1998
DOI: 10.1175/1520-0469(1998)055<0710:tdbasi>2.0.co;2
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Three-Dimensional Buoyancy- and Shear-Induced Local Structure of the Atmospheric Boundary Layer

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Cited by 215 publications
(251 citation statements)
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“…The peak in the wave number -weighted alongwind spectrum is at lower wave number than the peak in the crosswind spectrum. This is consistent with observations and LES model results [e.g., Khanna and Brasseur, 1998] that show energy-containing scales elongated in the direction of near-surface shear in comparison to the cross-shear direction. It is also consistent with Langmuir circulation cells with their axes approximately aligned with the wind [e.g., Weller et al, 1985;Weller and Price, 1988].…”
Section: à2supporting
confidence: 92%
“…The peak in the wave number -weighted alongwind spectrum is at lower wave number than the peak in the crosswind spectrum. This is consistent with observations and LES model results [e.g., Khanna and Brasseur, 1998] that show energy-containing scales elongated in the direction of near-surface shear in comparison to the cross-shear direction. It is also consistent with Langmuir circulation cells with their axes approximately aligned with the wind [e.g., Weller et al, 1985;Weller and Price, 1988].…”
Section: à2supporting
confidence: 92%
“…Several previous studies (e.g., Moeng and Sullivan 1994;Khanna and Brasseur 1998) have shown that the flow regime of the boundary layer in general, and the formation of roll vortices in particular, may be characterized by the stability parameter −z i /L, where z i is the boundary-layer depth and L is the Obukhov length, …”
Section: Extreme Imbalancementioning
confidence: 99%
“…Moeng and Sullivan (1994) and Khanna and Brasseur (1998) estimate roll vortex formation is characterized by smaller values for −z i /L (roughly 1.5 < −z i /L < 10), these studies were limited to the clear boundary layer. Given that nearly every day is cloudy in the YOGA dataset, and that z i is defined as the height of the steepest gradient in the buoyancy profile (Schalkwijk et al 2015), which typically occurs above the cloud layer, some discrepancy may be attributed to cloudiness.…”
Section: Extreme Imbalancementioning
confidence: 99%
“…To analyze the influence of wind-shear characteristics on the evolution of the CBL, long simulations and large domains are necessary to fulfill a quasy-stationarity flow pattern that matches with the prescribed surface fluxes, and to resolve the expected pattern for forced convection (Khanna and Brasseur, 1998). With DALES, resolutions up to 25 m and 6 m in the horizontal and vertical directions, respectively were considered.…”
Section: Sheared Convective Boundary Layermentioning
confidence: 99%