GABLS LES intercomparison

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Case description
Participants
Model details
LEM data

Results

GABLS LES Intercomparison

Model Details

A summary of the subgrid models and the advection schemes used by each participant is given in the table below. Where relevant, values of the Smagorinsky parameter, Cs, the ratio of basic mixing length to horizontal grid length, are given. Further discussion is given in the intercomparison paper Beare et al.

Participants Subgrid Models Advection Scheme
scalars momentum
MO Smagorinsky with backscatter, Cs=0.23 high res (6.25m and below), Cs=0.15 low res. TVD / ULTIMATE Piacsek-Williams central difference scheme
CSU Deardorff (1980), Cs=0.19 3-d monotonic and positive definite (Smolarkiewic-Grabowski) central difference in flux form with 3rd order Adams-Bashforth in time
IMUK Deardorff (1980), Cs=0.1 Piacsek-Williams central difference scheme
LLNL Nonlinear Deardorff, Cs=0.2 Pseudospectral method (Fox and Orszag, 1973) in the horizontal, second order central differencing in the vertical
NERSC Dynamic mixed subgrid closure, Vreman et al. (1994) Cs=0.14 (average) 2nd order central differencing with advection term written in divergence form (non-monotonic) 2nd order central differencing with advection term written in skew-symmetric form
WVU ARAP second order quasi-equilibrium closure model Sykes and Henn (1989) piecewise parabolic method (monotone) 2nd order central differencing and leapfrog in time
NCAR Sullivan, McWilliams and Moeng (1994), Cs=0.18 3d monotone scheme Koren (1993) "kappa=1/3 scheme" Pseudospectral method (Fox and Orszag, 1973) in the horizontal, second order central differencing in the vertical
UIB Two part Meso-NH scheme (Cuxart et al., 2000) positive definite second order central difference scheme second order central difference scheme
CORA Dynamic Smagorinsky, Cs=0.18 Pseudospectral method (Fox and Orszag, 1973) in the horizontal, second order central differencing in the vertical
WU Deardorff (1980), with changes to dissipation formulation. Piacsek-Williams central difference scheme
NRL Smagorinsky, Cs=0.17. Bott (1989), with second order polynomial Second order central difference with leapfrog in time

Subgrid Comparisons

Three participants also provided data for different subgrid model configurations, as summarised in the table below. The labels correspond to the legends used on the plots viewed by following the links on the left.

Participants Resolution Subgrid Models Label
MO 6.25 m Smagorinsky with backscatter, Cs=0.15 BKSCT, Cs=0.15
Smagorinsky with backscatter, Cs=0.23 BKSCT, Cs=0.23
Smagorinsky, Cs=0.15 SMAG
1m Smagorinsky with backscatter, Cs=0.23 BKSCT
Smagorinsky, Cs=0.23 SMAG
LLNL 6.25 m and 12.5 m Nonlinear Deardorff, Cs=0.2 NLD
Nonlinear Smagorinsky, Cs=0.2 NLSMAG
Smagorinsky, Cs=0.2 SMAG
NERSC 6.25 m Dynamic mixed subgrid closure, Cs=0.14 (average) DMS
Smagorinsky, Cs=0.1 SM, Cs=0.1
Smagorinsky, Cs=0.14 SM, Cs=0.14
Smagorinsky, Cs=0.23 SM, Cs=0.23