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ORI GIN AL PA PER
Critical rainfall to trigger landslides in Cunha Riverbasin, southern Brazil
Gean Paulo Michel • Roberto Fabris Goerl • Masato Kobiyama
Received: 22 May 2014 / Accepted: 10 September 2014 / Published online: 24 September 2014� Springer Science+Business Media Dordrecht 2014
Abstract In 2008, Rio dos Cedros city in Santa Catarina State, Brazil, suffered from
numerous landslides. The objective of the present study was, therefore, to apply the slope
stability model SHALSTAB to the Cunha River basin, which is located in this city, and to
estimate the rainfall necessary to trigger the landslides, which is defined as critical rainfall.
Some geotechnical parameters were determined through field survey and laboratory test. The
slope stability map elaborated with SHALSTAB was compared to the landslide inventory
map, which confirmed the good performance of this model for the study area. In the model
calibration, the values of the hydrologic ratio (q/T), which is the steady-state recharge (q) per
transmissivity (T), were determined in order to rearrange the classification of the slope
stability–instability conditions. After determining these values, the q value which is equiv-
alent to the critical rainfall was estimated. Based on the rainfall time series data from 1941 to
2011, the critical rainfall was determined 1,042.55 mm in 68 days, equivalent to a steady-
state recharge of 15.33 mm/day. This result implies that landslides in Rio dos Cedros city in
2008 were triggered by an association between intense rainfall and a long rainy period.
Keywords Landslides � SHALSTAB � Steady-state recharge � Critical rainfall
1 Introduction
There is a worldwide increase in life loss and material damages associated with natural
disasters. According to McDonald (2003), this increase is due to the rise in the number of
G. P. Michel (&) � M. KobiyamaInstituto de Pesquisas Hidraulicas, Universidade Federal do Rio Grande do Sul, Av. Bento Goncalves,9500, Caixa Postal 15029, Porto Alegre, RS 91501-970, Brazile-mail: [email protected]
R. F. GoerlDepartamento de Geociencias, Universidade Federal de Santa Catarina, Campus Universitario,Trindade, Florianopolis, SC 88040-900, Brazil
123
Nat Hazards (2015) 75:2369–2384DOI 10.1007/s11069-014-1435-6
people occupying susceptible areas as well as their low economic conditions that permit to
construct only very poor and unsafe houses. By using the available data of the Emergency
Disaster Data Base—EM-DAT of the Centre for Research on the Epidemiology of Disas-
ters—CRED, the temporal distribution of the world natural disasters during the period from
1900 to 2013 can be seen in Fig. 1. Though all kinds of disasters increase in frequency, the
hydrological disasters such as floods and landslides show the largest increase. It is noted that
about 50 % of people affected by the natural disasters suffered from the hydrological ones.
In Brazil, the recent occurrences of natural disasters have been more serious and det-
rimental, e.g., the landslides and floods in Santa Catarina State in 2008 (Frank and Se-
vegnani 2009), landslides in Angra dos Reis and Morro do Bumba regions in Rio de
Janeiro State in 2010 and landslides and floods in Teresopolis, Nova Friburgo and Pet-
ropolis cities in Rio de Janeiro State in 2011 (Avelar et al. 2011; Coelho Netto et al. 2011).
These disasters demonstrated that the Brazilian society is still unprepared to deal with such
hydrologically extreme events. Hence, it becomes more important to comprehend the
mechanisms that trigger the hydrological disasters and to establish adequate counter-
measures focusing on damage reduction.
Demonstrating how the disaster evolution performs during a city implementation from
floods to landslides, Kobiyama et al. (2010a) emphasized that the more attention might be
paid for landslides in Brazil. One of the most efficient countermeasures for reducing
landslide-related disasters is the mapping of susceptible areas.
To identify the locality of potential shallow landslide occurrence, there are several slope
stability models, e.g., SHALSTAB (Dietrich and Montgomery 1998; Montgomery and
Dietrich 1994), SINMAP (Pack et al. 1998) and TRIGRS (Baum et al. 2008). These models
have been worldwide accepted and utilized in the slope stability analysis (Cervi et al. 2010;
Chacon et al. 2006; D’Amato Avanzi et al. 2009; Huang and Kao 2006; Sorbino et al.
2009; Tarolli and Tarboton 2006; Terhorst and Kreja 2009; Yilmaz and Keskin 2009).
Applied for some Brazilian basins, SHALSTAB showed better performance than other
stability models (Vieira et al. 2009), specially on Cunha River basin (Michel et al. 2014);
thus, SHALSTAB was adopted in the present study.
SHALSTAB, in relation to the hydrological condition, adopts the assumption of O’loughlin
(1986), which considers a steady-state recharge that occurs when there is equilibrium between
inflows and outflows in the soil layer situated at a slope. This recharge allows predicting the
saturation level of the slopes. The above-mentioned condition never occurs naturally. However,
this assumption permits to simulate the effect of transient storms in increasing the water table,
generally responsible for triggering of landslides (Dietrich and Montgomery 1998; Hammond
et al. 1992). Though the effect of a transient storm could be simulated by the steady-state
recharge, there is no consensus about the numeric relation between them. According to Pack
et al. (2005), in the landslide modeling, the steady-state recharge is not related to a long-term
(e.g., annual) average of recharge, but related to a critical period of rainfall that can trigger
landslides. In the tropics where the soil is generally thicker, transient storms cannot trigger
landslides frequently because of the difficulty to significantly elevate the water table. Fur-
thermore, long rainy periods that resemble real steady-state recharge could lead the hillslope to
an unstable condition, allowing that a less intense storm triggers the landslide.
Dhakal and Sidle (2004) listed many studies about the characteristics of rainfall and
recharge associated with landslides. Some of them investigated the relationships between
the landslide occurrences and threshold values of rainfall for landslide hazard assessment,
prediction and warning systems. These studies generally consider the topographic and
geotechnical characteristics of the basin. Others studies are empirical and show the relation
between intensity and duration of the rainfall to trigger landslides (Caine 1980; Guzzetti
2370 Nat Hazards (2015) 75:2369–2384
123
et al. 2008; Saito et al. 2010). However, the relationship between the rainfall characteristics
(duration and amount) and the landslide triggering is still not very clear in cases where the
physical characteristics of the basin are considered.
In this context, the objectives of the present study were (1) to analyze the rainfall
associated with an extreme event occurred in Cunha River basin, Rio dos Cedros city,
Santa Catarina State, Brazil, in November 2008, by using some hydrological, geotechnical
and geomorphic analysis in association with SHALSTAB and (2) to determine the critical
rainfall necessary to trigger landslides.
2 Theory of SHALSTAB with soil cohesion
The Shallow Landsliding Stability Model (SHALSTAB) developed by Dietrich and
Montgomery (1998) is a mathematical computational model based on the combination
between a slope stability model and a hydrological model and freely available in the
internet. For stability analysis, this model uses the infinity slope theory and assumes the
hydrological steady state, the flow parallel to the surface and the Darcy’s law to estimate
the spatial distribution of the pore pressure. The simulations are performed in the ArcView
version 3.2, and the digital elevation model (DEM) provides data to calculate the upslope
drainage area and slope. Therefore, each pixel that composes the terrain contains a single
value to each morphometric parameter, enabling a discrete analysis.
The infinite slope analysis considers a uniform layer of soil over an infinite inclined
surface and ignores the effects caused by the boundaries. This analysis can be done in each
local where the slope length is much larger than the soil width, and only tangential stress
and normal stress at the base of the soil are considered.
The stability slope model is based on the Mohr–Coulomb law, in which, during the
rupture, the tangential stress is equal to the sum of the stabilizers efforts, i.e.,
s ¼ cþ ðr� uÞ � tan / ð1Þ
where s is the shear stress; c is the soil cohesion; r is the normal stress; u is the pore
pressure; and / is the soil internal friction angle. Considering the root strength and the
height of water table, Selby (1993) rewrote Eq. (1) and applied it to infinite slopes:
Fig. 1 Natural disaster occurrences and percentage of people affected by them from 1900 to 2013
Nat Hazards (2015) 75:2369–2384 2371
123
qs � g � z � sin h � cos h ¼ cr þ cs þ ðqs � g � z � cos2 h� qw � g � h � cos2 hÞ � tan / ð2Þ
where cr is the root cohesion; cs is the soil cohesion; h is the slope; qs is the soil density; qw
is the water density; g is the gravitational acceleration; z is the soil depth; and h is the water
table level above the failure plane.
Dietrich et al. (1995) solved Eq. (2) for h/z that represents the proportion of the satu-
rated soil column at instability condition. Though in their formulations the cohesion term
was ignored, the present study considers soil cohesion term because it can play an
important role in stability of tropical soils. Then, it is obtained:
h
z¼ qs
qw
� 1� tan htan /
� �þ c
cos2 h � tan / � qw � g � zð3Þ
When the soil layer is completely dry, the term h/z in Eq. (3) is set to zero, and a
minimum slope angle for unconditional instability is obtained. When the slope is steeper, it
is classified as unconditionally unstable:
tan h� tan /þ c
cos2 h � qs � g � zð4Þ
When the soil layer is saturated, the term h/z in Eq. (3) is set to one, and a maximum
angle for unconditional stability can be obtained:
tan h� tan / � 1� qw
qs
� �þ c
cos2 h � qs � g � zð5Þ
If the situation does not correspond to Eqs. (4) or (5), the hydrological model is
incorporated to predict the wetness necessary to cause the instability. The hydrological
model used in SHALSTAB follows the principles of Beven and Kirkby (1979) and
O’loughlin (1986), where the soil saturation (w) is related to the upslope drainage area (a),
the unit contour length (b), the slope steepness (h), the soil transmissivity (T) and the
steady-state recharge (q) of a certain point, i.e.,
w ¼ q � ab � T sin h
¼ h
zð6Þ
Replacing w for h/z, Eqs. (3) and (6) can be equated. Then, combining the infinite slope
stability model and the hydrological model, a hydrologic ratio (q/T) can be obtained:
q
T¼ b
a� sin h � qs
qw
� 1� tan htan /
� �þ c
cos2 h � tan / � qw � g � z
� �ð7Þ
This is the main equation applied in SHALSTAB, which considers the soil cohesion.
Hence, it is very clear that only rainfall data are not sufficient to predict the stability
level of a slope. The slope stability depends on many hydrological, geotechnical and
topographic variables. Based on geotechnical and topographic input data, SHALSTAB
calculates a minimal hydrologic ratio (q/T) where the conditions for instability are satis-
fied. The higher the ratio q/T, the lower the probability of a slope destabilization.
2372 Nat Hazards (2015) 75:2369–2384
123
3 Materials and methods
3.1 Study area
Many cities in Santa Catarina were affected by landslides and floods in November 2008,
mainly those located in Itajaı Valley (Frank and Sevegnani 2009). The Rio dos Cedros city
was severely damaged, having 8,561 people directly affected by the event and 96 people
homeless. The disaster damaged 191 low-class and 96 middle-class houses, and the eco-
nomic losses reached around US$ 1,754,272, of which US$ 1,138,187 in agriculture, US$
250,553 in cattle raising, US$ 33,191 in industry and US$ 332,340 in basic services (Goerl
et al. 2009). The present study area is the Cunha River basin, a rural basin in Rio dos
Cedros city, where seven large rapid shallow translational landslides occurred (Fig. 2).
Due to the great accumulation of water in the soil, the material released from the slopes
turned into debris flows that delivered a lot of sediment to the main channels. Kobiyama
et al. (2010b) measured the geometry and estimated the initial volume of four landslides/
debris flows that occurred in this basin. Among these, the volume of the biggest was
estimated in 50,000 m3 with a width of approximately 60 m and a thickness of 10 m, while
the smallest volume was estimated in 6,000 m3, 40 m wide and 10 m thick. All the
landslides occurred in the basin are rainfall-induced without anthropic contribution.
The Cunha River basin has 16.35 km2, and its altimetry varies from 90 m to 860 m. The
Cunha River has a mean slope of 8 % and altimetric amplitude of 640 m. The basin is
composed of gneiss (94 %) and shale (6 %). The inceptisols, classified as cambisoils by the
Brazilian System of Soil Classification (EMBRAPA 2009), are predominant and occupy
about 75 % of the basin area (IBGE 2003). These soils are mainly associated with steep
slopes and are composed by clayey material in this basin. The other 25 % of the basin area
is occupied by ultisols (classified as argisols in Brazilian classification).
3.2 Input data
3.2.1 Topographic data
The digital terrain model (DTM) was elaborated based on 5-m contour lines, obtained
through field survey with a Leica ADS-40 airborne digital sensor. The contour lines were
interpolated by the ArcGis version 9.3 Topo to Raster extension resulting in a raster map
consisting in cells of 5 m of resolution.
The landslide scars were determined by visual analysis of the basin orthophotos in
1:5,000 scale and from more than 3,000 georeferenced points collected by field survey with
a D-GPS and a total station. All the points collected showed a subcentimetric precision in
plan-altimetry. After identifying three parts of landslides (initiation, transport and depo-
sition) in the field, the present study plotted only the initiation areas on the landslide
inventory map which was used for calibrating the SHALSTAB model.
3.2.2 Rainfall data
Even though SHALSTAB can be applied without rainfall data, the contextualization of the
results depends on the rainfall analysis. Therefore, the hourly rainfall data were extracted
from three rain gauge stations located in Rio dos Cedros city (Fig. 2). Although the rain
gauges were not situated in Cunha River basin and were distant about 6–12 km from the
Nat Hazards (2015) 75:2369–2384 2373
123
basin and among them, the rainfall series was analyzed and the measured values were very
similar among them. During the field survey in the basin, ravines, grooves or overland flow
were not observed, which permits to conclude that there is no surface flow with rainfalls of
low–medium intensity in the major part of Cunha River basin. That is why the present
study assumes that all the rainfall infiltrates into the soil layer.
3.2.3 Geotechnical data
The present study assumed that the landslide faces represent the failure triggering condi-
tions. Ten undisturbed soil samples were collected in the landslide scars, all of which are
situated in the same type of soil (cambisoil) that covers approximately 75 % of the basin
area. These soil samples were conducted to laboratory where tests were carried out to
obtain the geotechnical information. The shear strength parameters of soil (internal friction
angle and cohesion) were determined by direct shear test with undisturbed saturated soil
samples in drained conditions.
Fig. 2 Location and altimetry of Cunha River basin
2374 Nat Hazards (2015) 75:2369–2384
123
By the relation between mass and volume of the saturated soil, the saturated soil bulk
density was determined. The particle size distributions of soil samples were determined
and used to estimate the saturated hydraulic conductivity (Ks) by the HYDRUS-1D soft-
ware that contains the Rosetta Lite Version 1.1 model proposed by Schaap et al. (2001).
This model generates the soil hydraulic properties from soil textural data. Though Ks
generally decreases with soil depth, the present study considered its value constant along
the soil depth.
The estimation of soil depth of the basin was done by field observations on the land-
slides scars. All the landslides in the basin occurred at a similar depth (*10 m).The mean
depth where the slope failures occurred was considered the soil layer depth for the entire
basin (Fig. 3).
3.3 Critical rainfall determination procedure
SHALSTAB uses Eq. (7) to designate the stability degree of the slope. This equation is
solved for two hydrological variables: q and T. Hence, it is a parameter-free model where
the stability classification is determined by the q/T ratio. According to Dietrich et al.
(1995), the amount of rainfall necessary to destabilize the slope, which is called the critical
rainfall in the present study, is directly proportional to Ks of the soil at the ground surface
and inversely proportional to the decline rate of Ks by the increment of soil depth. Con-
sidering the variability of Ks, T can be obtained by the integration of this parameter along
the soil depth. This study considered that there is no variation of Ks, and then, T was
calculated by the product between Ks and the soil thickness. The transmissivity is a
parameter that estimates the facility how the water in the soil is drained by the slope.
Slopes where soils have high T can rapidly lower the water table level during or after a
heavy rainfall, which contributes positively to the slope stability. Therefore, the effective
application of the model requires the estimation of T.
Dietrich and Montgomery (1998) originally proposed seven stability classes in
SHALSTAB. The two extreme classes refer to Eqs. (4) and (5) which represent uncon-
ditionally unstable and unconditionally stable areas, respectively. The other five classes are
established according to the q/T ratio. The standard values of q/T used by SHALSTAB as
thresholds of the stability classification were set by statistical analysis of landslides which
occurred in predicted unstable areas and total unstable areas in the basin (Dietrich et al.,
1995). The q/T values were determined so that the results included the largest number of
landslides and the smallest total unstable areas in the basin. These values were set as
stability thresholds. The higher value of q/T implies the lower probability of instability.
For a better understanding of the mechanism involved in critical rainfall, the present
study reduced the five classes of stability established by q/T values to two. Thus, the terrain
is here classified in four classes: unconditionally unstable, unstable, stable and uncondi-
tionally stable. This classification requires only one value of q/T as stability threshold.
Table 1 shows a comparison between the original and proposed classification.
In SHALSTAB application, the present study compared the landslide inventory map
with the unstable areas identified by the model. The q/T values that represented the stability
threshold were determined when unstable pixels coincide with the landslides occurrences
of the inventory map. By changing the q/T values, a reclassification of the SHALSTAB
results was performed. Hence, four values of q/T were established for the stability
threshold, resulting in four different stability maps.
The variation in q/T values also causes to vary the number of unstable pixels within
landslide scars, as well as the total unstable area within the basin. The present study
Nat Hazards (2015) 75:2369–2384 2375
123
assumed that only one unstable pixel within the landslide scar is sufficient for the model
success in prediction. The destabilization of a small area represented by few pixels can
destabilize a much larger volume of soil due to the relaxing of the slope strengths. When
there were different stability classes inside the same scar, the less stable class inside it
finally defined its classification.
In landslide modeling, the steady-state recharge (q) refers to a value to mimics the
behavior of ground saturation during a large storm (Dietrich and Montgomery 1998).
However, O’loughlin (1986) explained that a quasi-steady state occurs in basins where
drainage flux, hillslope outflow and the boundaries of saturation zones slightly vary. Then,
the present study considered that the conditions of the Cunha River basin during the
analyzed period resembled a quasi-steady state; thus, the real values of the rainfall series
were used in the modeling.
The determination of an actual q value requires the recognition of a rainfall period. The
ratio between the amount of rainfall and total time of this period may represents q (mm/
day). Though this period is associated with successive rainfall events which are capable to
trigger landslides, it is quite difficult to estimate its amplitude. To estimate the period able
to trigger landslides, a value of q was extracted from each q/T ratio which characterized the
four threshold conditions. The selection of q/T threshold values was executed by observing
the coincidence of predict unstable areas and registered landslides scars. After establishing
the q/T threshold values, the q values were calculated with the estimated value of T. These
values of q are related to an accumulated rainfall or critical rainfall.
Each value of q was sought within the rainfall series of the basin. A retrospective
accumulation of the rainfall from the triggering moment of landslides (9 a.m. of November
23, 2008) was calculated. Dividing the rainfall accumulated by the accumulated time,
several rainfall rate values that really occurred in the basin were obtained. When the value
Fig. 3 Head of a landslide in Cunha River basin
2376 Nat Hazards (2015) 75:2369–2384
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of the rainfall rate becomes equal to the q value calculated from the ratio q/T, the period
and the critical rainfall related to the landslides triggering were determined.
4 Results and discussion
4.1 Geotechnical characteristics of soils
The mean of each input parameter was used in the modeling. According to Ohta et al.
(1983), the values of Ks on the hydrological modeling can be considered an order of
magnitude (about 10 times) higher than those obtained in laboratory measurement due to
the preferential pathways. The Ks values estimated by HIDRUS-1D are, on average, one
order of magnitude smaller than measured (Schaap and Leij 2000). Mota and Kobiyama
(2011) compared the values of Ks measured in laboratory with those estimated by HY-
DRUS-1D of some Brazilian soils whose sampling locations are very close to the present
study. They reported that the values of Ks estimated by HYDRUS-1D were, in general,
from 10 to 100 times smaller than the measured ones. Thus, the value of Ks obtained with
HYDRUS-1D was raised in one order of magnitude for the present study.
Since the values measured for soil strength were similar for all soil samples, their mean
values were applied for the entire basin. The values adopted in the present study are
showed in Table 2.
4.2 Analysis of the stability model
The results of SHALSTAB simulation, using the parameters of Table 2, are shown in
Fig. 4 where the classification is based on seven stability classes established originally by
Dietrich and Montgomery (1998). The model considered most of the flat areas as
unconditionally stable, even in saturation conditions. Steeper areas were classified as
unstable areas, even in low soil moisture conditions. The unconditionally unstable areas are
extremely steep areas. In the areas where topography is not very flat or very steep, the
hydrological parameters determined the classification. The upslope drainage area has a
large influence on the classification determination. Regions with high flow concentration
due to the relief convergent curvature are almost classified as unstable areas.
All the seven inventoried landslides coincided with the two more unstable classes.
Among them, only one was in the unconditionally unstable class and the others in the
second more unstable class. Although the unconditionally unstable class areas did not
Table 1 Comparison between original and proposed classification
Original classification Proposed classification
Unconditionally unstable (Eq. 4) Unconditionally unstable (Eq. 4)
log q/T \ -3.1 Unstable
-3.1 [ log q/T [ -2.8 qT� b
a� sin h � qs
qw� ð1� tan h
tan /Þ þ ccos2 h�tan /�qw �g�z
n o
-2.8 [ log q/T [ -2.5 or
-2.5 [ log q/T [ -2.2 Stable
log q/T [ -2.2 qT\ b
a� sin h � qs
qw� ð1� tan h
tan /Þ þ ccos2 h�tan /�qw �g�z
n o
Unconditionally stable (Eq. 5) Unconditionally unstable (Eq. 5)
Nat Hazards (2015) 75:2369–2384 2377
123
contain more incidences of landslides than the second unstable class, it can be said that
SHALSTAB performance was satisfactory for the Cunha River basin. The mathematical
condition that leads an area to be classified as unconditionally unstable is physically unreal.
The classification of an area as unconditionally unstable indicates an error in the estimation
of parameters, generally soil thickness or soil strength. In a lot of cases, the places where
the model indicated unconditionally instability are sites of bedrock exposure (Dietrich and
Montgomery 1998).
4.3 Critical rainfall
The rainfall condition in Rio dos Cedros city during the second semester of 2008 played a
relevant role for triggering landslides. The daily and accumulated rainfalls from August 1
to November 23, 2008 are demonstrated in Fig. 5. The accumulated rainfall during this
period reached 1,200 mm which is about 2/3 of the mean annual rainfall in the city.
The stability map generated by SHALSTAB was reclassified to obtain the correct
q/T value which could be thought to trigger landslides in this basin. This value of q/T was
varied for four different patterns of classification. The value of log q/T used in each
reclassification was as follows: -3.4, -3.3, -3.1 and -2.8. For selecting these values,
some criteria were used. The smallest value of log q/T (= -3.4) was established when at
least one unstable pixel remained inside each landslide scar. The largest value of log
q/T (= -2.8) was obtained when the unstable area in the basin became larger than stable
area and the simulation results became unreal. The other values were adopted based on
Dietrich and Montgomery (1998). The variation on the log q/T values caused the variation
of density of unstable pixels in the landslide scars (Fig. 6) as well as the total unstable area
in the basin (Table 3).
Using the q/T values adopted for the reclassifications, the value of T and rainfall data,
the values of q, the time period (total number of days) and critical rainfall were calculated
(Table 4). The rainfall series of the basin from 1941 to 2011 was analyzed. Analogous
rainfall periods with the same or higher accumulated rainfall were searched in order to
verify the singularity of the events related to the q values shown in Table 4. In the rainfall
series of the basin, any event similar to the one with the critical rainfall (1,042.55 mm) and
the period (68 days) related to the steady-state recharge of 15.33 mm/day was not found.
Furthermore, 14, 30 and 6 analogous events were identified for log q/T = -3.3, -3.1 and
-2.8, respectively.
Figure 7 shows the complete rainfall series of the basin with daily rainfall values
grouped for 3, 8, 28 and 68 days of accumulation. It is clearly noted that only the critical
rainfall related to 68 days of accumulation had never occurred till November 2008. The
dwellers of the region and the local media had not reported the occurrence of landslides
with similar magnitude in this basin. Therefore, those landslides in Cunha River basin in
Table 2 Model input values ofsoil parameters
Parameter Value
Internal friction angle of soil (/) 31�Cohesion (c) 11,900 N/m2
Saturated soil density (qs) 1,815 kg/m3
Soil depth (z) 10 m
Saturated hydraulic conductivity (Ks) 0.38 m/day
2378 Nat Hazards (2015) 75:2369–2384
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November 23, 2008, were supposed to be triggered by the critical rainfall of 1,042.55 mm
in 68 days. It confirms quantitatively the conclusion of Kobiyama et al. (2010b) where, in
the case of landslides/debris flows in Cunha River basin, the triggering factor was not only
the rainfall intensity but also its accumulated value.
Fig. 4 Stability map of Cunha River basin, with seven original classes
Fig. 5 Daily and accumulates rainfall in Cunha River basin during the period from August 01, 2008, toNovember 23, 2008
Nat Hazards (2015) 75:2369–2384 2379
123
For a complementary analysis, the accumulated rainfall and log q/T were calculated for
periods that vary from 1 to 100 days before the landslides occurrence. The rainfall data
series from 1941 to 2008 were verified in order to find the analogous rainfall periods for
each corresponding accumulated rainfall value. Figure 8 shows that in the range from 37 to
92 days of accumulation, there is no analogous period with the same accumulated rainfall,
except the period of 50 days that has one analogous. Although there are other periods
without analogous, the accumulation of 68 days (log q/T = -3.4) is the unique one that
can be supported by a log q/T threshold value adequate to the proposed method. Periods
shorter than 68 days are related to higher log q/T values. If these values are used as rainfall
threshold, excessive unstable area could be created in the basin. On the other hand, periods
Fig. 6 Reclassification of stability map with different values of log q/T: a -3.4; b -3.3; c -3.1; and d -2.8
Table 3 Areas in four stability classes in Cunha River basin with different values of log q/T
Class Percentage of area (%)
log q/T = -3.4 log q/T = -3.3 log q/T = -3.1 log q/T = -2.8
Unconditionally unstable 1.46 1.46 1.46 1.46
Unstable 5 6.61 11.51 22.2
Stable 34.51 40.97 28 17.31
Unconditionally stable 59.03 59.03 59.03 59.03
2380 Nat Hazards (2015) 75:2369–2384
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longer than 68 days are related to smaller log q/T values. If used as rainfall threshold, it
could not detect the actual localities of landslides occurrence in this basin.
There are several empirical studies that proposed relations between rainfall thresholds
and triggering landslides (Caine 1980; Innes 1983; Larsen and Simon 1993; Aleotti 2004;
Cannon et al. 2008; Guzzetti et al. 2008; Dahal and Hasegawa 2008; Saito et al. 2010).
Although none of them could be applied for 68 days (1,632 h) of duration rainfall, all of
them were tested. The results obtained vary from -87 to ?30 % of the value estimated by
the physically based methodology adopted by this work (*0.64 mm/h). The most similar
value is from the equation proposed by Aleotti (2004), with a difference of approximately
26 %.
Other values of intensity tested and discarded by the present study (related to the
accumulated rainfall of 3, 8 and 28 days) were compared to the values obtained by the
empirical equations. The difference showed variability similar to the early comparison
between empirical equation and the selected intensity calculated by the present study.
Thus, for this case, it is difficult to define the specific rainfall intensity responsible for
triggering the landslides only with the empirical equation. This way, the physically based
methodology proposed in the present study can help to define it.
The q value responsible for triggering the landslides is under the condition of log q/
T = -3.4. This value is the smallest among the four conditions (Table 4) and is related to
Table 4 Values of q, period andaccumulated rainfall correspond-ing to four different values of logq/T
log q/T q (mm/day) Number of days Critical rainfall (mm)
-3.4 15.33 68 1042.55
-3.3 19.06 28 533.66
-3.1 27.09 8 216.76
-2.8 55.59 3 166.76
Fig. 7 Rainfall amount series: a 3 days; b 8 days; c 28 days; and d 68 days
Nat Hazards (2015) 75:2369–2384 2381
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the longer period. Then, it is said that a long rainy period can be as significant as shorter
periods of heavy rainfall for triggering landslides in tropical thicker soils. Heavy rainfalls
that occurred during a short period have higher q values that did not match to the calculated
recharges responsible for triggering landslides. In case of these larger recharges remain for
longer periods; the number of landslides in the studied basin would be much larger. The
landslides which occurred in Cunha River basin were triggered by a smaller recharge that
remains sufficient time to lead some slopes to a less stable condition. In tropical soils,
generally much thicker, the triggering of landslides requires a significant elevation of the
water table which often is not likely to be caused by isolated transient storms.
5 Conclusion
Heavy rainfalls and/or long rainy periods are the main triggering factors for landslides in
Brazil. Then, the present study focused on the Cunha River basin, Rio dos Cedros city
(Brazil), in which a lot of landslides occurred with these factors in 2008. After gaining
several geotechnical parameters through field survey and laboratory test, SHALSTAB with
soil cohesion was applied to identify the areas susceptible to landslides. The simulation
results were compared to the landslides inventory map, which confirmed that this model
had a good performance for this basin.
Rearranging the stability classes from seven to four and comparing the stability map
with the landslide inventory, the log q/T value responsible for triggering the landslides was
determined. After that, assuming that the conditions in the basin resemble a quasi-steady-
state subsurface flow, the q value which is equivalent to the critical rainfall was estimated,
i.e., 15.33 mm/day. By a retrospective accumulation of the rainfall series from the moment
of the landslides occurrence, this q value corresponds to 68 days of accumulation and a
total rainfall of 1,042.55 mm. Analyzing the rainfall series in the study basin from 1941 to
2008, any period with similar characteristics was not found. The calculated q value refers
to a long period of accumulation. It indicates the importance of the water accumulation in
the soil layer since larger recharges for shorter periods which occurred many times since
Fig. 8 Values of log q/T and number of analogous rainfall periods for different ranges of rainfallaccumulation period
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1941 did not trigger large landslides. This result permits to emphasize that the accumulated
rainfall plays a very important role in the landslide triggering mechanism.
Although the steady-state recharge never really occurs in a basin, its value is used by
SHALSTAB to predict unstable areas. According to Dietrich and Montgomery (1998), this
recharge value is not real, but must represents the effect of large transient storms in the
wetness. However, the relation between steady state of recharge and transient storms still
remains unclear, and more work should be done for the question.
Notwithstanding the good performance of SHALSTAB in the present study, there are
still some uncertainties in the analysis. Due to the difficulty to estimate the variability of
several hydrological and geotechnical input parameters in the basin, they were all con-
sidered homogenous in the present study. It could lead to underestimation or overesti-
mation of parameters, which could consequently cause some incoherence to the modeling
results.
The stability map generated by the SHALSTAB classifies the area by a hydrologic ratio
(q/T), which is not very easy to interpret and requires that its results are contextualized for
each basin with different hydrological characteristics. Therefore, in addition to geotech-
nical and topographic parameters, the hydrological data should be measured for a more
precise landslide prediction. In case there is a large error in estimating q/T values, the final
error would spread to the calculation of steady-state recharge, critical rainfall and related
period.
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