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Research Article

Stratospheric ozone over the United States in summer linked to observations of convection and temperature via chlorine and bromine catalysis

James G. Anderson, Debra K. Weisenstein, Kenneth P. Bowman, Cameron R. Homeyer, Jessica B. Smith, David M. Wilmouth, David S. Sayres, J. Eric Klobas, View ORCID ProfileStephen S. Leroy, John A. Dykema, and Steven C. Wofsy
PNAS June 20, 2017 114 (25) E4905-E4913; first published June 5, 2017; https://doi.org/10.1073/pnas.1619318114
James G. Anderson
aDepartment of Chemistry and Chemical Biology, Harvard University, Cambridge, MA 02138;
bDepartment of Earth and Planetary Sciences, Harvard University, Cambridge, MA 02138;
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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  • For correspondence: anderson@huarp.harvard.edu
Debra K. Weisenstein
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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Kenneth P. Bowman
dDepartment of Atmospheric Sciences, Texas A&M University, College Station, TX 77843;
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Cameron R. Homeyer
eSchool of Meteorology, University of Oklahoma, Norman, OK 73019
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Jessica B. Smith
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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David M. Wilmouth
aDepartment of Chemistry and Chemical Biology, Harvard University, Cambridge, MA 02138;
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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David S. Sayres
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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J. Eric Klobas
aDepartment of Chemistry and Chemical Biology, Harvard University, Cambridge, MA 02138;
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Stephen S. Leroy
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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  • ORCID record for Stephen S. Leroy
John A. Dykema
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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Steven C. Wofsy
bDepartment of Earth and Planetary Sciences, Harvard University, Cambridge, MA 02138;
cHarvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138;
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  1. Edited by John H. Seinfeld, California Institute of Technology, Pasadena, CA, and approved May 9, 2017 (received for review November 28, 2016)

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    Fig. 1.

    In the context of climate−chemistry coupling globally, the central United States in summer represents a combination of factors specific to both the geographic region and the season. Northerly flow of warm moist air from the Gulf of Mexico in combination with heating and convergence over the Great Plains frequently triggers powerful convection that injects water vapor into the stratosphere, where the upper level anticyclonic flow associated with the NAM can sequester the injection for up to a week or more over the United States. These conditions, in combination with cold stratospheric temperatures, can lead to heterogeneous catalysis on ubiquitous sulfate−water aerosols that converts inorganic chlorine to ClO and can initiate ozone loss through an array of gas-phase catalytic cycles. Potential future enhancements in sulfate from volcanic injection or geoengineering increase the likelihood of halogen activation and ozone loss.

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    Fig. 2.

    An example of the dependence of heterogeneous catalytic conversion of inorganic chlorine (Cly ≈ HCl + ClONO2) on temperature, water vapor, and sulfate loading is displayed in a manner that distinguishes rapid conversion of Cly to free radical form in the shaded region (with the threshold defined as 10% chlorine activation in the first diurnal period) from the unshaded region for which there is virtually no Cly to ClO conversion. These domains establish the photochemical framework for the analysis of convective addition of water, sulfate addition by volcanic injection or overt sulfate addition for SRM, or combinations thereof. The broad blue line dividing the perturbed and unperturbed domains corresponds to a sulfate reactive surface area of 2 μm2/cm3; the green line represents a shift in sulfate reactive surface area to 20 μm2/cm3.

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    Fig. 3.

    (A) The geographic distribution of deep stratospheric convective injection from the NEXRAD weather radar 3D mapping of storms in the summer (May–August 2004–2013) that penetrate more than 2 km above the local tropopause. (B) The vertical distribution of inferred HCl as a function of potential temperature in the stratosphere over the United States in summer for two latitude bins (blue and red points), where HCl is calculated using in situ O3 data from the NASA SEAC4RS mission. In situ measurements acquired by the National Oceanic and Atmospheric Administration chemical ionization mass spectrometer (CIMS) HCl instrument during the NASA AVE mission in June 2005 are included for comparison with the inferred HCl. Data acquired between 30°N to 50°N and 80°W to 105°W are shown. Also plotted are bin-averaged measurements of HCl acquired by MLS as a function of potential temperature, calculated from simultaneous measurements of temperature at the 100- and 68-hPa pressure levels (green squares). The dashed green lines indicate the range 1 SD from the mean for each 20 K potential temperature bin. The MLS satellite data were selected to be between 30°N to 50°N and 80°W to 105°W for June–August from 2004 to 2016. (C) The total number of storms that penetrate more than 2 km into the stratosphere over the central United States in May–August (black) and June–August (red) from 2004 to 2013 as a function of potential temperature. The calculated HCl mixing ratio is superimposed on the NEXRAD observations of frequency and penetration height.

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    Fig. 4.

    High spatial resolution in situ temperatures (gray dots) obtained during the NASA SEAC4RS mission over the United States in summer 2013. The distribution in temperature is, in part, due to gravity wave-driven temperature fluctuations. Bin-average profiles for these data are plotted in the red circles, and the smoothed mean profile, Tave, is represented by the solid red line. Similarly, the profile of minimum temperatures, Tmin, is shown in the cyan circles and line. Tmid (blue line) is defined as the temperature profile midway between Tave and Tmin. The July/August mean of RO temperatures for the same region (black dashed line) demonstrates agreement between the in situ and RO data sets of 2 K or less. Finally, the “standard atmosphere” temperature profile for July that has been used in the AER 2D model, averaged over a region extending from 33°N to 52°N is shown in the solid black line.

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    Fig. 5.

    The response of the four major rate-limiting steps in the catalytic removal of ozone to (A) temperature alone and (B) temperature plus convective addition of water vapor to a mixing ratio of 10 ppmv. The ozone loss rates, calculated using the AER 2D model, are shown after perturbation of temperature and/or water vapor. The three temperature profiles used in the model are shown in Fig. 4, and the temperature distribution is described in Observations of Temperatures in the Lower Stratosphere. A constant 10 ppmv water vapor perturbation between 12 km and 18 km is used to demonstrate the sensitivity in ozone loss rates as a function of altitude (see text).

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    Fig. 6.

    (A) The modeled response of ozone one week after a single convective injection for three different temperatures and water vapor mixing ratios elevated to 10 ppmv between 12 km and 18 km. The ozone profiles are calculated using the AER 2D model, and the three temperature profiles used in the model are shown in Fig. 4. A constant 10 ppmv water vapor perturbation between 12 km and 18 km is used to demonstrate the sensitivity in ozone concentration as a function of altitude. (B) The integrated fractional ozone loss between 14 km and 18 km after 1 wk, calculated as the difference between the modeled ozone profile using Tstd and the ozone profile using Tstd, Tave, or Tmid with convective addition of water vapor.

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Stratospheric ozone over United States in summer
James G. Anderson, Debra K. Weisenstein, Kenneth P. Bowman, Cameron R. Homeyer, Jessica B. Smith, David M. Wilmouth, David S. Sayres, J. Eric Klobas, Stephen S. Leroy, John A. Dykema, Steven C. Wofsy
Proceedings of the National Academy of Sciences Jun 2017, 114 (25) E4905-E4913; DOI: 10.1073/pnas.1619318114

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Stratospheric ozone over United States in summer
James G. Anderson, Debra K. Weisenstein, Kenneth P. Bowman, Cameron R. Homeyer, Jessica B. Smith, David M. Wilmouth, David S. Sayres, J. Eric Klobas, Stephen S. Leroy, John A. Dykema, Steven C. Wofsy
Proceedings of the National Academy of Sciences Jun 2017, 114 (25) E4905-E4913; DOI: 10.1073/pnas.1619318114
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    • Two-Dimensional Model Calculations Exploring the Sensitivity of the Rate-Limiting Steps in the Dominant Ozone Loss Processes to Perturbations in Temperature and Water Vapor
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