Gg. Katul et al., SKIN TEMPERATURE PERTURBATIONS INDUCED BY SURFACE-LAYER TURBULENCE ABOVE A GRASS SURFACE, Water resources research, 34(5), 1998, pp. 1265-1274
High-frequency (5 Hz) atmospheric surface layer (ASL) turbulent veloci
ty (u') and infrared skin temperature perturbations (T-s') were measur
ed above a grass-covered forest clearing and analyzed for cloud free c
onditions. These measurements were used to investigate mechanisms resp
onsible for the production of large short-lived T-s' perturbations cau
sed by rapid excursions in u'. To quantify the effects of u' on rapid
surface cooling, wavelet spectra of u' and T-s' and cospectra of u' T-
s' were computed. The u' wavelet power spectra were then analyzed usin
g Townsend's [1961, 1976] hypothesis. Townsend's hypothesis states tha
t ASL eddy motion can be decomposed into an active component, which is
a function of the ground shear stress (u) and height (z) above the z
ero plane displacement, and an inactive component, which is produced i
n the atmospheric boundary layer (ABL) outer region. A -1 power law in
the u' power spectrum was used as a signature for inactive eddy motio
n. Therefore the -1 power law was used to identify wavenumber ranges (
about 1.5 decades) associated with inactive eddy motion. The measured
T-s', wavelet spectra and u' T-s' cospectra identified with this waven
umber range demonstrate that much of the T-s' energy and [u'T-s'] are
due to inactive eddy motion, where the angle brackets indicate time av
eraging. Hence, in contrast to the laboratory experiments of Owen and
Thomson [1963], it is argued that skin temperature perturbations at th
e canopy-atmosphere interface of a grass-covered surface (small therma
l inertia) are strongly dependent on the inactive eddy motion produced
in the outer layer of the ABL.