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DISCUSSION. Yuefeng Zhou a , W. M. Yan a , L. G. Tham a , Fuchu Dai b and Ling Xu b a Department of Civil Engineering, The University of Hong Kong b Institute of Geology and Geophysics, Chinese Academy of Sciences. - PowerPoint PPT Presentation
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Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
6
DISCUSSION
Yuefeng Zhoua, W. M. Yana, L. G. Thama, Fuchu Daib and Ling Xub
aDepartment of Civil Engineering, The University of Hong Kong
bInstitute of Geology and Geophysics, Chinese Academy of Sciences
Stability Analysis of a Loess Slope with Water Stability Analysis of a Loess Slope with Water Infiltration Affected by CracksInfiltration Affected by Cracks
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Introduction Field investigation Numerical modeling Conclusion
Outline
In China, loess covers proximately 6.6% of the total area. Loess Plateau is the greatest bulk accumulation of loess on earth, the area of which is 31700 km2 (containing 50% of loess in China).Loess plateau is one of the most severe terrain in China for geohazards. In recent years great range of loess plateau is subject to serious and accelerated soil-water erosion. Loess landslide, as a typical geological disaster in China, occurs frequently in loess plateau and has been paid special attentions in recent years.
Introduction
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Introduction
Location: Location: Heifangtai Loess Plateau60 km southwest of Lanzhou, China
Description of the Study Area: Description of the Study Area: Loess thickness is 40 to 50 m.The bedrock is mainly mudstone and siltstone.Extensive cracks developed on the edge of loess plateau so that failure can be easily initiated.Agricultural production is the major economic source for local residents.
The Site
Climate:
The climate at Heifangtai plateau is temperate semiarid.
The average annual precipitation amount is 287 mm.
Under such a dry condition, a typical character shown
at Heifangtai plateau is that extremely steep slope.
Introduction
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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historic landslide
Yellow River
Introduction
groundwater seepage
From 1968 to 2010, more than 60 major landslides occured at Heifangtai Loess Plateau (13.7km2).
The reason for large amount of landslides at Heifangtai Plateau is the rise of groundwater table due to long-term and continuous irrigation of agricultural lands.
Based on early stage investigation, a typical slope was chosen at the edge of plateau to conduct this field test to simulate flooding irrigation to study stability of slope with water infiltration.
Introduction
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Field test
Range of installation
Principal section
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Date (yyyy-mm-dd)
Mo
istu
re c
on
ten
t (%
)
S1_M1 (0.5m)
S1_M2 (1m)
S1_M3 (2m)
S1_M4 (3m)
Field investigation
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-10
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Date (yyyy-mm-dd)
Su
cti
on
(k
Pa
)
S1_T1 (0.5m)
S1_T2 (1m)
S1_T3 (2m)
S1_T4 (3m)
Field investigation
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Field investigation
The slope angle was measured by compass
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Numerical modeling
Four layers of undisturbed samples were taken at a slope nearby at
the depth of 5m, 10m, 15m and 30m respectively. Then the samples
were airproofed by preservation membranes and wax.
ICU and CS tests were performed on undisturbed loess samples.
Soil properties (strength)
Kv is several times to several dozens times higher than Kh.
Permeability adopted here: Kv= 4.8 × 10-6 m/s; Kh=7 × 10-7m/s
Numerical modeling
Soil Properties (permeability)
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Numerical modeling
Suction (kPa)
0.01 0.1 1 10 100 1000 1e+004 1e+005 1e+006
Vol. W
ater Content (m
3/m3) (x 0.001)
0
50
100
150
200
250
300
350
400
450
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
1.E-06
1.E-05
0 1 10 100 1000
Suction (kPa)
Pe
rme
ab
ility
(m
/s)
Kv Kh
Fitting curves of SWCC for whole range by equation (Fredlund et al. 1994)Prediction of unsaturated permeability curves(Fredlund et al. 1994)
FOS=1.101 FOS=1. 115 (a)
(c)
(b)
(d)
Suction for (a) with cracks and (b) without cracks, and volumetric water content for (c) with cracks and (d) without cracks after irrigation on 17 Oct., 2009(3rd day)
Numerical modeling
Suction for (a) with cracks and (b) without cracks, and volumetric water content
for (c) with cracks and (d) without cracks after irrigation on 20 Oct., 2009 (6th day)
Numerical modeling
FOS=1.090 FOS=1.110 (a)
(c)
(b)
(d)
Suction for (a) with cracks and (b) without cracks, and volumetric water content
for (c) with cracks and (d) without cracks after irrigation on 24 Oct., 2009 (10th day)
Numerical modeling
FOS=1.068 FOS=1.108 (a)
(c)
(b)
(d)
Suction for (a) with cracks and (b) without cracks, and volumetric water content
for (c) with cracks and (d) without cracks after irrigation on 26 Oct., 2009 (12th day)
Numerical modeling
FOS=1.061 FOS=1.107 (a)
(c)
(b)
(d)
0.95
1.00
1.05
1.10
1.15
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Date (yyyy-mm-dd)
Fac
tor
of
Saf
ety
with cracks
without cracks
initial value (strength from CS tests)
initial value ( strength from ICU tests)
Numerical modeling
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Conclusions
With the consideration of cracks, the wetting zone is much deeper than without consideration.
Short term irrigation could only trigger local failure rather than global failure of slope.
The existence of cracks could be regarded as an effective way of discharging water for the stability of slope in short time.
Strength parameters from CS tests are more reliable than that from ICU tests
Investigation of Landslide Failure Mechanism in Liquefiable Loess Triggered by Water Infiltration
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Thank you!
Numerical modeling
0
0.5
1
1.5
2
2.5
3
3.5
-160 -140 -120 -100 -80 -60 -40 -20 0
Suction (kPa)D
ep
th (
m)
Initial value (numerical model) Initial value (field monitoring)
0.5m to ponding area(with cracks) 0m to ponding area(with cracks)
field monitoring results measuring span0.5m to ponding area(no cracks) 0m to ponding area(no cracks)
Comparison between simulated and monitored data
Numerical modeling
0.00
0.50
1.00
1.50
2.00
2.50
3.00
3.50
0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35
VWC
De
pth
(m
)
Initial value (numerical model) Initial value (field monitoring)0.5m to ponding area (with cracks) 0m to ponding area (with cracks)
0.5 m to ponding area (no cracks) 0 m to ponding area (no cracks)Field monitoring results
Comparison between simulated and monitored data