1965
DOI: 10.1175/1520-0493(1965)093<0727:nrfanl>2.3.co;2
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NUMERICAL RESULTS FROM A NINE-LEVEL GENERAL CIRCULATION MODEL OF THE ATMOSPHERE1

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Cited by 444 publications
(169 citation statements)
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“…The resulting dynamical models draw strongly on the heritage of General Circulation Models (GCMs). First developed in the 1960s-1980s-see, for example, Smagorinsky et al 1965 for a very early example-and continually developed since, GCMs are identical in concept to NWP models-insofar as they represent a physical model of the system one is attempting to predict or understand-but as they include more physical processes and must be run over longer timescales, they typically use much coarser resolution grid boxes than NWP. As in NWP, the use of ensembles in climate model simulations is common.…”
Section: Dynamical Modelsmentioning
confidence: 99%
“…The resulting dynamical models draw strongly on the heritage of General Circulation Models (GCMs). First developed in the 1960s-1980s-see, for example, Smagorinsky et al 1965 for a very early example-and continually developed since, GCMs are identical in concept to NWP models-insofar as they represent a physical model of the system one is attempting to predict or understand-but as they include more physical processes and must be run over longer timescales, they typically use much coarser resolution grid boxes than NWP. As in NWP, the use of ensembles in climate model simulations is common.…”
Section: Dynamical Modelsmentioning
confidence: 99%
“…The frictional force F (due to vertical mixing) in term 12 is determined by F = (∂ v τ/∂z)/ρ (Smagorinsky et al, 1965) with the absence of frictional stress at the top of z (referring to the thickness of the friction active layer which will be determined by parametrization experiments for best fit by consulting the planetary boundary layer (PBL) height data from the ECMWF NUMERICAL DIAGNOSTIC MODEL FOR FORCING OF GEOPOTENTIAL 2071 model). The frictional stress at the Earth's surface is given by v τ = ρC d |V sfc |V sfc (Lettau, 1959;Pedlosky, 1987, sections 2.8 and 3.12) with the drag coefficient C d = 2 × 10 −3 proposed by Delsol et al(1971) and Holloway and Manabe (1971).…”
Section: Derivation Of a Complete Geopotential Numerical Model And Scmentioning
confidence: 99%
“…Over land areas the surface fluxes are evaluated following relations similar to those given by Businger et al (1971). The vertical distribution of fluxes of momentum, heat and moisture between *=1 and * =0 .7 follows the mixing length concepts as in Smagorinsky et al (1965). Above the *=0.7 level, the fluxes vanish in this formulation.…”
Section: The Global Spectral Modelmentioning
confidence: 99%