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Passive scalar transport by travelling wave fields

机译:通过行波场进行被动标量传输

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We study turbulent transport of passive tracers by random wave fields of a rather general nature. A formalism allowing for spatial inhomogeneity and anisotropy of an underlying velocity field (such as that caused by a latitudinally varying Coriolis parameter) is developed, with the aim of treating problems of large-scale ocean transport by long internal waves. For the special case of surface gravity waves on deep water, our results agree with the earlier theory of Herterich & Hasselmann (1982), though even in that case we discover additional, off-diagonal elements of the diffusion tensor emerging in the presence of a mean drift. An advective diffusion equation including all components of the diffusion tensor D plus a mean, Stokes-type drift u is derived and applied to the case of baroclinic inertia-gravity (BIG) waves. This application is of particular interest for ocean circulation and climate modelling, as the mean drift, according to our estimates, is comparable to ocean interior currents; Furthermore, while on the largest (100 km and greater) scales, wave-induced diffusion is found to be generally small compared to classical eddy-induced diffusion, the two become comparable on scales below 10 km. These scales are near the present limit on the spatial resolution of eddy-resolving ocean numerical models. Since we find that u(z) and D-zz vanish identically, net vertical transport is absent in wave systems of this type. However, for anisotropic wave spectra the diffusion tensor can have non-zero off-diagonal vertical elements, D-xz and D-yz, and it is shown that their presence leads to non-positive definiteness of D, and a negative diffusion constant is found along a particular principal axis. However, the simultaneous presence of a depth-dependent mean horizontal drift rc(z) eliminates any potential unphysical behaviour. [References: 34]
机译:我们通过相当普遍的性质的随机波场研究被动示踪剂的湍流传输。为了解决由长内波引起的大规模海洋运输问题,提出了一种形式主义,该形式主义允许潜在的速度场存在空间不均匀性和各向异性(例如由纬度变化的科里奥利参数引起的速度场各向异性)。对于深水表面重力波的特殊情况,我们的结果与较早的Herterich&Hasselmann(1982)的理论一致,尽管即使在这种情况下,我们也发现了在存在水的情况下出现的扩散张量的其他非对角元素。平均漂移。推导包含对流张量D的所有分量加上均值Stokes型漂移u的对流扩散方程,并将其应用于斜压惯性重力(BIG)波的情况。这种应用对于海洋环流和气候模拟特别感兴趣,因为根据我们的估计,平均漂移可与海洋内部洋流相提并论。此外,虽然在最大的尺度上(100 km和更大),与经典的涡流诱导的扩散相比,波诱导的扩散通常较小,但在10 km以下的尺度上,两者可比。这些比例接近解析涡旋海洋数值模型空间分辨率的当前极限。由于我们发现u(z)和D-zz消失相同,因此在这种类型的波浪系统中没有净垂直传输。但是,对于各向异性波谱,扩散张量可以具有非零的非对角垂直元素D-xz和D-yz,并且表明它们的存在导致D的正定性,并且负扩散常数为沿特定主轴找到。但是,同时存在依赖于深度的平均水平漂移rc(z)消除了任何潜在的非物理行为。 [参考:34]

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