Structure of unsteady stably stratified turbulence with mean shear

被引:57
作者
Hanazaki, H
Hunt, JCR
机构
[1] Tohoku Univ, Inst Fluid Sci, Aoba Ku, Sendai, Miyagi 9808577, Japan
[2] UCL, Dept Space, London WC1E 6BT, England
[3] UCL, Dept Climate Phys & Geol Sci, London WC1E 6BT, England
[4] Delft Univ Technol, JM Burgers Ctr, Delft, Netherlands
关键词
D O I
10.1017/S0022112004007888
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
The statistics of unsteady turbulence with uniform stratification N (Brunt-Vaisala frequency) and shear alpha(=dU1/dx3) are analysed over the entire time range (0 < alphat < infinity) using rapid distortion theory (RDT) over a wide range of Richardson number Ri(= N-2/alpha(2)), and initial conditions. The solutions are found to be described by the Legendre functions of complex degree with pure-imaginary argument and are compared with previously published results of both direct numerical simulations (DNS) and experiments. In the initial stage of development many of the characteristics are similar to those in stratified flow with no shear, since the turbulence is determined by Nt at the leading order, and the effects of vertical shear a generally appear at higher order. It is shown how in developing turbulence for Ri > 0 and Ri > 0.25 respectively, oscillatory momentum and positive and negative density fluxes develop. Above a critical value of Ri(crit)(similar to0.3), their average values are persistently countergradient. This structural change in the turbulence is the primary mechanism whereby stable stratification reduces the fluxes and the production of variances. It is quite universal and differs from the energy and stability mechanisms of Richardson (1926) and Taylor (1931). The long-time asymptotics of the energy ratio ER(=PE/VKE) of the potential energy to the vertical kinetic energy generally decreases with Ri(greater than or equal to0.25), reaching the smallest value of 3/2 when there is no shear (Ri --> infinity). For strong mean shear (Ri < 0.25), RDT significantly overestimates ER since (as in unstratified shear flow) it underestimates the vertical kinetic energy VKE. The RDT results show that the asymptotic values of the energy ratio ER and the normalized vertical density flux are independent of the initial value of ER, in agreement with DNS. This independence of the initial condition occurs because the ratios of the contributions from the initial values PE0 and KE0 are the same for PE and VKE and can be explained by the linear processes. Stable stratification generates buoyancy oscillations in the direction of the energy propagation of the internal gravity wave and Suppresses the generation of turbulence by mean shear. Because the shear distorts the wavenumber fluctuations, the low-wavenumber spectrum of the vertical kinetic energy has the general form E-33(k) proportional to (alphatk)(-1), where (L(X)alphat)(-1) much less than k much less than L-X(-1) (L-X: integral scale). The viscous decay is controlled by the shear, so that the components of larger streamwise wavenumber k, decay faster. Then, combined with the spectrum distortion by the shear, the energy and the flux are increasingly dominated by the small-k(1) components as time elapses. They oscillate at the buoyancy period pi/N because even in a shear flow the components as k(1) --> 0 are weakly affected by the shear. The effects of stratification N and shear a at small scales are to reduce both VKE and PE. Even for the same Ri, larger N and alpha reduce the high-wavenumber components of VKE and PE. This supports the applicability of the linear assumption for large N and alpha. At large scales, the stratification and shear effects oppose each other, i.e. both VKE and PE decrease due to the stratification but they increase due to the shear. We conclude that certain of these unsteady results can be applied directly to estimate the properties of sheared turbulence in a statistically steady state, but others can only be applied qualitatively.
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页码:1 / 42
页数:42
相关论文
共 72 条
[1]  
[Anonymous], TURBULENT SHEAR FLOW
[2]   THE FORCE EXERTED ON A BODY IN INVISCID UNSTEADY NON-UNIFORM ROTATIONAL FLOW [J].
AUTON, TR ;
HUNT, JCR ;
PRUDHOMME, M .
JOURNAL OF FLUID MECHANICS, 1988, 197 :241-257
[3]  
Batchelor G., 1953, The theory of homogeneous turbulence
[4]   THE EFFECT OF RAPID DISTORTION OF A FLUID IN TURBULENT MOTION [J].
BATCHELOR, GK ;
PROUDMAN, I .
QUARTERLY JOURNAL OF MECHANICS AND APPLIED MATHEMATICS, 1954, 7 (01) :83-103
[5]   THE EFFECTS OF STABLE STRATIFICATION ON TURBULENT-DIFFUSION AND THE DECAY OF GRID TURBULENCE [J].
BRITTER, RE ;
HUNT, JCR ;
MARSH, GL ;
SNYDER, WH .
JOURNAL OF FLUID MECHANICS, 1983, 127 (FEB) :27-44
[6]  
Cambon C, 2003, STATISTICAL THEORIES AND COMPUTATIONAL APPROACHES TO TURBULENCE, P25
[7]   Recent developments in second-moment closure for buoyancy-affected flows [J].
Craft, TJ ;
Ince, NZ ;
Launder, BE .
DYNAMICS OF ATMOSPHERES AND OCEANS, 1996, 23 (1-4) :99-114
[8]  
CSANADY GT, 1964, J ATMOS SCI, V21, P439, DOI 10.1175/1520-0469(1964)021<0439:TDIASF>2.0.CO
[9]  
2
[10]  
DERBYSHIRE SH, 1994, J ATMOS SCI, V51, P3486, DOI 10.1175/1520-0469(1994)051<3486:AATSBL>2.0.CO