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Stefan Wirtz Vom Fachbereich VI (Geographie/Geowissenschaften ...

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Experimentelle Rinnenerosionsforschung vs. Modellkonzepte – Quantifizierung der hydraulischen und erosiven Wirksamkeit von Rinnen<br />

Table 2 Constant parameters<br />

Parameter Factor Value<br />

Discharge intensity [ L min -1 ] 9<br />

Setup Discharge quantity [L] 72<br />

Discharge time [min] 8<br />

Soil texture<br />

Loamy sand<br />

Organic matter [%] ~ 2.2<br />

Land use<br />

Arable land<br />

Transport Coefficient K t [s 2 m 0.5 kg -0.5 ] 0.0107<br />

Soil Vegetation cover [%] ~ 1<br />

Rock fragment cover [%] ~ 2<br />

Starting soil moisture [%] ~ 7.5<br />

Grain density [g cm -3 ] 2.65<br />

Dry bulk density [g cm -3 ] 1.68<br />

Average precipitation [mm a -1 ] 380<br />

Climate<br />

Average annual temperature [°C] 19.2<br />

Evapotranspiration rate [mm a -1 ] 1084<br />

Characterisation<br />

Semi arid<br />

2.2 Rill experiment<br />

The rill experiment consisted of two runs: in the first run the rill was tested under dry<br />

conditions; in a second run, 15 min later, the same rill was tested under wet conditions,<br />

therefore the influence of the initial soil moisture could be considered.<br />

For each run, a motor driven pump was used to maintain a constant discharge of 9 L min -1 for<br />

8 minutes, resulting in a total water flow of 72 L (<strong>Wirtz</strong> et al., 2010, <strong>Wirtz</strong> et al., 2012). In the<br />

used range of water quantity and pressure the fluctuations were very low so we can assume<br />

that the inflow was stable.<br />

The flow velocity within the rill was characterized by the travel time of the waterfront and of<br />

two colour tracers (food colourings (E 124 red and E 13 blue started at 3 and 6 minutes after<br />

the start of the experiment) measured for every meter using a chronograph. By means of this<br />

procedure, three velocity curves with the maximum flow velocities were recorded and<br />

changes in flow dynamics could be detected. Following Govers (1992b) we assumed that the<br />

mean flow velocity is reached, where the waterfront reaches 80 – 90 % of its maximum width.<br />

In our experiments, the difference between the front and this point could not easily be<br />

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