RCC-Mrx Chairwoman CEA - Senior Expert in Design Codes and Standards for Mechanical Components
Total Page：16
File Type：pdf, Size：1020Kb
Load more
Recommended publications
-
Development of an On-Line Fuel Failure Monitoring System For
DEVELOPMENT OF AN ON-LINE FUEL FAILURE MONITORING SYSTEM FOR CANDU REACTORS DEVELOPPEMENT D'UN SYSTEME DE SURVEILLANCE EN LIGNE POUR DES RUPTURES DE GAINES DES REACTEURS CANDU A Thesis Submitted to the Division of Graduate Studies of the Royal Military College of Canada by Stephen Jason Livingstone, BSc, MSc Sub-Lieutenant In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy March 2012 ©This thesis may be used within the Department of National Defence but copyright for open publication remains the property of the author. Library and Archives Bibliotheque et Canada Archives Canada Published Heritage Direction du Branch Patrimoine de I'edition 395 Wellington Street 395, rue Wellington Ottawa ON K1A0N4 Ottawa ON K1A 0N4 Canada Canada Your file Votre reference ISBN: 978-0-494-83407-7 Our file Notre reference ISBN: 978-0-494-83407-7 NOTICE: AVIS: The author has granted a non L'auteur a accorde une licence non exclusive exclusive license allowing Library and permettant a la Bibliotheque et Archives Archives Canada to reproduce, Canada de reproduire, publier, archiver, publish, archive, preserve, conserve, sauvegarder, conserver, transmettre au public communicate to the public by par telecommunication ou par Plnternet, preter, telecommunication or on the Internet, distribuer et vendre des theses partout dans le loan, distrbute and sell theses monde, a des fins commerciales ou autres, sur worldwide, for commercial or non support microforme, papier, electronique et/ou commercial purposes, in microform, autres formats. paper, electronic and/or any other formats. The author retains copyright L'auteur conserve la propriete du droit d'auteur ownership and moral rights in this et des droits moraux qui protege cette these. -
小型飛翔体／海外 ［Format 2］ Technical Catalog Category
小型飛翔体／海外 ［Format 2］ Technical Catalog Category Airborne contamination sensor Title Depth Evaluation of Entrained Products (DEEP) Proposed by Create Technologies Ltd & Costain Group PLC １．DEEP is a sensor analysis software for analysing contamination. DEEP can distinguish between surface contamination and internal / absorbed contamination. The software measures contamination depth by analysing distortions in the gamma spectrum. The method can be applied to data gathered using any spectrometer. Because DEEP provides a means of discriminating surface contamination from other radiation sources, DEEP can be used to provide an estimate of surface contamination without physical sampling. DEEP is a real-time method which enables the user to generate a large number of rapid contamination assessments- this data is complementary to physical samples, providing a sound basis for extrapolation from point samples. It also helps identify anomalies enabling targeted sampling startegies. DEEP is compatible with small airborne spectrometer/ processor combinations, such as that proposed by the ARM-U project – please refer to the ARM-U proposal for more details of the air vehicle. Figure 1: DEEP system core components are small, light, low power and can be integrated via USB, serial or Ethernet interfaces. 小型飛翔体／海外 Figure 2: DEEP prototype software ２．Past experience (plants in Japan, overseas plant, applications in other industries, etc) Create technologies is a specialist R&D firm with a focus on imaging and sensing in the nuclear industry. Createc has developed and delivered several novel nuclear technologies, including the N-Visage gamma camera system. Costainis a leading UK construction and civil engineering firm with almost 150 years of history. -
Re-Examining the Role of Nuclear Fusion in a Renewables-Based Energy Mix
Re-examining the Role of Nuclear Fusion in a Renewables-Based Energy Mix T. E. G. Nicholasa,∗, T. P. Davisb, F. Federicia, J. E. Lelandc, B. S. Patela, C. Vincentd, S. H. Warda a York Plasma Institute, Department of Physics, University of York, Heslington, York YO10 5DD, UK b Department of Materials, University of Oxford, Parks Road, Oxford, OX1 3PH c Department of Electrical Engineering and Electronics, University of Liverpool, Liverpool, L69 3GJ, UK d Centre for Advanced Instrumentation, Department of Physics, Durham University, Durham DH1 3LS, UK Abstract Fusion energy is often regarded as a long-term solution to the world's energy needs. However, even after solving the critical research challenges, engineer- ing and materials science will still impose significant constraints on the char- acteristics of a fusion power plant. Meanwhile, the global energy grid must transition to low-carbon sources by 2050 to prevent the worst effects of climate change. We review three factors affecting fusion's future trajectory: (1) the sig- nificant drop in the price of renewable energy, (2) the intermittency of renewable sources and implications for future energy grids, and (3) the recent proposition of intermediate-level nuclear waste as a product of fusion. Within the scenario assumed by our premises, we find that while there remains a clear motivation to develop fusion power plants, this motivation is likely weakened by the time they become available. We also conclude that most current fusion reactor designs do not take these factors into account and, to increase market penetration, fu- sion research should consider relaxed nuclear waste design criteria, raw material availability constraints and load-following designs with pulsed operation. -
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. -
Uranium (Nuclear)
Uranium (Nuclear) Uranium at a Glance, 2016 Classification: Major Uses: What Is Uranium? nonrenewable electricity Uranium is a naturally occurring radioactive element, that is very hard U.S. Energy Consumption: U.S. Energy Production: and heavy and is classified as a metal. It is also one of the few elements 8.427 Q 8.427 Q that is easily fissioned. It is the fuel used by nuclear power plants. 8.65% 10.01% Uranium was formed when the Earth was created and is found in rocks all over the world. Rocks that contain a lot of uranium are called uranium Lighter Atom Splits Element ore, or pitch-blende. Uranium, although abundant, is a nonrenewable energy source. Neutron Uranium Three isotopes of uranium are found in nature, uranium-234, 235 + Energy FISSION Neutron uranium-235, and uranium-238. These numbers refer to the number of Neutron neutrons and protons in each atom. Uranium-235 is the form commonly Lighter used for energy production because, unlike the other isotopes, the Element nucleus splits easily when bombarded by a neutron. During fission, the uranium-235 atom absorbs a bombarding neutron, causing its nucleus to split apart into two atoms of lighter mass. The first nuclear power plant came online in Shippingport, PA in 1957. At the same time, the fission reaction releases thermal and radiant Since then, the industry has experienced dramatic shifts in fortune. energy, as well as releasing more neutrons. The newly released neutrons Through the mid 1960s, government and industry experimented with go on to bombard other uranium atoms, and the process repeats itself demonstration and small commercial plants. -
Study of Macromolecule-Mineral Interactions on Nuclear Related Materials
Study of macromolecule-mineral interactions on nuclear related materials by Lygia Eleftheriou Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy Supervised by: Prof John Harding Dr Maria Romero-González The University of Sheffield Faculty of Engineering Department of Materials Science and Engineering September 2016 Declaration The work described within this thesis has been completed under the supervision of Prof J. Harding and Dr M. Romero-González at the University of Sheffield between September 2012 and September 2016. This thesis along with the work described here has been completed by the author with some exceptions indicated clearly at the relevant chapters. These include: (1) the construction of ceria models for the computational work that was completed by Dr Colin Freeman and Dr Shaun Hall (described in chapter 5), (2) the purification of peptidoglycan completed by Dr Stephane Mesnage (described in chapter 4) and (3) the electron microscopy analysis completed by Dr Mohamed Merroun (described in chapter 2). Lygia Eleftheriou September 2016 Acknowledgements I would like to express my sincere gratitude to my supervisors Dr Maria Romero González and Prof John Harding for all their support during the past four years. This work would not have been possible without their endless encouragement, guidance and advice. I would also like to thank Dr Colin Freeman, Dr Shaun Hall and Riccardo Innocenti Malini for all the hours they spent trying to make things work and all their help with the computational part of this project. In addition, I would like to thank Dr Simon Thorpe, Dr Stephane Mesnage and Mr Robert Hanson for their help with the analytical methods of this project. -
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. -
Nuclear Reactors Fuelled with Uranium Inevitably Produce Plutonium As a By-Product
The Secretary Joint Standing Committee on Treaties Inquiry into Nuclear Non-proliferation and Disarmament Dear Sir/Madam, I would like to submit the following submission to the Parliamentary Committee Inquiry into Nuclear Non- proliferation and Disarmament. Yours sincerely, Frank Barnaby. A submission to the Parliamentary Committee Inquiry into Nuclear Non- proliferation and Disarmament. Frank Barnaby Nuclear reactors fuelled with uranium inevitably produce plutonium as a by-product. This plutonium can be used by countries and by nuclear terrorists to fabricate nuclear weapons. The operation of nuclear-power reactors, therefore, has consequences for national, regional and global security. The more nuclear reactors there are the greater the security risks. Australia should recognise that these security risks outweigh the befits of producing electricity by nuclear power especially because the use of renewable sources of energy, combined with improvements in energy efficiency and the conservation of energy make the use of nuclear power unnecessary. As the world’s second largest exporter of uranium, Australia has a major responsibility to adopt policies to minimise the risks to security from nuclear proliferation and terrorism. To this end, Australia should use its influence to bring the Comprehensive Nuclear Test Ban Treaty (CTBT) into effect. It should not supply uranium to countries, like the USA and China, which have not yet ratified the CTBT. Moreover, Australia should promote the negotiation of a Comprehensive Fissile Material Cut-Off Treaty to prohibit the further production of fissile material usable for the production of nuclear weapons, prohibit the reprocessing of spent nuclear-power reactor fuel that has been produced by Australian uranium and should not support or encourage the use of Mixed Oxide (MOX) nuclear fuel or the use of Generation IV reactors, particularly fast breeder reactors. -
Physics 111 Fall 2007 Radioactive Decay Problems Solutions
Physics 111 Fall 2007 Radioactive Decay Problems Solutions 3 1. The 1 H isotope of hydrogen, which is called tritium (because it contains three nucleons), has a half-life of 12.33 yr. It can be used to measure the age of objects up to about 100 yr. It is produced in the upper atmosphere by cosmic rays and brought to Earth by rain. As an application, determine approximately the age of a bottle of wine 3 1 whose 1 H radiation is about 10 that present in new wine. Because the tritium in water is being replenished, we assume that the amount is constant until the wine is made, and then it decays. We find the number of half-lives from N n = 1 ; N ()2 0 n 0.10 = 1 , or n log 2 = log 10 , which gives n = 3.32. ()2 () Thus the time is t = nT = 3.32 12.33 yr = 41 yr. 1 ()() 2 2. Strontium-90 is produced as a nuclear fission product of uranium in both reactors and atomic bombs. Look at its location in the periodic table to see what other elements it might be similar to chemically, and tell why you think it might be dangerous to ingest. It has too many neutrons, and it decays with a half-life of about 29 yr. How 90 long will we have to wait for the amount of 38 Sr on the Earth’s surface to reach 1% of its current level, assuming no new material is scattered about? Write down the decay reaction, including the daughter nucleus. -
Perspective the Radioactivity of Atmospheric Krypton in 1949–1950
Proc. Natl. Acad. Sci. USA Vol. 94, pp. 7807–7810, July 1997 Perspective The radioactivity of atmospheric krypton in 1949–1950 Anthony Turkevich*, Lester Winsberg†, Howard Flotow‡, and Richard M. Adams§ Argonne National Laboratory, 9700 S. Cass Avenue, Argonne, IL 60439 Contributed by Anthony Turkevich, April 10, 1997 ABSTRACT The chemical element krypton, whose prin- Libby (in 1948; unpublished work) gave indications that these cipal source is the atmosphere, had a long-lived radioactive predictions were correct. The present report describes the content, in the mid-1940s, of less than 5 dpm per liter of technique that was used soon afterward to establish more krypton. In the late 1940s, this content had risen to values in precisely that atmospheric krypton in the late 1940s was much the range of 100 dpm per liter. It is now some hundred times more radioactive than it had been, and gives the results of some higher than the late 1940 values. This radioactivity is the early measurements of krypton samples isolated from the result of the dissolving of nuclear fuel for military and civilian atmosphere at that time.** purposes, and the release thereby of the fission product krypton-85 (half-life 5 10.71 years, fission yield 5 0.2%). The Measurement Technique present largest emitter of krypton-85 is the French reprocess- ing plant at Cap-de-la-Hague. The measurement technique that was used was influenced by those simultaneously being developed by Libby and Anderson It is generally known that the chemical element krypton, (9) to measure the radiocarbon content of samples of arche- isolated from the atmosphere in 1996, is radioactive. -
Highly Enriched Uranium: Striking a Balance
OFFICIAL USE ONLY - DRAFT GLOSSARY OF TERMS APPENDIX F GLOSSARY OF TERMS Accountability: That part of the safeguards and security program that encompasses the measurement and inventory verification systems, records, and reports to account for nuclear materials. Assay: Measurement that establishes the total quantity of the isotope of an element and the total quantity of that element. Atom: The basic component of all matter. Atoms are the smallest part of an element that have all of the chemical properties of that element. Atoms consist of a nucleus of protons and neutrons surrounded by electrons. Atomic energy: All forms of energy released in the course of nuclear fission or nuclear transformation. Atomic weapon: Any device utilizing atomic energy, exclusive of the means for transportation or propelling the device (where such means is a separable and divisible part of the device), the principal purpose of which is for use as, or for development of, a weapon, a weapon prototype, or a weapon test device. Blending: The intentional mixing of two different assays of the same material in order to achieve a desired third assay. Book inventory: The quantity of nuclear material present at a given time as reflected by accounting records. Burnup: A measure of consumption of fissionable material in reactor fuel. Burnup can be expressed as (a) the percentage of fissionable atoms that have undergone fission or capture, or (b) the amount of energy produced per unit weight of fuel in the reactor. Chain reaction: A self-sustaining series of nuclear fission reactions. Neutrons produced by fission cause more fission. Chain reactions are essential to the functioning of nuclear reactors and weapons. -
X-Ray and Neutron Sources
Chapter 1: Radioactivity Radioactivity from Direct Excitation X‐ray Emission 147 NPRE 441, Principles of Radiation Protection An Overview of Radiation Exposure to US Population 148 NPRE 441, Principles of Radiation Protection Chapter 1: Radioactivity Clinical X‐ray CT System The Siemens SOMATOM X clinical CT system 149 Chapter 1: Radioactivity X‐ray Imaging Examples 150 NPRE 441, Principles of Radiation Protection Chapter 1: Radioactivity X‐ray Generation –X‐ray Tube Andrew Webb, Introduction to Biomedical Imaging, 2003, Wiley‐ Interscience. Motor, Why? Filament Rotating target Electron beam? How are electrons generated? 151 NPRE 441, Principles of Radiation Protection Chapter 1: Radioactivity X‐ray Generation – Bremsstrahlung • Target nucleus positive charge (Z∙p+) attracts incident e‐ • Deceleration of an incident e‐ occurs in the proximity of the target atom nucleus • Energylostbye‐ is gained by the EM photon (x‐ray) generated • The impact parameter distance, the closest approach to the nucleus by the e‐ determines the amount of E loss • The Coulomb force of attraction varies strongly with distance ( 1/r2); ↓ distance →↑deceleration and E loss →↑photon E • Direct impact on the nucleus determines the maximum x‐ray E (Emax) 152 NPRE 441, Principles of Radiation Protection Chapter 1: Radioactivity X‐ray Generation – Bremsstrahlung Interestingly, this process creates a relatively uniform spectrum. Intensity = nh 0 Photon energy spectrum 153 NPRE 441, Principles of Radiation Protection Chapter 1: Radioactivity The Unfiltered Bremsstrahlung Spectrum Thick Target X‐ray Formation We can model target as a series of thin targets. Electrons successively loses energy as they moves deeper into the target. Electrons X‐rays Relative Intensity 0 Each layer produces a flat energy spectrum with decreasing peak energy level.