2009
DOI: 10.1175/2008mwr2582.1
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Large-Eddy Simulations of a Drizzling, Stratocumulus-Topped Marine Boundary Layer

Abstract: Cloud water sedimentation and drizzle in a stratocumulus-topped boundary layer are the focus of an intercomparison of large-eddy simulations. The context is an idealized case study of nocturnal stratocumulus under a dry inversion, with embedded pockets of heavily drizzling open cellular convection. Results from 11 groups are used. Two models resolve the size distributions of cloud particles, and the others parameterize cloud water sedimentation and drizzle. For the ensemble of simulations with drizzle and clou… Show more

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Cited by 236 publications
(414 citation statements)
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“…The horizontal grid spacing of these LES cases is fixed at 50 m, while the vertical grid is stretched, with a minimum spacing of 5 m near the surface and the capping temperature inversion to better resolve small-scale turbulence there. Further details of the model setup for the DYCOMS-II case are provided in Ackerman et al (2009). The ATEX cases are updated model runs with increased spatial resolution that are similar to the cases discussed in Fridlind and Ackerman (2011).…”
Section: Model and Methodologymentioning
confidence: 99%
“…The horizontal grid spacing of these LES cases is fixed at 50 m, while the vertical grid is stretched, with a minimum spacing of 5 m near the surface and the capping temperature inversion to better resolve small-scale turbulence there. Further details of the model setup for the DYCOMS-II case are provided in Ackerman et al (2009). The ATEX cases are updated model runs with increased spatial resolution that are similar to the cases discussed in Fridlind and Ackerman (2011).…”
Section: Model and Methodologymentioning
confidence: 99%
“…For example, the intercomparison based on DYCOMS-II demonstrated a substantial range in inter-model surface precipitation rates for the drizzling, stratocumulus-topped boundary layer case (see Ackerman et al, 2009). Ackerman et al (2009) argue that this range results from differences in model dynamics.…”
Section: Introductionmentioning
confidence: 99%
“…For example, the intercomparison based on DYCOMS-II demonstrated a substantial range in inter-model surface precipitation rates for the drizzling, stratocumulus-topped boundary layer case (see Ackerman et al, 2009). Ackerman et al (2009) argue that this range results from differences in model dynamics. Although evidence is presented for this claim, the fact that the microphysics and dynamics are coupled in these simulations means that it is difficult to say to what extent the spread can be attributed to the different numerical methods for dynamics alone or interactions between dynamics and microphysics.…”
Section: Introductionmentioning
confidence: 99%
“…This may explain why the SCM leaves excessive moisture in the sub-cloud layer as compared with SAM LES (see Figure 1(b)). Nevertheless, both SCM profiles of w 2 lie within the range of the LES models (grey shaded region in Figure 1(c)) that participated in the GCSS intercomparison (Ackerman et al, 2009). The vertical velocity variance w 2 indirectly influences rain, but because our simulations specify cloud droplet number it does not directly influence rain.…”
Section: Turbulence Thermodynamic and Cloud Fieldsmentioning
confidence: 69%
“…SAM has successfully performed LES of a variety of boundary layer cases, such as the DYCOMS-II RF01 marine stratocumulus case (Stevens et al, 2005), a trade-wind cumulus case (Siebesma et al, 2003), and a stable boundary layer case (Beare et al, 2006). Of special relevance is the fact that SAM produced comparable output to the other LES models in the recent DYCOMS-II RF02 intercomparison (Ackerman et al, 2009).…”
Section: Les Model: Sammentioning
confidence: 99%