A review of current knowledge concerning dry deposition of atmospheric mercury

• Published in: Atmospheric environment (1994) Vol. 43; no. 37; pp. 5853 - 5864
• Main Authors: Zhang, Leiming, Wright, L. Paige, Blanchard, Pierrette
• Format: Journal Article
• Language: English
• Published: Kidlington Elsevier Ltd 01.12.2009; Elsevier
• Subjects: Air–surface exchange; Applied sciences; Atmospheric pollution; Dry deposition velocity; Earth, ocean, space; Exact sciences and technology; External geophysics; Measurement and modelling; Meteorology; Pollution; Speciated mercury; Measurement and modelling; Dry deposition velocity; Air–surface exchange; Speciated mercury; Atmospheric fallout; Pollutant behavior; Deposition rate; Air; Review; Advanced infrared sounder; Modeling; Dry deposition; Air-surface exchange; Heavy metal; Transport process; Trace element; Air pollution; Poison; Mercury
• ISSN: 1352-2310; 1873-2844
• DOI: 10.1016/j.atmosenv.2009.08.019

The status of the current knowledge concerning the dry deposition of atmospheric mercury, including elemental gaseous mercury (Hg 0), reactive gaseous mercury (RGM), and particulate mercury (Hg p), is reviewed. The air–surface exchange of Hg 0 is commonly bi-directional, with daytime emission and nighttime deposition over non-vegetated surfaces and vegetated surfaces with small leaf area indices under low ambient Hg 0 conditions. However, daytime deposition has also been observed, especially when the ambient Hg 0 is high. Typical dry deposition velocities ( V d) for Hg 0 are in the range of 0.1–0.4 cm s −1 over vegetated surfaces and wetlands, but substantially smaller over non-vegetated surfaces and soils below canopies. Meteorological, biological, and soil conditions, as well as the ambient Hg 0 concentrations all play important roles in the diurnal and seasonal variations of Hg 0 air–surface exchange processes. Measurements of RGM deposition are limited and are known to have large uncertainties. Nevertheless, all of the measurements suggest that RGM can deposit very quickly onto any type of surface, with its V d ranging from 0.5 to 6 cm s −1. The very limited data for Hg p suggest that its V d values are in the range of 0.02–2 cm s −1. A resistance approach is commonly used in mercury transport models to estimate V d for RGM and Hg p; however, there is a wide range of complexities in the dry deposition scheme of Hg 0. Although resistance-approach based dry deposition schemes seem to be able to produce the typical V d values for RGM and Hg 0 over different surface types, more sophisticated air–surface exchange models have been developed to handle the bi-directional exchange processes. Both existing and newly developed dry deposition schemes need further evaluation using field measurements and intercomparisons within different modelling frameworks.