actinide science and radiochemistry

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1-1 Actinide Science and Radiochemistry Readings: Chart of the nuclides Modern Nuclear Chemistry: Chapter 1 Class organization Outcomes Grading History of radiation research Chart of the nuclides Description and use of chart Data Radiochemistry introduction Atomic properties Nuclear nomenclature X-rays Types of decays forces

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Page 1: Actinide Science and Radiochemistry

1-1

Actinide Science and Radiochemistry •  Readings:

❧  Chart of the nuclides ❧  Modern Nuclear Chemistry: Chapter 1

•  Class organization ❧  Outcomes ❧  Grading

•  History of radiation research •  Chart of the nuclides

❧  Description and use of chart ❧  Data

•  Radiochemistry introduction ❧  Atomic properties ❧  Nuclear nomenclature ❧  X-rays ❧  Types of decays ❧  forces

Page 2: Actinide Science and Radiochemistry

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Introduction •  Coursed developed with support from

Department of Energy-Nuclear Energy •  Extension of education and research

efforts in the UNLV Radiochemistry program

•  Course designed to increase potential pool of researchers for the nuclear fuel cycle ❧  Nuclear fuel ❧  Separations ❧  Waste forms ❧  Nuclear forensics and the fuel cycle ❧  Safeguards ❧  Nuclear reactors

•  Course will emphasize the role of radiochemistry in the nuclear fuel cycle

Page 3: Actinide Science and Radiochemistry

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History of Radiation Research •  1896 Discovery of radioactivity

❧  Becquerel used K2UO2(SO4)2• H2O exposed to sunlight and placed on photographic plates wrapped in black paper

❧  Plates revealed an image of the uranium crystals when developed

•  1898 Isolation of radium and polonium ❧  Marie and Pierre Curie isolated from U ore

•  1899 Radiation into alpha, beta, and gamma components, based on penetration of objects and ability to cause ionization ❧  Ernest Rutherford identified alpha

•  1909 Alpha particle shown to be He nucleus ❧  Charge to mass determined by Rutherford

•  1911 Nuclear atom model ❧  Plum pudding by Rutherford

•  1912 Development of cloud chamber by Wilson •  1913 Planetary atomic model (Bohr Model) •  1914 Nuclear charge determined from X rays

❧  Determined by Moseley in Rutherford’s laboratory

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History •  1919 Artificial transmutation by

nuclear reactions ❧  Rutherford bombarded 14N with

alpha particle to make 17O •  1919 Development of mass

spectrometer •  1928 Theory of alpha radioactivity

❧  Tunneling description by Gamow •  1930 Neutrino hypothesis

❧  Fermi, mass less particle with ½ spin, explains beta decay

•  1932 First cyclotron ❧  Lawrence at UC Berkeley

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History •  1932 Discovery of neutron

❧  Chadwick used scattering data to calculate mass, Rutherford knew A was about twice Z. Lead to proton-neutron nuclear model

•  1934 Discovery of artificial radioactivity ❧  Jean Frédéric Joliot & Irène

Curie showed alphas on Al formed P

•  1938 Discovery of nuclear fission ❧  From reaction of U with

neutrons, Hahn and Meitner •  1942 First controlled fission reactor •  1945 First fission bomb tested •  1947 Development of radiocarbon

dating

Page 6: Actinide Science and Radiochemistry

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Radiochemistry Introduction •  Radiochemistry

❧  Chemistry of the radioactive isotopes and elements ❧  Utilization of nuclear properties in evaluating and understanding chemistry ❧  Intersection of chart of the nuclides and periodic table

•  Atom ❧  Z and N in nucleus (10-14 m) ❧  Electron interaction with nucleus basis of chemical properties (10-10 m)

➠  Electrons can be excited *  Higher energy orbitals *  Ionization

➘  Binding energy of electron effects ionization ❧  Isotopes

➠  Same Z different N ❧  Isobar

➠  Same A (sum of Z and N) ❧  Isotone

➠  Same N, different Z ❧  Isomer

➠  Nuclide in excited state ➠  99mTc

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Chart of the Nuclides •  Presentation of data on nuclides

❧  Information on chemical element ❧  Nuclide information

➠  Spin and parity (0+ for even-even nuclides) ➠  Fission yield

❧  Stable isotope ➠  Isotopic abundance ➠  Reaction cross sections ➠  Mass

•  Radioactive isotope ❧  Half-life ❧  Modes of decay and energies ❧  Beta disintegration energies ❧  Isomeric states ❧  Natural decay series ❧  Reaction cross sections

•  Fission yields for isobars

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Chart of Nuclides

•  Decay modes ❧  Alpha ❧  Beta ❧  Positron ❧  Photon ❧  Electron capture ❧  Isomeric transition ❧  Internal conversion ❧  Spontaneous fission ❧  Cluster decay

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Table of the Isotopes •  Detailed information about each isotope

❧  Mass chain decay scheme ❧  mass excess (M-A)

➠ Mass difference, units in energy (MeV) ❧  particle separation energy ❧  Populating reactions and decay modes ❧  Gamma data

➠ Transitions, % intensities ❧  Decay levels

➠ Energy, spin, parity, half-life ❧  Structure drawing

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Page 11: Actinide Science and Radiochemistry

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Radioelements

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Technetium •  Confirmed in a December 1936

experiment at the University of Palermo ❧  Carlo Perrier and Emilio Segrè. ❧  Lawrence mailed molybdenum foil

that had been part of the deflector in the cyclotron

❧  Succeeded in isolating the isotopes 95,97Tc

❧  Named after Greek word τεχνητός, meaning artificial ➠ University of Palermo officials

wanted them to name their discovery "panormium", after the Latin name for Palermo, Panormus

❧  Segre and Seaborg isolate 99mTc

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Promethium

•  Promethium was first produced and characterized at ORNL in 1945 by Jacob A. Marinsky, Lawrence E. Glendenin and Charles D. Coryell 

•  Separation and analysis of the fission products of uranium fuel irradiated in the Graphite Reactor

•  Announced discovery in 1947 •  In 1963, ion-exchange methods were used at

ORNL to prepare about 10 grams of Pm from used nuclear fuel

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Np synthesis •  Neptunium was the first synthetic transuranium element of the

actinide series discovered ❧  isotope 239Np was produced by McMillan and Abelson in

1940 at Berkeley, California ❧  bombarding uranium with cyclotron-produced neutrons

➠  238U(n,γ)239U, beta decay of 239U to 239Np (t1/2=2.36 days) ❧  Chemical properties unclear at time of discovery

➠  Actinide elements not in current location ➠  In group with W

•  Chemical studies showed similar properties to U •  First evidence of 5f shell •  Macroscopic amounts

❧  237Np ➠  238U(n,2n)237U

*  Beta decay of 237U ➠  10 microgram

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Pu synthesis •  Plutonium was the second transuranium element of the actinide

series to be discovered ❧  The isotope 238Pu was produced in 1940 by Seaborg,

McMillan, Kennedy, and Wahl ❧  deuteron bombardment of U in the 60-inch cyclotron at

Berkeley, California ➠  238U(2H, 2n)238Np

*  Beta decay of 238Np to 238Pu ❧  Oxidation of produced Pu showed chemically different

•  239Pu produced in 1941 ❧  Uranyl nitrate in paraffin block behind Be target bombarded

with deuterium ❧  Separation with fluorides and extraction with diethylether ❧  Eventually showed isotope undergoes slow neutron fission

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Am and Cm discovery •  Problems with identification due to chemical

differences with lower actinides ❧  Trivalent oxidation state

•  239Pu(4He,n)242Cm ❧  Chemical separation from Pu ❧  Identification of 238Pu daughter from alpha

decay •  Am from 239Pu in reactor

❧  Also formed 242Cm •  Difficulties in separating Am from Cm and

from lanthanide fission products

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Bk and Cf discovery •  Required Am and Cm as targets

❧  Needed to produce theses isotopes in sufficient quantities ➠ Milligrams

❧  Am from neutron reaction with Pu ❧  Cm from neutron reaction with Am

•  241Am(4He,2n)243Bk ❧  Cation exchange separation

•  242Cm(4He,n)245Cf ❧  Anion exchange

Dowex 50 resin at 87 °C, elute with ammonium citrate

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Einsteinium and Fermium •  Debris from Mike test

❧  1st thermonuclear test •  New isotopes of Pu

❧  244 and 246 ➠  Successive neutron capture

of 238U ❧  Correlation of log yield versus

atomic mass •  Evidence for production of

transcalifornium isotopes ❧  Heavy U isotopes followed by

beta decay •  Ion exchange used to demonstrate

new isotopes

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Md, No, and Lr discovery •  1st atom-at-a-time chemistry

❧  253Es(4H,n)256Md •  Required high degree of chemical separation •  Use catcher foil

❧  Recoil of product onto foil ❧  Dissolved Au foil, then ion exchange

•  Nobelium controversy ❧  Expected to have trivalent chemistry ❧  1st attempt could not be reproduced

➠ Showed divalent oxidation state ❧  246Cm(12C,4n)254No

➠ Alpha decay from 254No ➠ Identification of 250Fm daughter using ion

exchange •  For Lr 249, 250, 251Cf bombarded with 10,11B •  New isotope with 8.6 MeV, 6 second half life

❧  Identified at 258Lr

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Actinide trends •  Trends in actinide chemistry

❧  Oxidation states ❧  f-electron role

•  Properties based on filling 5f orbitals ❧  Hybrid bonds involving f electrons

•  5f / 6d / 7s / 7p orbitals are of comparable energies over a range of atomic numbers ❧  especially U - Am

➠  Bonding can include any orbitals since energetically similar ➠  Explains tendency towards variable valency ➠  Trend towards covalent

*  Lanthanide complexes tend to be primarily ionic *  Exploit for actinide-lanthanide separations

•  Actinide complexes complexation with π-bonding ligands •  5f / 6d / 7s / 7p orbital energies are similar

❧  orbital shifts on order of chemical binding energies ❧  Electronic structure of element in given oxidation state may vary with ligand ❧  Difficult to state which orbitals are involved in bonding

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Electronic structure •  Electronic Configurations of Actinides are not always easy to confirm •  Competition between 5fn7s2 and 5fn-16d7s2 configurations

❧  for early actinides promotion 5f 6d occurs to provide more bonding electrons ➠  much easier than corresponding 4f 5d promotion in

lanthanides ❧  second half of actinide series similar to lanthanides

➠  Similarities for trivalent lanthanides and actinides •  5f orbitals have greater extension with respect to 7s and 7p than do 4f

relative to 6s and 6p orbitals ❧  5 f electrons can become involved in bonding

➠  ESR evidence for bonding contribution in UF3, but not in NdF3 *  Actinide f covalent bond contribution to ionic bond *  Lanthanide 4f occupy inner orbits that are not

accessible •  Enhanced by relativistic effects

❧  Increased velocity of s electrons ➠  Increase mass and shielding ➠  Extension of f orbitals

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Relativistic effects

•  5f electrons extend relatively far from the nucleus compared to 4f electrons ❧  5f electrons participate in

chemical bonding •  much-greater radial extent of

probability densities for 7s and 7p valence states compared with 5f valence states

•  5f and 6d radial distributions extend farther than shown by nonrelativistic calculations

•  7s and 7p distributions are pulled closer to ionic cores in relativistic calculations

Page 23: Actinide Science and Radiochemistry

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Actinide Electronic Structure

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Absorption Spectra and Magnetic Properties •  Electronic Spectra

❧  5fn transitions ➠  narrow bands (compared

to transition metal spectra)

➠  relatively uninfluenced by ligand field effects

➠  intensities are ca. 10x those of lanthanide bands

➠  complex to interpret •  Magnetic Properties

❧  hard to interpret ❧  spin-orbit coupling is large

➠  Russell-Saunders (L.S) Coupling scheme doesn't work, lower values than those calculated

*  LS assumes weak spin orbit coupling

➘  Sum spin and orbital angular momentum

➘  J=S+L ❧  Ligand field effects are

expected where 5f orbitals are involved in bonding

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Oxidation states •  General geometries high coordination

❧  Trivalent: octahedral ❧  Tetravalent: 8 coordination or greater

•  +2 ❧  Unusual oxidation state, common only for heaviest actinides

➠  No2+ and Md2+ are more stable than Eu2+ *  5f6d promotion

❧  Divalent No stabilize by full 5f14 ➠  Element Rn5f147s2

❧  Divalent actinides similar properties to divalent lanthanides and Ba2+ •  +3

❧  Most common oxidation state across actinides ➠  all trans-Americium elements except No

❧  Of marginal stability for early actinides ➠  Pa, U

❧  General properties resemble Ln3+ and are size-dependent ➠  Binary Halides, MX3 easily prepared and hydrolyzed to MOX

❧  Binary Oxides, M2O3 known for Ac, Pu and trans-Am elements

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Oxidation states •  +4

❧  Principal oxidation state for Th ➠  similar to group 4

❧  Very important, stable state for Pa, U, Pu ❧  Tetravalent Am, Cm, Bk and Cf are easily reduced

➠  Bk4+ is more oxidizing than Ce4+ ❧  MO2 known from Th to Cf (fluorite structure) ❧  MF4 are isostructural with lanthanide tetrafluorides

➠  MCl4 only known for Th, Pa, U & Np ❧  Hydrolysis / Complexation / Disproportionation are all important in aqueous phase

•  +5 ❧  Principal state for Pa (similar to group 5) ❧  For U, Np, Pu and Am the AnO2

+ ion is known ❧  Comparatively few other An(V) species are known

➠  fluorides fluoro-anions, oxochlorides, uranates, •  +6

❧  AnO22+ ions are important for U, Np, Pu, Am UO22+ is the most stable

❧  Few other compounds e.g. AnF6 (An = U, Np, Pu), UCl6, UOF4, U(OR)6 •  +7

❧  Only the marginally stable oxo-anions of Np and Pu, (AnO53-)

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Redox chemistry •  actinides are electropositive •  Pa - Pu show significant redox chemistry

❧  all 4 oxidation states of Pu can co-exist in appropriate conditions •  stability of high oxidation states peaks at U (Np) •  redox potentials show strong dependence on pH (data for Ac - Cm)

❧  high oxidation states are more stable in basic conditions ❧  even at low pH hydrolysis occurs ❧  tendency to disproportionation is particularly dependent on pH ❧  at high pH 3Pu4+ + 2H2O PuO2

2+ + 2Pu3+ + 4H+ •  early actinides have a tendency to form complexes

❧  complex formation influences reduction potentials ➠  Am4+(aq) exists when complexed by fluoride (15 M NH4F(aq))

•  radiation-induced solvent decomposition produces H• and OH• radicals ❧  lead to reduction of higher oxidation states e.g. PuV/VI, AmIV/VI

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Actinide metals •  Preparation of actinide metals

❧  Reduction of AnF3 or AnF4 with vapors of Li, Mg, Ca or Ba at 1100 – 1400 °C

❧  Other redox methods are possible ➠  Thermal decomposition of iodine species ➠  Am from Am2O3 with La

*  Am volatility provides method of separation •  Metals tend to be very dense

❧  U 19.07 g/mL ❧  Np 20.45 g/mL ❧  Am lighter at 13.7 g/mL

•  Some metals glow due to activity ❧  Ac, Cm, Cf

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CMPO

Np Chemistry: separation •  Most methods exploit redox chemistry of Np •  Solvent extraction

❧  2-thenoyltrifluoroacetone ➠  Reduction to Np(IV)

*  Extraction in 0.5 M HNO3 *  Back extract in 8 M HNO3

➘  Oxidation to Np(V), extraction into 1 M HNO3 •  Tributylphosphate (TBP)

❧  NpO2(NO3)2(TBP)2 and Np(NO3)4(TBP)2 are extracted species ➠  Extraction increases with increase concentration of TBP and

nitric acid *  1-10 M HNO3

➠  Separation from other actinides achieved by controlling Np oxidation state

•  Carbamoylphosphine oxide (CMPO) ❧  Usually used with TBP ❧  Nitric acid solutions ❧  Separation achieved with oxidation state adjustment

➠  Reduction of Pu and Np by Fe(II) sulfamate ➠  Np(IV) extracted into organic, then removed with carbonate,

oxalate, or EDTA

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Np solution chemistry •  Np exists from 3+ to 7+

❧  Stable oxidation state favored by acidity, ligands, Np concentration

•  5+ and 6+ forms dioxocations •  Redox potentials

❧  Some variations in values ➠  Due to slow kinetics from Np-O

bond making and breaking •  Determine ratios of each redox species

from XANES ❧  Use Nernst equation to determine

potentials •  Disproportionation

❧  NpO2+ forms Np4+ and NpO2

2+

➠  Favored in high acidity and Np concentration

❧  2NpO2+ +4 H+Np4+ + NpO2

2+ + 2H2O

❧  K for reaction increased by addition of complexing reagents ➠  K=4E-7 in 1 M HClO4 and

2.4E-2 in H2SO4

•  Control of redox species important consideration for experiments

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Np solution chemistry •  Applied to Np(III) to Np(VII) and coordination

complexes ❧  Applied to Np(V) spin-orbit coupling for

5f2

•  Absorption in HNO3 ❧  Np(IV): 715 nm ❧  Np(V): weak band at 617 nm ❧  Np(VI): below 400 nm

➠  No effect from 1 to 6 M nitric •  Np(VII) only in basic media

❧  NpO65-

➠  2 long (2.2 Å) and 4 short (1.85 Å) ➠  Absorbance at 412 nm and 620 nm

*  O pi 5f *  Number of vibrational states

➘  Between 681 cm-1 and 2338 cm-1

•  Np(VI) ❧  Studies in Cs2UO2Cl4 lattice ❧  Electronic levels identified at following

wavenumbers (cm-1) ➠  6880, 13277, 15426, 17478, and

19358 *  6880 cm-1 belongs to 5f1

configuration

2 M HClO4

Np(III) Np(IV)

Np(V) Np(VI)

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Np solution chemistry •  Np hydrolysis

❧  Np(IV)>Np(VI)>Np(III)>Np(V) ❧  For actinides trends with ionic radius

•  Np(III) ❧  below pH 4 ❧  Stable in acidic solution, oxidizes in air ❧  Potentiometric analysis for

determining K ❧  No Ksp data

•  Np(IV) ❧  hydrolyzes above pH 1

➠  Tetrahydroxide main solution species in equilibrium with solid based on pH independence of solution species concentration

•  Np(V) ❧  not hydrolyzed below pH 7

•  Np(VI) ❧  below pH 3-4

•  Np(VII) ❧  No data available

•  Oxidation state trends same as hydrolysis •  Stability trends for inorganic

❧  F->H2PO4->SCN->NO3

->Cl->ClO4-

❧  CO32->HPO4

2->SO42-

•  NpO2+ forms cation-cation complexes

❧  Fe>In>Sc>Ga>Al

[mM]

pH

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Plutonium Chemistry: Metal Pu •  Ca reduction •  Pyroprocessing

❧  PuF4 and Ca metal ➠  Start at 600 ºC goes to 2000 ºC ➠  Pu solidifies at bottom of crucible

❧  Direct oxide reduction ➠  Direct reduction of oxide with Ca metal ➠  PuO2, Ca, and CaCl2

❧  Molten salt extraction ➠  Separation of Pu from Am and lanthanides ➠  Oxidize Am to Am3+, remains in salt phase ➠  MgCl2 as oxidizing agent

*  Oxidation of Pu and Am, formation of Mg *  Reduction of Pu by oxidation of Am metal

❧  Electrorefining ➠  Liquid Pu oxidizes from anode ingot into ➠  molten salt electrode ➠  740 ºC in NaCl/KCl with MgCl2 as oxidizing agent

*  Oxidation to Pu(III) *  Addition of current causes reduction of Pu(III) at cathode *  Pu drips off cathode

•  Zone refining (700-1000 ºC) ❧  Purification from trace impurities

➠  Fe, U, Mg, Ca, Ni, Al, K, Si, oxides and hydrides ❧  Melt zone passes through Pu metal at a slow rate

➠  Impurities travel in same or opposite direction of melt direction ❧  Vacuum distillation removes Am ❧  Application of magnetic field levitates Pu

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Pu phase stability •  6 different Pu solid phases

❧  7th phase at elevated pressure

❧  fcc phase least dense •  Energy levels of allotropic

phases are very close to each other ❧  Pu extremely sensitive to

changes in temperature, pressure, or chemistry •  Densities of the allotropes vary

significantly ❧  dramatic volume changes

with phase transitions •  Crystal structure of the

allotropes closest to room temperature are of low symmetry ❧  more typical of minerals

than metals. •  Pu expands when it solidifies

from a melt •  Low melting point •  Liquid Pu has very large surface

tension with highest viscosity known near the melting point.

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Pu metal phases •  Low symmetry ground state for α phase due to 5f bonding

❧  Higher symmetry found in transition metals •  f orbitals have odd symmetry

❧  Basis for low symmetry (same as p orbitals Sn, In, Sb, Te) •  If Pu had only an f band contribution equilibrium lattice constant

smaller than measured ❧  Contribution from s-p band stabilizes larger volume ❧  f band is narrow at larger volume (low symmetry)

•  strong competition between the repulsive s-p band contribution and the attractive f band term induces instability near the ground state

•  For actinides f electron bonding increases up to Pu ❧  Pu has the highest phase instability

•  At Am the f electrons localize completely and become nonbonding ❧  At Am coulomb forces pull f electrons inside the valence shell ❧  leaving 2 or 3 in the s-p and d bands

•  f-f interaction varies dramatically with very small changes in interatomic distances ❧  lattice vibrations or heating

•  f-f and f-spd interactions with temperature may results in localization as Pu transforms from the α- to the δ-phase

•  Low Pu melting temperature due to f-f interaction and phase instability ❧  Small temperature changes induce large electronic changes

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Phase never observed, slow kinetics

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Pu solution chemistry •  Originally driven by the need to separate and purify Pu •  Complicated solution chemistry

❧  Five oxidation states (III to VII) ➠  Small energy separations between oxidation states ➠  All states can be prepared

*  Pu(III) and (IV) more stable in acidic solutions *  Pu(V) in near neutral solutions

➘  Dilute Pu solutions favored *  Pu(VI) and (VII) favored in basic solutions

➘  Pu(VII) stable only in highly basic solutions and strong oxidizing conditions

❧  Some evidence of Pu(VIII) •  Pu3+ and Pu4+ simple hydrates free species •  Plutonyl oxo species for Pu(V) and Pu(VI)

❧  Pu(V) effective charge 2.2 ❧  Pu(VI) effective charge 3.2

•  PuO4-

•  Redox chemistry instrumental in identifying species

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Pu solution chemistry •  Coordination number varies

❧  Large values, 8 to 10 for water coordination

•  Spectroscopic properties ❧  5f-5f transitions

➠  More intense than 4f of lanthanides

➠  Relativistic effects accentuate spin-orbit coupling

➠  Transitions observed spectroscopically

*  Forbidden transitions *  Sharp but not very

intense •  Pu absorption bands in visible and near

IR region ❧  Characteristic for each oxidation

state

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Pu aqueous chemistry: Hydrolysis/colloids •  In many systems solubility

derived Pu(IV) concentrations vary due to colloid formation

•  Colloids are 1- to 1000-nm size particles that remain suspended in solution

•  x-ray diffraction patterns show Pu(IV) colloids are similar to the fcc structure of PuO2 ❧  Basis for theory that

colloids are tiny crystallites PuO2, ➠  May include

some water saturated of hydrated surface

•  Prepared by addition of base or water to acidic solutions

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Pu aqueous chemistry: colloids •  XAFS studies of Pu(IV) colloids

❧  demonstrated that average fcc structure is simplistic

❧  additional chemical forms are present

❧  Variations in measured Pu(IV) concentrations may be related to the local structure

❧  colloids displays many discrete Pu–O distances ➠  2.25 Å to 3.5 Å

❧  amplitude of Pu–Pu is reduced, decrease in number of nearest neighbors ➠  four H atoms

incorporated into the Pu(IV) colloid structure could result in one Pu vacancy.

❧  EXAFS reveals that many atoms in the colloid structure are distributed in a non-Gaussian way ➠  several different

oxygen containing groups are present

*  O2–,, OH-, and OH2

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Am solution chemistry •  Oxidation states III-VI in solution

❧  Am(III,V) stable in dilute acid ❧  Am(V, VI) form dioxo cations

•  Am(III) ❧  Easy to prepare (metal dissolved in acid, AmO2 dissolution)

➠  Pink in mineral acids, yellow in HClO4 when Am is 0.1 M •  Am(IV)

❧  Requires complexation to stabilize ➠  dissolving Am(OH)4 in NH4F ➠  Phosphoric or pyrophosphate (P2O7

4-) solution with anodic oxidation ➠  Ag3PO4 and (NH4)4S2O8 ➠  Carbonate solution with electrolytic oxidation

•  Am(V) ❧  Oxidation of Am(III) in near neutral solution

➠  Ozone, hypochlorate (ClO-), peroxydisulfate ➠  Reduction of Am(VI) with bromide

•  Am(VI) ❧  Oxidation of Am(III) with S2O8

2- or Ag2+ in dilute non-reducing acid (i.e., sulfuric)

❧  Ce(IV) oxidizes IV to VI, but not III to VI completely ❧  2 M carbonate and ozone or oxidation at 1.3 V

•  Am(VII) ❧  3-4 M NaOH, mM Am(VI) near 0 °C ❧  Gamma irradiation 3 M NaOH with N2O or S2O8

2- saturated solution

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Am solution chemistry •  Am(III) has 9 inner sphere waters

❧  Others have calculated 11 and 10 (XAFS) ❧  Based on fluorescence spectroscopy

➠  Lifetime related to coordination *  nH2O=(x/τ)-y

➘  x=2.56E-7 s, y=1.43 ➘  Measurement of fluorescence lifetime in H2O and

D2O

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Am solution chemistry •  Disproportionation

❧  Am(IV) ➠  In nitric and perchloric acid ➠  Second order with Am(IV)

*  2 Am(IV)Am(III) + Am(V) *  Am(IV) + Am(V)Am(III) + Am(VI)

➘  Am(VI) increases with sulfate ❧  Am(V)

➠  3-8 M HClO4 and HCl *  3 Am(V) + 4 H+Am(III)+2Am(VI)+2 H2O

➠  Solution can impact oxidation state stability

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Solution absorption spectroscopy •  Am(III)

❧  7F05L6 at 503.2 nm (ε=410 L mol cm-1) ❧  Shifts in band position and molar absorbance indicates changes in water or

ligand coordination ❧  Solution spectroscopy compared to Am doped in crystals ❧  Absorbance measured in acids and carbonate

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Cm Chemistry •  5f7 has enhanced stability

❧  Half filled orbital ➠  Large oxidation

potential for IIIIV ➠  Cm(IV) is metastable

•  Cm(III) absorbance ❧  Weak absorption in near-

violet region ❧  Solution absorbance shifted

20-30 Å compared to solid ➠  Reduction of intensity

in solid due to high symmetry

*  f-f transitions are symmetry forbidden

❧  Spin-orbit coupling acts to reduce transition energies when compared to lanthanides

•  Cm(IV) absorbance ❧  Prepared from dissolution

of CmF4 ➠  CmF3 under strong

fluorination conditions

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Atomic and spectroscopic data •  Fluoresce from

595-613 nm ❧  Attributed to

6D7/28S7/2 transition

❧  Energy dependent upon coordination environment

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Nuclear Reactors •  Products of fission

❧  Heat ❧  Neutrons

➠ Further fission ➠ Capture

* Actinides, fertile-fissile reactions ➠ Number of neutron reactions possible

❧  Fission products •  Range of initial conditions

❧  Enrichment levels ❧  Reflector

➠ Material with low neutron reaction cross section

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Nuclear reactors •  Probable neutron energy from fission is 0.7 MeV

❧  Fast reactors ➠ High Z reflector

❧  Thermal reactors need to slow neutrons ➠ Water, D2O, graphite

* Low Z and low cross section •  Power proportional to number of available neutrons

❧  Should be kept constant under changing conditions ➠ Control elements and burnable poisons

❧  k=1 (multiplication factor) ➠ Ratio of fissions from one generation to the

next * k>1 at startup

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Nuclear reactors •  Control of fission

❧  0.1 msec for neutron from fission to react ➠ Need to have tight control ➠ 0.1 % increase per generation

* 1.001^100, 10 % increase in 10 msec •  Delayed neutrons useful in control

❧  Longer than 0.1 msec ❧  0.65 % of neutrons delayed from 235U

➠ 0.26 % for 233U and 0.21 % for 239Pu •  Fission product poisons influence reactors

❧  135Xe capture cross section 3E6 barns

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Nuclear Fission •  Basic reactor components

❧  Fuel ➠  For forensics fresh and used fuel considered

❧  Cooling ➠  Air, water, CO2

❧  Cladding ❧  Moderator

➠  Protons ➠  Carbon

*  Carbon needs more collision (114 versus 18), but has smaller reaction cross section

*  Windscale and Chernobyl graphite moderated •  Demonstrate by CP-1

❧  Graphite purified from B ❧  Cd control ❧  Moisture control ❧  2 kW, air cooled

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Nuclear Reactors

•  Pu isotopes ❧  For devices, minimize 240Pu

➠ 240Pu:239Pu 0.05 to 0.07 ❧  Different ratio for power reactors

•  Submarine reactors ❧  Water both moderator and coolant ❧  Highly enriched U

➠ Relatively high levels of 238Pu

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Thorium Fuel •  Th breeds 233U

❧  Blanket or mixed fuels •  Side reactions

❧  Formation of 232U, high gamma, from 231Th ➠ 231Th (25.4 hours) beta decay to 231Pa ➠ 231Pa(n,γ)232Pa, σ=260 b ➠ 232Pa (1.31 d) beta decay to 232U

•  Reactions for 231Th production ❧  232Th(n,2n)

➠ Need high energy neutrons ❧  230Th(n,γ), 23 b ❧  Decay of 235U

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Plutonium isotopics

•  Pu formed in core or from blanket ❧  U blanket may have a range of isotopic

composition ➠ Natural and anthropogenic

•  Pu formation from neutron capture on 238U ❧  239Pu becomes a target for higher isotope

production ➠ (n,γ) up to 241Pu ➠ Also some (n,2n) Emin =5.7 MeV

* 238Pu from 239Pu

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Plutonium isotopics

•  238Pu can also be produced through successive neutron capture on 235U ❧  235U(n,γ)236U ❧  236U(n,γ)237U ❧  237U beta decay to 237Np ❧  237Np(n,γ)238Np ❧  238Np beta decay to 238Pu

•  Mixture of Pu isotopics from fuel or blanket can act as a signature ❧  239Pu dominates at low burnups

➠ Device Pu has 6 % 240Pu

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Plutonium isotopics •  Neutron behavior and Pu isotopics coupled

❧  Pu isotopics influence by neutron fluence and energy

❧  neutron kinetic energy effected by reactor operating temperature

❧  Moderator influence due to rate of moderation ❧  Fuel size influences distance between neutron

generation and moderator ❧  Fuel composition can influence neutron

spectrum ➠ Depletion of neutron in 235U resonance

region

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Plutonium isotopics

•  Fluence influence ❧  240Pu production

➠ Capture on 239Np produces 240Np, which decays into 240Pu

➠ Competition between capture and decay

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Plutonium isotopics •  Computation from ORIGEN2 (average

composition) ❧  http://www-rsicc.ornl.gov/codes/ccc/ccc3/

ccc-371.html ❧  d isotope/dt integrated for spectrum of

neutron energies ➠ Relates to reactor type

❧  Net isotope formation for given conditions ➠ Reactor type library ➠ Decay constants

❧  Fuel composition input ➠ Solves for time and reactor power

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Plutonium isotopics •  ORIGEN does not consider variation of Pu production

in different fuel locations ❧  Actinides on edge of fuel experience softer neutron

spectra then center material ➠ Pu distribution varies with depth

* Isotopics and ratios with fission products vary

❧  Location of control elements also an influence •  ORIGEN useful for bulk •  Influence of moderator, enrichment, and burnup

greater than reactor power and operating temperature ❧  No ORIGEN library for graphite moderated

reactors for weapons Pu production

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Plutonium Isotopics

•  Evaluate ratios with 240Pu ❧  Mass 240:239

(MS) ❧  Activity 238/

(239+240) (alpha spectroscopy)

•  Varied reactor types, 37.5 MW/ton

•  Large Pu isotopic variation

•  Obvious variation for blanket and CANDU

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Plutonium Isotopics •  Comparison to

239Pu concentration ❧  Can provide

time since discharge ➠ 241Pu is time

sensitive •  Change in measure

and expect ratio can be used to determine time since discharge

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Plutonium Isotopics

•  Use for evaluating reactor power ❧  Mass

242:239 ration

❧  Activity 239/(239+240)

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Transplutonium Isotopics •  Am (242m, 243) and Cm (242, 244) sensitive to reactor

power ❧  Due to relative decay to 241Pu and formation of

241Am ➠ More 241Am is available for reactions from

longer times with low flux * Weapons grade Pu from 10 day to 2 year

irradiation •  From neutron reaction and beta decay of heavier Pu •  243Pu beta decay to 243Am

❧  Capture and decay to 244Cm •  Neutron capture on 241Am

❧  242Am states ❧  Ground state decay to 242Cm

•  Strong flux dependence on ratios

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6% 240Pu

•  244Cm and 243Am arise from multiple neutron capture on 241Pu

•  242Cm (t1/2=163 d) can determine time since discharge ❧  Change from expected value compared to other ratios

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Reprocessing •  Used nuclear fuel •  238Pu production •  233U production •  In fuel, fission products build up fast than Pu isotopes

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Reprocessing •  510 gU/g Pu for used fuel •  Majority of U remains, enrichment level to 0.62%

❧  Depends upon the level of burnup •  Reprocessing limitations

❧  Remote handling ❧  Criticality issues ❧  Limit impurities

•  Range of reprocessing techniques ❧  Precipitation ❧  Molten salt ❧  Ion exchange ❧  Fluoride volatility ❧  Solvent extraction

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Reprocessing •  BUTEX

❧  Dibutyl carbitol solvent ➠ Relatively poor separation from Ru

* 1E3 rather than 1E6 ➠ 1 g Pu has 1E7 dpm 106Ru

•  HEXONE ❧  Methylisobutylketone solvent ❧  Decontamination factors

➠ 1E4 Ru ➠ 1E5 for Zr, Nb, and Ce

* 1 g Pu has 1000 dpm 93Zr

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Reprocessing •  PUREX

❧  Zr, Tc, and Ru observed ❧  Ln, Np, and Th nonmegligible ❧  Nd is a key isotope, nature levels in reprocessing materials

➠  Natural and reactor Nd radios are plant signatures

35

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•  Isotopes in Pu from incomplete separation and decay

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Reprocessing •  Organic analysis

❧  Radiation effects ➠ Polymerization ➠ TBP degradation

* Di, mono, and phosphoric acid ➠ N-butonal and nitrobutane

•  Changes extraction behavior, limits extraction efficiency ❧  Formation of carboxylic acid, esters, ketones,

nitroorganic compounds •  Signatures from processing

❧  Range of sample states, including gas ❧  GC-MS methods

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Metals and Alloys •  Range of behavior

and phases for actinide metals ❧  Due to f-

electron behavior

•  Similarities for Th, U, and Pu ❧  Oxide coating ❧  Need of

complexing agent for dissolution in nitric acid

•  U and Pu pyrophoric •  Th limited solubility

in liquid U

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Metals and alloys •  Formation of metals from reaction of metal halides

with reducing elements ❧  Na, Ca, Mg

➠ Group 1 and 2 halide formation favored up to 1500 ºC

➠ Na has low boiling point relative to metal melting point

➠ Ca reaction extremely exothermic, melts reaction products

➠ MgF2 and CaF2 not soluble in molten U * Mg needs to limit formation of U oxides

due to solubility •  Reaction vessel must be coated to be inert

❧  CaF2, MgF2, BeO, ThO2, graphite (Mg only)

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Metals and alloys

•  Can also be formed from molten salt processes ❧  UF3 of UF4 in KCl/NaCl

➠ Reduction of U to metallic state ❧  Grain size determined by temperature and

current density •  Hydride/dehydriding results in high surface area U

❧  Too pyrophoric for use •  U metal purification by melting in vacuum under

Ar ❧  Graphite crucibles lined with CaO, MgO, or

ZrO2

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Metals and alloys •  Th metal from Ca reaction

❧  Higher Th melting point make reaction less energetic

❧  May require initiator ➠ I2, S, ZnCl2

•  For Th oxide with Ca, reaction in Ni boat ❧  Dissolve Ca product in water

➠ Need to consider Th metal dissolution kinetics

•  Th metal casting in BeO ❧  alumina, MgO, or CaO dissolve in Th metal

•  High purity Th from formation of volatile ThI4 ❧  Condense on cool surface

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Metals and alloy

•  For Pu reaction with oxides rather than fluorides limits neutron formation ❧  19F(α,n) ❧  CaO will coat Pu product, need to dissolve

dilute nitric acid •  Hydrogenation reaction

❧  Pu and PuH2+x

❧  Free from oxygen

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Review

•  Radiochemistry ❧  Interface between nucleus and electrons

•  Actinides ❧  Formed by nuclear reactions

➠ Natural (r-process) ➠ Synthetic reactions

•  Actinide chemistry influenced by 5f electrons •  Analytical methods key to nuclear forensics

methods from the nuclear fuel cycle