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The frictional layer in the observed momentum budget of the trades

Profiles of eddy momentum flux divergence are calculated as the residual in the momentum budget constructed from airborne circular dropsonde arrays ([Formula: see text] 220 km) for 13 days during the EUREC [Formula: see text] A/ATOMIC field campaign. The observed dynamical forcing averaged over all...

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Autores principales: Nuijens, L., Savazzi, A., de Boer, G., Brilouet, P‐E., George, G., Lothon, M., Zhang, D.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley & Sons, Ltd 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9828681/
https://www.ncbi.nlm.nih.gov/pubmed/36636229
http://dx.doi.org/10.1002/qj.4364
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author Nuijens, L.
Savazzi, A.
de Boer, G.
Brilouet, P‐E.
George, G.
Lothon, M.
Zhang, D.
author_facet Nuijens, L.
Savazzi, A.
de Boer, G.
Brilouet, P‐E.
George, G.
Lothon, M.
Zhang, D.
author_sort Nuijens, L.
collection PubMed
description Profiles of eddy momentum flux divergence are calculated as the residual in the momentum budget constructed from airborne circular dropsonde arrays ([Formula: see text] 220 km) for 13 days during the EUREC [Formula: see text] A/ATOMIC field campaign. The observed dynamical forcing averaged over all flights agrees broadly with European Centre for Medium‐Range Weather Forecasts (ECMWF) Integrated Forecasting System (IFS) forecasts. In the direction of the flow, a mean flux divergence (friction) exists over a 1.5‐km deep Ekman layer, and a mean flux convergence (acceleration) is present near cloud tops. The friction is countergradient between 1 and 1.5 km, where vertical wind shear exceeds the observed thermal wind. From the frictional profile, a 10‐m momentum flux of [Formula: see text] 0.1 N [Formula: see text] m [Formula: see text] is derived, in line with Saildrone turbulence measurements. A momentum flux divergence in the cross‐wind direction is pronounced near the surface and acts to veer the wind, opposing the friction‐induced cross‐isobaric wind turning. Weaker friction and upper‐level acceleration of easterly flow are observed when stronger winds and more vigorous convection prevail. Turbulence measurements on board the SAFIRE ATR‐42 aircraft and the Uncrewed Aircraft System (UAS) RAAVEN reveal pronounced spatial variability of momentum fluxes, with a non‐negligible contribution of mesoscales (5–30 km). The findings highlight the nontrivial impact of turbulence, convection, and mesoscale flows in the presence of diverse cloud fields on the depth and strength of the frictional layer.
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spelling pubmed-98286812023-01-10 The frictional layer in the observed momentum budget of the trades Nuijens, L. Savazzi, A. de Boer, G. Brilouet, P‐E. George, G. Lothon, M. Zhang, D. Q J R Meteorol Soc Research Articles Profiles of eddy momentum flux divergence are calculated as the residual in the momentum budget constructed from airborne circular dropsonde arrays ([Formula: see text] 220 km) for 13 days during the EUREC [Formula: see text] A/ATOMIC field campaign. The observed dynamical forcing averaged over all flights agrees broadly with European Centre for Medium‐Range Weather Forecasts (ECMWF) Integrated Forecasting System (IFS) forecasts. In the direction of the flow, a mean flux divergence (friction) exists over a 1.5‐km deep Ekman layer, and a mean flux convergence (acceleration) is present near cloud tops. The friction is countergradient between 1 and 1.5 km, where vertical wind shear exceeds the observed thermal wind. From the frictional profile, a 10‐m momentum flux of [Formula: see text] 0.1 N [Formula: see text] m [Formula: see text] is derived, in line with Saildrone turbulence measurements. A momentum flux divergence in the cross‐wind direction is pronounced near the surface and acts to veer the wind, opposing the friction‐induced cross‐isobaric wind turning. Weaker friction and upper‐level acceleration of easterly flow are observed when stronger winds and more vigorous convection prevail. Turbulence measurements on board the SAFIRE ATR‐42 aircraft and the Uncrewed Aircraft System (UAS) RAAVEN reveal pronounced spatial variability of momentum fluxes, with a non‐negligible contribution of mesoscales (5–30 km). The findings highlight the nontrivial impact of turbulence, convection, and mesoscale flows in the presence of diverse cloud fields on the depth and strength of the frictional layer. John Wiley & Sons, Ltd 2022-10-01 2022-10 /pmc/articles/PMC9828681/ /pubmed/36636229 http://dx.doi.org/10.1002/qj.4364 Text en © 2022 The Authors. Quarterly Journal of the Royal Meteorological Society published by John Wiley & Sons Ltd on behalf of Royal Meteorological Society. https://creativecommons.org/licenses/by/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Research Articles
Nuijens, L.
Savazzi, A.
de Boer, G.
Brilouet, P‐E.
George, G.
Lothon, M.
Zhang, D.
The frictional layer in the observed momentum budget of the trades
title The frictional layer in the observed momentum budget of the trades
title_full The frictional layer in the observed momentum budget of the trades
title_fullStr The frictional layer in the observed momentum budget of the trades
title_full_unstemmed The frictional layer in the observed momentum budget of the trades
title_short The frictional layer in the observed momentum budget of the trades
title_sort frictional layer in the observed momentum budget of the trades
topic Research Articles
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9828681/
https://www.ncbi.nlm.nih.gov/pubmed/36636229
http://dx.doi.org/10.1002/qj.4364
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