Publication | Closed Access
Buoyancy effects on the turbulent transport processes in the lower atmosphere
71
Citations
30
References
1981
Year
EngineeringFluid MechanicsTurbulenceScalar TransportBoundary LayerEarth ScienceAbstract Buoyancy EffectsTurbulent Transport ProcessesAtmospheric ScienceMicrometeorologyTransport PhenomenaLower AtmosphereMeteorologyBuoyancy EffectsHeat TransferEnvironmental Fluid DynamicAtmospheric ConditionAerospace EngineeringTurbulent Flow Heat TransferTurbulence ModelingAtmospheric TransportAtmospheric ProcessTurbulent Transport
Abstract Buoyancy effects on the turbulent transport processes in the atmospheric boundary layer above the surface layer have been investigated. Direct measurement of heat flux and wind and temperature profiles was made by sonic anemometers and the continuous ascending and descending operation of a kitoon, to determine the eddy diffusivity of heat and the local Richardson number. the present results, along with those of a parallel study on the stratified turbulence structure in a laboratory experiment were examined by comparison with previous results in the surface layer. Under stable conditions significantly different stability dependence in the surface layer and the layer above it is recognized; in the layer above the surface layer the eddy diffusivity of heat. K H , along with the ratio of the eddy diffusivities of heat and momentum, K H / K M , decrease remarkably with the gradient Richardson number, Ri, reaching a value of K H / K HO = 0.01 at Ri = 1 and under strongly stable conditions the ratio K H / K HO varies as (Ri) −2 , while in the surface layer the ratio K H / K M remains constant or decreases slightly. This contrasting behaviour in the surface layer and the layer above is presumed due to the modification of the turbulence structure and so the turbulent transport processes by the presence of the ground, as indicated by Gibson & Launder (1978). Under unstable conditions the ground effect is not so significant that results of the present observation along with the laboratory experiment may be applied to the entire region of the atmosphere. the ratios of K H / K HO and K H / K M increase as the stratification shifts from neutral to weakly unstable conditions. the ratio K H / K M takes a peak value of about 3 at Ri ∼ −0.2 and then falls gradually with increasing instability and attains the value of unity at Ri ∼ −10.0. This fact together with the increase of K m / K MO with increasing [Ri] results in a constant value of the ratio K H / K HO equal to about 6.0.
| Year | Citations | |
|---|---|---|
Page 1
Page 1