Pulsed Breakdown Phenomena in Partial Vacuum

Total Page:16

File Type:pdf, Size:1020Kb

Pulsed Breakdown Phenomena in Partial Vacuum PULSED BREAKDOWN PHENOMENA IN PARTIAL VACUUM by Zhenhong Li A thesis submitted to the Graduate Faculty of Auburn University in partial fulfillment of the requirements for the Degree of Master of Science Auburn, Alabama December 8, 2012 Copyright 2012 by Zhenhong Li Approved by Hulya Kirkici, Chair, Professor of Electrical and Computer Engineering Thaddeus Roppel, Associate Professor of Electrical and Computer Engineering Michael Baginski, Associate Professor of Electrical and Computer Engineering Abstract In this thesis, the pulse generation and pulsed breakdown phenomena have been studied in detail. Pulsed power is widely used in food processing, biotechnology, military defense, and industrial applications. The first part of this work covers the simulation and analysis of common high voltage DC and pulse generator circuits. Then high power switching techniques which are essential to the generation of pulsed power are also explored. Due to the rapid development of high energy laser and accelerator, high power switches capable of handling powers up to terawatts are in great demand in industry. Pseudospark switch using the hollow cathode effect is an example for these applications. Pseudospark discharge is triggered by many means and is challenging. Carbon Nanotubes (CNTs) triggering is achieved in pseudospark switches operated in helium and tested in the laboratory. The delay time of the triggered breakdown with several CNTs samples under different trigger voltages is summarized. As the second part of this research, the pulsed breakdown phenomena in partial vacuum are investigated thoroughly. Solid insulators are widely employed in power systems operating in atmospheric pressure and partial vacuum. However, the hold-off capability of an insulator in vacuum is limited by the surface flashover problem due to the cathode ‗triple-junction‘ effect. This is a common problem for space power and aerospace power systems. In this work, the surface flashover characteristics of nanodielectric materials composed of cast epoxy resin mixed with nano-dielectric particles in partial vacuum are studied. The samples except the control samples are made by adding nanoscale Al2O3 or TiO2 powder with predetermined ratios into the ii epoxy resin with known properties. The samples are cylindrical in shape (2.5 cm in diameter and 1 cm in thickness) and varying electrode configurations and spacing are used in this study. The surface flashover characteristics of the samples are investigated using both DC and 20 kHz pulsed-unipolar signals separately. The frequency and duty cycle of the pulsed signal are also varied in the experiments in order to obtain a clearer understanding of pulsed surface flashover in partial vacuum. Initially the cylindrical samples are sandwiched between two parallel plate electrodes, and the voltage, current, and light emission waveforms during the flashover events are recorded and analyzed. As a second test set, the electrodes laterally placed on the samples‘ flat surface and surface breakdown experiments conducted and comparisons to the parallel plate case are made. iii Acknowledgments The author would like to thank his advisor Dr. Hulya Kirkici for her patience and guidance on this research work during the past two years. Without her support this work would be impossible to achieve. The author would like to thank Dr. Baginski and Dr. Roppel for serving as the committee members. The author also would like to express appreciation to Ms. Linda Barresi and Mr. Calvin Cutshaw for their material assistance during this work. Thanks are also due to his group members, especially Rujun Bai, Haitao Zhao and Huirong Li who help him run the experiments over and over again. Finally, the author wishes to thank his mother and sisters, for their unfailing support and understanding. ξ Work partially sponsored by AFOSR grant # AF-FA9550-08-10051 iv Style manual or journal used Graduate School's Thesis and Dissertation Guide Computer software used Microsoft Office 2007 v Table of Contents Abstract ......................................................................................................................................... ii Acknowledgments ....................................................................................................................... iv List of Tables ............................................................................................................................... ix List of Figures ............................................................................................................................... x Chapter I INTRODUCTION & BACKGROUND ....................................................................... 1 1.1 Introduction ................................................................................................................ 1 1.2 Electrical Breakdown of Gases ................................................................................... 4 1.2.1 Townsend Mechanism ....................................................................................... 4 1.2.2 Paschen‘s Law ................................................................................................... 6 1.2.3 High Frequency Breakdown .............................................................................. 9 1.2.4 Pulsed Breakdown ........................................................................................... 11 1.2.5 Glow Discharge ............................................................................................... 13 1.2.6 Hollow Cathode Discharge .............................................................................. 14 1.3 Pulsed Power ............................................................................................................. 15 1.3.1 Pulsed Power Generation ................................................................................. 15 1.3.2 Power Switches ................................................................................................ 17 1.4 Surface Flashover...................................................................................................... 20 1.4.1 Space Environment & Spacecraft .................................................................... 20 1.4.2 Surface Flashover in Vacuum & Partial Vacuum ............................................ 22 vi Chapter II HIGH VOLTAGE GENERATOR SIMULATION & APPLICATION ................... 24 2.1 High Voltage DC Power Supply .............................................................................. 24 2.2 High Voltage Pulse Generator ................................................................................. 27 2.3 Application: CNTs Initiated Hollow Cathode Discharge ......................................... 31 2.3.1 Experiments Setup ........................................................................................... 33 2.3.2 Experiment Results & Discussions .................................................................. 33 Chapter III SURFACE FLASHOVER IN PARTIAL VACUUM ............................................. 36 3.1 Sample Preparation .................................................................................................. 36 3.2 Experimental Setup ................................................................................................... 38 3.3 Experimental Procedure ............................................................................................ 40 3.4 Breakdown Voltage versus Pressure ......................................................................... 41 3.4.1 DC Breakdown Voltage versus Pressure ......................................................... 43 3.4.2 Pulsed Breakdown Voltage versus Pressure .................................................... 46 3.5 Electrode Configurations Effect on Breakdown Voltage ......................................... 49 3.6 Breakdown Voltage versus Pulse Parameters ........................................................... 51 3.6.1 Breakdown Voltage versus Frequency ............................................................ 52 3.6.2 Breakdown Voltage versus Duty Cycle ........................................................... 54 3.7 Surface Effect on Breakdown Voltage ..................................................................... 54 3.8 Conclusions ............................................................................................................... 57 Chapter IV CONCLUSIONS ...................................................................................................... 59 References ................................................................................................................................... 61 Appendix A SPICE Listing for Pulse Generator Circuit .......................................................... A-1 Appendix B Surface Breakdown Voltages vs. Pressure (Sandwiched Electrode) .................... B-1 vii Appendix C Surface Breakdown Voltages vs. Pressure (Lateral Electrode) ............................ C-1 Appendix D Surface Breakdown Voltages vs. Pressure (Machined Samples) ......................... D-1 Appendix E Surface Breakdown Voltages vs. Frequency ........................................................ E-1 Appendix F Surface Breakdown Voltages vs. Duty Cycle ........................................................ F-1 viii List of Tables Table 2.1 CNTs sample list ......................................................................................................... 34 Table 3.1 Nanodielectric sample
Recommended publications
  • Lecture 09 Closing Switches.Pdf
    High-voltage Pulsed Power Engineering, Fall 2018 Closing Switches Fall, 2018 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University Switch fundamentals The importance of switches in pulsed power systems In high power pulse applications, switches capable of handling tera-watt power and having jitter time in the nanosecond range are frequently needed. The rise time, shape, and amplitude of the generator output pulse depend strongly on the properties of the switches. The basic principle of switching is simple: at a proper time, change the property of the switch medium from that of an insulator to that of a conductor or the reverse. To achieve this effectively and precisely, however, is rather a complex and difficult task. It involves not only the parameters of the switch and circuit but also many physical and chemical processes. 2/44 High-voltage Pulsed Power Engineering, Fall 2018 Switch fundamentals Design of a switch requires knowledge in many areas. The property of the medium employed between the switch electrodes is the most important factor that determines the performance of the switch. Classification Medium: gas switch, liquid switch, solid switch Triggering mechanism: self-breakdown or externally triggered switches Charging mode: Statically charged or pulse charged switches No. of conducting channels: single channel or multi-channel switches Discharge property: volume discharge or surface discharge switches 3/44 High-voltage Pulsed Power Engineering, Fall 2018 Characteristics of typical switches A. Trigger pulse: a fast pulse supplied externally to initiate the action of switching, the nature of which may be voltage, laser beam or charged particle beam.
    [Show full text]
  • CATHODE LIGHT STRIP Single-Lamp Modular Cold Cathode Fluorescent Fixture • Model CLS
    CATHODE LIGHT STRIP Single-Lamp Modular Cold Cathode Fluorescent Fixture • Model CLS U.S. and international patents pending. Conference Room, Anadarko Petroleum Photo: Eric Long Washington, DC Architect: Davis Carter Scott © 2002 Cathode Lighting Systems Inc. 8020 Queenair Drive, Gaithersburg, MD 20879 • ph: 301 921 4120 • fax: 301 963 3050 e-mail: [email protected] • website: www.CathodeLightingSystems.com INALLY, THE LOOK OF A CUSTOM COLD CATHODE INSTALLATION IN AN OFF- FTHE-SHELF MODULAR SYSTEM. OUR ARCHITECTURAL-GRADE COLD CATHODE FIXTURE MAKES DESIGNING SEAMLESS SPECIAL EFFECTS LIGHTING EASIER THAN EVER. LAMPS ARE ILLUMINATED FROM END TO END, CREATING TRUE SHADOWLESS LINEAR FLUORESCENT LIGHT. STANDARD INTEGRAL DIMMING BALLASTS, SIMPLE INSTALLATION, AND A LAMP LIFE OF 50,000 HOURS MAKE CATHODE LIGHT STRIP THE CLEAR CHOICE WHEN THE HIGHEST-QUALITY LONG-LIFE LIGHTING EFFECTS ARE REQUIRED. CATHODE LIGHT STRIP, PERFECT ELEGANCE WAS NEVER SO EASY. Model CLS-4 shown equipped with a warm white (30TC) lamp. FEATURES: • SEAMLESS ILLUMINATION: Lamp illumination is • DIMMABLE: Fixtures are supplied standard with integral complete, from end to end, with no dark spots or socket dimmable ballasts. shadow. • ALL FIXTURES DIM AT THE SAME RATE: Cathode Light • ULTRA-LONG LAMP LIFE: The cold cathode lamp has Strip has been engineered to dim evenly from fixture to a life of 50,000 hours +. fixture, regardless of length or combinations of differing • LOW PROFILE: Just 2 5/8" wide and 3 1/2" tall, much lengths. smaller than traditional custom cold cathode. • STREAMLINED AND LIGHTWEIGHT: Fixtures are • AVAILABLE IN A VARIETY OF LENGTHS: With eight made from satin anodized architectural-grade, snap-fit standard sizes available, fixtures can be combined or aluminum extrusion.
    [Show full text]
  • X-Ray Spectra from a Brass-Target Plasma Triode Abstract in This
    X-ray Spectra from a Brass-target Plasma Triode Eiichi SATO, Haruo OBARA, Toshiyuki ENOMOTO, Etsuro TANAKA Hidezo MORI, Toshiaki KAWAI, Toshio ICHIMARU, Akira OGAWA Shigehiro SATO, Kazuyoshi TAKAYAMA Jun ONAGAWA I) Department of Physics , Iwate Medical University 2) Department of Radiological Technology , College of Medical Science, Tohoku University 3) The 3rd Department of Surge ry, Toho University School of Medicine 4) Department of Nutrition al Science, Faculty of Applied Bioscience, Tokyo University of Agriculture 5) Department of Cardiac Physiology , National Cardiovascular Center Research Institute 6) Electron Tube Division #2, Hamamatsu Photonics K. K. 7) Department of Radiologi cal Technology, School of Health Sciences, Hirosaki University 8) Department of Neurosurgery , School of Medicine, Iwate Medical University 9) Department of Microbiolog y, School of Medicine, Iwate Medical University 10) Tohoku University Biomedical Engineering Research Organization II) Department of Electronics , Faculty of Engineering, Tohoku Gakuin University Research Code No.: 200, 204.1 Keywords:Flash x-ray,Brass target, Weaklyionized linear plasma, Characteristicx-rays, Absorptionof zinc Kj3rays Abstract In this paper, we describe a recentlydeveloped table-top plasma x-ray generator utilizing a brass-targettriode, which we used in preliminary experiments for the superpositionof K-series characteristicx-rays in weakly ionized plasma and for producing their higher harmonics. In the plasma flash x-raygenerator, a 200 nF condenser was charged,and flash x-rays were producedby discharging.The x-ray tube was a demountabletriode with a brass target containing65% copper and 35% zinc by weight, and a turbomolecularpump evacuatedair from the tube with a pressure of 1 mPa. Targetevaporation led to the formationof weakly ionized linear plasma, consistingof metal ions and electrons,around the rod target, and intense characteristicx-rays were produced.
    [Show full text]
  • G-Tran Series Sensor Unit Model Sc1 Cold-Cathode Ion
    No. SK00-8431-EI-023-03 G-TRAN SERIES SENSOR UNIT MODEL SC1 COLD-CATHODE ION GAUGE INSTRUCTION MANUAL This manual is for the SC1 cold-cathode ion gauges of the following serial numbers. Serial No. 02300G and higher Read this manual before operation and keep it at hand for immediate reference. Components Division, ULVAC , Inc. 2500 Hagizono, Chigasaki City, Kanagawa-ken, Japan http://www.ulvac.co.jp/ Prior to Operation Upon receipt of this gauge, make sure that it is the correct model you ordered and that it is not damaged in transit. Read this instruction manual before installing, operating, inspecting, or maintaining the product and fully understand the safety precautions, specifications and operating procedures regarding the product. The copyright of this instruction manual is held by ULVAC, Inc. You are prohibited from copying any portion of this instruction manual without the consent of ULVAC Inc. You are also prohibited from disclosing or transferring this instruction manual to third parties without the express written consent of ULVAC Inc. The contents described in this instruction manual are subject to change without prior notice because of changes in specifications or because of product improvements. Safety Denotations Safety symbols are used throughout this instruction manual to call the operator's attention to safety. The terminology used in safety symbols is classified below. Indicate status of urgency of danger when failure to comply with DANGER results in serious personal injury or death The work ignoring this warning will lead to serious damage to human life or factory facility (including this equipment) at a high probability.
    [Show full text]
  • MP1010B Cold Cathode Fluorescent Lamp Driver the Future of Analog IC Technology
    MP1010B Cold Cathode Fluorescent Lamp Driver The Future of Analog IC Technology DESCRIPTION FEATURES The MP1010B is a power solution IC that offers • Integrated Power Switches a true complete solution for driving a Cold • 6.0V to 23V Variable Supply Voltage with Cathode Fluorescent Lamps (CCFL). This Regulated Lamp Current. Power IC converts unregulated DC voltage to a • Rated 12W Power Output at 12V Input nearly pure sine wave required to ignite and • Open Lamp Regulation operate the CCFL. Based on proprietary power • Current and Voltage Feedback Control topology and control techniques it greatly • Logic Level Burst Mode Control increases the power conversion efficiency. • Supports Open/Short Lamp Protection EVALUATION BOARD REFERENCE • Soft-Start Board Number Dimensions • Short Circuit Protected Output • High Energy Start Pulse EV1010B-00A 3.75”X x 0.4”Y x 0.25”Z • Analog and Burst Mode Dimming APPLICATIONS • LCD Backlight Inverter for Notebook Computers • Web Pads, GPS, Desktop Displays, Portable DVD, Car Video Display Systems “MPS” and “The Future of Analog IC Technology” are Registered Trademarks of Monolithic Power Systems, Inc. The MP1010B is covered by US Patents 6,633,138, 6,316,881, 6,114,814. TYPICAL APPLICATION Rs Cft2 Rdamp Cft1 Cref N1 CbaR Ccomp CbtR Rft Cp N/A 20 19 18 17 16 15 14 13 12 11 HV IN FT FB OL 2 REF BSTR OUTR PGND AGND COMP Rbosc 1 MP1010B T1 CN1 BR IL BOS T/B EN DR IN OUTL PGND BSTL 1 2 3 4 5 6 7 8 9 J1 10 ABRT 5 Rabr Cabr CbtL DBRT 4 Cdrv Rbdr EN 3 Cisb Ren1 N/A Cs1 Cs2 Rlfb Resd Cen Cdbr Rbleed Ren2 CbaL Cbosc Risb Csfb Rsfb GND 2 Cba2 F1 / 1A Cba1 VBATT 1 FUSE MP1010B Rev.
    [Show full text]
  • Letter Circular 817: Fluorescent Lamps
    . RPT : RMC U. S. DEPARTMENT OF COMMERCE Letter IV- 3 NATIONAL BUREAU OF STANDARDS Circular WASHINGTON 25 LC-817 ‘February 4, 1946 ^^(Sup^geding FLUORESCENT LAMPS Contents^" - O* _ , Page I. Introduction . ........ jg*,. ..... 1 II. Work of the National Bureau- of, Standards on Fluorescent Lamps ...... .X ........ 4 III. Description of the . Lamp\ . ^ 4 IV. General Information .... ...... 3 V. Does the Fluorescent Lamp Have Any Deleterious Effect on Vision or the Eye? 4 VI. Bibliography .......... 6 I . Introduction The development of fluorescent lamps and their possibilities for general and decorative lighting purposes have brought many requests for information to the Bureau. This letter circular has been prepared to answer such inquiries. It contains information which has been accumulated in answering these letters, but is not an exhaustive treatise on the subject. II Work of the National Bureau of Standards on Fluorescent Lamps. , The development of fluorescent lamps by their manufacturers is progressing so rapidly that, although the Bureau has studied the radiation from these lamps, as discussed in Section V, it has as yet made no extensive tests to compare the efficiencies or costs of operation of fluorescent and incandescent lamps. Such information is given by the manufacturers and is referred to below. A letter circular on Fluorescence and Phosphorescence, LC-550, was issued by the Bureau under date of April 1, 1939; it is available, without cost, upon written request. Ill Description of Lamps The most commonly used type of fluorescent lamp is made in the form of a tubular bulb with a filament- type electrode sealed in each end.
    [Show full text]
  • High Speed Plasma Diagnostics for Laser Plasma Interaction and Fusion Studies
    Sadhan& Vol. 24, Part 6, December 1999, pp. 513 549. ~' Printed in India High speed plasma diagnostics for laser plasma interaction and fusion studies V N RAI, M SHUKLA, H C PANT and D D BHAWALKAR Laser Programme, Centre for Advanced Technology, PO CAT, Indore 452 013, India e-mail: [email protected] MS received 26 February 1998; revised 25 May 1999 Abstract. Laser plasma interaction and fusion studies involve many high speed plasma diagnostics to determine the various parameters for explaining the physical processes taking place in plasma. Detection and analysis of short-term or transient radiations (X-ray and visible) are the bases for diagnosing the physical processes occurring during laser-plasma interaction or similar radiation-emitting processes. This paper reviews the development of various high speed plasma diagnostics which are not only applicable in determining the temporal, spatial and spectral properties of X-rays for this purpose but also have wide use in various other fields of research. Keywords. Laser-plasma interaction; fusion studies; transient radiations; high speed plasma. 1. Introduction Interaction of a high intensity laser light with matter (solid target) first vaporizes material from the surface which ultimately gets converted into plasma (ionized gas). This laser produced plasma expands into the vacuum where propagation of laser light is modified by the free electrons present in the plasma (Jacob et al 1976; Cairn & Sanderson 1980; Max 1982; Kruer 1988; Radziemski & Cramers 19891. The plasma formed by a high intensity or small time duration laser has very steep density and temperature gradients as compared to the plasma formed by the low intensity or long time duration laser.
    [Show full text]
  • INFORMATION CIRCULAR Original: ENGLISH (Unofficial Electronic Edition) ______
    INF INFCIRC/254/Rev.3/Part 2*/ 24 February 1998 International Atomic Energy Agency GENERAL Distr. INFORMATION CIRCULAR Original: ENGLISH (Unofficial electronic edition) ___________________________________________________________________________ COMMUNICATION RECEIVED FROM CERTAIN MEMBER STATES REGARDING GUIDELINES FOR THE EXPORT OF NUCLEAR MATERIAL, EQUIPMENT AND TECHNOLOGY Nuclear-related Dual-use Transfers 1. The Director General has received notes verbales dated 30 September 1997 from the Resident Representatives to the Agency of Argentina, Australia, Austria, Belgium, Bulgaria, Canada, the Czech Republic, Denmark, France, Germany, Greece, Hungary, Ireland, Italy, Japan, Republic of Korea, New Zealand, Norway, Poland, Portugal, Romania, the Russian Federation, the Slovak Republic, South Africa, Spain, Sweden, Switzerland, Ukraine, the United Kingdom of Great Britain and Northern Ireland, and the United States of America relating to the export of nuclear material, equipment and technology. 2. The purpose of the notes verbales is to provide further information about the Guidelines for Transfers of Nuclear-related Dual-use Equipment, Material and related Technology in accordance with which the relevant Governments act. 3. In the light of the wish expressed at the end of each note verbale, the text of the notes verbales is attached. The attachment to these notes verbales is also reproduced in full. _____________________ */ INFCIRC/254/Rev.3/Part 1 contains Guidelines for Nuclear Transfers ANNEX NOTE VERBALE The Permanent Mission of [Member State] presents its compliments to the Director General of the International Atomic Energy Agency and has the honour to refer to its [relevant previous communication(s)] concerning the decision of the Government of [Member State] to act in accordance with the Guidelines for Transfers of Nuclear-Related Dual-Use Equipment, Material and Related Technology currently published as document INFCIRC/254/Rev.2/Part 2/MOD.
    [Show full text]
  • Mercury in Cold Cathode Fluorescent Lamps for General Lighting Purposes (Category 5)
    EUROPEAN COMMISSION DIRECTORATE-GENERAL ENVIRONMENT Directorate G - Sustainable Development and Integration ENV.G.4 - Sustainable Production & Consumption DIRECTIVE 2011/65/EU1 ON THE RESTRICTION OF THE USE OF CERTAIN HAZARDOUS SUBSTANCES IN ELECTRICAL AND ELECTRONIC EQUIPMENT (ROHS). REQUESTS FOR ADDITIONAL EXEMPTION PROPOSALS FOR FURTHER EXEMPTIONS FROM THE REQUIREMENTS OF ARTICLE 4(1) OF DIRECTIVE 2011/65/EU FOR SPECIFIC APPLICATIONS OF LEAD, MERCURY, CADMIUM, HEXAVALENT CHROMIUM. Mercury in cold cathode fluorescent lamps for general lighting purposes (Category 5). Submitted by: ANIE Federazione with one of its federated associations - Associazione Nazionale Produttori Illuminazione ANIE Federazione represents the electrotechnical and electronic companies operating in Italy. With its 10 Associations, ANIE unites strategic players to deliver significant support to the growth of the national industry network and to contribute to its success on international markets. The Federation promotes the competitiveness of member companies with reference to different production factors. It maintains relations with Italian and international authorities and institutions to protect the sector’s interests. Information: Criteria Please provide supporting technical and scientific evidence a) Name address and contact ANIE Federazione details of the applicant; Via Vincenzo Lancetti, 43 20158 Milano, Italy Phone: +39 02.3264.317 Fax: +39 02.3264.212 b) Information on the material or Specific constructional characteristics for CCFLs for General component and the specific Lighting purposes: uses of the substance in the 1 OJ L 174, 1.7.2011, p. 88 1 Information: Criteria Please provide supporting technical and scientific evidence material and component for 1. Dimensions: Lamps often are made to follow the profile of which an exemption, or its the building / room structure and this imply that lamps will revocation, is requested and its have specific (and not standard) rounded curves (also with particular characteristics; small radius) on every geometrical axe.
    [Show full text]
  • Light-Emitting Diode - Wikipedia, the Free Encyclopedia
    Light-emitting diode - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Light-emitting_diode From Wikipedia, the free encyclopedia A light-emitting diode (LED) (pronounced /ˌɛl iː ˈdiː/[1]) is a semiconductor Light-emitting diode light source. LEDs are used as indicator lamps in many devices, and are increasingly used for lighting. Introduced as a practical electronic component in 1962,[2] early LEDs emitted low-intensity red light, but modern versions are available across the visible, ultraviolet and infrared wavelengths, with very high brightness. When a light-emitting diode is forward biased (switched on), electrons are able to recombine with holes within the device, releasing energy in the form of photons. This effect is called electroluminescence and the color of the light (corresponding to the energy of the photon) is determined by the energy gap of Red, green and blue LEDs of the 5mm type 2 the semiconductor. An LED is usually small in area (less than 1 mm ), and Type Passive, optoelectronic integrated optical components are used to shape its radiation pattern and assist in reflection.[3] LEDs present many advantages over incandescent light sources Working principle Electroluminescence including lower energy consumption, longer lifetime, improved robustness, Invented Nick Holonyak Jr. (1962) smaller size, faster switching, and greater durability and reliability. LEDs powerful enough for room lighting are relatively expensive and require more Electronic symbol precise current and heat management than compact fluorescent lamp sources of comparable output. Pin configuration Anode and Cathode Light-emitting diodes are used in applications as diverse as replacements for aviation lighting, automotive lighting (particularly indicators) and in traffic signals.
    [Show full text]
  • Appendix I Klhctrohics for Magihg Atom Probe 1.1
    APPENDIX I KLHCTROHICS FOR MAGIHG ATOM PROBE 1.1 ZHTRODDCTIOH The major limitation of PIM lies in its inability to chemically identify the imaging species. The atom probe PIM^ can give us the information about the chemical nature of a single atom (or a group of atoms) on the specimen tip surface. Panitz '-^ introduced a new technique known as Imaging Atom Probe (lAP), which gives the spatial distribution of the surface species. It mass analyzes the field evaporated species from the specimen surface on the basis of time of flight mass spectroscopy. The lAP, which is essentially a field desorption microscope with time gated microchannel plate (MCP) detector, is a powerful tool for studying a number of metallurgical problems. The electronic circuitry built in this laboratory for the lAP (figure 1.1) consisted of (i) two high voltage nanosecond pulsers, one for field evaporation from the tip and another for MCP activation, (ii) a variable delay network, and (iii) a master pulser to synchronize the whole operation. The two high voltage pulsers were identical, except the output pulse amplitude. Each of them comprised of the Krytron pulser and the avalanche transistor pulser used for grid triggering the Krytron. The combination of the master pulser and the variable delay network was used to get the two pulses having an adjustable time interval between them. These pulses were used to tri^er the avalanche transistor pulsers. Thus, the high voltage pulse for field evaporation and the MCP activation pulse after a presettable time delay "t" were obtained. The time gated images of the desired species are obtainable by deciding the delay time from following equation 73 CRYOSTAT ChteVRON MICROCHANNEL ^ PLATE - SCREEAi '4 ;5 ^ lOM —WWW -• +5 kV ^Vdc -vv5/J^ -• + 1-3kV 50M -VWWw -• + 0-3 kV 500 pP 5wi i:_--500p F X KRYTRON KRYTRON PULSER PULSER AVALANCHE VARIABLE AVAL/INCHE TR-ANSISTOR TRANSfS TOR PELAY PULSER PULSER NETWORK M/^STER PULSER.
    [Show full text]
  • Pseudospark Switches
    CERN 87-13 Proton Synchrotron Machine Division 14 December 1987 ORGANISATION EUROPÉENNE POUR LA RECHERCHE NUCLÉAIRE CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH PSEUDOSPARK SWITCHES P. Billault, H. Riege and M. van Gulik CERN, Geneva, Switzerland E. Boggasch and K. Frank Phys. Inst., University of Erlangen-Nùrnberg, Erlangen, Fed. Rep. Germany R. Seebôck Siemens AG, Erlangen, Fed. Rep. Germany GENEVA 1987 © Copyright CERN, Genève, 1987 Propriété littéraire et scientifique réservée pour Literary and scientific copyrights reserved in all tous les pays du monde. Ce document ne peut countries of the world. This report, or any part être reproduit ou traduit en tout ou en partie of it, may not be reprinted or translated without sans l'autorisation écrite du Directeur général du written permission of the copyright holder, the CERN, titulaire du droit d'auteur. Dans les cas Director-General of CERN. However, permis-' appropriés, et s'il s'agit d'utiliser le document à sion will be freely granted for appropriate des fins non commerciales, cette autorisation non-commercial use. sera volontiers accordée. If any patentable invention or registrable design Le CERN ne revendique pas la propriété des is described in the report, CERN makes no claim inventions brevetables et dessins ou modèles to property rights in it but offers it for the free susceptibles de dépôt qui pourraient être décrits use of research institutions, manufacturers and dans le présent document; ceux-ci peuvent être others. CERN, however, may oppose any librement utilisés par les instituts de recherche, attempt by a user to claim any proprietary or les industriels et autres intéressés.
    [Show full text]