Extent and Energetics of the Hawaiian Lee Countercurrent

Direct velocity observations from drogued drifters in the Hawaiian Island region are used to map the time-mean and seasonal variability of the Hawaiian Lee Countercurrent (HLCC). The density of these data has more than doubled since the initial discovery of the HLCC. They provide valuable absolute e...

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Main Authors: Rick Lumpkin, Pierre J. Flament
Format: Article
Language:English
Published: The Oceanography Society 2013-03-01
Series:Oceanography
Subjects:
Online Access:http://tos.org/oceanography/archive/26-1_lumpkin.pdf
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spelling doaj-50084fa45fc3475bb90f38e7c6a7c7c52020-11-25T01:41:19ZengThe Oceanography SocietyOceanography1042-82752013-03-012615865Extent and Energetics of the Hawaiian Lee CountercurrentRick LumpkinPierre J. FlamentDirect velocity observations from drogued drifters in the Hawaiian Island region are used to map the time-mean and seasonal variability of the Hawaiian Lee Countercurrent (HLCC). The density of these data has more than doubled since the initial discovery of the HLCC. They provide valuable absolute estimates of HLCC velocity structure and variability, complementing data derived from geostrophy and numerical simulations. The data demonstrate that the HLCC has a peak annual mean velocity > 9 cm s–1, with the strongest velocities along 19.75°N and eastward speeds in the longitudinal range 170°W to 157°W. The HLCC is relatively weak from March to May compared to its strength in other months. In the longitude band 160°–168°W, an eddy-to-mean energy flux of 3.3 ± 1.2 µW m–3 is found in the annual mean associated with the Reynolds shear stress, maintaining the shear between the HLCC and the North Equatorial Current to its south. This shear stress is associated with energetic anticyclonic eddies that are shed from the Big Island of Hawaii and propagate west-southwest. This energy flux is nearly twice as large during the peak HLCC months of August to January. It is sufficient to spin up the HLCC in O(10 days), and it is associated with an eddy spin-down time of O(100 days).http://tos.org/oceanography/archive/26-1_lumpkin.pdfdrogued driftersHawaiian Lee CountercurrentHLCC
collection DOAJ
language English
format Article
sources DOAJ
author Rick Lumpkin
Pierre J. Flament
spellingShingle Rick Lumpkin
Pierre J. Flament
Extent and Energetics of the Hawaiian Lee Countercurrent
Oceanography
drogued drifters
Hawaiian Lee Countercurrent
HLCC
author_facet Rick Lumpkin
Pierre J. Flament
author_sort Rick Lumpkin
title Extent and Energetics of the Hawaiian Lee Countercurrent
title_short Extent and Energetics of the Hawaiian Lee Countercurrent
title_full Extent and Energetics of the Hawaiian Lee Countercurrent
title_fullStr Extent and Energetics of the Hawaiian Lee Countercurrent
title_full_unstemmed Extent and Energetics of the Hawaiian Lee Countercurrent
title_sort extent and energetics of the hawaiian lee countercurrent
publisher The Oceanography Society
series Oceanography
issn 1042-8275
publishDate 2013-03-01
description Direct velocity observations from drogued drifters in the Hawaiian Island region are used to map the time-mean and seasonal variability of the Hawaiian Lee Countercurrent (HLCC). The density of these data has more than doubled since the initial discovery of the HLCC. They provide valuable absolute estimates of HLCC velocity structure and variability, complementing data derived from geostrophy and numerical simulations. The data demonstrate that the HLCC has a peak annual mean velocity > 9 cm s–1, with the strongest velocities along 19.75°N and eastward speeds in the longitudinal range 170°W to 157°W. The HLCC is relatively weak from March to May compared to its strength in other months. In the longitude band 160°–168°W, an eddy-to-mean energy flux of 3.3 ± 1.2 µW m–3 is found in the annual mean associated with the Reynolds shear stress, maintaining the shear between the HLCC and the North Equatorial Current to its south. This shear stress is associated with energetic anticyclonic eddies that are shed from the Big Island of Hawaii and propagate west-southwest. This energy flux is nearly twice as large during the peak HLCC months of August to January. It is sufficient to spin up the HLCC in O(10 days), and it is associated with an eddy spin-down time of O(100 days).
topic drogued drifters
Hawaiian Lee Countercurrent
HLCC
url http://tos.org/oceanography/archive/26-1_lumpkin.pdf
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