2004
DOI: 10.1357/002224004774201681
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Wind-driven barotropic gyre I: Circulation control by eddy vorticity fluxes to an enhanced removal region

Abstract: It is well known that the barotropic, wind-driven, single-gyre ocean model reaches an inertiallydominated equilibrium with unrealistic circulation strength when the explicit viscosity is reduced to realistically low values. It is shown here that the overall circulation strength can be controlled nonlocally by retaining thin regions of enhanced viscosity parameterizing the effects of increased mixing and topographic interaction near the boundaries. The control is possible even when the inertial boundary layer w… Show more

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Cited by 34 publications
(50 citation statements)
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“…This is consistent with the barotropic single-gyre solutions (Fox-Kemper and Pedlosky 2004), which have no thickness fluxes. The thickness flux recirculates in the form of the large-scale, cyclonic gyre that covers the WBC/EJ region.…”
Section: Vorticity-type Componentssupporting
confidence: 89%
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“…This is consistent with the barotropic single-gyre solutions (Fox-Kemper and Pedlosky 2004), which have no thickness fluxes. The thickness flux recirculates in the form of the large-scale, cyclonic gyre that covers the WBC/EJ region.…”
Section: Vorticity-type Componentssupporting
confidence: 89%
“…The flux maintains the global PV budget (17) by transporting PV from the boundaries into the basin interior and from one gyre to the other. In the first mechanism, PV generated on the boundary is fluxed through the viscous boundary layer by the diffusion, then it is picked up and fluxed farther away by the eddies (Fox-Kemper and Pedlosky 2004). The boundary source of PV is large when the relative vorticity has large horizontal gradient in the off-boundary direction, as it occurs here in the western basin.…”
Section: Full Time-mean Eddy Fluxesmentioning
confidence: 97%
“…a viscous sublayer), as eddies flux PV into the high friction boundary layer, where it can be dissipated more effectively. Fox-Kemper and Pedlosky (2004) illustrate that inertia and friction can co-exist effectively in a balanced gyre circulation, and that friction is necessary even in a strongly inertial system.…”
Section: Introductionmentioning
confidence: 89%
“…As discussed in Fox- Kemper and Pedlosky (2004), in ocean models with constant viscosity, if the inertial boundary layer is larger than the frictional boundary layer, i.e. the advection of PV is stronger than the dissipation of PV, the inertial boundary layer expands until it fills the entire domain.…”
Section: Introductionmentioning
confidence: 99%
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