Rotation Mirror Planes and Inversion Center Bravais Lattice ! •! Primitive (P): lattice points on the cell corners only.! ! ! •! Body (I): one additional lattice point at the center of the cell.! ! ! •! Face (F): one additional lattice point at the center of each of the faces of the cell.! ! ! •! Base (C): one additional lattice point at the center of each of one pair of the cell faces.! Space Group Projections - P222 Origin b c Origin Equivalent positions a a (x,y,z) (-x,-y, z) c Origin b (-x,y,-z) (x,-y,-z) a Origin b Projections - P2221 Origin b c Origin Equivalent positions a a (x,y,z) (-x,-y, z+1/2) c Origin b (-x,y,-z+1/2) (x,-y,-z) a Origin b Projections - P21212 Origin b c Origin Equivalent positions a a (x,y,z) (-x,-y, z) c Origin b (-x+1/2,y+1/2,-z) (x+1/2,-y+1/2,-z) a Origin b Projections - P212121 Origin b c Origin Equivalent positions a a (x,y,z) (-x+1/2,-y, z+1/2) c Origin b (-x,y+1/2,-z+1/2) (x+1/2,-y+1/2,-z) a Origin b Crystal Preparation for Data Collection • X-rays used for diffraction is ionizing. • Free radical formation of water molecules • Free radicals destroy crystal integrity, particularly at synchrotrons. • Flash-cooling crystals to liquid nitrogen temperatures reduces radiation damage. • Need to prevent the formation of crystalline ice • Add cryoprotectant to crystal Cryoprotectant • Selection of a suitable cryoprotectant involves some trial and error • A suitable cryoprotectant will cool to cryogenic temperature without ice formation, physical damage to the crystal, and preserve diffraction. • To assay for the proper concentration, mix the cryoprotectant with the crystallization reagent and add to crystal. • Examples - Glycerol, low MW PEG, Ethylene glycol, sugars, Butandiol, 2-Methyl-2,4- pentanediol Cryoprotection Loops “Home” Source - Rotating Anode National Synchrotron Light Source NSLS II – Coming Soon! NSLS NSLS II • $912 million to design and build • State-of-the-art facility that produces x-rays up to 10,000 times brighter than NSLS http://www.bnl.gov/ps/nsls2/about-NSLS-II.asp Experimental Floor at NSLS X29 Beamline NSLS Beam Stop Crystal Cold Stream X-rays Diffraction Pattern Radiation Damage Crystal after data collection Position of the beam is in red Diffraction Pattern.
Recommended publications
  • Nano-Characterization of Ceramic-Metallic Interpenetrating Phase Composite Material Using Electron Crystallography
    YOUNGSTOWN STATE UNIVERSITY Nano-Characterization of Ceramic-Metallic Interpenetrating Phase Composite Material using Electron Crystallography by Marjan Moro Submitted in Partial Fulfillment of the Requirements for the Degree of Master of Science in Engineering in the Mechanical Engineering Program Mechanical and Industrial Engineering May 2012 Nano-Characterization of Ceramic-Metallic Interpenetrating Phase Composite Material using Electron Crystallography by Marjan Moro I hereby release this thesis to the public. I understand that this thesis will be made available from the OhioLINK ETD Center and the Maag Library Circulation Desk for public access. I also authorize the University or other individuals to make copies of this thesis as needed for scholarly research. Signature: Marjan Moro, Student Date Approvals: Dr. Virgil C. Solomon, Thesis Advisor Date Dr. Matthias Zeller, Committee Member Date Dr. Timothy R. Wagner, Committee Member Date Dr. Hyun W. Kim, Committee Member Date Dr. Peter J. Kasvinsky, Dean of Graduate Studies Date i Abstract Interpenetrating phase composites (IPCs) have unique mechanical and physical proper- ties and thanks to these they could replace traditional single phase materials in numbers of applications. The most common IPCs are ceramic-metallic systems in which a duc- tile metal supports a hard ceramic making it an excellent composite material. Fireline, Inc., from Youngstown, OH manufactures such IPCs using an Al alloy-Al2O3 based ceramic-metallic composite material. This product is fabricated using a Reactive Metal Penetration (RMP) process to form two interconnected networks. Fireline products are used, among others, as refractory materials for handling of high temperature molten metals. A novel route to adding a shape memory metal phase within a ceramic matrix has been proposed.
    [Show full text]
  • Crystal Structures
    Crystal Structures Academic Resource Center Crystallinity: Repeating or periodic array over large atomic distances. 3-D pattern in which each atom is bonded to its nearest neighbors Crystal structure: the manner in which atoms, ions, or molecules are spatially arranged. Unit cell: small repeating entity of the atomic structure. The basic building block of the crystal structure. It defines the entire crystal structure with the atom positions within. Lattice: 3D array of points coinciding with atom positions (center of spheres) Metallic Crystal Structures FCC (face centered cubic): Atoms are arranged at the corners and center of each cube face of the cell. FCC continued Close packed Plane: On each face of the cube Atoms are assumed to touch along face diagonals. 4 atoms in one unit cell. a 2R 2 BCC: Body Centered Cubic • Atoms are arranged at the corners of the cube with another atom at the cube center. BCC continued • Close Packed Plane cuts the unit cube in half diagonally • 2 atoms in one unit cell 4R a 3 Hexagonal Close Packed (HCP) • Cell of an HCP lattice is visualized as a top and bottom plane of 7 atoms, forming a regular hexagon around a central atom. In between these planes is a half- hexagon of 3 atoms. • There are two lattice parameters in HCP, a and c, representing the basal and height parameters Volume respectively. 6 atoms per unit cell Coordination number – the number of nearest neighbor atoms or ions surrounding an atom or ion. For FCC and HCP systems, the coordination number is 12. For BCC it’s 8.
    [Show full text]
  • Crystal Structure of a Material Is Way in Which Atoms, Ions, Molecules Are Spatially Arranged in 3-D Space
    Crystalline Structures – The Basics •Crystal structure of a material is way in which atoms, ions, molecules are spatially arranged in 3-D space. •Crystal structure = lattice (unit cell geometry) + basis (atom, ion, or molecule positions placed on lattice points within the unit cell). •A lattice is used in context when describing crystalline structures, means a 3-D array of points in space. Every lattice point must have identical surroundings. •Unit cell: smallest repetitive volume •Each crystal structure is built by stacking which contains the complete lattice unit cells and placing objects (motifs, pattern of a crystal. A unit cell is chosen basis) on the lattice points: to represent the highest level of geometric symmetry of the crystal structure. It’s the basic structural unit or building block of crystal structure. 7 crystal systems in 3-D 14 crystal lattices in 3-D a, b, and c are the lattice constants 1 a, b, g are the interaxial angles Metallic Crystal Structures (the simplest) •Recall, that a) coulombic attraction between delocalized valence electrons and positively charged cores is isotropic (non-directional), b) typically, only one element is present, so all atomic radii are the same, c) nearest neighbor distances tend to be small, and d) electron cloud shields cores from each other. •For these reasons, metallic bonding leads to close packed, dense crystal structures that maximize space filling and coordination number (number of nearest neighbors). •Most elemental metals crystallize in the FCC (face-centered cubic), BCC (body-centered cubic, or HCP (hexagonal close packed) structures: Room temperature crystal structure Crystal structure just before it melts 2 Recall: Simple Cubic (SC) Structure • Rare due to low packing density (only a-Po has this structure) • Close-packed directions are cube edges.
    [Show full text]
  • Division of Academic Affairs Technology Fee – Project Proposal 2015
    Division of Academic Affairs Technology Fee – Project Proposal 2015 Proposal Deadline: Wednesday, January 21, 2015 Project Proposal Type Instructional Technology Enhancement Project (ITEP) Focused projects proposed by an individual or small team with the intention of exploring new applications of instructional technology. ITEPs will typically be led by a faculty “principal investigator.” ITEPs are time-limited projects (up to two years in length) and allocations of Technology Fee funds to these projects are non-recurring. Project Title Crystallography Training Across the Sciences Total Amount of Funding Requested $9,100 Primary Project Coordinator Tim Royappa, Department of Chemistry Crystallography Training Across the Sciences Tim Royappa Department of Chemistry I. Project Description a. Introduction Crystallography has become an indispensable technique in the physical and life sciences. Its im- portance is demonstrated in Table 1, which outlines the chief developments in crystallography since its inception in the early 20th century. In fact, 2014 was designated as the International Year of Crystallography, and the key contributions of crystallography to a wide variety of science disciplines were celebrated across the globe. The reason that crystallography is so important is that it is the best way to elucidate the atomic structure of matter, leading to a better understanding of its physical, chemical and biological properties. Era Discovery/Advance in Crystallography Major Awards Diffraction of X-rays by crystals discovered by Paul Nobel Prize in Physics (1914) Ewald and Max von Laue; von Laue formulates the to von Laue; Nobel Prize in 1910s basics of crystallography; William L. Bragg works out Physics (1915) to Bragg and the fundamental equation of crystallography his father, William H.
    [Show full text]
  • MSE 403: Ceramic Materials
    MSE 403: Ceramic Materials Course description: Processing, characteristics, microstructure and properties of ceramic materials. Number of credits: 3 Course Coordinator: John McCloy Prerequisites by course: MSE 201 Prerequisites by topic: 1. Basic knowledge of thermodynamics. 2. Elementary crystallography and crystal structure. 3. Mechanical behavior of materials. Postrequisites: None Textbooks/other required 1. Carter, C.B. and Norton, M.G. Ceramic Materials Science and Engineering, materials: Springer, 2007. Course objectives: 1. Review of crystallography and crystal structure. 2. Review of structure of atoms, molecules and bonding in ceramics. 3. Discussion on structure of ceramics. 4. Effects of structure on physical properties. 5. Ceramic Phase diagrams. 6. Discussion on defects in ceramics. 7. Introduction to glass. 8. Discussion on processing of ceramics. 9. Introduction to sintering and grain growth. 10. Introduction to mechanical properties of ceramics. 11. Introduction to electrical properties of ceramics. 12. Introduction to bioceramics. 13. Introduction to magnetic ceramics. Topics covered: 1. Introduction to crystal structure and crystallography. 2. Fundamentals of structure of atoms. 3. Structure of ceramics and its influence on properties. 4. Binary and ternary phase diagrams. 5. Point defects in ceramics. 6. Glass and glass-ceramic composites. 7. Ceramics processing and sintering. 8. Mechanical properties of ceramics. 9. Electrical properties of ceramics. 10. Bio-ceramics. 11. Ceramic magnets. Expected student outcomes: 1. Knowledge of crystal structure of ceramics. 2. Knowledge of structure-property relationship in ceramics. 3. Knowledge of the defects in ceramics (Point defects). 4. Knowledge of glass and glass-ceramic composite materials. 5. Introductory knowledge on the processing of bulk ceramics. 6. Applications of ceramic materials in structural, biological and electrical components.
    [Show full text]
  • Multidisciplinary Design Project Engineering Dictionary Version 0.0.2
    Multidisciplinary Design Project Engineering Dictionary Version 0.0.2 February 15, 2006 . DRAFT Cambridge-MIT Institute Multidisciplinary Design Project This Dictionary/Glossary of Engineering terms has been compiled to compliment the work developed as part of the Multi-disciplinary Design Project (MDP), which is a programme to develop teaching material and kits to aid the running of mechtronics projects in Universities and Schools. The project is being carried out with support from the Cambridge-MIT Institute undergraduate teaching programe. For more information about the project please visit the MDP website at http://www-mdp.eng.cam.ac.uk or contact Dr. Peter Long Prof. Alex Slocum Cambridge University Engineering Department Massachusetts Institute of Technology Trumpington Street, 77 Massachusetts Ave. Cambridge. Cambridge MA 02139-4307 CB2 1PZ. USA e-mail: [email protected] e-mail: [email protected] tel: +44 (0) 1223 332779 tel: +1 617 253 0012 For information about the CMI initiative please see Cambridge-MIT Institute website :- http://www.cambridge-mit.org CMI CMI, University of Cambridge Massachusetts Institute of Technology 10 Miller’s Yard, 77 Massachusetts Ave. Mill Lane, Cambridge MA 02139-4307 Cambridge. CB2 1RQ. USA tel: +44 (0) 1223 327207 tel. +1 617 253 7732 fax: +44 (0) 1223 765891 fax. +1 617 258 8539 . DRAFT 2 CMI-MDP Programme 1 Introduction This dictionary/glossary has not been developed as a definative work but as a useful reference book for engi- neering students to search when looking for the meaning of a word/phrase. It has been compiled from a number of existing glossaries together with a number of local additions.
    [Show full text]
  • Basic Crystallography – Data Collection and Processing
    Basic Crystallography – Data collection and processing Louise N. Dawe, PhD Wilfrid Laurier University Department of Chemistry and Biochemistry References and Additional Resources Faculty of Science, Bijvoet Center for Biomolecular Research, Crystal and Structural Chemistry. ‘Interpretation of Crystal Structure Determinations’ 2005 Course Notes: http://www.cryst.chem.uu.nl/huub/notesweb.pdf The University of Oklahoma: Chemical Crystallography Lab. Crystallography Notes and Manuals. http://xrayweb.chem.ou.edu/notes/index.html Müller, P. Crystallographic Reviews, 2009, 15(1), 57-83. Müller, Peter. 5.069 Crystal Structure Analysis, Spring 2010. (Massachusetts Institute of Technology: MIT OpenCourseWare), http://ocw.mit.edu/courses/chemistry/5- 069-crystal-structure-analysis-spring-2010/. License: Creative Commons BY-NC-SA X-ray Crystallography Data Collection and Processing • Select and mount the crystal. • Center the crystal to the center of the goniometer circles (instrument maintenance.) • Collect several images; index the diffraction spots; refine the cell parameters; check for higher metric symmetry • Determine data collection strategy; collect data. • Reduce the data by applying background, profile (spot- shape), Lorentz, polarization and scaling corrections. • Determine precise cell parameters. • Collect appropriate information for an absorption correction. (Index the faces of the crystal. A highly redundant set of data is sufficient for an empirical absorption correction.) • Apply an absorption correction to the data. (http://xrayweb.chem.ou.edu/notes/collect.html) Single crystal diffraction of X-rays Principle quantum number n = 1 K level Note: The non SI unit Å is normally used. n = 2 L level 1 Å = 10-10 m n = 3 M level etc… L to K transitions produce 'Ka' emission M to K transitions produce 'Kb' emission.
    [Show full text]
  • Structure Determination by X-Ray Crystallography
    Chem 406: Biophysical Chemistry Lecture 7: Structure Determination by X-ray Crystallography I. Introduction A. Most of the structures in the Protein Data Bank (PDB) were determined by x-ray diffraction. 1. PDB Statistics 2. Other names for x-ray diffraction a. x-ray crystallography b. crystallography B. In the past couple of years there has been a growing number of structures, particularly of small proteins and peptides, that have been solved using a combination nuclear magnetic resonance (NMR) and computational chemistry. 1. PDB Statistics C. The structural information obtained from these techniques are the coordinates of the atoms in the molecule. Overhead 1 (Print out of a PDB file) II. Image magnification A. We will look first at techniques that determine structures by producing images; these include light microscopy, electron microscopy and X-ray crystallography; first, though, we need to look into the properties of light. B. Light 1. The wavelike nature of light (electromagnetic radiation) a. Light waves are depicted as having oscillating electric and magnetic field components that are at right angles to one another. b. These waves are described using the following parameters. Overhead 2 and on board ( a light wave) i. wavelength () ii. frequency ( = c/) iii. Energy (E = h) 1. The constant h, is Planck’s constant and is equal to 6.63 x 10-34 Js (Joule-seconds). 2. Light scattering and refraction a. When light passes through matter the oscillating electrical field polarizes the atoms present in the matter. i. Remember that atoms are made of a nucleus containing positively charged protons and is surrounded by negatively charged electrons.
    [Show full text]
  • Simplified Protein Design Biased for Prebiotic Amino Acids Yields A
    Simplified protein design biased for prebiotic amino acids yields a foldable, halophilic protein Liam M. Longo, Jihun Lee1, and Michael Blaber2 Department of Biomedical Sciences, Florida State University, Tallahassee, FL 32306-4300 Edited by Brian W. Matthews, University of Oregon, Eugene, OR, and approved December 19, 2012 (received for review November 9, 2012) A compendium of different types of abiotic chemical syntheses reducing the potential diversity of interactions that can be encoded identifies a consensus set of 10 “prebiotic” α-amino acids. Before the to that of currently proposed theoretic limits for foldability (14– emergence of biosynthetic pathways, this set is the most plausible 16) (thus, to be able to support protein foldability, the 10 pre- resource for protein formation (i.e., proteogenesis) within the overall biotic amino acids would need to be a remarkably efficient selec- process of abiogenesis. An essential unsolved question regarding tion); (ii) aromatic residues, key contributors to extensive van der this prebiotic set is whether it defines a “foldable set”—that is, does Waals interactions in hydrophobic cores that serve as a driving force it contain sufficient chemical information to permit cooperatively for protein collapse, are absent in the prebiotic alphabet; and (iii) folding polypeptides? If so, what (if any) characteristic properties there are no basic amino acids in the prebiotic set, thus restricting might such polypeptides exhibit? To investigate these questions, protein design to acidic polypeptides, limiting the presence of salt two “primitive” versions of an extant protein fold (the β-trefoil) were bridge interactions and resulting in acidic pI (1, 3). produced by top-down symmetric deconstruction, resulting in a re- To date, there has been no experimental demonstration that the duced alphabet size of 12 or 13 amino acids and a percentage of prebiotic set of amino acids comprises a foldable set; additionally, prebiotic amino acids approaching 80%.
    [Show full text]
  • Geochemistry and Crystallography of Recrystallized Sedimentary Dolomites
    Goldschmidt2019 Abstract Geochemistry and crystallography of recrystallized sedimentary dolomites GEORGINA LUKOCZKI1*, PANKAJ SARIN2, JAY M. GREGG1, CÉDRIC M. JOHN3 1 Oklahoma State University, Boone Pickens School of Geology, Stillwater, OK, USA 2 Oklahoma State University, School of Materials Science and Engineering, Tulsa, OK, USA 3 Imperial College London, Department of Earth Science and Engineering, London, UK (*Correspondence: [email protected]) Most sedimentary dolomites [CaMg(CO3)2] are meta- stable upon formation and either transform into more stable dolomite via recrystallization, or persist as meta-stable phases over deep geological time. The stability of dolomite has long been considered to be influenced by ordering and stoichiometry [1]; however, how recrystallization alters the crystal structure and chemistry of dolomites remains poorly understood. In order to better understand the relationship between various chemical and crystallographic properties and the underlying geological processes, sedimentary dolomites, formed in various diagenetic environments, were investigated in detail. The innovative aspect of this study is the application of high resolution diffraction techniques, such as sychrotron X-ray and neutron diffraction, together with various geochemical proxies, including clumped isotopes, to characterize recrystallized sedimentary dolomites. The age of the studied samples ranges from Holocene to Cambrian. The diagenetic environments of dolomitization and recrystallization were determined primarily on the basis of petrographic and geochemical data [2, 3, 4]. Rietveld refinement of high-resolution diffraction data revealed notable differences in crystallographic parameters across the various dolomite types. Several dolomite bodies have been identified as potential sites for CO2 sequestration [5]; therefore, new insights into what factors control dolomite ordering and stoichiometry will contribute to an improved understanding of dolomite reactivity and may be particularly important for CO2 sequestration studies.
    [Show full text]
  • Crystal Structure
    Physics 927 E.Y.Tsymbal Section 1: Crystal Structure A solid is said to be a crystal if atoms are arranged in such a way that their positions are exactly periodic. This concept is illustrated in Fig.1 using a two-dimensional (2D) structure. y T C Fig.1 A B a x 1 A perfect crystal maintains this periodicity in both the x and y directions from -∞ to +∞. As follows from this periodicity, the atoms A, B, C, etc. are equivalent. In other words, for an observer located at any of these atomic sites, the crystal appears exactly the same. The same idea can be expressed by saying that a crystal possesses a translational symmetry. The translational symmetry means that if the crystal is translated by any vector joining two atoms, say T in Fig.1, the crystal appears exactly the same as it did before the translation. In other words the crystal remains invariant under any such translation. The structure of all crystals can be described in terms of a lattice, with a group of atoms attached to every lattice point. For example, in the case of structure shown in Fig.1, if we replace each atom by a geometrical point located at the equilibrium position of that atom, we obtain a crystal lattice. The crystal lattice has the same geometrical properties as the crystal, but it is devoid of any physical contents. There are two classes of lattices: the Bravais and the non-Bravais. In a Bravais lattice all lattice points are equivalent and hence by necessity all atoms in the crystal are of the same kind.
    [Show full text]
  • The American Mineralogist Crystal Structure Database
    American Mineralogist, Volume 88, pages 247–250, 2003 The American Mineralogist crystal structure database ROBERT T. DOWNS* AND MICHELLE HALL-WALLACE Department of Geosciences, University of Arizona, Tucson, Arizona 85721-0077, U.S.A. ABSTRACT A database has been constructed that contains all the crystal structures previously published in the American Mineralogist. The database is called “The American Mineralogist Crystal Structure Database” and is freely accessible from the websites of the Mineralogical Society of America at http://www.minsocam.org/MSA/Crystal_Database.html and the University of Arizona. In addition to the database, a suite of interactive software is provided that can be used to view and manipulate the crystal structures and compute different properties of a crystal such as geometry, diffraction patterns, and procrystal electron densities. The database is set up so that the data can be easily incorporated into other software packages. Included at the website is an evolving set of guides to instruct the user and help with classroom education. INTRODUCTION parameters; (5) incorporating comments from either the origi- The structure of a crystal represents a minimum energy con- nal authors or ourselves when changes are made to the origi- figuration adopted by a collection of atoms at a given tempera- nally published data. Each record in the database consists of a ture and pressure. In principle, all the physical and chemical bibliographic reference, cell parameters, symmetry, atomic properties of any crystalline substance can be computed from positions, displacement parameters, and site occupancies. An knowledge of its crystal structure. The determination of crys- example of a data set is provided in Figure 1.
    [Show full text]