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Atmospheric Measurement Techniques An interactive open-access journal of the European Geosciences Union
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Volume 6, issue 5 | Copyright
Atmos. Meas. Tech., 6, 1111-1140, 2013
© Author(s) 2013. This work is distributed under
the Creative Commons Attribution 3.0 License.

Research article 02 May 2013

Research article | 02 May 2013

Intercomparison of NO3 radical detection instruments in the atmosphere simulation chamber SAPHIR

H.-P. Dorn1, R. L. Apodaca2, S. M. Ball3, T. Brauers1, S. S. Brown4, J. N. Crowley5, W. P. Dubé4, H. Fuchs1,4, R. Häseler1, U. Heitmann6, R. L. Jones7, A. Kiendler-Scharr1, I. Labazan5, J. M. Langridge7,*, J. Meinen8, T. F. Mentel1, U. Platt9, D. Pöhler9, F. Rohrer1, A. A. Ruth6, E. Schlosser1,**, G. Schuster5, A. J. L. Shillings7, W. R. Simpson2, J. Thieser9,***, R. Tillmann1, R. Varma6,****, D. S. Venables10, and A. Wahner1 H.-P. Dorn et al.
  • 1Institute of Energy and Climate Research, IEK-8: Troposphere, Forschungszentrum Jülich, Julich, Germany
  • 2Department of Chemistry and Biochemistry and Geophysical Institute, University of Alaska, Fairbanks, AK, USA
  • 3Department of Chemistry, University of Leicester, Leicester, UK
  • 4Earth System Research Laboratory, National Oceanic and Atmospheric Administration, Boulder, CO, USA
  • 5Max Planck Institute for Chemistry, Mainz, Germany
  • 6Physics Department & Environmental Research Institute, University College Cork, Cork, Ireland
  • 7Department of Chemistry, University of Cambridge, Cambridge, UK
  • 8Institute for Meteorology and Climate Research – Atmospheric Aerosol Research, Karlsruhe Institute of Technology, Karlsruhe, Germany
  • 9Institute of Environmental Physics, University of Heidelberg, Heidelberg, Germany
  • 10Chemistry Department and Environmental Research Institute, University College Cork, Cork, Ireland
  • *now at: Earth System Research Laboratory, NOAA, Boulder, CO, USA
  • **now at: Institute for Meteorology and Climate Research, IMK-AAF, Karlsruhe Institute of Technology, Karlsruhe, Germany
  • ***now at: Max Planck Institute for Chemistry, Mainz, Germany
  • ****now at: Physics Department, National Institute of Technology Calicut, Calicut, India

Abstract. The detection of atmospheric NO3 radicals is still challenging owing to its low mixing ratios (≈ 1 to 300 pptv) in the troposphere. While long-path differential optical absorption spectroscopy (DOAS) has been a well-established NO3 detection approach for over 25 yr, newly sensitive techniques have been developed in the past decade. This publication outlines the results of the first comprehensive intercomparison of seven instruments developed for the spectroscopic detection of tropospheric NO3. Four instruments were based on cavity ring-down spectroscopy (CRDS), two utilised open-path cavity-enhanced absorption spectroscopy (CEAS), and one applied "classical" long-path DOAS. The intercomparison campaign "NO3Comp" was held at the atmosphere simulation chamber SAPHIR in Jülich (Germany) in June 2007. Twelve experiments were performed in the well-mixed chamber for variable concentrations of NO3, N2O5, NO2, hydrocarbons, and water vapour, in the absence and in the presence of inorganic or organic aerosol. The overall precision of the cavity instruments varied between 0.5 and 5 pptv for integration times of 1 s to 5 min; that of the DOAS instrument was 9 pptv for an acquisition time of 1 min. The NO3 data of all instruments correlated excellently with the NOAA-CRDS instrument, which was selected as the common reference because of its superb sensitivity, high time resolution, and most comprehensive data coverage. The median of the coefficient of determination (r2) over all experiments of the campaign (60 correlations) is r2 = 0.981 (quartile 1 (Q1): 0.949; quartile 3 (Q3): 0.994; min/max: 0.540/0.999). The linear regression analysis of the campaign data set yielded very small intercepts (median: 1.1 pptv; Q1/Q3: −1.1/2.6 pptv; min/max: −14.1/28.0 pptv), and the slopes of the regression lines were close to unity (median: 1.01; Q1/Q3: 0.92/1.10; min/max: 0.72/1.36). The deviation of individual regression slopes from unity was always within the combined accuracies of each instrument pair. The very good correspondence between the NO3 measurements by all instruments for aerosol-free experiments indicates that the losses of NO3 in the inlet of the instruments were determined reliably by the participants for the corresponding conditions. In the presence of inorganic or organic aerosol, however, differences in the measured NO3 mixing ratios were detectable among the instruments. In individual experiments the discrepancies increased with time, pointing to additional NO3 radical losses by aerosol deposited onto the filters or on the inlet walls of the instruments. Instruments using DOAS analyses showed no significant effect of aerosol on the detection of NO3. No hint of a cross interference of NO2 was found. The effect of non-Lambert–Beer behaviour of water vapour absorption lines on the accuracy of the NO3 detection by broadband techniques was small and well controlled. The NO3Comp campaign demonstrated the high quality, reliability and robustness of performance of current state-of-the-art instrumentation for NO3 detection.

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