南大西洋和南极中间水中的氯氟甲烷

Mark J. Warner , Ray F. Weiss
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引用次数: 80

摘要

利用南大西洋大气中溶解氯氟甲烷(CFMs) F-11和F-12的分布研究了南极中间水(AAIW)的通风和环流。以AAIW为代表的等气旋地面CFM分布与最近进入西南大西洋副热带环流的通风水并在该环流周围进行反气旋平流相一致。环流向西流动的北支在南美洲海岸附近明显分裂,一些水向南流动,在环流中再循环,其余水沿巴西海岸向北流动。在赤道,这股向北的洋流又分岔了,一股沿着赤道向东,另一股继续流入北半球。在热带大西洋东部,在副热带环流和赤道舌区之间的气旋环流中,CFM的浓度极低。沿本初子午线,混合层露头与副热带环流北缘之间的27.2 θσ等压面F-11和F-12浓度符合一维平流扩散模式。该模式假设cfm仅通过从混合层露头向副热带环流南缘的北扩散进入管热带环流,其在环流内的分布受平流和扩散过程控制。速度和涡流扩散系数由最小二乘拟合数据计算。然后用这些值计算平均耗氧速率,该速率与使用其他随时间变化的地球化学示踪剂模型计算的速率一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Chlorofluoromethanes in South Atlantic Antartic intermediate water

Distribution of the dissolved atmospheric chlorofluoromethanes (CFMs) F-11 and F-12 in the South Atlantic Ocean are used to study the ventilation and circulation of Antarctic Intermediate Water (AAIW). CFM distributions on an isopycnal surface representative of AAIW are consistent with recently ventilated water entering the subtropical gyre in the southwestern Atlantic and then being advected anticyclonically around this gyre. The westward-flowing northern limb of the gyre apparently divides near the coast of South America with some water flowing southward to recirculate in the gyre, and the balance flowing northward along the coast of Brazil. At the equator this northward current divides again with one branch going eastward along the equator and the other continuing into the Northern Hemisphere. In the eastern tropical Atlantic, the CFM concentrations on this isopycnal surface in the cyclonic gyre are extremely low between the subtropical gyre and the equatorial tongue. Along the prime meridian, the F-11 and F-12 concentrations on the 27.2 θσ isopycnal surface between the mixed layer outcrop and the northern edge of the subtropical gyre are fitted to a one-dimensional advection-diffusion model. This model assumes that the CFMs enter the tubtropical gyre solely by northward diffusion from the mixed layer outcrop to the southern edge of the subtropical gyre, and that their distributions within the gyre are controlled by both advective and diffusive processes. Velocity and eddy diffusion coefficients are calculated from a least-squares fit to the data. These values are then used to calculate a mean oxygen consumption rate which is consistent with rates calculated using models of other time-dependent geochemical tracers.

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