Synergy between Short-Range Lidar and In Situ Instruments for Determining the Atmospheric Boundary Layer Lidar Ratio

Author:

Bedoya-Velásquez Andres Esteban1ORCID,Ceolato Romain1ORCID,Titos Gloria23ORCID,Bravo-Aranda Juan Antonio23,Casans Andrea23ORCID,Patrón Diego23,Fernández-Carvelo Sol23,Guerrero-Rascado Juan Luis23ORCID,Alados-Arboledas Lucas23ORCID

Affiliation:

1. ONERA, The French Aerospace Lab, Université de Toulouse, FR 31055 Toulouse, France

2. Department of Applied Physics, Sciences Faculty, University of Granada, 18071 Granada, Spain

3. Andalusian Institute for Earth System Research, IISTA-CEAMA, University of Granada, 18006 Granada, Spain

Abstract

Short-range elastic backscatter lidar (SR-EBL) systems are remote sensing instruments for studying low atmospheric boundary layer processes. This work presents a field campaign oriented to filling the gap between the near-surface aerosol processes regarding aerosol radiative properties and connecting them with the atmospheric boundary layer (ABL), centering attention on the residual layer and the ABL transition periods. A Colibri Aerosol Lidar (CAL) instrument, based on the short-range lidar with high spatio-temporal resolution, was used for the first time in the ACTRIS AGORA facility (Andalusian Global Observatory of the Atmosphere) in Granada (Spain). This study showed the possibility of combining lidar and in situ measurements in the lowermost 150 m. The results address, on the one hand, the characterization of the short-range lidar for developing a method to find the calibration constant of the system and to correct the incomplete overlap to further data exploitation. On the other hand, relevant radiative properties such as the temporal series of the aerosol lidar ratio and extinction coefficient were quantified. The campaign was divided in three different periods based on the vehicular emission peak in the early mornings, namely, before, during, and after the emission peak. For before and after the emission peak data classification, aerosol properties presented closer values; however, large variability was obtained after the emission peak reaching the maximum values of extinction and a lidar ratio up to 51.5 ± 11.9 (Mm)−1 and 36.0 ± 10.5 sr, respectively. During the emission peaks, the values reached for extinction and lidar ratio were up to 136.8 ± 26.5 (Mm)−1 and 119.0 ± 22.7 sr, respectively.

Funder

European research of mobility program

ONERA

Publisher

MDPI AG

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