Research Reactor Utilization

Total Page:16

File Type:pdf, Size:1020Kb

Research Reactor Utilization ATOMIC EEttEY AGEECY STUDY GROUP oar KSSSARCII RSACTOR UTILIZATION -."Casa'ccia, Italy, 2-6 February 19?0 PRODUCTION 01? RAJDIOISOTOSCS IK RESEARCH REACTORS V.V. Bochkarev, V.i. Levin Radioactive isotope producee sar researcn di h reactorr sfo nearly a quarter of a centurjr* Is addition to the increase in number of these reactors their geographic location has been rapid- ly expanded* At present in the whole world we count already several hundreds of research reactors, many of them having neutron from'1012 to 5-10*15 c/cm2.scc. The proble researcf mo h reacto productioe th r usr efo f no radioisotopes and labelled compounds is therefore of much signi- ficance especially as related to short-lived isotopes and to medi- cal preparations of these isotopes primarily for countries and areas remoted from the main v/orld centers of isotope production* Recently many countries have commenced isotope production, organi- sing isotope radio chemi-cal laboratorie theit sa r research reactors Production of isotopes in research reactors (as a rule being mul- tipurpose) however is not -she only task of these facilities and even usually not the forst one. Taking account of all said above IAEA already in November 1962 held a seminar on short-lived isotopes production in small research reactors and their use. In 1966 IAEA, published a special manua isotopn lo e production (Manua Radioisotopf lo e Production, Technical Reports, Serie s6J)N whicn , i basi e hth c aspectf so this problem arc discussed* Radioisotope productio researcn ni h reactor mans sha y diffe- rent aspects whicf o l h ,al canno discussee tb singla n di e paper* 243 However, some "basic aspects might be difined and illustrated by examples* In the p^eofcnt paper we do not consider purely engineering problems connected with desig maintenancd nan variouf eo s auxi- liary loadin unloading- g (and other) devices. These problems requir separatea e discussio probleme welth s n a s la s o« protecti\ boxes and othor specific equipment used in further procesci^s of irradiated materials* considet no V.'o d e r method technologd san productionf yo , control and certification of labelld compounds and specific pr*;?:-- rations with radioactive compound thess sa independene ear t prob- lems. V/o concentrate our attention on the very process of isotope production in research reactors. generan I l nearl radioisotopel yal producee b n a sca n di nuclear reactor although productio neutron-deficienf no t ivaclides requires the bombardment of initial targets v/ith charged particles This procedur raann ei y more caseb en sca effectivel y performed acceleratorf o e us e bcyclotronthaa l yth firsd f al ts o an f to * Altogc-cher 1500 raaioisotopes are know, out of them for regular productio availabls ni mort eno e than 155-14-0 oneo- ,in cluding abou p~educe0 t10 nuclean di r reactors obvious i t .I o that the choice of isotopes for production is determined by locc.1 r.oeds and its operation program. In addition it should be notec. that out of the great number of reactor isotopes the folio-wins 25 may be asevii"l '~ to the cost widely used in industry, agricul- ture, biology and. medicine /except the transuranium elements/1 1 52 35 42 *B, *0, «fc, P, S, K, *5Ca, 51Cr, 55*,, 244 652n, icierejf o Besids s i noto t tt si e a. grou short-:f po . tvcd isotopeo use therapn di y a&i dia&ioctic 'T?s( , '''c^, 'yfl'ic, , 1*1, Wat) and in other fields C28^, " main propsrtieo of fcb.e a'oove isotope & are presented in Sables 1b d l.aan 2h.es groupo tw e s aal:e up A-0 pe- rl isotope cenal f to s i:ore or less regularly produced in nuclear reactors. By their pro- duction volune (total activity, cost, the numb a r of supplies; an dassortneAe alsth y ob compoundf to sourced san s they probably exceed 98 per cei.t of the total production* Ail these isotopes can bo produced in research reactors of medium povre productiot rbu oojsf no theif o e a (tritium^ corbon-14, long-lived isotope fissioa f so n product group and. cobalt-60n )i these conditions is practically unreasonable. The general schema of radioa.ctive isotope production in a reactor consists of 5 n&li. stages. 1. The choice of a suitable target snd its irradiation conditions* Targ. 2 e v preparatio irradiatiod nan n i reactor£a . 3* Processing of the irradiated target and production of necessara y compound or drug. 4. Analysis, measuremen necessarf i d tan ybiologicaa l con- trol and certification of a ready-aade product. 5* Packin deliveryr gfo * 245 considee w w Ho r sbiae question relation si tho nt e firso ttw thstageo t e d primarsan y processin irradiatef go d targets* Sine target choice« 2he choice of initial chemical materials - targets for irradiation, plays an important role in the whole matter of isotope production* 3te initial materials should meet Many serious and often contradictory requirements* .She first one is quite certain irradiatio wf no e targe reactoa n ti r shoul2 d0 safe* Vhe second requirement is related to the rational choice of a type Of irradiated naterial f^on the point of view of obtaining an optimum yield and specific activity of the necessary isotope; third is related - to the production of necessary isotopes wi'sl sh radioisotpic purity choice th £ort e o e;t th hof- . necessary isotopes from the point of view of convenience o.f further proces- sin irradiatef go d material (separatio necessara f no y isotope frotargee mth direcr to t pi-oa-.ctici labellea f io d compound). As for the second requiresent, i.e. effective use of neutron fluxe exposurd san e tim o"stainind ean g larger isotope yields, it eight appear that irradiation «.£ necessary material in an ele- mentar fore th ym n fori ol r amostlo y compact compounds wite hth maximum content of the principal, elexent is of greater advantage* But the fourth requirement (prccarcing of the target) forces one to reject such.choice and to us» suitable compounds even at the expense of significant vrorsenirg in the utilisation of the useful volume in a reactor* She third .requirement (radioisotopic purity of the product) is usually settled by compromise in relation to other conditions tar satisfo et y tris requiremen rula s s eti a very difficult* 246 generan I propee lth r target choic achievo et necessae eth - ry specific activity in the irradiation and to obtain the least quantit radioisotopif yo c impuritie connectes si d ttit nocace hth - sity to consider nany factors and essentially depends on the irra- .diation conditions. If we consider only tie simplest v/ay of isotope production by neutron capture reaction than v/e should distinguish at Itast three source radioisotopif so c impurities: radioactive impurities by activation of other chemical elements contained in the irra- diated material, formatio differenf no t radioactive isotopef so the principal element and, ilnally formatio othef no r radioactive isotopes by paralell and secondary processes in isotope activatioi in a nuclear reactor. Naturally the materials to be irradiated should be of grea- test chemical purity and chemical compounds selected for target preparation should introduc lease th et quantity of. radioactive, at any rate - long-lived impurities into the principal radioioo- tope. Certainly, often it is possible to eliminate radioactive impurities of other ic-otopes by radiocheraical methods but thic procedur mors ei e difficul sometimed tan s even practically it^js- feible wit isotopee hth same th e f selemento * Therefore radioiso- topic futurpurite th f eyo radioactive product shoul providee db d for beforhand, These questions v.'il discussee lb mora n edi detailed Torn considerinn i processee gth targef so t irradiatio reactora n ni * Isotope,production ways* Of practical value for isotope productio followine th e nar g nuclear reactions excite neuty db - reactorr^',a n 3i : 247 1« C&tV - reactio) n c£ 'radio. iiv$ sout^on capture C-* c-iccci.w/ capture of two aud xacre aotttrossu* 2» (n,1^ ) v.'ith subsequent isotope de.cay leading ti v';.c- formation of secondary radioactive product* 3* Eeac-cicns -.7ifti charged particles cr^issios:: (n, %) cr«i Cnsct ) and (n, 2^:} rd&ction* 4, Secondary reactions (t, r;) ;^-:d (t, n) v/ith taltcns fo;r:'.c~ ^ by neutron reaction cX;i(*i.,ol), and clso :-;->cc:idAr7 -.vitii roccil protons jrciousec «i'rc.di&.-;:in i . c i:yf :o d rials \vith i'sct re&ctor noutrons. $* Mission rcacticn ln,-y }* A nors deudlsd di.scv.ssio.-. ^cilc;7o. fi;otopc G of She noct part oi' v?:.3.v.s-.ts be oouained "by VR,^) reactic-i. 2ho yields cf this se^ct*c>i; uav al- decreasy l e v/ith tlae iricr.-;aso ou* aa'a^rML inersy* Irradiation of tho target- therefors ?i e performe reacton di r channoie *./itn prc- do^inatic thermaf ao l neuvrons* In cUoooinc irradiation conditions oosides activation croi<s - sectio «h.f no c initial i^vtop necessars i t ei consideo yt r u number of other factors SMo activates aa d i&otope abundance, isotopic and non-isotopic impurities in the tsr^et, half~livos thf o e radioacvivo product ,^.;acr production anini-;^i"iieas ait , foraation cross-section lattee th f sro an;L cross-section o^ r-sut- ron captur radioactive th y eb e pi--auct» Irraaiatior.
Recommended publications
  • Specification for Low Alpha Lead in Wafer Bump Applications
    Application Notes 47 Molter Street Cranston, Rhode Island 02910-1032 401-781-6100 • [email protected] • www.technic.com Specification for Low Alpha Lead in Wafer Bump Applications Background Alpha particles are positively charged nuclear particles consisting of two protons bound to two neutrons. Alpha particles are emitted spontaneously in some types of radioactive decay. Although alpha particle emissions are capable of penetrating only short distances, they are pernicious in creating computer memory or logic faults known as “soft faults”. Soft faults are individual events that are difficult to detect and isolate. Intel engineers working with IBM Fishkill, NY first identified the problem in 1979. The C-DIP’s (ceramic package DRAM) of that era were plated with gold and the alpha emissions were traced to the gold plated kovar package lids. Uranium or thorium decay and generate alpha particles with energies as high as 8.78 MeV. A flux of 5 MeV is capable of penetrating 25 um of silicon, resulting in 1.4 M electron hole pairs. If the electron accumulation exceeds a specific charge depending on the operating voltage and well design of the device, the cell may switch from “1” to “0”. There is no permanent damage and therefore the defect is referred to as a “soft” error. Design projections indicate that as device voltages decrease their sensitivity to alpha emissions increases. Alpha emissions are also common from tin lead deposited in the form of bumps for flip chip applications. The potential is significant for tin lead bumps due to the number of bumps and their close proximity to the sensitive IC well structure.
    [Show full text]
  • (RAPID) Method to Nuclear Materials
    University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 5-2020 Development and Applications of the Rapid Analysis of Post- Irradiation Debris (RAPID) Method to Nuclear Materials Emilie Fenske University of Tennessee, [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Recommended Citation Fenske, Emilie, "Development and Applications of the Rapid Analysis of Post-Irradiation Debris (RAPID) Method to Nuclear Materials. " PhD diss., University of Tennessee, 2020. https://trace.tennessee.edu/utk_graddiss/5883 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Emilie Fenske entitled "Development and Applications of the Rapid Analysis of Post-Irradiation Debris (RAPID) Method to Nuclear Materials." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Nuclear Engineering. Howard Hall, Major Professor We have read this dissertation and recommend its acceptance: Steven Skutnik, Alan Icenhour, Robert Counce, Benjamin Roach, Cole Hexel Accepted for the Council: Dixie L. Thompson Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Development and Applications of the Rapid Analysis of Post-Irradiation Debris (RAPID) Method to Nuclear Materials A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville Emilie Fenske May 2020 Copyright © 2020 by Emilie Kiersten Fenske All rights reserved.
    [Show full text]
  • Thesis Front Matter
    Research Report on Development of analytical strategies to measure radioisotopes of tin in the environment Prepared by Mohammad Majibur Rahman Graduate Program (PhD) Supervisor: Dr. Ian Clark Co-supervisor: Dr. Liam Kieser Earth and Environmental Sciences: Specialization in Chemical and Environmental Toxicology Submitted to The Office of Graduate and Postdoctoral Studies Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Earth and Environmental Sciences: Specialization in Chemical and Environmental Toxicology DECEMBER 13, 2018 © Mohammad Majibur Rahman, Ottawa, Canada, 2018 This page has intentionally been left blank. Abstract Quantification of tin isotopes in environmental samples, particularly the radioactive 126Sn, is important for processes such as the biomonitoring of organotin species, long-term nuclear waste storage and treatment planning. The detection of 126Sn by mass spectrometric methods is, however, hampered by the presence of the stable 126Te isotope. Therefore, separation of tin from tellurium is crucial to minimize isobaric interferences that limit the quantification of 126Sn by Accelerator Mass Spectrometry (AMS) and other instrumental techniques. In the present study, three major accomplishments are discussed: i) development of an analytical strategy to separate tin from tellurium, ii) monitoring of anionic interferences in the separation of tin from tellurium, and iii) suppression of 126Te background to allow the detection of 126Sn by AMS. Section I (Chapter 2): In the first phase of the project, an analytical survey was carried out using four Eichrom resins (TRU, TEVA, UTEVA, and DGA) to identify a suitable solid phase chromatographic material to separate tin from tellurium. Standard metal solutions were spiked on batch tests in two acids (HCl and HNO3) at concentrations ranging from 0.20 to 6.0 mol L–1, and the spiked analytes in solution were measured by ICP-MS.
    [Show full text]
  • Arxiv:1006.4033V2 [Nucl-Ex] 8 Sep 2010
    Discovery of Calcium, Indium, Tin, and Platinum Isotopes S. Amos, J. L. Gross, M. Thoennessen∗ National Superconducting Cyclotron Laboratory and Department of Physics and Astronomy, Michigan State University, East Lansing, MI 48824, USA Abstract Currently, twenty-four calcium, thirty-eight indium, thirty-eight tin and thirty-nine platinum isotopes have been observed and the discovery of these isotopes is discussed here. For each isotope a brief synopsis of the first refereed publication, including the production and identification method, is presented. arXiv:1006.4033v2 [nucl-ex] 8 Sep 2010 ∗Corresponding author. Email address: [email protected] (M. Thoennessen) Preprint submitted to Atomic Data and Nuclear Data Tables November 1, 2018 Contents 1. Introduction . 4 2. Discovery of 35−58Ca ................................................................................... 5 2.1. 36Ca ............................................................................................ 5 2.2. 37Ca ............................................................................................ 7 2.3. 38Ca ............................................................................................ 7 2.4. 39Ca ............................................................................................ 7 2.5. 40Ca ............................................................................................ 7 2.6. 41Ca ............................................................................................ 8 2.7. 42;43Ca .........................................................................................
    [Show full text]
  • Arxiv:2006.05774V1 [Nucl-Ex] 10 Jun 2020 Bevddi Observed Aoaois Hl Ie,Cnd 0 1P0 K0J Canada River, Chalk Laboratories, Keywords: Pairs
    Systematic reduction of the proton-removal cross section in neutron-rich medium-mass nuclei J. D´ıaz-Cort´esa, J. Benlliurea, J.L. Rodr´ıguez-S´ancheza, H. Alvarez-Pol´ a, T. Aumannb, C.A. Bertulanic, B. Blankd, E. Casarejosa,1, D. Cortina-Gila, D. Dragosavaca, V. F¨ohre, A. Garganof, M. Gasc´ona, W. Gawlikowiczh, A. Heinzi, K. Helariuttaj, A. Keli´c-Heile, S. Luki´ce, F. Montese,2, D. P´erez-Loureiroa,3, L. Pie´nkowskig, K-H. Schmidte, M. Stanioue, K. Suboti´ck, K. S¨ummerere, J. Taiebl, A. Trzci´nskag aIGFAE, Universidade de Santiago de Compostela, E-15782 Spain bInstitut f¨ur Kernphysik, Technische Universit¨at Darmstadt, 64289 Darmstadt, Germany cTexas A&M University-Commerce, 75428 Commerce, Texas, United States of America dCentre d’Etudes Nucleaires, F-33175 Bordeaux-Gradignan Cedex, France eGSI Helmholtzzentrum f¨ur Schwerionenforschung, D-64291 Darmstadt, Germany fIstituto Nazionale di Fisica Nucleare, Complesso Universitario di Monte S. Angelo, Via Cintia, I-80126 Napoli, Italy gHeavy Ion Laboratory, University of Warsaw, PL-02-093 Warsaw, Poland hCardinal Stefan Wyszynski University, PL-01-938 Warsaw, Poland iChalmers University of Technology, SE-41296 Gothenburg, Sweden jUniversity of Helsinki, FI-00014 Helsinki, Finland kInstitute of Nuclear Sciences Vinˇca, University of Belgrade, 11001 Belgrade, Serbia lCEA, DAM, DIF F-91297 Arpajon, France Abstract Single neutron- and proton-removal cross sections have been systematically measured for 72 medium-mass neutron- rich nuclei around Z=50 and energies around 900A MeV using the FRagment Separator (FRS) at GSI. Neutron- removal cross sections are described by considering the knock-out process together with initial- and final-state inter- actions.
    [Show full text]
  • Radiation Therapy and Dosing Material Transport Methodology Robert O'brien University of Nevada, Las Vegas, [email protected]
    UNLV Theses, Dissertations, Professional Papers, and Capstones 12-1-2016 Radiation Therapy and Dosing Material Transport Methodology Robert O'brien University of Nevada, Las Vegas, [email protected] Follow this and additional works at: https://digitalscholarship.unlv.edu/thesesdissertations Part of the Biomechanical Engineering Commons, Biomedical Commons, and the Biomedical Devices and Instrumentation Commons Repository Citation O'brien, Robert, "Radiation Therapy and Dosing Material Transport Methodology" (2016). UNLV Theses, Dissertations, Professional Papers, and Capstones. 2891. https://digitalscholarship.unlv.edu/thesesdissertations/2891 This Dissertation is brought to you for free and open access by Digital Scholarship@UNLV. It has been accepted for inclusion in UNLV Theses, Dissertations, Professional Papers, and Capstones by an authorized administrator of Digital Scholarship@UNLV. For more information, please contact [email protected]. RADIATION THERAPY AND DOSING MATERIAL TRANSPORT METHODOLOGY By Robert James O’Brien Master of Science, Materials and Nuclear Engineering University of Nevada, Las Vegas 2006 Bachelor of Science, Mechanical Engineering University of Nevada, Las Vegas 2005 Bachelor of Science, Applied Physics University of Nevada, Las Vegas 2005 A dissertation submitted in partial fulfillment of the requirements for the Doctor of Philosophy in Engineering – Mechanical Engineering Department of Mechanical Engineering Howard R. Hughes College of Engineering The Graduate College University of Nevada, Las Vegas December 2016 Copyright by Robert O’Brien, 2017 All Rights Reserved Dissertation Approval The Graduate College The University of Nevada, Las Vegas November 16, 2016 This dissertation prepared by Robert James O’Brien entitled Radiation Therapy and Dosing Material Transport Methodology is approved in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Engineering – Mechanical Engineering Department of Mechanical Engineering William Culbreth, Ph.D.
    [Show full text]
  • A New Method of Pure 111In Production by Proton-Induced Nuclear Reactions with Enriched 112Sn 19 Consequently with Low Activity)
    NUKLEONIKA 2007;52(1):17−27 ORIGINAL PAPER 111 A new method of pure In production Emil Bìták, Edward Rurarz, by proton-induced nuclear reactions Stefan Mikołajewski, with enriched 112Sn Jolanta Wojtkowska Abstract. We aimed at finding out a simple and reliable way of 111In production with the highest radionuclide purity from its grand parent 111Sb and parent 111Sn nuclei, produced by the 112Sn(p,2n)111Sb and 112Sn(p,pn)111Sn reactions, respectively. The target was a metallic 112Sn sample enriched to 84%. We have measured activation cross sections for seven reactions on an enriched 112Sn sample induced by 23.6 ± 0.8 MeV energy protons. Gamma-ray spectroscopy with 55 60 high-purity germanium detectors has been used. We also identified the activities of Co (T1/2 = 17.5 h) and Cu (T1/2 = 23.7 min) in proton beam monitoring Ni foils, induced in the natNi(p,X)55Co and natNi(p,X)60Cu reactions at 22.8 MeV proton energy. The cross sections determined for these reactions are: σ[natNi(p,X)55Co] = 36.6 ± 4 mb and σ[natNi(p,X)60Cu] = 64.4 ± 7 mb. The measured cross sections of reactions on tin isotopes are: σ[112Sn(p,n)112Sb] = 4 ± 0.8 mb; σ[112Sn(p,2n)111Sb] = 182 ± 26 mb; σ[112Sn(p,pn)111Sn] = 307 ± 35 mb; σ[114Sn(p,2n)113Sb] = 442 ± 52 mb; σ[117Sn(p,n)117Sb] = 15 ± 3 mb; σ[117Sn(p,p’γ)117mSn] = 0.37 ± 0.06 mb; σ[115Sn(p,2p)114m2In] = 0.01 ± 0.002 mb.
    [Show full text]
  • Stdin (Ditroff)
    50Ma02 The Hyper®ne Structure of the Stable Isotopes of Indium A. K. Mann, P. Kusch, Phys. Rev. 77, 427 (1950). 50Ma03 The Beta-Spectrum of Ca45 P. Macklin, L. Feldman, L. Lidofsky, C. S. Wu, Phys. Rev. 77, 137 (1950). 50Ma05 Study of Neodymium and Promethium Activities Induced by Neutron Irradiation of Neodymium J. A. Marinsky, L. E. Glendenin, NNES 9, 1264 (1950). 50Ma14 New Isotope of Neptunium L. B. Magnusson, S. G. Thompson, G. T. Seaborg, Phys. Rev. 78, 363 (1950). 50Ma15 The Fission Yield of Xe133 and Fine Structure in the Mass Yield Curve J. Macnamara, C. B. Collins, H. G. Thode, Phys. Rev. 78, 129(1950). 50Ma27 D. G. E. Martin, H. O. W. Richardson, Proc. Phys. Soc. (London) 63A, 223 (1950). 50Ma29 Neutron De®cient Isotopes of Iodine L. Marquez, I. Perlman, Phys. Rev. 78, 189 (1950). 50Ma50 A Table of Nuclear Moments, January 1950 J. E. Mack, Revs. Modern Phys. 22, 64 (1950). 50Ma65 R. Malm, W. W. Buechner, Phys. Rev. 80, 771 (1950). 50Ma76 The Natural Radioactivity of In115 E. A. Martell, W. F. Libby, Phys. Rev. 80, 977 (1950). 50Mc12 Radiation from Au197*(7x10-9 sec) F. K. McGowan, Phys. Rev. 78, 325A (1950). 50Mc22 Short-Lived Isomers F. K. McGowan, ORNL-694, p. 19 (1950). 50Mc60 A 5.7 x 10-9 sec Isomeric State in Ir191 F. K. McGowan, Phys. Rev. 79, 404 (1950). 50Mc64 A3x10-9 sec. Isomeric State in Eu153 F. K. McGowan, Phys. Rev. 80, 482 (1950). 50Mc79 A 1.7 x 10-9 sec Isomeric State in Er166 F.
    [Show full text]
  • Stable Isotope Separation in Calutrons
    Printed ill tho llnitzd Statss ot 4mcm 4vailsble frurii Nations' Technical Information Service U S :3ep?rtmelli uf Commerce 5285 Port 4oyal Cosd Spririizflald Viryinis 22161 NTlS ptwiodes P~III~~Copy ,498, Microfiche P,C1 I his rcpoti \*!is prspxed as an account of >,dSi-k sponsored by a3 agsncy of the United Sraies Governr;,ent. Neither thc !J nited Skiics i<n.~cti $IK~: nor any agency th2reof. no? any of thzir employoes, (ciakc?.Aijy ivarranty, express or irripiled, or assunias any legal liability or responsibility for ihe accuracy. compleienass, or usefulness of any inforriraiton. ;p ius, product, or process disclosed, or represents that its usewould not infr privately o-v?d ilghts Rcferencc herein to ai-y specific commercial product, process, or service by trade nziile, Zi'adei*lark, manufacturer, or otherwise, does not necsssarily constitute or imply its enduisemcat, recorn,n faVOiii-,g by ille United States(;ovc;riiiie!ii 01- any Zgency thereof Th opinions of auiihols cxp:essed here:!: d~ ~iui neccssarily statc or refisc?!host of the United Sta?ezGovernmer:?or any ngcncy therccf. ____ ___________... ..... .____ ORNL/TM-10356 OPERATIONS DIVISION STABLE ISOTOPE SEPARATION IN CALUTRONS: FORTY YEARS OF PRODUCTION AND DISTRIBUTION W. A. Bell J. G. Tracy Date Published: November 1987 Prepared by the OAK RIDGE NATIONAL LABORATORY Oak Ridge, Tennessee 37831 operated by MARTIN MARIETTA ENERGY SYSTEMS, INC. for the U.S. DEPARTMENT OF ENERGY under Contract No. DE-AC05-840R21400 iti CONTENTS Page ACKNOWLEDGMENTS ................................................. iv I. INTRODUCTION .............................................. 1 11. PROGRAM EVOLUTION ......................................... 1 111. RESEARCH AND DEVELOPMENT .................................. 5 IV. CHEMISTRY ................................................. 8 V.
    [Show full text]
  • Francis W. Aston
    FRANCIS W. A STON Mass spectra and isotopes Nobel Lecture, December 12, 1922 Dalton’s statement of the Atomic Theory, which has been of such incalcu- lable value in the development of chemistry, contained the postulate that "atoms of the same element are similar to one another, and equal in weight". The second part of this postulate cannot, in general, be tested by chemical methods, for numerical ratios are only to be obtained in such methods by the use of quantities of the element containing countless myriads of atoms. At the same time it is somewhat surprising, when we consider the complete absence of positive evidence in its support, that no theoretical doubts were publicly expressed until late in the nineteenth century. There are two methods by which the postulate can be tested experi- mentally, either by comparing the weights of the individual atoms, or al- ternatively by demonstrating that samples of an element can exist which though chemically identical yet have different atomic weights. The latter method, by which the existence of isotopes was first proved, has been fully dealt with in the previous lecture by Professor Soddy. The more direct method, with which this lecture is concerned, can be applied by means of the analysis of positive rays. The condition for the development of these rays is briefly ionization at low pressure in a strong electric field. Ionization, which may be due to col- lisions or radiation, means in its simplest case the detachment of one electron from a neutral atom. The two resulting fragments carry charges of electricity of equal quantity but of opposite sign.
    [Show full text]
  • The Radiochemistry of Indium
    E958r i C.9.. National Academy v“ of Sciences 1National Research Council NUCLEAR SCIENCE SERIES The Radiochemistry of Iridium 3“#L7 :, ,fy% COMMITTEE ON NUCLEAR SCIENCE L.F.CUR~, Chafrman ROBLEY D.EVANS,ViceChuirmun NationalBureauofStadarde MaeeachueetteInetituteofTechnology J.A.DeJUREN,Secretury WeMnghouee ElectricCorporation H.J.CURTIS W. WAYNE MEINKE BrookhavenNationalLaboratog UniversityofMichigan SAMUEL EPSTELN ROBERT L.PLAT ZMAN Callforn.laInetItuteofTechuol~ ArgonoeNationalLeboratmg HERBERT GOLDSTEIN A. H.SNELL NwlearDevelopmentCorporationof Of&RidgeNationalLaboratory America E.A.UEHLING H.JoGOMBERG Unlveret@ofWaehlngton UnlvereltyofMlcldgan D.M. VAN PATTER E.D.KLEMA BartolReeearchFoundation NorthweetarnUniveretty G.G.MANOV Tmcerleb,Inc. LIAISON MEMBERS PAUL C.AEBERSOLD W. D.URRY AtomicEne~ Commieaion U.S.AlrForce J.HOWARD MaMILLEN WILLIAM E.WRIGHT NationalscienceFoudatkon OfficeofNavalReseamh SUBCOMMIllEE ON RADIOCHEMISTRY W. WAYNE MEINKE,Chutrwaam HAROLD SURBY UnlvereityofMichtsan MoundLahoretory GREGORY R.CHOPPIN GEORGE LEDDICOTTE FlorklaStateUnlvereity OakRidgeNationalLaboratory GEORGE A.COWAN JULIAN NTELSEN LoeAlamoeSckmtlflcLaboratog Hanfod Lahoratoriee ARTHUR W. FAIRHALL ELLISP.STEINBERG UnlvereltyofWashington ArgonneNationalLaboratory JEROME HUDIS PETER C.STEVENSON Brddmven NationalLaboratory UniversityofCaltfornta(Llvemore) EARL HYDE LEO YAFFE UnlvereltyofCalifornia(Bgrkeley) McGU1 Unlvereity CONSULTANTS NATHAN BALLOU WILLIAM MARLOW Naval~iologlcalDefeneeLaboratory NationalBureauofStandamie JAMES DeVOE UntveieityofMhhigan
    [Show full text]
  • Tail As the .:J:J Ref~ Ax; ¥10 'T:"-T Dfgtj..Tl ~ ,..U~ [.!Lt·V
    Anomalies in the Fermi Effect • ... be conbi~e~,.CL bjvsome as equally probable, or even more ~:Sa"b ~ s tfi:aR the fixst=aite"!'f'l'autive •. While we "ffhal.l ~ 4 ~ a.~.a,.fyf---c __.,. emphasize the pas si bili ty o 4his eeeond vie'fvj~we will · t.A----~ . (J ¢::6 d.t"ia: -; ~~.... ~. ,,-..A( ~ not discuss £? in ~ etail as the .:j:j rEf~ ax; ¥10 't:"-t dfGtJ..tL ~ ,..u~ [.!lt·v ...... ~YJ ~- ~. r/ ~ This unequal treatment is not due to a biased opinion in . ~,.,,,~ . ~ !-'. ' 'M·•/. favour of one of e ·· ' views, and seems -t;o-..b€ just'fied (/~A rt• f.-# £r.~- .-/ ~ e.e i.o I~,_,_ "-!- H . .t:/ ,d"~ t~t .vrlk t.~ 1 ~-.. a : . , . - · by t h e fact that the f1Fst VJ:ew- leads \ to a number of p otentially pas si ble ~l r ( • (-(;;-- -~~ "1:1 /experiments wnich may decide / 3:-rr~~~ , ·o-: a ~ n. ~ , I~ - "/Z,_ - /t , .y /I(, " ,. /.. ' . .... I /7<Vt.. (,_.1' ~~ whereas it se5!ms to be diffipul t to think of cn ~. t'- ,.. (, ...... 1 #t.r t~- ....-.~..., "'<../ t<t.,.-< ""'"' t t( /'l'n J ( "t·C experiments,. ~t'O a:mc t · decision o·n-~ a - - - "' ANOMALIB.S IN TilE FERMI EFFECT 1) Amaldi, D'Agostino and Segre have found that neutrons Which have been slowed down by paraffin wax induce in indium two radio­ active half-life periods (16 eea. and 54 min.). T.A. Cha~ers and 2) I have subsequently reported that indium can also be comparatively strongly activated with a third period of several hours if irradiated by neutrons from a radon alpha-particle beryllium source in the ab- sence of hydrogen-containing substances, and we raised the question whether its existence can be satisfactorily explained without a new assumption.
    [Show full text]