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Atmospheric Measurement Techniques An interactive open-access journal of the European Geosciences Union
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Volume 9, issue 4 | Copyright
Atmos. Meas. Tech., 9, 1799-1816, 2016
https://doi.org/10.5194/amt-9-1799-2016
© Author(s) 2016. This work is distributed under
the Creative Commons Attribution 3.0 License.

Research article 26 Apr 2016

Research article | 26 Apr 2016

Dead time effect on the Brewer measurements: correction and estimated uncertainties

Ilias Fountoulakis1, Alberto Redondas2, Alkiviadis F. Bais1, Juan José Rodriguez-Franco2, Konstantinos Fragkos1, and Alexander Cede3,4 Ilias Fountoulakis et al.
  • 1Aristotle University of Thessaloniki, Laboratory of Atmospheric Physics, Thessaloniki, Greece
  • 2Agencia Estatal de Meteorología, Izaña Atmospheric Research Center, Tenerife, Canary Islands, Spain
  • 3NASA/Goddard Space Flight Center, Greenbelt, MD, USA
  • 4LuftBlick, Kreith, Austria

Abstract. Brewer spectrophotometers are widely used instruments which perform spectral measurements of the direct, the scattered and the global solar UV irradiance. By processing these measurements a variety of secondary products can be derived such as the total columns of ozone (TOC), sulfur dioxide and nitrogen dioxide and aerosol optical properties. Estimating and limiting the uncertainties of the final products is of critical importance. High-quality data have a lot of applications and can provide accurate estimations of trends.

The dead time is specific for each instrument and improper correction of the raw data for its effect may lead to important errors in the final products. The dead time value may change with time and, with the currently used methodology, it cannot always be determined accurately. For specific cases, such as for low ozone slant columns and high intensities of the direct solar irradiance, the error in the retrieved TOC, due to a 10ns change in the dead time from its value in use, is found to be up to 5%. The error in the calculation of UV irradiance can be as high as 12% near the maximum operational limit of light intensities. While in the existing documentation it is indicated that the dead time effects are important when the error in the used value is greater than 2ns, we found that for single-monochromator Brewers a 2ns error in the dead time may lead to errors above the limit of 1% in the calculation of TOC; thus the tolerance limit should be lowered. A new routine for the determination of the dead time from direct solar irradiance measurements has been created and tested and a validation of the operational algorithm has been performed. Additionally, new methods for the estimation and the validation of the dead time have been developed and are analytically described. Therefore, the present study, in addition to highlighting the importance of the dead time for the processing of Brewer data sets, also provides useful information for their quality control and re-evaluation.

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The dead time (DT) is characteristic for each Brewer spectrophotometer and non-proper correction of the raw data for its effect may lead to important errors in UV, AOD and TOC measurements. Quantitative estimation of the DT-related uncertainties shown that a 2 ns error in the DT may lead to errors greater than 1 % in TOC. The operational algorithm for the DT calculation and correction is validated and the development of new methods for the estimation of DT is described.
The dead time (DT) is characteristic for each Brewer spectrophotometer and non-proper correction...
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