低频率运动的温度水平平流

Harry L. Bryden
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引用次数: 54

摘要

通过使用温度水平平流作为速度的函数的表示并在水平电流的垂直方向上旋转,可以以很小的误差估计低频水平平流的温度。在这些误差范围内,温度水平平流解释了40天内波实验(IWEX)期间观测到的局部温度变化。水平平流的重要性表明,主要的热平衡不是像平均分层线性化的波浪模式所假定的那样,由垂直平流平衡的局地温度变化。这些估计表明,一个更合适的线性模型应该基于一个平均状态,包括平均水平温度梯度,从而包括水平速度的平均垂直切变。然而,平均状态不是长期平均状态,而是与超过40天测量周期的时间尺度运动相关的状态。利用这种线性化,与斜压不稳定模型进行了比较,研究了不同时间尺度运动之间的能量传递。在该模型中,平均场和扰动场之间的势能传递方向可以通过负水平平流与局部温度变化之间的时间相位滞后符号来确定。对于这些估计,负水平平流导致局部变化,表明平均势能在以扰动势能为代价的情况下增加。然而,这个相位滞后与零相差不大,因此需要更长的记录来确定势能传递的方向。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Horizontal advection of temperature for low-frequency motions

Estimates of low-frequency horizontal advection of temperature are made with small errors by using a representation of horizontal advection of temperature as a function of the speed and turning about the vertical of the horizontal current. Within these errors the horizontal advection of temperature accounts for the observed local time changes of temperature during the 40-day Internal Wave Experiment (IWEX) period. The importance of horizontal advection indicates the dominant heat balance is not that of local time change of temperature balanced by vertical advection of temperature as assumed in wave models linearized about a mean stratification. These estimates suggest that a more appropriate linear model should be based on a mean state including mean horizontal gradients of temperature and hence a mean vertical shear of horizontal velocity. The mean state is not that of the long-term mean, however, but one associated with motions of time-scale longer than the measurement period of 40 days. Using this linearization, comparisons are made with a baroclinic instability model to investigate energy transfer between motions of different time-scales. In the context of this model, the direction of potential energy transfer between the mean and perturbation fields can be determined from the sign of the temporal phase lag between negative horizontal advection and local change of temperature. For these estimates negative horizontal advection leads local change suggesting that mean potential energy is increasing at the expense of perturbation potential energy. This phase lag, however, is not significantly different from zero so that a longer record is needed to establish the direction of potential energy transfer.

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