Y. Brunet et Mr. Irvine, The control of coherent eddies in vegetation canopies: Streamwise structure spacing, canopy shear scale and atmospheric stability, BOUND-LAY M, 94(1), 2000, pp. 139-163
An analogy has been established between a plane mixing layer and the atmosp
heric flow near the top of a vegetation canopy. It is based on a common fea
ture, a strong inflection in the mean velocity profile, responsible for hyd
rodynamical instabilities that set the pattern for the coherent eddies and
determine the turbulence length scales. In an earlier study, this analogy w
as tested using a small data set from thirteen experiments, all in near-neu
tral conditions. It provided a good prediction of the streamwise spacing La
mbda(w) of the dominant canopy eddies (evaluated from time series of vertic
al velocity) that appears to depend on a shear length scale L-s = U(h)/U'(h
), where h is canopy height, U is mean velocity and U' the vertical gradien
t dU/dz. The present analysis utilizes an extensive data set of approximate
ly 700 thirty-minute runs, from six experiments on two forest sites and a m
aize crop, with a large range of stability conditions. Lambda(w) was estima
ted for each run using the wavelet transform as an objective, automated det
ection method. First, the variations of Lambda(w) and L-s with atmospheric
stability are discussed. Neutral and unstable values exhibit a large scatte
r whereas in stable conditions both variables decrease with increasing stab
ility. It is subsequently found that Lambda(w) is directly related to L-s,
in a way close to the neutral prediction Lambda(w) /h = 8.1L(s)/h. The Stro
uhal number S-tr = L-s /Lambda(w) is then shown to vary with atmospheric st
ability, weakly in unstable conditions, more significantly in stable condit
ions. Altogether these results suggest that, to some extent, the plane mixi
ng-layer analogy can be extended to non-neutral conditions. It is argued th
at the primary effect of atmospheric stability, at least in stable conditio
ns, is to modify the shear length scale L-s through changes in U(h) and U'(
h), which in turn determines the streamwise spacing of the active, coherent
motions.