Occupational Radiation Exposure from Naval Reactors' Department of Energy Facilities
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Navy Columbia-Class Ballistic Missile Submarine Program
Navy Columbia (SSBN-826) Class Ballistic Missile Submarine Program: Background and Issues for Congress Updated September 14, 2021 Congressional Research Service https://crsreports.congress.gov R41129 Navy Columbia (SSBN-826) Class Ballistic Missile Submarine Program Summary The Navy’s Columbia (SSBN-826) class ballistic missile submarine (SSBN) program is a program to design and build a class of 12 new SSBNs to replace the Navy’s current force of 14 aging Ohio-class SSBNs. Since 2013, the Navy has consistently identified the Columbia-class program as the Navy’s top priority program. The Navy procured the first Columbia-class boat in FY2021 and wants to procure the second boat in the class in FY2024. The Navy’s proposed FY2022 budget requests $3,003.0 (i.e., $3.0 billion) in procurement funding for the first Columbia-class boat and $1,644.0 million (i.e., about $1.6 billion) in advance procurement (AP) funding for the second boat, for a combined FY2022 procurement and AP funding request of $4,647.0 million (i.e., about $4.6 billion). The Navy’s FY2022 budget submission estimates the procurement cost of the first Columbia- class boat at $15,030.5 million (i.e., about $15.0 billion) in then-year dollars, including $6,557.6 million (i.e., about $6.60 billion) in costs for plans, meaning (essentially) the detail design/nonrecurring engineering (DD/NRE) costs for the Columbia class. (It is a long-standing Navy budgetary practice to incorporate the DD/NRE costs for a new class of ship into the total procurement cost of the first ship in the class.) Excluding costs for plans, the estimated hands-on construction cost of the first ship is $8,473.0 million (i.e., about $8.5 billion). -
US COLD WAR AIRCRAFT CARRIERS Forrestal, Kitty Hawk and Enterprise Classes
US COLD WAR AIRCRAFT CARRIERS Forrestal, Kitty Hawk and Enterprise Classes BRAD ELWARD ILLUSTRATED BY PAUL WRIGHT © Osprey Publishing • www.ospreypublishing.com NEW VANGUARD 211 US COLD WAR AIRCRAFT CARRIERS Forrestal, Kitty Hawk and Enterprise Classes BRAD ELWARD ILLUSTRATED BY PAUL WRIGHT © Osprey Publishing • www.ospreypublishing.com CONTENTS INTRODUCTION 4 ORIGINS OF THE CARRIER AND THE SUPERCARRIER 5 t World War II Carriers t Post-World War II Carrier Developments t United States (CVA-58) THE FORRESTAL CLASS 11 FORRESTAL AS BUILT 14 t Carrier Structures t The Flight Deck and Hangar Bay t Launch and Recovery Operations t Stores t Defensive Systems t Electronic Systems and Radar t Propulsion THE FORRESTAL CARRIERS 20 t USS Forrestal (CVA-59) t USS Saratoga (CVA-60) t USS Ranger (CVA-61) t USS Independence (CVA-62) THE KITTY HAWK CLASS 26 t Major Differences from the Forrestal Class t Defensive Armament t Dimensions and Displacement t Propulsion t Electronics and Radars t USS America, CVA-66 – Improved Kitty Hawk t USS John F. Kennedy, CVA-67 – A Singular Class THE KITTY HAWK AND JOHN F. KENNEDY CARRIERS 34 t USS Kitty Hawk (CVA-63) t USS Constellation (CVA-64) t USS America (CVA-66) t USS John F. Kennedy (CVA-67) THE ENTERPRISE CLASS 40 t Propulsion t Stores t Flight Deck and Island t Defensive Armament t USS Enterprise (CVAN-65) BIBLIOGRAPHY 47 INDEX 48 © Osprey Publishing • www.ospreypublishing.com US COLD WAR AIRCRAFT CARRIERS FORRESTAL, KITTY HAWK AND ENTERPRISE CLASSES INTRODUCTION The Forrestal-class aircraft carriers were the world’s first true supercarriers and served in the United States Navy for the majority of America’s Cold War with the Soviet Union. -
3 Gamma-Ray Detectors
3 Gamma-Ray Detectors Hastings A Smith,Jr., and Marcia Lucas S.1 INTRODUCTION In order for a gamma ray to be detected, it must interact with matteu that interaction must be recorded. Fortunately, the electromagnetic nature of gamma-ray photons allows them to interact strongly with the charged electrons in the atoms of all matter. The key process by which a gamma ray is detected is ionization, where it gives up part or all of its energy to an electron. The ionized electrons collide with other atoms and liberate many more electrons. The liberated charge is collected, either directly (as with a proportional counter or a solid-state semiconductor detector) or indirectly (as with a scintillation detector), in order to register the presence of the gamma ray and measure its energy. The final result is an electrical pulse whose voltage is proportional to the energy deposited in the detecting medhtm. In this chapter, we will present some general information on types of’ gamma-ray detectors that are used in nondestructive assay (NDA) of nuclear materials. The elec- tronic instrumentation associated with gamma-ray detection is discussed in Chapter 4. More in-depth treatments of the design and operation of gamma-ray detectors can be found in Refs. 1 and 2. 3.2 TYPES OF DETECTORS Many different detectors have been used to register the gamma ray and its eneqgy. In NDA, it is usually necessary to measure not only the amount of radiation emanating from a sample but also its energy spectrum. Thus, the detectors of most use in NDA applications are those whose signal outputs are proportional to the energy deposited by the gamma ray in the sensitive volume of the detector. -
1. Gamma-Ray Detectors for Nondestructive Analysis P
1. GAMMA-RAY DETECTORS FOR NONDESTRUCTIVE ANALYSIS P. A. Russo and D. T. Vo I. INTRODUCTION AND OVERVIEW Gamma rays are used for nondestructive quantitative analysis of nuclear material. Knowledge of both the energy of the gamma ray and its rate of emission from the unknown mass of nuclear material is required to interpret most measurements of nuclear material quantities. Therefore, detection of gamma rays for nondestructive analysis of nuclear materials requires both spectroscopy capability and knowledge of absolute specific detector response. Some techniques nondestructively quantify attributes other than nuclear material mass, but all rely on the ability to distinguish elements or isotopes and measure the relative or absolute yields of their corresponding radiation signatures. All require spectroscopy and most require high resolution. Therefore, detection of gamma rays for quantitative nondestructive analysis (NDA) of the mass or of other attributes of nuclear materials requires spectroscopy. A previous book on gamma-ray detectors for NDA1 provided generic descriptions of three detector categories: inorganic scintillation detectors, semiconductor detectors, and gas-filled detectors. This report described relevant detector properties, corresponding spectral characteristics, and guidelines for choosing detectors for NDA. The current report focuses on significant new advances in detector technology in these categories. Emphasis here is given to those detectors that have been developed at least to the stage of commercial prototypes. The type of NDA application – fixed installation in a count room, portable measurements, or fixed installation in a processing line or other active facility (storage, shipping/receiving, etc.) – influences the choice of an appropriate detector. Some prototype gamma-ray detection techniques applied to new NDA approaches may revolutionize how nuclear materials are quantified in the future. -
DRC-2016-012921.Pdf
CLN-SRT-011 R1.0 Page 2 of 33 Introduction ................................................................................................................................ 3 Sources of Radiation .................................................................................................................. 3 Radiation: Particle vs Electromagnetic ....................................................................................... 5 Ionizing and non- ionizing radiation ............................................................................................ 8 Radioactive Decay ....................................................................................................................10 Interaction of Radiation with Matter ...........................................................................................15 Radiation Detection and Measurement .....................................................................................17 Biological Effects of Radiation ...................................................................................................18 Radiation quantities and units ...................................................................................................18 Biological effects .......................................................................................................................20 Effects of Radiation by Biological Organization .........................................................................20 Mechanisms of biological damage ............................................................................................21 -
Portable Front-End Readout System for Radiation Detection
Portable Front-End Readout System for Radiation Detection by Maris Tali THESIS for the degree of MASTER OF SCIENCE (Master in Electronics) Faculty of Mathematics and Natural Sciences University of Oslo June 2015 Det matematisk- naturvitenskapelige fakultet Universitetet i Oslo Portable Front-End Readout System for Radiation Detection Maris Tali Portable Front-End Readout System for Radiation Detection Maris Tali Portable Front-End Readout System for Radiation Detection Acknowledgements First of all, I would like to thank my advisor, Ketil Røed, for giving me the opportunity to write my master thesis on such an interesting and challenging subject as radiation instrumentation and measurement. I would also like to thank him for his insight and guidance during my master thesis and for the exciting opportunities during my studies to work in a real experimental environment. I would also like to thank the Electronic Laboratory of the University of Oslo, specif- ically Halvor Strøm, David Bang and Stein Nielsen who all gave me valuable advice and assistance and without whom this master thesis could not have been finished. Lastly, I would like to thank the co-designer of the system whom I worked together with during my master thesis, Eino J. Oltedal. It is customary to write that half of ones master thesis belongs to ones partner. However, this is actually the case in this instance so I guess 2/3 of my master thesis is yours and I definitely could not have done this without you. So, thank you very much! Oslo, June 2015 Maris Tali I Maris Tali Portable Front-End Readout System for Radiation Detection Contents Acknowledgments I Glossary VI List of Figures X List of Tables X Abstract XI 1 Introduction 1 1.1 Background and motivation . -
Class Ballistic Missile Submarine Program: Background and Issues for Congress
Navy Columbia (SSBN-826) Class Ballistic Missile Submarine Program: Background and Issues for Congress (name redacted) Specialist in Naval Affairs June 29, 2018 Congressional Research Service 7-.... www.crs.gov R41129 Navy Columbia (SSBN-826) Class Ballistic Missile Submarine Program Summary The Columbia (SSBN-826) class program, previously known as the Ohio replacement program (ORP) or SSBN(X) program, is a program to design and build a new class of 12 ballistic missile submarines (SSBNs) to replace the Navy’s current force of 14 Ohio-class SSBNs. The Navy has identified the Columbia-class program as the Navy’s top priority program. The Navy wants to procure the first Columbia-class boat in FY2021. The Navy’s proposed FY2019 budget requests $3,005.3 million in advance procurement (AP) funding and $704.9 million in research and development funding for the program. The Navy as of January 2017 estimated the procurement cost of the lead ship in the class at $8.2 billion in constant 2017 dollars, not including several billion dollars in additional cost for plans for the class, and the average unit procurement cost of ships 2 through 12 in the program at $6.5 billion each in constant FY2017 dollars. An April 2018 Government Accountability Office (GAO) report assessing selected major DOD weapon acquisition programs stated that the estimated total acquisition cost of the Columbia-class program is $102,075.3 million (about $102.1 billion) in constant FY2018 dollars, including $12,901.0 million (about $12.9 billion) in research and development costs and $89,174.3 million (about $89.2 billion) in procurement costs. -
Navy Columbia (SSBN-826) Class Ballistic Missile Submarine Program: Background and Issues for Congress
Navy Columbia (SSBN-826) Class Ballistic Missile Submarine Program: Background and Issues for Congress Updated February 26, 2020 Congressional Research Service https://crsreports.congress.gov R41129 Navy Columbia (SSBN-826) Class Ballistic Missile Submarine Program Summary The Columbia (SSBN-826) class program is a program to design and build a class of 12 new ballistic missile submarines (SSBNs) to replace the Navy’s current force of 14 aging Ohio-class SSBNs. The Navy has identified the Columbia-class program as the Navy’s top priority program. The Navy wants to procure the first Columbia-class boat in FY2021. Research and development work on the program has been underway for several years, and advance procurement (AP) funding for the first boat began in FY2017. The Navy’s proposed FY2021 budget requests $2,891.5 million in procurement funding, $1,123.2 million in advance procurement (AP) funding, and $397.3 million in research and development funding for the program. The Navy’s FY2021 budget submission estimates the total procurement cost of the 12-ship class at $109.8 billion in then-year dollars. A May 2019 Government Accountability Office (GAO) report assessing selected major DOD weapon acquisition programs stated that the estimated total acquisition (development plus procurement) cost of the Columbia-class program as of June 2018 was $103,035.2 million (about $103.0 billion) in constant FY2019 dollars, including $13,103.0 million (about $13.1 billion) in research and development costs and $89,932.2 million (about $89.9 billion) -
Sea Power to Stop British Fleeing
NAVY / MARINE CORPS / COAST GUARD / MERCHANT MARINE SPECIAL REPORT: EXPEDITIONARY WARFARE June 2019 $5.00 NAVY LEAGUE OF THE UNITED STATES www.navyleague.org SEA-AIR-SPACE 2019 ROUNDUP / DEFENSE BUDGET SHOWDOWN / ABOARD THE USS LEWIS B. PULLER THE SHAPE OF FREEDOM THE SHAPE OF FREEDOM The Shape of Freedom the shape of freedom Accelerating LPD Flight II will enhance naval capacity and lethality and bring a flexible, survivable and a ordable warship that our Navy-Marine Corps Team needs now. Accelerating this next generation warship helps provide distributed maritime capability, leverages a hot production line, and is an important and continued investment in a supplier base of 400 companies in 30 states. HUNTINGTONINGALLS.COM/LPD-FLIGHT-II PRESIDENT’S MESSAGE Thank You! BY ALAN KAPLAN, NAVY LEAGUE NATIONAL PRESIDENT Thank you for the opportunity and honor of serving you. There have been many accomplishments that our headquarters and volunteer team can be proud of over the last two of years. Leading this charge has been such a privilege. Serving as your national president has been a humbling expe- rience, and working side by side with all of you, as we worked together diligently, as a team, to elevate our organization’s mission to new heights, has been an honor. Our Navy League is now an organization of action, but we are also good at listening. We pay very close attention to what our sea service leaders are saying. Their challenges and what they are focused on are equally important to us as we advocate and educate for their well-being. -
Senate Hearings Before the Committee on Appropriations
S. HRG. 109–130 Senate Hearings Before the Committee on Appropriations Department of Defense Appropriations Fiscal Year 2006 109th CONGRESS, FIRST SESSION H.R. 2863 DEPARTMENT OF DEFENSE NONDEPARTMENTAL WITNESSES Department of Defense Appropriations, 2006 (H.R. 2863) S. HRG. 109–130 DEPARTMENT OF DEFENSE APPROPRIATIONS FOR FISCAL YEAR 2006 HEARINGS BEFORE A SUBCOMMITTEE OF THE COMMITTEE ON APPROPRIATIONS UNITED STATES SENATE ONE HUNDRED NINTH CONGRESS FIRST SESSION ON H.R. 2863 AN ACT MAKING APPROPRIATIONS FOR THE DEPARTMENT OF DEFENSE FOR THE FISCAL YEAR ENDING SEPTEMBER 30, 2006, AND FOR OTHER PURPOSES Department of Defense Nondepartmental witnesses Printed for the use of the Committee on Appropriations ( Available via the World Wide Web: http://www.gpoaccess.gov/congress/index.html U.S. GOVERNMENT PRINTING OFFICE 99–854 PDF WASHINGTON : 2005 For sale by the Superintendent of Documents, U.S. Government Printing Office Internet: bookstore.gpo.gov Phone: toll free (866) 512–1800; DC area (202) 512–1800 Fax: (202) 512–2250 Mail: Stop SSOP, Washington, DC 20402–0001 COMMITTEE ON APPROPRIATIONS THAD COCHRAN, Mississippi, Chairman TED STEVENS, Alaska ROBERT C. BYRD, West Virginia ARLEN SPECTER, Pennsylvania DANIEL K. INOUYE, Hawaii PETE V. DOMENICI, New Mexico PATRICK J. LEAHY, Vermont CHRISTOPHER S. BOND, Missouri TOM HARKIN, Iowa MITCH MCCONNELL, Kentucky BARBARA A. MIKULSKI, Maryland CONRAD BURNS, Montana HARRY REID, Nevada RICHARD C. SHELBY, Alabama HERB KOHL, Wisconsin JUDD GREGG, New Hampshire PATTY MURRAY, Washington ROBERT F. BENNETT, Utah BYRON L. DORGAN, North Dakota LARRY CRAIG, Idaho DIANNE FEINSTEIN, California KAY BAILEY HUTCHISON, Texas RICHARD J. DURBIN, Illinois MIKE DEWINE, Ohio TIM JOHNSON, South Dakota SAM BROWNBACK, Kansas MARY L. -
Semiconductor Detectors Silvia Masciocchi GSI Darmstadt and University of Heidelberg
Semiconductor detectors Silvia Masciocchi GSI Darmstadt and University of Heidelberg 39th Heidelberg Physics Graduate Days, HGSFP Heidelberg October 10, 2017 Semiconductor detector: basics IONIZATION as in gas detectors → Now in semiconductors = solid materials with crystalline structure (Si, Ge, GaAs) → electron-hole pairs (instead of electron-ion) + use microchip technology: structures with few micrometer precision can be produced at low cost. Read-out electronics can be directly bonded to the detectors + only a few eV per electron-hole pair → 10 times more charge produced (wrt gas) → better energy resolution + high density compared to gases → need only thin layers (greater stopping power) – apart from silicon, the detectors need to be cooled (cryogenics) – crystal lattices → radiation damage [email protected] Semiconductor detectors, October 11, 2017 2 Applications Main applications: ● γ spectroscopy with high energy resolution ● Energy measurement of charged particles (few MeV) and particle identification (PID) via dE/dx (multiple layers needed) ● Very high spatial resolution for tracking and vertexing A few dates: 1930s – very first crystal detectors 1950s – first serious developments of particle detectors 1960s – energy measurement devices in commerce [email protected] Semiconductor detectors, October 11, 2017 3 Semiconductor detectors: outline ● Principle of operation of semiconductor detectors ● Properties of semiconductors (band structure) ● Intrinsic material ● Extrinsic (doped) semiconductors ● p-n junction ● Signal generation ● Energy measurement with semiconductor detectors ● Position measurement with semiconductor detectors ● Radiation damage [email protected] Semiconductor detectors, October 11, 2017 4 Principle of operation ● Detector operates as a solid state ionization chamber ● Charged particles create electron-hole pairs ● Place the crystal between two electrodes that set up an electric field → charge carriers drift and induce a signal ● Less than 1/3 of energy deposited goes into ionization. -
Internal and External Exposure Exposure Routes 2.1
Exposure Routes Internal and External Exposure Exposure Routes 2.1 External exposure Internal exposure Body surface From outer space contamination and the sun Inhalation Suspended matters Food and drink consumption From a radiation Lungs generator Radio‐ pharmaceuticals Wound Buildings Ground Radiation coming from outside the body Radiation emitted within the body Radioactive The body is equally exposed to radiation in both cases. materials "Radiation exposure" refers to the situation where the body is in the presence of radiation. There are two types of radiation exposure, "internal exposure" and "external exposure." External exposure means to receive radiation that comes from radioactive materials existing on the ground, suspended in the air, or attached to clothes or the surface of the body (p.25 of Vol. 1, "External Exposure and Skin"). Conversely, internal exposure is caused (i) when a person has a meal and takes in radioactive materials in the food or drink (ingestion); (ii) when a person breathes in radioactive materials in the air (inhalation); (iii) when radioactive materials are absorbed through the skin (percutaneous absorption); (iv) when radioactive materials enter the body from a wound (wound contamination); and (v) when radiopharmaceuticals containing radioactive materials are administered for the purpose of medical treatment. Once radioactive materials enter the body, the body will continue to be exposed to radiation until the radioactive materials are excreted in the urine or feces (biological half-life) or as the radioactivity weakens over time (p.26 of Vol. 1, "Internal Exposure"). The difference between internal exposure and external exposure lies in whether the source that emits radiation is inside or outside the body.