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. 2022 Jan 19;7(4):3462-3469.
doi: 10.1021/acsomega.1c05838. eCollection 2022 Feb 1.

Oxygen Isotope Fractionation in U3O8 during Thermal Processing in Humid Atmospheres

Affiliations

Oxygen Isotope Fractionation in U3O8 during Thermal Processing in Humid Atmospheres

Michael R Klosterman et al. ACS Omega. .

Abstract

The incorporation of oxygen isotopes from water into uranium oxides during industrial processing presents a pathway for determining a material's geographical origin. This study is founded on the hypothesis that oxygen isotopes from atmospheric water vapor will exchange with isotopes of oxygen in solid uranium oxides during thermal processing or calcination. Using a commonly encountered oxide, U3O8, the exchange kinetics and equilibrium fractionation with water vapor (in a concentration range of 50-55% relative humidity) were investigated using processing temperatures of 400, 600, and 800 °C. In an atmosphere containing only water vapor diluted in N2, oxygen isotope equilibration in U3O8 occurred within 12 h at 400 °C and within 2 h at 600 and 800 °C. Fractionation factors (1000lnα, U3O8-H2O) between the water and oxide were -12.1, -11.0, and -8.0 at 400, 600, and 800 °C, respectively. With both humidity and O2 present in the calcining atmosphere, isotopic equilibration is attained within 2 h at and above 400 °C. In this mixed atmosphere, which was designed to emulate Earth's troposphere, isotopes are incorporated preferentially from water vapor at 400 °C and from O2 at 600 and 800 °C. Rapid and temperature/species-dependent isotope exchange also elucidated the impact of retrograde exchange in humid air, showing a shift from O2-dependent to H2O-dependent fractionation as U3O8 cooled from 800 °C. These results confirm that uranium oxides inherit oxygen isotopes from humidity during thermal processing, illuminating an important mechanism in the formation of this forensic signature.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Figure 1
Figure 1
Setup for calcination experiments. Water vapor diffuses through membrane tubing submerged in the reservoir and is subsequently diluted with a second stream of dry gas. The RH is controlled by flowmeters for each gas stream.
Figure 2
Figure 2
U3O8_d (δ18O = −43.3‰) was calcined in an atmosphere of vapor from H2O_e (δ18Ov = −8.8‰) diluted to 50–55% RH in N2. Samples heated at 600 and 800 °C appear to achieve equilibrium with water vapor within 2 h, while U3O8 calcined at 400 °C reaches equilibrium within 2–12 h.
Figure 3
Figure 3
Oxygen isotope fractionation factors between U3O8 and water vapor compared to calculated fractionation for other U-oxides from equations provided by Hattori and Halas and Zheng.,
Figure 4
Figure 4
U3O8_e (δ18O = −16.7‰) was calcined in an atmosphere of vapor from H2O_d (δ18Ov = −26.2‰) diluted to 50–55% RH in dry air (δ18OO2 = +23.2‰). Samples calcined at 400, 600, and 800 °C all appear to equilibrate within 2 h.
Figure 5
Figure 5
Fractionation between U3O8 and water vapor [top] and fractionation between U-oxides and atmospheric O2 [bottom] during 72 hr calcining experiments. Data for fractionation between UOx and dry air (N2/O2, gray squares) are reproduced from Klosterman et al., with amorphous UO3 at 400 °C and U3O8 at 600 and 800 °C and calcination times of 20 h.
Figure 6
Figure 6
δ18O values for U3O8 (initial δ18O = −16.7‰) calcined for 1 h in a mixed atmosphere (18O-depleted H2O vapor + air with 18O-enriched O2). U3O8 was cooled from 800 °C in either an inert atmosphere or the mixed atmosphere at different rates.

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