Abstract

Abstract. The National Institute of Standards and Technology Advanced Radiometer (NISTAR) onboard the Deep Space Climate Observatory (DSCOVR) provides continuous full-disk global broadband irradiance measurements over most of the sunlit side of the Earth. The three active cavity radiometers measure the total radiant energy from the sunlit side of the Earth in shortwave (SW; 0.2–4 µm), total (0.4–100 µm), and near-infrared (NIR; 0.7–4 µm) channels. The Level 1 NISTAR dataset provides the filtered radiances (the ratio between irradiance and solid angle). To determine the daytime top-of-atmosphere (TOA) shortwave and longwave radiative fluxes, the NISTAR-measured shortwave radiances must be unfiltered first. An unfiltering algorithm was developed for the NISTAR SW and NIR channels using a spectral radiance database calculated for typical Earth scenes. The resulting unfiltered NISTAR radiances are then converted to full-disk daytime SW and LW flux by accounting for the anisotropic characteristics of the Earth-reflected and emitted radiances. The anisotropy factors are determined using scene identifications determined from multiple low-Earth orbit and geostationary satellites as well as the angular distribution models (ADMs) developed using data collected by the Clouds and the Earth's Radiant Energy System (CERES). Global annual daytime mean SW fluxes from NISTAR are about 6 % greater than those from CERES, and both show strong diurnal variations with daily maximum–minimum differences as great as 20 Wm−2 depending on the conditions of the sunlit portion of the Earth. They are also highly correlated, having correlation coefficients of 0.89, indicating that they both capture the diurnal variation. Global annual daytime mean LW fluxes from NISTAR are 3 % greater than those from CERES, but the correlation between them is only about 0.38.

Highlights

  • The Earth’s climate is determined by the amount and distribution of the incoming solar radiation absorbed and the outgoing longwave radiation (OLR) emitted by the Earth

  • To determine the global daytime mean anisotropic factors, we use the anisotropies characterized in the Clouds and the Earth’s Radiant Energy System (CERES) angular distribution models (ADMs), and they are selected based upon the scene-type information provided by the Earth Polychromatic Imaging Camera (EPIC) composite for every EPIC field of view (FOV)

  • For a given EPIC FOV (j ), its anisotropic factor is determined based upon the Sun–EPIC viewing geometry and the scene identification information provided by the EPIC composite: Rj (θ0, θ e, φe, χ e)

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Summary

Introduction

The Earth’s climate is determined by the amount and distribution of the incoming solar radiation absorbed and the outgoing longwave radiation (OLR) emitted by the Earth. Su et al (2018) described the methodology to derive the global mean daytime shortwave (SW) anisotropic factors by using the CERES angular distribution models (ADMs) and a cloud property composite based on lower-Earth orbit satellite imager retrievals. These SW anisotropic factors were applied to EPIC broadband SW radiances, which were estimated from EPIC narrowband observations based upon narrowband-to-broadband regressions, to derive the global daytime SW fluxes.

NISTAR observation
Standard 15 Standard
Global daytime shortwave and longwave anisotropic factors
CERES ADMs
EPIC composite data
Calculating global daytime anisotropic factors
NISTAR shortwave and longwave flux
Findings
Conclusions and discussion

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