Uranium: Its Uses and Hazards
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FACT SHEET Office of Public Affairs
FACT SHEET Office of Public Affairs Phone: 301-415-8200 Email: [email protected] Uranium Recovery Background The production of fuel for nuclear power plants starts with taking uranium ore from the ground and then purifying and processing it through a series of steps. Uranium recovery focuses on extracting natural uranium ore from the earth and concentrating (or milling) that ore. These recovery operations produce a product, called "yellowcake," which is then transported to a succession of fuel cycle facilities where the yellowcake is transformed into fuel for nuclear power reactors. In addition to yellowcake, uranium recovery operations generate waste products, called byproduct materials, that contain low levels of radioactivity. The NRC does not regulate uranium mining or mining exploration, but does have authority over milling of mined materials and in situ processes used to recover uranium, as well as mill tailings. Today’s conventional uranium mills and in situ recovery (ISR) facilities are operating safely and in a manner that is protective of the environment. The NRC regulates these facilities in close coordination with other Federal agencies and State and Tribal governments and provides technical support and guidance to those Agreement States that have authority over uranium recovery activities. Discussion The NRC becomes involved in uranium recovery operations when the ore is processed and physically or chemically altered. This happens either in a conventional, heap leach uranium mill, or ISR. For that reason, the NRC regulates ISR facilities as well as uranium mills and the disposal of liquid and solid wastes from uranium recovery operations (including mill tailings). -
Implementing Safeguards-By-Design at Natural Uranium Conversion Plants
NIS Office of Nuclear Safeguards and Security Safeguards-By-Design Facility Guidance Series (NGSI-SBD-002) August 2012 Implementing Safeguards-by-design at Natural Uranium Conversion Plants U.S. DEPARTMENT OF ENERG National Nuclear Security AdministrationY IMPLEMENTING SAFEGUARDS-BY-DESIGN AT NATURAL URANIUM CONVERSION PLANTS Lisa Loden John Begovich Date Published: July 2012 iii CONTENTS Page CONTENTS ......................................................................................................................................... IV 1. INTRODUCTION AND PURPOSE ................................................................................................. 1 2. KEY DEFINITIONS ......................................................................................................................... 2 3. SAFEGUARDS AT NUCPS ............................................................................................................. 7 3.1 SAFEGUARDS OBJECTIVES ................................................................................................. 7 3.2 TRADITIONAL AND INTEGRATED SAFEGUARDS ......................................................... 7 3.3 SAFEGUARDS RESPONSIBILITIES ..................................................................................... 8 3.3.1 STATE REGULATORY AUTHORITY RESPONSIBILITIES ..................................... 8 3.3.2 IAEA RESPONSIBILITIES ............................................................................................ 9 4. ELEMENTS OF FACILITY DESIGN THAT ARE RELEVANT -
A Measurement of the 2 Neutrino Double Beta Decay Rate of 130Te in the CUORICINO Experiment by Laura Katherine Kogler
A measurement of the 2 neutrino double beta decay rate of 130Te in the CUORICINO experiment by Laura Katherine Kogler A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Physics in the Graduate Division of the University of California, Berkeley Committee in charge: Professor Stuart J. Freedman, Chair Professor Yury G. Kolomensky Professor Eric B. Norman Fall 2011 A measurement of the 2 neutrino double beta decay rate of 130Te in the CUORICINO experiment Copyright 2011 by Laura Katherine Kogler 1 Abstract A measurement of the 2 neutrino double beta decay rate of 130Te in the CUORICINO experiment by Laura Katherine Kogler Doctor of Philosophy in Physics University of California, Berkeley Professor Stuart J. Freedman, Chair CUORICINO was a cryogenic bolometer experiment designed to search for neutrinoless double beta decay and other rare processes, including double beta decay with two neutrinos (2νββ). The experiment was located at Laboratori Nazionali del Gran Sasso and ran for a period of about 5 years, from 2003 to 2008. The detector consisted of an array of 62 TeO2 crystals arranged in a tower and operated at a temperature of ∼10 mK. Events depositing energy in the detectors, such as radioactive decays or impinging particles, produced thermal pulses in the crystals which were read out using sensitive thermistors. The experiment included 4 enriched crystals, 2 enriched with 130Te and 2 with 128Te, in order to aid in the measurement of the 2νββ rate. The enriched crystals contained a total of ∼350 g 130Te. The 128-enriched (130-depleted) crystals were used as background monitors, so that the shared backgrounds could be subtracted from the energy spectrum of the 130- enriched crystals. -
Compilation and Evaluation of Fission Yield Nuclear Data Iaea, Vienna, 2000 Iaea-Tecdoc-1168 Issn 1011–4289
IAEA-TECDOC-1168 Compilation and evaluation of fission yield nuclear data Final report of a co-ordinated research project 1991–1996 December 2000 The originating Section of this publication in the IAEA was: Nuclear Data Section International Atomic Energy Agency Wagramer Strasse 5 P.O. Box 100 A-1400 Vienna, Austria COMPILATION AND EVALUATION OF FISSION YIELD NUCLEAR DATA IAEA, VIENNA, 2000 IAEA-TECDOC-1168 ISSN 1011–4289 © IAEA, 2000 Printed by the IAEA in Austria December 2000 FOREWORD Fission product yields are required at several stages of the nuclear fuel cycle and are therefore included in all large international data files for reactor calculations and related applications. Such files are maintained and disseminated by the Nuclear Data Section of the IAEA as a member of an international data centres network. Users of these data are from the fields of reactor design and operation, waste management and nuclear materials safeguards, all of which are essential parts of the IAEA programme. In the 1980s, the number of measured fission yields increased so drastically that the manpower available for evaluating them to meet specific user needs was insufficient. To cope with this task, it was concluded in several meetings on fission product nuclear data, some of them convened by the IAEA, that international co-operation was required, and an IAEA co-ordinated research project (CRP) was recommended. This recommendation was endorsed by the International Nuclear Data Committee, an advisory body for the nuclear data programme of the IAEA. As a consequence, the CRP on the Compilation and Evaluation of Fission Yield Nuclear Data was initiated in 1991, after its scope, objectives and tasks had been defined by a preparatory meeting. -
Two Paths to a Nuclear Bomb Iran Has Historically Pursued Work on Both Uranium- and Plutonium-Weapons Programs, Western O Cials Say
Two Paths to a Nuclear Bomb Iran has historically pursued work on both uranium- and plutonium-weapons programs, Western ocials say. The 2015 nuclear deal set temporary limits on a wide range of Iran's nuclear work and committed Tehran to never work on nuclear weapons. Here's how far down those paths Iran is. Creating weapons-grade nuclear fuel Uranium 1 Low-grade uranium ore is 2 Centrifuges are set up in 3 Enriching uranium to 5% is the 4 It takes roughly 200 kg to 250 kg of 20% mined and chemically treated cascades to enrich the uranium. most time-consuming part of enriched uranium to produce the 25 kg of to produce a concentrated The sophisticated process can producing weapons-grade material. 90% enriched uranium, the amount needed yellowcake. After a conversion take years to establish. Iran Iran on Monday exceeded its for a bomb. Iran has reached 20% purity in process, it is fed into produced around 20,000 basic permitted 300-kg stockpile of the past but has never enriched above that centrifuges. centrifuges but is doing research uranium enriched to 3.67%. level. The enriched uranium is converted to Weaponizing nuclear fuel on more advanced machines. uranium metal for weapon use. Deploying the nuclear fuel in a Centrifuges weapon presents technical challenges, many of which Iran isn’t believed to have mastered. Detonating the 5% enriched Uranium Yellowcake Uranium 20% weapon requires a fission ore hexaflouride uranium 90% reaction. The nuclear payload 25kg must be attached to a missile, and the payload must be able 200-250 kg to withstand reentry through through earth's atmosphere as Plutonium it descends to its target. -
Lecture 22 Alpha Decay 1 Introduction 2 Fission and Fusion
Nuclear and Particle Physics - Lecture 22 Alpha decay 1 Introduction We have looked at gamma decays (due to the EM force) and beta decays (due to the weak force) and now will look at alpha decays, which are due to the strong/nuclear force. In contrast to the previous decays which do not change A, alpha decays happen by emission of some of the 4 nucleons from the nucleus. Specifically, for alpha decay, an alpha particle, 2He, is ejected so generically A A−4 4 X − Y + He Z !Z 2 2 for some X and Y . Y clearly has a different number of nucleons to X. Compare how alpha and beta decays move the nuclei around in Z,N plane N β+ β- α Z Note that gamma decays cannot change Z, N or A. 2 Fission and fusion Alpha decay is in fact only one specific case of a whole range of processes which involve emission of nucleons. These range from single proton or neutron emission up to splitting the nucleus into two roughly equal parts. Particularly in the latter case, these are called fission decays. Which nuclei would we expect to fission? The binding energy per nucleon curve shows that 56 the maximum occurs around 26Fe and drops off to either side. Hence, both small A and large A nuclei are less strongly bound per nucleon than medium A. This means there will be some energy release if two small nuclei are combined into a larger one, a process called fusion which will be discussed later in the course. -
Radioactive Decay
North Berwick High School Department of Physics Higher Physics Unit 2 Particles and Waves Section 3 Fission and Fusion Section 3 Fission and Fusion Note Making Make a dictionary with the meanings of any new words. Einstein and nuclear energy 1. Write down Einstein’s famous equation along with units. 2. Explain the importance of this equation and its relevance to nuclear power. A basic model of the atom 1. Copy the components of the atom diagram and state the meanings of A and Z. 2. Copy the table on page 5 and state the difference between elements and isotopes. Radioactive decay 1. Explain what is meant by radioactive decay and copy the summary table for the three types of nuclear radiation. 2. Describe an alpha particle, including the reason for its short range and copy the panel showing Plutonium decay. 3. Describe a beta particle, including its range and copy the panel showing Tritium decay. 4. Describe a gamma ray, including its range. Fission: spontaneous decay and nuclear bombardment 1. Describe the differences between the two methods of decay and copy the equation on page 10. Nuclear fission and E = mc2 1. Explain what is meant by the terms ‘mass difference’ and ‘chain reaction’. 2. Copy the example showing the energy released during a fission reaction. 3. Briefly describe controlled fission in a nuclear reactor. Nuclear fusion: energy of the future? 1. Explain why nuclear fusion might be a preferred source of energy in the future. 2. Describe some of the difficulties associated with maintaining a controlled fusion reaction. -
Arxiv:1901.01410V3 [Astro-Ph.HE] 1 Feb 2021 Mental Information Is Available, and One Has to Rely Strongly on Theoretical Predictions for Nuclear Properties
Origin of the heaviest elements: The rapid neutron-capture process John J. Cowan∗ HLD Department of Physics and Astronomy, University of Oklahoma, 440 W. Brooks St., Norman, OK 73019, USA Christopher Snedeny Department of Astronomy, University of Texas, 2515 Speedway, Austin, TX 78712-1205, USA James E. Lawlerz Physics Department, University of Wisconsin-Madison, 1150 University Avenue, Madison, WI 53706-1390, USA Ani Aprahamianx and Michael Wiescher{ Department of Physics and Joint Institute for Nuclear Astrophysics, University of Notre Dame, 225 Nieuwland Science Hall, Notre Dame, IN 46556, USA Karlheinz Langanke∗∗ GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany and Institut f¨urKernphysik (Theoriezentrum), Fachbereich Physik, Technische Universit¨atDarmstadt, Schlossgartenstraße 2, 64298 Darmstadt, Germany Gabriel Mart´ınez-Pinedoyy GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany; Institut f¨urKernphysik (Theoriezentrum), Fachbereich Physik, Technische Universit¨atDarmstadt, Schlossgartenstraße 2, 64298 Darmstadt, Germany; and Helmholtz Forschungsakademie Hessen f¨urFAIR, GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany Friedrich-Karl Thielemannzz Department of Physics, University of Basel, Klingelbergstrasse 82, 4056 Basel, Switzerland and GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany (Dated: February 2, 2021) The production of about half of the heavy elements found in nature is assigned to a spe- cific astrophysical nucleosynthesis process: the rapid neutron capture process (r-process). Although this idea has been postulated more than six decades ago, the full understand- ing faces two types of uncertainties/open questions: (a) The nucleosynthesis path in the nuclear chart runs close to the neutron-drip line, where presently only limited experi- arXiv:1901.01410v3 [astro-ph.HE] 1 Feb 2021 mental information is available, and one has to rely strongly on theoretical predictions for nuclear properties. -
Alpha-Decay Chains of Z=122 Superheavy Nuclei Using Cubic Plus Proximity Potential with Improved Transfer Matrix Method
Indian Journal of Pure & Applied Physics Vol. 58, May 2020, pp. 397-403 Alpha-decay chains of Z=122 superheavy nuclei using cubic plus proximity potential with improved transfer matrix method G Naveyaa, S Santhosh Kumarb, S I A Philominrajc & A Stephena* aDepartment of Nuclear Physics, University of Madras, Guindy Campus, Chennai 600 025, India bDepartment of Physics, Kanchi Mamunivar Centre for Post Graduate Studies, Lawspet, Puducherry 605 008, India cDepartment of Physics, Madras Christian College, Chennai 600 059, India Received 4 May 2020 The alpha decay chain properties of Z = 122 isotope in the mass range 298 A 350, even-even nuclei, are studied using a fission-like model with an effective combination of the cubic plus proximity potential in the pre and post-scission regions, wherein the decay rates are calculated using improved transfer matrix method, and the results are in good agreement with other phenomenological formulae such as Universal decay law, Viola-Seaborg, Royer, etc. The nuclear ground-state masses are taken from WS4 mass model. The next minimum in the half-life curves of the decay chain obtained at N=186,178 & 164 suggest the shell closure at N=184, 176 & 162 which coincides well with the predictions of two-centre shell model approach. This study also unveils that the isotopes 298-300, 302, 304-306, 308-310, 312,314122 show 7, 5, 4, 3, 2 and 1 decay chain, respectively. All the other isotopes from A = 316 to 350 may undergo spontaneous fission since the obtained SF half -lives are comparatively less. The predictions in the present study may have an impact in the experimental synthesis and detection of the new isotopes in near future. -
Isotopic Composition of Fission Gases in Lwr Fuel
XA0056233 ISOTOPIC COMPOSITION OF FISSION GASES IN LWR FUEL T. JONSSON Studsvik Nuclear AB, Hot Cell Laboratory, Nykoping, Sweden Abstract Many fuel rods from power reactors and test reactors have been punctured during past years for determination of fission gas release. In many cases the released gas was also analysed by mass spectrometry. The isotopic composition shows systematic variations between different rods, which are much larger than the uncertainties in the analysis. This paper discusses some possibilities and problems with use of the isotopic composition to decide from which part of the fuel the gas was released. In high burnup fuel from thermal reactors loaded with uranium fuel a significant part of the fissions occur in plutonium isotopes. The ratio Xe/Kr generated in the fuel is strongly dependent on the fissioning species. In addition, the isotopic composition of Kr and Xe shows a well detectable difference between fissions in different fissile nuclides. 1. INTRODUCTION Most LWRs use low enriched uranium oxide as fuel. Thermal fissions in U-235 dominate during the earlier part of the irradiation. Due to the build-up of heavier actinides during the irradiation fissions in Pu-239 and Pu-241 increase in importance as the burnup of the fuel increases. The composition of the fission products varies with the composition of the fuel and the irradiation conditions. The isotopic composition of fission gases is often determined in connection with measurement of gases in the plenum of punctured fuel rods. It can be of interest to discuss how more information on the fuel behaviour can be obtained by use of information available from already performed determinations of gas compositions. -
Global Fissile Material Report 2006 a Table of Contents
IPF M Global Fis sile Material Report Developing the technical basis for policy initiatives to secure and irreversibly reduce stocks of nuclear weapons and fissile materials 2006 Over the past six decades, our understanding of the nuclear danger has expanded from the threat posed by the vast nuclear arsenals created by the super- powers in the Cold War to encompass the prolifera- tion of nuclear weapons to additional states and now also to terrorist groups. To reduce this danger, it is essential to secure and to sharply reduce all stocks of highly enriched uranium and separated plutonium, the key materials in nuclear weapons, and to limit any further production. The mission of the IPFM is to advance the technical basis for cooperative international policy initiatives to achieve these goals. A report published by Global Fissile The International Panel on Fissile Materials (IPFM) www.fissilematerials.org Program on Science and Global Security Princeton University Material Report 2006 221 Nassau Street, 2nd Floor Princeton, NJ 08542, USA First report of the International Panel on Fissile Materials First report of the International Panel on Fissile Materials Developing the Technical Basis for Policy Initiatives to Secure and Irreversibly Reduce Stocks of Nuclear Weapons and Fissile Materials www.fissilematerials.org Global Fissile Material Report 2006 a Table of Contents About the IPFM 1 Summary 2 I. Background 5 1 Fissile Materials and Nuclear Weapons 6 2 Nuclear-Weapon and Fissile-Material Stocks 12 3 Production and Disposition of Fissile -
Recent Developments in Radioactive Charged-Particle Emissions
Recent developments in radioactive charged-particle emissions and related phenomena Chong Qi, Roberto Liotta, Ramon Wyss Department of Physics, Royal Institute of Technology (KTH), SE-10691 Stockholm, Sweden October 19, 2018 Abstract The advent and intensive use of new detector technologies as well as radioactive ion beam facilities have opened up possibilities to investigate alpha, proton and cluster decays of highly unstable nuclei. This article provides a review of the current status of our understanding of clustering and the corresponding radioactive particle decay process in atomic nuclei. We put alpha decay in the context of charged-particle emissions which also include one- and two-proton emissions as well as heavy cluster decay. The experimental as well as the theoretical advances achieved recently in these fields are presented. Emphasis is given to the recent discoveries of charged-particle decays from proton-rich nuclei around the proton drip line. Those decay measurements have shown to provide an important probe for studying the structure of the nuclei involved. Developments on the theoretical side in nuclear many-body theories and supercomputing facilities have also made substantial progress, enabling one to study the nuclear clusterization and decays within a microscopic and consistent framework. We report on properties induced by the nuclear interaction acting in the nuclear medium, like the pairing interaction, which have been uncovered by studying the microscopic structure of clusters. The competition between cluster formations as compared to the corresponding alpha-particle formation are included. In the review we also describe the search for super-heavy nuclei connected by chains of alpha and other radioactive particle decays.