Abstract

Abstract. Measurements of spectral irradiance between 306 and 1020 nm were performed with a GUVis-3511 multi-channel filter radiometer at Smith Rock State Park, Oregon, during the total solar eclipse of 21 August 2017. The radiometer was equipped with a shadowband, allowing the separation of the global (sun and sky) and direct components of solar radiation. Data were used to study the wavelength-dependent changes in solar irradiance at Earth's surface. Results were compared with theoretical predictions using three different parameterizations of the solar limb darkening (LD) effect, which describes the change in the solar spectrum from the Sun's center to its limb. Results indicate that the LD parameterization that has been most widely used during the last 15 years underestimates the LD effect, in particular at UV wavelengths. The two alternative parameterizations are based on two independent sets of observations from the McMath–Pierce solar telescope. When these parameterizations are used, the observed and theoretical LD effects agree to within 4 % for wavelengths larger than 400 nm and occultation of the solar disk of up to 97.8 %. Maximum deviations for wavelengths between 315 and 340 nm are 7 %. These somewhat larger differences compared to the visible range may be explained with varying aerosol conditions during the period of observations. The aerosol optical depth (AOD) and its wavelength dependence was calculated from measurements of direct irradiance. When corrected for the LD effect, the AOD decreases over the period of the eclipse: from 0.41 to 0.34 at 319 nm and from 0.05 to 0.04 at 1018 nm. These results show that AODs can be accurately calculated during an eclipse if the LD effect is corrected. The total ozone column (TOC) was derived from measurements of global irradiance at 306 and 340 nm. Without correction for the LD effect, the retrieved TOC increases by 20 DU between the first and second contact of the eclipse. With LD correction, the TOC remains constant to within natural variability (±2.6 DU or ±0.9 % between first and second contact and ±1.0 DU or ±0.3 % between third and fourth contact). In contrast to results of observations from earlier solar eclipses, no fluctuations in TOC were observed that could be unambiguously attributed to gravity waves, which can be triggered by the supersonic speed of the Moon's shadow across the atmosphere. Furthermore, systematic changes in the ratio of direct and global irradiance that could be attributed to the solar eclipse were not observed, in agreement with results of three-dimensional (3-D) radiative transfer (RT) models. Our results advance the understanding of the effects of solar LD on the spectral irradiance at Earth's surface, the variations in ozone during an eclipse, and the partitioning of solar radiation in direct and diffuse components.

Highlights

  • A total solar eclipse could be observed on 21 August 2017 across the United States, from Oregon in the west to South Carolina in the east (Pasachoff, 2017)

  • We validate the solar limb darkening (LD) parameterizations by the three methods discussed in Sect. 6; present the ratio of direct-to-global irradiance; show the aerosol optical depth (AOD) and total ozone column (TOC) derived from our measurements before, during, and after the eclipse; and compare measurements near and during totality with reconstructed measurements for the same period but without the Moon occluding the Sun

  • The excellent agreement between the solar LD effect derived from our measurements and theoretical predictions for wavelengths above 400 nm suggests that the parameterizations of LD by Pierce and Neckel are correct to within the measurement uncertainty for this wavelength range

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Summary

Introduction

A total solar eclipse could be observed on 21 August 2017 across the United States, from Oregon in the west to South Carolina in the east (Pasachoff, 2017). Petkov: Measurements of spectral irradiance shadowband to separate the two components Data collected during this campaign can be used for studying processes initiated in the atmosphere by the passing of the Moon’s shadow and for validating three-dimensional (3-D) radiative transfer (RT) calculations that simulate the irradiance at Earth’s surface during the period of totality (Emde and Mayer, 2007). Increasing TOCs were reported for measurements from Dobson spectrophotometers (Bojkov, 1968) and Norsk institutt for luftforskning (NILU) UV multifilter instruments (Antón et al, 2010), while measurements with Brewer spectrophotometers generally decrease as an eclipse progresses (Kazadzis et al, 2007). These differences cannot be explained with a real change in TOC but must be an artifact from either measurement or data processing

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