U. Hogstrom et H. Bergstrom, ORGANIZED TURBULENCE STRUCTURES IN THE NEAR-NEUTRAL ATMOSPHERIC SURFACE-LAYER, Journal of the atmospheric sciences, 53(17), 1996, pp. 2452-2464
The Tiederman method, which was originally designed for unambiguous de
tection of ''bursts'' in the buffer layer of smooth surface laboratory
boundary-layer flow, is shown to work equally well in the neutral atm
ospheric surface layer. It enables estimation of characteristic timesc
ales of significant structures responsible for the momentum transport:
mean duration of and mean interval between bursts (upward transport o
f momentum deficit) and mean duration and interval between sweeps (dow
nward transport of momentum excess). Data representing near neutral co
nditions from three field experiments over hat and homogeneous areas b
ut with very different roughness characteristics are used in the analy
sis. For two low vegetation sites (i.e., the measuring heights are ver
y much larger than the roughness sublayer height), it is found that al
l above-mentioned timescales are constant for any height and identical
at the two sites. Scaling the results with the friction velocity indi
cates the corresponding scaling height to be proportional to the scali
ng height of the neutral boundary layer. The third site is a forest si
te, and the measurements were taken in the roughness sublayer. Here ca
nopy inflection scaling is found to apply. The structures identified w
ith the Tiederman method are shown to be responsible for more than 90%
of the momentum flux, most of which is accomplished by a mean Bow com
ponent within the structures. Results are discussed in light of direct
numerical simulation results for fully turbulent but low Reynolds num
ber how over a dynamically smooth surface and large-eddy simulation re
sults for a high Reynolds number case, and these show encouraging cons
istencies for the logarithmic layer. Turbulence production at the surf
ace is, however, fundamentally different in the rough atmospheric case
compared to the smooth case and is presumably governed by canopy wind
profile inflection instability.