Jp. Lagouarde et al., Analysis of the limits of the C-T(2)-profile method for sensible heat fluxmeasurements in unstable conditions, AGR FOR MET, 105(1-3), 2000, pp. 195-214
We present a test of the C-T(2)-profile method described by Hill et al. [J.
Atmos. Ocean. Technol. 9 (5) (1992) 526] to estimate the surface sensible
heat flux over an homogeneous surface. A comparison with traditional eddy c
orrelation measurements performed over a pasture (during the SALSA-Mexico e
xperiment) using three identical large aperture scintillometers (LASs) alon
g a 330 m propagation path and placed at heights 2.50, 3.45 and 6.45 m is f
irst given. Scintillometer derived fluxes using the classical method at one
level [Agric. For. Meteorol. 76 (1995) 149] reveal that the three scintill
ometers provide consistent measurements but underestimate by 15% the flux o
btained with the 3D sonic anemometer. This is attributed to spatial non-hom
ogeneities of the experimental site. Considerable scatter (and even the imp
ossibility of performing computations) is found when using the C-T(2) -prof
ile method which is particularly prone to errors in nearly neutral and high
ly unstable conditions. The sensitivity of these errors to the accuracy of
scintillometer measurements, the calibration errors and the measurement hei
ghts is investigated numerically. Simulations are made assuming a normal di
stribution of the relative error for C-N(2) With standard deviations a betw
een 2 and 5% and no calibration error in a first step. Only calibration err
ors (up to 4% between instruments) are simulated in a second step. They con
firm that the profile method degrades very rapidly with the accuracy of C-N
(2): for instance the RMS error for H reaches 68 W m(-2) land the cases of
impossible computation 28%) for a realistic a = 5% value, with heights 2.50
and 3.45 m. Results appear slightly less sensitive to small calibration er
rors. The choice of the measurement heights z(1) and z(2) is also analysed:
a ratio z(2)/z(1) similar to 3 or 4 with z(1) > 2m seems the best compromi
se to minimise errors in H. Nevertheless the accuracy of the profile method
is always much lower than that given by the classical method using measure
ments at one level, provided a good estimate of roughness length is availab
le. We conclude that the C-T(2)-profile method is not suitable for routine
applications. (C) 2000 Elsevier Science B.V. All rights reserved.