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Spectroscopy of Neutron-Rich 34,35,36,37,38 P Populated In
PHYSICAL REVIEW C 92, 044308 (2015) , , , , Spectroscopy of neutron-rich 34 35 36 37 38P populated in binary grazing reactions R. Chapman,1,* A. Hodsdon,1 M. Bouhelal,2 F. Haas,3 X. Liang,1 F. Azaiez,4 Z. M. Wang,1 B. R. Behera,5 M. Burns,1 E. Caurier,3 L. Corradi,5 D. Curien,3 A. N. Deacon,6 Zs. Dombradi,´ 7 E. Farnea,8 E. Fioretto,5 A. Gadea,5 F. Ibrahim,4 A. Jungclaus,9 K. Keyes,1 V. Kumar, 1 S. Lunardi,8 N. Marginean,˘ 5,10 G. Montagnoli,8 D. R. Napoli,5 F. Nowacki,3 J. Ollier,1,11 D. O’Donnell,1,12 A. Papenberg,1 G. Pollarolo,13 M.-D. Salsac,14 F. Scarlassara,8 J. F. Smith,1 K. M. Spohr,1 M. Stanoiu,10 A. M. Stefanini,5 S. Szilner,5,15 M. Trotta,5 and D. Verney4 1School of Engineering and Computing, University of the West of Scotland, Paisley PA1 2BE, United Kingdom, and The Scottish Universities Physics Alliance (SUPA) 2Laboratoire de Physique Appliquee´ et Theorique,´ Universite´ Larbi Tebessa,´ Tebessa,´ Algerie´ 3IPHC, UMR7178, CNRS-IN2P3, and Universite´ de Strasbourg, F-67037 Strasbourg Cedex 2, France 4IPN, IN2P3-CNRS and Universite´ Paris-Sud, F-91406 Orsay Cedex, France 5INFN, Laboratori Nazionali di Legnaro, I-35020 Legnaro, Padova, Italy 6Schuster Laboratory, University of Manchester, Manchester M13 9PL, United Kingdom 7MTA ATOMKI, P.O. Box 51, H-4001 Debrecen, Hungary 8Dipartimento di Fisica and INFN-Sezione di Padova, Universita` di Padova, I35131 Padova, Italy 9Instituto de Estructura de la Materia, CSIC, E-28006 Madrid, Spain 10Horia Hulubei National Institute of Physics and Nuclear Engineering-IFIN-HH, Strasse Atomistilor No. -
Stable Isotopes of Cobalt Properties of Cobalt
Stable Isotopes of Cobalt Isotope Z(p) N(n) Atomic Mass Natural Abundance Nuclear Spin Co-59 27 32 58.93320 100.00% 7/2- Cobalt was discovered in 1735 by Georg Brandt. Its name derives from the German word kobald, meaning "goblin" or "evil spirit." Minerals containing cobalt were used by the early civilizations of Egypt and Mesopotamia for coloring glass deep blue. Cobalt oxide is used today to add a pink or blue color to glass. It is also an important trace element in soils and necessary for animal nutrition. The most important modern use of cobalt is in the manufacture of various wear-resistant and superalloys. Its alloys have shown high resistance to corrosion and oxidation at high temperatures. Radioactive Cobalt-60 is used in radiography and in the sterilization of food. A silvery-white, shining, hard, ductile, somewhat malleable metal, cobalt is also ferromagnetic, with permeability two-thirds that of iron. It has exceptional magnetic properties in alloys. It is attached by dilute hydrochloric and sulfuric acids. It corrodes readily in air, and it has unusual coordinating properties, especially the trivalent ion. It is noncombustible except in powder form. Cobalt occurs in two allotropic modifications over a wide range of temperatures: the crystalline close-packed- hexagonal form is known as the alpha form, which turns into the beta (or gamma) form above 417 ºC. In finely powdered form, cobalt ignites spontaneously in air. Reactions with acetylene and bromine pentafluoride proceed to incandescence and can become violent. The metal is moderately toxic by ingestion. Inhalation of dusts can damage lungs. -
Review Article the Copper Radioisotopes: a Systematic Review with Special Interest to Cu
Hindawi Publishing Corporation BioMed Research International Volume 2014, Article ID 786463, 9 pages http://dx.doi.org/10.1155/2014/786463 Review Article The Copper Radioisotopes: A Systematic Review with Special Interest to 64Cu Artor Niccoli Asabella,1 Giuseppe Lucio Cascini,2 Corinna Altini,1 Domenico Paparella,1 Antonio Notaristefano,1 and Giuseppe Rubini1 1 NuclearMedicine,UniversityofBariAldoMoro,PiazzaG.Cesare11,70124Bari,Italy 2 Nuclear Medicine, University of Catanzaro Magna Graecia, Viale Europa, Localita´ Germaneto, 88100 Catanzaro, Italy Correspondence should be addressed to Artor Niccoli Asabella; [email protected] Received 23 December 2013; Accepted 18 April 2014; Published 7 May 2014 Academic Editor: Gianluca Valentini Copyright © 2014 Artor Niccoli Asabella et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Copper (Cu) is an important trace element in humans; it plays a role as a cofactor for numerous enzymes and other proteins crucial 63 for respiration, iron transport, metabolism, cell growth, and hemostasis. Natural copper comprises two stable isotopes, Cu and 65 60 61 62 64 Cu, and 5 principal radioisotopes for molecular imaging applications ( Cu, Cu, Cu, and Cu) and in vivo targeted radiation 64 67 therapy ( Cu and Cu). The two potential ways to produce Cu radioisotopes concern the use of the cyclotron or the reactor. A noncopper target is used to produce noncarrier-added Cu thanks to a chemical separation from the target material using ion exchange chromatography achieving a high amount of radioactivity with the lowest possible amount of nonradioactive isotopes. -
THE NATURAL RADIOACTIVITY of the BIOSPHERE (Prirodnaya Radioaktivnost' Iosfery)
XA04N2887 INIS-XA-N--259 L.A. Pertsov TRANSLATED FROM RUSSIAN Published for the U.S. Atomic Energy Commission and the National Science Foundation, Washington, D.C. by the Israel Program for Scientific Translations L. A. PERTSOV THE NATURAL RADIOACTIVITY OF THE BIOSPHERE (Prirodnaya Radioaktivnost' iosfery) Atomizdat NMoskva 1964 Translated from Russian Israel Program for Scientific Translations Jerusalem 1967 18 02 AEC-tr- 6714 Published Pursuant to an Agreement with THE U. S. ATOMIC ENERGY COMMISSION and THE NATIONAL SCIENCE FOUNDATION, WASHINGTON, D. C. Copyright (D 1967 Israel Program for scientific Translations Ltd. IPST Cat. No. 1802 Translated and Edited by IPST Staff Printed in Jerusalem by S. Monison Available from the U.S. DEPARTMENT OF COMMERCE Clearinghouse for Federal Scientific and Technical Information Springfield, Va. 22151 VI/ Table of Contents Introduction .1..................... Bibliography ...................................... 5 Chapter 1. GENESIS OF THE NATURAL RADIOACTIVITY OF THE BIOSPHERE ......................... 6 § Some historical problems...................... 6 § 2. Formation of natural radioactive isotopes of the earth ..... 7 §3. Radioactive isotope creation by cosmic radiation. ....... 11 §4. Distribution of radioactive isotopes in the earth ........ 12 § 5. The spread of radioactive isotopes over the earth's surface. ................................. 16 § 6. The cycle of natural radioactive isotopes in the biosphere. ................................ 18 Bibliography ................ .................. 22 Chapter 2. PHYSICAL AND BIOCHEMICAL PROPERTIES OF NATURAL RADIOACTIVE ISOTOPES. ........... 24 § 1. The contribution of individual radioactive isotopes to the total radioactivity of the biosphere. ............... 24 § 2. Properties of radioactive isotopes not belonging to radio- active families . ............ I............ 27 § 3. Properties of radioactive isotopes of the radioactive families. ................................ 38 § 4. Properties of radioactive isotopes of rare-earth elements . -
Annual Report 1951 National Bureau of Standards
Annual Report 1951 National Bureau of Standards Miscellaneous Publication 204 UNITED STATES DEPARTMENT OF COMMERCE Charles Sawyer, Secretary NATIONAL BUREAU OF STANDARDS A. V. Astint, Director Annual Report 1951 National Bureau of Standards For sale by the Superintendent of Documents, U. S. Government Printing Office Washington 2 5, D. C. Price 50 cents CONTENTS Page 1. General Review 1 2. Electricity 16 Beam intensification in a high-voltage oscillograph 17, Low-temperature dry cells 17, High-rate batteries 17, Battery additives 18. 3. Optics and Metrology 18 The kinorama 19, Measurement of visibility for aircraft 20, Antisubmarine aircraft searchlights 20, Resolving power chart 20, Refractivity 21, Thermal expansivity of aluminum alloys 21. 4. Heat and Power . 21 Thermodynamic properties of materials 22, Synthetic rubber and other high polymers 23, Combustors for jet engines 24, Temperature and composition of flames 25, Engine "knock" 25, Low-temperature physics 26, Medical physics instrumentation 28. 5. Atomic and Radiation Physics 28 Atomic standard of length 29, Magnetic moment of the proton 29, Spectra of artificial elements 31, Photoconductivity of semiconductors 31, Radiation detecting instruments 32, Protection against radiation 32, X-ray equipment 33, Atomic and molecular ions 35, Electron physics 35, Tables of nuclear data 35, Atomic energy levels 36. 6. Chemistry 36 Radioactive carbohydrates 36, Dextran as a substitute for blood plasma 37, Acidity and basicity in organic solvents 37, Interchangeability of fuel gases 38, Los Angeles "smog" 39, Infrared spectra of alcohols 39, Electrodeposi- tion 39, Development of analytical methods 40, Physical constants 42. 7. Mechanics 42 Turbulent flow 43, Turbulence at supersonic speeds 43, Dynamic properties of materials 43, High-frequency vibrations 44, Hearing loss 44, Physical properties by sonic methods 44, Water waves 46, Density currents 46, Precision weighing 46, Viscosity of gases 46, Evaporated thin films 47. -
Hydrogen Transmutation of Nickel in Glow Discharge
International Journal of Materials Science ISSN 0973-4589 Volume 12, Number 3 (2017), pp. 405-409 © Research India Publications http://www.ripublication.com Hydrogen Transmutation of Nickel in Glow Discharge Vladimir K. Nevolin National Research University of Electronic Technology (MIET), Moscow, Russia. Abstract Background: The possibility of the existence of subatomic hydrogen states was theoretically predicted previously. Objectives: Prove that the transmutation of elements is possible in specially prepared conditions for hydrogen. Methodology: By comparing the mass spectra of deposits on silicon substrates and target electrodes, it is shown that a change in the composition is observed in a magnetron Argon. Results: An increase in the concentration of 62 60 the nickel isotope 28 Ni and a decrease in the isotope concentration 28 Ni are shown. Conclusion: These results confirm the results obtained earlier in the heat generator Rossi, who worked more than a year, found an increase in the 62 isotope 28 Ni due to a decrease in the proportion of other isotopes. Keywords: transmutation, isotopes of nickel, glow discharge, argon, hydrogen INTRODUCION It is considered that the cold transmutation of elements (cold nuclear reactions) has been experimentally demonstrated [1]. On the basis of this phenomenon, energy generators are created in which long-term release of thermal energy in excess of expended energy is observed [2]. From many experimental studies it can be seen that hydrogen, which plays a pivotal role in the reaction zone, may be delivered through a variety of chemical compounds; for example, using lithium aluminium hydride LiAlH4. An analysis of the products of nuclear reactions suggests the possibility of many simultaneous nuclear fusion and decomposition reactions [3]. -
Chapter 2 Atoms, Molecules and Ions
Chapter 2 Atoms, Molecules and Ions PRACTICING SKILLS Atoms:Their Composition and Structure 1. Fundamental Particles Protons Electrons Neutrons Electrical Charges +1 -1 0 Present in nucleus Yes No Yes Least Massive 1.007 u 0.00055 u 1.007 u 3. Isotopic symbol for: 27 (a) Mg (at. no. 12) with 15 neutrons : 27 12 Mg 48 (b) Ti (at. no. 22) with 26 neutrons : 48 22 Ti 62 (c) Zn (at. no. 30) with 32 neutrons : 62 30 Zn The mass number represents the SUM of the protons + neutrons in the nucleus of an atom. The atomic number represents the # of protons, so (atomic no. + # neutrons)=mass number 5. substance protons neutrons electrons (a) magnesium-24 12 12 12 (b) tin-119 50 69 50 (c) thorium-232 90 142 90 (d) carbon-13 6 7 6 (e) copper-63 29 34 29 (f) bismuth-205 83 122 83 Note that the number of protons and electrons are equal for any neutral atom. The number of protons is always equal to the atomic number. The mass number equals the sum of the numbers of protons and neutrons. Isotopes 7. Isotopes of cobalt (atomic number 27) with 30, 31, and 33 neutrons: 57 58 60 would have symbols of 27 Co , 27 Co , and 27 Co respectively. Chapter 2 Atoms, Molecules and Ions Isotope Abundance and Atomic Mass 9. Thallium has two stable isotopes 203 Tl and 205 Tl. The more abundant isotope is:___?___ The atomic weight of thallium is 204.4 u. The fact that this weight is closer to 205 than 203 indicates that the 205 isotope is the more abundant isotope. -
22.101 Applied Nuclear Physics (Fall 2006) Problem Set No. 1 Due: Sept
22.101 Applied Nuclear Physics (Fall 2006) Problem Set No. 1 Due: Sept. 13, 2006 Problem 1 Before getting into the concepts of nuclear physics, every student should have some feeling for the numerical values of properties of nuclear radiations, such as energy and speed, wavelength, and frequency, etc. This involves some back of the envelope calculations using appropriate universal constants. (i) A thermal neutron in a nuclear reactor is a neutron with kinetic energy equal to kBT, where kB is the Boltzmann’s constant and T is the temperature of the reactor. Explain briefly the physical basis of this statement. Taking T to be the room temperature, 20C, calculate the energy of the thermal neutron (in units of ev), and then find its speed v (in cm/sec), the de Broglie wavelength λ (in A) and circular frequency ω (radian/sec). Compare these values with the energy, speed, and interatomic distance of atoms that make up the materials in the reactor. What is the point of comparing the neutron wavelength with typical atomic separations in a solid? (ii) Consider a 2 Kev x-ray, calculate the frequency and wavelength of this photon. What would be the point of comparing the x-ray wavelength with that of the thermal neutron? For an electron with wavelength equal to that of the thermal neutron, what energy would it have? 2 2 (iii) The classical radius of the electron, defined as e / mec , with e being the electron charge, me the electron rest mass, and c the speed of light, has the value of 2.818 x 10-13 cm. -
Problem Set 3 Solutions
22.01 Fall 2016, Problem Set 3 Solutions October 9, 2016 Complete all the assigned problems, and do make sure to show your intermediate work. 1 Activity and Half Lives 1. Given the half lives and modern-day abundances of the three natural isotopes of uranium, calculate the isotopic fractions of uranium when the Earth first formed 4.5 billion years ago. Today, uranium consists of 0.72% 235U, 99.2745% 238U, and 0.0055% 234U. However, it is clear that the half life of 234U (245,500 years) is so short compared to the lifetime of the Earth (4,500,000,000 years) that it would have all decayed away had there been some during the birth of the Earth. Therefore, we look a little closer, and find that 234U is an indirect decay product of 238U, by tracing it back from its parent nuclides on the KAERI table: α β− β− 238U −! 234T h −! 234P a −! 234U (1) Therefore we won’t consider there being any more 234U than would normally be in equi librium with the 238U around at the time. We set up the two remaining equations as follows: −t t ;235 −t t ;238 = 1=2 = 1=2 N235 = N0235 e N238 = N0238 e (2) Using the current isotopic abundances from above as N235 and N238 , the half lives from n 9 t 1 1 the KAERI Table of Nuclides t =2;235 = 703800000 y; t =2;238 = 4:468 · 10 y , and the lifetime of the earth in years (keeping everything in the same units), we arrive at the following expressions for N0235 and N0238 : N235 0:0072 N238 0:992745 N0235 =−t = 9 = 4:307N0238 =−t = 9 = 2:718 (3) =t1 ;235 −4:5·10 =7:038·108 =t1 ;238 −4:5·10 =4:468·109 e =2 e e =2 e Finally, taking the ratios of these two relative abundances gives us absolute abundances: 4:307 2:718 f235 = = 0:613 f238 = = 0:387 (4) 4:307 + 2:718 4:307 + 2:718 235U was 61.3% abundant, and 238U was 38.7% abundant. -
Załącznik Nr 3 Do Wniosku O Przeprowadzenie Postępowania Habilitacyjnego
Załącznik nr 3 do wniosku o przeprowadzenie postępowania habilitacyjnego Author's review of his own writings 1. Jan Kurpeta 2. Posiadane dyplomy, stopnie naukowe Degree of Doctor of Philosophy in physics, University of Warsaw, Faculty of Physics, year 1999, title of dissertation: „Properties of the neutron-rich nuclei at the edge of known nuclei area.” Master of Science and Engineering, Warsaw University of Technology, Faculty of Technical Physics and Applied Mathematics, year 1993, title of master's thesis: „Influence of nucleon effective mass on single particle motion in the deformed nuclei.” 3. Informacje o dotychczasowym zatrudnieniu w jednostkach naukowych University of Warsaw, Faculty of Physics, Institute of Experimental Physics, Nuclear Spectroscopy Division, assistant professor since15 February 2001 University of Leuven (Belgium), Instituut voor Kern- en Stralingsfysica, post-doc position from 1 September 1998 to 31 October 1999 University of Jyväskylä (Finland), Faculty of Physics, scholarship from Center for International Mobility, PhD studies from 3 February to 15 December 1995 University of Warsaw, Faculty of Physics, Institute of Experimental Physics, Nuclear Spectroscopy Division, PhD studies from October 1993 to September 1998 Space Research Center Polish Academy of Sciences in Warsaw, Department of Planetary Geodesy, part time job for 6 months in 1993 1 4. Wskazanie osiągnięcia* wynikającego z art. 16 ust. 2 ustawy z dnia 14 marca 2003 r. o stopniach naukowych i tytule naukowym oraz o stopniach i tytule w zakresie sztuki (Dz. U. nr 65, poz. 595 ze zm.): a) tytuł osiągnięcia naukowego Structure of exotic, neutron-rich fission fragments of mass around A = 110. b) Jednotematyczny cykl publikacji przedstawiających osiągnięcie naukowe [A1] J. -
DISSERTATION By
CYCLOTRON BOMBARDMENTS WITH HE3 a n d r 3 DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philisophy in the Graduate School of The Ohio State University By Thomas William Donaven, 3.S., M.A The Ohio State University 1952 Approved by Adviser ( fe/\J TABLE OF CONTENTS Cyclotron Bombardments with He^ or H3 Acknowledgements Page Introduction 1 Description of Apparatus 3 Method of Operation 13 Purification of He^ or 17 Results 20 Conclusions 30 References 32 Miscellaneous Photographs 36 Autobiography 1*0 i 918254 Acknowledgements It is with deep appreciation that I extend thanks to Professor M. L. Pool for his guidance in this work. Special thanks is also due to Dr. D. N. Kundu for his advice, help, and cooperation in this project. Acknowledgement is also made to Mr. Paul Weiler and Mr. Donald Moore of the cyclotron staff, and to the machine shop under Mr. Carl McWhirt, for their aid in completing this work. The support given me through fellowships by The Ohio State University Physics Department and by the Oak Ridge Institute of Nuclear Studies is gratefully acknowledged. ii INTRODUCTION The naturally occurring elements whose atoms are heavier than Bismuth, i.e. Po, At, Rn, Fr, Th, Pa, U, etc. are all radioactive. The remainder of the elements may be made radioactive by hitting them with high speed nuclei of other elements. The elements whose nuclei are normally used to create radioactivity are hydrogen and helium. In order to give a nucleus a high speed with the minimum of equipment, it is necessary to strip all of the electrons from the atom, leaving its bare nucleus to be accelerated. -
I N Dc International Nuclear Data Committee Iaea
International Atomic Energy Agency INDC(CCP)-335 Distr.: L I N DC INTERNATIONAL NUCLEAR DATA COMMITTEE TRANSLATION OF SELECTED PAPERS PUBLISHED IN YADERNYE KONSTANTY (NUCLEAR CONSTANTS 3, 1990) (Original Report in Russian was distributed as INDC(CCP)-328/G) Translated by A. Lorenz for the International Atomic Energy Agency July 1991 IAEA NUCLEAR DATA SECTION, WAG RAMERSTRASSE 5, A-1400 VIENNA INDC(CCP)-335 Distr.: L TRANSLATION OF SELECTED PAPERS PUBLISHED IN YADERNYE KONSTANTY (NUCLEAR CONSTANTS 3, 1990) (Original Report in Russian was distributed as INDC(CCP)-328/G) Translated by A. Lorenz for the International Atomic Energy Agency July 1991 Reproduced by the IAEA in Austria August 1991 91-03116 Contents The Total Neutron Cross-section and Resonance Parameters for the Even 58,60,62,64^ isotopes for Energies Ranging from 2eV to 8000eV (Pages 27-38 of Original) By L.L. Litvinskij, P.N. Vorona, V.G. Krivenko, V.A. Libtnan, A.V. Murzin, G.N. Novosselov, N.A. Trofimova, O.L. Tchervonnaya The 54Fe(n,a)51Cr Thermal Neutron Reaction Cross-section (Pages 39-43 of Original) By S.P. Makarov, G.A. Pik-Pitchak, Yu.F. Rodionov, V.V. Khmyzov, Yu.A. Yashin 19 Isotopic Dependence of Radiative Capture Cross-sections for 30 keV Neutrons (Pages 44-52 of Original) By Yu. N. Trof imov 25 Evaluation of Particle Emission Spectra for Isotopes of Chromium, Iron and Nickel for the BROND Data Library (Pages 53-66 of Original) By A.V. Zelenetskij , A.B. Pashchenko 33 Comparison of Measured and Calculated Cross-sections of a Large Number of Nuclides (Pages 67-79 of Original) By A.V.