Design and Development of an External Fast Neutron Beam Facility at the Ohio State University Research Reactor

Total Page:16

File Type:pdf, Size:1020Kb

Design and Development of an External Fast Neutron Beam Facility at the Ohio State University Research Reactor Design and Development of an External Fast Neutron Beam Facility at the Ohio State University Research Reactor Thesis By Andrew M. Zapp Graduate Program in Nuclear Engineering The Ohio State University 2019 Master‟s Examination Committee: Dr. Vaibhav Sinha, Advisor Dr. Lei Cao Copyright by Andrew M. Zapp 2019 Abstract The ability of the Ohio State University Research Reactor, OSURR, to conduct experiments from the generation of the neutron flux is important in conducting research by the University and external entities that require a flux of this magnitude. In particular, research involving a fast neutron flux is of interest due to the different interactions fast neutrons have as opposed to thermal neutrons. The OSURR is able to operate up to 500 kW, which creates a neutron flux in the order of 1013 n/cm2-s. Currently, Beam Port 2 provides a thermal neutron beam profile of 30 mm in diameter for experimentation such as neutron depth profiling, activation analysis, and evaluation of radiation damage to electronics. Beam Port 1 uses a sample area located adjacent and perpendicular to the fuel plates of the reactor for in-core irradiation. During experimentation, the remainder of Beam Port 1 must be plugged with removable concrete shielding to prevent radiation exposure that can be upwards of 1x104 rem/hr. The upgrade to Beam Port 1 consists of a collimator to shape the neutron flux from the reactor into a beam of fast neutrons, similar in diameter to Beam Port 2, in order to irradiate samples external to the reactor. In addition, mobile external shielding is designed to prevent exceeding the exposure limits of 5 rem/yr when the facility is in use. With this upgrade the research reactor has the ability to conduct simultaneous experiments with a fast and thermal neutron beam, external to the biological shielding, without releasing any harmful exposure. i Acknowledgements I would first like to thank my Nuclear Engineering graduate advisor, Dr. Vaibhav Sinha, for his help throughout this process. I would also like to thank the efforts conducted by my fellow graduate students Ibrahim Oksuz and Matthew Van Zile, who are in the Ohio State University Nuclear Engineering program, under the supervision of Dr. Lei Cao. This would not be possible without the substantial support and guidance from the staff at the Ohio State University Nuclear Reactor Laboratory. In particular, Mr. Andrew Kauffman, the Associate Director, and Mr. Joel Hatch, the Research Engineer, provided a significant amount of their time and effort in collaboration of this design. This work is supported by The Ohio State University and the Department of Energy through NEUP General Scientific Infrastructure Support Program for grant no. RU-17-13347, “A Request for Upgrade of the Ohio State University Research Reactor Beam Ports Infrastructure”. ii Vita 2005 B.A. International Studies, Russian Minor, Miami University (OH) 2008 Naval Nuclear Training Command Graduate 2007-2015 Nuclear trained Machinist Mate, USS Seawolf 2018 Presentation at SORMA XVII, “Design and Development of an External Fast Neutron Beam Facility at the Ohio State University Research Reactor”, University of Michigan Fields of Study Major Field: Nuclear Engineering iii Table of Contents Abstract i Acknowledgements ii Vita iii Fields of Study iii List of Figures vii List of Tables x 1 Introduction 1 2 Theory 4 2.1 Reactor/Source 4 2.1.1 Neutron Interactions/Properties 6 2.1.2 Gamma Interactions/Properties 8 2.2 Shielding 9 2.2.1 Neutron Shielding 9 2.2.2 Gamma Shielding 10 2.3 Collimation 12 2.3.1 Illuminator 16 2.3.2 Beam Filter 17 2.3.3 Aperture 19 3 Materials 20 3.1 Collimator Materials 20 3.1.1 Graphite Illuminator 20 3.1.2 Bismuth and Sapphire Filters 25 3.1.3 Aperture Pieces 34 3.1.3.1 Borated Cement 36 3.1.3.2 Metamic® (Borated Aluminum) 38 3.1.3.3 Lead 40 3.1.4 Aluminum 6061 as Structural Material 42 3.2 Beam Stop Shielding Materials 45 iv 3.2.1 Borated Polyethylene 45 3.2.2 Metamic® 46 3.2.3 Lead 47 4 Design 49 4.1 Existing Structure 51 4.1.1 Beam Port 2 Facility 51 4.1.2 Beam Port 1 Current Lay-out 53 4.2 MCNP Simulations 60 4.2.1 Collimator MCNP Simulations 61 4.2.2 Beam Stop MCNP Simulations 62 4.3 Design Calculations 63 4.3.1 Collimator Calculations 63 4.3.2 Shielding Calculations 67 4.3.2.1 Fast Neutrons 67 4.3.2.2 Gammas 70 4.4 Collimator Final Designs 70 4.4.1 Design Process 70 4.4.2 Beam Port 1 72 4.4.2.1 Inner Collimator 72 4.4.2.2 Outer Collimator 74 4.4.3 Beam Port 2 75 4.4.3.1 Inner Collimator 75 4.4.4 Aluminum Structural Considerations 77 4.5 External Shielding Design 80 4.5.1 Beam Stop 81 4.5.2 Rail/Lift System 84 4.5.2.1 PBC Linear Components 85 4.5.2.2 Joyce-Dayton Components 87 4.5.2.3 Fabricated Components 90 4.6 Future Work 91 5 Conclusions 93 v References 95 Appendix A: Drawings Index 99 Appendix B: MATLAB Code for Table 4-6 103 Appendix C: MCNP Code for Figure 4-9 104 Appendix D: Additional Weight and Cost Estimates 110 vi List of Figures Figure 2-1: Elastic neutron scattering collision 6 Figure 2-2: Different gamma interactions with respect to the materials Z number and gamma energy (Knoll 2010) 9 Figure 2-3: Attenuation coefficients based on energy for NaI (Knoll 2010) 12 Figure 2-4: General image plane for a source showing the image plane and distance (ASTM E803 1996) 14 Figure 2-5: Final Collimator design for the Beam Port 2 upgrade in 2012 (Turkoglu 2012) 15 Figure 2-6: Neutron Cross Sections for Carbon (Lamarsh 2001) 17 Figure 3-1: Graphite, Beam Port 1 23 Figure 3-2: Graphite, Beam Port 2 24 Figure 3-3: 3-D image of Graphite with aluminum case for Beam Port 2 25 Figure 3-4: Three single-crystal Sapphires (left) used in the 2012 upgrade to Beam Port 2 (Turklogu 2012) 26 Figure 3-5: Gamma attenuation for different thicknesses of Bismuth 27 Figure 3-6: Bismuth total cross-section for 1 - 600 meV neutron energy ranges (Freund 1983) 28 Figure 3-7: Bismuth total cross-section for 10-3 - 10 eV neutron energy ranges (Adib 2003) 29 Figure 3-8: Total neutron cross section for 209Bi, from .0125 eV – 5 MeV (NNDC) 30 Figure 3-9: Poly-crystal Bismuth molded into an aluminum holder (Turklogu 2012) 31 Figure 3-10: 3-D image of new Sapphire holder 32 Figure 3-11: Bismuth encased in Aluminum shell 33 3 6 10 Figure 3-12: σabs of He, Li, and B for a large range of neutron energies (Knoll 2010) 35 Figure 3-13: Borated Cement piece for Inner Collimator 38 Figure 3-14: Metamic® Apertures 40 Figure 3-15: Attenuation coefficients for Lead (Lamarsh 2001) 41 vii Figure 3-16: Lead Apertures 41 Figure 3-17: Stress-Strain Curves (Oberg 2012) 42 Figure 3-18: Example of Borated Polyethylene sheet drawing 46 Figure 3-19: Example of Metamic® sheet drawing 47 Figure 3-20: 3-D model of lead sheet 48 Figure 4-1: Rear View of Beam Port 2 (OSURR n.d.) 52 Figure 4-2: Overhead view of Beam Port 2 (OSURR n.d.) 53 Figure 4-3: Beam Port 1 at exit of the port (OSURR n.d.) 54 Figure 4-4: 3-D overhead view of Beam Ports inside the OSURR 55 Figure 4-5: 3-D view of Beam Ports inside the OSURR 56 Figure 4-6: 3-D cut-out of the Shutter Box Assembly in the “Open” (left) and “Shut” (right) position 57 Figure 4-7: Removal of the Shutter Box Assembly (OSURR n.d.) 57 Figure 4-8: Shutter Box Assembly when removed for maintenance (OSURR n.d.) 58 Figure 4-9: MCNP model of the collimator 60 Figure 4-10: Neutron transmittance through 4” of Bismuth from neutron energies of .0125 eV – 10 MeV 64 Figure 4-11: Neutron transmittance showing the energy range corresponding to 1/v cross section range (.0125 eV – 1 keV) 65 Figure 4-12: Final neutron flux through Bismuth 66 Figure 4-13: Collimated fast neutron flux 66 Figure 4-14: Example of drawing assembly 71 Figure 4-15: Example of individual drawing used for above assembly 72 Figure 4-16: Inner Collimator, Beam Port 1 73 Figure 4-17: Inner Collimator Aluminum Shell, Beam Port 1 73 Figure 4-18: Outer Collimator 74 Figure 4-19: Inner Collimator Aluminum Shell 75 Figure 4-20: Inner Collimator, Beam Port 2 76 Figure 4-21: Inner Collimator Aluminum Shell, Beam Port 2 76 Figure 4-22: Shield plug handling tool end (OSURR n.d.) 77 Figure 4-23: 3-D model of Aluminum shell cap design for removing the collimator 78 viii Figure 4-24: Stress and beam load case for Aluminum shell extending into the reactor pool (Oberg 2012) 79 Figure 4-25: 3-D Model of Beam Stop 82 Figure 4-26: 3-D model of Beam Stop cut-out showing Lead inserted in the back 83 Figure 4-27: Double roller pillow block data from PBC Linear (PBC Linear n.d.) 85 Figure 4-28: 3-D model of PBC linear components with bottom frame 86 Figure 4-29: 3-D model showing the removable section of railing 86 Figure 4-30: Beam Port 2 (Left) Beam Shutter without Lead components, (Right) 3-D model of Beam Shutter with Lead components (Turklogu 2012) 87 Figure 4-31: Typical machine screw jack with a lifting screw (Joyce/Dayton n.d.) 88 Figure 4-32: Machine screw jack with a traveling nut (Joyce/Dayton n.d.) 89 Figure 4-33: 3-D model of Joyce-Dayton Components 90 Figure 4-34: 3-D model of bottom frame (left) and middle frame (right) 91 Figure 4-35: 3-D Model of all components 91 ix List of Tables Table 2-1: OSURR Neutron flux data at different areas of the core (OSURR n.d.) 4 Table 2-2: Energy loss values for Hydrogen and Carbon 7 Table 3-1: Carbon nuclide data (NNDC n.d.) 21 Table 3-2: Comparison of the three filter materials and associated densities and cross sections 30 Table 3-3: Bismuth nuclide data (NNDC n.d.) 31 Table 3-4: Boron nuclide data (NNDC n.d.) 34 Table 3-5: Composition data of Borated Cement vs.
Recommended publications
  • Doe Nuclear Physics Reactor Theory Handbook
    DOE-HDBK-1019/2-93 JANUARY 1993 DOE FUNDAMENTALS HANDBOOK NUCLEAR PHYSICS AND REACTOR THEORY Volume 2 of 2 U.S. Department of Energy FSC-6910 Washington, D.C. 20585 Distribution Statement A. Approved for public release; distribution is unlimited. This document has been reproduced directly from the best available copy. Available to DOE and DOE contractors from the Office of Scientific and Technical Information, P.O. Box 62, Oak Ridge, TN 37831. Available to the public from the National Technical Information Service, U.S. Department of Commerce, 5285 Port Royal., Springfield, VA 22161. Order No. DE93012223 DOE-HDBK-1019/1-93 NUCLEAR PHYSICS AND REACTOR THEORY ABSTRACT The Nuclear Physics and Reactor Theory Handbook was developed to assist nuclear facility operating contractors in providing operators, maintenance personnel, and the technical staff with the necessary fundamentals training to ensure a basic understanding of nuclear physics and reactor theory. The handbook includes information on atomic and nuclear physics; neutron characteristics; reactor theory and nuclear parameters; and the theory of reactor operation. This information will provide personnel with a foundation for understanding the scientific principles that are associated with various DOE nuclear facility operations and maintenance. Key Words: Training Material, Atomic Physics, The Chart of the Nuclides, Radioactivity, Radioactive Decay, Neutron Interaction, Fission, Reactor Theory, Neutron Characteristics, Neutron Life Cycle, Reactor Kinetics Rev. 0 NP DOE-HDBK-1019/1-93 NUCLEAR PHYSICS AND REACTOR THEORY FOREWORD The Department of Energy (DOE) Fundamentals Handbooks consist of ten academic subjects, which include Mathematics; Classical Physics; Thermodynamics, Heat Transfer, and Fluid Flow; Instrumentation and Control; Electrical Science; Material Science; Mechanical Science; Chemistry; Engineering Symbology, Prints, and Drawings; and Nuclear Physics and Reactor Theory.
    [Show full text]
  • Nuclear Waste Transmutation in Subcritical Reactors Driven by Target-Distributed Accelerators
    Nuclear Waste Transmutation in Subcritical Reactors Driven by Target-Distributed Accelerators Anatoly Blanovsky Teacher Technology Center, 7850 Melrose Ave., Los Angeles, CA 90046, USA E-mail [email protected] Abstract-A radioactive waste transmutation system based extensively on existing nuclear power technology is presented. By replacing the control rods with neutron generators, we could maintain good power distribution and perform long-lived waste burning in high flux subcritical reactors (HFSR). To increase neutron source intensity the HFSR is divided into two zones: a booster and a blanket. A neutron gate (absorber and moderator) imposed between two zones permits fast neutrons from the booster to flow to the blanket. Neutrons moving in the reverse direction are moderated and absorbed. The design is based on a small pressurized water reactor (PWR), fission electric cell (FEC), target-distributed accelerator (TDA) and power monitoring system with in-core gamma-ray detectors, now under development in several countries. The FEC is essentially a high-voltage power source that directly converts the kinetic energy of the fission fragments into electrical potential of about 2MV. The TDA, in which an FEC electric field compensates for lost beam energy in the target, offers a new approach to obtain large neutron fluxes. INTRODUCTION I. HFSR CONCEPT In the conventional reactor, nuclear energy With self-amplifying due to feedback, (electrical in nature) is converted to thermal, then to blanket and booster multiplication factors of k=0.95 mechanical and then to electrical energy. To achieve and 0.98, respectively, an external neutron source the high degree of the burn-up, only fresh low rate of at least 10.sup.15 n/s is needed to drive the enriched uranium fuel is used.
    [Show full text]
  • Nureg/Cr-6760 Ornl/Tm-2000-321
    NUREG/CR- 6760 ORNL/TM-2000-321 Study of the Effect of Integral Burnable Absorbers for PWR Burnup Credit Oak Ridge National Laboratory U.S. Nuclear Regulatory Commission Office of Nuclear Regulatory Research Washington, DC 20555-0001 AVAILABILITY OF REFERENCE MATERIALS IN NRC PUBLICATIONS NRC Reference Material Non-NRC Reference Material technical As of November 1999, you may electronically access Documents available from public and special NUREG-series publications and other NRC records at libraries include all open literature items, such as NRC's Public Electronic Reading Room at books, journal articles, and transactions, Federal www.nrc.gov/NRC/ADAMS/index.html. Register notices, Federal and State legislation, and Publicly released records include, to name a few, congressional reports. Such documents as theses, NUREG-series publications; FederalRegister notices; dissertations, foreign reports and translations, and applicant, licensee, and vendor documents and non-NRC conference proceedings may be purchased organization. correspondence; NRC correspondence and internal from their sponsoring memoranda; bulletins and information notices; inspection and investigative reports; licensee event Copies of industry codes and standards used in a reports, and Commission papers and their substantive manner in the NRC regulatory process are attachments. maintained at The NRC Technical Library NRC publications in the NUREG series, NRC Two White Flint North regulations, and Title 10, Energy, in the Code of 11545 Rockville Pike Federal Regulations may also be purchased from one Rockville, MD 20852-2738 of these two sources. 1. The Superintendent of Documents These standards are available in the library for are U.S. Government Printing Office reference use by the public.
    [Show full text]
  • Load Following with a Passive Reactor Core Using the SPARC Design
    UPTEC ES 16 023 Examensarbete 30 hp 13 Juni 2016 Load following with a passive reactor core using the SPARC design Sebastian Leo Eile Svanström Abstract Load following with a passive reactor core using the SPARC design Sebastian Leo Eile Svanström Teknisk- naturvetenskaplig fakultet UTH-enheten This thesis is a follow up on "SPARC fast reactor design: Design of two passively metal-fuelled sodium-cooled pool-type small modular fast reactors with Autonomous Besöksadress: Reactivity Control" by Tobias Lindström (2015). In this thesis the two reactors Ångströmlaboratoriet Lägerhyddsvägen 1 designed by Lindström in said thesis were evaluated. The goal was to determine the Hus 4, Plan 0 reactors ability to load follow as well as the burnup of the neutron absorber used in the passive control system. Postadress: Box 536 751 21 Uppsala To be able to determine the dynamic behaviour of the reactors the reactivity feedbacks of the cores were modelled using Serpent, a Monte Carlo simulation Telefon: software for 3D neutron transport calculations. These feedbacks were then 018 – 471 30 03 implemented into a dynamic simulation of the core, primary and secondary circulation Telefax: and steam generator. The secondary circulation and feedwater flow were used to 018 – 471 30 00 regulate steam temperature and turbine power. The core was left at constant coolant flow and no control rods were used. Hemsida: http://www.teknat.uu.se/student The simulations showed that the reactor was able to load follow between 100 % and 40 % of rated power at a speed of 6 % per minute. It was also shown that the reactor could safely adjust its power between 100 % and 10 % of rated power suggesting that load following is possible below 40 % of rated power but at a lower speed.
    [Show full text]
  • Concept of an Accelerator-Driven Advanced Nuclear Energy System
    Article Concept of an Accelerator-Driven Advanced Nuclear Energy System Xuesong Yan, Lei Yang *, Xunchao Zhang and Wenlong Zhan Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China; [email protected] (X.Y.); [email protected] (X.Z.); [email protected] (W.Z.) * Correspondence: [email protected]; Tel.: +86-931-4969-187 Academic Editor: Hiroshi Sekimoto Received: 24 March 2017; Accepted: 10 May 2017; Published: 7 July 2017 Abstract: The utilization of clean energy is a matter of primary importance for sustainable development as well as a vital approach for solving worldwide energy-related issues. If the low utilization rate of nuclear fuel, nuclear proliferation, and insufficient nuclear safety can be solved, nuclear fission energy could be used as a sustainable and low-carbon clean energy form for thousands of years, providing steady and base-load electrical resources. To address these challenges, we propose an accelerator-driven advanced nuclear energy system (ADANES), consisting of a burner system and a fuel recycle system. In ADANES, the ideal utilization rate of nuclear fuel will be >95%, and the final disposal of nuclear waste will be minimized. The design of a high-temperature ceramic reactor makes the burner system safer. Part of fission products (FPs) are removed during the simple reprocessing in the fuel recycle system, significantly reducing the risks of nuclear proliferation of nuclear technology and materials. The ADANES concept integrates nuclear waste transmutation, nuclear fuel breeding, and safety power production, with an ideal closed loop operation of nuclear fission energy, constituting a major innovation of great potential interest for future energy applications.
    [Show full text]
  • Fuel Burnup Analysis of the TRIGA Mark II Reactor at the University of Pavia
    Fuel burnup analysis of the TRIGA Mark II Reactor at the University of Pavia Davide Chiesaa,b, Massimiliano Clemenzaa,b, Stefano Pozzia,b, Ezio Previtalia,b, Monica Sistia,b, Daniele Allonic,d, Giovanni Magrottic,d, Sergio Manerac,d, Michele Pratac,d, Andrea Salvinic,d, Antonio Cammie,b, Matteo Zanettie, Alberto Sartorif aPhysics Department \G. Occhialini" of Milano-Bicocca University, piazza della Scienza 3, 20126 Italy bINFN section of Milano-Bicocca, piazza della Scienza 3, 20126 Italy cLaboratorio Energia Nucleare Applicata (L.E.N.A.) of the University of Pavia, via Aselli 41, Pavia 27100, Italy dINFN section of Pavia, via A. Bassi 6, Pavia 27100, Italy ePolitecnico di Milano, Department of Energy, CeSNEF (Enrico Fermi Center for Nuclear Studies), via La Masa 34, 20156 Milano, Italy fSISSA mathLab, International School for Advanced Studies, Via Bonomea 265, 34136 Trieste, Italy Abstract A time evolution model was developed to study fuel burnup for the TRIGA Mark II reactor at the University of Pavia. The results were used to predict the effects of a complete core reconfiguration and the accuracy of this pre- diction was tested experimentally. We used the Monte Carlo code MCNP5 to reproduce system neutronics in different operating conditions and to anal- yse neutron fluxes in the reactor core. The software that took care of time evolution, completely designed in-house, used the neutron fluxes obtained by MCNP5 to evaluate fuel consumption. This software was developed specif- ically to keep into account some features that differentiate experimental re- actors from power ones, such as the daily on/off cycle and the long fuel lifetime.
    [Show full text]
  • A Fission-Fusion Hybrid Reactor in Steady-State L-Mode Tokamak Configuration with Natural Uranium
    PSFC/RR-11-1 A Fission-Fusion Hybrid Reactor in Steady-State L-Mode Tokamak Configuration with Natural Uranium Reed, M., Parker, R., Forget, B.* *MIT Department of Nuclear Science & Engineering January 2011 Plasma Science and Fusion Center Massachusetts Institute of Technology Cambridge MA 02139 USA A Fission-Fusion Hybrid Reactor in Steady-State L-mode Tokamak Configuration with Natural Uranium Mark Reed, Ronald R. Parker, Benoit Forget Massachusetts Institute of Technology January 2011 Abstract The most prevalent criticism of fission-fusion hybrids is simply that they are too exotic - that they would exacerbate the challenges of both fission and fusion. This is not really true. Intriguingly, hybrids could actually be more viable than stand-alone fusion reactors while mitigating many challenges of fission. This work develops a conceptual design for a fission-fusion hybrid reactor in steady-state L-mode tokamak configuration with a subcritical natural or depleted uranium pebble bed blanket. A liquid lithium- lead alloy breeds enough tritium to replenish that consumed by the D-T fusion reaction. Subcritical operation could obviate the most challenging fuel cycle aspects of fission. The fission blanket augments the fusion power such that the fusion core itself need not have a high power gain, thus allowing for fully non-inductive (steady-state) low confinement mode (L-mode) operation at relatively small physical dimensions. A neutron transport Monte Carlo code models the natural uranium fission blanket. Maximizing the fission power while breeding sufficient tritium allows for the selection of an optimal set of blanket parameters, which yields a maximum prudent fission power gain of 7.7.
    [Show full text]
  • Part Twenty-Nine Reactor Operation with Feedback Effects
    22.05 Reactor Physics - Part Twenty-Nine Reactor Operation with Feedback Effects 1. Reference Material: See pp. 368 – 372 in “Light Water Reactor Control Systems,” in Wiley Encyclopedia of Electrical and Electronics Engineering. 2. Point of Adding Heat – Hot Operating Crucial concepts are: Types of power-dependent feedback — Coolant Temperature — Fuel Temperature (Doppler Effect) — Void Coefficient — Xenon/Samarium Time scales of each feedback mechanism Estimated Critical Position 3. Coolant Temperature As the temperature of the primary coolant increases, it becomes less dense. This causes: — Less neutron moderation — Increased neutron leakage Hence, as coolant temperature rises, negative reactivity is generated. This makes reactors self-regulating. Time scale is primary loop circuit time ~ 30 s. Negative temperature coefficients are required for all U.S., European, and Asian reactors. They provide a safety feature. But, under certain accidents they make the situation worse: — Steam line break — Control rod drop In both of these cases, the reactor cools off and the negative coefficient causes a positive reactivity insertion. 1 4. Void Coefficient The primary coolant in both PWRs and BWRs performs several functions. These are: — Removal of heat. — Moderation of neutrons so as to continue the neutron chain reaction. — Shielding during maintenance. If the coolant becomes less dense, it becomes less efficient as a moderator. One way to decrease coolant density is to decrease its temperature. Another is to create voids in it. This occurs in BWRs when steam bubbles form. BWRs can be controlled by adjusting the recirculation flow which in turn controls the rate at which voids are swept out of the core.
    [Show full text]
  • On Minor Actinide Transmutation in Hard Neutron Spectra
    Why Faster is Better - On Minor Actinide Transmutation in Hard Neutron Spectra DANIEL WESTLÉN Doctoral Thesis Stockholm, Sweden 2007 TRITA-FYS KTH ISSN 0280-316X School of Engineering Sciences ISRN KTH/FYS/--07:05--SE SE-106 91 Stockholm ISBN 978-91-7178-567-1 SWEDEN Akademisk avhandling som med tillstånd av Kungl Tekniska högskolan framlägges till offentlig granskning för avläggande av teknologie doktorsexamen i fysik fredagen den 2007-02-23 klockan 14.15 i hörsal F3, Lindstedtsvägen 26. © Daniel Westlén, January 2007 Tryck: Universitetsservice US AB ii Abstract In this thesis, options for efficient transmutation of transuranium elements are discussed. The focus is on plutonium, americium and curium mainly because of their long-term contribution to the radiotoxicity of spent nuclear fuel. Two innovative helium-cooled core designs are proposed, dedicated to the transmutation of actinides. The performance of the more promising of the two is studied in realistic transient fuel cycle scenarios. During the 1150 day irradiation cycle, a minor actinide consumption of 355 kg/GWth·year is achieved. An analysis of the efficiency of spallation neutron sources in helium-cooled cores is also performed. It is shown that the proton source efficiency, ψ∗, is improved by about 10% when helium is used as coolant, rather than lead-bismuth eutectic. Further, a proposal is made to transmute actinides in the upper part of a BWR core. A net consumption of transuranics is shown possible in the BWR park already when 50% of the BWR fuel is of the proposed evolutionary type. The thesis concludes that efficient transmutation of transuranic elements in dedicated helium-cooled subcritical cores is possible.
    [Show full text]
  • Plutonium Fuel in Thermal Reactors; And
    NUCLEAR ENERGY AGENCY AN ASSESSMENT NUCLEAR ENERGY AGENCY PLUTONIUM RIB AN ASSESSMENT REPORT BY AN EXPERT GROUP ORGANISATION FOR ECONOMIC CO-OPERATION AND DEVELOPMENT Pursuant to article 1 of the Convention signed in Paris on 14th December 1960, and which came into force on 30th September 1961, the Organisation for Economic Co-operation and Development (OECD) shall promote policies designed: - to achieve the highest sustainable economic growth and employment and a rising standard of living in Member countries, while maintaining financial stability, and thus to contribute to the development of the world economy; - to contribute to sound economic expansion in Member as well as non-member countries in the process of economic development; and - to contribute to the expansion of world trade on a multilateral, non-discriminatory basis in accordance with international obligations. The original Member countries of the OECD are Austria, Belgium, Canada, Denmark, France, the Federal Republic of Germany, Greece, Iceland, Ireland, Italy, Luxembourg, the Netherlands, Norway, Portugal, Spain, Sweden, Switzerland, Turkey, the United Kingdom and the United States. The following countries became Members subsequently through accession at the dates indicated hereafter: Japan (28th April 1964), Finland (28th January 1969), Australia (7th June 1971) and New Zealand (29th May 1973). The Socialist Federal Republic of Yugoslavia takes part in some of the work of the OECD (agreement of 28th October 1961). The OECD Nuclear Energy Agency (NEA) was established on 1st February 1958 under the name of the OEEC European Nuclear Energy Agency. It received its present designation on 20th April 1972, when Japan became its first non-European full Member.
    [Show full text]
  • TRANSMUTATION of AMERICIUM and CURIUM in a LANTHANIDE MATRIX COMPANY WIDE CW-123700-CONF-018 Revision 0
    Conference Paper TRANSMUTATION OF AMERICIUM AND CURIUM IN A LANTHANIDE MATRIX COMPANY WIDE CW-123700-CONF-018 Revision 0 Prepared by Rédigé par Hyland Bronwyn Reviewed by Vérifié par Edwards Geoffrey W R Approved by Approuvé par Hyland Bronwyn 2012/07/04 2012/07/04 UNRESTRICTED ILLIMITÉ Atomic Energy of Énergie Atomique du Canada Limited Canada Limitée Chalk River, Ontario Chalk River (Ontario) Canada K0J 1J0 Canada K0J 1J0 Proceedings of Global 2011 Nagoya, Japan, December 11-15, 2011 UNRESTRICTED CW-123700-CONF-018 Transmutation of Americium and Curium in a Lanthanide Matrix B. HYLAND1, E.D COLLINS2, R. J. ELLIS2, G. DEL CUL2 and M. MAGILL1 1Chalk River Laboratories, Atomic Energy of Canada Limited, Canada, K0J 1J0 Tel: +1(613)584-9243 ex. 44707 , Fax: +1(613)584-8198 , Email: [email protected] 2Oak Ridge National Laboratory (ORNL), Oak Ridge, Tennessee, U.S.A. Abstract – With world stockpiles of used nuclear fuel increasing, the long-term remediation of used fuel is a growing concern. Many of the transuranic (TRU) actinides in nuclear spent fuel produce decay heat for long durations, resulting in significant nuclear waste management challenges. Partitioning and transmutation of the spent fuel is one possibility to deal with the long-lived transuranic actinides. It is desirable to develop a partitioning and transmutation scheme that is as straightforward as possible for both the reprocessing step and the transmutation in reactor. This study looks at a reprocessing scheme that is simplified to keep the americium, curium and lanthanides together in one recycle stream. These actinides can be transmuted to fissionable isotopes and then to shorter-lived fission products in a CANDU reactor.
    [Show full text]
  • DOE Fundamentals Handbook Nuclear
    Department of Energy Fundamentals Handbook NUCLEAR PHYSICS AND REACTOR THEORY Module 3 Reactor Theory (Nuclear Parameters) Reactor Theory (Nuclear Parameters) DOE-HDBK-1019/2-93 TABLE OF CONTENTS TABLE OF CONTENTS LIST OF FIGURES ................................................ iii LIST OF TABLES ................................................. iv REFERENCES ................................................... v OBJECTIVES .................................................... vi NEUTRON LIFE CYCLE ............................................ 1 Infinite Multiplication Factor, k∞ .................................... 2 Four Factor Formula ........................................... 2 Fast Fission Factor, ( ) ......................................... 3 Resonance Escape Probability, (p) ................................. 3 Thermal Utilization Factor, (f) .................................... 4 Reproduction Factor, (η) ........................................ 6 Effective Multiplication Factor .................................... 8 Fast Non-Leakage Probability ( f) ................................. 9 Thermal Non-Leakage Probability ( t)............................... 9 Six Factor Formula ........................................... 10 Neutron Life Cycle of a Fast Reactor .............................. 14 Summary ................................................. 14 REACTIVITY ................................................... 17 Application of the Effective Multiplication Factor ...................... 17 Reactivity ................................................
    [Show full text]