Pb Sorption at the Barite (001)-Water Interface

Jacquelyn N. Bracco, Sang Soo Lee, Inva Braha, Amanda Dorfman, Paul Fenter, Andrew G. Stack

Research output: Contribution to journalArticlepeer-review

9 Scopus citations

Abstract

Sorption of ions at the mineral-water interface is an important factor that determines the fate of toxic metals in the environment. Here, we use barite as a model substrate to understand the interaction of toxic-metal lead (Pb) with ionic crystals. The coverage and location of Pb sorbed to the (001) surface was measured as a function of aqueous Pb concentration ([Pb]aq) using in situ specular resonant anomalous X-ray reflectivity (RAXR) to determine the sorption capacity and process. The results show that Pb sorption occurs via incorporation (primarily within the top barite layer ∼3 Å in depth) and adsorption (mostly as an inner-sphere complex at ∼2 Å in height) simultaneously. Both the incorporated and adsorbed Pb coverages increase with increasing [Pb]aq up to [Pb]aq ≈ 200 μM, above which the adsorbed fraction increases more rapidly than the incorporated fraction. This enhanced adsorption has a height distribution that is further extended (≥15 Å from the surface) than that observed in lower [Pb]aq. This change in distribution is interpreted as arising from additional sorption of outer-sphere species or Pb-bearing phases precipitated on the surface. Desorption experiments in Pb-free solutions show that the incorporated fraction is more resistant to removal than the adsorbed fraction, consistent with the speciation-dependent stabilities premised in the classical sorption models.

Original languageEnglish
Pages (from-to)22035-22045
Number of pages11
JournalJournal of Physical Chemistry C
Volume124
Issue number40
DOIs
StatePublished - Oct 8 2020

Funding

The authors would like to gratefully acknowledge Peng Yang and four anonymous reviewers for the comments on this manuscript. This work was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Chemical Sciences, Geosciences, and Biosciences Division. This research used the resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by the Argonne National Laboratory under Contract no. DE-AC02-06CH11357. We acknowledge the support of GeoSoilEnviroCARS (Sector 13), which is supported by the National Science Foundation—Earth Sciences (EAR-1634415), and the Department of Energy, Geosciences (DE-FG02-94ER14466). The U.S. Government retains for itself, and others acting on its behalf, a paid-up nonexclusive, irrevocable worldwide license in the said article to reproduce, prepare derivative works, distribute copies to the public, and perform publicly and display publicly, by or on behalf of the Government.

FundersFunder number
National Science Foundation—Earth SciencesEAR-1634415
U.S. Department of EnergyDE-FG02-94ER14466
Office of Science
Basic Energy Sciences
Argonne National LaboratoryDE-AC02-06CH11357
Chemical Sciences, Geosciences, and Biosciences Division

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