2005
DOI: 10.1007/s10546-005-3780-1
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Single-Column Model Intercomparison for a Stably Stratified Atmospheric Boundary Layer

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Cited by 312 publications
(381 citation statements)
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“…A possible explanation is that, to avoid numerical instability potentially resulting from thermal decoupling of the surface and atmosphere, operational models tend to overestimate the level of background turbulence in very stable conditions. This is a common problem for climate models as well (Tjernström et al, 2005), and was also revealed in the Global Energy and Water Cycle Experiment (GEWEX) Atmospheric Boundary Layer Study (GABLS) experiments (Cuxart et al, 2006;Steeneveld et al, 2006;Svensson et al, 2011).…”
Section: Discussionmentioning
confidence: 81%
“…A possible explanation is that, to avoid numerical instability potentially resulting from thermal decoupling of the surface and atmosphere, operational models tend to overestimate the level of background turbulence in very stable conditions. This is a common problem for climate models as well (Tjernström et al, 2005), and was also revealed in the Global Energy and Water Cycle Experiment (GEWEX) Atmospheric Boundary Layer Study (GABLS) experiments (Cuxart et al, 2006;Steeneveld et al, 2006;Svensson et al, 2011).…”
Section: Discussionmentioning
confidence: 81%
“…gradient Richardson number or Obukhov length, see Delage and Girard (1992), Delage (1997), Mahrt and Vickers (2003), Han et al (2009)]. 1.5-order models formulate diffusivity as a function of turbulent kinetic energy (e = 1 2 (u 2 + v 2 + w 2 )) and/or other variances of turbulent fluctuating components in addition to mixing length and stability (Mellor and Yamada 1974;Bougeault and Lacarrere 1989;Bélair et al 1999;Cuxart et al 2006). Full second-and third-order models may eliminate the need for momentum and heat diffusivity parametrization because they formulate and solve all second-and third-moment equations, respectively.…”
Section: Downgradient Transportmentioning
confidence: 99%
“…by vertical diffusion of momentum, heat, moisture, and other atmospheric constituents above the surface layer (Cuxart et al 2006). In this approach all relevant equations are simplified by Reynolds averaging, where each variable of interest is decomposed into a mean and a turbulent fluctuating part (X = X + X ).…”
Section: Introductionmentioning
confidence: 99%
“…Even at the top of the rotor, where we expect fetch to matter most, reduction of the patch area, from 56.3 2 to 20 2 km 2 , yields a wind-speed increase that is only 22 % smaller than the original result. Some caution is advised, however, as studies have found the WRF model to produce unrealistically large vertical mixing (e.g., Cuxart and Holtslag 2006;Storm et al 2010), which may explain some of the insensitivity of rotor-layer wind speed to patch size. …”
Section: Impacts Across the Wind Farm In Various Stability Regimesmentioning
confidence: 99%