Investigating the Reactivity of Size-Selected Metal Oxide Clusters for Organophosphorus Nerve Agent Decomposition

Total Page:16

File Type:pdf, Size:1020Kb

Investigating the Reactivity of Size-Selected Metal Oxide Clusters for Organophosphorus Nerve Agent Decomposition INVESTIGATING THE REACTIVITY OF SIZE-SELECTED METAL OXIDE CLUSTERS FOR ORGANOPHOSPHORUS NERVE AGENT DECOMPOSITION By Nicolas G. Blando A dissertation submitted to Johns Hopkins University in conformity with the requirements of the degree of Doctor of Philosophy. Baltimore, Maryland August 2020 © 2020 Nicolas G. Blando All Rights Reserved Abstract Metal and metal oxide nanostructures of varying size and composition are currently the industry standard for protection against chemical warfare agents (CWAs), yet there is limited understanding of the effects that the size and composition of the nanostructures have on the reaction mechanisms. Ultra-small, size-selected metal oxide clusters offer the opportunity of a nearly limitless number of unstudied candidate species as well as a chance to understand reactivity trends that may drive the discovery of more engineered catalysts. Clusters are small aggregates of atoms, <1000, which often display intriguing properties in that size range due quantum confinement, undercoordination and other emergent properties. In this work, the history and development of molecular beam techniques that support the study of size-selected clusters in-vacuo are discussed, leading up to the construction of a novel beamline apparatus designed for the synthesis and deposition of size-selected clusters for reactivity studies. Using these techniques, size selected manganese oxide, niobium oxide, tungsten oxide, copper molybdenum oxide, and copper zirconium oxide clusters were each studied for their ability to adsorb and decompose the organophosphorus nerve agent simulant dimethyl methylphosphonate. Advisor: Dr. Kit H. Bowen Committee: Dr. Howard Fairbrother Dr. Lan Cheng ii Acknowledgments I have been amazingly lucky to have the mentors and support that has allowed me, and even pushed me, to make it to this point. First, I’d like to thank my PhD advisor, Dr. Kit Bowen, who has given me every opportunity to succeed and become a better scientist and experimentalist. I recognize that my path to Johns Hopkins and to becoming a successful experimentalist was largely because he saw potential in me, and I could never thank him enough for that opportunity. Besides the important laboratory experience and mentorship he offered, I’d like to thank him for the opportunity to attend large conferences around the US and world, where experiences I had with collaborators and peers will be cherished forever. Second, I’d like to thank my graduate research committee members, Dr. Howard Fairbrother, Dr. Lan Cheng, and Dr. Art Bragg, for taking the time to be part of my graduate career. I’m particularly grateful to Dr. Fairbrother as well as his students for their support over the years. Next I would like to thank the members of my “sub-group”, the surface team, who have I have spent the last 3 years getting to know. I will forever be indebted to Dr. Zachary Hicks, our original sub-group leader, for the potential he saw in me and his decision to bring me into his project. His never-ending curiosity and drive were a wonderful example for a young scientist. Learning from and getting to know Linjie Wang has been one of the high points of my graduate career. She is a thoughtful and caring person, but as a scientist her power of deduction is without equal, and it has been a privilege to learn from and with her these last few years. Similarly, learning from Mike Denchy and watching him grow into an adept scientist the last couple years has been a privilege, his unwavering determination to fully understand the system or project at hand will continue to serve him well in life. In my short time with Ben Bilik, I have been impressed by his curiosity, and know that he will be iii extremely successful if he can apply that in the Bowen Lab, and similarly, Lucas Hansen’s theoretical prowess will make him a strong experimentalist. Throughout my 6 years in the Bowen lab, there is no one I have been closer to than Dr. Sandra Ciborowski. Her companionship since the very first day of graduate classes and the years of friendship and support since have been invaluable. She is a brilliant scientist and adept problem solver that I know will continue to impress others. Similarly, Mary Marshall was one of the first graduate students I worked closely with, and it has been a great experience to watch her grow into an adept experimentalist, whose advise I often seek, for both science and life questions. It has been gratifying to watch Zhaoguo Zhu become an extremely talented and well-rounded scientist, his personality will continue to brighten rooms wherever he goes. Rachel Harris is an extremely determined scientist and engineer, I have no doubt her tenacity will take her far after she is done at Johns Hopkins. My undergraduate research advisor Kris Hagel is responsible for introducing me to experimental physics, and I will always be grateful that he started that ball rolling. His enthusiasm and ingenuity set a high bar for any scientist. I’d like to thank the chemistry building manager, Boris Steinberg, who has been a great resource for work problems and life advice, and does an enormous amount of work behind the scenes to facilitate our research. My brother Robert for believing in me when no one, including myself, did. I’d like to thank my partner Allie for the endless adventures and unwavering support she has offered. And finally, my parents, without whom I would certainly not be here today. They provided me all the opportunity and skills that I could ever need, but it was their support along the way that I cherish most. iv Table of Contents Abstract .................................................................................................................. ii Acknowledgments ................................................................................................ iii List of Figures ..................................................................................................... viii I Atoms to Clusters ....................................................................................... 1 II Catalysis ..................................................................................................... 7 III Molecular Beams and Mass Spectrometry, a Historical Perspective ....... 11 III.1 Mass Spectrometry ............................................................................... 13 III.1.1 Magnetic Sector Mass Spectrometer ............................................. 15 III.1.2 Quadrupole Mass Spectrometer ..................................................... 18 IV Ion Sources for Cluster Beams ................................................................. 24 IV.1 Condensation and Cooling ................................................................... 25 IV.1.1 Supersonic Expansion ................................................................... 26 IV.2 Pulsed Arc Cluster Ionization Source (PACIS) ................................... 30 IV.3 Laser Vaporization Source ................................................................... 31 IV.3.1 Laser Vaporization Rod Source ..................................................... 33 IV.3.2 Laser Vaporization Disk Source .................................................... 37 IV.4 DC Magnetron Sputtering Source ........................................................ 39 V Ion Transport System ............................................................................... 45 V.1 Ion Guides ............................................................................................ 46 V.2 Electrostatic Optics .............................................................................. 52 V.2.1 Electrostatic Aperture ..................................................................... 52 v V.2.2 Electrostatic Quadrupole Bender .................................................... 55 V.2.3 Thin Plate Einzel Lens .................................................................... 58 VI Vacuum chambers and pumping system .................................................. 60 VI.1 Vacuum theory ..................................................................................... 60 VI.1.1 Differential Pumping ..................................................................... 63 VI.1.2 Vacuum Pumps .............................................................................. 63 VI.2 Cluster Deposition Pumping System ................................................... 67 VII Deposition and analysis system ............................................................... 74 VII.1 Deposition chamber ............................................................................ 74 VII.2 Analysis Techniques and Instrumentation .......................................... 76 VII.2.1 Residual Gas Analyzer ................................................................. 76 VII.2.2 Temperature Programmed Reaction/Desorption Spectroscopy ... 78 VII.3 Photoelectron Spectroscopy for Surface Analysis .............................. 82 VII.3.1 Electron Kinetic Energy Analyzer ............................................... 86 VII.3.2 Low Energy Electron Diffraction Spectroscopy .......................... 89 VII.3.3 Scanning Tunneling Microscope .................................................. 92 VIII Preliminary results of DMMP decomposition on novel metal oxide cluster compositions 95 VIII.1 Brief History of Chemical Weapons .................................................. 95 VIII.2 Development of Nerve Agents .......................................................... 96 VIII.2.1 Organophosphorus
Recommended publications
  • Cathode Rays 89 Cathode Rays
    Cathode Rays 89 Cathode Rays Theodore Arabatzis C The detection of cathode rays was a by-product of the investigation of the discharge of electricity through rarefied gases. The latter phenomenon had been studied since the early eighteenth century. By the middle of the nineteenth century it was known that the passage of electricity through a partly evacuated tube produced a glow in the gas, whose color depended on its chemical composition and its pressure. Below a certain pressure the glow assumed a stratified pattern of bright and dark bands. During the second half of the nineteenth century the discharge of electricity through gases became a topic of intense exploratory experimentation, primarily in Germany [21]. In 1855 the German instrument maker Heinrich Geißler (1815– 1879) manufactured improved vacuum tubes, which made possible the isolation and investigation of cathode rays [23]. In 1857 Geissler’s tubes were employed by Julius Pl¨ucker (1801–1868) to study the influence of a magnet on the electrical dis- charge. He observed various complex and striking phenomena associated with the discharge. Among those phenomena were a “light which appears about the negative electrode” and a fluorescence in the glass of the tube ([9], pp. 122, 130). The understanding of those phenomena was advanced by Pl¨ucker’s student and collaborator, Johann Wilhelm Hittorf (1824–1914), who observed that “if any ob- ject is interposed in the space filled with glow-light [emanating from the negative electrode], it throws a sharp shadow on the fluorescent side” ([5], p. 117). This effect implied that the “rays” emanating from the cathode followed a straight path.
    [Show full text]
  • Tracing the Recorded History of Thin-Film Sputter Deposition: from the 1800S to 2017
    Review Article: Tracing the recorded history of thin-film sputter deposition: From the 1800s to 2017 Cite as: J. Vac. Sci. Technol. A 35, 05C204 (2017); https://doi.org/10.1116/1.4998940 Submitted: 24 March 2017 . Accepted: 10 May 2017 . Published Online: 08 September 2017 J. E. Greene COLLECTIONS This paper was selected as Featured ARTICLES YOU MAY BE INTERESTED IN Review Article: Plasma–surface interactions at the atomic scale for patterning metals Journal of Vacuum Science & Technology A 35, 05C203 (2017); https:// doi.org/10.1116/1.4993602 Microstructural evolution during film growth Journal of Vacuum Science & Technology A 21, S117 (2003); https://doi.org/10.1116/1.1601610 Overview of atomic layer etching in the semiconductor industry Journal of Vacuum Science & Technology A 33, 020802 (2015); https:// doi.org/10.1116/1.4913379 J. Vac. Sci. Technol. A 35, 05C204 (2017); https://doi.org/10.1116/1.4998940 35, 05C204 © 2017 Author(s). REVIEW ARTICLE Review Article: Tracing the recorded history of thin-film sputter deposition: From the 1800s to 2017 J. E. Greenea) D. B. Willett Professor of Materials Science and Physics, University of Illinois, Urbana, Illinois, 61801; Tage Erlander Professor of Physics, Linkoping€ University, Linkoping,€ Sweden, 58183, Sweden; and University Professor of Materials Science, National Taiwan University Science and Technology, Taipei City, 106, Taiwan (Received 24 March 2017; accepted 10 May 2017; published 8 September 2017) Thin films, ubiquitous in today’s world, have a documented history of more than 5000 years. However, thin-film growth by sputter deposition, which required the development of vacuum pumps and electrical power in the 1600s and the 1700s, is a much more recent phenomenon.
    [Show full text]
  • Nanoscience Education
    Livre de Lyon Academic Works of Livre de Lyon Educational Sciences 2020 NANOSCIENCE EDUCATION Ruhan Benlikaya Balikesir University, [email protected] Follow this and additional works at: https://academicworks.livredelyon.com/edu_sci Part of the Education Commons Recommended Citation Benlikaya, Ruhan, "NANOSCIENCE EDUCATION" (2020). Educational Sciences. 35. https://academicworks.livredelyon.com/edu_sci/35 This Book is brought to you for free and open access by Livre de Lyon, an international publisher specializing in academic books and journals. Browse more titles on Academic Works of Livre de Lyon, hosted on Digital Commons, an Elsevier platform. For more information, please contact [email protected]. ACADEMIC STUDIES IN EDUCATIONAL SCIENCES Editor Prof. Dr. Hulya GUR Lyon 2020 Editor • Prof. Dr. Hulya GUR 0000-0001-8479-8811 Cover Design • Aruull Raja First Published • December 2020, Lyon ISBN: 978-2-38236-041-5 © copyright All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by an means, electronic, mechanical, photocopying, recording, or otherwise, without the publisher’s permission. The chapters in this book have been checked for plagiarism by Publisher • Livre de Lyon Address • 37 rue marietton, 69009, Lyon France website • http://www.livredelyon.com e-mail • [email protected] PREFACE This book provides a detailed and up-to-date overview of works in education, science and mathematics education. This book is informative for especially educators, reseachers, academics, postgraduate students, preservive teachers, teachers and school leaders own development. It gives suggestions to educators, reseachers, academics, postgraduate students, preservive teachers, teachers, school leadersand policy makers and so on..
    [Show full text]
  • FORMAT Bulletin
    Members’ Paper From IRPS Bulletin Vol 10 No 3 September/October, 1996 ONE HUNDRED YEARS OF ELECTRONS above hypothesis but also to the brilliant discoveries made in the closing years of the 19th century: that of X- Leif Gerwarda and Christopher Cousinsb rays by Wilhelm Conrad Röntgen in 1895 and that of radioactivity by Henri Becquerel in 1896. a. Department of Physics, Technical University of Denmark, Lyngby, Denmark Cathode rays occurs when electricity is discharged in a rarefied gas. At a given low pressure of the gas, rays are b. Department of Physics, University of Exeter, emitted from the negative pole, the cathode. The Exeter, UK cathode rays themselves are invisible, but they can be observed by the phosphorescence that they induce at the The search for the true nature of electricity led walls of the glass tube and by the shadows from objects to the discovery of the electron and the proof placed in their path. The cathode rays propagate in that it is a constituent of all atoms. These straight lines, but unlike ordinary light rays they can be achievements gave the scientists the first deflected by a magnetic field. definite line of attack on the constitution of the atom and on the structure of matter. The phenomena exhibited by the electric discharge in rarefied gas had long been familiar from studies by In a lecture on 'The Stability of Atoms' given to the Royal Julius Plücker, Wilhelm Hittorf, Eugen Goldstein and Society of Arts in 1924, Ernest Rutherford said: other physicists. In a lecture delivered before the British Association at the Sheffield Meeting in 1879, William The trend of physics during the past twenty-five years has Crookes first used the expression radiant matter or been largely influenced by three fundamental discoveries matter in the ultra-gaseous state, to explain the made in the closing years of the nineteenth century.
    [Show full text]
  • Unit II. the Atom: Early Models
    Unit II. The Atom: Early Models READING ASSIGNMENT 1: Read Ch. 5 p107-112. Build a time line showing the scientists who contributed to our understanding of the atom and their contributions. You will add to this time line as the unit progresses. I. A History of the Atomic Theory- “How Small is Small” A. Democritus- Greek- “atomos” – indivisible -“All matter is composed of indivisible units.” Atoms of Salt, Water & Iron. The chemical properties were conserved in the structure of the atoms B. John Dalton- English Physicist (1766-1844) . See a section of Dalton's book as well as an excerpt of his writings. Dalton’s Atomic Theory- 1. All elements are composed of atoms and the atom is the smallest piece of that element 2. All atoms of the same element are the same. These atoms then have the same mass. 3. Atoms of different elements combine in whole number ratios producing compounds. a. Law of Definite Proportions ( Law of Constant Composition) - All compounds are composed of specific ratios of elements. -This was actually coined by Joseph Proust, which Dalton used to develop his theory. 4. Chemical reactions occur when atoms are separated, joined or rearranged. ASSIGNMENT 1. Quiz over Dalton's Atomic Theory II. Composition of the Atom & Historical Atomic Models Simplified View of the Subatomic Particles. A. Electron- negative particles, very small 1. William Crookes (1832-1919)- Cathode Ray Tube- (Crookes Tube) -cathode rays- a. travel from cathode to anode in straight lines b. heated metals placed in path of rays c. deflected by electric & magnetic charges- shows rays are made of negative particles.
    [Show full text]
  • Dissertation
    Dissertation submitted to the Combined Faculties for the Natural Sciences and for Mathematics of the Ruperto-Carola University of Heidelberg, Germany for the degree of Doctor of Natural Sciences Put forward by Master of Science Fabian Heiße Born in Zschopau Oral examination: October 16th, 2019 High-precision measurement of the proton’s atomic mass First referee: Priv. Doz. Dr. Wolfgang Quint Second referee: Prof. Dr. Selim Jochim Groß sind die Werke des HERRN; wer sie erforscht, der hat Freude daran. Die Bibel, Buch der Psalmen, Kapitel 111 Vers 2. Hochpräzise Messung der atomaren Masse des Protons Zusammenfassung - Im Rahmen dieser Doktorarbeit wurden große Teile des neuen Penningfallen-Experimentes LIONTRAP (Light-Ion Trap) aufgebaut, das gesamte Experiment erstmalig in Betrieb genommen und vollständig charak- terisiert. Weiterhin wurden die ersten beiden Messkampagnen zur Bestimmung der atomaren Masse des Protons und des Sauerstoffatoms durchgeführt. Das LIONTRAP Experiment ist speziell für die Massenbestimmung von leich- ten Ionen optimiert. Dabei wird die Zyklotronfrequenz eines hochgeladenen Kohlenstoffions mit der des zu messenden Ions verglichen, um über dieses Zyk- lotronfrequenzverhältnis die atomare Masse des Ions zu extrahieren. Dafür wurde in LIONTRAP die harmonischste zylindrische Penningfalle realisiert, welche bisher in der Literatur beschrieben wurde. In der ersten Messkampagne wurde die atomare Masse des Protons mit einer bisher unerreichten relativen Genauigkeit von 3 × 10−11 bestimmt. Der neue Messwert ist nicht nur einen Faktor drei genauer als der zum Zeitpunkt der Messung gültige Literaturwert, sondern weist auch eine Diskrepanz von drei Standardabweichungen dazu auf. Zusätzlich wurde auch noch der zweitgenauste Wert für die Sauerstoffmasse bestimmt, welcher mit dem Literaturwert über- einstimmt.
    [Show full text]
  • The Cathode Ray Tube Site, Crookes Tubes. 09/20/2006 09:21 AM
    The Cathode Ray Tube site, Crookes tubes. 09/20/2006 09:21 AM The Cathode Ray Tube site electronic glassware Crookes tubes history and Physics Instruments The scientist Sir William Crookes paved the way for many discoveries. He worked in his own laboratory in PREV HOME NEXT London where he did all of his experiments with different types of near vacuum tubes. A lot of Crookes tubes stood at the base of further discoveries like the X-ray tube and the Braun tube which developed later on into our well known TV tube. German glassblowers like Otto Pressler, Emil Gundelach and Müller-Uri made many types of Crookes, Hittorf and Geissler tubes in the beginning of the 20th Century. The tubes were sold to schools and universities for classroom demonstration by companies like Max Kohl and Leybold. In WW II the Pressler factory was bombed but they managed to go on, after the war the name changed in VEB and produced then manly radiometers for hard western currency. On the website of Jogis-Röhrenbude you can find the complete Pressler story. The biography of Sir William Crookes can be found on the website of the University of Oxford For everyone who likes to know more about the background of this old tubes, there is now a new book in German language. Check this website for more info. Caution. Sir William Crookes When these tubes are activated with high 1832-1919 voltage a small amount of soft X-Ray's are produced ! Don't use tensions more than 5000 Volts. The Maltese Cross tube is one of the most famous Crookes tubes.
    [Show full text]
  • From Electrons to Quarks
    From electrons to quarks –- 1st part: the development of Particle Physics Outline: ● What is particle physics -- why do it? ● Early days – atoms, electron, proton ● Models of the atom – Thomson, Rutherford, Bohr ● Cosmic rays ● Detectors – scintillators, cloud chamber, emulsion, bubble chamber, spark chamber ● More particles: neutron, positron ● Muon, pion ● Kaon – “strange particles” ● Webpages of interest http://www-d0.fnal.gov (Fermilab homepage) http://sg1.hep.fsu.edu/~wahl/Quarknet/index.html (has links to many particle physics sites) http://www.fnal.gov/pub/tour.html (Fermilab particle physics tour) http://ParticleAdventure.org/ (Lawrence Berkeley Lab.) http://www.cern.ch (CERN -- European Laboratory for Particle Physics) What is particle physics? ● particle physics or high energy physics is looking for the smallest constituents of matter • (the “ultimate building blocks”) and for the fundamental forces between them; aim is to find description in terms of the smallest number of particles and forces (“interactions”) ● at given length scale, it is useful to describe matter in terms of specific set of constituents which can be treated as fundamental; at shorter length scale, these fundamental constituents may turn out to consist of smaller parts (be “composite”) ● concept of “smallest building block” changes in time: in 19th century, atoms were considered smallest building blocks, early 20th century research: electrons, protons, neutrons; now evidence that nucleons have substructure - quarks; going down the size ladder: atoms -- nuclei -- nucleons -- quarks – preons, strings ???... ??? WHY CAN'T WE SEE ATOMS? ● “seeing an object” = detecting light that has been reflected off the object's surface ● light = electromagnetic wave; ● “visible light”= those electromagnetic waves that our eyes can detect ● “wavelength” of e.m.
    [Show full text]
  • Mass Spectrometry—The Early Years
    International Journal of Mass Spectrometry 349–350 (2013) 3–8 Contents lists available at ScienceDirect International Journal of Mass Spectrometry j ournal homepage: www.elsevier.com/locate/ijms Mass spectrometry—The early years ∗ K.S. Sharma Department of Physics and Astronomy, University of Manitoba, Winnipeg, Canada R3T 2N2 a r t i c l e i n f o a b s t r a c t Article history: In 1913 J.J. Thomson constructed his famous positive-ray parabola apparatus at Cambridge and discovered Received 21 March 2013 two isotopes of neon. He subsequently discovered other isotopes. His work confirmed the concept of Received in revised form 22 May 2013 isotopes and provided an explanation for deviations of atomic weights determined through chemical Accepted 23 May 2013 techniques from the “whole number rule”. This achievement marks the beginning of the field of mass Available online 5 June 2013 spectroscopy which is celebrating its 100th anniversary in 2013. His student Aston extended this work by constructing an instrument that we properly term a mass spectrometer and contributed significantly to Keywords: our first glimpses into the binding energy of the nucleus. Independently, Dempster constructed a similar Atomic masses instrument at the University of Chicago also provided contributions to our knowledge of nuclear masses. Nuclear physics The birth of this field of measurement has its roots in nuclear physics and chemistry. It has grown to be Mass spectrometry History the driver of a huge international industry and is utilized as a tool in almost every field of science. This Instrumental paper will recount the early days of the field.
    [Show full text]
  • Vacuum Science & Technology Time Line, 1500–1799
    Vacuum Science & Technology Time Line, 1500–1799 Time Line Color Code Key Related scientific developments Anders Celsius Vacuum devices (1701-1744) Radio & electronics Mayow Apparatus ca. 1669 suggests new temperature Otto von Guericke scale. This scale is revised Historical events Magdeberg hemisphere John Mayow (1641-1679) Rene Descartes in 1745 by Carl von Linn¾ (1707-1778) Vacuum gauges demonstration suggests that air may be (1596-1650) 1654 made up of two different gases 1742 Vacuum pumps in his Principa Philosophiae Experiments by Richard 1674 suggests that a vacuum Captions Townley (1628-1707) and Jakob Hermann cannot exist Vacuum device manufacturing Henry Power (1623-1668) (1678-1733) 1644 establish PV law for expansion postulates that pressure is (later called Boyle’s Law or proportional to density and Marriotte’s Law) to the square of the average Ferdinand II, 1660 velocity of the particles Grand Duke of Tuscany, in motion invents liquid-in-glass 1716 thermometer In response to Boyle’s ideas, 1641 Franciscu Linus (1595-1675) Otto von Guericke’s suggest the properties of a air pump vacuum is due to invisible thread-like Hero of Alexandria writes 1672 “funiculus” that strive to hold Pneumatias summarizing nearby objects together what is then known about Evangelista Torricelli 1660 syphons, pumps, etc. (1608-1647) Johannes van Helmont ~150 B.C.E. Substitutes mercury for George Ernts Stahl defines “gas” (Flemish = chaos) water in overhead pump introduces idea of to mean an air-like substance 1644 phlogiston as the 1620 agent of
    [Show full text]
  • Tuesday, November 08, 2011 Eugen Goldstein Was Born on September 5
    Eugen Goldstein was born on September 5, 1850 in Gleiwitz, Upper Silesia, now Gliwice Poland. He studied physics Breslau for one year, then under Hermann von Helmoltz in Berlin, who was also a physicist. He worked on research at the Berlin Observatory from 1878 until 1890 ("Goldstein, eugen," ), (Soylent Communications, 2011) . At the Berlin Observatory he worked on the relations between electricity and cosmic phenomena and managed to reproduce comet tails in gas discharge tubes (Hedens M. 2002). In 1927 he was appointed head of the astrophysical section of Potsdam Observatory ("Goldstein, eugen," ). The work that Goldstein did with cathode rays was very important to his future experiments, during one these experiments he discovered the proton. Goldstein proved that cathode rays could induce chemical reactions that are normally caused by sunlight, known as photochemical reactions, he also proved that the features of the rays were not due to the material of which the cathode was made (Oracle think quest). Eugen Goldstein died on December 25, 1930 in Berlin, Germany, he was eighty years old. Before Goldstein’s experiment it was believed that the atom resembled a billiard ball, a small solid sphere. It was believed that the atoms had had different pieces and was not a whole, as had been suggested by John Dalton. Before Goldstein’s discovery it was believed that the atom was made up of electrons that were meshed together (Carpi, 2003). During his experiment Goldstein believed that since an atom was electrically neutral there must be a balancing particle, since they had already discovered the existence of the negatively charged particle there had to be a positive particle (Learning Hub).
    [Show full text]
  • – by Julia Cipo, Holger Kersten –
    THE GAS DISCHARGE PHYSICS IN THE 19th CENTURY (PART II) – by Julia Cipo, Holger Kersten – Johann Wilhelm Gotthilf-Eugen Hittorf Goldstein * March 17th, 1824 in Bonn, Germany * September 5th, 1850 in Gleiwitz, Poland † November 28th, 1914 in Münster, Germany † December 25th, 1930 in Berlin, Germany Johann Wilhelm Hittorf was a german physicist, chemist and a student and as- Gotthilf-Eugen Goldstein was a german physicist, known for his work sistant of Julius Plücker. He continued the work of Plücker and kept using the on the electrical discharge phenomena and on the cathode rays. He geissler tubes and the induction apparatus created by Heinrich Daniel Rühm- also discovered the canal rays and was a student and friend of the *3 korff. As well as Faraday he used thinned gases, watching their glow discharges physicist Hermann von Helmholtz, and the spectra of each element. He extended the geissler tube by adding poten- who encouraged him in this researches. After naming the “cathode rays” this way tial probes with the purpose of studying the voltage fl ow. This way Hittorf could *1 because of their source: the cathode, Goldstein focussed on studying the proper- describe that “the glowing was a process, where a current transition between ties of them. So in 1876 he found out, that these rays were emitted perpendicular the gas particles and the ones in the cathode takes place”. Then he studied the to the cathode surface. In 1886 he discovered the anode rays, which were gen- rays from the cathode to the anode, by calling them “the rays of the negative light” because of the current of nega- erated by positively charged particles after the electrons were removed from the tive charges.
    [Show full text]