SUBSEQUENT PROCESSING OF DEM RESULTS
DEMs for further processing were available with the
parameters listed in table 1. A five point margin was
cut from the models to eliminate marginal effects that
might be caused by the surrounding frame, thus result-
ing in 45,600 elevation points on 0.182 m? in the labor-
atory models (and 102,400 from 0.92 m° in the field
models). For each microrelief two characteristic values
were computed, i.e. the indices RRC (random roughness
coefficient, according to Currence & LoveLy 1970) and
the ratio TSA/MA (total surface area to map area, this
helps providing a quantitative measure for the raindrop
density).
Parameter Laboratory Field
Area of measurement 0.2 m? 0.98 m?
Spacing 2mm 3mm
Height resolution 0.2 mm 0.2 mm
Number of data 50,000 108,900
Table 1: Parameters for microrelief measurement
RRC represents the variance of the smoothed height
values. Smoothing results in elimination of external
relief effects like slope and directional relief elements.
TSA/MA was computed as ratio of the sum of all surface
areas of the DEM (there are 45,171 resp. 101,761 raster
squares) divided by the DEM ground area (i.e. the TSA
mapped on the ground). For the registration of spatial
structures in the microreliefs semivariograms were com-
puted. These data were smoothed too, in order to get
out trends and the low-frequency variance caused by
slope.
DETERMINISTIC MODELS
Effective input of rainfall energy
For calculation of the effective rainfall energy that hits
the soil surface, the total surface area (explained above)
and as well the normal component of rainfall energy,
depending on the angle of drop impact, is needed.
This parameter is computed by determining the slope
of the soil surface in each grid square of 4 mm? for lab
and 9 mm! for field plots. Assuming vertical rainfall
and a horizontal soil surface, the normal component
of the impact energy corresponds to the total kinetic
energy. With increasing slope at the striking point the
normal component decreases with respect to the impact
vector, leading to a decrease in effective energy. The
normal component thus is proportional to the cosine
of the slope at the impact point (fig. 2).
Effective input of kinetic rain energy with respect to
TSA and amount of rainfall may be expressed as:
E.eff = ma/tsa * X (cos a * E.kin) (1)
a = soil surface slope; ma = map area (m°); tsa = total surface area (m?)
e.kin
surface area
map area
Fig. 2: Relation between surface slope, impact angle
and the distribution of impact force
o = slope angle, E.kin = kinetic energy of raindrop, n = normal component
of impact force, t = tangential component of impact force
Depressional storage
Storage capacity was determined by finding each depres-
sion in the relief and estimating its circumference, sur-
face area and volume. Identification of a depression
was carried out starting from the pour point, defined as
the lowest point between two or more depressions and
within an elevated area. With the pour point as basis,
closed contour lines were determined that laid either
at the same or at a lower height than that of the pour
point. The area within such a contour line was defined
as a depression. Thus the extent of a depression is
equal to the length of the respective contour line. The
vertical distance between the lowest point and the pour
point is the maximum filling height. The surface area
was calculated using vector geometrics the same way
as for the TSA. Elevated areas within a depression (is-
lands) were subtracted. This technique of finding depres-
sions complies with the theory proposed by Uuau &
Dickinson (1979) and Huanc & Braprorp (19908). How-
ever, they began from a local depression and identified
the pour point by checking the list of neighboring
points until finding a point with a lower elevation.
This leads to more or less rectangular depression forms.
The procedure proposed here has the advantage, that
the whole depression is characterized independently
of its form.
RESULTS AND DISCUSSION
Microrelief characterization
The microrelief parameters obtained from the DEMs
are summarized in table 2.
In all cases, rainfall lowers the TSA/MA ratio by about
0.1. Thus, the total surface area of the three microrelief
treatments differs significantly and the relative change
caused by rainfall is slightly greater for the fine micro-
relief. In the field experiments the ratio of TSA/MA for
both sites showed values that were comparable to that
from the lab. Thus, the laboratory simulations seem to
be representative of natural conditions as measured in