The WRF Single-Moment 6-Class Microphysics Scheme (WSM6)
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Cites methods or result from "The WRF Single-Moment 6-Class Micro..."
...Columns correspond to model physical processes: radiation (Rad), microphysics (MP), cumulus parameterization (CP), planetary boundary layer/vertical diffusion (PBL), and surface physics (Sfc)....
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...2 Yonsei University (YSU) PBL The Yonsei University PBL (Hong et al., 2006) is the next generation of the MRF PBL, also using the countergradient terms to represent fluxes due to non-local gradients....
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...57 8.4.2 Noah LSM . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 58 ii 8.4.3 Rapid Update Cycle (RUC) Model LSM . . . . . . . . . . . . . . . . . . 58 8.5 Planetary Boundary Layer . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 58 8.5.1 Medium Range Forecast Model (MRF) PBL . . . . . . . . . . . . . . . ....
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...59 8.5.2 Yonsei University (YSU) PBL . . . . . . . . . . . . . . . . . . . . . . . . 59 8.5.3 Mellor-Yamada-Janjic (MYJ) PBL . . . . . . . . . . . . . . . . . . . . ....
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...2 Yonsei University (YSU) PBL The Yonsei University PBL (Hong et al., 2006) is the next generation of the MRF PBL, also using the countergradient terms to represent fluxes due to non-local gradients. This adds to the MRF PBL (Hong and Pan, 1996) an explicit treatment of the entrainment layer at the PBL top. The entrainment is made proportional to the surface buoyancy flux in line with results from studies with large-eddy models (Noh et al., 2003). The PBL top is defined using a critical bulk Richardson number of zero (compared to 0.5 in the MRF PBL), so is effectively dependent on the buoyancy profile, in which the PBL top is defined at the maximum entrainment layer (compared to the layer at which the diffusivity becomes zero). A smaller magnitude of the counter-gradient mixing in the YSU PBL produces a well-mixed boundary-layer profile, whereas there is a pronounced over-stable structure in the upper part of the mixed layer in the case of the MRF PBL. Details are available in Hong et al. (2006), including the analysis of the interaction between the boundary layer and precipitation physics....
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5,363 citations
Cites methods from "The WRF Single-Moment 6-Class Micro..."
...…2.0 of the WRF was used with the Noah land surface model (Chen and Dudhia 2001), and WRF single-moment six-class microphysics (Hong et al. 2004; Hong and Lim 2006), Dudhia (1989) simple cloudinteractive shortwave, and rapid radiative transfer model longwave radiation (Mlawer et al. 1997)…...
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References
3,300 citations
"The WRF Single-Moment 6-Class Micro..." refers methods in this paper
...2005), bulk microphysics schemes include the Kessler, Purdue Lin (Lin et al. 1983), Ferrier (new ETA), Wrf-Single-MomentMicrophysics (WSMMPs) (Hong et al....
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...In the WRF model (Skamarock et al. 2005), bulk microphysics schemes include the Kessler, Purdue Lin (Lin et al. 1983), Ferrier (new ETA), Wrf-Single-MomentMicrophysics (WSMMPs) (Hong et al. 2004) and Thompson (Thompson et al. 2004, MWR)....
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2,277 citations
"The WRF Single-Moment 6-Class Micro..." refers background or methods in this paper
...3a and 3b shows that the major contribution of the components in the WSM6 scheme is due to the effect of particular ingredients of ice microphysical processes in Hong et al.(2004), rather than the differences in the sedimentation velocity for snow and graupel....
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...It is found that the reason for the major differences in the simulated precipitation between the WSM6 and PLIN are due to the revised microphysics of Hong et al. (2004), not due to the smaller terminal velocity for graupel in the WSM6 than in the PLIN....
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...1983), Ferrier (new ETA), Wrf-Single-MomentMicrophysics (WSMMPs) (Hong et al. 2004) and Thompson (Thompson et al....
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...In the WRF model (Skamarock et al. 2005), bulk microphysics schemes include the Kessler, Purdue Lin (Lin et al. 1983), Ferrier (new ETA), Wrf-Single-MomentMicrophysics (WSMMPs) (Hong et al. 2004) and Thompson (Thompson et al. 2004, MWR)....
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