Radiological Characterization of Shut Down Nuclear Reactors
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Selection of Retrieval Techniques for Irradiated Graphite During Reactor Decommissioning - 11587
WM2011 Conference, February 27 - March 3, 2011, Phoenix, AZ Selection of Retrieval Techniques for Irradiated Graphite during Reactor Decommissioning - 11587 D.J. Potter*, R.B. Jarvis*, A.W. Banford*, L. Cordingley*, and M. Grave** * National Nuclear Laboratory, Chadwick House, Birchwood Park, Warrington, Cheshire, WA3 6AE, UK ** Doosan Babcock, Baltic Business Centre, Gateshead, NE8 3DA, UK ABSTRACT Globally, around 230,000 tonnes of irradiated graphite requires retrieval, treatment, management and/or disposal. This waste has arisen from a wide range of reactors, predominantly from the use of graphite moderated reactors for base-load generation, but also from experimental research facilities. Much of the graphite is presently still in the reactor core while other graphite is stored in a variety of forms in waste stores. The first step in the management of this significant waste stream is retrieval of the graphite from its present location. Doosan Babcock and the UK National Nuclear Laboratory are participants in the CARBOWASTE European research project which brings together organisations from a range of countries with an irradiated graphite legacy to address the graphite waste management challenge. This paper describes the issues associated with retrieval of graphite from reactors, potential approaches to graphite retrieval and the information needed to select a particular retrieval method for a specified application. Graphite retrieval is viewed within the context of the wider strategy for the management of irradiated graphite waste streams. The paper identifies the challenges of graphite retrieval and provides some examples where modelling can be used to provide information to support retrievals design and operations. INTRODUCTION A four year collaborative European Project ‘Treatment and Disposal of Irradiated Graphite and other Carbonaceous Waste (CARBOWASTE)’ was launched in April 2008 under the 7th EURATOM Framework Programme [1]. -
Solar Greenhouse Heating Final Report Mcgill University BREE 495 - Engineering Design 3 Group 2 Matthew Legrand, Abu Mahdi Mia, Nicole Peletz-Bohbot, Mitchell Steele
Solar Greenhouse Heating Final Report McGill University BREE 495 - Engineering Design 3 Group 2 Matthew LeGrand, Abu Mahdi Mia, Nicole Peletz-Bohbot, Mitchell Steele Supported by: 1 Executive Summary The Macdonald Campus Horticultural Centre begins seeding in late-February to provide fresh fruit and produce to students, staff, and community members, as well as to offer educational tours and sustained research opportunities throughout the summer and fall semester. An electrically-heated long tunnel greenhouse is currently used for seeding and germination prior to planting. However, as temperatures in February and March are quite variable, seeded trays are often transported to the indoor centre and back to the greenhouse when temperatures become more favourable. As the current system is both time and energy intensive, an alternative was needed to extend the greenhouse growing season by providing an effective, safe, sustainable, cost-efficient, and accessible solution; a solar thermal heating system was designed. The system consists of two automated fluid circuits. The first circuit operates throughout the day by absorbing heat from a liquid-finned solar thermal heat exchanger and transferring it to a water-glycol fluid, which is then pumped to a hot-water tank inside the greenhouse. The second circuit is initiated when soil temperatures reach below 10°C. An electric heating element is used in the hot water tank when the heat exchanger cannot provide enough heat. The heated water then circulates from the tank to tubing under the greenhouse tables, heating the seedbed soil through free convection. Through rigorous testing and simulations the system was optimized, it was determined to be economically advantageous compared to the current system, and risks as well as safety concerns were mitigated and addressed. -
Interior Heat and Temperature
1 Heat and temperature within the Earth Several scenarios are arguable for the original accretion of the Earth. It may have accreted rapidly and so retained much of the gravitational potential energy as internal heat. It may have accreted slowly enough to have radiated most of the heat of gravitational potential into space and so have been relatively cool in its interior. If so, its interior must have heated quite quickly as a result of radioactive decays. If Earth’s accretion arose shortly after supernoval explosions had formed the dust cloud from which the proto-solar nebula condensed, the cloud would have contained substantial quantities of short-lived radionuclei that would have quickly warmed the interior. In any event the heat flow through the surface of the Earth into space attests to a very warm interior at the present time. 1.1 Gravitational energy retained as heat in a condensing planet or the Sun Recall that von Helmholtz recognized that the gravitational energy contained within the Sun could account for its shining for between 20 and 40 × 106 years. How can we estimate this energy? Let’s do the physics and calculate the heat equiv- alence of the gravitational accretion energy for the Earth. • Starting from an extended and “absolutely” cold (i.e. 0K) cloud... • Somewhere a small mass Mc of radius r assembles, perhaps under electrostatic or magnetic forces. 3 • The volume of our centre, presume a sphere, is then, Vc = 4/3πr and its density, ρ is such that Mc = ρVc. • Now, suppose that at some great distance Rstart a small element of mass, dm, is waiting to fall in upon this gravitating centre. -
WASH-1097.Pdf
WASH 1097 UC-80 THE USE OF THORIUM IN NUCLEAR POWER REACTORS JUNE 1969 PREPARED BY Brookhaven National Laboratory AND THE Division of Reactor Development and Technology WITH THE ASSISTANCE OF ARGONNE NATIONAL LABORATORY BABCOCK & WILCOX GULF GENERAL ATOMIC OAK RIDGE NATIONAL LABORATORY PACIFIC NORTHWEST LABORATORY For sale by the Superintendent of Documents, U.S. Government Printing Office Washington, D.C. 20402 - Price $1.25 FOREWORD This report on "The Use of Thorium in Nuclear Power Reactors" was prepared under the direction of the Division of Reactor Development and Technology, U.S.A.E.C., as part of an overall assessment of the Civilian Nuclear Power Program initiated in response to a request in 1966 by the Joint Committee on Atomic Energy. It represents the results of the inquiry by the Thorium Systems Task Force whose membership included representatives of Babcock & Wilcox Company, Gulf General Atomic Company, the Argonne National Laboratory, the Brookhaven National Laboratory, the Oak Ridge National Laboratory, the Pacific Northwest Laboratory, and the U.S. Atomic Energy Commission. Publication of this report, which provides information basic to the AEC reactor development program, completes one phase of the evaluation effort outlined in the 1967 Supplement to the 1962 Report to the President on Civilian Nuclear Power, issued in February 1967. The 1967 Supplement outlined changes since 1962 in the technical, economic and resource picture and provided background for further study. Specifically, this report represents the consensus of the task force on the potential use of the thorium cycle and the specific thorium fueled reactor designs which have been proposed. -
Nuclear Power
No.59 z iii "Ill ~ 2 er0 Ill Ill 0 Nuclear Family Pia nning p3 Chernobyl Broadsheet ·, _ I. _ . ~~~~ George Pritchar d speaks CONTENTS COMMENT The important nuclear development since the Nuclear Family Planning 3 last SCRAM Journal was the Government's The CEGB's plans, and the growing opposition, after Sizewell B by go ahead for Sizewell B: the world's first HUGH RICHARDS. reactor order since Chernobyl, and Britain's News 4-6 first since the go ahead was given to Torness Accidents Will Happen 1 and Heysham 2 in 1978. Of great concern is Hinkley Seismic Shocker 8-9 the CEGB's announced intention to build "a A major article on seismic safety of nuclear plants in which JAMES small fanilty• of PWRs, starting with Hinkley GARRETT reveals that Hinkley Point C. At the time of the campaign In the Point sits on a geological fault. south west to close the Hinkley A Magnox Trouble at Trawsfynydd 10-11 station, and .a concerted push in Scotland to A summary of FoE's recent report on increasing radiation levels from prevent the opening of Torness, another Trawsfynydd's by PATRICK GREEN. nuclear announcement is designed to divide Pandora's POX 12 and demoralise the opposition. But, it should The debate over plutonium transport make us more determined. The article on the to and from Dounreay continues by facing page gives us hope: the local PETE MUTTON. authorities on Severnside are joining forces CHERNOBYL BROADSHEET to oppose Hinkley C, and hopefully they will Cock-ups and Cover-ups work closely with local authorities in other "Sacrificed to • • • Nuclear Power" threatened areas - Lothian Region, The Soviet Experience Northumberland, the County Council Coalition "An Agonising Decision• 13 against waste dumping and the Nuclear Free GEORGE PRITCHARD explains why Zones - to formulate a national anti-nuclear he left Greenpeoce and took a job strategy. -
Physics 160 Stellar Astrophysics Prof
Physics 160 Stellar Astrophysics Prof. Adam Burgasser Lecture 15 Star Evolu?on I: Stellar Timescales & Post Main Sequence Evolu?on 20 November 2013 Announcements • HW #7 now online, due Friday • Errors in last week’s lectures & HW 6 • First observing lab(s) tomorrow (weather pending) Physics 160 Fall 2013 Lecture 15: Star Evolution I: Stellar Lifetimes and Post Main Sequence Evolution 20 November 2013 PRELIMS • Announcements [5 min] MATERIAL [45 min] • [5 min] Review • [15 min] MS timescales • [20 min] Schonberg-ChandreseKhar limit DEMONSTRATIONS/EXERCISES MATERIALS 1 Physics 160 Fall 2013 Review • we’ve walKed through Pre-MS evolution – Jean’s collapse, homologous contraction & fragmentation, adiabatic limit and preferred stellar mass scale, Hayashi & Henyey tracks, disKs/jets/planets • this messy process leads to a distribution of masses – the mass function – which shows a surprisingly universal form • Now let’s see how stars die Timescales • Free-fall – for homologous collapse, ~ 105 yr • Kelvin-Helmholtz – L ~ GM2Δ(1/R)/Δt ~ 105-107 yr (≈40 Myr for Sun) • Nuclear burning timescale: τMS ~ εMc2/L, ε is conversation factor o From Stefan-Boltzmann, density, ideal gas and pressure gradient we can derive scaling relations between L and M and T and M and o τMS ~ 1010 yr (M/Msun)-2.5 Evolution along the MS • H->He => µ -> ½ -> 4/3 • P ~ ρT/µ => core ρ & T increase 4 • L ~ εnuc ~ ρT => Luminosity increases too • Increased energy flow => radius increases • For Sun, ΔL ~ 50%, ΔT ~ 100 K since ZAMS • Faint young Sun paradox: why wasn’t Earth -
Eighth World Conference on Nondestructive Testing Huitieme Conference Moiudiale Sur Les Essais Non Destructifs
./ 1ÍOIS_ UJ._ EIGHTH WORLD CONFERENCE ON NONDESTRUCTIVE TESTING HUITIEME CONFERENCE MOIUDIALE SUR LES ESSAIS NON DESTRUCTIFS A NONDESTRUCTIVE EXAMINATION PROGRAM FOR UNCLAD CARBON-COMPOSITE REACTOR FUEL ELEMENTS UN PROGRAMME D'KSSAIS NON DESTRUCTIFS POUR LES ELEMENTS COMBUSTIBLES DE REACTEUR NON GAINÊS EN COMPOSITE DU CARBONE FULLBRIGHT H. J. LOS ALAMOS, NEW MEXICO LOS ALAMOS SCIENTIFIC LABORATORY U. S. A. SUMMARY- ^ non<lestructive testing program for the examination of (U,Zr)C—C reactor fuel elements is described. RESUME :O n décrit un programme d'essais non destructifs pour examiner les elements combustibles de réacteur en (U.Zr)C-C. I. INTRODUCTION The Los Alamos Scientific Laboratory has been active for the past twenty years in the development and testing of graphitic-based high temperature reactor fuel elements. The initial involvement was in the field of nuclear propulsion systems. Project Rover began as a program to develop a nuclear-powered, hydrogen-propelled rocket engine. The target exhaust temperature of the propellant was about 2775 K. The fuel element for such an engine would have to maintain its integrity and strength at higher temperatures and would have to resist currosion by the hot hydrogen gas, which is very reactive. These constraints limited the choice of materials to a very few. Carbon melts above about 3800 K, has excellent high-tenperature strength, and is not a strong neutron absorber. It is very reactive to high temperature hydrogen. The basic fuel element foi the Rover Program became uranium-loaded graphite. The enriched uranium fuel was incorporated into the graphite matrix as uranium oxide, later as py- rolytic-carbon coated uranium dicarbide inicrospheres, and, aosf recently, as a solid solution of uranium carbide and zirconium carbide. -
2.10. Neutron Activation of Paintings
2.10. Neutron activation of paintings Possible applications: • Pigment analysis by activation techniques • Neutron radiography by neutron absorption ⇒ Autoradiography Requires neutron irradiation of the entire painting using homogenous neutron flux followed by subsequent point by point raster activation measurement. Technical approach with reactors Neutron guide line is needed for providing sufficient neutron flux (~1014 neutrons/cm2/s) for activation of bulky materials outside the reactor core! 4,7 m shielding door shielding neutrons painting 2.5 m Activation with subsequent X-ray and γ-ray detection 63Cu(n,γ)64Cu, Cu(x) 202Hg(n,γ)203Hg, Hg(x) X-ray data provides pigment position γ-ray data provides pigment characteristics Timescale and Radiation Sensitivity Anthony van Dyck, Saint Rosalie praying for the Plague stricken of Palermo 1624 radiograph Pigment identification by analysis of time dependence for characteristic activity 3rd run Pigment identification by analysis of time dependence for characteristic activity 6th run Pigment identification by analysis of time dependence for characteristic activity 8th run Young man in the background Maryan Wynn Ainsworth et al. Art and Autoradiography; Metropolitan Museum of Art, New York; (1987) 12-18 Van Dyck Self-Portrait Head also visible in X-ray radiograph Self-Portrait of van Dyck 1622 St. Sebastian ca 1649 Painting in the Gemäldegalerie Berlin original by Georges de la Tour (1593-1652) French Court Painter Original in Louvre, question about authorship of copy, George de la Tour himself or by his son Entienne de la Tour? Neutron radiated 109 n/cm2s Neutron induced γ activity is recorded in different time steps: e.g. -
A Comparison of Advanced Nuclear Technologies
A COMPARISON OF ADVANCED NUCLEAR TECHNOLOGIES Andrew C. Kadak, Ph.D MARCH 2017 B | CHAPTER NAME ABOUT THE CENTER ON GLOBAL ENERGY POLICY The Center on Global Energy Policy provides independent, balanced, data-driven analysis to help policymakers navigate the complex world of energy. We approach energy as an economic, security, and environmental concern. And we draw on the resources of a world-class institution, faculty with real-world experience, and a location in the world’s finance and media capital. Visit us at energypolicy.columbia.edu facebook.com/ColumbiaUEnergy twitter.com/ColumbiaUEnergy ABOUT THE SCHOOL OF INTERNATIONAL AND PUBLIC AFFAIRS SIPA’s mission is to empower people to serve the global public interest. Our goal is to foster economic growth, sustainable development, social progress, and democratic governance by educating public policy professionals, producing policy-related research, and conveying the results to the world. Based in New York City, with a student body that is 50 percent international and educational partners in cities around the world, SIPA is the most global of public policy schools. For more information, please visit www.sipa.columbia.edu A COMPARISON OF ADVANCED NUCLEAR TECHNOLOGIES Andrew C. Kadak, Ph.D* MARCH 2017 *Andrew C. Kadak is the former president of Yankee Atomic Electric Company and professor of the practice at the Massachusetts Institute of Technology. He continues to consult on nuclear operations, advanced nuclear power plants, and policy and regulatory matters in the United States. He also serves on senior nuclear safety oversight boards in China. He is a graduate of MIT from the Nuclear Science and Engineering Department. -
Advanced Nuclear Power and Fuel Cycle Technologies: Outlook and Policy Options
Order Code RL34579 Advanced Nuclear Power and Fuel Cycle Technologies: Outlook and Policy Options July 11, 2008 Mark Holt Specialist in Energy Policy Resources, Science, and Industry Division Advanced Nuclear Power and Fuel Cycle Technologies: Outlook and Policy Options Summary Current U.S. nuclear energy policy focuses on the near-term construction of improved versions of existing nuclear power plants. All of today’s U.S. nuclear plants are light water reactors (LWRs), which are cooled by ordinary water. Under current policy, the highly radioactive spent nuclear fuel from LWRs is to be permanently disposed of in a deep underground repository. The Bush Administration is also promoting an aggressive U.S. effort to move beyond LWR technology into advanced reactors and fuel cycles. Specifically, the Global Nuclear Energy Partnership (GNEP), under the Department of Energy (DOE) is developing advanced reprocessing (or recycling) technologies to extract plutonium and uranium from spent nuclear fuel, as well as an advanced reactor that could fully destroy long-lived radioactive isotopes. DOE’s Generation IV Nuclear Energy Systems Initiative is developing other advanced reactor technologies that could be safer than LWRs and produce high-temperature heat to make hydrogen. DOE’s advanced nuclear technology programs date back to the early years of the Atomic Energy Commission in the 1940s and 1950s. In particular, it was widely believed that breeder reactors — designed to produce maximum amounts of plutonium from natural uranium — would be necessary for providing sufficient fuel for a large commercial nuclear power industry. Early research was also conducted on a wide variety of other power reactor concepts, some of which are still under active consideration. -
Assessing Potential Induced Radioactivity in Materials Processed with X-Ray Energy Above 5 Mev: Assessment Protocols and Practical Experience
FERMILAB-PUB-20-562-DI Assessing potential induced radioactivity in materials processed with X-ray energy above 5 MeV: Assessment protocols and practical experience Hervé Michel1; Thomas Kroc2; Brian J. McEvoy 3; Deepak Patil4 Pierre Reppert5; Mark A. Smith6 1Director, Radiation Technology EMEAA, STERIS, Hogenweidstrasse 6, 4658 Däniken, Switzerland, [email protected] 2Applications Physicist for Technology Development, Fermilab, Batavia, Illinois, USA, [email protected] 3Senior Director Global Technologies, STERIS, IDA Business & Technology Park, Tullamore, County Offaly, R35 X865, Ireland, [email protected] 4Senior Director, Radiation Technology, 1880 Industrial Drive, Libertyville, IL 60048 [email protected] 5Validation Manager, STERIS, Hogenweidstrasse 6, 4658 Däniken, Switzerland, [email protected] 6Managing Director, Ionaktis, LLC, PO Box 11599, Charlotte, NC 28220 USA [email protected] Abstract In accordance with ISO11137-1 section 5.1.2, ‘the potential for induced radioactivity in product shall be assessed’. This article describes how compliance to this requirement may be achieved using qualified test methods. Materials of consideration are conceptually discussed. Results of testing conducted on products processed with a 7.5 MeV X-ray irradiation process are provided. As X-ray becomes more widely used in healthcare sterilization, having standard assessment protocols for activation coupled with a shared database of material test results will benefit all healthcare product manufacturers seeking to avail of this innovative technology. This manuscript has been authored by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the U.S. Department of Energy, Office of Science, Office of High Energy Physics. 1. Introduction Radioactive material of natural origin is ubiquitous in nature, widely varying in type and amount. -
Boron-Proton Nuclear-Fusion Enhancement Induced in Boron-Doped Silicon Targets by Low-Contrast Pulsed Laser
PHYSICAL REVIEW X 4, 031030 (2014) Boron-Proton Nuclear-Fusion Enhancement Induced in Boron-Doped Silicon Targets by Low-Contrast Pulsed Laser † A. Picciotto,1,* D. Margarone,2, A. Velyhan,2 P. Bellutti,1 J. Krasa,2 A. Szydlowsky,3,4 G. Bertuccio,5 Y. Shi,5 A. Mangione,6 J. Prokupek,2,7 A. Malinowska,4 E. Krousky,8 J. Ullschmied,8 L. Laska,2 M. Kucharik,7 and G. Korn2 1Micro-Nano Facility, Fondazione Bruno Kessler, 38123 Trento, Italy 2Institute of Physics ASCR, v.v.i. (FZU), ELI-Beamlines Project, 182 21 Prague, Czech Republic 3Institute of Plasma Physics and Laser Microfusion, 01-497 Warsaw, Poland 4National Centre for Nuclear Research, 05-400 Otwock, Poland 5Politecnico di Milano, Department of Electronics Information and Bioengineering, 22100 Como, Italy 6Institute of Advanced Technologies, 91100 Trapani, Italy 7Czech Technical University in Prague, FNSPE, 115 19 Prague, Czech Republic 8Institute of Plasma Physics of the ASCR, PALS Laboratory, 182 00 Prague, Czech Republic (Received 12 January 2014; revised manuscript received 1 April 2014; published 19 August 2014) We show that a spatially well-defined layer of boron dopants in a hydrogen-enriched silicon target allows the production of a high yield of alpha particles of around 109 per steradian using a nanosecond, low-contrast laser pulse with a nominal intensity of approximately 3 × 1016 Wcm−2. This result can be ascribed to the nature of the long laser-pulse interaction with the target and with the expanding plasma, as well as to the optimal target geometry and composition. The possibility of an impact on future applications such as nuclear fusion without production of neutron-induced radioactivity and compact ion accelerators is anticipated.