1996
DOI: 10.1007/978-3-662-03204-6
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Ocean Circulation Theory

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Cited by 440 publications
(386 citation statements)
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“…The first condition corresponds to noslip boundary condition, the second corresponds to a condition of a vanishing tangential stress, the last one corresponds to a relation beetween the eddy flux of the total vorticity and the large scale vorticity field, see [14] page 34. What condition on the boundary due to the diffusion term, do we have to choose ?…”
Section: Introductionmentioning
confidence: 99%
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“…The first condition corresponds to noslip boundary condition, the second corresponds to a condition of a vanishing tangential stress, the last one corresponds to a relation beetween the eddy flux of the total vorticity and the large scale vorticity field, see [14] page 34. What condition on the boundary due to the diffusion term, do we have to choose ?…”
Section: Introductionmentioning
confidence: 99%
“…It the dissipation is small, which means E 1, do this choice has some influence on the global circulation character ? This choice is not so clear as it is pointed out by J. Pedlosky in [14] page 35.…”
Section: Introductionmentioning
confidence: 99%
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“…The nondimensional parameter α r is introduced here to study the effects of the wind stress on the dynamics; its value can be allowed to range between 0 and 1.8 (equivalent to taking the wind stress from abnormally low to abnormally high, as in [12]). The term τ dim /ρ 0 h is dictated by the Ekman pumping on the surface Ekman boundary layer, and is also related to the leading order Coriolis term f 0 k × v in the quasi-geostrophic asymptotics; see Pedlosky [23].…”
Section: The Wind-driven Double-gyre Quasi-geostrophic Model Of Larmentioning
confidence: 99%
“…Given that in the interior of the ocean, motion along isopycnal surfaces is strongly favored over motion across them, this is a good first approximation (Pedlosky, 1998). …”
Section: Introductionmentioning
confidence: 99%