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首页> 外文期刊>Journal of Physical Oceanography >A Unified Model Spectrum for Anisotropic Stratified and Isotropic Turbulence in the Ocean and Atmosphere
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A Unified Model Spectrum for Anisotropic Stratified and Isotropic Turbulence in the Ocean and Atmosphere

机译:海洋和大气各向异性分层和各向同性湍流的统一模型谱

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In the decade or so below the Ozmidov wavenumber (N-3/epsilon)(1/2), that is, on scales between those attributed to internal gravity waves and isotropic turbulence, ocean and atmosphere measurements consistently find k(1/3) horizontal wavenumber spectra for horizontal shear u(h) and horizontal temperature gradient T-h and m(-1) vertical wavenumber spectra for vertical shear u(z) and strain xi(z). Dimensional scaling is used to construct model spectra below as well as above the Ozmidov wavenumber that reproduces observed spectral slopes and levels in these two bands in both vertical and horizontal wavenumber. Aspect ratios become increasingly anisotropic below the Ozmidov wavenumber until reaching similar to O(f/N), where horizontal shear u(h) similar to f. The forward energy cascade below the Ozmidov wavenumber found in observations and numerical simulations suggests that anisotropic and isotropic turbulence are manifestations of the same nonlinear downscale energy cascade to dissipation, and that this turbulent cascade originates from anisotropic instability of finescale internal waves at horizontal wavenumbers far below the Ozmidov wavenumber. Isotropic turbulence emerges as the cascade proceeds through the Ozmidov wavenumber where shears become strong enough to overcome stratification. This contrasts with the present paradigm that geophysical isotropic turbulence arises directly from breaking internal waves. This new interpretation of the observations calls for new approaches to understand anisotropic generation of geophysical turbulence patches.
机译:在Ozmidov波数(N-3 / epsilon)(1/2)以下的十年左右的时间里,即在归因于内部重力波和各向同性湍流的尺度之间,海洋和大气测量值始终得出k(1/3)水平剪切力u(h)和水平温度梯度Th和m(-1)的水平波数谱垂直剪切力u(z)和应变xi(z)的垂直波数谱。维比例缩放用于构造Ozmidov波数以下和Ozmidov波数以上的模型光谱,该模型在垂直和水平波数中均再现了这两个波段中观察到的光谱斜率和水平。在Ozmidov波数以下,长宽比变得越来越各向异性,直到达到与O(f / N)相似的水平,而水平剪切u(h)与f相似。在观测和数值模拟中发现的Ozmidov波数以下的正向能量级联表明,各向异性和各向同性湍流是相同的非线性降级能量级联到耗散的表现,并且该湍流级联源自水平波数远低于此的细尺度内部波的各向异性不稳定性。奥兹米多夫波数。各向同性湍流随着级联通过Ozmidov波数而出现,在那里剪切变得足够强大以克服分层。这与目前的范例相反,地球物理学的各向同性湍流直接来自破坏内部的波。对观测结果的这种新解释要求采用新方法来理解地球物理湍流斑块的各向异性生成。

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