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000012520 084__ $$2WoS$$aEnvironmental Sciences
000012520 084__ $$2WoS$$aSoil Science
000012520 084__ $$2WoS$$aWater Resources
000012520 1001_ $$0P:(DE-Juel1)129548$$aVanderborght, J.$$b0$$uFZJ
000012520 245__ $$aWithin-Field Variability of Bare Soil Evaporation Derived from Eddy Covariance Measurements
000012520 260__ $$aMadison, Wis.$$bSSSA$$c2010
000012520 300__ $$a943-954
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000012520 440_0 $$010301$$aVadose Zone Journal$$v9$$x1539-1663$$y4
000012520 500__ $$aThis research was supported by the German Research Foundation DFG (Transregional Collaborative Research Centre 32-Patterns in Soil-Vegetation-Atmosphere Systems: Monitoring, modelling and data assimilation). We thank Marius Schmidt and Karl Schneider from the University of Cologne for providing meteorologic data from the Selhausen test site and Axel Knaps for providing us with meteorologic data from the Forschungszentrum Julich. A. Graf would like to thank the DFG for funding through the project GR 2687/3-1 "Links between local scale and catchment scale measurements and modelling of gas exchange processes over land surfaces."
000012520 520__ $$aBare soil evaporation was measured with the eddy-covariance method at the Selhausen field site. The site has a distinct gradient in soil texture, with a considerably higher stone content at the upper part of the field. We investigated the effect of different soil properties in the upper and lower parts of the field on evaporation using eddy covariance (EC) measurements that were combined with a footprint model. Because only one EC station was available, simultaneous evaporation measurements from the two field parts were not available. Therefore, measurements were put into the context of meteorologic and soil hydrologic conditions. Meteorologic conditions were represented by the potential evaporation, i.e., the maximum evaporation that is determined by the energy available for evaporation. The influence of precipitation and soil hydrologic conditions on the actual evaporation rate was represented by a simple soil evaporation model. The amount of water that could be evaporated at the potential rate from the lower part of the field was found to be large and considerably larger than from the upper part of the field. The difference in evaporation led to threefold larger predicted percolation or runoff in the upper than the lower part of the field. Simulations using the Richards equation were able to reproduce the differences in evaporation between the lower and upper parts of the field and relate them to the different groundwater table depths in the two parts of the field.
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000012520 7001_ $$0P:(DE-Juel1)129461$$aGraf, A.$$b1$$uFZJ
000012520 7001_ $$0P:(DE-Juel1)VDB70177$$aSteenpass, C.$$b2$$uFZJ
000012520 7001_ $$0P:(DE-Juel1)VDB63507$$aScharnagl, B.$$b3$$uFZJ
000012520 7001_ $$0P:(DE-Juel1)VDB72509$$aProlingheuer, N.$$b4$$uFZJ
000012520 7001_ $$0P:(DE-Juel1)129469$$aHerbst, M.$$b5$$uFZJ
000012520 7001_ $$0P:(DE-Juel1)138662$$aHendricks-Franssen, H.-J.$$b6$$uFZJ
000012520 7001_ $$0P:(DE-Juel1)129549$$aVereecken, H.$$b7$$uFZJ
000012520 773__ $$0PERI:(DE-600)2088189-7$$a10.2136/vzj2009.0159$$gVol. 9, p. 943-954$$p943-954$$q9<943-954$$tVadose zone journal$$v9$$x1539-1663$$y2010
000012520 8567_ $$uhttp://dx.doi.org/10.2136/vzj2009.0159
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