ARTFUL DODGERS at PEACH BOTTOM in January 2010, Workers
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Study of Advanced Lwr Cores for Effective Use of Plutonium and Mox Physics Experiments
STUDY OF ADVANCED LWR CORES FOR EFFECTIVE USE OF PLUTONIUM AND MOX PHYSICS EXPERIMENTS T. YAMAMOTO, H. MATSU-URA*, M. UEJI, H. OTA XA9953266 Nuclear Power Engineering Corporation, Toranomon, Minato-ku, Tokyo T. KANAGAWA Mitsubishi Heavy Industries, Ltd, Nishi-ku, Yokohama K. SAKURADA Toshiba Corporation, Isogo-ku, Yokohama H.MARUYAMA Hitachi, Ltd, Hitachi-shi Japan Abstract Advanced technologies of full MOX cores have been studied to obtain higher Pu consumption based on the advanced light water reactors (APWRs and ABWRs). For this aim, basic core designs of high moderation lattice (H/HM ~5) have been studied with reduced fuel diameters in fuel assemblies for APWRs and those of high moderation lattice (H/HM ~6) with addition of extra water rods in fuel assemblies for ABWRs. The analysis of equilibrium cores shows that nuclear and thermal hydraulic parameters satisfy the design criteria and the Pu consumption rate increases about 20 %. An experimental program has been carried out to obtain the core parameters of high moderation MOX cores in the EOLE critical facility at the Cadarache Centre as a joint study of NUPEC, CEA and CEA's industrial partners. The experiments include a uranium homogeneous core, two MOX homogeneous cores of different moderation and a PWR assembly mock up core of MOX fuel with high moderation. The program was started from 1996 and will be completed in 2000. 1. INTRODUCTION In Japan, the MOX fuel demonstration programs have been performed successfully and reload size use of MOX fuel has been prepared. The recycling of plutonium in light water reactors is expected to continue in several decades. -
1 Phys:1200 Lecture 36 — Atomic and Nuclear Physics
1 PHYS:1200 LECTURE 36 — ATOMIC AND NUCLEAR PHYSICS (4) This last lecture of the course will focus on nuclear energy. There is an enormous reservoir of energy in the nucleus and it can be released either in a controlled manner in a nuclear reactor, or in an uncontrolled manner in a nuclear bomb. The energy released in a nuclear reactor can be used to produce electricity. The two processes in which nuclear energy is released – nuclear fission and nuclear fusion, will be discussed in this lecture. The biological effects of nuclear radiation will also be discussed. 36‐1. Biological Effects of Nuclear Radiation.—Radioactive nuclei emit alpha, beta, and gamma radiation. These radiations are harmful to humans because they are ionizing radiation that have the ability to remove electrons from atoms and molecules in human cells. This can lead to the death or alterations of cells. Alteration of the cell can transform a healthy cell into a cancer cell. The hazards of radiation can be minimized by limiting ones overall exposure to radiation. However, there is still some uncertainty in the medical community about the possibility the effect of a single radioactive particle on the bottom. In other words, are the effects cumulative, or can a single exposure lead to cancer in the body. Exposure to radiation can produce either short term effects appearing within minutes of exposure, or long term effects that may appear in years or decades or even in future generations due to changes in DNA. The effects of absorbing ionizing radiation is measured in a unit called the rem. -
Enrico Fermi
Fermi, Enrico Inventors and Inventions Enrico Fermi Italian American physicist Fermi helped develop Fermi-Dirac statistics, which liceo (secondary school) and, on the advice of Amidei, elucidate the group behavior of elementary particles. joined the Scuola Normale Superiore at Pisa. This elite He also developed the theory of beta decay and college, attached to the University of Pisa, admitted only discovered neutron-induced artificial radioactivity. forty of Italy’s top students, who were given free board Finally, he succeeded in producing the first sustained and lodging. Fermi performed exceedingly well in the nuclear chain reaction, which led to the discovery highly competitive entrance exam. He completed his of nuclear energy and the development of the university education after only four years of research and atomic bomb. studies, receiving his Ph.D. in physics from the Univer- sity of Pisa and his undergraduate diploma from the Born: September 29, 1901; Rome, Italy Scuola Normale Superiore in July, 1922. He became Died: November 28, 1954; Chicago, Illinois an expert theoretical physicist and a talented exper- Primary field: Physics imentalist. This rare combination provided a solid foun- Primary inventions: Controlled nuclear chain dation for all his subsequent inventions. reaction; Fermi-Dirac statistics; theory of beta decay Life’s Work After postdoctoral work at the University of Göttingen, Early Life in Germany (1922-1923), and the University of Leiden, Enrico Fermi (ehn-REE-koh FUR-mee) was the third in the Netherlands (fall, 1924), Fermi took an interim po- child of Alberto Fermi and Ida de Gattis. Enrico was very sition at the University of Florence in December, 1924. -
Nuclear Weapons Technology 101 for Policy Wonks Bruce T
NUCLEAR WEAPONS TECHNOLOGY FOR POLICY WONKS NUCLEAR WEAPONS TECHNOLOGY 101 FOR POLICY WONKS BRUCE T. GOODWIN BRUCE T. GOODWIN BRUCE T. Center for Global Security Research Lawrence Livermore National Laboratory August 2021 NUCLEAR WEAPONS TECHNOLOGY 101 FOR POLICY WONKS BRUCE T. GOODWIN Center for Global Security Research Lawrence Livermore National Laboratory August 2021 NUCLEAR WEAPONS TECHNOLOGY 101 FOR POLICY WONKS | 1 This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory in part under Contract W-7405-Eng-48 and in part under Contract DE-AC52-07NA27344. The views and opinions of the author expressed herein do not necessarily state or reflect those of the United States government or Lawrence Livermore National Security, LLC. ISBN-978-1-952565-11-3 LCCN-2021907474 LLNL-MI-823628 TID-61681 2 | BRUCE T. GOODWIN Table of Contents About the Author. 2 Introduction . .3 The Revolution in Physics That Led to the Bomb . 4 The Nuclear Arms Race Begins. 6 Fission and Fusion are "Natural" Processes . 7 The Basics of the Operation of Nuclear Explosives. 8 The Atom . .9 Isotopes . .9 Half-life . 10 Fission . 10 Chain Reaction . 11 Critical Mass . 11 Fusion . 14 Types of Nuclear Weapons . 16 Finally, How Nuclear Weapons Work . 19 Fission Explosives . 19 Fusion Explosives . 22 Staged Thermonuclear Explosives: the H-bomb . 23 The Modern, Miniature Hydrogen Bomb . 25 Intrinsically Safe Nuclear Weapons . 32 Underground Testing . 35 The End of Nuclear Testing and the Advent of Science-Based Stockpile Stewardship . 39 Stockpile Stewardship Today . 41 Appendix 1: The Nuclear Weapons Complex . -
Detailed B Depletion in Control Rods Operating in a Nuclear Boiling
UPTEC K11 015 Examensarbete 30 hp Februari 2011 Detailed 10B depletion in control rods operating in a Nuclear Boiling Water Reactor John Johnsson Abstract Detailed 10B depletion in control rods operating in a Nuclear Boiling Water Reactor John Johnsson Teknisk- naturvetenskaplig fakultet UTH-enheten In a nuclear power plant, control rods play a central role to control the reactivity of the core. In an inspection campaign of three control rods (CR 99) operated in the Besöksadress: KKL reactor in Leibstadt, Switzerland, during 6 respectively 7 consecutive cycles, Ångströmlaboratoriet Lägerhyddsvägen 1 defects were detected in the top part of the control rods due to swelling caused by 10 Hus 4, Plan 0 depletion of the neutron-absorbing B isotope (Boron-10). In order to correlate these defects to control rod depletion, the 10B depletion has in this study been Postadress: calculated in detail for the absorber pins in the top node of the control rods. Box 536 751 21 Uppsala Today the core simulator PLOCA7 is used for predicting the behavior of the reactor Telefon: core, where the retrievable information from the standard control rod follow-up is 018 – 471 30 03 the average 10B depletion for clusters of 19 absorber holes i.e. one axial node. 10 Telefax: However, the local B depletion in an absorber pin may be significantly different 018 – 471 30 00 from the node average depletion that is re-ceived from POLCA7. To learn more, the 10B depletion has been simulated for each absorber hole in the uppermost node using Hemsida: the stochastic Monte Carlo 3D simulation code MCNP as well as an MCNP- based http://www.teknat.uu.se/student 2D-depletion code (McScram). -
22.05 Reactor Physics – Part One Course Introduction
22.05 Reactor Physics – Part One Course Introduction 1. Instructor: John A. Bernard 2. Organization: Homework (20%) Four Exams (20% each; lowest grade is dropped) Final Exam (3.0 hours) (20%) 3. Text: The text book for this course is: Introduction to Nuclear Engineering, 3rd Edition, by John Lamarsh. This covers basic reactor physics as part of a complete survey of nuclear engineering. Readings may also be assigned from certain of the books listed below: Nuclear Reactor Analysis by A. F. Henry Introduction to Nuclear Power by G. Hewitt and J. Collier Fundamentals of Nuclear Science and Engineering by J. Shultis and R. Faw Atoms, Radiation, and Radiation Protection by J. Turner Nuclear Criticality Safety by R. Kneif Radiation Detection and Measurement by G. Knoll 4. Course Objective: To quote the late Professor Allan Henry: “The central problem of reactor physics can be stated quite simply. It is to compute, for any time t, the characteristics of the free-neutron population throughout an extended region of space containing an arbitrary, but known, mixture of materials. Specifically we wish to know the number of neutrons in any infinitesimal volume dV that have kinetic energies between E and E + ∆E and are traveling in directions within an infinitesimal angle of a fixed direction specified by the unit vector Ω. If this number is known, we can use the basic data obtained experimentally and theoretically from low-energy neutron physics to predict the rates at which all possible nuclear reactions, including fission, will take place throughout the region. Thus we can 1 predict how much nuclear power will be generated at any given time at any location in the region.” There are several reasons for needing this information: Physical understanding of reactor safety so that both design and operation is done intelligently. -
Memorandum to Participants JASON 1994 Summer Study
Hydronnclear Testing and the Comprehensive Test Ban: Memorandum to Participants JASON 1994 Summer Study Natural Resources Defense Council, Inc. 1350 New York Avenue, NW, Suite 300 Washington, D.C. 20005 Tel (main): (202) 783-7800 Cochran (direct dial): (202) 624-9329 Paine (direct dial): (202) 624-9350 Fax: (202) 783-5917 INTERNET: [email protected] Although no commonly accepted defInition exists, a "hydronuclear test" may be generally described as a nuclear weapons test, or high-explosive driven criticality experiment, characterized by a nuclear energy release that is insuffIcient to heat the core material to the plasma temperatures that would cause it to explode "like a bomb." In such a test, the TNT equivalent energy release from fission would therefore not exceed the amount released by the chemical high explosive used to compress the fIssile material, and could be considerably ,less. Nuclear-weapon states, and possibly other states, also perform high-explosive driven implosion experiments using fusjon material, although" these' are not nonnally characterized as "hydronuclear tests". Hydronuclear tests can serve a useful role in the development of the full spectrum of unboosted fIssion weapons, including'first generation nuclear weapons of the implosion type with yields in the 5 to 30 kiloton range, more sophisticated designs with yields up to about a megaton, and advanced micro-nuclear weapons with yields of 5 to 500 tons. For pure fIssion weapons hydronuclear tests can be used to:' * optimize the timing of initiation of the -
Boiling Water Reactor Control Rod CR 82M-1
Nuclear Fuel Boiling Water Reactor Control Rod CR 82M-1 Background CR 82M-1 Design The boiling water reactor (BWR) control rod of The hafnium tip of the CR 82M-1 design protects today must meet high operational demands and at the control rod from absorber material swelling the same time contribute to decreased operational when operated in the shutdown mode; i.e., costs for the plant operator. withdrawn from the core. The flexible B4C inventory allows for either matched or high- Description reactivity worth control rods. As structural material, American Iron and Steel Institute 316L stainless The Westinghouse BWR control rod design steel is an irradiation-resistant steel, not readily consists of four stainless steel sheets welded sensitized to irradiation-assisted stress corrosion together to form a cruciform-shaped rod. Each cracking. With an extremely low-cobalt content sheet has horizontally drilled holes to contain the (< 0.02%) in the wing material, these control rods absorber materials (B4C powder and hafnium). can play a significant role in as-low-as-reasonably- This design allows significantly more B4C to be achievable efforts. The design, with horizontally contained in the rod compared to the original drilled absorber holes, limits the washout of control rods of most reactors. B4C in the event of an anomaly in a wing, thus maintaining full reactivity worth. Westinghouse CR 82M-1 control rod for all types of BWRs Westinghouse BWR control rod CR 82M-1 Benefits CR 82M-1 is an evolutionary design based on 45 years of control rod operation -
Cm Element of the Day Curium (Kewreeәm) Is a Transuranic Radioactive Chemical Element with the Symbol Cm and Atomic Number 96
Cm Element of the Day Curium (kewreeәm) is a transuranic radioactive chemical element with the symbol Cm and atomic number 96. This element of the actinide series was named after Marie Curie and her husband Pierre Curie both were known for their research on radioactivity. Most curium is produced by bombarding uranium or plutonium with neutrons in nuclear reactors – one ton of spent nuclear fuel contains about 20 grams of curium. Curium is a hard, dense, silvery metal with a relatively high melting point and boiling point for an actinide. Curium readily oxidizes, and its oxides are a dominant form of this element. When introduced into the human body, curium accumulates in the bones, lungs and liver, where it promotes cancer. All known isotopes of curium are radioactive and have a small critical mass for a sustained nuclear chain reaction. Curium is used in production of heavier actinides and of the 238Pu radionuclide for power sources in artificial pacemakers. It served as the α source in the alpha particle Xray spectrometers used to analyze rock composition. Curium's outer electrons have a principal quantum level of four. How many electrons may fit into this orbital? 1 Chemistry 1. WarmUp 5 2. Review Book Homework 10 3. Notes 20 4. Complete POGIL Activity 30 5. Test Review 20 Announcements Due Today: Mole Airlines Extra Credit Due Today: Read pages 317 to 331 and answer questions 1 9 odd, 15, 17, 19 and 25. Begin work on Study Guide! Will be available after school today. Semester Review Session Thursday at 3:00 pm 2 Homework Review 3 POGIL Activity with Modeling Kits! Turn in 4 Review/Notes 5 Quantum Numbers Review Questions 1. -
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. -
Nuclear Power
MORE CHAPTER 11, #6 Nuclear Power Nuclear Fission Reactors The discovery that several neutrons are emitted in the fission process led to specula- tion concerning the possibility of using these neutrons to initiate other fissions, thereby producing a chain reaction. On December 2, 1942, less than four years after Hahn and Strassmann’s discovery of fission, a group led by Enrico Fermi produced the first self-sustaining chain reaction in a nuclear reactor that they had constructed at the University of Chicago.24 To sustain a chain reaction in a fission reactor, one of the neutrons (on the average) emitted in the fission of 235U must be captured by another 235U nucleus and cause it to fission. The reproduction factor k of a reactor is defined as the average number of neutrons from each fission that cause a subsequent fission. In the case of 235U the maximum possible value of k is about 2.4, but it is normally less than this for two important reasons: (1) some of the neutrons may escape from the region contain- ing fissionable nuclei, and (2) some of the neutrons may be captured by nonfissioning nuclei in the reactor. If k is exactly 1, the reaction will be self-sustaining. If it is less than 1, the reaction will die out. If k is significantly greater than 1, the reaction rate will increase rapidly and “run away.” In the design of nuclear bombs, such a runaway reaction is necessary. In power reactors, the value of k must be kept very nearly equal to 1 (see Figure 11-50). -
Accident-Tolerant Control Rod
NEA/NSC/DOC(2013)9 Accident-tolerant control rod Hirokazu Ohta, Takashi Sawabe, Takanari Ogata Central Research Institute of Electric Power Industry (CRIEPI), Japan Boron carbide (B4C) and hafnium (Hf) metal are used for the neutron absorber materials of control rods in BWRs, and silver-indium-cadmium (Ag-In-Cd) alloy is used in PWRs. These materials are clad with stainless steel. The eutectic point of B4C and iron (Fe) is about 1 150°C and the melting point of Ag-In-Cd alloy is about 800°C, which are lower than the temperature of zircaloy – steam reaction increases rapidly (~1 200°C). Accordingly, it is possible that the control rods melt and collapse before the reactor core is significantly damaged in the case of severe accidents. Since the neutron absorber would be separated from the fuels, there is a risk of re-criticality, when pure water or seawater is injected for emergency cooling. In order to ensure sub-criticality and extend options of emergency cooling in the course of severe accidents, a concept of accident-tolerant control rod (ACT) has been derived. ACT utilises a new absorber material having the following properties: • higher neutron absorption than current control rod; • higher melting or eutectic temperature than 1 200°C where rapid zircaloy oxidation occurs; • high miscibility with molten fuel materials. The candidate of a new absorber material for ATC includes gadolinia (Gd2O3), samaria (Sm2O3), europia (Eu2O3), dysprosia (Dy2O3), hafnia (HfO2). The melting point of these materials and the liquefaction temperature with Fe are higher than the rapid zircaloy oxidation temperature.