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Fourth Study Conference on BALTEX Scala Cinema Gudhjem

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( z )<br />

∂H<br />

H = H f − z f ⋅<br />

∂z<br />

0 (4)<br />

with flight level zf .<br />

Thus the combinati<strong>on</strong> of low-level flights with an inverse<br />

model (LLF+IM) allows the determinati<strong>on</strong> of the areaaveraged<br />

turbulent surface fluxes from square-shaped flight<br />

patterns at <strong>on</strong>ly <strong>on</strong>e low altitude (e.g. at 100 m or<br />

less)without any supporting data from other systems.<br />

4. Verificati<strong>on</strong> in LES<br />

Simulated flight measurements over homogeneous and<br />

heterogeneous terrain in a LES (Schröter et al. 2000) were<br />

c<strong>on</strong>sulted to verify the LLF+IM method. Area- and timeaveraged<br />

turbulent fluxes were derived directly from the<br />

LES model. These 'true' data were then used to quantify<br />

statistical and systematic errors of the inverse method.<br />

Within the LES model virtual measurement flights at five<br />

altitudes within the artificial CBL were performed using a<br />

3D box pattern, Both the mean fluxes and the extrapolated<br />

(using LLF+IM) surface fluxes agreed very well with the<br />

given 'true' data.<br />

Figure . 2 : Sensible heat flux measured with Do 128<br />

and Helipod during the LITFASS-98 joint field<br />

experiment.<br />

5. LITFASS-98 Measurements<br />

During the LITFASS-98 experiment (Beyrich et al. 2002)<br />

airborne measurements using the helicopter-borne<br />

turbulence probe Helipod (Bange and Roth 1999) and the<br />

research aircraft Do 128 (Corsmeier et al. 2001) were<br />

performed to determine area-averaged vertical turbulent<br />

fluxes. Both systems are equipped with sophisticated sensors<br />

to measure turbulent fluctuati<strong>on</strong>s and fluxes very precisely.<br />

The experimental site near the meteorological observatory at<br />

Lindenberg / Germany was characterized by its str<strong>on</strong>g<br />

heterogeneity. Both airborne systems flew synchr<strong>on</strong>ously<br />

3D box patterns. The area-averaged fluxes (Fig. 2) agreed<br />

very well at comm<strong>on</strong> flight levels. The linear extrapolati<strong>on</strong><br />

to the ground led to values within the statistical uncertainty<br />

of ground-based measurements.<br />

The analysis of <strong>on</strong>ly the lowest flight levels yield even better<br />

results: Using the LLF+IM method (blue lines) very similar<br />

vertical gradients of the heat flux were calculated for both<br />

airborne systems. With <strong>on</strong>ly a small discrepancy of less than<br />

10 Wm -2 to each other, the extrapolated lines calculated with<br />

LLF+IM matched the ground-based micro-meteorological<br />

stati<strong>on</strong>s and the scintillometer, as well as the upper tower<br />

measurements.<br />

-68-<br />

6. Tharandt 2001 Experiment<br />

During the Tharandt experiment in the framework of the<br />

STINHO-1campaign a low-level grid pattern was flown<br />

with the Do 128 research aircraft. The site c<strong>on</strong>sisted<br />

mainly of a large forest surrounded by grassland and<br />

agriculture. The difference in surface temperature was<br />

clearly visible in the infra-red measurements performed by<br />

the Do 128. Due to its larger surface roughness it was<br />

expected that the forest developed larger sensible heat flux<br />

than the surrounding grass, even though the surface<br />

temperature of the latter was significantly higher. To<br />

prove this thesis the LLF-IM method was applied to the<br />

airborne measurements at about 150 m above the ground<br />

(Fig. 3). Although the heat fluxes measured at the flight<br />

altitude differed <strong>on</strong>ly by a few Wm -2 from each other, at<br />

the surface the flux above the forest was about 10 Wm -2<br />

larger than above the surrounding grassland. This was due<br />

to the clearly larger vertical flux gradient that bel<strong>on</strong>ged to<br />

the forest. At about 350 m above the ground the<br />

extrapolated flux profiles of grassland and wood were<br />

united. Whether this is a kind of a turbulent flux blending<br />

height will be subject to further research.<br />

Figure . 3 : Sensible heat flux measured with the Do<br />

128 aircraft over Tharandt forest and grassland in<br />

2001.<br />

References<br />

Bange, J. and R. Roth, 1999: Helicopter-Borne Flux<br />

Measurements in the Nocturnal Boundary Layer Over<br />

Land - a Case <str<strong>on</strong>g>Study</str<strong>on</strong>g>. Boundary- Layer Meteorol., 92,<br />

295-325, 1999..<br />

Beyrich, F., H.-J. Herzog, and J. Neisser: The LITFASS<br />

Project of DWD and the LITFASS- 98 Experiment:<br />

The Project Strategy and the Experimental Setup.<br />

Theor. Appl. Climatol., 73, 3-18, 2002.<br />

Corsmeier, U., R. Hankers, and A. Wieser: Airborne<br />

Turbulence Measurements in the Lower Troposphere<br />

Onboard the Research Aircraft Dornier 128-6, D-<br />

IBUF. Meteor. Z., N. F., 4, 315-329, 2001.<br />

Grunwald, J., N. Kalthoff, F. Fiedler, and U. Corsmeier:<br />

Applicati<strong>on</strong> of Different Flight Strategies to<br />

Determine Areally Averaged Turbulent Fluxes. Beitr.<br />

Phys. Atmosph., 71, 283-302, 1998.<br />

Schröter, M., J. Bange, and S. Raasch: Simulated Airborne<br />

Flux Measurements in a LES Generated C<strong>on</strong>vective<br />

Boundary Layer. Boundary-Layer Meteorol., 95, 437-<br />

456, 2000.<br />

Tarantola, A.: Inverse Problem Theory. Elsevier,<br />

Amsterdam, 613 pp, 1987.<br />

Wolff, M. and J. Bange: Inverse Method as an Analysing<br />

Tool for Airborne Measurements. Meteor. Z., N. F., 9,<br />

361-376, 2000.

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