Exchange flow through the strait of gibraltar as simulated by a s-coordinate hydrostatic model and a z-coordinate nonhydrostatic model

G. Sannino, J. C. S. Garrido, L. Liberti, L. Pratt
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引用次数: 28

Abstract

The Mediterranean Sea is a semi-enclosed basin displaying an active thermohaline circulation (MTHC) that is sustained by the atmospheric forcing and controlled by the narrow and shallow Strait of Gibraltar (hereinafter SoG). The atmospheric forcing drives the Mediterranean basin toward a negative budget of water and heat. Over the basin, evaporation exceeds the sum of precipitation and river discharge, while a net heat flux is transferred to the overlying atmosphere through the sea surface. These fluxes are balanced by the exchange flow that takes place in Gibraltar. Within the SoG, the MTHC takes the form of a two-way exchange: an upper layer of fresh and relatively warm Atlantic water spreads in the Mediterranean basin, and a lower layer of colder and saltier Mediterranean water sinks as a tongue in the North Atlantic at intermediate depths. The interaction between the intense tidal forcing [Candela et al., 1990] and the complex geometry of the SoG (Figure 3.1a) influences the two-way exchange via hydraulic control [Bryden and Stommel, 1984]. The exchange is subject to vigorous mixing and entrainment [Wesson and Gregg, 1994] as well as intermittent hydraulic controls over the main sills and in its narrowest sections [Sannino et al., 2007; Sannino et al., 2009a]. The simultaneous presence in the SoG of at least two cross sections in which the exchange is controlled drives the strait dynamics toward the so-called maximal regime [Bryden and Stommel, 1984; Armi and Farmer, 1988]. If the exchange is subject to only one hydraulic control, the regime is called submaximal. The two regimes have different implications for property fluxes, response time, and other physical characteristics of the coupled circulation in the SoG and Mediterranean Sea. The maximal regime can be expected to have larger heat, salt, and mass fluxes and to respond more slowly to changes in stratification and thermohaline forcing within the Mediterranean Sea and the North Atlantic Ocean [Sannino et al., 2009a]. As first recognized by Bray et al. [1995], the strong entrainment and mixing present in the Strait of Gibraltar lead to the formation of a thick interfacial layer where density and velocity change gradually in the vertical direction. They also argued that the classical two-layer approach used to describe the two-way exchange was insufficient to account for the flow regime in the SoG. They found that a three-layer system, which includes an active interface layer, best represents the exchange through the SoG. The presence of a thick interfacial layer complicates the estimation of the hydraulic state of the flow exchange using the two-layer hydraulic theory. Such difficulty has been recently overcome by Sannino et al. [2007] who analyzed for the fist time the hydraulic regime of the exchange flow applying a three-layer hydraulic theory. Doing so they considered the thick interfacial layer as an active participant of the hydraulic regime. The hydraulic studies conducted by Sannino et al. [2007] were based on the analysis of numerical simulations. The simulations were carried out using a σ-coordinate model 3
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用s坐标流体静力模型和z坐标非流体静力模型模拟直布罗陀海峡交换流
地中海是一个半封闭的盆地,表现出活跃的热盐环流(MTHC),该环流由大气强迫维持,并由狭窄而浅的直布罗陀海峡(以下简称直布罗陀海峡)控制。大气强迫使地中海盆地的水和热呈负平衡。在盆地上空,蒸发量超过降水和河流流量的总和,同时净热通量通过海面传递给上覆大气。这些流动被发生在直布罗陀的交换流量所平衡。在SoG内部,MTHC以双向交换的形式存在:上层新鲜和相对温暖的大西洋水在地中海盆地扩散,下层较冷和较咸的地中海水在北大西洋的中等深度下沉。强烈的潮汐强迫[Candela et al., 1990]和SoG的复杂几何形状(图3.1a)之间的相互作用通过水力控制影响双向交换[Bryden and Stommel, 1984]。交换受到强烈的混合和夹带[Wesson和Gregg, 1994]以及主要技能和最窄部分的间歇性液压控制[Sannino等人,2007;Sannino等,2009 [a]。在SoG中同时存在至少两个交换受到控制的横截面,将海峡动力学推向所谓的最大状态[Bryden和Stommel, 1984;Armi and Farmer, 1988]。如果交换只受一种液压控制,则称为次最大状态。这两种机制对南海和地中海耦合环流的性质通量、响应时间和其他物理特征有不同的影响。预计最大状态将具有更大的热、盐和质量通量,并且对地中海和北大西洋内分层和热盐强迫的变化反应更慢[Sannino等,2009a]。Bray等人[1995]首先发现,直布罗陀海峡存在强烈的夹带和混合,导致形成一个厚的界面层,密度和速度在垂直方向上逐渐变化。他们还认为,用于描述双向交换的经典两层方法不足以解释SoG中的流态。他们发现一个三层系统,其中包括一个活动接口层,最好地代表了通过SoG的交换。厚界面层的存在使得用两层水力理论估计流动交换的水力状态变得复杂。最近,Sannino等人[2007]克服了这一困难,首次运用三层水力理论分析了交换流的水力状态。在这样做时,他们认为厚界面层是水力制度的积极参与者。Sannino等[2007]的水力研究是基于数值模拟分析。仿真采用σ-坐标模型3
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