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Published byMarcus Grant Modified over 9 years ago
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Surface Analysis Surface interface controls many aspects of chemistry
Catalysts Corrosion Thin films Surfaces Methods
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Surface Boundary between solid and other phase Gas, vacuum, liquid
Surface differs from solid bulk Decarburised surface layer on the seal rim. Preferential grain boundary oxidation evident
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Spectroscopic Surface Methods
Incident beam and secondary beam Photons, electrons Incident particle not same as secondary
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X-ray photoelectron spectroscopy
Examination of surface with x-rays and measurement of electrons Evaluation of elements on surface by x-rays and Auger A+g->A+*+e- Electron energy (Ek) is measured Eb=g-Ek-w w is work function
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XPS The momentum p of the outgoing electron is determined from the kinetic energy
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XPS spectra Chemical shifts can be observed
Variation with oxidation state Substituant groups
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Auger Electron Spectroscopy
A+e1-->A+*+e1-’+eA- Relaxation can occur in two ways A+* => A++ + eA- eA- = Auger electron A+* => A+ + gf Auger emission types KLL LMM MNN Removal, transition to removed state, ejection of electron favored by low atomic number elements hnf => fluorescence photon
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Auger Electron Spectroscopy
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Similar to other procedures for fuel preparation
Ceramic Synthesis Dried at 90°C Calcination, Reduction, Sintering Final Product Precipitate-acetone mix from Zr, Th, U salts with NH4OH ≈5 g total salt Similar to other procedures for fuel preparation
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Ceramic Synthesis Parameters
Use of H2 and reduction step examined Calcination Performed in air at 750 oC for one hour Reduction One hour at 600 oC under Ar/4% H2 Powders placed in 5 mm die and cold pressed at 55 MPa for 1-2 minutes Low pressure, higher surface area Not to standard fuel surface areas Sintering Performed in air or Ar/4% H2(g) at 1500 oC for 4 hours
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Ceramic Characterization
EDX (Energy Dispersive X-ray) (e-) Emission of characteristic X-rays XRD (X-ray diffraction) (g) EELS (Electron Energy Loss Spectroscopy) (e-) Loss of energy by monoenergetic e- Can be used to determine oxidation state 3d3/2 -> 5f5/2 (M4) and 3d5/2 -> 5f7/2 (M5) ratio Based on lanthanides XANES/EXAFS (g) Oxidation state and near neighbor chemistry
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Element bright in EDX mapping
EDX Results 0.5m TEM Picture Th Zr U Mg Element bright in EDX mapping Two phases found Low mutual solubility of Zr and Th Zr rich and Th rich phase Little solubility of Th in Zr U and Mg distributed throughout the ceramic
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XRD Results: Standards
U3O8 ThO2 UO2
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Influence of synthesis conditions
Zr6Th3UO20 Calcined in air/No reduction Calcined in air/Reduction No effect on the inclusion of reduction step: U as U(IV)
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XRD Results U is reduced to the tetravalent state in Zr-Th-U ceramic
Th and Zr stabilize tetravalent U Calcine in air, no reduction step, sinter under Ar/4% H2 Zr-U ceramic requires reduction step Calcination performed under reducing conditions more U incorporated into the ZrO2 lattice structure Unit Cell Measured for Th3UO8 Å
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Th-U solid solution cell parameters
Black points from Hubert et al (2001)
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EELS Spectra ZrTh3UO10
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EELS analysis Evaluation of U oxidation state
Multiple analysis of samples Evaluation of M4/M5 ratio for U UO2: 0.41±0.03 U3O8: 0.48±0.04 Th3UO8: 0.40±0.03 ZrTh3UO10: 0.40±0.03 Tetravalent U for above samples U oxidation with higher Zr is noted in some samples Air ingress into furnace
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X-ray Absorption Spectroscopy
Utilizes x-rays from synchrotron source to probe local structure High intensity, broad spectral range Spectra can be separated into regions containing different information Global technique yields average structure of sample
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XAS setup
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XAS spectrum
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XANES Spectroscopy X-Ray Absorption Near Edge Structure
Region between absorption edge and start of EXAFS oscillations, up to 40 eV above edge Absolute position of edge contains information on oxidation state Also contains information on vacant orbitals, electronic configuration, and site symmetry
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EXAFS Spectroscopy X-ray Absorption Fine Structure
Above absorption edge, photoelectrons created by absorption of x-ray Backscattering photoelectrons effect x-ray absorption Oscillations in absorption above edge Oscillations used to determine atomic number Distance coordination number of nearest neighbors
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XAS Procedure Scanned U, Th, and Zr separately Th L 3 edge to k = 13
U L 3 edge to k = 14 Zr K edge to k = 14 U L 2 edge also scanned Th EXAFS interference in U spectra due to proximity of edges
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Th and U Edges
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Uranium XANES Tetravalent U for Zr=0 or 1
U oxidation evident with higher Zr Agrees with EELS
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Th3UO8 EXAFS
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EXAFS Analysis EXAFS equation
Phase(k) and Amp(k) calculated from theory Fit data to determine: N coordination number R bond length s Debye-Waller term
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EXAFS Zr and U interchangeability limited Mg affects U solubility
Increase in Mg decrease in U solubility ThO2 structure U and Th completely interchangeable in lattice Th-Th(U): Å Th-O: Å
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Th-Th(U) and Th-O distance
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Characterization Results
Two phases Th rich and Zr rich Tetravalent U in ZrTh3UO10 and Th3UO8 Identified by EELS and XANES Unit Cell Parameter and Th interatomic distances agree with other work Solubility Experiments pH 4, 7, and 10 under Ar, pH 4, 5.25, 6.5 under Ar/10% CO2 Collect samples up to 5 months
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