4.7 Article

The effects of springtime mid-latitude storms on trace gas composition determined from the MACC reanalysis

Journal

ATMOSPHERIC CHEMISTRY AND PHYSICS
Volume 15, Issue 6, Pages 3605-3628

Publisher

COPERNICUS GESELLSCHAFT MBH
DOI: 10.5194/acp-15-3605-2015

Keywords

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Funding

  1. University of Edinburgh through the Principal's Career Development Scholarship
  2. Edinburgh Global Research Scholarship Award
  3. School of Geosciences, University of Edinburgh

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The relationship between springtime air pollution transport of ozone (O-3) and carbon monoxide (CO) and mid-latitude cyclones is explored for the first time using the Monitoring Atmospheric Composition and Climate (MACC) reanalysis for the period 2003-2012. In this study, the most intense spring storms (95th percentile) are selected for two regions, the North Pacific (NP) and the North Atlantic (NA). These storms (similar to 60 storms over each region) often track over the major emission sources of East Asia and eastern North America. By compositing the storms, the distributions of O-3 and CO within a 'typical' intense storm are examined. We compare the storm-centered composite to background composites of 'average conditions' created by sampling the reanalysis data of the previous year to the storm locations. Mid-latitude storms are found to redistribute concentrations of O-3 and CO horizontally and vertically throughout the storm. This is clearly shown to occur through two main mechanisms: (1) vertical lifting of CO-rich and O-3-poor air isentropically, from near the surface to the mid- to upper-troposphere in the region of the warm conveyor belt; and (2) descent of O-3-rich and CO-poor air isentropically in the vicinity of the dry intrusion, from the stratosphere toward the mid-troposphere. This can be seen in the composite storm's life cycle as the storm intensifies, with area-averaged O-3 (CO) increasing (decreasing) between 200 and 500 hPa. The influence of the storm dynamics compared to the background environment on the composition within an area around the storm center at the time of maximum intensity is as follows. Area-averaged O-3 at 300 hPa is enhanced by 50 and 36% and by 11 and 7.6% at 500 hPa for the NP and NA regions, respectively. In contrast, area-averaged CO at 300 hPa decreases by 12% for NP and 5.5% for NA, and area-averaged CO at 500 hPa decreases by 2.4% for NP while there is little change over the NA region. From the mid-troposphere, O-3-rich air is clearly seen to be transported toward the surface, but the downward transport of CO-poor air is not discernible due to the high levels of CO in the lower troposphere. Area-averaged O-3 is slightly higher at 1000 hPa (3.5 and 1.8% for the NP and NA regions, respectively). There is an increase of CO at 1000 hPa for the NP region (3.3%) relative to the background composite and a similar to slight decrease in area-averaged CO for the NA region at 1000 hPa (-2.7%).

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