Ingo Haag and
Bernhard Westrich
Institut für Wasserbau, Universität Stuttgart, 70550 Stuttgart, Germany
phone: ++49 711 685 4726; E-mail: ingo.haag@iws.uni-stuttgart.de
Abstract: The
erosion threshold of cohesive sediments is an important parameter, because in
water systems fine-grained particles are the major transport agent of many
contaminants. However, the erosion behaviour of cohesive sediments, is not yet
well understood. To gain some insight into the processes governing the
stabilisation of cohesive sediments, various sediment properties were analysed
for their correlation with the erosion threshold of natural fine-grained bed
sediments, which was determined as a function of sediment depth. Sediment
consolidation, grain-size, and biological slimes (EPS) were found to be
significant factors influencing erosion resistance. The combined effect of these
mechanisms could either be considered with the consistency index as one overall
parameter or by combining the water content, the percentage of grains smaller
than 20 µm, and the content of colloidal carbohydrates in a multiple linear
regression model. Hence, the results highlight that the erosion threshold of
fine-grained cohesive sediments is not governed by one single mechanism, but
rather by a combination of physical, chemical, and biological processes which
are active at the same time. For a better understanding of the erosion behaviour
of cohesive sediments it seems therefore advisable to conduct further
experiments with both, well defined artificial and undisturbed natural
sediments.
Keywords: cohesive
sediments, erosion threshold, physicochemical properties
Most
water contaminants are primarily transported in association with fine-grained
cohesive sediments (FCS). From an environmental management perspective it is
therefore of utmost importance to be able to predict the erosion threshold of
FCS
(Haag et al., 2000)
. However, whilst the erosion
behaviour of non-cohesive coarse-grained sediments is well understood and can be
predicted since the landmark work of
Shields (1936)
, up to date no universally
valid theory for the erosion behaviour of FCS exists. The objective of the
present study is to shed some light on the mechanisms that control the erosion
threshold of natural FCS, by correlating experimentally determined critical
erosion shear stresses (τc,e) with various biological and
physicochemical sediment properties.
Erosion resistance of FCS is mainly controlled by inter-particle forces. The strength of these forces is governed by biological sediment parameters and electrochemical properties of sediment and pore water. Depending on species assemblage and organism density bioturbation by macro-biota (e.g. worms) may cause both, increasing or decreasing erosion resistance. Micro-organisms (algae, bacteria, fungi) however, generally increase sediment stability. The stabilising effect of surface films (mats) of algae or bacteria has been investigated quite frequently for both, artificial and natural sediments. In these investigations it was found that biological slimes, the so called extracellular polymeric substances (EPS) play a major role in biological sediment stabilisation, by making the surface smoother and interconnecting particles. EPS or as a surrogate colloidal carbohydrate concentration has been reported to correlate with τc,e (e.g. Paterson, 1997) .
The
strength of electrochemical bonding is primarily governed by the surface charge
density of the sediment particles and the valencies and concentration of the
ions present in the pore water solution
(Sposito,
1984)
. Even the effect of EPS, which are macromolecular
polyelectrolytes, can partially be interpreted as electrochemical. Charge
density tends to increase with increasing organic carbon content and decreasing
grain size. Also mechanical sediment consolidation and the decrease of porosity
(increase of bulk density) does enhance the strength of electrochemical
inter-particle bonding. Consequently, a variety of chemical and physical
parameters, including the sodium adsorption ratio, organic carbon content,
grain-size distribution, water content, and bulk density have been proposed as
master variables for the erosion behaviour of FCS (for an overview see
Haag et
al., 1999b)
.
Most
of the erosion investigations correlating erosion thresholds to sediment
properties have been performed with artificial or disturbed sediments. Although
Lau and
Droppo (2000)
showed that the conditions under which FCS were
deposited play a major role for their erosion behaviour, cohesive sediments with
natural layering and state of consolidation have rarely been investigated. Up to
date most investigations, in particular those dealing with biological
stabilisation, have focused on the sediment surface. Less attention has been
paid to deeper sediment layers which have been subject to long term
consolidation. However, since EPS are excreted by almost all micro-organisms
(including anaerobic bacteria) they can also be expected to control the bio-stabilisation
of deeper sediment layers. Also most studies concentrated on one single sediment
property or stabilising mechanism, not considering the combined effect of
several mechanisms which is likely to be important for natural sediments.
During
the years 1997 and 1998 several undisturbed sediment cores (13.5 cm in diameter
and 60 to 130 cm in length) were taken in the backwater region of a reservoir of
the River Neckar in south-west Germany. At least two parallel cores were sampled
in close proximity to each other. Vertical profiles of bulk densities of all
cores were measured non-intrusively by using a γ-ray-densitometer.
Comparing density profiles of parallel cores allows to check whether they have
similar vertical profiles of sediment properties. For details about sampling
procedures and density measurements see Haag
et al. (1999a)
. If, on the basis of the density profiles, parallel cores were
considered to be similar, one of them served to experimentally determine the
critical shear stress of mass erosion (τc,e) as a function of
sediment depth. Erosion experiments were carried out in the SETEG-system (Kern
et al., 1999)
. The second one of the parallel cores was cut into sections. In an
attempt to gain almost uniformly textured sub-samples, the core was cut at
depths of significant bulk density changes. The resulting 147 sub-samples of
eight cores were homogenised and the following sediment properties were
determined for all of them: grain size fraction smaller than 20 µm (d<20
[%]), water content relative to dry mass (WC [%]), total organic carbon content
(TOC [%]), bulk density (ρ [g/cm3]), and cation exchange
capacity (CEC [mmolc/kg]). For the sub-samples of two cores, liquid
and plastic limits, plasticity and consistency indexes, and the content of
colloidal carbohydrates (as an indicator for the EPS content) were determined.
Detailed record of the procedures used to gain these sediment properties is
given by Haag et al.
(1999b)
.
With a mean TOC, clay and silt content of 5, 22 and 61%, respectively, the sediments were found to be rather fine-grained and rich in organic carbon on average. However, few layers with coarse particles, low TOC and consequently increased bulk densities could be detected. They are most probably the result of sedimentation during the receding limbs of flood events (Haag et al., 2000) . Often these layers were also characterised by sudden decreases of τc,e in the corresponding parallel core, indicating the predominance of non-cohesive particles (Fig. 1). Because of this clearly non-cohesive character the corresponding data of these layers were excluded from the data pool prior to further analysis. After excluding clearly non-cohesive layers, the remaining values of τc,e were ascribed to the corresponding sediment property values of the parallel cores.

Fig. 1 Vertical profiles of bulk density and of τc,e of a sediment core from the River Neckar.
Correlation analyses
of
and the eleven sediment properties
given in Table 1 were performed. The most commonly used correlation coefficient
after Pearson (r) assumes a linear relation. Kendall’s (tau) and Spearman’s
(rho) correlation coefficients are based on rank analyses and are therefore also
applicable to non-linear relationships. The absolute values of the three
correlation measures are not directly comparable, but their significance (p,
probability of error) is (Helsel and Hirsch, 1992).
Table 1 shows the
computed correlation coefficients and their significance. Sediment depth, bulk
density, the fraction of fines, and the consistency index are positively
correlated to
with high significance. Also the
EPS content (measured as colloidal carbohydrates) seems to be positively
correlated with
. However, the probability of error is about 10%, which
might be due to the small number of values (32) that were available for this
analysis. The water content is negatively correlated with
. The negative correlation of
with TOC and CEC is very uncertain,
and cannot be explained by any of the mechanisms causing cohesion.
Table 1
Correlation coefficients of
with sediment properties and their
significance.
|
Sediment property |
depth |
ρ |
d<20 |
WC |
TOC |
CEC |
WL |
WP |
IP |
IC |
EPS* |
|
number of pairs n |
119 |
118 |
118 |
119 |
118 |
119 |
34 |
34 |
34 |
36 |
32 |
|
Kendall’s tau |
0.34 |
0.18 |
0.19 |
-0.23 |
-0.01 |
-0.06 |
0.17 |
0.12 |
0.18 |
0.50 |
0.20 |
|
p [%] |
<0.1 |
0.4 |
0.2 |
<0.1 |
90.9 |
30.6 |
15.0 |
32.8 |
14.2 |
<0.1 |
10.8 |
|
Spearman’s rho |
0.49 |
0.26 |
0.30 |
-0.33 |
-0.02 |
-0.09 |
0.25 |
0.18 |
0.26 |
0.66 |
0.28 |
|
p [%] |
<0.1 |
0.5 |
0.1 |
<0.1 |
83.4 |
32.1 |
16.0 |
30.2 |
13.8 |
<0.1 |
11.9 |
|
Pearson’s r |
0.47 |
0.22 |
0.29 |
-0.34 |
-0.02 |
-0.13 |
0.20 |
0.20 |
0.20 |
0.64 |
0.31 |
|
p [%] |
<0.1 |
1.7 |
0.1 |
<0.1 |
86.8 |
17.0 |
25.3 |
26.8 |
26.3 |
<0.1 |
8.3 |
* measured as colloidal
carbohydrates
The correlation with depth, density, and water content can be attributed
to the effect of sediment consolidation, which increases with depth and causes a
higher bulk density and lower water content. On the other hand also a grain size
effect is still apparent: a higher fraction of d < 20 µm does have a
positive effect on sediment stability. Since the bulk density is negatively
correlated with d<20, the grain size effect may obscure part of the
consolidation effect and vice versa.
Despite the significance of several correlations
the magnitude of Pearson’s r is rather low, indicating that the percentage of
variance of
being
explained by linear regression against one single parameter is well below 25%
except for the consistency index. The strong correlation between erosion
threshold and consistency index is not surprising, because IC is an
overall measure of the cohesion within the sediment, comprising the effects of
various mechanisms. The relationship however is clearly not linear. As shown in
Figure 2, rather the logarithms of
are
linearly correlated to the consistency index. The regression which could be
fitted best to the data is also given in Figure 2 along with the 95%-prediction
interval. Note that the regression is based on two sediment cores (36 samples)
only and that
is plotted
in a logarithmic scale. As indicated by the 95%-prediction interval the scatter
of the data around the regression line is rather high, with a standard error of
the estimate of 1.6 N/m2.

Fig. 2 Consistency index vs. τc,e and regression results.
The residuals of the regression given in Figure 2 were not significantly
correlated with any of the remaining ten sediment properties, indicating that IC
already comprises most of the influences of the other sediment parameters.
Consequently the remaining uncertainty cannot be ascribed to the influence of
any single sediment property.
Since the consistency index comprises the effects of various mechanisms
that sum up to the total cohesion and erosion resistance of the sediment, it is
not possible from the given relationship to gain further insight into the
mechanisms underlying sediment stabilisation. Therefore, on the basis of the
correlation analyses, as an alternative a multiple regression approach was
considered. As pointed out above sediment depth, bulk density, and water content
are measures of sediment consolidation; d<20 is a measure of the influence of
grain size on
(influencing
the chemical bonding); EPS is a measure of the biological sediment stabilisation.
Therefore, a regression model combining one of the three consolidation
parameters with d<20 and EPS should be applicable to predict the erosion
threshold. Plots of
versus
the above mentioned sediment properties indicated linear relationships. Hence a
multiple linear regression model was chosen. The model combining WC with d<20
and EPS yielded the highest r2 and the lowest standard error, and was
therefore chosen as most appropriate. In Figure 3 the performance of the
multiple linear regression model is compared with that of the single parameter
model only including IC. Even though the multiple regression model
includes three parameters, the standard error is only slightly reduced. For both
statistical models the data scatter around the line of perfect agreement
increases with
. Thus, higher erosion
thresholds are associated with higher prediction uncertainties. The remaining
uncertainty is likely owing to inaccuracies in determining
and
sediment properties, the influence of additional parameters not considered here,
and probably most importantly to errors arising from considering two parallel
cores instead of one single core.

Fig. 3 Performance of the two regression models for τc,e.
Considering the scatter and the resulting standard errors neither of the
equations in Figure 3 can be used to accurately predict the erosion threshold of
Neckar River sediments or of cohesive sediments in general, but they may well
serve as a rough estimate. The results also highlight the importance of
considering the influence of several mechanisms which contribute to erosion
resistance of FCS. Sediment consistency and stability both arise from the
combined effects of biological, chemical, and physical processes. Hence, the
integral parameter IC is the only single parameter considered in this
study which can be used to explain an appreciable part of the variance of
. Similarly high
degrees of correlation might be gained with rheometric parameters
(Otsubo and Muraoka, 1988)
. In contrast, none of the
single properties which can clearly be interpreted as biological, chemical, or
physical stabilisation parameter explains more than ca. 20% of the total
variance of
(Table
1). Only a combination of parameters taking all three mechanisms into account,
performs similarly well in explaining the variance of
as does IC
alone.
The erosion
investigations conducted in this study clearly demonstrate, that the critical
shear stress of erosion for natural cohesive sediments can only be explained as
the combined effect of various mechanisms. The erosion threshold is highly
correlated to the consistency index of the sediments. However, the consistency
itself is the product of other parameters or processes, and therefore this
correlation does not give further insight into the actual cause of erosion
resistance. Considering three parameters which can be ascribed to biological,
chemical, and physical (consolidation) stabilisation mechanisms yields similarly
good predictions as the consistency index. This allows one to interpret the
overall erosion resistance as an effect of a combination of all three processes.
Hence, this
study shows, that investigating natural sediments (with depth) does very well
serve to elucidate the mechanisms which govern the erosion resistance of
cohesive sediments. On the other hand, experiments with artificial sediments
allow to gradually change single sediment properties and to evaluate the effects
of these changes on the erosion behaviour. However, it is difficult to account
for all possible influences and to simulate long term processes such as
consolidation with artificial systems. Therefore, in order to come closer to a
unified theory of erosion resistance for fine-grained cohesive sediments, a
combination of both approaches seems to be most promising.
Acknowledgements
The authors
would like to thank the federal state of Baden-Württemberg/Germany for
financing this work; grant PW 96 182. We are also indebted to Dr. Ulrich Kern
for many invaluable discussions on the topic.
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