Fuel Cycle Chemistry • Chemistry in the fuel cycle Uranium Separation Fluorination and enrichment • Chemistry in fuel speciation • Fundamental of fission products and actinides Production Solution chemistry Speciation Spectroscopy • Focus on chemistry in the fuel cycle Speciation (chemical form) Oxidation state Ionic radius and molecular size 11-1 Reactor basics • Utilization of fission process to create heat Heat used to turn turbine and produce electricity • Requires fissile isotopes 233U, 235U, 239Pu Need in sufficient concentration and geometry • 233U and 239Pu can be created in neutron flux • 235U in nature Need isotope enrichment induced fission cross section for 235U and 238U as function of the neutron energy. 11-2 Nuclear properties • Fission properties of uranium Defined importance of element and future investigations Identified by Hahn in 1937 200 MeV/fission 2.5 neutrons • Natural isotopes 234,235,238U Ratios of isotopes established 234: 0.005±0.001 235: 0.720±0.001 238: 99.275±0.002 • 233U from 232Th 11-3 Uranium chemistry • Separation and enrichment of U • Uranium separation from ore Solvent extraction Ion exchange • Separation of uranium isotopes Gas centrifuge Laser 11-4 Natural U chemistry • Natural uranium consists of 3 isotopes 234U, 235U and 238U • Members of the natural decay series Earth’s crust contains 3 - 4 ppm U As abundant as As or B • U is also chemically toxic Precautions should be taken against inhaling uranium dust Threshold limit is 0.20 mg/m3 air About the same as for lead • U is found in large granitic rock bodies formed by slow cooling of the magma about 1.7 - 2.5 E 9 years ago 11-5 Natural U chemistry • • • • • • U is also found in younger rocks at higher concentrations called “ore bodies” Ore bodies are located downstream from mountain ranges Atmosphere became oxidizing about 1E9 years ago Rain penetrated into rock fractures, oxidizing the uranium to U(VI) Dissolving it as an anionic carbonate or sulfate complexes Water and the dissolved U migrated downstream, reducing material was encountered forming ore bodies * Reduction to insoluble U(IV) (U4+) compounds Most important mineral is uraninite (UO2+x, x = 0.01 to 0.25) Inorganic (pyrite) or organic (humic) matter Uranium concentration is 50 - 90% Carnotite (a K + U vanadate) 54% U U is often found in lower concentrations, of the order of 0.01 - 0.03% in association with other valuable minerals such as apatite (phosphate rock), shale, or peat 11-6 Uranium minerals URANINITE UO2 uranium oxide CARNOTITE K2(UO2)2(VO4)2• 1-3 H2O hydrated potassium uranyl vanadate AUTUNITE Ca(UO2)2(PO4)2•10 H2O11-7 hydrated calcium uranyl phosphate. Uranium solution chemistry • Uranyl(VI) most stable in solution Uranyl(V) and U(IV) can also be in solution U(V) prone to disproportionation Stability based on pH and ligands Redox rate is limited by change in species Making or breaking yl oxygens * UO22++4H++2e-U4++2H2O • yl oxygens have slow exchange Half life 5E4 hr in 1 M HClO4 Rate of exchange catalyzed by UV light • yl forms from f orbitals in U 11-8 Aqueous solution complexes • Strong Lewis acid • Hard electron acceptor F->>Cl->Br-I Same trend for O and N group based on electrostatic force as dominant factor • Hydrolysis behavior U(IV)>U(VI)>>>U(III)>U(V) • Uranium coordination with ligand can change protonation behavior HOCH2COO- pKa=17, 3.6 upon complexation of UO2 Inductive effect * Electron redistribution of coordinated ligand * Exploited in synthetic chemistry • U(III) and U(V) No data in solution Base information on lanthanide or pentavalent actinides 11-9 Uranyl chemical bonding • • Bonding molecular orbitals sg2 su2 pg4 pu4 Order of HOMO is unclear * pg< pu< sg<< su proposed Gap for s based on 6p orbitals interactions 5fd and 5ff LUMO Bonding orbitals O 2p characteristics Non bonding, antibonding 5f and 6d Isoelectronic with UN2 Pentavalent has electron in non-bonding orbital 11-10 11-11 11-12 Uranyl chemical bonding • Linear yl oxygens from 5f characteristic 6d promotes cis geometry • yl oxygens force formal charge on U below 6 Net charge 2.43 for UO2(H2O)52+, 3.2 for fluoride systems Net negative 0.43 on oxygens Lewis bases * Can vary with ligand in equatorial plane * Responsible for cation-cation interaction * O=U=O- - -M * Pentavalent U yl oxygens more basic • Small changes in U=O bond distance with variation in equatoral ligand • Small changes in IR and Raman frequencies Lower frequency for pentavalent U Weaker bond 11-13 11-14 Acid-Leach Process for U Milling U ore Water H2SO4 40-60°C Steam NaClO3 Crushing & Grinding Slurry Acid Leaching Separation Tailings Solvent Extraction Recovery, Precipitation Drying (U3O8) Organic Solvent NH4+ 11-15 In situ mining Acidic solution (around pH 2.5) 11-16 Uranium purification • TBP extraction Based on formation of nitrate species UO2(NO3)x2-x + (2-x)NO3- + 2TBP UO2(NO3)2(TBP)2 11-17 Solvent Extraction • • • • • Two phase system for separation Sample dissolved in aqueous phase Normally acidic phase Aqueous phase contacted with organic containing ligand Formation of neutral metal-ligand species drives solubility in organic phase Organic phase contains target radionuclide May have other metal ions, further separation needed Variation of redox state, contact with different aqueous phase Back extraction of target radionuclide into aqueous phase Distribution between organic and aqueous phase measured to evaluate chemical behavior 11-18 Solvent extraction • • Distribution coefficient [M]org/[M]aq=Kd Used to determine separation factors for a given metal ion Ratio of Kd for different metal ions Distribution can be used to evaluate stoichiometry Plot log Kd versus log [X], slope is stoichiometry 11-19 U Fluorination HNO3 U ore concentrates Solvent extraction purification Conversion to UO3 H2 Reduction UO2 HF UF4 Mg U metal F2 UF6 MgF2 11-20 Fuel Fabrication Enriched UF6 Calcination, Reduction Pellet Control 40-60°C UO2 Tubes Fuel Fabrication Other species for fuel nitrides, carbides Other actinides: Pu, Th 11-21 U enrichment • Utilizes gas phase UF6 Gaseous diffusion lighter molecules have a higher velocity at same energy * Ek=1/2 mv2 For 235UF6 and 238UF6 • 235UF6 impacts barrier more often 11-22 Gas centrifuge • Centrifuge pushed heavier 238UF6 against wall with center having more 235UF6 Heavier gas collected near top • Enriched UF6 converted into UO2 UF6(g) + 2H2OUO2F2 + 4HF Tc follows light U fraction if present • Ammonium hydroxide is added to the uranyl fluoride solution to precipitate ammonium diuranate 2UO2F2 + 6NH4OH (NH4)2U2O7 + NH4F + 3 H2O • Calcined in air to produce U3O8 and heated with hydrogen to make UO2 Final Product 11-23 • • • • • Laser Enrichment Based on photoexcitation Atomic Vapor Laser Isotope Separation (AVLIS) Molecular Laser Isotope Separation (MLIS) Separation of Isotopes by Laser Excitation (SILEX). All use laser systems, optical systems, and separation module system AVLIS used a uranium-iron (UFe) metal alloy Three excitation wavelengths used SILEX and MLIS use UF6 238U absorption peak 502.74 nm, 235U is 502.73 nm Use of tunable lasers so only 235U is excited Then excited to ion state Charge separation by electrostatic 11-24 Radiochemistry in reactor • Speciation in irradiated fuel • Utilization of resulting isotopics • Fuel confined in reactor to fuel region Potential for interaction with cladding material Initiate stress corrosion cracking Chemical knowledge useful in events where fuel is outside of cladding • Some radionuclides generated in structural material 11-25 Radionuclides in fresh fuel • Actual Pu isotopics in MOX fuel may vary Activity dominated by other Pu isotopes Ingrowth of 241Am MOX fuel fabrication in glove boxes 11-26 Fission process • • • Recoil length about 10 microns, diameter of 6 nm About size of UO2 crystal 95 % of energy into stopping power Remainder into lattice defects * Radiation induced creep High local temperature from fission 3300 K in 10 nm diameter Delayed neutron fission products 0.75 % of total neutrons 137-139I and 87-90Br as examples Some neutron capture of fission products eff sf 11-27 Fuel variation during irradiation • • • • Chemical composition Radionuclide inventory Pellet structure Higher concentrations of Ru, Rh, and Pd in Pu fuel • Total activity of fuel effected by saturation Tends to reach maximum • Radionuclide fuel distribution studied Fission gas release Axial distribution by gamma scanning Radial distribution to evaluate flux 11-28 Perovskite phase (A2+B4+O3) • Most fission products homogeneously distributed in UO2 matrix • With increasing fission product concentration formation of secondary phases possible Exceed solubility limits in UO2 • Perovskite identified oxide phase U, Pu, Ba, Sr, Cs, Zr, Mo, and Lanthanides Mono- and divalent elements at A • Mechanism of formation Sr and Zr form phases Lanthanides added at high burnup 11-29 Epsilon phase • Metallic phase of fission products in fuel Mo (24-43 wt %) Tc (8-16 wt %) Ru (27-52 wt %) Rh (4-10 wt %) Pd (4-10 wt %) • Grain sizes around 1 micron • Concentration nearly linear with fuel burnup 5 g/kg at 10MWd/kg U 15 g/kg at 40 MWd/kg U 11-30 Epsilon Phase • Formation of metallic phase promoted by higher linear heat high Pd concentrations (20 wt %) indicate a relatively low fuel temperature Mo behavior controlled by oxygen potential High metallic Mo indicates O:M of 2 O:M above 2, more Mo in UO2 lattice 11-31of the Relative partial molar Gibbs free energy of oxygen fission product oxides and UO2 Properties of fission products in oxide fuel 11-32 Burnup • • • Measure of extracted energy Fraction of fuel atoms that underwent fission %FIMA (fissions per initial metal atom) Actual energy released per mass of initial fuel Gigawatt-days/metric ton heavy metal (GWd/MTHM) Megawatt-days/kg heavy metal (MWd/kgHM) Burnup relationship Plant thermal power times days of dividing by the mass of the initial fuel loading Converting between percent and energy/mass by using energy released per fission event. typical value is 200 MeV/fission 100 % burnup around 1000 GWd/MTHM Determine burnup Find residual concentrations of fissile nuclides after irradiation Burnup from difference between final and initial values Need to account for neutron capture on fissile nuclides Find fission product concentration in fuel Need suitable half-life Need knowledge of nuclear data * cumulative fission yield, neutron capture cross section Simple analytical procedure 137Cs(some migration issues) 142Nd(stable isotope), 152Eu are suitable fission products Neutron detection also used 11-33 Need to minimize 244Cm Fuel variation during irradiation 11-34 Radionuclide Inventories • Fission Products generally short lived (except 135Cs, 129I) ß, emitters geochemical behavior varies • Activation Products Formed by neutron capture (60Co) ß, emitters Lighter than fission products can include some environmentally important elements (C,N) • Actinides alpha emitters, long lived 11-35 Plutonium • Isotopes from 228≤A≤247 • Important isotopes 238Pu 237Np(n,)238Np * 238Pu from beta decay of 238Np * Separated from unreacted Np by ion exchange Decay of 242Cm 0.57 W/g Power source for space exploration * 83.5 % 238Pu, chemical form as dioxide * Enriched 16O to limit neutron emission 6000 n s-1g-1 0.418 W/g PuO2 150 g PuO2 in Ir-0.3 % W container 11-36 Pu nuclear properties • 239Pu 2.2E-3 W/g Basis of formation of higher Pu isotopes 244-246Pu first from nuclear test • Higher isotopes available Longer half lives suitable for experiments 11-37 11-38 Questions 1. What drives the speciation of actinides and fission products in spent nuclear fuel? What would be the difference between oxide and metallic fuel? 2. Describe two processes for enriching uranium. Why does uranium need to be enriched? What else could be used instead of 235U? 3. What are the similarities and differences between lanthanides and actinides? 4. What are some trends in actinide chemistry? 11-39 Pop Quiz • What are the influences of 5f electrons on the chemistry of the actinides? 11-40