cfm2007-1575.pdf
TRANSCRIPT
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A study of a slope failure case in unsaturated marly clay
M. Jamei*, H. Guiras, K. Ben Hamouda &M. Hatira
Civil Engineering Laboratory, National Engineering Scholl of Tunis (ENIT), B.P. 37, Le Belvdre Tunis,
Tunisia
ABSTRACT
The analysis of the some experimental field data on the unsaturated unstable slope constituted
with a marly clay soil showed that the swelling and collapse phenomena were the origin of the landslide
problem. In the studied case, field investigation data and laboratory tests based on the water retention
curve determination were analysed. The recorded pore-water pressure field helped us to identify the
hydrological conditions. In fact, the wetting and drying cycles involve the total suction and the degree of
saturation changes. To predict the shallow slope failure, a constitutive model taking into account the
suction effect as well as their dependence on degree of saturation is proposed. It is especially remarkable
that the collapse phenomenon is well reproduced when the model incorporates suction changes and
saturated preconsolidation stress. The analysis of the slope failure, basing on the field data and the
theoretical study, shows the hydraulic and mechanical effects.
RSUM
Lanalyse des rsultats issus dune exprimentation in situ dun talus instable constitu de
largile marneuse, montre que la nature gonflante de cette argile et son fort potentiel deffondrement sont
lorigine de cette rupture. Dans cette tude et en se basant sur des rsultats des essais in situ et de
laboratoire pour la dtermination dune part des caractristiques hydriques du site, et dautre part des
caractristiques physiques et mcaniques et de la courbe de rtention deau de largile constituant le talus,
on analyse leffet des cycles hydriques sur la variation de la succion, conduisant ainsi une rupturesuperficielle du talus. Un modle de prdiction de la variation de la rsistance au cisaillement incluant la
prdiction de leffondrement est propos. Par ailleurs, on montre que leffet de leffondrement sur la
diminution de la rsistance au cisaillement est bien pris en compte en introduisant la succion et la
contrainte de prconsolidation saturation.
Key-words:
slope failure; unsaturated marly clay; constitutive model
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1 Introduction
The landslide cases were more frequent in the Northern West of Tunisia. Every year the
Tunisian government invests large amounts of money to repair the damages caused by the
slopes failure along the national roads. This area belongs to a semi-arid region, with a mountain
relief, different climatic seasons and an important variation of rainfall intensity (from 6.5mm in
July to 80mm in January). The rainfall events lead to unstable slopes, often during the wet
season and particularly after the long dry season. Since one of the major geotechnical problems
is to design safe and economical dimensions for the slopes and to make well infrastructure roads
functional, interested has been mainly focused in hydraulic and mechanical origin of the
landslide kind frequently observed in the mentioned above region. The interaction of the
hydraulic and the mechanical aspects has been studied (water retention curve, permeability and
soil shear variation due to the suction changes). Conventional slope stability analyses using the
principles of saturated soil mechanics indicated the safe conditions for the slope (factor of safety
ranges respectively between 6.2 and 7.5 with the undrained shear parameters and between 1.17
and 1.43 with the effective shear parameters). These factors of safety values were corresponded
to an average 80 kPa of undrained cohesion and 4 for the undrained friction angle. The
effective failure parameters are c= 4kPa and ' = 10). Nevertheless, as the conventionally slope
stability is based on saturated shear parameters assuming the soil to be either dry or completely
saturated, this approach can lead to the worst case scenario of the slope behaviour (Kerrie
Fabious et al. 2004) and consequently leads to the conservatively analysis. Hence, in this case,
the conventional slope stability study appears not efficient to explain the observed slopes failure
or leads to an erroneous result (it is the case when the undrained shear parameters are taken into
account in the safety factor calculation). Besides, the contribution of matric suction towards an
increase in shear strength may be taken into account in the slope stability, particularly here for
the study case, where the ground water table is deep and the slip planes are shallow (e.g. the
shallow landslide: Figure 1). Mechanical effects associated with suction changes tend to be
more complex to study if the soil is like a marly clay, which presents a collapse or a swelling
phenomena (with a decrease of suction) and shrinkage (with an increase of suction). This is one
of the reasons for the present study in which we give an attention to found a theoretical simply
model which leads to more understanding of the landslides problems observed in the marly
clayey soils. This first part of the paper presents the site and field instrumentation data. These
results provide an overall picture of the landslide phenomenon and give an idea to the hydraulic
parameters variation effect on the slope failure mechanism. Summarized physical and
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mechanical parameters are also given. In the second part of the paper, interested is focused
firstly on the collapse response of the marly clay soil and secondly on an alternative model
combining the principle of the Barcelona model (BBM, 1990) and those proposed by other
authors (Vanappilli et al. 1996), Kerrie Fabius et al. (2004).
2 Description of the site and instrumentation
2.1 Soil profile and properties
The site is constituted by a success of slopes crossed by road (the average inclination of
the different slopes in this site is 22, Figure 1). Important observed shallow failures are with
the depth ranging 2m to 3m. The slope studied in the paper has an angle 15 and a transversal
length 150m (Figure 1).
FIG. 1 Slope profile and collapse of the marly clay after the wetting season
(at the saturation state)
The site is in semi-arid area with average annual rainfall intensity in this region is 600mm,
which the most party has been during september to march (Figure 2). For the economical
raisons, just two boreholes were drilled in the mid-slope of monitored area and used for
sampling and installing a piezometer. To describe the eventual movement of ground surface
some landmarks were installed across the profile and a topographic measurement was taken
each month. The physical and mechanical parameters from the boreholes around mid-slope are
shown in Table 1. Parameters in Table 1 indicate the fine soil character (97 % < 80m) and
relatively its high plasticity (the average value of plasticity indice Ip is 30%). The densities (wet,
dry and particle specific) are also given. The increase of the dry density is naturally related to
the earth weight effect. The shear tests which were performed in undrained conditions show the
low values of friction angles and a not important cohesion value. These tests correspond to a
degree of saturation Sraround 92%.
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0,0
50,0
100,0
150,0
200,0
250,0
SEPT
OCTO
NOVE
DECE
JAN
FEVR
MAR
AVPIL
MAY
JUIN
JUIL
AUG
rainfall
2000/01
2001/02
2002/03
2003/04
2004/05
FIG. 2Rainfall intensity during 2000-2005
Granulometry Atterbergs Limit Densitiesdepth
%>0,42mm %
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3 A model to describe the slope failure and the collapse strains
The model is based on the soil-water characteristic curve as tool to predict the shear
stress function for an unsaturated soil (Vanappilli et al. 1996). In this paper, using the fitting
parameters given by Jamei et al. (2007), the soil-water characteristic curve was obtained (Fig. 5-
b) across the particle size distribution (Fig. 5-a).
0
10
20
30
40
50
60
70
80
90
100
0,0001 0,001 0,01 0,1 1 10part icle size( mm )
Percentagea
ccruedbyweight(%
0
5
10
15
20
25
30
35
1 10 100 1000 10000 100000
Succion (kPa)
watercontent(%)
FIG. 5-a: particle size distribution curve FIG. 5-b: soil-water characteristic curve
The fundamental equation relating the suction and the diameter of equivalent particles (Jamei et
al. 2007) is:2 cos
s
i
w i
Ts
g r
= (1)
Where: s i = soil water pressure related to the meniscus at the equivalent particle (i); T s= surface
tension of water; =contact angle; w = density of water; g = acceleration due to gravity andri =
pore radius of particle (i). The model is based on the shear strength function (2-a) for
unsaturated soil proposed by Fredlund et al. (1996) which, in this paper, has been extended
including the apparent preconsolidation stress.
( ) ( )rwn ac u tg s = + + tg , wsat
w
w = (2-a) and (2-b)
Where: ua = air pressure related; n the total net normal stress; s the matric suction; w the not
dimensional water content defined by (2-b). r is a soil parameter which related to the plasticity
of soils and is the water content for saturated soil. In order to introduce the relation
between the collapse phenomenon and the preconsolidation stress, the equation (2-a) is
modified by (3):
satw
( )0
*0
0*
0
( ) ;( )
p
p
wn a
pc u tg s r
p = + + = (3)
The two stresses and were given by Alonso et al. (2003)0p*
0( )p
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0
max
n
cr c
sp p p
s
= + (4)
Equation (4) provides the current yield confining stress, , for a suction s and a current
(actual) saturation confining stress . As shown by Alonso et al. (2003) provides theintensity of the expected collapse. For a given initial (high) suction the collapse strains
can be predicted. In (4) the n is a soil parameter depending on the LC yield curve (BBM
model). The current confining stress can be related with the preconsolidation stress
(5). The Figures (6-a) and (6-b) show respectively the response of the model to predict the shear
stress evolution according to the suction changes (Fig. 6-a) and the dependence of the
constitutive model with the parameter r (Fig. 6-b).
0p
crp cp
maxs
crp*
0( )p
*
0( )or op p= + p (5)
0
20
40
60
80
100
120
140
160
180
200
0 100 200 300 400 500
Suction (kPa)
S
h
e
a
r
stren
th
k
P
a
Predictedcurve
effectif vertical stress = 20 kPa
0
20
40
60
80
100
120
140
160
180
200
0 100 200 300 400 500
Suction (kPa)
S
h
ea
r
str
en
th
k
P
a
r = 1
r = 2
r = 3
effectif vertical stress = 20 kPa
FIG. 6-a: shear strength-suction relationship FIG. 6-b: shear strength-suction evolution with r
4 Conclusions
The study has provided a case of unsaturated shallow failure slope due to the diminution of
suction and principally due the humidification and drainage cycles. The experimental site data
gives an idea on this phenomenon. The model takes into account the effect of the suction
changes on the collapse phenomenon, including the water retention curve data. It allows also to
a quantitative variation of the soil shear stress during the wetting process. Then, it may be leads
to the failure slope prediction across the safety factor calculation.
References
Alonso, E.E. & Romero E. 2003, Collapse behaviour of sand. In Proceeding Asian Conferenceon Unsaturated Soils, Japan, 325-333.
Jamei, M., Guiras, H. & Mokni N. 2007, A retention curve prediction for unsaturated clay soils,
2nd International Conference Mechanics of unsaturated soils, 7th- 9
thMarch , Bauhaus-
Universitt Weimar, Germany.
Kerrie Fabius & Thunder Bay 2004, Slope Hazard Management with the cautionary zone
approach: a case history. 57th
Canadian Geotechnical Conference. Quebec City, Canada.
Vanapalli, S.K., Fredlund, D.G, Pufahl, D.E., & Cliftron, A.W.1996 Model for prediction of
shear strength with respect to soil suction, Canad. Geot. J., 33: 379-392.
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