| 作成者 |
|
|
|
|
|
| 本文言語 |
|
| 出版者 |
|
| 発行日 |
|
| 収録物名 |
|
| 巻 |
|
| 開始ページ |
|
| 出版タイプ |
|
| アクセス権 |
|
| 権利関係 |
|
|
|
| 関連DOI |
|
|
|
| 概要 |
With the aim of assessing internal wave-driven mixing in the ocean, we develop a new technique for direct numerical simulations of stratified turbulence. Since the spatial scale of oceanic internal gr...avity waves is typically much larger than that of turbulence, fully incorporating both in a model would require a high computational cost, and is therefore out of our scope. Alternatively, we cut out a small domain periodically distorted by an unresolved large-scale internal wave and locally simulate the energy cascade to the smallest scales. In this model, even though the Froude number of the outer wave, 𝐹𝑟, is small such that density overturn or shear instability does not occur, a striped pattern of disturbance is exponentially amplified through a parametric subharmonic instability. When the disturbance amplitude grows sufficiently large, secondary instabilities arise and produce much smaller-scale fluctuations. Passing through these two stages, wave energy is transferred into turbulence energy and will be eventually dissipated. Different from the conventional scenarios of vertical shear-induced instabilities, a large part of turbulent potential energy is supplied from the outer wave and directly used for mixing. The mixing coefficient 𝛤=𝜖_𝑃/𝜖, where 𝜖 is the dissipation rate of kinetic energy and 𝜖𝑃 is that of available potential energy, is always greater than 0.5 and tends to increase with 𝐹𝑟. Although our results are mostly consistent with the recently proposed scaling relationship between 𝛤 and the turbulent Froude number, 𝐹𝑟_𝑡, the values of 𝛤 obtained here are larger by a factor of about two than previously reported.続きを見る
|
Mendeley出力
