海洋中的日暖层:能量学、非维缩放和参数化

M. Schmitt, H. T. Pham, S. Sarkar, K. Klingbeil, L. Umlauf
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摘要

昼暖层(DWLs)在太阳辐射强、风力弱至中等、面波效应小的日子里形成于海洋表面附近。在这里,我们使用理想化的第二时刻湍流模型,并通过大涡流模拟(LES)进行验证,来研究整个物理相关参数空间内 DWL 的特性、动力学和能量学。这两类模型都包含朗缪尔湍流(LT)。我们发现,在平衡波条件下,LT 只对 DWL 厚度和其他体积参数产生轻微的改变,但会导致表面温度和速度的强烈下降,可能对海气耦合产生影响。通过比较热带和研究较少的高纬度 DWL,我们发现 LT 对能量预算有很大影响,高纬度的旋转强烈地改变了 DWL 的能量学,抑制了净能量转换和夹带。我们确定了 DWL 演化的关键非尺寸参数,并发现 Price 等人(1986 年)的比例关系可靠地代表了包括高纬度 DWL 在内的宽广参数空间中的 DWL 体积特性。我们提出了不同的修正模式系数集,其中包括由于低纬度和我们更先进的湍流模式的其他方面造成的 DWL 变深,以描述正午和下午 DWL 温度峰值期间的 DWL 特性,我们发现在广泛的参数范围内,温度峰值出现在 15:00-16:30 左右。
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Diurnal Warm Layers in the ocean: Energetics, non-dimensional scaling, and parameterization
Diurnal Warm Layers (DWLs) form near the surface of the ocean on days with strong solar radiation, weak to moderate winds, and small surface-wave effects. Here, we use idealized second-moment turbulence modelling, validated with Large Eddy Simulations (LES), to study the properties, dynamics and energetics of DWLs across the entire physically relevant parameter space. Both types of models include representations of Langmuir turbulence (LT). We find that LT only slightly modifies DWL thicknesses and other bulk parameters under equilibrium wave conditions, but leads to a strong reduction in surface temperature and velocity with possible implications for air-sea coupling. Comparing tropical and the less frequently studied high-latitude DWLs, we find that LT has a strong impact on the energy budget and that rotation at high latitudes strongly modifies the DWL energetics, suppressing net energy turnover and entrainment. We identify the key non-dimensional parameters for DWL evolution and find that the scaling relations of Price et al. (1986) provide a reliable representation of the DWL bulk properties across a wide parameter space, including high-latitude DWLs. We present different sets of revised model coefficients that include the deepening of the DWL due to LT and other aspects of our more advanced turbulence model to describe DWL properties at midday and during the DWL temperature peak in the afternoon, which we find to occur around 15:00-16:30 for a broad range of parameters.
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