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download pdf - Institut für Umweltphysik - Ruprecht-Karls-Universität ...

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3.1. SOIL PHYSICS 99<br />

3.1.3 Physical processes in the capillary fringe<br />

Moritz Mie<br />

Abstract In order to understand the impact of different factors on size and shape of the capillary<br />

fringe, we use high-resolution measurements of the water saturation obtained from imaging techniques.<br />

The most important part of this work is to explain the nonlinear behavior of the capillary fringe by<br />

changing the water table. Moreover we try to understand the connection between this non-linear<br />

behavior and the hysteresis of the soil-water characteristic.<br />

motor control Hele−Shaw cell<br />

digital camera<br />

Figure 3.3: Sketch of the experimental setup: A transparent sand-filled Hele-Shaw cell is placed<br />

between a diffusive light source and a digital camera. The water table in the cell is controlled by a<br />

motor connected to a computer<br />

Background In the last century most of the<br />

research efforts by soil scientists and hydrologists<br />

have focused on the vadose zone and on the<br />

groundwater region, respectively. Mostly the impact<br />

of the transition zone, the capillary fringe,<br />

has been ignored. The thickness of this zone depends<br />

on the properties of the respective soil, particularly<br />

on the pore space and on the surface<br />

roughness of the sand grains. With this experiment<br />

we investigate the influence of a periodically<br />

changing water table on size and shape of the capillary<br />

fringe.<br />

Methods and results To measure the water<br />

content that is needed to determine the height of<br />

the capillary fringe we use a Hele-Shaw cell that<br />

consists of two parallel 50 × 30 cm 2 glass plates<br />

with a 3 mm gap filled with homogeneous sand.<br />

At the bottom, the cell is connected to a movable<br />

water reservoir. We use the Light Transmission<br />

Method (LTM) that is based on the fact that<br />

the intensity of transmitted light can be used as a<br />

proxy of water content. The calibration of LTM<br />

with respect to water saturation is done by simultaneous<br />

measurements of X-ray and light transmission.<br />

A digital camera takes interval photos<br />

during the whole experiment. By subtracting the<br />

dry sand image from all images we get a normalized<br />

image time series which represents the water<br />

content in our sand column. In the first experimental<br />

series we measure the dynamics of water<br />

saturation for different water table. We chose different<br />

amplitudes and frequencies for the water table<br />

change. By analysing the first experiments we<br />

found that in the experiments with high frequencies<br />

(period of one hour) the system never reaches<br />

equilibrium. In experiments with lower frequencies<br />

(period of 24 hours) the state of equilibrium<br />

during the first imbibition process is reached after<br />

some hours. Subsequent cycles show a much<br />

faster equilibration.<br />

Outlook Interpreting the results of this experiment<br />

is one part of the future work. This encompasses<br />

the study of limiting cycles as well as the<br />

nonlinear damping characteristics of the capillary<br />

fringe. Moreover we are going to do some similar<br />

experiments with changing parameters. For instance<br />

we will use different velocities of the water<br />

table change by slow or fast drainage and imbibition.<br />

Another parameter to change is the surface<br />

roughness of the sand grains. Different kinds of<br />

sand might have different impact on the shape of<br />

the capillary fringe.

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