2012
DOI: 10.1029/2011jc007228
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Direct observations of microscale turbulence and thermohaline structure in the Kuroshio Front

Abstract: [1] Direct observations of microstructure near the Kuroshio Front were conducted in August 2008 and October 2009. These show negative potential vorticity (PV) in the mixed layer south of the front, where directly measured turbulent kinetic energy dissipation rates are an order magnitude larger than predicted by wind-scaling. These elevated dissipation rates scale better with an empirical scaling, which considers local wind and Ekman buoyancy flux driven by downfront wind. Near-zero PV in the thermocline under … Show more

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Cited by 72 publications
(62 citation statements)
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References 65 publications
(119 reference statements)
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“…3a) of similar magnitudes as observed during 2008 (Nagai et al 2009) and previous studies in the Kuroshio (Rainville and Pinkel 2004) and Gulf Stream (Winkel et al 2002;Inoue et al 2010). Horizontal and vertical wavelengths are l h ; O(10) km and l z ; O(100) m, respectively.…”
Section: B Near-inertial Shearsupporting
confidence: 84%
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“…3a) of similar magnitudes as observed during 2008 (Nagai et al 2009) and previous studies in the Kuroshio (Rainville and Pinkel 2004) and Gulf Stream (Winkel et al 2002;Inoue et al 2010). Horizontal and vertical wavelengths are l h ; O(10) km and l z ; O(100) m, respectively.…”
Section: B Near-inertial Shearsupporting
confidence: 84%
“…A freefall towyo CTD (Underway CTD) was used to measure upper-500-m temperature and salinity every 14.8 km in the 2012 survey. During 2008, five Falmouth CTD profiles of temperature and salinity to 500-m and TurboMAP-II microstructure profiles to 300-m depth were collected every 28 km (Nagai et al 2009). During 17-24 October 2009, five north-south transects were sampled across the Kuroshio to measure CTD and microstructure at 5-8 stations with 9-km resolution in each section (Nagai et al 2012).…”
Section: A Kuroshio Surveysmentioning
confidence: 99%
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“…Among these mechanisms, particular interest has been focused on forced buoyancy loss at the ocean surface. Convective heat loss is known to intensify frontal ageostrophic circulations within submesoscale filaments [ Yoshikawa et al ., ], but more recently the buoyancy flux achieved by down‐front winds through the cross‐front Ekman transport of dense water over light has emerged as a potentially more prominent generation mechanism at strong fronts [ Thomas and Lee , ; Lee et al ., ; Thomas and Joyce , ; Nagai et al ., ]. Recent efforts have attempted to diagnose the relative influence of cooling versus wind‐driven buoyancy loss by quantifying the reduction in surface Ertel potential vorticity (EPV), EPV=ωa·b, where ωa=f+ζ is the absolute vorticity, due to each process [ Yoshikawa et al ., ].…”
Section: Introductionmentioning
confidence: 99%