An Early Explanation of the Periodic Table
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Spectroscopy from 1916 to 1940
PRE-1940 Spectroscopy from 1916 to 1940 Patricia Daukantas uring the first quarter century of The Optical Society (OSA), spectroscopy led to major insights into atomic and molecular physics and paved the way for important practical D applications. Optical spectroscopy existed for decades before the formation of OSA, but it was empirical and descriptive in its nature. Spectroscopists had carefully measured the wavelengths of spectral lines associated with various elements, but the subatomic mechanisms that created these lines were not yet fully understood. Twenty-four years later, as the world lurched toward the second all-encompassing war of the twentieth century, the spectroscopic fingerprints of atoms and molecules had provided vital evidence for the emerging quantum theory. Experimentalists refined their techniques and discovered previously unknown phenomena. Spectroscopy and Quantum Mechanics A few years before OSA was formed, Niels Bohr had proposed his model of the hydrogen atom, which explained the empirical Rydberg formula for the spectral lines of atomic hydrogen, at least to a first approximation. Theodore Lyman completed his investigations of the ultraviolet emission lines of hydrogen, beginning at 1216 Å in 1914. Little happened in spectroscopy during World War I, but the field came raging back shortly after the armistice. In 1919, Arnold Sommerfeld, doctoral adviser to multiple Nobel Laureates, published Atombau und Spektralinien (Atomic Structure and Spectral Lines). William F. Meggers, who would become the 1949–1950 OSA president, opined that “spectroscopists were amazed that our meager knowledge of atomic structure and the origin of spectra could be expanded into such a big book” [1]. The same year, Sommerfeld and another German physicist, Walther Kossel, formulated the displacement law now named after them [1]. -
A Bibliography of Experimental Saturation Properties of the Cryogenic Fluids1
National Bureau of Standards Library, K.W. Bldg APR 2 8 1965 ^ecknlcai rlote 92c. 309 A BIBLIOGRAPHY OF EXPERIMENTAL SATURATION PROPERTIES OF THE CRYOGENIC FLUIDS N. A. Olien and L. A. Hall U. S. DEPARTMENT OF COMMERCE NATIONAL BUREAU OF STANDARDS THE NATIONAL BUREAU OF STANDARDS The National Bureau of Standards is a principal focal point in the Federal Government for assuring maximum application of the physical and engineering sciences to the advancement of technology in industry and commerce. Its responsibilities include development and maintenance of the national stand- ards of measurement, and the provisions of means for making measurements consistent with those standards; determination of physical constants and properties of materials; development of methods for testing materials, mechanisms, and structures, and making such tests as may be necessary, particu- larly for government agencies; cooperation in the establishment of standard practices for incorpora- tion in codes and specifications; advisory service to government agencies on scientific and technical problems; invention and development of devices to serve special needs of the Government; assistance to industry, business, and consumers in the development and acceptance of commercial standards and simplified trade practice recommendations; administration of programs in cooperation with United States business groups and standards organizations for the development of international standards of practice; and maintenance of a clearinghouse for the collection and dissemination of scientific, tech- nical, and engineering information. The scope of the Bureau's activities is suggested in the following listing of its four Institutes and their organizational units. Institute for Basic Standards. Electricity. Metrology. Heat. Radiation Physics. Mechanics. Ap- plied Mathematics. -
Route to High-Energy Density Polymeric Nitrogen T-N Via Heâˆ'n Compounds
ARTICLE DOI: 10.1038/s41467-018-03200-4 OPEN Route to high-energy density polymeric nitrogen t- N via He−N compounds Yinwei Li1, Xiaolei Feng2,3, Hanyu Liu4, Jian Hao1, Simon A.T. Redfern 3,5, Weiwei Lei6, Dan Liu6 & Yanming Ma2,7 Polymeric nitrogen, stabilized by compressing pure molecular nitrogen, has yet to be recovered to ambient conditions, precluding its application as a high-energy density material. 1234567890():,; Here we suggest a route for synthesis of a tetragonal polymeric nitrogen, denoted t-N, via He-N compounds at high pressures. Using first-principles calculations with structure searching, we predict a class of nitrides with stoichiometry HeN4 that are energetically stable (relative to a mixture of solid He and N2) above 8.5 GPa. At high pressure, HeN4 comprises a polymeric channel-like nitrogen framework filled with linearly arranged helium atoms. The nitrogen framework persists to ambient pressure on decompression after removal of helium, forming pure polymeric nitrogen, t-N. t-N is dynamically and mechanically stable at ambient pressure with an estimated energy density of ~11.31 kJ/g, marking it out as a remarkable high- energy density material. This expands the known polymeric forms of nitrogen and indicates a route to its synthesis. 1 School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China. 2 State Key Laboratory of Superhard Materials, College of Physics, Jilin University, Changchun 130012, China. 3 Department of Earth Sciences, University of Cambridge, Downing Street, Cambridge CB2 3EQ, UK. 4 Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA. 5 Center for High Pressure Science and Technology Advanced Research (HPSTAR), Shanghai 201203, China. -
Chemical Bonding: the Journey from Miniature Hooks to Density Functional Theory
molecules Review Chemical Bonding: The Journey from Miniature Hooks to Density Functional Theory Edwin C. Constable * and Catherine E. Housecroft Department of Chemistry, University of Basel, BPR 1096, Mattenstrasse 24a, CH-4058 Basel, Switzerland; [email protected] * Correspondence: [email protected]; Tel.: +41-61-207-1001 Academic Editor: Antonio J. Mota Received: 10 May 2020; Accepted: 3 June 2020; Published: 5 June 2020 Abstract: Our modern understanding of chemistry is predicated upon bonding interactions between atoms and ions resulting in the assembly of all of the forms of matter that we encounter in our daily life. It was not always so. This review article traces the development of our understanding of bonding from prehistory, through the debates in the 19th century C.E. bearing on valence, to modern quantum chemical models and beyond. Keywords: bonding; valency; affinity, structure; history of science 1. Introduction Bonding is what separates chemistry from physics. If the understanding of atoms and their component particles belongs primarily to the realm of physics, then chemistry is concerned with the aggregation of atoms into chemical entities held together by bonds. If science is a language, and atoms are the letters, bonding is the mechanism by which the letters are combined into words. The International Union of Pure and Applied Chemistry (IUPAC) states that “there is a chemical bond between two atoms or groups of atoms in the case that the forces acting between them are such as to lead to the formation of an aggregate with sufficient stability to make it convenient for the chemist to consider it as an independent ‘molecular species’” [1]. -
Physics of Solids Under Strong Compression
Rep. Prog. Phys. 59 (1996) 29–90. Printed in the UK Physics of solids under strong compression W B Holzapfel Universitat-GH¨ Paderborn, Fachbereich Physik, Warburger Strasse 100, D-33095 Paderborn, Germany Abstract Progress in high pressure physics is reviewed with special emphasis on recent developments in experimental techniques, pressure calibration, equations of state for simple substances and structural systematics of the elements. Short sections are also devoted to hydrogen under strong compression and general questions concerning new electronic ground states. This review was received in February 1995 0034-4885/96/010029+62$59.50 c 1996 IOP Publishing Ltd 29 30 W B Holzapfel Contents Page 1. Introduction 31 2. Experimental techniques 31 2.1. Overview 31 2.2. Large anvil cells (LACs) 33 2.3. Diamond anvil cells (DACs) 33 2.4. Shock wave techniques 39 3. Pressure sensors and scales 42 4. Equations of state (EOS) 44 4.1. General considerations 44 4.2. Equations of state for specific substances 51 4.3. EOS data for simple metals 52 4.4. EOS data for metals with special softness 55 4.5. EOS data for carbon group elements 58 4.6. EOS data for molecular solids 59 4.7. EOS data for noble gas solids 60 4.8. EOS data for hydrogen 62 4.9. EOS forms for compounds 63 5. Phase transitions and structural systematics 65 5.1. Alkali and alkaline-earth metals 66 5.2. Rare earth and actinide metals 66 5.3. Ti, Zr and Hf 68 5.4. sp-bonded metals 68 5.5. -
Answer on Question #49847, Physics, Atomic Physics Task: Sir
Answer on Question #49847, Physics, Atomic Physics Task: sir... why should we take shell K L M N letters in Niels bohr's experiment not A B C D s Answer: The K, L, M-shell labels were not proposed by Bohr as part of his original 1913 quantum model of the atom but were rather the result of experimental studies of the phenomenon of X-ray fluorescence made by the British physicist, Charles Glover Barkla, in the period 1906-1911. Barkla characterized the secondary radiations produced when samples of the elements were exposed to an X-ray beam in terms of both their homogeneity and penetrating ability (measured in terms of the number of sheets of aluminum metal required to absorb them). He found that these secondary X-rays fell into two classes, which he labeled K and L, based on the observation that the K radiation was more penetrating than the L radiation. He also observed that the production of K versus L radiation correlated with the atomic eights of the elements, with the elements Ca through Rh producing only K radiation, W through Bi producing only L radiation, and Ag through Ce producing a mixture of both. In 1913 these latter observations were refined by the British physicist, Henry Moseley (1887-1915), in his classic study of the relationship between the frequency of the secondary X-rays and the atomic numbers of the elements. Rationalization of the Barkla-Moseley X-ray fluorescence results in terms of the Bohr model is usually credited to a 1914 paper by the German physicist, Walther Kossel (1888- 1956), who argued that the K radiation was due to an excited electron falling back into a vacancy in the first shell of an atom, and the L radiation to an excited electron falling back into a vacancy in the second shell . -
Polymeric Nitrogen by Plasma Enhanced Chemical Vapor Deposition
New Jersey Institute of Technology Digital Commons @ NJIT Dissertations Electronic Theses and Dissertations Fall 1-31-2015 Polymeric nitrogen by plasma enhanced chemical vapor deposition El Mostafa Benchafia New Jersey Institute of Technology Follow this and additional works at: https://digitalcommons.njit.edu/dissertations Part of the Materials Science and Engineering Commons Recommended Citation Benchafia, El Mostafa, "Polymeric nitrogen by plasma enhanced chemical vapor deposition" (2015). Dissertations. 98. https://digitalcommons.njit.edu/dissertations/98 This Dissertation is brought to you for free and open access by the Electronic Theses and Dissertations at Digital Commons @ NJIT. It has been accepted for inclusion in Dissertations by an authorized administrator of Digital Commons @ NJIT. For more information, please contact [email protected]. Copyright Warning & Restrictions The copyright law of the United States (Title 17, United States Code) governs the making of photocopies or other reproductions of copyrighted material. Under certain conditions specified in the law, libraries and archives are authorized to furnish a photocopy or other reproduction. One of these specified conditions is that the photocopy or reproduction is not to be “used for any purpose other than private study, scholarship, or research.” If a, user makes a request for, or later uses, a photocopy or reproduction for purposes in excess of “fair use” that user may be liable for copyright infringement, This institution reserves the right to refuse to accept -
Emil Rupp, Albert Einstein and the Canal Ray Experiments on Wave-Particle Duality
Emil Rupp, Albert Einstein and the Canal Ray Experiments on Wave-Particle Duality: Scientific Fraud and Theoretical Biasa Jeroen van Dongen* Institute for History and Foundations of Science Utrecht University PO Box 80.000, 3508 TA Utrecht, the Netherlands & Einstein Papers Project, California Institute of Technology, Pasadena, CA 91125 USA Abstract In 1926 Emil Rupp published a number of papers on the interference properties of light emitted by canal ray sources. These articles, particularly one paper that came into being in close collaboration with Albert Einstein, drew quite some attention as they probed the wave versus particle nature of light. They also significantly propelled Rupp’s career, even though that from the outset they were highly controversial. This article will review this episode, and in particular Rupp’s collaboration with Einstein. Evidence that Rupp forged his results is presented and their critical reception in the socially and politically divided German physics community is discussed. These divisions fail to explain the full dynamic; the latter is attempted by turning to the role that theoretical bias on occasion has in assessing experiment. Einstein’s responses in particular are analysed in this context. Introduction: the career of Emil Rupp “[Emil] Rupp, in the late twenties, early thirties, was regarded as the most important and most competent experimental physicist. He did incredible things. [...] Later, it turned out that everything that he had ever published, everything, was forged. This had gone on for ten years, ten years!”1 As this quote of Walther Gerlach illustrates, the first third of the twentieth century witnessed one of the biggest scandals in physics: the rise and fall of Emil Rupp. -
Pressure-Induced Stability and Polymeric Nitrogen in Alkaline Earth
RSC Advances View Article Online PAPER View Journal | View Issue Pressure-induced stability and polymeric nitrogen in alkaline earth metal N-rich nitrides (XN ,X¼ Ca, Cite this: RSC Adv.,2021,11, 17222 6 Sr and Ba): a first-principles study† Zhipeng Liu, Shuli Wei, * Yanhui Guo, Haiyang Sun, Hao Sun, Qiang Chang and Yuping Sun * Multi-nitrogen or polynitrogen compounds can be used as potential high energy-density materials, so they have attracted great attention. Nitrogen can exist in alkaline earth metal nitrogen-rich (N-rich) compounds in the form of single or double bonds. In recent years, to explore N-rich compounds which are stable and easy to synthesize has become a new research direction. The N-rich compounds XN6 (X ¼ Ca, Sr and Ba) have been reported under normal pressure. In order to find other stable crystal structures, we have performed XN6 (X ¼ Ca, Sr and Ba) exploration under high pressure. We found that SrN6 has a new P1 phase at a pressure of 22 GPa and an infinite nitrogen chain structure, and BaN6 has a new C2/m phase Creative Commons Attribution-NonCommercial 3.0 Unported Licence. at 110 GPa, with an N6 ring network structure. Further, we observed that the infinite nitrogen chain and 2 the N6 ring network structure contain typical covalent bonds formed by the hybridization of the sp and 3 sp orbitals of N, respectively. It is found that both SrN6 and BaN6 are semiconductor materials and the N-2p orbital plays an important role in the stability of the crystal structure for P1-SrN6 and C2/m-BaN6. -
Chymists: That Strange Class of Mortals
CHYMISTS: THAT STRANGE CLASS OF MORTALS Caricatures of Famous Chemists with a Few Physicists and Biologists Added BY WILLIAM B. JENSEN Oesper Collections Cincinnati 2010 CHYMISTS: THAT STRANGE CLASS OF MORTALS Caricatures of Famous Chemists with a Few Physicists and Biologists Added BY WILLIAM B. JENSEN Oesper Collections Cincinnati 2010 “The chymists are a strange class of mortals, impelled by an almost insane impulse to seek their pleasures amid smoke and vapor, soot and flame, poisons and poverty. Yet among all these evils I seem to live so sweetly that may I die if I were to changes places with the Persian King.” Johann Joachim Becher Physica Subterranea, 1667 INTRODUCTION The majority of the following caricatures were done more than 40 years ago when I was a junior at the University of Wisconsin-Madison and attending Aaron Ihde’s lectures on the history of chemistry. Each week, rather than taking lecture notes, I would instead select one of the chemists that Ihde was lecturing on and do a caricature based on the portraits found in Ihde’s textbook, The Development of Modern Chemistry (1964). This original set has since been supplemented by about another half-dozen caricatures prompted by requests over the years from various individuals and journals. In the 1970s there was little interest in these drawings, but with the passage of time, a sort of underground demand for them has spontaneously arisen among teachers and students of chemistry and many have since been reproduced on coffee mugs, T-shirts, and on various internet sites. More recently I was informed that one of them (Robert Bunsen) was even being used as the logo for a rock band. -
Vi. Properties of Nitrogen Contents
VI. PROPERTIES OF NITROGEN CONTENTS A. Vapor Pressure 1. Vapor Pressure at Saturation B. Specific Volume 1. Specific Volume at Saturation C. Compressibility Factor 1. Compressibility for Nitrogen D. Specific Heat 1. Liquid Nitrogen at Saturation (CU) 2. Gaseous Nitrogen (Cp) / E. Heat of Vaporization 1. Heat of Vaporization and Enthalpy o ‘I itrogen Liquid and Vapor. F. Ent Aalpy 1. Table of Nitrogen Properties’ 2, Temperature-Entropy Chart for Nitrogen G. Thermal Conductivity 1. Liquid Nltrogen 2. Gaseous Nitrogen H. Dielectric Constant 1. Liquid Nitrogen 2. Gaseous Nitrogen I. Surf ace Tension 1. Liquid Nitrogen J. vi sco sity 1. Liquid Nitrogen 2. Gaseous Nitrogen K. Velocity of Sound 1. Liquid Nitrogen 2. Gaseous Nitrogen VI-INDEX Vapor Pressure of Saturated Nitrogen Temperature Pressure * Pres sure (K) ( ATM) PSIA 63.150 0.123 . 1.808 64 .OOO o .I44 2.116 65 .OOO O ,172 2.528 66 .ooo O e203 2 0983 67.000 0.240 3.527 68 .ooo 0.281 4.130 69 .ooo 0.328 4.820 70 .OOO 0.380 5 0585 71 .ooo 0.439 6.453 72 .OOO 0 9505 7.422 73.000 0.579 8 -509 74 .ooo 0 .660 9.699 75.000 0 -750 11.022 76 .ooo 0.849. 12.477 77.000 0 -958 14.079 77.364 1.ooo 14.696 78 .ooo 1.077 15.828 79.000 1.207 17.738 80 .ooo 3. -349 19.825 81 .ooo e503 .22,088 82 .OOO 1.6701 24.542 83 .OOO 1.850 27.188 84 .ooo 2.045 ' 30.053 85 .OOO 2.254 33 125 86 .ooo 2.480 36.446 87 .ooo 2.721 39 988 88 .ooo 2.980 43.794 89 .ooo 3 256 47.850 go. -
Isolated Hydrogen in II–VI Zinc–Chalcogenide Widegap Semiconductors Modelled by the Muon Analogue
Rui C¶esarVil~ao Isolated hydrogen in II{VI zinc{chalcogenide widegap semiconductors modelled by the muon analogue Faculdade de Ci^enciase Tecnologia Universidade de Coimbra Coimbra { 2007 ii Rui C¶esarVil~ao Isolated hydrogen in II{VI zinc{chalcogenide widegap semiconductors modelled by the muon analogue [Hidrogenio¶ isolado em calcogenos¶ de zinco da fam¶³lia II-VI com propriedades semicondutoras e intervalo largo de energias proibidas, estudado atraves¶ da analogia com o muao]~ Disserta»c~aode doutoramento em F¶³sica, especialidade de F¶³sicaExperimental, submetida `aFaculdade de Ci^enciase Tecnologia, Universidade de Coimbra Coimbra - 2007 iv Aos meus Pais A` Susana vi Abstract We have investigated the behaviour of isolated hydrogen in II{VI zinc chalco- genide widegap semiconductors, by means of the positive-muon analogue. A broad program of muon-spin rotation, relaxation and resonance measurements was under- taken for monocrystalline samples of ZnSe, upon adequate characterization (parti- cularly on the electrical transport properties, by means of Hall-e®ect and resistivity measurements). Two compact paramagnetic muonium states MuI and MuII were identi¯ed and the interconversion process was characterized. Capture of a second ¡ electron by MuII, forming the negative ion MuII was observed as well. This charged state becomes thermally unstable above 60 K and we relate this to possible ioni- zation to the conduction band and estimate the corresponding acceptor level. In adition to ZnSe, monocrystalline samples of ZnS and ZnTe were investigated. Only one paramagnetic state is observed in ZnS, whose behaviour is shown to be much similar to that of MuII in ZnSe. In ZnTe, only a diamagnetic state is observed, which we suggest corresponds to a deep donor in this material.