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Effects of grid geometry on non-equilibrium dissipation in grid turbulence
http://hdl.handle.net/2237/26571
http://hdl.handle.net/2237/26571d3934afe-be60-457e-bb92-7268d920d1eb
名前 / ファイル | ライセンス | アクション |
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1_2E4973416.pdf ファイル公開:2018/01/01 (2.6 MB)
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Item type | 学術雑誌論文 / Journal Article(1) | |||||
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公開日 | 2017-06-06 | |||||
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タイトル | Effects of grid geometry on non-equilibrium dissipation in grid turbulence | |||||
言語 | en | |||||
著者 |
Nagata, Koji
× Nagata, Koji× Saiki, Teppei× Sakai, Yasuhiko× Ito, Yasumasa× Iwano, Koji |
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アクセス権 | open access | |||||
アクセス権URI | http://purl.org/coar/access_right/c_abf2 | |||||
権利 | ||||||
言語 | en | |||||
権利情報 | Copyright 2017 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. The following article appeared in (Physics of Fluids. v.29, n.1, 2017, p.015102) and may be found at (http://dx.doi.org/10.1063/1.4973416). | |||||
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内容記述タイプ | Abstract | |||||
内容記述 | A total of 11 grids in four families, including single- and multi-scale grids, are tested to investigate the development and decay characteristics of grid-generated turbulence. Special attention has been focused on dissipation and non-equilibrium characteristics in the decay region. A wide non-equilibrium region is observed for fractal square grids with three and four iterations. The distributions of the Taylor microscale λ, integral length scale Lu, and dissipation coefficient Cε show that a simple combination of large and small grids does not reproduce elongated non-equilibrium regions as realized by the fractal square grid. On the other hand, a new kind of grid, quasi-fractal grids, in which the region of the smaller fractal elements (N=2–4) of the fractal square grid is replaced by regular grids, successfully reproduce a similar flow field and non-equilibrium nature to that seen in the fractal square grid case. This suggests that the combination of large square grid and inhomogeneously arranged smaller grids produces an elongated non-equilibrium region. The dissipation coefficient Cε is better collapsed using Re0=t0U∞/ν (where t0 is the thickness of the largest grid bar, U∞ the inflow velocity, and ν the kinematic viscosity) as a global/inlet Reynolds number rather than ReM=MU∞/ν (where M is the mesh size) [P. C. Valente and J. C. Vassilicos, “Universal dissipation scaling for non-equilibrium turbulence,” Phys. Rev. Lett. 108, 214503 (2012)]. | |||||
言語 | en | |||||
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出版者 | AIP Publishing | |||||
言語 | en | |||||
言語 | ||||||
言語 | eng | |||||
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資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||
資源タイプ | journal article | |||||
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出版タイプ | VoR | |||||
出版タイプResource | http://purl.org/coar/version/c_970fb48d4fbd8a85 | |||||
DOI | ||||||
関連タイプ | isVersionOf | |||||
識別子タイプ | DOI | |||||
関連識別子 | https://doi.org/10.1063/1.4973416 | |||||
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収録物識別子タイプ | PISSN | |||||
収録物識別子 | 1070-6631 | |||||
書誌情報 |
en : Physics of Fluids 巻 29, 号 1, p. 015102-015102, 発行日 2017-01 |
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値 | publisher | |||||
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識別子 | http://dx.doi.org/10.1063/1.4973416 | |||||
識別子タイプ | DOI | |||||
URI | ||||||
識別子 | http://hdl.handle.net/2237/26571 | |||||
識別子タイプ | HDL |