Mass Fractionation and the Isotopic Anomalies of Xenon and Krypton in Ordinary Chondrites

Total Page:16

File Type:pdf, Size:1020Kb

Mass Fractionation and the Isotopic Anomalies of Xenon and Krypton in Ordinary Chondrites und gravimetrischen 24: Stimmung der Ergebnisse macht deutlich, daß früher für 25 °C veröffentlichte Werte von 10~9 oder gar Z)n = 1,0-10~6 cm2 s_1 10~20 cm2 s-1 auf den Einfluß von Grenzflächen- Messungen mit leichtem Wasserstoff. Sowohl die reaktionen zurückzuführen sind. Messungen mit Tritium als auch die röntgenogra- phischen und gravimetrischen Methoden sind von Herrn Prof. Dr. E. WICKE möchten wir an dieser Durchtrittshemmungen unabhängig. Die Überein- Stelle für wertvolle Hinweise und anregende Diskus- sionen herzlich danken. — Der Deutschen Forschungs- 24 E. WICKE U. A. OBERMANN, Z. Physik. Chem. N.F. (im gemeinschaft danken wir für die Unterstützung unserer Drude). — A. OBERMANN, Diplomarbeit, Münster 1970. Arbeit mit Personal- und Sachmitteln. Mass Fractionation and the Isotopic Anomalies of Xenon and Krypton in Ordinary Chondrites E. W. HENNECKE and 0. K. MANUEL Department of Chemistry, Universiy of Missouri, Rolla, Missouri (USA) (Z. Naturforsch. 26 a, 1980—1986 [1971] ; received 7 August 1971) The abundance and isotopic composition of all noble gases are reported in the Wellman chon- drite, and the abundance and isotopic composition of xenon and krypton are reported in the gases released by stepwise heating of the Tell and Scurry chondrites. Major changes in the isotopic com- position of Xe result from radiogenic Xe129 and from variations in the isotopic mass fractionation pattern in the different temperature fractions. The isotopic composition of trapped krypton in the different temperature fractions of the Tell and Scurry chondrites displays smaller fractional changes than xenon, but the isotopic composition of these two gases covary in the manner expected from mass dependent fractionation. Many clues of early geologic events have been noted that a comparison of the earth's inventory of recorded in the stable noble gases, He, Ne, Ar, Kr noble gases with the solar abundances of these ele- and Xe. The chemical inertness and volatile nature, ments shows preferential loss from terrestrial mate- even at relatively low temperatures, resulted in al- rial of the gases lighter than krypton. Subsequent most complete loss of these elements from more work on noble gases in terrestrial sediments 3 found condensable material when solid planetary matter high concentrations of xenon which, when added to formed in our solar system. Many isotopic anoma- the atmospheric inventory of noble gases, show that lies of these elements have been generated in solid the earth's fractionation of noble gases extends to planetary material subsequent to this separation, by the heaviest stable gas, xenon. The trapped noble induced nuclear reactions and by natural radio- gases in stone meteorites display a similar fractio- active decay of more abundant elements. nation pattern 4' 5 with the xenon preferentially re- Although the generation of isotopic anomalies of tained over neon by a factor 104 — 105. all the stable noble gases by nuclear processes is SIGNER and SUESS 6 discussed the role of mass well documented, there is also evidence for the pro- fractionation in generating isotopic anomalies of duction of isotopic anomalies of noble gases by neon and argon in planetary material. They noted simple isotopic masä fractionation at the time of a covariance of Ar36/Ar38, Ne20/Ne22 and Ne20/Ar36 the separation of these from more condensable ele- ratios in atmospheric and meteoritic gases. MA- ments. In 1949 SUESS 1 and BROWN 2 independently NUEL 7 reported variations in the trapped Ne20/Ne22 Reprint requests to Prof. Dr. O. K. MANUEL, Department 4 J. H. REYNOLDS, Phys. Rev. Letters 4, 351 [1960]. of Chemistry, University of Missouri-Rolla, Rolla/Missouri 5 O. K. MANUEL and M. W. ROWE, Geochim. Cosmochim. 65401, USA. Acta 28. 1999 [1964]. 1 H. E. SUESS, J. Geol. 57, 600 [1949], 6 P. SIGNER and H. E. SUESS. in: Earth Science and Meteo- 2 H. BROWN, The Atmosphere of the Earth and the Planets, rites, North-Holland Publ. Co., Amsterdam 1963. University of Chicago Press, Chicago 1949. 7 O. K. MANUEL, Geochim. Cosmochim. Acta 31, 2413 [1967]. 3 R. A. CANALAS, E. C. ALEXANDER, JR., and O. K. MANUEL, J. Geophys. Res. 73, 3331 [1968]. and Ne21/Ne22 ratios in the different temperature der to obtain additional data with which to examine fractions of the Fayetteville meteorite and suggested the current framework of ideas on the origin of that these variations result from isotopic mass frac- noble gas anomalies in meteorites. Samples of three tionation. However, PEPIN and coworkers8-10 re- ordinary chondrites were used for this investigation. ported that there is no sign that diffusive fractiona- tion is responsible for any of the isotopic variations Measurements of meteoritic neon. Recent results on the isotopic composition of trapped meteoritic He, Ne and Ar in Relatively large meteorite samples, weighing about the laboratories at Minnesota, Chicago and Rice 10 grams each, were used in this study. These were purchased from the American Meteorite Laboratory have been attributed to nuclear reactions 10 ~14, but (AML). The name and type of each meteorite, the 15-17 other authors have maintained that the ob- sample weight and the AML catalogue number of the served variations result from simple isotopic frac- specimen from which our samples were taken are as tionation. follows: The Wellman, Texas olivine bronzite chon- drite, 10.888 grams from specimen # H 12.56; the For the heavy noble gases, a similar divergence Tell, Texas olivinie hypersthene chondrite, 8.474 grams, of opinions has developed. SRINIVASAN et al.18 first from specimen #H 24.67; and the Scurry, Texas oli- suggested that spontaneous fission of superheavy vine bronzite chondrite, 7.909 grams, from specimen elements may be responsible for the enrichment of #H 65.25. heavy xenon isotopes in carbonaceous chondrites. The samples were mounted in side-arm chambers of a quartz extraction bottle. The samples were heated to ANDERS and HEYMANN 19 have arrived at a similar ~ 60 °C overnight to remove surface contamination, conclusion by comparing the excess heavy xenon the molybdenum crucible was degassed at 1800 °C and isotopes with the content of volatile elements in the pressure of the system reduced to 5 x 10-8 Torr. carbonaceous chondrites, and EBERHARDT et al. 20 The extraction bottle and preliminary "getters" were then isolated from the rest of the system by metal bel- have interpreted the isotopic composition of solar- lows valves, the sample to be analyzed was then drop- type xenon as evidence for large amounts of fissio- ped magnetically into the molybdenum crucible which genic xenon in carbonaceous chondrites. However, was heated by a radiofrequency induction heater. An KURODA and MANUEL 15 recently pointed out that optical pyrometer was used to estimate the extraction the enrichment of heavy xenon isotopes in carbon- temperatures. Each extraction temperature was main- tained for 30 minutes, and the evolved gases were aceous and gas-rich meteorites is paralleled by an cleaned in the extraction system by titanium at 850 °C enrichment of heavy neon isotopes. These authors and by copper-oxide at 550 °C. After these preliminary concluded that the enrichment of the heavier isoto- "getters" were cooled to room temperature, the gases pes of both gases result from isotopic mass fractio- were then pumped through the metal valve into a sec- ond clean-up system by adsorption on charcoal cooled nation. Additional evidence for the production of witl liquid N2 or solid C02 . After isolating the gases isotopic anomalies of meteoritic xenon and krypton in the second clean-up system, they were driven from by fractionation have been reported from noble gas the charcoal at 200 °C and exposed to a second surface analyses of the LEOVILLE 21 and POTTER22 chon- of titanium sponge at 850 °C. drites. In the case of Wellman, the noble gases were se- parated into four fractions for analysis by adsorption This study of the isotopic composition of noble on charcoal; the boiling temperature of N2 released gases in ordinary chondrites was undertaken in or- He and Ne, the sublimation temperature of C02 re- 8 R. 0. PEPIN, Earth Planet. Sei. Letters 2,13 [1967]. 17 B. SRINIVASAN and O. K. MANUEL, On the Isotopic Com- 9 R. 0. PEPIN, Origin and Distribution of the Elements, Per- position of Trapped Helium and Neon in Carbonaceous gamon Press, Oxford and New York 1968. Chondrites, Earth Planet. Sei. Letters, in press [1971]. 10 D. C. BLACK and R. 0. PEPIN, Earth Planet. Sei. Letters 6, 18 B. SRINIVASAN, E. C. ALEXANDER, JR., O. K. MANUEL, and 395 [1969]. D. E. TROUTNER, Phys. Rev. 179,1166 [1969]. 11 D. C. BLACK, Meteoritics 4, 260 [1969]. 19 E. ANDERS and D. HEYMANN, Science 164, 821 [1969]. 12 D. C. BLACK, Geochim. Cosmochim. Acta 34, 132 [1970]. 20 P. EBERHARDT, J. GEISS, H. GRAF, N. GRÖGLER, U. KRÄ- 13 E. ANDERS, D. HEYMANN, and E. MAZOR, Geochim. Cosmo- HENBÜHL, H. SCHWALLER, J. SCHWARZMÜLLER, and A. chim. Acta 34,127 [1970]. STETTLER, Geochim. Cosmochim. Acta Supp. 1, 2, 1037 14 E. MAZOR, D. HEYMANN, and E. ANDERS, Geochim. Cosmo- [1970]. chim. Acta 34, 781 [1970]. 21 O. K. MANUEL, R. J. WRIGHT, D. K. MILLER, and P. K. 15 P. K. KURODA and 0. K. MANUEL, Nature London 227, KURODA, J. Geophys. Res. 75, 5639 [1970]. 1113 [1970]. 22 O. K. MANUEL, D. K. MILLER, R. J. WRIGHT, and P. K. 16 0. K. MANUEL, Meteoritics 5, 207 [1970]. KURODA, Solar Type Krypton, submitted to J. Geophys. Res. [1971]. leased Ar, the freezing point of Hg released Kr, and analyses, where the identical procedures were followed finally the Xe was released from the charcoal at 150 °C. for gases evolved from a hot molybdenum crucible, For Tell and Scurry the noble gases were pumped into showed no significant contamination except at mass 78.
Recommended publications
  • Table 2.Iii.1. Fissionable Isotopes1
    FISSIONABLE ISOTOPES Charles P. Blair Last revised: 2012 “While several isotopes are theoretically fissionable, RANNSAD defines fissionable isotopes as either uranium-233 or 235; plutonium 238, 239, 240, 241, or 242, or Americium-241. See, Ackerman, Asal, Bale, Blair and Rethemeyer, Anatomizing Radiological and Nuclear Non-State Adversaries: Identifying the Adversary, p. 99-101, footnote #10, TABLE 2.III.1. FISSIONABLE ISOTOPES1 Isotope Availability Possible Fission Bare Critical Weapon-types mass2 Uranium-233 MEDIUM: DOE reportedly stores Gun-type or implosion-type 15 kg more than one metric ton of U- 233.3 Uranium-235 HIGH: As of 2007, 1700 metric Gun-type or implosion-type 50 kg tons of HEU existed globally, in both civilian and military stocks.4 Plutonium- HIGH: A separated global stock of Implosion 10 kg 238 plutonium, both civilian and military, of over 500 tons.5 Implosion 10 kg Plutonium- Produced in military and civilian 239 reactor fuels. Typically, reactor Plutonium- grade plutonium (RGP) consists Implosion 40 kg 240 of roughly 60 percent plutonium- Plutonium- 239, 25 percent plutonium-240, Implosion 10-13 kg nine percent plutonium-241, five 241 percent plutonium-242 and one Plutonium- percent plutonium-2386 (these Implosion 89 -100 kg 242 percentages are influenced by how long the fuel is irradiated in the reactor).7 1 This table is drawn, in part, from Charles P. Blair, “Jihadists and Nuclear Weapons,” in Gary A. Ackerman and Jeremy Tamsett, ed., Jihadists and Weapons of Mass Destruction: A Growing Threat (New York: Taylor and Francis, 2009), pp. 196-197. See also, David Albright N 2 “Bare critical mass” refers to the absence of an initiator or a reflector.
    [Show full text]
  • An Introduction to Isotopic Calculations John M
    An Introduction to Isotopic Calculations John M. Hayes ([email protected]) Woods Hole Oceanographic Institution, Woods Hole, MA 02543, USA, 30 September 2004 Abstract. These notes provide an introduction to: termed isotope effects. As a result of such effects, the • Methods for the expression of isotopic abundances, natural abundances of the stable isotopes of practically • Isotopic mass balances, and all elements involved in low-temperature geochemical • Isotope effects and their consequences in open and (< 200°C) and biological processes are not precisely con- closed systems. stant. Taking carbon as an example, the range of interest is roughly 0.00998 ≤ 13F ≤ 0.01121. Within that range, Notation. Absolute abundances of isotopes are com- differences as small as 0.00001 can provide information monly reported in terms of atom percent. For example, about the source of the carbon and about processes in 13 13 12 13 atom percent C = [ C/( C + C)]100 (1) which the carbon has participated. A closely related term is the fractional abundance The delta notation. Because the interesting isotopic 13 13 fractional abundance of C ≡ F differences between natural samples usually occur at and 13F = 13C/(12C + 13C) (2) beyond the third significant figure of the isotope ratio, it has become conventional to express isotopic abundances These variables deserve attention because they provide using a differential notation. To provide a concrete the only basis for perfectly accurate mass balances. example, it is far easier to say – and to remember – that Isotope ratios are also measures of the absolute abun- the isotope ratios of samples A and B differ by one part dance of isotopes; they are usually arranged so that the per thousand than to say that sample A has 0.3663 %15N more abundant isotope appears in the denominator and sample B has 0.3659 %15N.
    [Show full text]
  • Toxicological Profile for Plutonium
    PLUTONIUM 1 1. PUBLIC HEALTH STATEMENT This public health statement tells you about plutonium and the effects of exposure to it. The Environmental Protection Agency (EPA) identifies the most serious hazardous waste sites in the nation. These sites are then placed on the National Priorities List (NPL) and are targeted for long-term federal clean-up activities. Plutonium has been found in at least 16 of the 1,689 current or former NPL sites. Although the total number of NPL sites evaluated for this substance is not known, strict regulations make it unlikely that the number of sites at which plutonium is found would increase in the future as more sites are evaluated. This information is important because these sites may be sources of exposure and exposure to this substance may be harmful. When a substance is released from a large area, such as an industrial plant, or from a container, such as a drum or bottle, it enters the environment. This release does not always lead to exposure. You are normally exposed to a substance only when you come in contact with it. You may be exposed by breathing, eating, or drinking the substance, or by skin contact. However, since plutonium is radioactive, you can also be exposed to its radiation if you are near it. External exposure to radiation may occur from natural or man-made sources. Naturally occurring sources of radiation are cosmic radiation from space or radioactive materials in soil or building materials. Man- made sources of radioactive materials are found in consumer products, industrial equipment, atom bomb fallout, and to a smaller extent from hospital waste and nuclear reactors.
    [Show full text]
  • Chromium-Nickel Steels Depleted of Nickel Stable Isotope Ni-58 As a Material for Fast Reactor Claddings
    IAEA-CN-114/15p Chromium-Nickel steels depleted of nickel stable isotope Ni-58 as a material for fast reactor claddings G.L.Khorasanov, A.P.Ivanov, A.I.Blokhin, N.A.Demin Institute of Physics and Power Engineering named after A.I.Leypunsky 1, Bondarenko square, Obninsk, Kaluga region, 249033 Russia Tel.: +7-08439-98505, Fax: +7-095-2302326, E-mail: [email protected] INTRODUCTION Presently, the creation of new materials for fast reactor (FR) claddings is one of the main tasks of the nuclear engineering [1]. Now the Russian austenitic steel grade TchS68 with 15 % of nickel content is used as a material for the Russian FR BN-600 claddings [2]. With such a cladding the BN-600 fuel rod is stably operating during 10 years up to the fuel burn-up fraction of 10 % of heavy atoms (h.a.). The cladding material becomes swelled and unfit for further service after the fuel burn-up fraction of 10 % h.a. The task of increasing the fuel burn-up fraction up to 14 % h.a. is now the principal one for the BN-600 operation. For this purpose the new radiation–resistant austenitic steel grade EK164 with 19 % of nickel content is now developing in the Bochvar Institute, Russia [3]. It is generally assumed that steel swelling is caused by the combined action of radiation damage and helium accumulation in the irradiated material. In this case, nickel stable isotope, Ni-58 (its content in natural nickel is equal to 68%) is a source of helium creation. After 4 neutron capture via (n,g) reaction, Ni-58 is transmuted to radioisotope Ni-59 (T1/2=7.6⋅10 years) which has a high value of (n,α) reaction cross-section for thermal and epithermal neutrons.
    [Show full text]
  • Lithium Isotope Fractionation During Uptake by Gibbsite
    Available online at www.sciencedirect.com ScienceDirect Geochimica et Cosmochimica Acta 168 (2015) 133–150 www.elsevier.com/locate/gca Lithium isotope fractionation during uptake by gibbsite Josh Wimpenny a,⇑, Christopher A. Colla a, Ping Yu b, Qing-Zhu Yin a, James R. Rustad a, William H. Casey a,c a Department of Earth and Planetary Sciences, University of California, One Shields Avenue, Davis, CA 95616, United States b The Keck NMR Facility, University of California, One Shields Avenue, Davis, CA 95616, United States c Department of Chemistry, University of California, One Shields Avenue, Davis, CA 95616, United States Received 5 November 2014; accepted in revised form 8 July 2015; available online 15 July 2015 Abstract The intercalation of lithium from solution into the six-membered l2-oxo rings on the basal planes of gibbsite is well-constrained chemically. The product is a lithiated layered-double hydroxide solid that forms via in situ phase change. The reaction has well established kinetics and is associated with a distinct swelling of the gibbsite as counter ions enter the interlayer to balance the charge of lithiation. Lithium reacts to fill a fixed and well identifiable crystallographic site and has no solvation waters. Our lithium-isotope data shows that 6Li is favored during this intercalation and that the À À solid-solution fractionation depends on temperature, electrolyte concentration and counter ion identity (whether Cl ,NO3 À or ClO4 ). We find that the amount of isotopic fractionation between solid and solution (DLisolid-solution) varies with the amount of lithium taken up into the gibbsite structure, which itself depends upon the extent of conversion and also varies À À À with electrolyte concentration and in the counter ion in the order: ClO4 <NO3 <Cl .
    [Show full text]
  • Isotopic Composition of Fission Gases in Lwr Fuel
    XA0056233 ISOTOPIC COMPOSITION OF FISSION GASES IN LWR FUEL T. JONSSON Studsvik Nuclear AB, Hot Cell Laboratory, Nykoping, Sweden Abstract Many fuel rods from power reactors and test reactors have been punctured during past years for determination of fission gas release. In many cases the released gas was also analysed by mass spectrometry. The isotopic composition shows systematic variations between different rods, which are much larger than the uncertainties in the analysis. This paper discusses some possibilities and problems with use of the isotopic composition to decide from which part of the fuel the gas was released. In high burnup fuel from thermal reactors loaded with uranium fuel a significant part of the fissions occur in plutonium isotopes. The ratio Xe/Kr generated in the fuel is strongly dependent on the fissioning species. In addition, the isotopic composition of Kr and Xe shows a well detectable difference between fissions in different fissile nuclides. 1. INTRODUCTION Most LWRs use low enriched uranium oxide as fuel. Thermal fissions in U-235 dominate during the earlier part of the irradiation. Due to the build-up of heavier actinides during the irradiation fissions in Pu-239 and Pu-241 increase in importance as the burnup of the fuel increases. The composition of the fission products varies with the composition of the fuel and the irradiation conditions. The isotopic composition of fission gases is often determined in connection with measurement of gases in the plenum of punctured fuel rods. It can be of interest to discuss how more information on the fuel behaviour can be obtained by use of information available from already performed determinations of gas compositions.
    [Show full text]
  • 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.
    [Show full text]
  • Mass Fraction and the Isotopic Anomalies of Xenon and Krypton in Ordinary Chondrites
    Scholars' Mine Masters Theses Student Theses and Dissertations 1971 Mass fraction and the isotopic anomalies of xenon and krypton in ordinary chondrites Edward W. Hennecke Follow this and additional works at: https://scholarsmine.mst.edu/masters_theses Part of the Chemistry Commons Department: Recommended Citation Hennecke, Edward W., "Mass fraction and the isotopic anomalies of xenon and krypton in ordinary chondrites" (1971). Masters Theses. 5453. https://scholarsmine.mst.edu/masters_theses/5453 This thesis is brought to you by Scholars' Mine, a service of the Missouri S&T Library and Learning Resources. This work is protected by U. S. Copyright Law. Unauthorized use including reproduction for redistribution requires the permission of the copyright holder. For more information, please contact [email protected]. MASS FRACTIONATION AND THE ISOTOPIC ANOMALIES OF XENON AND KRYPTON IN ORDINARY CHONDRITES BY EDWARD WILLIAM HENNECKE, 1945- A THESIS Presented to the Faculty of the Graduate School of the UNIVERSITY OF MISSOURI-ROLLA In Partial Fulfillment of the Requirements for the Degree MASTER OF SCIENCE IN CHEMISTRY 1971 T2572 51 pages by Approved ~ (!.{ 1.94250 ii ABSTRACT The abundance and isotopic composition of all noble gases are reported in the Wellman chondrite, and the abundance and isotopic composition of xenon and krypton are reported in the gases released by stepwise heating of the Tell and Scurry chondrites. Major changes in the isotopic composition of xenon result from the presence of radio­ genic Xel29 and from isotopic mass fractionation. The isotopic com­ position of trapped krypton in the different temperature fractions of the Tell and Scurry chondrites also shows the effect of isotopic fractiona­ tion, and there is a covariance in the isotopic composition of xenon with krypton in the manner expected from mass dependent fractiona­ tion.
    [Show full text]
  • Lithium Isotope Separation a Review of Possible Techniques
    Canadian Fusion Fuels Technology Project Lithium Isotope Separation A Review of Possible Techniques Authors E.A. Symons Atomic Energy of Canada Limited CFFTP GENERAL CFFTP Report Number s Cross R< Report Number February 1985 CFFTP-G-85036 f AECL-8 The Canadian Fusion Fuels Technology Project represents part of Canada's overall effort in fusion development. The focus for CFFTP is tritium and tritium technology. The project is funded by the governments of Canada and Ontario, and by Ontario Hydro. The Project is managed by Ontario Hydro. CFFTP will sponsor research, development and studies to extend existing experience and capability gained in handling tritium as part of the CANDU fission program. It is planned that this work will be in full collaboration and serve the needs of international fusion programs. LITHIUM ISOTOPE SEPARATION: A REVIEW OF POSSIBLE TECHNIQUES Report No. CFFTP-G-85036 Cross Ref. Report No. AECL-8708 February, 1985 by E.A. Symons CFFTP GENERAL •C - Copyright Ontario Hydro, Canada - (1985) Enquiries about Copyright and reproduction should be addressed to: Program Manager, CFFTP 2700 Lakeshore Road West Mississauga, Ontario L5J 1K3 LITHIUM ISOTOPE SEPARATION: A REVIEW OF POSSIBLE TECHNIQUES Report No. OFFTP-G-85036 Cross-Ref Report No. AECL-87O8 February, 1985 by E.A. Symons (x. Prepared by: 0 E.A. Symons Physical Chemistry Branch Chemistry and Materials Division Atomic Energy of Canada Limited Reviewed by: D.P. Dautovich Manager - Technology Development Canadian Fusion Fuels Technology Project Approved by: T.S. Drolet Project Manager Canadian Fusion Fuels Technology Project ii ACKNOWLEDGEMENT This report has been prepared under Element 4 (Lithium Compound Chemistry) of the Fusion Breeder Blanket Program, which is jointly funded by AECL and CFFTP.
    [Show full text]
  • Uranium-233 at the Hanford Nuclear Site
    Uranium-233 at the Hanford Nuclear Site December 2002 Fact Sheet 320-086 Division of Environmental Health Office of Radiation Protection INTRODUCTION Hanford’s historical mission was the production of fissile material for nuclear weapons. Most significantly, the fissile material Plutonium-239 was produced by irradiating Uranium-238 in nuclear reactors. In the mid 1960’s, and again in the early 1970’s, smaller scale efforts were carried out to experiment with producing the fissile material Uranium-233 by irradiating Thorium-232. PHYSICAL PROPERTIES? Uranium has three isotopes that exist naturally. They are Uranium-234, Uranium-235, and Uranium-238. Uranium -233 is man-made. Some properties of these isotopes are listed below. Property U-233 U-234 U-235 U-238 Natural abundance 0 0.0055 0.7200 99.2745 by weight (%) Natural abundance 0 49.65 2.25 48.10 by radioactivity (%) Half life (years) 160,000 246,000 700 million 4.5 billion DETECTION AND ANALYSIS All of these uranium is otopes emit alpha radiation. Typically, uranium is measured in environmental samples by detecting the alpha radiation. Alpha spectroscopy methods are able to detect and differentiate alpha radiation from each of the three natural isotopes, so that concentrations may be reported for each isotope. Alpha radiation emitted from U-233 is detectable by alpha spectroscopic methods, however, it is difficult to differentiate between the alpha radiation emitted from U-233 and U-234. If U-233 is present in quantities similar to U-234, U-233 can be differentiated and its concentration identified and reported separately. This situation has not been observed in environmental samples analyzed for isotopic uranium at Hanford.
    [Show full text]
  • Nickel Isotope Variations in Terrestrial Silicate Rocks and Geological
    Nickel Isotope Variations in Terrestrial Silicate Rocks and Geological Reference Materials Measured by MC-ICP-MS Bleuenn Gueguen, Olivier Rouxel, Emmanuel Ponzevera, Andrey Bekker, Yves Fouquet To cite this version: Bleuenn Gueguen, Olivier Rouxel, Emmanuel Ponzevera, Andrey Bekker, Yves Fouquet. Nickel Iso- tope Variations in Terrestrial Silicate Rocks and Geological Reference Materials Measured by MC- ICP-MS. Geostandards and Geoanalytical Research, Wiley, 2013, 37, pp.297-317. 10.1111/j.1751- 908X.2013.00209.x. insu-00846624 HAL Id: insu-00846624 https://hal-insu.archives-ouvertes.fr/insu-00846624 Submitted on 18 Feb 2014 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Received Date: 03-Aug-2012 Revised Date: 12-Dec-2012 Accepted Date: 17-Dec-2012 Article Type: Original Article Nickel Isotope Variations in Terrestrial Silicate Rocks and Geological Reference Materials Measured by MC-ICP-MS Bleuenn Gueguen (1, 2)*, Olivier Rouxel (1, 2), Emmanuel Ponzevera (2), Andrey Bekker (3) Article and Yves Fouquet (2) (1) Institut Universitaire Européen de la Mer, UMR 6538, Université de Bretagne Occidentale, BP 80, F- 29280 Plouzané, France (2) IFREMER, Centre de Brest, Unité Géosciences Marines, 29280 Plouzané, France (3) University of Manitoba, Department of Geological Sciences, Winnipeg, MB, R3T 2N2, Canada * Corresponding author.
    [Show full text]
  • Plutonium (Pu) Fact Sheet
    Plutonium (Pu) November 2002 Fact Sheet 320-080 Division of Environmental Health Office of Radiation Protection WHO DISCOVERED PLUTONIUM? Plutonium was first produced by Glenn T. Seaborg, Joseph W. Kennedy, Edward M. McMillan and Arthur C. W ohl by bombarding an isotope of uranium, uranium-238, with deuterons that had been accelerated in a device called a cyclotron. This created neptunium-238 and two free neutrons. Neptunium-238 has a half-life of 2.1 days and decays into plutonium -238 through beta decay. Although they conducted their work at the University of California in 1941, their discovery was not revealed to the rest of the scientific community until 1946 because of wartime security concerns. Plutonium was the second transuranic elem ent of the actinide series to be discovered. By far of greatest importance is the isotope 239Pu, which has a half-life of more than 20,000 years. The complete detonation of a kilogram of plutonium produces an explosion equal to about 20,000 tons of chemical explosive. The isotope 238Pu was used in the American Apollo lunar missions to power seismic and other equipment on the lunar surface. WHAT IS PLUTONIUM USED FOR? Only two of plutonium's isotopes, plutonium-238 and plutonium-239, have found uses outside of basic research. Plutonium-238 is used in radioisotope thermoelectric generators to provide electricity for space probes that venture too far from the sun to use solar power, such as the Cassini and Galileo probes. It also provides the electricity source in implanted cardiac pacemakers, space satellites, and navigation beacons.
    [Show full text]