Precise Determination of Sm/Nd Ratios, Sm and Nd Isotopic Abundances in Standard Solutions*

Total Page:16

File Type:pdf, Size:1020Kb

Precise Determination of Sm/Nd Ratios, Sm and Nd Isotopic Abundances in Standard Solutions* Precise determination of Sm/Nd ratios, Sm and Nd isotopic abundances in standard solutions* G. J. WASS~KBUKC;.S. B. JA(.OBStNt, D. J. D~PAoLo:. M. T. MCCULLOCH~ and T. WEN The Lunatic Asylum of the Charles Arms Laboratory. Division of Geological and Planetary Sciences. California Institute of Technology. Pasadena. CA 91125. IJ.S.A. Abstract -The methods used for precise calibrations of Sm,,Nd ratios and the average isotopic abun- dances obtained for normal Sm and Nd are given. A mixed Sm-Nd normal solution with a precisely known ‘47Sm;‘44Nd ratio close to the nominal average chondritic value is described and the calibration discussed. Aliquots of this standard.solution are available on request and may be useful for precise interlaboratory calibration of Sm and Nd INTRODUCTION and may not be stoichiometric. They demonstrated that PHILPOTTSand SCHNETZLER(1970) had calibrated FURTHCR DEVELOPMENTof the 147Smp143Nd method both Sm and Nd spikes erroneously by about ll”,, for understanding early lunar, terrestrial, and meteor- due to nonstoichiometry. MASUDA, NAKAMURA and ite evolution must rely on precise determination of TANAKA (1973) have also noted similar problems with the age and the initial ‘43Nd;‘44Nd ratio. One critical spike calibrations for determinations of REE in chon- factor is the determination of the ratio 147Sm/‘44Nd. dritic meteorites. NAKAMURA and TA~SUMOX) (1980) A difference of l”,, in the 147Sm/‘44Nd between two reported recently that the Sm/Nd ratios they samples will result in a difference of 1.1 e-units in measured for the achondrites Moama, Moore ‘43Nd/‘44Nd over the age of the earth (1 E-unit = 1 County, and Pasamonte were too low by 1.3”,, due to part in 104). To adequately measure the 147Sm/144Nd problems in spike calibrations and revised their pub- ratio by isotope dilution thus requires tracer solutions lished ages by -6OMyr. To avoid such problems whose concentrations are known accurately. Determi- which may result from using rare earth salts as stan- nation of the concentration of a Nd tracer solution is dards we have instead always used ultrapure Sm and done by mixing a measured mass of the tracer sol- Nd metals from the Ames Laboratory (cf. DEPAOLO ution with a measured mass of a solution containing and WASSERBURC;.1976; BEAUDRY and GSCHNEIDNER. isotopically normal Nd in known concentration and 1978; DEPAOL~, 1978). This procedure has also been then measuring the isotopic composition of the mix- adopted by NYQUIST, SHIH, WOODEN, BANSAL. and ture. Thus independent of mass spectrometric errors. WIESMANN(1979) and the results by these two labora- the precise determination of Sm/Nd ratios ultimately tories appear to be in good agreement as discussed by depends on absolute gravimetric standards for Sm JACOBSENand WASSERBURG(1980). Significant discre- and Nd. We have therefore expended a major effort pancies are apparent between the meteorite data that on preparing and calibrating solutions using absolute we now use for describing average chondritic standards. The results obtained are described in this 147Smm143Nd evolution and previously published paper. Aliquots of these standards are available to the meteorite data (see JACOBSENand WASSFRHLIKG,1980). scientific community for the comparison of isotopic The present paper should fully document the pro- abundances and the calibration of Sm and Nd iso- cedures used in this laboratory and may give a basis topic tracers. This will hopefully reduce the propa- for resolving some of the observed discrepancies in gation of errors in this rapidly developing field. the future. GAST, HUBBAKI) and WIESMANN (1970) have pointed out that spike calibration for the rare-earth elements (REE) is a difficult problem because the nor- PREPARATION OF NORMAL SOLUTIONS mal suprapure standard salts contain CO2 or HZ0 The Sm and Nd normal solutions were prepared * Division Contribution No. 3512 (369). from ultrapure chunks of metal obtained from the t Present address: Department of Geological Sciences. Ames Laboratory (see BEAUDRY and GSCHNIJIINFK, Harvard Ilniversity. Cambridge. MA 02138. U.S.A. 1978, for extensive discussion). The first batch of : Present address: Department of Earth and Space metals was obtained in 1975 and is called NdA and Sciences. University of California. Los Angeles, Los SmA (Table 1). The second batch of metals was Angclcs. CA 90024, (J.S.A. S Present address: Research School of Earth Sciences, obtained in 1978 and is called Ndcc, Nd/I. Smr and The :2ustralian National Ilniversity. Canberra. Australia. Smfi (Table 1). The Sm and Nd metals contain less 2311 2312 c;. j. WASSFRHI1RG Cf tl/ Table 1. Sm AND Nd NORMALS AND TRACERS Table 2. WEIGHTS OF METALS AND GRAVIMETRil CONCENTRATIONSOF NORMAL SOLUTIONS Neodymium Samarium AND Sm/Nd MIXED NORMAL Weight (grams) Concentration:: Normal metals NdA, a, S SrnA,a. d AMES CIT (llR/R, (- 1 gram each) --..-..-____ Normal solutions nNdA insmA IlNdA 1.06230 1.06240 1174.14 (- 1 or 2 liters each) nNda nSma IlSmA 0.307298 0.30726 333.411 nNdS nsmf? nNdu 0.91893 0.91892 999.:32 nSma 0.96209 0.96216 504.Ulr. Mixed normal - 1.5 liters nNdS + - U.45 liters nS@ nNdS 1.07015 1.07008 565.087 solution IlSUlS 1.12380 1.12351 607.77.i Oxide tracers 150Nd203(- 10 mS) "'Sln203(.~20 mg) Mixed Sm-Nd normal solution n(Sm/Nd)D: [Ndl = 434.070 up/g; [Sml = 141.140 l>R/**, Tracer solutions T Nd150 ? Sml47 (Sm/NdjWEIGHT= 0.32515 ______~~.---- than 100 ppm of cation impurities (Ames analysis). chosen because it is a low abundance ~sotopc m The amount of anion impurities (H. 0, N. c’. F. Cl) in nature and is not isobaric with any Nd isotope lSJSn~ the metal was measured to be less than 100 ppm at is the least abundant samarium isotope. b11t ma) the Ames Laboratory. It is however possible that the interfere with ‘44Nd if chemical separation of Sm and metal could have taken up some anion impurities Nd is not perfect. ‘49Sm and ‘s”Sm arc \ar~,&lc in during subsequent handling. The different metal lunar samples and meteorites due to neutron capture chunks (A, a, /?) had been weighed and sealed in eva- effects and ‘52Sm and 154Sm are the most abundant cuated Pyrex vials at the Ames Laboratory. Upon Sm isotopes. The ratio ‘48Sm, is4Sm can bc used to removal from the vials the metal chunks were re- provide a precise estimate of mass discrimination. By weighed with a semi-micro balance (precision and ac- adding about twice the 14’Srn already present m the curacy + 10 pg) prior to dissolution. The balance was sample a precise Sm concentration may be obtained checked with Class S weights calibrated against NBS and precise corrections can be made for other iso- weights. These weights agreed mostly within weighing topes such that ‘4gSm/‘54Sm and i50Sm,“54Sm in the error of the values given by the Ames Laboratory sample can be measured to monitor neutron capture (Table 2). The metals were transferred to I 2 I. effects if desired. polyethylene bottles, dissolved in 2.5 N HCI, and the Stock solutions of lsoNd and ‘“‘Sm tracers were resulting gravimetric concentrations are given in prepared in 1975 from oxide powders obtained from Table 2. The concentrations were obtained by weigh- Oak Ridge (DEPAOLO, 1978), Following usual pra\i- ing these bottles on a double pan balance (precision metric procedures these were repeatedly heated to and accuracy _t 10 mg). No corrections were made for 800 C in a furnace until the change in weight between buoyancy since these effects are negligible. two successive weighings was less than 0.05”,, of the The normal solutions are called nNdA. nNda. etc. total weight of the powder. The total weight loss was (see Table 1). From the normal solutions nNd/l and about 15”;. Since only - 10-20 mg of these powders nSm/l we made a mixed normal solution with an were weighed (Table 3), the concentrations of the Sm/Nd ratio very close to the average chondritic tracer solution were considered to be correct to about ratio. The gravimetric concentrations and the Sm/Nd 0.3”,,, however. no precise determination of the stoi- weight ratio for this mixed normal solution (called chiometry was done. The tracer solutions are called ‘T’ CIT Sm,/Nd standard) are also given in Table 2. Nd150 and T Sm147 respectively and their nominal gravimetric concentrations are given in Table 3 SELECTION AND PREPARATION OF TRACER SOLUTIONS THE ISOTOPIC COMPOSITION OF NORMAL Sm AND Nd The selection of tracers is important and they have been chosen from available tracers to optimize the Nd and Sm isotopic compositions were measured measurement of both “‘Ndi’44Nd ratios and Sm on the Lunatic I and III mass spectrometers (W.~SSEK- and Nd concentrations on totally spiked samples. For BURG, PAPANASTASSIOU, NENOW and BAukwh. 1969) Nd, a 961, pure i’“Nd tracer was chosen because as NdO+ and Sm’, respectively. following the pro- ““Nd is a low-abundance isotope in nature The small amounts of the other isotopes present in this Table 3. WEIGHT OF TRACER OXIDE POWDERS AND tracer cause only small changes in the relative abun- GRAVINETRIC CDNBNTRATIONS OF TRACERS dances of all the other Nd isotopes for which precise Weight rkxlcentrat;ons corrections can be made. Thus a precise determi- nation of the Nd concentration and all isotopic ratios T Nd150 10.58 mg IsaNd 5.253 US '53Nd$'3ii: to.03 tn.015 except 150Nd/i44Nd can be obtained by adding a similar amount of lsoNd tracer as the amount present T Sm147 20.42 mg '47Sm*03 10.732 ,,g'"iFmir@jlg kO.04 to.021 in the sample. For Sm a 98”,, pure 14’Sm tracer was Samarium and neodymium in standard solutions 2313 cedures described in detail by EUGSTER, TERA, BUR- clearly below this trend.
Recommended publications
  • 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 .
    [Show full text]
  • Chemical and Isotropic Tracers of Natural Gas and Formation Waters in Fractured Shales
    Chemical and isotopic tracers of natural gas and formation waters in Note: this document may contain some elements that are not fully fractured shales accessible to users with disabilities. If you need assistance accessing any information in this document, please contact [email protected]. Jennifer McIntosh, Melissa Schlegel, Brittney Bates Department of Hydrology & Water Resources University of Arizona, Tucson AZ EPA Technical Workshop Feb 24-25, 2011 Outline of Presentation 1)) What is the chemical and isotoppgic signature of formation waters and natural gas in fractured shales? 2) How does it compare with shallow drift aquifers, coalbeds, and other deep geologic formations? Illinois Basin-Case Study - 3 organic-rich formations: glacial drift, Penn. coal, & Dev. fractured shale - organicorganic-rich Ordov. ShaleShale, not part ooff this study m 500 20 km Schlegel et al. (in press, 2011, Geochimica et Cosmochimica Acta) Illinois Basin-Case Study - microbial methane in all 3 units - thermogenic methane in shale and coal m 500 20 km Schlegel et al. (in press, 2011, Geochimica et Cosmochimica Acta) Illinois Basin - water & gas samples Shallow aquifers Penn. Coals Dev. Shale Limestone aquifers 9New data (white symbols): Schlegel et al. (in press) 9Previous data (black symbols): McIntosh et al., 2002; Strąpoć et al., 2007, 2008a,b; Coleman et al, 1988 Fingerprint of natural gases 1000000 Shallow Aquifers 100000 High C1/C2, no C3 Coals 10000 1000 Shale 100 10 Shallow aquifers Penn. Coals Dev. Shale Thermogenic gas 1 -80 -75 -70 -65 -60 -55 -50 -45 -40 13 δ CCH4 (ä PDB) 13 9In general, 3 organic-rich units have different gas compositions (C1/C2+C3) and δ C-CH4 values.
    [Show full text]
  • F:\Forensic Geology\Ice Man Isotopes.Wpd
    NAME 89.215 - FORENSIC GEOLOGY DEMISE OF THE ICE MAN - ISOTOPIC EVIDENCE I. Introduction Stable and radiogenic isotopic data have been used in a variety of fields to answer a wide range of scientific questions. The nucleus of an atom consists of protons (+1 charge) and neutrons (0 charge), two types of particles that have essentially the same atomic mass. The number of protons in a nucleus determines the element. For example, a nucleus with 1 proton is a hydrogen nucleus, a nucleus with 2 protons is a helium nucleus. Isotopes of an element contain the same number of protons but different numbers of neutrons. For example, there are three isotopes of hydrogen: (1) ordinary hydrogen which contains one proton and no neutrons and has an atomic mass of one; (2) deuterium which contains one proton and one neutron and has an atomic mass of two; and (3) tritium which contains one proton and two neutrons and has an atomic mass of three. The convention used to show the numbers of types of particles in a nucleus is to place the number of protons (called the atomic number) at the bottom left of the element symbol and the number of protons plus neutrons (called the atomic mass) at the upper left of the element symbol. For example, the tritium isotope is 3 shown as 1H . II. Stable isotopes Stable isotopes are not radioactive, they do not spontaneously breakdown to other atoms. In a previous exercise you used radioactive carbon to determine when the Ice Man was killed. There are three isotopes of carbon: (1) carbon 12 which contains 6 protons and 6 neutrons giving an atomic mass of 12; (2) carbon 13 which contains 6 protons and 7 neutrons giving an atomic mass of 13; and (3) carbon 14 which contains 6 protons and 8 neutrons giving an atomic mass of 14.
    [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]
  • Isotope Geochemistry of Carbonate Dissolution and Reprecipitation in Soils R
    SOIL SCIENCE Vol. 122, No. I Copyright © 1976 by The Williams &Wilkin s Co. I'rintedin U.S.A. ISOTOPE GEOCHEMISTRY OF CARBONATE DISSOLUTION AND REPRECIPITATION IN SOILS W. SALOMONS' AND W. G. MOOK Laboratoryof Inorganic Chemistry'.The University of Groningen, Zernikelaan, Paddepoel,Groningen, the Netherlands, and Physics Laboratory, University of Groningen, Westersingel 34, Groningen, the Netherlands Received for publication May 21, 197/> ABSTRACT The processes of dissolution and reprecipitation of carbonates in soils developed on carbonate rocks, loess-derived soils, and marine clay soils were studied with the methods of stable isotope geochemistry. Between 10 and 50 percent of the carbonates present in the upper part of soils developed on carbonate rocks are newly formed. In loess-derived soils and in marine clay soils, up to 100 percent of the carbonates present may be newly formed. The efficiency of the dissolution-reprecipitation process varies between 10 and 30 percent. In the salt marsh investigated the dissolution is caused by the action of biogenic carbon dioxide. INTRODUCTION pies by treatment with 95 percent orthophos- Carbonates are an important constituent of phoric acid. The presence of organic matter in the soil. The processes they are subject to are most soil samples analyzed introduces an error dissolution followed by (partial) reprecipita­ in both the carbon and oxygen isotopic composi­ tion. Reprecipitation can be easily recognized tion of less than 0.37„o (Salomons 1974). when it results in macroscopic concretions. Since this small shift has no influence on our However, when the newly formed carbonates conclusions, the time-consuming step of remov­ are finely divided they are difficult to detect by ing the organic matter from the sample prior to conventional methods.
    [Show full text]
  • Nuclear and Isotopic Techniques for Marine Pollution Monitoring
    NUCLEAR AND ISOTOPIC TECHNIQUES FOR MARINE POLLUTION MONITORING A. Introduction The greatest natural resource on the Planet, the World Ocean is both the origin of most life forms and the source of survival for hundredsth of millions of people. Pollution of the oceans was an essential problem of the 20 century that was associated with the rapid industrializationst and unplanned occupation of coastal zones It continues to be a concern in the 21 century. The most serious environmental problems encountered in coastal zones are presented by runoff of agricultural nutrients, heavy metals, and persistent organic pollutants, such as pesticides and plastics. Oil spills from ships and tankers continually present a serious threat to birds, marine life and beaches. Also, many pesticides that are banned in most industrialized countries remain in use today, their trans-boundary pathway of dispersion affecting marine ecosystems the world over. In addition to these problems, ocean dumping of radioactive waste has occurred in the past, and might occur again, with authorised discharges of radioactive substances from nuclear facilities into rivers and coastal areas contributing to the contamination of the marine environment. A trans-boundary issue, marine pollution is often caused by inland economic activities, which lead to ecological changes in the marine environment. Examples include the use of chemicals in agriculture, atmospheric emissions from factories and automobiles, sewage discharges into lakes and rivers, and many other phenomena taking place hundreds or thousands of kilometres away from the seashore. Sooner or later, these activities affect the ecology of estuaries, bays, coastal waters, and sometimes entire seas, consequently having an impact on the economy related to maritime activities.
    [Show full text]
  • Stable Isotopes of Carbon and Nitrogen in the Study of Avian and Mammalian Trophic Ecology
    Color profile: Disabled Composite Default screen 1 REVIEW/SYNTHÈSE Stable isotopes of carbon and nitrogen in the study of avian and mammalian trophic ecology Jeffrey F. Kelly Abstract: Differential fractionation of stable isotopes of carbon during photosynthesis causes C4 plants and C3 plants to have distinct carbon-isotope signatures. In addition, marine C3 plants have stable-isotope ratios of carbon that are 13 12 intermediate between C4 and terrestrial C3 plants. The direct incorporation of the carbon-isotope ratio ( C/ C) of plants into consumers’ tissues makes this ratio useful in studies of animal ecology. The heavy isotope of nitrogen (15N) is preferentially incorporated into the tissues of the consumer from the diet, which results in a systematic enrichment in nitrogen-isotope ratio (15N/14N) with each trophic level. Consequently, stable isotopes of nitrogen have been used pri- marily to assess position in food chains. The literature pertaining to the use of stable isotopes of carbon and nitrogen in animal trophic ecology was reviewed. Data from 102 studies that reported stable-isotope ratios of carbon and (or) nitrogen of wild birds and (or) mammals were compiled and analyzed relative to diet, latitude, body size, and habitat moisture. These analyses supported the predicted relationships among trophic groups. Carbon-isotope ratios differed among species that relied on C3,C4, and marine food chains. Likewise, nitrogen-isotope ratios were enriched in terres- trial carnivorous mammals relative to terrestrial herbivorous mammals.
    [Show full text]
  • Correcting for Naturally Occurring Mass Isotopologue Abundances in Stable-Isotope Tracing Experiments with Polymid
    H OH metabolites OH Article Correcting for Naturally Occurring Mass Isotopologue Abundances in Stable-Isotope Tracing Experiments with PolyMID Heesoo Jeong 1, Yan Yu 2, Henrik J. Johansson 3, Frank C. Schroeder 2, Janne Lehtiö 3 and Nathaniel M. Vacanti 1,3,* 1 Division of Nutritional Sciences, Cornell University, Ithaca, NY 14853, USA; [email protected] 2 Boyce Thompson Institute and Department of Chemistry and Chemical Biology, Cornell University, Ithaca, NY 14853, USA; [email protected] (Y.Y.); [email protected] (F.C.S.) 3 Science for Life Laboratory, Department of Oncology-Pathology, Karolinska Institutet, 17165 Solna, Sweden; [email protected] (H.J.J.); [email protected] (J.L.) * Correspondence: [email protected] Abstract: Stable-isotope tracing is a method to measure intracellular metabolic pathway utilization by feeding a cellular system a stable-isotope-labeled tracer nutrient. The power of the method to resolve differential pathway utilization is derived from the enrichment of metabolites in heavy isotopes that are synthesized from the tracer nutrient. However, the readout is complicated by the presence of naturally occurring heavy isotopes that are not derived from the tracer nutrient. Herein we present an algorithm, and a tool that applies it (PolyMID-Correct, part of the PolyMID software package), to computationally remove the influence of naturally occurring heavy isotopes. Citation: Jeong, H.; Yu, Y.; Johansson, The algorithm is applicable to stable-isotope tracing data collected on low- and high- mass resolution H.J.; Schroeder, F.C.; Lehtiö, J.; mass spectrometers. PolyMID-Correct is open source and available under an MIT license. Vacanti, N.M.
    [Show full text]
  • How Atoms Differ A
    Warm Up # Cathode Ray Tube Evacuated tube Anode Cathode − + 1. What did the cathode ray tube help to discover? Battery 2. Which scientist thought of using the cathode ray tube? How Atoms Differ a. Properties of Subatomic Particles Particle Symbol Location Relative Relative Actual Charge mass mass (g) outside 1 Electron e- the 9.11 x nucleus -1 1840 10-28 g in the 1.673 x Proton p+ nucleus +1 1 10-24 g in the 1.675 x Neutron 0 n nucleus 0 1 10-24 g Elements on the Periodic Table b. Atomic Number • the number of protons in an atom • Identifies element c. Mass Number •represents the total number of protons and neutrons in the nucleus Mass number A ZX atomic number d. Isotopes • Atoms that have the same number of protons but have a different masses • Ex: 3 isotopes of carbon: 12 13 14 6C 6C 6C e. Average Atomic Mass • the weighted average of the isotopes of that element. • Formula: % mass % Atomic mass abundance of abundance mass of ( ) ( of ) = of x Isotope + of x + … an element Isotope #2 Isotope #1 #1 Isotope #2 Average Atomic Mass • The mass of an atom is so small it is difficult to work with, so chemists have developed an atomic standard to compare all the masses • The standard is the atomic mass unit (amu) • If the mass of an element is not close to a whole number, it is because the atom has several isotopes • The atomic mass is the weighted average of the isotopes of that element Example 1 Silver has two naturally occurring isotopes.
    [Show full text]
  • Office of Radiation Protection Department of Health 7171 Cleanwater Lane, Bldg
    DOH 320-029 Environmental Radiation Program Hanford Environmental Oversight Program 2000 Data Summary Report Environmental Health Programs DOH 320-029 Environmental Radiation Program Hanford Environmental Oversight Program 2000 Data Summary Report Scott Van Verst Lynn Albin Washington State Department of Health For more information or additional copies of this report, contact: Environmental Radiation Section Office of Radiation Protection Department of Health 7171 Cleanwater Lane, Bldg. 5 P.O. Box 47827 Olympia WA 98504 360-236-3251 Email: [email protected] FAX: 360-236-2255 Summary The Washington State Department of Health (DOH) has operated an environmental radiation monitoring program since 1961. The early program looked primarily at atmospheric fallout and off-site environmental impacts related to Hanford operations. Currently, the DOH conducts radiological surveillance in many geographical areas of the state and routinely splits (co-samples) environmental samples with state licensed and federal environmental monitoring programs. Since 1985, the Washington State Department of Health’s Hanford Environmental Oversight Program has participated with the U.S. Department of Energy (DOE) in the collection of environmental samples on or near the Hanford Site. The purpose of the program is to independently verify the quality of DOE environmental monitoring programs at the Hanford Site, and to assess the potential for public health impacts. This report is a summary of the data collected for the Hanford Environmental Oversight Program in 2000. The Oversight Program’s objectives are met through collection and analyses of environmental samples and interpretation of results. DOH samples are either split or co-located with samples collected by the DOE contractors.
    [Show full text]
  • Isotopes Are Atoms with the Same # of Protons (Making Them the SAME ELEMENT), but Have a Different # of Neutrons
    Each element has a unique # of protons. So…EVERY SINGLE ATOM of that element MUST HAVE the SAME number of protons, ALWAYS! This is the reason why each element has a unique Atomic Number that never changes! Isotopes are atoms with the same # of protons (making them the SAME ELEMENT), but have a different # of neutrons. Having different # of neutrons for the same element means that the isotopes will have different mass numbers, too! There are 3 isotopes of oxygen: 8 8 8 O8 O9 O10 neutronsOxygen neutronsOxygen neutronsOxygen ALL oxygen16 isotopes 17have an atomic 18# of 8, so they all have 8 protons! How many protons does each isotope have? How many neutrons does each isotope have? There are 3 isotopes of carbon: 6 6 6 C6 C7 C8 neutronsCarbon neutronsCarbon neutronsCarbon ALL carbon12 isotopes 13have an atomic #14 of 6, so they all have 6 protons! How many protons does each isotope have? How many neutrons does each isotope have? Atomic Masses on the periodic table are normally decimals. WHY?? Atomic Masses are decimals because it is an AVERAGE mass of all of the element’s isotopes. Some isotopes are more common than others, so this is a weighted average. 5 So the Mass # from the periodic table is B always closest to the most common Boron isotope’s mass. 10.81 In the universe, there are MUCH more carbon-12 atoms that exist than carbon-13 and carbon-14 atoms. 6 C Carbon- 12 Carbon 12.01 When you find the weighted average of the masses of the carbon isotopes, the average will be closest to 12! The Atomic Mass of calcium is 40.08.
    [Show full text]
  • Isotopic Compositions of the Elements 1983
    Pure & Appi. Chem., Vol. 56, No. 6, pp. 675—694, 1984. 0033—4545/84 $3.00+0.00 Printed in Great Britain. Pergamon Press Ltd ©1984 IUPAC INTERNATIONALUNION OF PURE AND APPLIED CHEMISTRY INORGANIC CHEMISTRY DIVISION COMMISSION ON ATOMIC WEIGHTS AND ISOTOPIC ABUNDANCES* ISOTOPIC COMPOSITIONS OF THE ELEMENTS 1983 Prepared for publication by N. E. HOLDEN1, R. L. MARTIN2 and I. L. BARNES3 1Brookhaven National Laboratory, Upton, New York 11973, USA 2Monash University, Clayton, Victoria 3168, Australia 3National Bureau of Standards, Washington, DC 20234, USA *Membership of the Commission for the period 1981—85 is as follows: R. L. MARTIN (Chairman 1983—85, Secretary 1981—83); J. R. DE LAETER (Secretary 1983—85, Associate 1981—83); R. C. BARBER (Titular 1981—85); I. L. BARNES (Titular 1981—85); P. DE BIEVRE (Associate 1981—85); T. L. CHANG (Titular 1983—85); T.B. COPLEN (Associate 1983—85); R. GONFIANTINI (Associate 1981—83); N. N. GREENWOOD (Associate 1981—83); R. HAGEMANN (Titular 1981—83); K. G. HEUMANN (Associate 1983—85); N. E. HOLDEN (Associate 1983—85, Chairman 1981—83); W. H. JOHNSON (Associate 1981—85); T. J. MURPHY (Titular 1981—85); H. S. PEISER (Associate 1981—85); C. E. REES (Associate 1983—85); K. J. R. ROSMAN (Associate 1983—85); M. SHIMA (Associate 1981—85). ISOTOPIC COMPOSITIONS OF THE ELEMENTS 1983 Abstract —TheCommission's biennial review of isotopic compositions as determined by mass spectrometry and other relevant methods has been undertaken by the Subcommittee for the Assessment of Isotopic Composition (SAIC). The Subcommittee's critical evaluation of the published literature element by element forms the basis of the Table of Isotopic Compositions as Determined by Mass Spectrometry, 1983, which is presented in this Report.
    [Show full text]