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Fig. 9.2
Laboratory set-up to study the problem of sorption experimentally. The graduated cylinder maintains
the water at the point of entry ( x = 0), at constant pressure in the manner of a Mariotte bottle. At the
start of the experiment ( t = 0), the water supply through the flexible tubing is opened; after a certain
time t , at the end of the experiment, the 1 cm sections of the horizontal soil column tubing can be
rapidly taken apart, to determine their soil water content as θ = θ ( x ). (From Nielsen
et al ., 1962.)
Fig. 9.3
Soil water content distribution θ = θ ( x ) in Columbia silt loam, obtained after three different times of
horizontal infiltration by means of the apparatus shown in Figure 9.2, with the pressure at the inlet
maintained at 2 hPa (or roughly 2.04 cm of water column). The curve for 740 min is the best fit line
through the data points (circles); the curves for 88 min and 344 min are calculated from the curve for
740 min on the basis of Boltzmann similarity, that is by multiplying it by (88 / 740) 1 / 2 and
(344 / 740) 1 / 2 , respectively. (After Nielsen et al ., 1962.)
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