HTO and selenate diffusion through compacted Na-, Na–Ca-, and Ca-montmorillonite

• Published in: Applied geochemistry Vol. 170; p. 106090
• Main Authors: Fox, Patricia M., Tournassat, Christophe, Steefel, Carl, Nico, Peter S.
• Format: Journal Article
• Language: English
• Published: United States Elsevier Ltd 01.09.2024; Elsevier
• Subjects: Anion exclusion; Engineered barriers; Interlayer cation; Radioactive waste; Sciences of the Universe; Selenium diffusion; Interlayer cation; Selenium diffusion; Anion exclusion; Radioactive waste; Engineered barriers; Selenium diffusion radioactive waste interlayer cation engineered barriers anion exclusion; interlayer cation; radioactive waste; anion exclusion; engineered barriers
• ISSN: 0883-2927; 1872-9134
• DOI: 10.1016/j.apgeochem.2024.106090

Radionuclide transport in smectite clay barrier systems used for nuclear waste disposal is controlled by diffusion, with adsorption significantly retarding transport rates. While a relatively minor component of spent nuclear fuel, 79Se is a major driver of the safety case for spent fuel disposal due to its long half-life (3.3 × 105 yr) and its low adsorption to clay (KD < 10 L/kg), thus a thorough understanding of Se diffusion through clay is critical for understanding the long-term safety of spent fuel disposal systems. Through-diffusion experiments with tritiated water (HTO, conservative tracer) and Se(VI) were conducted with a well-characterized, purified montmorillonite source clay (SWy-2) under a constant ionic strength (0.1 M) and three different electrolyte compositions: Na+, Ca2+, and a Na + -Ca2+ mixture at pH 6.5 in order to probe the effects of electrolyte composition and interlayer cation composition on clay microstructure, Se(VI) aqueous speciation, and ultimately diffusion. The results were modeled using a reactive transport modeling approach to determine values of porosity (ε), De (effective diffusion coefficient), and KD (distribution coefficient for adsorption). HTO diffusive flux was higher in Ca-montmorillonite (De = 1.68 × 10−10 m2 s−1) compared to Na-montmorillonite (De = 7.83 × 10−11 m2 s−1). This increase in flux is likely due to a greater degree of clay layer stacking in the presence of Ca2+ compared to Na+, which leads to larger inter-particle pores. Overall, the Se(VI) flux was much lower than the HTO flux due to anion exclusion, with Se(VI) flux following the order Ca (De = 1.03 × 10−11 m2 s−1) > Na–Ca (De = 2.12 × 10−12 m2 s−1) > Na (De = 1.28 × 10−12 m2 s−1). These differences in Se(VI) flux are due to a combination of factors, including (1) larger accessible porosity in Ca-montmorillonite due to clay layer stacking and smaller electrostatic effects compared to Na-montmorillonite, (2) larger accessible porosity for neutral-charge CaSeO4 species which makes up 32% of aqueous Se(VI) in the pure Ca system, and (3) possibly higher Se(VI) adsorption for Ca-montmorillonite. Through a combination of experimental and modeling work, this study highlights the compounding effects that electrolyte and counterion compositions can have on radionuclide transport through clay. Diffusion models that neglect these effects are not transferable from laboratory experimental conditions to in situ repository conditions. •Selenate diffusion through clay is limited by anion exclusion.•Clay layer stacking in Ca-montmorillonite promotes higher HTO and Se diffusion.•Formation of neutral aqueous CaSeO4 species increases Se(VI) flux.•Models must consider aqueous speciation to be applied repository conditions.