Curium in Space
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Spent Nuclear Fuel Pools in the US
Spent Nuclear Fuel Pools in the U.S.: Reducing the Deadly Risks of Storage front cover WITH SUPPORT FROM: WITH SUPPORT FROM: By Robert Alvarez 1112 16th St. NW, Suite 600, Washington DC 20036 - www.ips-dc.org May 2011 About the Author Robert Alvarez, an Institute for Policy Studies senior scholar, served as a Senior Policy Advisor to the Secre- tary of Energy during the Clinton administration. Institute for Policy Studies (IPS-DC.org) is a community of public scholars and organizers linking peace, justice, and the environment in the U.S. and globally. We work with social movements to promote true democracy and challenge concentrated wealth, corporate influence, and military power. Project On Government Oversight (POGO.org) was founded in 1981 as an independent nonprofit that investigates and exposes corruption and other misconduct in order to achieve a more effective, accountable, open, and ethical federal government. Institute for Policy Studies 1112 16th St. NW, Suite 600 Washington, DC 20036 http://www.ips-dc.org © 2011 Institute for Policy Studies [email protected] For additional copies of this report, see www.ips-dc.org Table of Contents Summary ...............................................................................................................................1 Introduction ..........................................................................................................................4 Figure 1: Explosion Sequence at Reactor No. 3 ........................................................4 Figure 2: Reactor No. 3 -
Table 2.Iii.1. Fissionable Isotopes1
FISSIONABLE ISOTOPES Charles P. Blair Last revised: 2012 “While several isotopes are theoretically fissionable, RANNSAD defines fissionable isotopes as either uranium-233 or 235; plutonium 238, 239, 240, 241, or 242, or Americium-241. See, Ackerman, Asal, Bale, Blair and Rethemeyer, Anatomizing Radiological and Nuclear Non-State Adversaries: Identifying the Adversary, p. 99-101, footnote #10, TABLE 2.III.1. FISSIONABLE ISOTOPES1 Isotope Availability Possible Fission Bare Critical Weapon-types mass2 Uranium-233 MEDIUM: DOE reportedly stores Gun-type or implosion-type 15 kg more than one metric ton of U- 233.3 Uranium-235 HIGH: As of 2007, 1700 metric Gun-type or implosion-type 50 kg tons of HEU existed globally, in both civilian and military stocks.4 Plutonium- HIGH: A separated global stock of Implosion 10 kg 238 plutonium, both civilian and military, of over 500 tons.5 Implosion 10 kg Plutonium- Produced in military and civilian 239 reactor fuels. Typically, reactor Plutonium- grade plutonium (RGP) consists Implosion 40 kg 240 of roughly 60 percent plutonium- Plutonium- 239, 25 percent plutonium-240, Implosion 10-13 kg nine percent plutonium-241, five 241 percent plutonium-242 and one Plutonium- percent plutonium-2386 (these Implosion 89 -100 kg 242 percentages are influenced by how long the fuel is irradiated in the reactor).7 1 This table is drawn, in part, from Charles P. Blair, “Jihadists and Nuclear Weapons,” in Gary A. Ackerman and Jeremy Tamsett, ed., Jihadists and Weapons of Mass Destruction: A Growing Threat (New York: Taylor and Francis, 2009), pp. 196-197. See also, David Albright N 2 “Bare critical mass” refers to the absence of an initiator or a reflector. -
The Nuclear Waste Primer September 2016 What Is Nuclear Waste?
The Nuclear Waste Primer September 2016 What is Nuclear Waste? Nuclear waste is the catch-all term for anything contaminated with radioactive material. Nuclear waste can be broadly divided into three categories: • Low-level waste (LLW), comprised of protective clothing, medical waste, and other lightly-contaminated items • Transuranic waste (TRU), comprised of long-lived isotopes heavier than uranium • High-level waste (HLW), comprised of spent nuclear fuel and other highly-radioactive materials Low-level waste is relatively short-lived and easy to handle. Currently, four locations for LLW disposal exist in the United States. Two of them, Energy Solutions in Clive, Utah and Waste Control Specialists in Andrews, Texas, accept waste from any U.S. state. Transuranic waste is often a byproduct of nuclear weapons production and contains long-lived radioactive elements heavier than uranium, like plutonium and americium. Currently, the U.S. stores TRU waste at the Waste Isolation Pilot Plant (WIPP) near Carlsbad, New Mexico. High-level waste includes spent nuclear fuel and the most radioactive materials produced by nuclear weapons production. Yucca Mountain is the currently designated high-level waste repository for the United States. 1 | What is Spent Nuclear Fuel? Spent nuclear fuel (SNF), alternatively referred to as used nuclear fuel, is the primary byproduct of nuclear reactors. In commercial power reactors in the U.S., fuel begins as uranium oxide clad in a thin layer of zirconium-aluminum cladding. After several years inside of the reactor, around fi ve percent of the uranium has been converted in some way, ranging from short-lived and highly radioactive fi ssion products to long-lived actinides like plutonium, americium, and neptunium. -
NOBELIUM Element Symbol: No Atomic Number: 102
NOBELIUM Element Symbol: No Atomic Number: 102 An initiative of IYC 2011 brought to you by the RACI KERRY LAMB www.raci.org.au NOBELIUM Element symbol: No Atomic number: 102 The credit for discovering Nobelium was disputed with 3 different research teams claiming the discovery. While the first claim dates back to 1957, it was not until 1992 that the International Union of Pure and Applied Chemistry credited the discovery to a research team from Dubna in Russia for work they did in 1966. The element was named Nobelium in 1957 by the first of its claimed discoverers (the Nobel Institute in Sweden). It was named after Alfred Nobel, a Swedish chemist who invented dynamite, held more than 350 patents and bequeathed his fortune to the establishment of the Nobel Prizes. Nobelium is a synthetic element and does not occur in nature and has no known uses other than in scientific research as only tiny amounts of the element have ever been produced. Nobelium is radioactive and most likely metallic. The appearance and properties of Nobelium are unknown as insufficient amounts of the element have been produced. Nobelium is made by the bombardment of curium (Cm) with carbon nuclei. Its most stable isotope, 259No, has a half-life of 58 minutes and decays to Fermium (255Fm) through alpha decay or to Mendelevium (259Md) through electron capture. Provided by the element sponsor Freehills Patent and Trade Mark Attorneys ARTISTS DESCRIPTION I wanted to depict Alfred Nobel, the namesake of Nobelium, as a resolute young man, wearing the Laurel wreath which is the symbol of victory. -
Nuclear Transmutation Strategies for Management of Long-Lived Fission
PRAMANA c Indian Academy of Sciences Vol. 85, No. 3 — journal of September 2015 physics pp. 517–523 Nuclear transmutation strategies for management of long-lived fission products S KAILAS1,2,∗, M HEMALATHA2 and A SAXENA1 1Nuclear Physics Division, Bhabha Atomic Research Centre, Mumbai 400 085, India 2UM–DAE Centre for Excellence in Basic Sciences, Mumbai 400 098, India ∗Corresponding author. E-mail: [email protected] DOI: 10.1007/s12043-015-1063-z; ePublication: 27 August 2015 Abstract. Management of long-lived nuclear waste produced in a reactor is essential for long- term sustenance of nuclear energy programme. A number of strategies are being explored for the effective transmutation of long-lived nuclear waste in general, and long-lived fission products (LLFP), in particular. Some of the options available for the transmutation of LLFP are discussed. Keywords. Nuclear transmutation; long-lived fission products; (n, γ ) cross-section; EMPIRE. PACS Nos 28.41.Kw; 25.40.Fq; 24.60.Dr 1. Introduction It is recognized that for long-term energy security, nuclear energy is an inevitable option [1]. For a sustainable nuclear energy programme, the management of long-lived nuclear waste is very critical. Radioactive nuclei like Pu, minor actinides like Np, Am and Cm and long-lived fission products like 79Se, 93Zr, 99Tc, 107Pd, 126Sn, 129I and 135Cs constitute the main waste burden from a power reactor. In this paper, we shall discuss the management strategies for nuclear waste in general, and long-lived fission products, in particular. 2. Management of nuclear waste The radioactive nuclei which are produced in a power reactor and which remain in the spent fuel of the reactor form a major portion of nuclear waste. -
Royal Society of Chemistry Input to the Ad Hoc Nuclear
ROYAL SOCIETY OF CHEMISTRY INPUT TO THE AD HOC NUCLEAR RESEARCH AND DEVELOPMENT ADVISORY BOARD The Royal Society of Chemistry (RSC) was pleased to hear of the instigation of the Ad Hoc Nuclear Research and Development Advisory Board (the Board) following the findings of the House of Lords Science and Technology Committee Inquiry ‘Nuclear Research and Development Capabilities’.1,2 The RSC is the largest organisation in Europe for advancing the chemical sciences. Supported by a network of 47,000 members worldwide and an internationally acclaimed publishing business, its activities span education and training, conferences and science policy, and the promotion of the chemical sciences to the public. This document represents the views of the RSC. The RSC has a duty under its Royal Charter "to serve the public interest" by acting in an independent advisory capacity, and it is in this spirit that this submission is made. To provide input to the Board the RSC has performed a wide consultation with the chemical science community, including members of both our Radiochemistry and Energy Sector Interest Groups and also our Environment Sustainability and Energy Division. September 2012 The Role of Chemistry in a Civil Nuclear Strategy 1 Introduction Chemistry and chemical knowledge is essential in nuclear power generation and nuclear waste management. It is essential that a UK civil nuclear strategy recognises the crucial role that chemistry plays, both in research and innovation and in the development of a strong skills pipeline. As the RSC previously articulated in our response to the House of Lords Inquiry, 3 nuclear power is an important component of our current energy mix. -
Security of Supply of Medical Radioisotopes - a Clinical View Dr Beverley Ellis Consultant Radiopharmacist
Security of Supply of Medical Radioisotopes - a clinical view Dr Beverley Ellis Consultant Radiopharmacist Nuclear Medicine Centre Manchester University NHS Foundation Trust Nuclear Medicine § Approx 35 million clinical radionuclide imaging procedures worldwide § Globally 2nd most common imaging technique after CT (higher than MR) 20 million in USA 9 million in Europe 3 million in Japan 3 million in rest of the world Approx 700, 000 nuclear medicine procedures per year in UK Myocardial Perfusion - Ischaemia Stress Stress SA Rest Stress VLA Rest Stress HLA Rest Rest Tc-99m Bone Scans Normal Metastases Mo-99/Tc-99m Generator Supply Tc-99m Radiopharmaceutical Production Mo-99 Shortages Design of Clinical Services to Reduce Tc-99m Use § Optimisation of generator management – Efficiency savings – Delivery and extraction schedules – Patient scheduling § Improved communication – Customers – Suppliers § Improved software – gamma cameras – Produce comparable quality images using less radioactivity Global Situation § OECD/Nuclear Energy Agency (NEA) – Set up High Level Group (HLG-MR) in 2009 – Security of supply of Mo-99 and Tc-99m – Established 6 principles e.g. full cost recovery and outage reserve capacity – Issued a series of publications Global Situation § AIPES (Association of Imaging Producers & Equipment supplies) (Now called Nuclear Medicine Europe) – Support coordination of research reactor schedules Global Situation § Increased Mo-99 Production Capacity – Mo-99 suppliers – acquire additional capacity to cover shortfalls (Outage -
4. Particle Generators/Accelerators
Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing 4. Particle Generators/Accelerators Diana Adlienė Department of Physics Kaunas University of Technolog y Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing This project has been funded with support from the European Commission. This publication reflects the views only of the author. Polish National Agency and the Commission cannot be held responsible for any use which may be made of the information contained therein. Date: Oct. 2017 DISCLAIMER This presentation contains some information addapted from open access education and training materials provided by IAEA TABLE OF CONTENTS 1. Introduction 2. X-ray machines 3. Particle generators/accelerators 4. Types of industrial irradiators The best accelerator in the universe… INTRODUCTION • Naturally occurring radioactive sources: – Up to 5 MeV Alpha’s (helium nuclei) – Up to 3 MeV Beta particles (electrons) • Natural sources are difficult to maintain, their applications are limited: – Chemical processing: purity, messy, and expensive; – Low intensity; – Poor geometry; – Uncontrolled energies, usually very broad Artificial sources (beams) are requested! INTRODUCTION • Beams of accelerated particles can be used to produce beams of secondary particles: Photons (x-rays, gamma-rays, visible light) are generated from beams -
Installation of the Cyclotron Based Clinical Neutron Therapy System in Seattle
Proceedings of the Tenth International Conference on Cyclotrons and their Applications, East Lansing, Michigan, USA INSTALLATION OF THE CYCLOTRON BASED CLINICAL NEUTRON THERAPY SYSTEM IN SEATTLE R. Risler, J. Eenmaa, J. Jacky, I. Kalet, and P. Wootton Medical Radiation Physics RC-08, University of Washington, Seattle ~ 98195, USA S. Lindbaeck Instrument AB Scanditronix, Uppsala, Sweden Sumnary radiation areas is via sliding shielding doors rather than a maze, mai nl y to save space. For the same reason A cyclotron facility has been built for cancer a single door is used to alternately close one or the treatment with fast neutrons. 50.5 MeV protons from a other therapy room. All power supplies and the control conventional, positive ion cyclotron are used to b0m computer are located on the second floor, above the bard a semi-thick Beryllium target located 150 am from maintenance area. The cooler room contains a heat the treatment site. Two treatment rooms are available, exchanger and other refrigeration equipment. Not shown one with a fixed horizontal beam and one with an iso in the diagram is the cooling tower located in another centric gantry capable of 360 degree rotation. In part of the building. Also not shown is the hot lab addition 33 51 MeV protons and 16.5 - 25.5 MeV now under construction an an area adjacent to the deuterons are generated for isotope production inside cyclotron vault. It will be used to process radio the cyclotron vault. The control computer is also used isotopes produced at a target station in the vault. to record and verify treatment parameters for indi vidual patients and to set up and monitor the actual radiation treatment. -
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering at the Massachusetts Institute of Technology June 2007 © 2007 Leslie Dewan All rights reserved The author hereby grants to MIT permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part in any medium now known or hereafter created. Signature of Author: Leslie Dewan Department of Nuclear Science and Engineering May 16, 2007 Certified by: David G. Cory Professor of Nuclear Science and Engineering Thesis Supervisor Accepted by: David G. Cory Professor of Nuclear Science and Engineering Chairman, NSE Committee for Undergraduate Students Leslie Dewan 1 of 23 5/16/07 22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering on May 16, 2007 in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering ABSTRACT This thesis describes the design and construction of a cyclotron capable of accelerating protons to 2 MeV. A cyclotron is a charged particle accelerator that uses a magnetic field to confine particles to a spiral flight path in a vacuum chamber. An applied electrical field accelerates these particles to high energies, typically on the order of mega-electron volts. -
The Supply of Medical Isotopes
The Supply of Medical Isotopes AN ECONOMIC DIAGNOSIS AND POSSIBLE SOLUTIONS The Supply of Medical Isotopes AN ECONOMIC DIAGNOSIS AND POSSIBLE SOLUTIONS The Supply of Medical Isotopes AN ECONOMIC DIAGNOSIS AND POSSIBLE SOLUTIONS This work is published under the responsibility of the Secretary-General of the OECD. The opinions expressed and arguments employed herein do not necessarily reflect the official views of OECD member countries. This document, as well as any data and any map included herein, are without prejudice to the status of or sovereignty over any territory, to the delimitation of international frontiers and boundaries and to the name of any territory, city or area. Please cite this publication as: OECD/NEA (2019), The Supply of Medical Isotopes: An Economic Diagnosis and Possible Solutions, OECD Publishing, Paris, https://doi.org/10.1787/9b326195-en. ISBN 978-92-64-94550-0 (print) ISBN 978-92-64-62509-9 (pdf) The statistical data for Israel are supplied by and under the responsibility of the relevant Israeli authorities. The use of such data by the OECD is without prejudice to the status of the Golan Heights, East Jerusalem and Israeli settlements in the West Bank under the terms of international law. Photo credits: Cover © Yok_onepiece/Shutterstock.com. Corrigenda to OECD publications may be found on line at: www.oecd.org/about/publishing/corrigenda.htm. © OECD 2019 You can copy, download or print OECD content for your own use, and you can include excerpts from OECD publications, databases and multimedia products in your own documents, presentations, blogs, websites and teaching materials, provided that suitable acknowledgement of OECD as source and copyright owner is given. -
Cyclotrons: Old but Still New
Cyclotrons: Old but Still New The history of accelerators is a history of inventions William A. Barletta Director, US Particle Accelerator School Dept. of Physics, MIT Economics Faculty, University of Ljubljana US Particle Accelerator School ~ 650 cyclotrons operating round the world Radioisotope production >$600M annually Proton beam radiation therapy ~30 machines Nuclear physics research Nuclear structure, unstable isotopes,etc High-energy physics research? DAEδALUS Cyclotrons are big business US Particle Accelerator School Cyclotrons start with the ion linac (Wiederoe) Vrf Vrf Phase shift between tubes is 180o As the ions increase their velocity, drift tubes must get longer 1 v 1 "c 1 Ldrift = = = "# rf 2 f rf 2 f rf 2 Etot = Ngap•Vrf ==> High energy implies large size US Particle Accelerator School ! To make it smaller, Let’s curl up the Wiederoe linac… Bend the drift tubes Connect equipotentials Eliminate excess Cu Supply magnetic field to bend beam 1 2# mc $ 2# mc " rev = = % = const. frf eZion B eZion B Orbits are isochronous, independent of energy ! US Particle Accelerator School … and we have Lawrence’s* cyclotron The electrodes are excited at a fixed frequency (rf-voltage source) Particles remain in resonance throughout acceleration A new bunch can be accelerated on every rf-voltage peak: ===> “continuous-wave (cw) operation” Lawrence, E.O. and Sloan, D.: Proc. Nat. Ac. Sc., 17, 64 (1931) Lawrence, E.O. & Livingstone M.S.: Phys. Rev 37, 1707 (1931). * The first cyclotron patent (German) was filed in 1929 by Leó Szilard but never published in a journal US Particle Accelerator School Synchronism only requires that τrev = N/frf “Isochronous” particles take the same revolution time for each turn.