Angular distribution of energy spectrum in two-dimensional β-plane turbulence in the long-wave limit
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The time-evolution of two-dimensional decaying turbulence governed by the long-wave limit, in which L_{D}IL → 0, of the quasi-geostrophic equation is investigated numerically. Here, LD is the Rossby radius of deformation, and L is the characteristic length scale of the flow. In this system, the ratio of the linear term that originates from the β-term to the nonlinear terms is estimated by a dimensionless number, γ = βL_{D}^{2}IU, where β is the latitudinal gradient of the Coriolis parameter, and U is the characteristic velocity scale. As the value of γ increases, the inverse energy cascade becomes more anisotropic. When γ ⩾ 1, the anisotropy becomes significant and energy accumulates in a wedge-shaped region where |I|>{√3}|k| in the two-dimensional wavenumber space. Here, k and I are the longitudinal and latitudinal wavenumbers, respectively. When γ is increased further, the energy concentration on the lines of I = ±{√3}K is clearly observed. These results are interpreted based on the conservation of zonostrophy, which is an extra invariant other than energy and enstrophy and was determined in a previous study. Considerations concerning the appropriate form of zonostrophy for the long-wave limit and a discussion of the possible relevance to Rossby waves in the ocean are also presented.
収録刊行物
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- Physics of Fluids
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Physics of Fluids 25 (7), 2013-07-18
AIP Publishing LLC
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詳細情報 詳細情報について
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- CRID
- 1050282810754516352
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- NII論文ID
- 120005323020
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- NII書誌ID
- AA10986202
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- ISSN
- 10706631
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- HANDLE
- 2433/178670
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- 本文言語コード
- en
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- 資料種別
- journal article
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- データソース種別
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- IRDB
- CiNii Articles