The Share of the Mean Turbulent Kinetic Energy in the Near-Neutral Surface Layer for High and Low Wind Speeds

We examine the dependence on wind speed of the share of the mean turbulent kinetic energy among the three velocity components in the near-neutral surface layer. To contrast the general behaviour and the local effects, four datasets are considered, corresponding to different surfaces and environmenta...

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Published inBoundary-layer meteorology Vol. 172; no. 1; pp. 81 - 106
Main Authors Schiavon, M., Tampieri, F., Bosveld, F. C., Mazzola, M., Castelli, S. Trini, Viola, A. P., Yagüe, C.
Format Journal Article
LanguageEnglish
Published Dordrecht Springer Netherlands 01.07.2019
Springer
Springer Nature B.V
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Abstract We examine the dependence on wind speed of the share of the mean turbulent kinetic energy among the three velocity components in the near-neutral surface layer. To contrast the general behaviour and the local effects, four datasets are considered, corresponding to different surfaces and environmental conditions. For high wind speeds (i.e., wind speed ≈ 10 ms - 1 ), the shares are well-defined and about the same for all sites. As wind speed decreases (becoming ≈ 1 ms - 1 ), large record-to-record variability occurs giving, on average, an almost isotropic state for the horizontal velocity components. Through spectral analysis, we relate this behaviour to the low-frequency, submeso motions and to the lack of conditions required by Reynolds averaging. The implications for modelling are also discussed, showing that the wind speed, or a related quantity, must be accounted for, besides stability, in second-order closures.
AbstractList We examine the dependence on wind speed of the share of the mean turbulent kinetic energy among the three velocity components in the near-neutral surface layer. To contrast the general behaviour and the local effects, four datasets are considered, corresponding to different surfaces and environmental conditions. For high wind speeds (i.e., wind speed \[\approx {10}\,{\hbox {ms}^{-1}}\]), the shares are well-defined and about the same for all sites. As wind speed decreases (becoming \[\approx {1}\,{\hbox { ms}^{-1}}\]), large record-to-record variability occurs giving, on average, an almost isotropic state for the horizontal velocity components. Through spectral analysis, we relate this behaviour to the low-frequency, submeso motions and to the lack of conditions required by Reynolds averaging. The implications for modelling are also discussed, showing that the wind speed, or a related quantity, must be accounted for, besides stability, in second-order closures.
We examine the dependence on wind speed of the share of the mean turbulent kinetic energy among the three velocity components in the near-neutral surface layer. To contrast the general behaviour and the local effects, four datasets are considered, corresponding to different surfaces and environmental conditions. For high wind speeds (i.e., wind speed ≈ 10 ms - 1 ), the shares are well-defined and about the same for all sites. As wind speed decreases (becoming ≈ 1 ms - 1 ), large record-to-record variability occurs giving, on average, an almost isotropic state for the horizontal velocity components. Through spectral analysis, we relate this behaviour to the low-frequency, submeso motions and to the lack of conditions required by Reynolds averaging. The implications for modelling are also discussed, showing that the wind speed, or a related quantity, must be accounted for, besides stability, in second-order closures.
We examine the dependence on wind speed of the share of the mean turbulent kinetic energy among the three velocity components in the near-neutral surface layer. To contrast the general behaviour and the local effects, four datasets are considered, corresponding to different surfaces and environmental conditions. For high wind speeds (i.e., wind speed [Formula omitted]), the shares are well-defined and about the same for all sites. As wind speed decreases (becoming [Formula omitted]), large record-to-record variability occurs giving, on average, an almost isotropic state for the horizontal velocity components. Through spectral analysis, we relate this behaviour to the low-frequency, submeso motions and to the lack of conditions required by Reynolds averaging. The implications for modelling are also discussed, showing that the wind speed, or a related quantity, must be accounted for, besides stability, in second-order closures.
Audience Academic
Author Yagüe, C.
Mazzola, M.
Tampieri, F.
Bosveld, F. C.
Schiavon, M.
Viola, A. P.
Castelli, S. Trini
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  surname: Schiavon
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  organization: Department of Physics and Astronomy, Univeristy of Bologna, Institute of Atmospheric Sciences and Climate - ISAC-CNR
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  givenname: F.
  surname: Tampieri
  fullname: Tampieri, F.
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  surname: Bosveld
  fullname: Bosveld, F. C.
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  givenname: A. P.
  surname: Viola
  fullname: Viola, A. P.
  organization: Institute of Atmospheric Sciences and Climate - ISAC-CNR
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  givenname: C.
  surname: Yagüe
  fullname: Yagüe, C.
  organization: Dpt. Física de la Tierra y Astrofísica, Facultad de CC. Físicas, Universidad Complutense de Madrid
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Keywords Low wind speed
Turbulent kinetic energy
Submeso motions
Velocity spectra
Dissipation rate
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Snippet We examine the dependence on wind speed of the share of the mean turbulent kinetic energy among the three velocity components in the near-neutral surface...
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StartPage 81
SubjectTerms Analysis
Atmospheric Protection/Air Quality Control/Air Pollution
Atmospheric Sciences
Closures
Components
Dependence
Earth and Environmental Science
Earth Sciences
Environmental conditions
Force and energy
Kinetic energy
Low wind speeds
Meteorology
Modelling
Research Article
Reynolds averaging
Spectral analysis
Stability
Surface boundary layer
Surface layers
Turbulent kinetic energy
Velocity
Wind
Wind speed
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Title The Share of the Mean Turbulent Kinetic Energy in the Near-Neutral Surface Layer for High and Low Wind Speeds
URI https://link.springer.com/article/10.1007/s10546-019-00435-6
https://www.proquest.com/docview/2183932637
Volume 172
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