scholarly journals Review on Mesoscale Eddy Studies in the Kuroshio Extension Region

2013 ◽  
Vol 02 (01) ◽  
pp. 1-8 ◽  
Author(s):  
笑 张
OCEANS 2009 ◽  
2009 ◽  
Author(s):  
T. G. Jensen ◽  
T. Campbell ◽  
T. A. Smith ◽  
R. J. Small ◽  
R. Allard

2018 ◽  
Vol 123 (11) ◽  
pp. 8548-8567 ◽  
Author(s):  
Jinlin Ji ◽  
Changming Dong ◽  
Biao Zhang ◽  
Yu Liu ◽  
Bin Zou ◽  
...  

2006 ◽  
Vol 36 (3) ◽  
pp. 457-473 ◽  
Author(s):  
Bo Qiu ◽  
Peter Hacker ◽  
Shuiming Chen ◽  
Kathleen A. Donohue ◽  
D. Randolph Watts ◽  
...  

Abstract Properties and seasonal evolution of North Pacific Ocean subtropical mode water (STMW) within and south of the Kuroshio Extension recirculation gyre are analyzed from profiling float data and additional hydrographic and shipboard ADCP measurements taken during 2004. The presence of an enhanced recirculation gyre and relatively low mesoscale eddy variability rendered this year favorable for the formation of STMW. Within the recirculation gyre, STMW formed from late-winter convection that reached depths greater than 450 m near the center of the gyre. The lower boundary of STMW, corresponding to σθ ≃ 25.5 kg m−3, was set by the maximum depth of the late-winter mixed layer. Properties within the deep portions of the STMW layer remained largely unchanged as the season progressed. In contrast, the upper boundary of the STMW layer eroded steadily as the seasonal thermocline deepened from late April to August. Vertical eddy diffusivity responsible for this erosion was estimated from a budget analysis of potential vorticity to be in the range of ∼2–5 × 10−4 m2 s−1. The latitudinal extent of the STMW formation was narrow, extending from 30°N to the Kuroshio Extension jet near 35°N. South of 30°N, STMW did not form locally but was transported from the recirculation gyre by lateral induction.


1998 ◽  
Vol 103 (5) ◽  
pp. 2790-2790
Author(s):  
Gang Yuan ◽  
Hidetoshi Fujimori ◽  
Toshiaki Nakamura ◽  
Iwao Nakano ◽  
Takashi Kamoshida ◽  
...  

1998 ◽  
Vol 103 (5) ◽  
pp. 2790-2790
Author(s):  
Hidetoshi Fujimori ◽  
Iwao Nakano ◽  
Toshiaki Nakamura ◽  
Guan Yuan ◽  
Takashi Kamoshida ◽  
...  

2000 ◽  
Vol 108 (5) ◽  
pp. 2586-2586
Author(s):  
Gang Yuan ◽  
Humio Mitsudera ◽  
Iwao Nakano ◽  
Hidetoshi Fujimori ◽  
Yasushi Yoshikawa ◽  
...  

2020 ◽  
Author(s):  
Guidi Zhou ◽  
Xuhua Cheng

<p>The decadal variability of the Kuroshio Extension (KE) is investigated using altimeter observations (AVISO) and the output of an ocean model (OFES). It is shown that the KE decadal variability is manifested in its strength, latitudinal position, and zonal extent, as well as the associated mesoscale eddy activity. Two differences between the two datasets are identified: (a) In OFES, the eddy activity positively correlates with the KE mode index when it leads by a few years, whereas in AVISO the two are negatively and concurrently correlated. (b) In OFES, the positive KE mode is associated with large meanders of the Kuroshio south of Japan, but in AVISO they are irrelevant. These differences indicate that the generation mechanism of KE's decadal variability is different in OFES and the real ocean. The sea surface height anomaly (SSHA) is then decomposed into major components including the wind-driven Rossby waves and residual (intrinsic) variability. The relationship between the two components are virtually the same in OFES and in AVISO, showing a negative correlation when the wind-driven part leads by a few years. Further diagnostics based on OFES reveals that the residual SSHA originates from the downstream region over the Shatsky Rise, slowly propagates westward, and is driven by eddy potential energy transfer. The OFES results partly conform to the intrinsic relaxation oscillation theory put forth by idealized model analyses, but in the latter the SSHA signal originates from the upstream Kuroshio. A new mechanism is then proposed for OFES: the decadal variability of the KE is first a result of the intrinsic relaxation oscillation probably excited by wind forcing, which regulates the strength of the KE’s inflow and thus modulates the downstream topography interaction, resulting in different downstream mesoscale eddy activity that further feeds back on the mean-flow. The mechanism for the real ocean is also reassessed.</p>


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