Ocean eddy dynamics in a coupled ocean - Atmosphere model

被引:35
作者
Berloff, P. [1 ]
Dewar, W.
Kravtsov, S.
McWilliams, J.
机构
[1] Woods Hole Oceanog Inst, Dept Phys Oceanog, Woods Hole, MA 02543 USA
[2] Univ Cambridge, Dept Appl Math & Theoret Phys, Cambridge CB2 1TN, England
[3] Florida State Univ, Dept Oceanog, Tallahassee, FL 32306 USA
[4] Univ Wisconsin, Dept Math Sci, Milwaukee, WI 53201 USA
[5] Univ Calif Los Angeles, Dept Atmospher & Ocean Sci, Los Angeles, CA 90024 USA
关键词
D O I
10.1175/JPO3041.1
中图分类号
P7 [海洋学];
学科分类号
0707 ;
摘要
The role of mesoscale oceanic eddies is analyzed in a quasigeostrophic coupled ocean-atmosphere model operating at a large Reynolds number. The model dynamics are characterized by decadal variability that involves nonlinear adjustment of the ocean to coherent north-south shifts of the atmosphere. The oceanic eddy effects are diagnosed by the dynamical decomposition method adapted for nonstationary external forcing. The main effects of the eddies are an enhancement of the oceanic eastward jet separating the subpolar and subtropical gyres and a weakening of the gyres. The flow- enhancing effect is due to nonlinear rectification driven by fluctuations of the eddy forcing. This is a nonlocal process involving generation of the eddies by the flow instabilities in the western boundary current and the upstream part of the eastward jet. The eddies are advected by the mean current to the east, where they backscatter into the rectified enhancement of the eastward jet. The gyre- weakening effect, which is due to the time- mean buoyancy component of the eddy forcing, is a result of the baroclinic instability of the westward return currents. The diagnosed eddy forcing is parameterized in a non-eddy-resolving ocean model, as a nonstationary random process, in which the corresponding parameters are derived from the control coupled simulation. The key parameter of the random process - its variance - is related to the large-scale flow baroclinicity index. It is shown that the coupled model with the non-eddy-resolving ocean component and the parameterized eddies correctly simulates climatology and low-frequency variability of the control eddy-resolving coupled solution.
引用
收藏
页码:1103 / 1121
页数:19
相关论文
共 45 条
[1]   On rectification of randomly forced flows [J].
Berloff, PS .
JOURNAL OF MARINE RESEARCH, 2005, 63 (03) :497-527
[2]   On dynamically consistent eddy fluxes [J].
Berloff, PS .
DYNAMICS OF ATMOSPHERES AND OCEANS, 2005, 38 (3-4) :123-146
[3]   Random-forcing model of the mesoscale oceanic eddies [J].
Berloff, PS .
JOURNAL OF FLUID MECHANICS, 2005, 529 :71-95
[4]  
Berloff PS, 1999, J PHYS OCEANOGR, V29, P1925, DOI 10.1175/1520-0485(1999)029<1925:LSLFVI>2.0.CO
[5]  
2
[6]  
DESER C, 1993, J CLIMATE, V6, P1743, DOI 10.1175/1520-0442(1993)006<1743:SCVOTN>2.0.CO
[7]  
2
[8]  
Dewar WK, 2003, J PHYS OCEANOGR, V33, P1057, DOI 10.1175/1520-0485(2003)033<1057:NMOA>2.0.CO
[9]  
2
[10]  
Feliks Y, 2004, J ATMOS SCI, V61, P961, DOI 10.1175/1520-0469(2004)061<0961:LVITMA>2.0.CO