Atmospheric Chemistry and Physics (Sep 2008)

Photolysis frequency measurement techniques: results of a comparison within the ACCENT project

  • K. C. Clemitshaw,
  • D. E. Heard,
  • N. Mihalopoulos,
  • C. Plass-Dülmer,
  • U. Platt,
  • H.-P. Dorn,
  • P. S. Monks,
  • M. Kortner,
  • L. J. Clapp,
  • W. J. Bloss,
  • M. Vrekoussis,
  • E. Tensing,
  • G. Stange,
  • M. Gillmann,
  • S. Sanghavi,
  • G. K. Corlett,
  • B. Bohn,
  • F. X. Meixner,
  • A. S. H. Prevot,
  • R. Schmitt

Journal volume & issue
Vol. 8, no. 17
pp. 5373 – 5391

Abstract

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An intercomparison of different radiometric techniques measuring atmospheric photolysis frequencies <i>j</i>(NO<sub>2</sub>), <i>j</i>(HCHO) and <i>j</i>(O<sup>1</sup>D) was carried out in a two-week field campaign in June 2005 at Jülich, Germany. Three double-monochromator based spectroradiometers (DM-SR), three single-monochromator based spectroradiometers with diode-array detectors (SM-SR) and seventeen filter radiometers (FR) (ten <i>j</i>(NO<sub>2</sub>)-FR, seven <i>j</i>(O<sup>1</sup>D)-FR) took part in this comparison. For <i>j</i>(NO<sub>2</sub>), all spectroradiometer results agreed within &plusmn;3%. For <i>j</i>(HCHO), agreement was slightly poorer between &minus;8% and +4% of the DM-SR reference result. For the SM-SR deviations were explained by poorer spectral resolutions and lower accuracies caused by decreased sensitivities of the photodiode arrays in a wavelength range below 350 nm. For <i>j</i>(O<sup>1</sup>D), the results were more complex within +8% and &minus;4% with increasing deviations towards larger solar zenith angles for the SM-SR. The direction and the magnitude of the deviations were dependent on the technique of background determination. All <i>j</i>(NO<sub>2</sub>)-FR showed good linearity with single calibration factors being sufficient to convert from output voltages to <i>j</i>(NO<sub>2</sub>). Measurements were feasible until sunset and comparison with previous calibrations showed good long-term stability. For the <i>j</i>(O<sup>1</sup>D)-FR, conversion from output voltages to <i>j</i>(O<sup>1</sup>D) needed calibration factors and correction functions considering the influences of total ozone column and elevation of the sun. All instruments showed good linearity at photolysis frequencies exceeding about 10% of maximum values. At larger solar zenith angles, the agreement was non-uniform with deviations explainable by insufficient correction functions. Comparison with previous calibrations for some <i>j</i>(O<sup>1</sup>D)-FR indicated drifts of calibration factors.