scholarly journals Effects of adjacent wall on turbulent jets. 2nd Report. Turbulence energy balance.

1990 ◽  
Vol 56 (524) ◽  
pp. 926-934
Author(s):  
Kouzou SUDOU ◽  
Toshihiro TAKAMI ◽  
Naonori KURODA
1988 ◽  
Vol 110 (2) ◽  
pp. 216-221 ◽  
Author(s):  
S. Fu ◽  
P. G. Huang ◽  
B. E. Launder ◽  
M. A. Leschziner

Computations are reported for three axisymmetric turbulent jets, two of which are swirling and one containing swirl-induced recirculation, obtained with two models of turbulence: a differential second-moment (DSM) closure and an algebraic derivative thereof (ASM). The models are identical in respect of all turbulent processes except that, in the ASM scheme, stress transport is represented algebraically in terms of the transport of turbulence energy. The comparison of the results thus provides a direct test of how well the model of stress transport adopted in ASM schemes simulates that of the full second-moment closure. The comparison indicates that the ASM hypothesis seriously misrepresents the diffusive transport of the shear stress in nonswirling axisymmetric flows, while in the presence of swirl the defects extend to all stress components and are aggravated by a failure to account for influential (additive) swirl-related stress-transport terms in the algebraic modelling process. The principal conclusion thus drawn is that in free shear flows where transport effects are significant, it is advisable to adopt a full second-moment closure if turbulence modelling needs to proceed beyond the eddy-viscosity level.


2016 ◽  
Author(s):  
Maxime Litt ◽  
Jean-Emmanuel Sicart ◽  
Delphine Six ◽  
Patrick Wagnon ◽  
Warren D. Helgason

Abstract. Over mountain glaciers, large errors may affect turbulent surface heat fluxes estimated with the bulk-aerodynamic (BA) method. That might lead to uncertainties in estimating melt from surface energy balance (SEB). During the summers of 2006 and 2009, in the atmospheric surface layer of Saint-Sorlin Glacier (French Alps, 45° N, 6.1° E, ~3 km2), mean air-temperature and wind-speed vertical profiles and high frequency Eddy-Covariance (EC) data were collected to characterize the turbulence and the turbulent fluxes. We studied the influence of the BA method errors on the melt estimations, calculating the SEB alternatively with turbulent fluxes obtained from the BA and the EC methods. We classified our results in terms of large-scale forcing. In weak synoptic forcing, local thermal effects dominated the wind circulation. On the glacier, weak katabatic flows with a wind-speed maximum at low height (2–3 m) were detected 71 % of the time and were generally associated with weak turbulent kinetic energy (TKE) and turbulent fluxes. When the large-scale forcing was strong, the wind in the valley aligned with the glacier flow, intense downslope flows were observed, no wind-speed maximum was visible below 5 m, TKE and turbulent fluxes were often intense. For both regimes, the surface layer turbulence production was probably not at equilibrium with dissipation because of the interaction of large-scale orographic disturbances with the flow when the forcing was strong, or low-frequency oscillations of the katabatic flow when the forcing was weak. When TKE was low, all turbulent fluxes calculation methods provided similar fluxes. When TKE was large, the EC method provided larger fluxes than the BA method. This underestimation was compensated by increasing the BA flux estimates using melt-calibrated effective roughness lengths. Though strong forcing was more frequently associated with large TKE events than weak forcing conditions, differences between the different SEB estimates remained in both cases within the error range of observed melt.


1975 ◽  
Vol 15 (1) ◽  
pp. 137-139 ◽  
Author(s):  
V. I. Bukreev ◽  
V. A. Kostomakha ◽  
Yu. M. Lytkin

2005 ◽  
Vol 2005.42 (0) ◽  
pp. 387-388
Author(s):  
Michiharu ISHII ◽  
Atsushi SASAKI ◽  
Masaharu MATSUBARA ◽  
Yoshiaki TSUCHIYA ◽  
Toshihiko IKEDA

1976 ◽  
Vol 16 (4) ◽  
pp. 535-543
Author(s):  
V. B. Librovich ◽  
V. I. Lisitsyn

1994 ◽  
Vol 144 ◽  
pp. 315-321 ◽  
Author(s):  
M. G. Rovira ◽  
J. M. Fontenla ◽  
J.-C. Vial ◽  
P. Gouttebroze

AbstractWe have improved previous model calculations of the prominence-corona transition region including the effect of the ambipolar diffusion in the statistical equilibrium and energy balance equations. We show its influence on the different parameters that characterize the resulting prominence theoretical structure. We take into account the effect of the partial frequency redistribution (PRD) in the line profiles and total intensities calculations.


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