Estimates of eddy diffusivity in bottom boundary layer of the Bornholm Deep

V. Paka, V. Zhurbas
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引用次数: 1

Abstract

Reliable estimate of eddy diffusivity in the bottom boundary layer (BBL) of the Bornholm Deep is the issue of practical importance because it would control dispersion of the chemical warfare agents dumped in the Deep after WW II [Helcom, 1994]. The most common way to arrive at an estimate of the eddy diffusivity, K is to apply a well-known parameterization of mixing in the Baltic halocline due to internal wave instability suggested by [A. Stigebrandt, 1987] K = min(Kmax, alpha/N), where Kmax is the maximum value of K, N is the buoyancy frequency, and alpha =1times10-7 m2 s-2 [H.E.M. Meier, 2007] or alpha = 0.87times10-7 m2 s-2 [H.-U. Lass, 2003] is the empirical constant. Taking NBBL =0.02 s-1 for near-bottom layer and Nhalocline =0.03 s-1 for the halocline in the Bornholm Deep [J. Elken, 1996] one obtains KBBL= 0.5times10-5 m2 s-1 and Khalocline = 0.33times10-5 m2 s-1. However, the above estimate of KBBL does not take into account the possibility of enhancement of eddy diffusivity in BBL due shear instability of the near-bottom current and a variety of mechanisms of boundary mixing [J.H. Reissmann, 2007]. Numerical simulations based on the Princeton Ocean Model with a second and a half moment turbulence closure by Mellor and Yamada [1982] embedded brought for eddy diffusivity in the Bornholm Deep BBL and the BBL thickness the values of KBBL1= 2.5times10-4 m2 s-1 and hBBL1 = 2 m respectively. Eddy diffusivity in the Bornholm Deep BBL can be also estimated using data of tow-yo CTD profiling in a near-bottom layer performed aboard R/V Shelf in Summer 2006.
博恩霍尔姆深底边界层涡动扩散系数的估计
对Bornholm深水底边界层(BBL)涡漩扩散率的可靠估计具有实际重要性,因为它将控制二战后倾倒在深水中的化学战剂的扩散[Helcom, 1994]。估算涡旋扩散系数K的最常用方法是应用众所周知的波罗的海盐跃层由内波不稳定性引起的混合参数化[a]。Stigebrandt, 1987] K = min(Kmax, alpha/N),其中Kmax为K的最大值,N为浮力频率,alpha =1倍10-7 m2 s-2 [H.E.M.。Meier, 2007]或alpha = 0.87times10-7 m2 s-2 [h - u。Lass, 2003]是经验常数。取近底层NBBL =0.02 s-1,盐斜=0.03 s-1 [J]。Elken, 1996]得到KBBL= 0.5times10-5 m2 s-1, Khalocline = 0.33times10-5 m2 s-1。然而,上述对KBBL的估计没有考虑到近底流剪切不稳定和多种边界混合机制对BBL涡旋扩散率增强的可能性[J.H.]Reissmann, 2007]。基于普林斯顿海洋模式的数值模拟,嵌入了Mellor和Yamada[1982]的秒半湍流关闭,得到Bornholm深部BBL的涡动扩散系数和BBL厚度分别为KBBL1= 2.5times10-4 m2 s-1和hBBL1 = 2 m。利用2006年夏季在R/V Shelf上进行的近底层两yo CTD剖面数据,也可以估计Bornholm深层BBL的涡流扩散系数。
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