A Review of Stored Energy Release of Irradiated Graphite

Total Page:16

File Type:pdf, Size:1020Kb

A Review of Stored Energy Release of Irradiated Graphite Nidia C. Gallego P.O. Box 2008 Oak Ridge, TN 37831-6087 Telephone (865) 241-9459 FAX: (865) 576-8424 e-mail: [email protected] September 29, 2011 Makuteswara Srinivasan U.S. Nuclear Regulatory Commission RES/DE/CMB M.S. T-10 M10 Washington, DC 20555-0001 Dear Srini: Milestone Report ORNL/TM-2011/378 in completion of Task 1 for JCN N6988 / V6210 Attached is the subject ORNL/TM Report entitled: “A Review of Stored Energy Release of Irradiated Graphite” documenting work under Task 1 for project JCN N6988 / V6210, “HTGR Graphite Stored Energy Release,” If you have any questions regarding the report or need additional information, please contact me. Sincerely, Nidia Gallego Carbon Materials Technology Group Materials Science and Technology Division Enclosure c/enc: L. D. Aloisi T. D. Burchell M. Gavrilas J. J. Simpson [email protected] [email protected] File-RC ORNL/TM-2011/378 A Review of Stored Energy Release of Irradiated Graphite September 2011 Prepared by N. C. Gallego T. D. Burchell DOCUMENT AVAILABILITY Reports produced after January 1, 1996, are generally available free via the U.S. Department of Energy (DOE) Information Bridge. Web site http://www.osti.gov/bridge Reports produced before January 1, 1996, may be purchased by members of the public from the following source. National Technical Information Service 5285 Port Royal Road Springfield, VA 22161 Telephone 703-605-6000 (1-800-553-6847) TDD 703-487-4639 Fax 703-605-6900 E-mail [email protected] Web site http://www.ntis.gov/support/ordernowabout.htm Reports are available to DOE employees, DOE contractors, Energy Technology Data Exchange (ETDE) representatives, and International Nuclear Information System (INIS) representatives from the following source. Office of Scientific and Technical Information P.O. Box 62 Oak Ridge, TN 37831 Telephone 865-576-8401 Fax 865-576-5728 E-mail [email protected] Web site http://www.osti.gov/contact.html This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof. ORNL/TM-2011/378 Materials Science and Technology Division A Review of Stored Energy Release of Irradiated Graphite N. C. Gallego T. D. Burchell Manuscript Completed: April 2011 Date Published: September 2011 Prepared for Division of Engineering Office of Nuclear Regulatory Research U.S. NUCLEAR REGULATORY COMMISSION Washington, DC 20555 NRC Job Code V6210 Prepared by OAK RIDGE NATIONAL LABORATORY Oak Ridge, Tennessee 37831-6283 managed by UT-BATTELLE, LLC for the U.S. DEPARTMENT OF ENERGY under contract DE-AC05-00OR22725 This page is intentionally left blank. ii Contents Figures .......................................................................................................................................................... v Tables .......................................................................................................................................................... vii Executive Summary ..................................................................................................................................... ix Acknowledgments ........................................................................................................................................ xi Acronyms and Abbreviations .................................................................................................................... xiii 1 Introduction ............................................................................................................................................ 1 2 Graphite and Its Role in HTGRs ............................................................................................................ 3 3 Irradiation-Induced Damage in Graphite ................................................................................................ 6 3.1 Effect of neutron irradiation on graphite properties ..................................................................... 6 3.1.1 Effects of irradiation on dimensional changes ................................................................. 6 3.1.2 Effects of irradiation on mechanical properties ............................................................... 9 3.1.3 Effects of irradiation on thermal conductivity ............................................................... 10 3.1.4 Effects of irradiation on thermal expansion ................................................................... 11 3.1.5 Effects of irradiation on specific heat ............................................................................ 12 3.1.6 Effects of irradiation on electrical resistivity ................................................................. 12 3.2 Theory of displacement damage due to neutron irradiation ....................................................... 12 4 Wigner Energy ..................................................................................................................................... 17 4.1 Total stored energy of irradiated graphite .................................................................................. 17 4.2 Rate of release of stored energy of irradiated graphite ............................................................... 19 4.3 Interpretation of stored energy data ............................................................................................ 22 4.3.1 Effects of irradiation dose at low irradiation temperatures ............................................ 22 4.3.2 Effects of irradiation temperature .................................................................................. 25 4.3.3 Effects of the degree of graphitization ........................................................................... 31 4.3.4 Release curves at high annealing temperatures ............................................................. 33 5 Implications of the Wigner Energy Content ......................................................................................... 43 6 Stored Energy and HTGR .................................................................................................................... 45 7 Summary .............................................................................................................................................. 48 Appendix A. Conversion Factors for Irradiation Dose ............................................................................... 49 References ................................................................................................................................................... 50 iii This page is intentionally left blank. iv Figures 1. SC-MHR reactor system cutaway showing graphite core components ................................................ 4 2. Schematic of lattice defects introduced by radiation in graphite .......................................................... 7 3. Neutron irradiation-induced a-axis shrinkage behavior of pyrolytic graphite showing the effects of graphitization temperature on the magnitude of the dimensional changes ........................... 8 4. Irradiation-induced volume changes for H-451 graphite at two irradiation temperatures .................... 9 5. Dimensional change behavior of H-451 graphite at an irradiation temperature of 600 °C and 900 °C ............................................................................................................................................. 9 6. Neutron irradiation-induced Young’s modulus changes for GraphNOL N3M at irradiation temperatures 600 and 875 °C .............................................................................................................. 10 7. Temperature dependence of thermal conductivity in the irradiated and unirradiated condition for typical nuclear grade graphite ....................................................................................................... 11 8. The irradiation-induced changes in CTE (25–500 °C) for GraphNOL N3M graphite at two irradiation temperatures ...................................................................................................................... 12 9. Sequential HRTEM images illustrating the formation rates of interlayer defects at different temperatures with the same time scale (0 to 220 seconds) .................................................................. 14 10. Normalized formation rate of the clusters of I-V pair defects per unit area of bilayer estimated in HRTEM images recorded at different temperatures ....................................................................... 15 11. Accumulation of total stored energy as a function of dose in graphite at various irradiation temperatures .......................................................................................................................................
Recommended publications
  • Testimony of L Wayne,D Dupont,B Norton,M Kaku,M Pulido, R Kohn
    _ _ __ l I - PA N E L- [ " * u hv/s3 | CNEMICAI, REACTIONS I | Introduction 1. In 1957,~a very serious fire occurred at a non-power reactor located at Vindscale, England. Although the reactor was a production reactor, it had a number of sinhities to the UCIA reacter-- fuel containing uranium metal clad in aluminum, with a graphite moderator / reflector, and normal operation at relatively low temperatures, which permitted build-up of stored "Vigner" energy in the graphite. Release of that r stored energy contributed to the cause of the fire, which resulted in extensive daanse and 20,000 curies of iodine-131 being released to the environment. Milk contaminated with I-131 had to be disposed of in an area of 200 square miles around the reactor because of the accident. , l 2 In 1960, the UCIA Argonaut-type reactor began operation. Its Hasards Analysis did not addrissa Vigner energy storage, and a brief paragraph ; dismissed the potential for fire largely based on the assertion that | "none of the anterials of construction of the reactor are infh==mble." (p.62) 3. As the Windacale fire showed, and as shall be discussed in detail below, that assertion is dangerously untrue.* The graphite can burns i the uranium metal can burns the angnesium can burns even the aluminum ' under sono circumstances will burn. And ignoring Vigner energy can like- vise be dangerous. 4 It has further been asserted that the only chemical reaction of signif- icance to be considered for the UCIA reactor is a water reaction with aluminum, and that aluminum weald have to be in the form of metal filings | for such a reaction to occur.
    [Show full text]
  • The New Nuclear Forensics: Analysis of Nuclear Material for Security
    THE NEW NUCLEAR FORENSICS Analysis of Nuclear Materials for Security Purposes edited by vitaly fedchenko The New Nuclear Forensics Analysis of Nuclear Materials for Security Purposes STOCKHOLM INTERNATIONAL PEACE RESEARCH INSTITUTE SIPRI is an independent international institute dedicated to research into conflict, armaments, arms control and disarmament. Established in 1966, SIPRI provides data, analysis and recommendations, based on open sources, to policymakers, researchers, media and the interested public. The Governing Board is not responsible for the views expressed in the publications of the Institute. GOVERNING BOARD Sven-Olof Petersson, Chairman (Sweden) Dr Dewi Fortuna Anwar (Indonesia) Dr Vladimir Baranovsky (Russia) Ambassador Lakhdar Brahimi (Algeria) Jayantha Dhanapala (Sri Lanka) Ambassador Wolfgang Ischinger (Germany) Professor Mary Kaldor (United Kingdom) The Director DIRECTOR Dr Ian Anthony (United Kingdom) Signalistgatan 9 SE-169 70 Solna, Sweden Telephone: +46 8 655 97 00 Fax: +46 8 655 97 33 Email: [email protected] Internet: www.sipri.org The New Nuclear Forensics Analysis of Nuclear Materials for Security Purposes EDITED BY VITALY FEDCHENKO OXFORD UNIVERSITY PRESS 2015 1 Great Clarendon Street, Oxford OX2 6DP, United Kingdom Oxford University Press is a department of the University of Oxford. It furthers the University’s objective of excellence in research, scholarship, and education by publishing worldwide. Oxford is a registered trade mark of Oxford University Press in the UK and in certain other countries © SIPRI 2015 The moral rights of the authors have been asserted All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, without the prior permission in writing of SIPRI, or as expressly permitted by law, or under terms agreed with the appropriate reprographics rights organizations.
    [Show full text]
  • Neutronics Analysis of a Modified Pebble Bed Advanced High Temperature Reactor
    NEUTRONICS ANALYSIS OF A MODIFIED PEBBLE BED ADVANCED HIGH TEMPERATURE REACTOR THESIS Presented in Partial Fulfillment of the Requirements for the Degree of Master of Science in the Graduate School of The Ohio State University By Jorge Abejón Orzáez Ingeniero Industrial, Diplôme d’Ingénieur ****** The Ohio State University 2009 Thesis Committee: Approved by: Dr. Thomas E. Blue, Advisor __________________ Dr. Xiaodong Sun, Co-Advisor __________________ Advisor Nuclear Engineering Graduate Program ABSTRACT The objective of this research is to, based on the original design for the Pebble Bed Advanced High Temperature Reactor (PB-AHTR), develop an MCNPX model of the reactor core with the objective to attain criticality and to breed new fuel. A brief but complete description of a first approach to the PB-AHTR will be provided and a MCNPX model will be run in order to ascertain the difficulties of that configuration. On the second part, a modification of the original model will be evaluated and compared in order to resolve the difficulties encountered in the original design. Finally, in an effort to optimize the design, an evolutionary approach will be analyzed, based on the previous model, and conclusions will be attained ii Dedicated to my family and friends iii ACKNOWLEDGEMENTS I would like to thank Dr. Blue and Dr. Sun for all their guidance and assistance throughout my time as a graduate student. I would like to thank John Kulisek as a reference, guide and friend throughout my entire Master’s Degree program. I would like to thank Jeremy Chenkovich and Steven Stone for their help and their patience with me in my first steps in the Master’s Degree program.
    [Show full text]
  • Management of Radioactive Waste Containing Graphite: Overview of Methods
    energies Review Management of Radioactive Waste Containing Graphite: Overview of Methods Leon Fuks * , Irena Herdzik-Koniecko, Katarzyna Kiegiel and Grazyna Zakrzewska-Koltuniewicz Centre for Radiochemistry and Nuclear Chemistry, Institute of Nuclear Chemistry and Technology, 16 Dorodna, 03-161 Warszawa, Poland; [email protected] (I.H.-K.); [email protected] (K.K.); [email protected] (G.Z.-K.) * Correspondence: [email protected]; Tel.: +48-22-504-1360 Received: 30 July 2020; Accepted: 4 September 2020; Published: 7 September 2020 Abstract: Since the beginning of the nuclear industry, graphite has been widely used as a moderator and reflector of neutrons in nuclear power reactors. Some reactors are relatively old and have already been shut down. As a result, a large amount of irradiated graphite has been generated. Although several thousand papers in the International Nuclear Information Service (INIS) database have discussed the management of radioactive waste containing graphite, knowledge of this problem is not common. The aim of the paper is to present the current status of the methods used in different countries to manage graphite-containing radioactive waste. Attention has been paid to the methods of handling spent TRISO fuel after its discharge from high-temperature gas-cooled reactors (HTGR) reactors. Keywords: graphite; irradiated graphite; graphite processing; radioactive waste; waste management; waste disposal; spent TRISO fuel 1. Introduction As of December 31, 2018, 451 nuclear power reactors were in operation and produced 392,779 MWe of electricity. Fifty-five reactors, with a net capacity of 57,441 MWe, were under construction, while 172 reactors were permanently shut down [1].
    [Show full text]
  • Nuclear Glossary 2007-06
    Forschungszentrum Karlsruhe Technik und Umwelt GLOSSARY OF NUCLEAR TERMS Winfried Koelzer © Forschungszentrum Karlsruhe GmbH, Karlsruhe, April 2001 Postfach 3640 · 76021 Karlsruhe, Germany Original title: Lexikon zur Kernenergie, ISBN 3-923704-32-1 Translation by Informationskreis KernEnergie The reproduction of trade names, identifications, etc. in this glossary does not justify the assumption that such names may be considered free in the sense- of the laws regulating the protection of trade marks and brands and that therefore they may be used by everyone. No guarantee is given for the correctness of numerical data. Pictures by: Argonne National Lab., Argonne Aulis-Verlag Deubner & Co., Cologne Forschungszentrum Karlsruhe, Karlsruhe Informationskreis Kernenergie, Bonn A Absorbed dose The absorbed dose D is the quotient of the average energy transferred to the matter in a volume element by ionizing radiation and the mass of the matter in this volume element: _ d ε D = . dm The unit of the absorbed dose is joule divided by kilogram (J·kg-1) and its special unit name is gray (Gy). The former unit name was rad (symbol: rd or rad).1 Gy = 100 rd; 1 rd = 1/100 Gy. Absorbed dose rate Quotient of absorbed dose per unit of time. Unit: Gy/h. Absorber Any material "stopping" ionizing radiation. Alpha radiation can already be totally absorbed by a sheet of paper; beta radiation is absorbed by a few centimetres of plastic material or 1 cm of aluminium. Materials with a high →atomic number and high density are used for gamma radiation absorbers (lead, steel, concrete, partially with special additions). Neutron absorbers such as boron, hafnium and cadmium are used in control rods for reactors.
    [Show full text]
  • Thermophysical Properties of Materials for Nuclear Engineering: a Tutorial and Collection of Data
    Thermophysical Properties of Materials For Nuclear Engineering: A Tutorial and Collection of Data INTERNATIONAL ATOMIC ENERGY AGENCY VIENNA 2008 The originating Section of this publication in the IAEA was: Nuclear Power Technology Development Section International Atomic Energy Agency Wagramer Strasse 5 P.O. Box 100 A-1400 Vienna, Austria THERMOPHYSICAL PROPERTIES OF MATERIALS FOR NUCLEAR ENGINEERING: A TUTORIAL AND COLLECTION OF DATA IAEA, VIENNA, 2008 IAEA-THPH ISBN 978–92–0–106508–7 © IAEA, 2008 Printed by the IAEA in Austria November 2008 FOREWORD Renewed interest in the potential of nuclear energy to contribute to a sustainable worldwide energy mix is strengthening the IAEA’s statutory role in fostering the peaceful uses of nuclear energy, in particular the need for effective exchanges of information and collaborative research and technology development among Member States on advanced nuclear power technologies (Articles III-A.1 and III-A.3). To meet Member States’ needs, the IAEA conducts activities to foster information exchange and collaborative research development in the area of advanced nuclear reactor technologies. These activities, implemented with the advice and support of the various technical working groups of the IAEA’s Department of Nuclear Energy, include coordination of collaborative research, organization of international information exchange and analyses of globally available technical data and results, with a focus on reducing nuclear power plant capital costs and construction periods while further improving performance, safety and proliferation resistance. In other activities, evolutionary and innovative advances are catalyzed for all reactor lines such as advanced water cooled reactors, high temperature gas cooled reactors, liquid metal cooled reactors and accelerator driven systems, including small and medium sized reactors.
    [Show full text]
  • Thorium Research in the Manhattan Project Era
    University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Masters Theses Graduate School 5-2014 Thorium Research in the Manhattan Project Era Kirk Frederick Sorensen University of Tennessee - Knoxville, [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_gradthes Recommended Citation Sorensen, Kirk Frederick, "Thorium Research in the Manhattan Project Era. " Master's Thesis, University of Tennessee, 2014. https://trace.tennessee.edu/utk_gradthes/2758 This Thesis is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Masters Theses by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a thesis written by Kirk Frederick Sorensen entitled "Thorium Research in the Manhattan Project Era." I have examined the final electronic copy of this thesis for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Master of Science, with a major in Nuclear Engineering. Ondrej Chvala, Major Professor We have read this thesis and recommend its acceptance: Laurence Miller, Howard Hall Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Thorium Research in the Manhattan Project Era A Thesis Presented for the Master of Science Degree The University of Tennessee, Knoxville Kirk Frederick Sorensen May 2014 © by Kirk Frederick Sorensen, 2014 All Rights Reserved. ii to my patient and wonderful wife Quincy..
    [Show full text]
  • A Selected Bibliography of Publications By, and About, Eugene Wigner
    A Selected Bibliography of Publications by, and about, Eugene Wigner Nelson H. F. Beebe University of Utah Department of Mathematics, 110 LCB 155 S 1400 E RM 233 Salt Lake City, UT 84112-0090 USA Tel: +1 801 581 5254 FAX: +1 801 581 4148 E-mail: [email protected], [email protected], [email protected] (Internet) WWW URL: http://www.math.utah.edu/~beebe/ 08 June 2021 Version 1.108 Title word cross-reference + [LPN11]. 0 [OW84]. $1 [Duf46]. 1=2 [Lan87, OW84]. $15.00 [Kol60]. 2 [LR83, RI03]. 3 [Bru85, Bru87, Loc76, RY03, SG75, Win76]. 3j [Max10]. $4.00 [Bec58, Edw60]. $49.50 [Sch85]. 6 [Bru85, Bru87, RY03, SG75]. 6j [LY09, Max10]. 6 × 9 [Wig65c]. 6 × 9:25 [Bec58, Edw60]. $7.50 [Pai67a, Wei69a]. $7.75 [Wig65c]. $8 [Wig64f]. 9 [CD79, Ear81, Hol73a, Jan68, Wu72, Wu73]. 9j [Max10, Ros98, Ros99]. ∗ 4 8 + [Fro79]. [CPCF99]. [BW37, WB36]. 2 [LPN11, SBR 86]. 3 [DA73]. n [BGL67, Tem07]. A [Wig36a]. β [RW54, WB36, Wig39a]. C∗ [BG02, BG03, CIMS08]. C2 [Pos00]. D [Mar06a, PFG06, Nou99]. E(2) 2 [Got71]. E = mc [KN19]. h [CMS77]. ¯h → 0 [Ara95]. ISOn [Wol71]. IUn [Wol72]. j [Bru85, Bru87, CD79, Ear81, Hol73a, Jan68, JF16, Loc76, RY03, SG75, Win76, Wu72, Wu73]. ≤ 80 [CM66]. m [Beh94]. C2 [Pos01]. }l(1|n) [LSV08]. SU (3) [RSdG99]. SU (3) ⊃ U (2) [PD98]. SU (n) [PD98]. µ [BZ74]. N [HW35]. n ≥ 2 [SW67]. O(5) [HST74]. O(5) ⊆ O(3) [CFM78]. O(¯h8) 1 2 [Sha92]. O(n) [Gou81, Gou86b]. OSp(1; 2) [ZY88]. SA(4; R) [LNPC92]. πN → πBs [KAUZ71].
    [Show full text]
  • Irradiated Graphite Waste - Stored Energy
    Irradiated Graphite Waste - Stored Energy A thesis submitted to the University of Manchester for the degree of Doctor of Philosophy in the Faculty of Engineering and Physical Sciences 2012 Michael Lasithiotakis School of Materials Materials Performance Centre 1 2 List of Contents List of Contents List of Contents 3 List of Figures 5 List of Tables 8 Abstract 9 Declaration 10 Copyright Statement 11 Rationale for Submitting the Thesis in Alternative Format 12 Acknowledgements 13 Dedication 14 Chapter 1 - Introduction and Context of Research 15 Graphite 15 Nuclear reactors 17 Decommissioning of a Nuclear Facility 17 Radioactive Waste-Disposal of Radioactive Waste 17 Wigner Energy – An additional hazard during decommissioning. 21 The Windscale fire event – A nuclear accident that directly involved Wigner energy release 23 Chapter 2 - Literature Review 25 Stored Energy Release 25 Defects 27 Annealing of Defects 32 Kinetics of Stored Energy Release 37 Ion irradiation : A Method to Simulate Irradiation Damage. 48 Chapter 3- Methods 51 Differential Scanning Calorimetry 51 X-ray Diffraction 55 Raman Spectroscopy 62 Chapter 4 - Publication I: Application of an Independent Parallel Reactions Model to the Annealing Kinetics on BEPO Irradiated Graphite 67 3 List of Contents Chapter 5 - Publication II: Annealing of ion irradiation damage in nuclear graphite 68 Chapter 6 - Publication III: Application of an Independent Parallel Reactions Model on the Annealing Kinetics of BEPO Irradiated Graphite 69 Chapter 7 - General Conclusions and Future Work 70 Bibliography 73 Total Word Count : 43,227 words 4 List of Figures List of Figures Figure 1.1. Pg 16. A scheme of the manufacturing stages of nuclear graphite.
    [Show full text]
  • Radiation-Damage Robust, Engineered, Self-Repairing Meso-Materials L
    Radiation-Damage Robust, Engineered, Self-repairing Meso-Materials L. Popa-Simil* *LAAS, Los Alamos Academy of Sciences Los Alamos, NM 87544, USA, [email protected] ABSTRACT chain of free radical polymerization reactions with other molecules, yielding compounds with increasing molecular Nuclear power is one of the most compact, long lasting and weight. Liquids lack fixed internal structure, therefore the might be the most safe and environmentally friendly energy effects of radiation is limited to radiolysis that is altering source if it might be done right, by achieving the harmony the chemical composition of the liquids, one of the primary between the nuclear reactions inside and the material mechanisms is formation of free radicals. structure these reactions took place. All liquids are subject to radiation damage, with few The structural materials used inside a nuclear power source, exotic exceptions as liquid metals like molten sodium or mainly stainless steel, zircalloy, etc., are suffering the LBE, where there are no chemical bonds to be disrupted. radiation damage, and achieving high burnup factors, or Liquid water or hydrogen fluoride, produces gaseous near perfect burning is practically impossible using the hydrogen and oxygen respectively fluorine, which present metallic alloys, due to safety reasons. spontaneously react back to releasing the reaction energy. Producing robust materials with micro-structure shape Absorption of neutrons in hydrogen nuclei leads to memory, like SiN, Ti, composites, etc., whose properties to buildup of deuterium and tritium in the water. be constant with neutron fluence, or dose after impaired by Two main approaches to reduce radiation damage are: radiation damage, come back to the initial structure and -reducing the amount of energy deposited in the recover, process also known as self-repairing mechanism.
    [Show full text]
  • Eugene Wigner and Nuclear Energy P. 3 Memoir of the Uranium Project P
    Introduction: Eugene Wigner and Nuclear Energy p. 3 Memoir of the Uranium Project p. 23 The Pre-Chicago Days Annotation p. 133 For Discussion of the Homogeneous and Lattice Arrangements for Power Plants p. 135 Approximation for Radius of Sphere Sufficient for Chain Reaction in Light Isotope p. 142 Diffusion of Slow Neutrons in Absorbing Materials p. 149 Solution of Boltzmann's Equation for Monoenergetic Neutrons in an Infinite p. 154 Homogeneous Medium Review of the Measurements of the Resonance Absorption of Neutrons by Uranium in Bulk p. 165 Resonance Absorption of Neutrons by Spheres p. 168 Effect of Geometry on Resonance Absorption of Neutrons by Uranium p. 179 Effect of Temperature on Total Resonance Absorption of Neutrons by Spheres of Uranium p. 184 Oxide Absorption of Thermal Neutrons in Uranium p. 188 Density of Neutrons in Carbon Block with and without Absorbing Material p. 219 Reactor Engineering at Chicago, 1942-1945, and at Clinton, 1946-1947 Annotation p. 239 Plutonium-Producing Reactors Report of the Committee for the Examination of the Moore-Leverett Design of a He-Cooled p. 244 Plant General Considerations Concerning the Lattice Structure p. 254 Survey of the Power Plant Problem p. 257 A Plant with Water Cooling p. 262 On a Plant with Water Cooling p. 264 Preliminary Process Design of Liquid Cooled Power Plant Producing 5 x 10[superscript p. 297 5] kW Memorandum from P-9 Committee p. 360 Breeders Breeders and Converters: Minutes of Lecture on April 7, 1945 p. 376 Preliminary Calculations on a Breeder with Circulating Uranium p. 381 New Ideas for Nuclear Reactors p.
    [Show full text]
  • Thorium Research in the Manhattan Project Era
    Thorium Research in the Manhattan Project Era Kirk Sorensen August 14, 2013 Abstract Research on thorium as an energy source began in 1940 under the direction of Glenn Seaborg at the University of California, Berkeley. Following the discovery of plutonium-239 and its fissile qualities, similar experiments demonstrated that uranium-233 bred from thorium was also fissile. Seaborg viewed uranium-233 as a potential backup to plutonium-239, whose production was one of the Manhattan Project’s primary efforts. The central appeal of U-233 was that the chemistry of uranium was well understood, unlike plutonium, but plutonium-239 had the potential to be produced from natural uranium in a critical nuclear reactor. Natural thorium lacked fissile isotopes and so a critical nuclear reactor (to produce U-233) from tho- rium alone was not possible. Not until the X-10 graphite reactor was constructed at Oak Ridge in 1943 was sufficient U-233 created to conclusively assess its nuclear properties, which were found to be superior to Pu-239 in a thermal-spectrum reactor. Early production of plutonium at X-10 showed significant contamination by Pu-240, which made plutonium unsuitable for simple "gun-type" nuclear weapons. Researchers in the "Metallurgical Laboratory" at the Uni- versity of Chicago, which included Seaborg’s chemistry group, suggested that the plutonium produced be used as a fuel in a special reactor to convert thorium to uranium-233 for weapons. This effort encountered many severe difficulties in fuel fabrication and dissolution. Seaborg also recognized the severe issue that uranium-232 contamination would play in any effort to use uranium-233 for weapons.
    [Show full text]