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The Effects of Mesoscale Eddies on the Stratification and Transport of an Ocean with a Circumpolar Channel

机译:中尺度涡旋对绕极通道海洋的分层和输运的影响

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摘要

The effects of eddies in a primitive equation ocean model configured in a single hemisphere domain with circumpolar channels at their poleward ends are investigated; in particular, two regimes for the mass balance in the channel are investigated. With small overlying winds, the channel stratification is largely set by diffusion operating in the gyre portion of the domain: the depth scale varies with a fractional power of the diffusivity but has little dependence on the wind stress. As the winds are increased, the depth becomes increasingly controlled by a tendency toward small residual circulation. In this limit, a scaling theory is derived for the stratification in the channel that predicts the overall depth of the thermocline as a power of the wind stress and that allows the eddy length scale to differ from the channel length scale. The predicted depth depends on the details of the closure chosen for the eddy buoyancy flux, but in general it varies as some fractional power of the wind stress, and a channel-only numerical simulation agrees well with this prediction. When a gyre region is added to the channel, vertical diffusion in the gyre exerts some control on the channel stratification even at higher winds, forcing the mass balance into a mixed regime in which both eddy and diffusive effects are important. The depth scale varies less with the wind stress than in a channel-only configuration, and the residual mean circulation in the channel is maintained by the convergence of cross-isopycnal eddy buoyancy fluxes.
机译:研究了在单半球域中配置的原始方程海洋模型中涡流的影响,该半球域的极点两端具有绕极通道;特别是,研究了通道中两种质量平衡机制。在上覆小风的情况下,通道分层主要是由在该区域的回旋部分中的扩散作用决定的:深度尺度随扩散率的分数幂而变化,但对风应力的依赖性很小。随着风的增加,深度变得越来越倾向于通过残余循环较小的趋势来控制。在此限制下,推导了通道中分层的定标理论,该理论将温跃层的总深度作为风应力的幂进行预测,并允许涡流长度标度与通道长度标度不同。预测深度取决于为涡流浮力选择的闭合细节,但总的来说,它随风应力的分数功率而变化,仅基于通道的数值模拟与该预测非常吻合。当将回旋区添加到通道中时,回旋中的垂直扩散即使在较高风向时也可对通道分层施加一些控制,从而迫使质量平衡进入混合状态,在该混合状态中,涡旋和扩散效应都很重要。深度标度在风应力作用下的变化要比仅在通道中的变化小,并且通道中的剩余平均循环通过跨等深涡流浮力通量的收敛而得以维持。

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