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UNIVERSITY GHENT<br />

UNIVERSITEIT<br />

GENT<br />

INTERUNIVERSITY PROGRAMME<br />

MASTER OF SCIENCE IN<br />

PHYSICAL LAND RESOURCES<br />

Universiteit Gent<br />

Vrije Universiteit Brussel<br />

Belgium<br />

<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong><br />

<strong>Numerical</strong> <strong>Modeling</strong> Techniques<br />

September 2009<br />

Promotor:<br />

Prof. F. De Smedt<br />

Co-promotor:<br />

Dr. J. Moeyersons<br />

Master dissertation in partial fulfilment<br />

of the requirements for the Degree of<br />

Master of Physical L<strong>and</strong> Resources<br />

by: Shimelies Ahmed Aboye


<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong><br />

<strong>Numerical</strong> <strong>Modeling</strong> Techniques<br />

September 2009<br />

Vrije Universiteit Brussel


i<br />

Acknowledgments<br />

First of all, I would like to express my deep <strong>and</strong> sincere gratitude to my promoter Prof. dr. ir<br />

F. De Smedt. His critical comments, advice, <strong>and</strong> guidance have been invaluable to me during<br />

this research. Above all, I am highly grateful for his timely, detailed <strong>and</strong> untiring corrections.<br />

I would like to extend my heartfelt acknowledgment to my co-promoter Dr Jan Moeyersons.<br />

This study would have never been possible, if it were not for his support in various ways. He<br />

not only provided me substantial data to work in his lab but also guided me during the<br />

subsequent data analysis. I am greatly indebted for his patience, underst<strong>and</strong>ing <strong>and</strong><br />

encouragement.<br />

My acknowledgments to VLIR for financially supporting my study.<br />

Special thanks to Dr ir Philippe Trefois for providing me important technical advice<br />

throughout this work. I cordially acknowledge Ine V<strong>and</strong>ecasteele for her support <strong>and</strong> creating<br />

a conducive atmosphere during my stay in the Royal Central African Museum.<br />

My appreciation also goes to Anja Cosemans for her valuable support during my study. I am<br />

thankful to my friend Eskedil Abebaw for being there when I was in need. I also appreciate<br />

the cooperation from CORE consulting engineers.<br />

Finally, I would like to thank my mother Birukt Assaye. I am where I am because of her.<br />

Shimelies Ahmed<br />

Brussels, August 2009<br />

<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Modeling</strong> Techniques


ii<br />

Abstract<br />

Rain-fall triggered slope instabilities are common problems in the hilly <strong>and</strong> mountainous<br />

terrains of the highl<strong>and</strong>s of Ethiopia. To cope up with l<strong>and</strong>slide disasters on a regional basis,<br />

regional l<strong>and</strong>slide study is considered to be the primary mitigative measure. This study is<br />

conducted: (1) to determine the l<strong>and</strong>slide susceptibility of a 497 km² area in Hagere Selam,<br />

northern Ethiopia; (2) to test different numerical models of slope stability analysis, <strong>and</strong> select<br />

the most suitable prediction technique that can be used in similar regions; (3) to describe the<br />

statistical relations of l<strong>and</strong>slide frequency with the physical parameters contributing to the<br />

initiation of l<strong>and</strong>slides.<br />

A l<strong>and</strong>slide inventory of the study area is primary compiled from existing digital maps,<br />

previous studies <strong>and</strong> aerial photographs. 30 debris flows, 7 l<strong>and</strong>slide belts, 4 l<strong>and</strong>slides in the<br />

Antalo supersequence, 12 l<strong>and</strong>slides in Imba Degua <strong>and</strong> Chini ridges, <strong>and</strong> 2 slumps are<br />

identified. The l<strong>and</strong>slide database amounts to about 20% of the study area.<br />

Three steady state scenarios, completely dry, half saturated <strong>and</strong> saturated, are considered for<br />

the deterministic modeling. In addition, 4 statistical techniques are treated: statistical index,<br />

weighting factor, certainty factor <strong>and</strong> l<strong>and</strong>slide susceptibility methods. For each of these<br />

approaches, three different combinations of causative factors are employed. A comprehensive<br />

evaluation of the obtained l<strong>and</strong>slide susceptibility maps is achieved by a model validation<br />

whereby the outputs are justified by comparing them with the l<strong>and</strong>slide inventory.<br />

The hazard maps from the statistical index, weighting factor <strong>and</strong> l<strong>and</strong>slide susceptibility<br />

methods, are highly similar, as indicated by an average of 75% of the area being classified in<br />

the same susceptibility class by these models. The Certainty factor <strong>and</strong> weighting factor<br />

methods confirm to be more powerful prediction techniques than the other statistical models.<br />

The half saturated physically based model provides a comparable result to some of the<br />

statistical outputs. It correctly designates 75% of the inventoried l<strong>and</strong>slides.<br />

Among the entire hazard maps, certainty factor model 1 is selected to be the best model for<br />

identifying l<strong>and</strong>slides. The prediction accuracy of this model is 87%. Compared to the other<br />

methods, it gives the highest posterior probability of l<strong>and</strong>slides in the very high susceptibility<br />

category (0.107). Moreover, it has the smallest probability of l<strong>and</strong>slide bodies in the low<br />

<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Modeling</strong> Techniques


iii<br />

hazard zone (0.005). Accordingly, it is concluded that 41% of the area is under high <strong>and</strong> very<br />

high l<strong>and</strong>slide hazard, 15% is moderately susceptible, <strong>and</strong> 44% is free from l<strong>and</strong>slide risk.<br />

Based on the combined steady state deterministic model, it is concluded that 34.6% of the<br />

study area is unconditionally stable, <strong>and</strong> will not fail under any circumstances unless major<br />

destabilizing activities occur. If extreme rainfall event leads to full soil saturation, 12.4% of<br />

the area will face instability under moderate destabilizing actions, 13.7% of the area will<br />

likely fail under minor destabilizing forces, <strong>and</strong> 17.7% of the area needs stabilization methods<br />

to control instability. L<strong>and</strong>slides will be mobilized in about 16.7% of the area, if the soil is<br />

half saturated; 4.93% of the area will likely fail under any condition, <strong>and</strong> hence stabilization<br />

techniques are recommended.<br />

Finally, it is indicated that slope gradient, lithology, elevation, slope aspect, <strong>and</strong> l<strong>and</strong> use are<br />

statistically significant in predicting slope instability, while faulting, slope shape, proximity to<br />

drainage lines, <strong>and</strong> closeness to roads are found to be unrelated to the l<strong>and</strong>sliding in the study<br />

area. The results of this study demonstrate that slope instability can be effectively modeled by<br />

using <strong>GIS</strong> technology <strong>and</strong> numerical modeling techniques.<br />

<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Modeling</strong> Techniques


<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Modeling</strong> Techniques<br />

iv


v<br />

Table of contents<br />

Acknowledgments .................................................................................................................. i<br />

Abstract ................................................................................................................................. ii<br />

Table of contents ....................................................................................................................v<br />

List of figures ..................................................................................................................... viii<br />

List of Tables .........................................................................................................................x<br />

List of symbols .................................................................................................................... xii<br />

Chapter 1: Introduction ...........................................................................................................1<br />

1.1 Objectives of the study ..................................................................................................2<br />

1.2 Study Area ....................................................................................................................2<br />

1.3 Outline of the thesis ......................................................................................................3<br />

Chapter 2: Literature review ...................................................................................................5<br />

2.1 Factors influencing slope stability .................................................................................5<br />

2.1.1 Gravity ...................................................................................................................5<br />

2.1.2 The effect of water ..................................................................................................6<br />

2.1.3 Geological factors ...................................................................................................6<br />

2.1.4 Soil Properties ........................................................................................................7<br />

2.1.5 The effect of vegetation ..........................................................................................8<br />

2.1.6 Triggering events ....................................................................................................8<br />

2.2 L<strong>and</strong>slide inventory .......................................................................................................9<br />

2.3 Anticipation of l<strong>and</strong>slide hazards ................................................................................. 10<br />

2.4 <strong>GIS</strong> methods ............................................................................................................... 11<br />

Chapter 3: Methodology <strong>and</strong> data preparation ....................................................................... 13<br />

3.1 L<strong>and</strong>slide Inventory mapping ...................................................................................... 13<br />

3.1.1 Mechanism of failures........................................................................................... 17<br />

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vi<br />

3.2 Geotechnical parameters ............................................................................................. 20<br />

3.3 Soil depth .................................................................................................................... 25<br />

3.4 Causative factor maps preparation ............................................................................... 27<br />

3.4.1 <strong>Slope</strong> factor ......................................................................................................... 27<br />

3.4.2 Geological factor ................................................................................................ 28<br />

3.4.3 Distance to faults factor ....................................................................................... 29<br />

3.4.4 Elevation factor ................................................................................................... 30<br />

3.4.5 L<strong>and</strong> use factor .................................................................................................... 31<br />

3.4.6 <strong>Slope</strong> Shape .......................................................................................................... 33<br />

3.4.7 Aspect .................................................................................................................. 33<br />

3.4.8 Distance to streams ............................................................................................... 34<br />

3.4.9 Distance to roads .................................................................................................. 34<br />

3.4.10 Wetness index ..................................................................................................... 36<br />

Chapter 4: Deterministic models ........................................................................................... 37<br />

4.1 Physical based models ................................................................................................. 37<br />

4.1.1 <strong>Stability</strong> of infinite slopes ..................................................................................... 37<br />

4.1.2 Input parameters ................................................................................................... 40<br />

4.1.3 Critical depth ........................................................................................................ 43<br />

4.1.4 Factor of safety calculation ................................................................................... 46<br />

Chapter 5: Statistical <strong>Analysis</strong> approach ............................................................................... 60<br />

5.1 General ....................................................................................................................... 60<br />

5.2 Bivariate statistical analysis ......................................................................................... 61<br />

5.2.1 Statistical index method ........................................................................................ 61<br />

5.2.2 Statistical weighting factor analysis ...................................................................... 75<br />

5.2.3 Certainty factor analysis........................................................................................ 83<br />

5.2.4 L<strong>and</strong>slide susceptibility analysis ........................................................................... 91<br />

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vii<br />

Chapter 6: Comparison <strong>and</strong> Conclusion ................................................................................ 96<br />

6.1 Comparison <strong>and</strong> discussion ......................................................................................... 96<br />

6.2 Conclusions............................................................................................................... 106<br />

6.3 Recommendations ..................................................................................................... 112<br />

References .......................................................................................................................... 113<br />

Appendix ............................................................................................................................ 123<br />

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viii<br />

List of figures<br />

Figure 1.1 Location map of the study area ..............................................................................3<br />

Figure 3.1 L<strong>and</strong>slide Inventory map ..................................................................................... 15<br />

Figure 3.2 Photographic views of some slides ....................................................................... 16<br />

Figure 3.3 L<strong>and</strong>slide mechanism 1........................................................................................ 17<br />

Figure 3. 4 L<strong>and</strong>slide mechanism 2 ....................................................................................... 18<br />

Figure 3.5 Areal distribution of geologic layers .................................................................... 20<br />

Figure 3.6 <strong>Slope</strong> map ............................................................................................................ 27<br />

Figure 3.7 Geologic map ...................................................................................................... 29<br />

Figure 3.8 Distance to faults map .......................................................................................... 30<br />

Figure 3.9 Elevation map ...................................................................................................... 31<br />

Figure 3.10 L<strong>and</strong> use factor map ........................................................................................... 32<br />

Figure 3.11 <strong>Slope</strong> shape <strong>and</strong> Aspect...................................................................................... 33<br />

Figure 3.12 Distance to streams ............................................................................................ 35<br />

Figure 3.13 Distance to roads ............................................................................................... 35<br />

Figure 3.14 Wetness index map ............................................................................................ 36<br />

Figure 4.1 (a) <strong>and</strong> (b) - infinite slope force diagrams............................................................. 37<br />

Figure 4.2 (a) saturated unit weight map, (b) dry unit weight map......................................... 41<br />

Figure 4.3 (a) cohesion map, (b) angle of internal friction map ............................................. 42<br />

Figure 4. 4 Critical depth to lower boundary under fully saturated condition ......................... 44<br />

Figure 4.5 Critical depth, (a) under half saturated, (b) under dry conditions .......................... 45<br />

Figure 4.6 Areal distribution of critical depths under saturated, half sat <strong>and</strong> dry scenarios .... 46<br />

Figure 4.7 Classified factor of safety map under dry condition .............................................. 47<br />

Figure 4.8 Classified factor of safety map for half saturated condition .................................. 50<br />

Figure 4.9 Classified factor of safety map under full saturated condition............................... 53<br />

Figure 4.10 <strong>Stability</strong> map based on three steady state scenarios ............................................ 56<br />

Figure 4.11 Areal distribution of stability classes under three steady state scenarios ............. 56<br />

Figure 4.12 <strong>Stability</strong> under three steady state scenarios vs slope classes ................................ 58<br />

Figure 5.1 Percentage of observed training l<strong>and</strong>slides versus LSI (SI model 1) ..................... 67<br />

Figure 5.2 L<strong>and</strong>slide hazard map (SI model 1) ...................................................................... 68<br />

Figure 5.3 Areal distribution of susceptibility classes (SI model 1) ....................................... 68<br />

Figure 5.4 Percentage of observed training l<strong>and</strong>slides versus LSI (SI model 2) ..................... 70<br />

<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Modeling</strong> Techniques


ix<br />

Figure 5.5 L<strong>and</strong>slide hazard map (SI model 2) ...................................................................... 71<br />

Figure 5.6 Areal distribution of susceptibility classes (SI model 2) ....................................... 71<br />

Figure 5.7 % of observed training l<strong>and</strong>slides VS LSI (SI model3)......................................... 73<br />

Figure 5.8 Areal distribution of susceptibility classes (SI model 3) ....................................... 73<br />

Figure 5.9 L<strong>and</strong>slide hazard map (SI model 3) ...................................................................... 74<br />

Figure 5.10 Percentage of observed training l<strong>and</strong>slides versus LSI. Model 1 (A), Model 2 (B),<br />

<strong>and</strong> Model 3 (C) ................................................................................................. 77<br />

Figure 5.11 Areal distribution of susceptibility classes .......................................................... 78<br />

Figure 5.12 L<strong>and</strong>slide hazard map (a) SWF model 1, (b) SWF model 2 ................................ 80<br />

Figure 5.13 L<strong>and</strong>slide hazard map (a) SWF model 3 ............................................................. 81<br />

Figure 5.14 Percentage of observed training l<strong>and</strong>slides versus CF value: Model 1(A), Model<br />

2(B), Model 3(c), <strong>and</strong> percentage area of susc. Classes (D)................................. 88<br />

Figure 5.15 L<strong>and</strong>slide hazard map (a) CF model 1, (b) CF model2 ....................................... 89<br />

Figure 5.16 L<strong>and</strong>slide hazard map CF model 3 ..................................................................... 90<br />

Figure 5.17 L<strong>and</strong>slide hazard map (a) LS (model 1), (b) LS (model2)................................... 93<br />

Figure 5.18 L<strong>and</strong>slide hazard map LS (model 3) ................................................................... 94<br />

Figure 5.19 Areal distribution of the hazard classes, LS method ........................................... 94<br />

Figure 6.1 Comparison of instability classes with the inventory (Mx = model x).................. 97<br />

Figure 6.2 Comparison between the accuracies of the employed methodologies ................... 98<br />

Figure 6.3 Cumulative % of observed l<strong>and</strong>slides versus cumulative % area ........................ 102<br />

Figure 6.4 A map displaying matching between statistical <strong>and</strong> deterministic methods ......... 106<br />

Figure 6.5 Final Hazard maps based on (A) CF model 1, <strong>and</strong> (B) combined steady state<br />

deterministic methods ......................................................................................................... 111<br />

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x<br />

List of Tables<br />

Table 2.1 Triggering events influencing slope stability ...........................................................8<br />

Table 2.2 Characteristics of l<strong>and</strong>slide susceptibility methods ................................................ 12<br />

Table 3.1 Shear strength parameters ..................................................................................... 22<br />

Table 3.2 Range of shear strength parameters for weathered formations ............................... 22<br />

Table 3.3 Friction angle values for rocks at joints ................................................................. 23<br />

Table 3.4 Angle of friction <strong>and</strong> unit weight values of soils derived from geologic layers ...... 23<br />

Table 3.5 Cohesion <strong>and</strong> friction angle values of soils derived from geologic layers............... 24<br />

Table 3.6 Cohesion <strong>and</strong> friction angle values of soils ............................................................ 24<br />

Table 3.7 Final compiled shear strength parameters .............................................................. 25<br />

Table 4.1 Classification of factor of safety values ................................................................. 40<br />

Table 4.2 Model validation under dry condition .................................................................... 47<br />

Table 4.3 <strong>Stability</strong> vs slope classes ....................................................................................... 48<br />

Table 4.4 <strong>Stability</strong> vs geologic formations ............................................................................ 48<br />

Table 4.5 Model validation under half saturated condition .................................................... 50<br />

Table 4.6 <strong>Stability</strong> vs slope classes under semi saturated condition ....................................... 51<br />

Table 4.7 <strong>Stability</strong> vs geologic formations under semi saturated scenario.............................. 51<br />

Table 4.8 Model validation under fully saturated condition ................................................... 53<br />

Table 4.9 <strong>Stability</strong> versus slope classes ................................................................................. 54<br />

Table 4.10 <strong>Stability</strong> vs geologic formations .......................................................................... 54<br />

Table 4.11 Combined factor of safety classification .............................................................. 55<br />

Table 4.12 Validation of the model (a) with the whole database (b) with validation group .... 57<br />

Table 4.13 <strong>Stability</strong> vs geologic formations .......................................................................... 59<br />

Table 5.1 Weight assignment, statistical index method ......................................................... 63<br />

Table 5.2 Validation of SI model 1 ....................................................................................... 69<br />

Table 5.3 Validation of SI model 2 ....................................................................................... 72<br />

Table 5.4 Validation SI model 3 ........................................................................................... 74<br />

Table 5.5 Weighting factor values ........................................................................................ 76<br />

Table 5.6 Parameters of LSI map <strong>and</strong> cutoff values .............................................................. 78<br />

Table 5.7 Validation of SWF models .................................................................................... 81<br />

Table 5.8 Certainty factor values .......................................................................................... 84<br />

Table 5.9 Parameters of the CF map <strong>and</strong> cutoff values .......................................................... 87<br />

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Table 5.10 Validation of certainty factor method of analysis ................................................. 90<br />

Table 5.11 Weight values for the l<strong>and</strong>slide susceptibility method ......................................... 92<br />

Table 5.12 Validation results for l<strong>and</strong>slide susceptibility method of analysis ........................ 95<br />

Table 6.1 Areal distribution summary (M x = model x) ........................................................ 96<br />

Table 6.2 Posterior probabilities of all methods .................................................................. 100<br />

Table 6.3 Agreed areas on stability classes using statistical index method ........................... 102<br />

Table 6.4 Agreed areas on stability classes using statistical WF method ............................. 103<br />

Table 6.5 Agreed areas on stability classes using statistical CF method .............................. 104<br />

Table 6.6 Agreed areas on stability classes by four bivariate methods ................................. 104<br />

Table 6.7 Agreed areas on by physically based <strong>and</strong> certainty factor methods ...................... 105<br />

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xii<br />

List of symbols<br />

<strong>GIS</strong><br />

Geographic Information Systems.<br />

Fs<br />

Factor of safety<br />

SRTM<br />

Shuttle Radar Topography Mission<br />

SI<br />

Statistical index<br />

SWF<br />

Statistical weighting factor<br />

WF<br />

Weighting factor<br />

CF<br />

Certainty Factor.<br />

SI_M1 Statistical index model 1<br />

SI_M2 Statistical index model 2<br />

SI_M3 Statistical index model 3<br />

WF_1 Weighting factor model 1<br />

WF_2 Weighting factor model 2<br />

WF_3 Weighting factor model 3<br />

CF_1<br />

Certainty Factor.<br />

CF_2<br />

Certainty Factor.<br />

CF_3<br />

Certainty Factor.<br />

LS_1 L<strong>and</strong>slide susceptibility model 1<br />

LS_2 L<strong>and</strong>slide susceptibility model 2<br />

LS_3 L<strong>and</strong>slide susceptibility model 3<br />

LSS<br />

L<strong>and</strong>slide susceptibility<br />

FAO<br />

Food <strong>and</strong> Agricultural organization<br />

A<br />

Total area of the entire map<br />

A* Total area of l<strong>and</strong>slides in the entire map.<br />

Aij Area of l<strong>and</strong>slides in a certain class i of parameter j.<br />

CFij Certainty factor given to a certain class i of parameter j.<br />

DEM<br />

Digital Elevation Model.<br />

f<br />

The l<strong>and</strong>slide density within the entire map.<br />

Vs<br />

Versus<br />

a.m.s.l<br />

Above sea level<br />

npix<br />

Number of pixels<br />

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Chapter 1: Introduction<br />

Natural hazards are inherent in mountain environments. Of these, l<strong>and</strong>slides probably<br />

constitute the most common <strong>and</strong> dreaded hazard for mountain society everywhere. A<br />

l<strong>and</strong>slide is defined as the movement of a mass of rock, earth, or debris down a slope. Bates<br />

& Jackson (1987) defined a l<strong>and</strong>slide as the downslope transport under gravitational influence<br />

of soil <strong>and</strong> rock material. Usually the displaced material moves over relatively confined zone<br />

or surface of shear.<br />

Destructions caused by catastrophic l<strong>and</strong>slides are a worldwide phenomenon, <strong>and</strong> the rapid<br />

increase of population during this century has augmented the problem. Varnes (1981) reported<br />

that, during the period from 1971-1974 an average of nearly 600 people per year, worldwide,<br />

were killed by l<strong>and</strong>slides.<br />

Rainfall triggered l<strong>and</strong>slides are common problems in many areas of the hilly <strong>and</strong><br />

mountainous regions of the highl<strong>and</strong>s of Ethiopia. Gezahegn (1998), Ayalew (1999),<br />

Temesgen et al. (2001), Nyssen et al. (2002), Ayalew & Yamagishi (2004), Ayenew &<br />

Barbieri (2004), Woldearegay et al. (2004) indicate l<strong>and</strong>slides in these terrains have been<br />

affecting human lives, infrastructures, agricultural l<strong>and</strong>s <strong>and</strong> the natural environment.<br />

Although l<strong>and</strong>slides have been observed for at least the last three decades, in more recent<br />

times the sensitivity of both the public <strong>and</strong> administrative bodies to these events has increased<br />

as more <strong>and</strong> more people are now living in the areas affected. Indeed, l<strong>and</strong>slides or l<strong>and</strong>slidegenerated<br />

problems have claimed about 300 lives, damaged over 100 km of asphalt road,<br />

demolished more than 200 dwelling houses <strong>and</strong> devastated in excess of 500 ha of l<strong>and</strong> in<br />

Ethiopia in the years 1991-1998 (Ayalew, 1999). Despite this, however, the causes <strong>and</strong><br />

mechanisms of slope failures remain poorly understood <strong>and</strong> so far, little effort has been made<br />

to reduce losses from l<strong>and</strong>slides <strong>and</strong> l<strong>and</strong>slide-generated hazards.<br />

Although it could be said that the occurrence or non-occurrence of l<strong>and</strong>slides depend mainly<br />

on natural causes <strong>and</strong> factors, such as geological <strong>and</strong> geo-hydrological characteristics of any<br />

locality, exogenous factors such as intense precipitation over a short time interval <strong>and</strong><br />

earthquakes also trigger <strong>and</strong> accelerate l<strong>and</strong>slides. Similarly, growing human <strong>and</strong> animal<br />

populations in mountainous regions create other imbalances such as deforestation <strong>and</strong><br />

encroachment on steep slopes. Construction activities have also a positive contribution to<br />

slope instabilities. Hence the complexity of these causes increases due to natural <strong>and</strong> human<br />

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Chapter 1: Introduction 2<br />

factors. And along with these, the human <strong>and</strong> economic consequences of such incidents are<br />

becoming more damaging, adding to the miseries of people who are already in the grip of<br />

poverty.<br />

1.1 Objectives of the study<br />

Most l<strong>and</strong>slide studies in Ethiopia are confined to either individual cases or the hazard prone<br />

sectors of linear infrastructures. In this paper, a systematic study of l<strong>and</strong>slides, including<br />

hazard mapping <strong>and</strong> risk assessment on a larger scale is intended to be carried out. The main<br />

focus is to assess the stability of slopes from geomorphological, geological <strong>and</strong> geotechnical<br />

point of views. Therefore, we will deal with:<br />

‣ Compiling a l<strong>and</strong>slide inventory for the study area<br />

‣ Factor of safety calculations <strong>and</strong> hazard assessment using infinite slope model<br />

‣ L<strong>and</strong>slide hazard mapping using four statistical approaches i.e. statistical index,<br />

statistical weighting factor, certainty factor <strong>and</strong> l<strong>and</strong>slide susceptibility analysis. In<br />

addition, three different causative factor combinations will be dealt for each of these<br />

methods.<br />

‣ A comparison between the results of the employed methodologies <strong>and</strong> the inventory.<br />

‣ A comparison between the accuracies of the models.<br />

‣ Selection of a suitable physically based scenario <strong>and</strong> statistical model.<br />

‣ Matching between statistical model outputs.<br />

‣ Matching between the selected deterministic <strong>and</strong> statistical outputs.<br />

‣ Selection of the final representative hazard map.<br />

‣ Identifying the responsible triggering factors.<br />

1.2 Study Area<br />

The study area of this research is located in Dogua’s Tembien district, Tigray, Ethiopia. It<br />

encompasses about 497 km² area within the geographic boundaries: 13°34’20’’N to<br />

13°44’44’’N latitude <strong>and</strong> 39°05’29’’E to 39°18’58’’E longitude. The altitude ranges between<br />

1370 <strong>and</strong> 2835 m a.m.s.l. The region has an average annual rainfall of 750 mm showing a<br />

bimodal distribution with a first minor peak from March to May, <strong>and</strong> a second major peak<br />

(i.e. 80% of the annual rainfall) from June to September. Daily air temperature is explained by<br />

large variations, from 5°C to 28°C (Nyssen et al., 2005).<br />

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This area, located in the Geba <strong>and</strong> Werei river catchments, was selected because the highest<br />

points reveal the most complete geological section of the region, <strong>and</strong> because of the<br />

availability of data as several studies have been carried out there (Nyssen et al., 2000;<br />

Gebremichael et al., 2005; Descheemaeker et al., 2006; Moeyersons et al., 2008; Van Den<br />

Eeckhaut et al., 2009). Figure 1.1 shows the location of the study area.<br />

Figure 1.1 Location map of the study area<br />

1.3 Outline of the thesis<br />

Chapter 2 presents a brief review of literatures based on factors triggering<br />

l<strong>and</strong>slides, l<strong>and</strong>slide inventory, Anticipation of l<strong>and</strong>slides <strong>and</strong> <strong>GIS</strong> methods.<br />

In chapter 3, methodology <strong>and</strong> data preparation will be discussed. Available data<br />

will be used to generate causative factor maps. Moreover, a l<strong>and</strong>slide inventory<br />

will be compiled.<br />

Chapter 4 focuses on deterministic approach of analyzing slopes. Critical<br />

engineering depth <strong>and</strong> factor of safety maps will be prepared for three steady state<br />

conditions. In the same way, a combined factor of safety map will be generated.<br />

The accuracy of the models will be cross validated by using the inventory.<br />

Statistical methods will be discussed in chapter 5. A total of 12 models will be<br />

constructed on the basis of the causative link between l<strong>and</strong>slides <strong>and</strong> triggering<br />

factors.<br />

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Chapter 1: Introduction 4<br />

The model outputs will be checked against the inventory to test the prediction<br />

capacity of the methods.<br />

A comparison of the model outputs, a conclusion on the best prediction <strong>and</strong><br />

identification of the responsible triggering factors will be made in chapter 6.<br />

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Chapter 2: Literature review<br />

Instability related issues in engineered as well as natural slopes are the common challenges to<br />

both researchers <strong>and</strong> professionals. In construction areas, instability may result due to rainfall,<br />

increase in groundwater table or change in stress conditions. Similarly, natural slopes that<br />

have been stable for many years may suddenly fail in response to changes in geometry,<br />

external forces or loss in shear strength (Abramson et al., 2002). According to Tayler & Burns<br />

(2005), earthquakes can be considered as the greatest threats to the long‐term stability of<br />

slopes in earthquake active zones. Moreover, the long‐term stability is associated with<br />

weathering <strong>and</strong> chemical influences that may decrease the shear strength <strong>and</strong> create tension<br />

cracks. In such circumstances, therefore, the evaluation of slope stability conditions becomes<br />

a primary concern (Prasad, 2006).<br />

2.1 Factors influencing slope stability<br />

The varied topographic features of the earth’s surface are possible only because the shear<br />

strength of the soil exceeds shearing stresses imposed by gravity or other loadings. <strong>Slope</strong><br />

failure not only can occur in the steepest slope but sometimes occur in relatively flat slopes.<br />

Factors leading to instability can generally be classified based on the effect they have on<br />

slopes (Varnes, 1984; Yokota & Iwamatsu, 1999; Chigira, 2002).<br />

2.1.1 Gravity<br />

The main force responsible for mass wasting is gravity. Gravity is the force that acts<br />

everywhere on the Earth's surface, pulling everything in a direction toward the center of the<br />

earth. On a slope, the force of gravity can be resolved into two components: a component<br />

acting perpendicular to the slope <strong>and</strong> component acting tangential to the slope. On a steeper<br />

slope, the shear stress or tangential component of gravity increases <strong>and</strong> the perpendicular<br />

component of gravity decreases. Therefore, the down-slope movement of a material is favored<br />

by steep slope angles which increase the shear stress, <strong>and</strong> anything that reduces the shear<br />

strength, such as lowering the cohesion among the particles or lowering the frictional<br />

resistance.<br />

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Chapter 2: Literature review 6<br />

2.1.2 The effect of water<br />

Dry unconsolidated grains will form a pile with a slope angle determined by the angle<br />

of repose. The angle of repose is the steepest angle at which a pile of unconsolidated<br />

grains remains stable, <strong>and</strong> is controlled by the frictional contact between the grains. In<br />

general, for dry materials the angle of repose increases with increasing grain size, but<br />

usually lies between about 30 <strong>and</strong> 37 o (Upreti & Dhital, 1996).<br />

Slightly wet unconsolidated materials exhibit a very high angle of repose because<br />

surface tension between the water <strong>and</strong> the solid grains tends to hold the grains in place.<br />

When the material becomes saturated with water, the angle of repose is reduced to<br />

very small values <strong>and</strong> the material tends to flow like a fluid. This is because the water<br />

gets between the grains <strong>and</strong> eliminates grain to grain frictional contacts.<br />

Another aspect of water that affects slope stability is pore water pressure. In some cases fluid<br />

pressure can be built in such a way that water can support the weight of the overlying<br />

rock/soil mass. When this occurs, friction is reduced, <strong>and</strong> thus the shear strength holding the<br />

material on the slope is also reduced, resulting in slope failure. Pore water pressure built up<br />

within a regolith is directly related to the increase in groundwater table. Presumably, such<br />

actions are also controlled by subsurface flow parameters i.e. precipitation, soil physical<br />

properties <strong>and</strong> infiltration capacity. The dynamic conditions of pore water pressure built up<br />

during different storm events are directly related to l<strong>and</strong>slide initiations (O’Loughlin &<br />

Pearce, 1982; Sidle & Swanston, 1982; Sidle, 1984).<br />

2.1.3 Geological factors<br />

Translational/rotational slides generally occur in relatively cohesive, homogeneous soils <strong>and</strong><br />

rocks. L<strong>and</strong>slide events are strongly controlled by the nature of the regolith material<br />

(Thomson, 1971; Sawnston, 1978; Yokota & Iwamatsu, 1999; Wakatsuki et al., 2005).<br />

Failure commonly occurs along bedrock bedding planes that are deep-seated <strong>and</strong> dip in the<br />

same direction as the slope surface. In saturated conditions, incompetent material may fail<br />

under overburden weight <strong>and</strong> high pore pressures, resulting in a deep-seated rotational-type<br />

failure. Translational slides commonly are controlled structurally by surfaces of weakness<br />

such as faults, joints, bedding planes, <strong>and</strong> contacts between bedrock <strong>and</strong> overlying deposits<br />

(Sidle & Ochiai, 2006). Generally slope stability is influenced by the following geological<br />

factors:<br />

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Chapter 2: Literature review 7<br />

‣ Type <strong>and</strong> engineering-geological properties of soils/rocks, their distribution, <strong>and</strong> the<br />

effect of groundwater on these properties<br />

‣ Geological structures such as cleavage, joints, faults <strong>and</strong> folds<br />

‣ Stresses in geological history<br />

Engineering-geological properties<br />

Lithological units, such as basalts, shales, s<strong>and</strong>stones <strong>and</strong> limestones have different shear<br />

strength characteristics because of the varying conditions under which they are formed. They<br />

also have different mineral constituents <strong>and</strong> fabrics. Therefore, they undergo different changes<br />

in strength on remolding i.e. sensitivity (Malik, 1996; Upreti & Dhital, 1996).<br />

Geological structures<br />

Geological structures, such as bedding, joints, foliation, cleavage, schistosity, <strong>and</strong> faults are<br />

potentially weak planes in a slope. Their strength is generally less than in the surrounding<br />

intact rock. It is therefore imperative to know their orientation in relation to slope angle,<br />

direction, <strong>and</strong> strength along such potential weak planes (Sidle & Ochiai, 2006).<br />

Stresses in geological history<br />

In addition to the geological structure <strong>and</strong> lithology, weathering plays an important role.<br />

Mechanical <strong>and</strong> chemical weatherings change the strength parameters of the rock <strong>and</strong> soil<br />

considerably. In many l<strong>and</strong>slide events, chemical alterations, such as hydration <strong>and</strong> ion<br />

exchange in clay, are thought to have contributed to triggering l<strong>and</strong>slides (Zaruba & Mencl,<br />

1982). Geological history is also an important factor in determining the response of materials<br />

to excavation or l<strong>and</strong>slides. In over consolidated materials, stresses stored may not have been<br />

completely released at the time of slope formation <strong>and</strong> this result in an outward movement at<br />

the base of the slopes (Tianchi, 1990; Deoja et al., 1991; Chalise & Karki; 1995, Malik,<br />

1996).<br />

2.1.4 Soil Properties<br />

Both the hydraulic properties <strong>and</strong> the shear strength behaviors of soils can affect the stability<br />

of a slope with or without a rainstorm. Another attributed effect is the presence of soils that<br />

contain a high proportion of a type of clay mineral called smectites or montmorillinites.<br />

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Chapter 2: Literature review 8<br />

Such clay minerals exp<strong>and</strong> when they become wet as water enters the crystal structure <strong>and</strong><br />

increases the volume of the mineral. When such clays dry out, the loss of water causes the<br />

volume to decrease <strong>and</strong> the clays to shrink or compact. Failure is attributed with pore water<br />

pressure built up on such soils.<br />

2.1.5 The effect of vegetation<br />

It is well understood that vegetation influences slope stability in two ways: through<br />

hydrological effects <strong>and</strong> mechanical effects. Hydrological effects involve the removal of soil<br />

water by evapotranspiration through vegetation, which lead to an increase in soil suction or a<br />

reduction in pore-water pressure, hence, an increase in the soil shear strength. The shear<br />

strength of the soil is also increased through the mechanical effects of the plant root matrix<br />

system (Greenway, 1987; Anju, 2005).<br />

2.1.6 Triggering events<br />

A mass-wasting event can occur any time a slope becomes unstable. Sometimes, as in the case<br />

of creep or solifluction, the slope is always unstable <strong>and</strong> the process is continuous. On the<br />

other h<strong>and</strong>, triggering events can happen that cause a sudden instability. The triggering<br />

mechanisms could be shocks <strong>and</strong> earthquakes (Keefer, 2002), slope modification,<br />

undercutting or changes in hydraulic characteristics (De. Vleeschauwer & De Smedt, 2002).<br />

Table 2.1 Triggering events influencing slope stability<br />

Increased stresses<br />

1. External loads such as buildings,<br />

roads, etc<br />

Decreased Strength<br />

1. Swelling of clays by adsorption of<br />

water.<br />

2. Increase in unit weight by<br />

increased in moisture content.<br />

3. Removal of part of slope by<br />

excavation.<br />

4. Undermining caused by tunneling,<br />

collapse of underground caverns, or<br />

seepage erosion.<br />

5. Shock caused by earthquake or<br />

blasting.<br />

6. Tension cracks.<br />

2. Pore water pressure.<br />

3. Breakdown of loose or<br />

honeycombed structure of soil with<br />

shock, vibration or seismic activity.<br />

4. Hair cracking from alternate<br />

swelling <strong>and</strong> shrinking or from<br />

tension.<br />

5. Strain <strong>and</strong> progressive failure in<br />

sensitive soils<br />

6. Deterioration of cementing<br />

material.<br />

7. Water pressure in cracks. 7. Loss of capillary tension on drying<br />

8. Weathering – chemical or biochemical<br />

deterioration.<br />

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2.2 L<strong>and</strong>slide inventory<br />

A clear underst<strong>and</strong>ing of l<strong>and</strong>slide conditions <strong>and</strong> a more detailed assessment of the l<strong>and</strong>slide<br />

hazard of the area concerned are essential to make a systematic l<strong>and</strong>slide inventory. All<br />

failures recorded in historical <strong>and</strong> technical documents, investigated <strong>and</strong> identified or by aerial<br />

photographic analysis, should be registered. Compiling the locations <strong>and</strong> conditions of<br />

existing l<strong>and</strong>slide zones is the basic requirement before performing any slope stability<br />

analysis (Van Westen, 1993; Van Westen et al., 2006). A l<strong>and</strong>slide is a natural geologicgeomorphologic<br />

phenomenon in which the soil <strong>and</strong>/or rock mass resting on top of a sliding<br />

surface starts to slowly or rapidly move downslope because of the pull of gravity. By the time<br />

the l<strong>and</strong>slide activity ceases, a specific topography associated with the l<strong>and</strong>slides will be<br />

formed. A l<strong>and</strong>slide inventory is, therefore, carried out to identify the newly formed<br />

topographic feature. The analysis of aerial photography is a quick <strong>and</strong> valuable technique for<br />

identifying l<strong>and</strong>slides, because it provides a three-dimensional overview of the terrain <strong>and</strong><br />

indicates human activities. Generally aerial photographs are used to identify specific<br />

geomorphic features that reflect l<strong>and</strong>slide topography. Important geomorphic features are<br />

those associated with the failure of large, deep-seated l<strong>and</strong>slides involving bedrock <strong>and</strong> thick<br />

soil as well as large rockslide <strong>and</strong> rockfall deposits. Tianchi et al. (2001) <strong>and</strong> Dikau et al.<br />

(1996) explain the geomorphic features that can be used as indicators of l<strong>and</strong>sliding on<br />

stereoscopic pairs of aerial photographs.<br />

Steep crescent-shaped surface that is concave down slope, minor scarps, grabens, fault<br />

blocks <strong>and</strong> trees that lean uphill describe l<strong>and</strong>forms in the head region of l<strong>and</strong>slides.<br />

Relatively flat hillside areas, circular or oval hillside ponds, hillside terrain with<br />

transverse ridges <strong>and</strong> secondary scraps indicate interior body of a l<strong>and</strong>slide.<br />

Crescent –shaped ridge that is convex down slope, trees that lean downhill or at<br />

various angles depict the foot region <strong>and</strong> zone of earth flow.<br />

Sometimes, l<strong>and</strong>slide features are not easily recognized due to vegetation cover, alteration of<br />

the terrain by human activities, or surface erosion that modifies l<strong>and</strong>slide features. The<br />

advantages of preparing inventories by interpreting aerial photographs <strong>and</strong> field examination<br />

are, (1) It is rather quick <strong>and</strong> inexpensive, (2) It shows where l<strong>and</strong>slide processes seem to be<br />

concentrated, <strong>and</strong> correspondingly, it shows where more detailed studies are likely to be<br />

undertaken in the future (Tianchi et al., 2001).<br />

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2.3 Anticipation of l<strong>and</strong>slide hazards<br />

The three types of l<strong>and</strong>slide hazard assessment studies important to planners, engineers <strong>and</strong><br />

the public are:<br />

‣ Long term predictions: It is used to delineate areas that might have hazards caused by<br />

l<strong>and</strong>slides for the purpose of l<strong>and</strong> use planning, regional hazard assessment <strong>and</strong><br />

preventation, urban development, <strong>and</strong> evaluation of environmental changes after<br />

deforestation. One important principle of the long-term prediction is that the past is the<br />

key to the future. This means that l<strong>and</strong>slides will probably occur as a result of the<br />

same geologic, geomorphic, <strong>and</strong> hydrologic situations that led to past <strong>and</strong> current<br />

l<strong>and</strong>slides. Based on this assumption, it is possible to estimate the type, frequency <strong>and</strong><br />

occurrences of l<strong>and</strong>slides in a study area. Making such a prediction involves carrying<br />

out geologic <strong>and</strong> geomorphic studies <strong>and</strong> aerial photo interpretation. It means, it<br />

consists of preparing regional, or reconnaissance l<strong>and</strong>slide maps, such as inventory<br />

maps, l<strong>and</strong>slide hazard maps <strong>and</strong> susceptibility maps that identify <strong>and</strong> delineate<br />

regional l<strong>and</strong>slide problem areas <strong>and</strong> conditions in which they occur. These maps can<br />

also be used to predict the relative degree of hazard in a l<strong>and</strong>slide area (Tianchi, 1990;<br />

Deoja et al., 1991; Chalise & Karki, 1995).<br />

‣ Geotechnical methods: These methods are used to quantitatively asses slope stability<br />

under man-made conditions such as changes in topography, hydrologic conditions. In<br />

addition, those methods are employed to analyze old l<strong>and</strong>slides under anticipated<br />

seismic or meteorologic conditions. When making such computations, it is important<br />

in all aspects of the study, including geologic definitions, to underst<strong>and</strong> the<br />

relationship between the subsurface geometry <strong>and</strong> strength parameters of the slide<br />

plane with natural conditions. Due to high cost, this method can only be applied to<br />

those slopes on which large risks are expected according to the long term conditions,<br />

or on which economically important engineering operations are being carried out. The<br />

basic characteristics of these models are based on different mathematical <strong>and</strong> physical<br />

models (Malik, 1996; Thakur, 1996; Upreti & Dhital, 1996).<br />

‣ Short term predictions: Such predictions are used for evacuation before an imminent<br />

large scale l<strong>and</strong>slide. They are based on (1) field measurements of displacements,<br />

rainfall <strong>and</strong> pore water pressures (2) forerunning indicators of l<strong>and</strong>slides (Tianchi,<br />

1990; Deoja et al., 1991; Chalise & Karki, 1995; Malik, 1996).<br />

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2.4 <strong>GIS</strong> methods<br />

The recent development of <strong>GIS</strong> technology for data integration, combined with the<br />

availability of digital elevation models of acceptable quality to analyze geographic <strong>and</strong><br />

geologic data, has greatly increased the applicability of many techniques for l<strong>and</strong>slide hazard<br />

assessment (Brabb, 1984; Varnes, 1984; Van Westen, 1994; Carrara et al., 1995). Most of the<br />

conventional <strong>GIS</strong> techniques for l<strong>and</strong>slide mapping are based on ‘map overlaying’, which<br />

only allows for the comparison of different maps on the same location <strong>and</strong> scale by placing<br />

them one on top of the other <strong>and</strong> using the criteria for l<strong>and</strong>slide assessment. Such techniques<br />

for modeling slope instability have been employed by different investigators. Reviews<br />

outlining the methods are given by, Hansen (1984), Carrara et al. (1995), Hutchinson (1995),<br />

Soeters <strong>and</strong> Van Westen (1996), Van Westen et al. (1997), Long (2008). The methods for<br />

ranking slope instability factors <strong>and</strong> assigning different susceptibility levels can be divided<br />

into:<br />

‣ Qualitative or quantitative: Qualitative methods are subjective. They establish<br />

susceptibility heuristically, <strong>and</strong> portray susceptibility levels using descriptive<br />

(qualitative) expressions. Such techniques depend highly on experience, knowledge<br />

<strong>and</strong> previous works on the study area. It is based on how well <strong>and</strong> how much the<br />

investigator underst<strong>and</strong>s the geomorphological processes acting upon the terrain. On<br />

the contrary, Quantitative methods produce numerical estimates, i.e. probabilities of<br />

the occurrence of l<strong>and</strong>slide incident in any susceptibility zone (Guzzetti et al., 2005).<br />

‣ Direct mapping methods are those that recognize the spatial distribution of l<strong>and</strong>slides<br />

directly from existing failure zones or using specific knowledge of areas of potential<br />

instability. A direct method consists of geomorphological mapping of l<strong>and</strong>slide<br />

susceptibility in the field, using aerial photographs or from satellite images<br />

(Verstappen, 1983; Nossin, 1989). It still relies on the ability of the investigator to<br />

estimate actual <strong>and</strong> potential slope failures. Indirect mapping techniques are those that<br />

employ causative relationship based on possible triggering factors to estimate<br />

potential instability. Indirect methods for l<strong>and</strong>slide susceptibility assessment are<br />

essentially stepwise. Guzzetti et al. (2005) determined the requirements of Indirect<br />

methods as:<br />

Recognition <strong>and</strong> mapping of l<strong>and</strong>slides over a target region or a subset of it<br />

(i.e. the training area), which is obtained by preparing a l<strong>and</strong>slide inventory<br />

map.<br />

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Chapter 2: Literature review 12<br />

<br />

Identification <strong>and</strong> mapping of the physical factors which are directly or<br />

indirectly correlated with slope instability (the triggering factors).<br />

<br />

An estimate of the relative contribution of the triggering factors in generating<br />

slope failures.<br />

<br />

Classification of the l<strong>and</strong> surfaces into domains of different levels of<br />

susceptibility.<br />

<br />

Assessment of the model performance (validation).<br />

Table 2.2 Characteristics of l<strong>and</strong>slide susceptibility methods proposed by Van Westen et al. (1997a)<br />

Direct Indirect<br />

Qualitative Quantitative<br />

Geomorphological mapping <br />

Heuristic (index-based) <br />

<strong>Analysis</strong> of inventories <br />

Statistical modeling <br />

Process based (conceptual) <br />

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Chapter 3: Methodology <strong>and</strong> data preparation<br />

3.1 L<strong>and</strong>slide Inventory mapping<br />

L<strong>and</strong>slide inventory maps show locations <strong>and</strong> characteristics of l<strong>and</strong>slides that have moved in<br />

the past but generally do not indicate the mechanism(s) that triggered them. The geologic,<br />

topographic <strong>and</strong> climatic conditions that led to past slope failures often provide clues to the<br />

locations <strong>and</strong> conditions of future slope failures. Therefore, inventory maps provide useful<br />

information about the potential for future l<strong>and</strong>sliding. It is the most straightforward initial<br />

approach to any l<strong>and</strong>slide hazard study <strong>and</strong> such inventories are the basis for most<br />

susceptibility mapping techniques (Dai et al., 2002). In addition, recognizing the type <strong>and</strong><br />

recency of l<strong>and</strong>sliding can also facilitate the scope <strong>and</strong> design of site-specific geotechnical<br />

investigations <strong>and</strong> guide slope remediation strategies.<br />

Inventory maps are prepared primarily by geomorphic analysis of aerial photographs <strong>and</strong><br />

secondarily by field reconnaissance, interpretation of topographic map contours <strong>and</strong> review of<br />

previous mappings.<br />

Detailed geomorphological investigations (Nyssen et al., 2002; Moeyersons et al., 2006,<br />

2008) were needed to realize that l<strong>and</strong>slides <strong>and</strong> related mass movement topography occupy<br />

an important part of the l<strong>and</strong>scape in the Hagere Selam area.<br />

Moeyersons et al. (2008) distinguishes several mass movements. The first type is rockfall<br />

produced by detachment <strong>and</strong> toppling during the rainy season from 357 km rocky<br />

escarpments <strong>and</strong> cliffs with a height of more than 10m. The rock fragments tumble, topple<br />

<strong>and</strong> roll down the valley, sometimes to about 100m. A detailed inventory in the study area<br />

indicates that rockfall alone is responsible for a cliff recession rate up to 3.7 cm/century which<br />

is 3.7m³ of rockfall per annum (Nyssen et al., 2006). Three dormant debris flows are also<br />

recognized. The first type includes the preferential mobilizations of the geologic layers resting<br />

over the Amba Aradom s<strong>and</strong>stone, the plateau layers. It includes the lower <strong>and</strong> upper trap<br />

basalt layers, s<strong>and</strong>wiched whitish s<strong>and</strong>y-clayey lacustrine deposits, <strong>and</strong> the expansive clays<br />

obtained from the weathering of the basalts. These l<strong>and</strong>slides dominantly occur below the<br />

tabular extensions of Amba Aradom s<strong>and</strong>stone <strong>and</strong> flow over the cliff <strong>and</strong> descend very far<br />

down in to the valley. Sometimes, these debris flows include detached fragments of the lower<br />

layers, Amba Aradam s<strong>and</strong>stone <strong>and</strong> Antalo limestone.<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 14<br />

The other, rather uncommon, debris flow occurs in the Antalo supersequence. It is attributed<br />

with the presence of massive <strong>and</strong> hard layers which act like aquitards/aquicludes that block<br />

the passage of water to lower layers <strong>and</strong> thus result in pore water pressure built up. Finally,<br />

gigantic debris flows <strong>and</strong> rock slides occur around dolerite dyke ridges resulting in deposition<br />

of fresh dolerite rock boulders over a typical corestone weathering profile (Moeyersons et al.,<br />

2008; Twidale, 1982).<br />

For this study, major geomorphic <strong>and</strong> geologic features are interpreted using aerial<br />

photographs with a scale of 1:50,000 (Ethiopian Mapping Authority, 1994) <strong>and</strong> a<br />

topographical map of Hagere Selam area on a scale of 1:50,000 (Ethiopian Mapping<br />

Authority, 1996). Site investigation results obtained from previous studies, Nyssen et al.<br />

(2002, 2006), Moeyersons et al. (2006, 2008) are thoroughly assessed. Digital photographs<br />

obtained from the metadata of the Royal Central Africa museum are exploited to build the<br />

relationship between the recognized features of the aerial photographs with the reality.<br />

The aerial photographs which were used for this study are ETH94:R2/26 +0789, +0790,<br />

+0791, ETH94:R2/27 +0826, +0827, +0828, +0829, +0830, <strong>and</strong> ETH94:R3/28 +0864, +0865,<br />

+0866, +0867.<br />

Moeyersons et al. (2008) identified 28 debris flows, 7 l<strong>and</strong>slide belts, 6 debris <strong>and</strong> rock slides,<br />

5 l<strong>and</strong>slides in the Antalo supersequence <strong>and</strong> 10 l<strong>and</strong>slides in Imba Degua <strong>and</strong> Chini ridges.<br />

In this study, according to the interpretation, we produced a l<strong>and</strong>slide inventory map<br />

consisting of cliffs associated with rock falls <strong>and</strong> l<strong>and</strong>slides zones (debris flows, debris slides,<br />

rock slides <strong>and</strong> slumps).<br />

We identified 30 debris flows, 7 l<strong>and</strong>slide belts, 4 l<strong>and</strong>slides in the Antalo supersequence, 12<br />

l<strong>and</strong>slides in Imba Degua <strong>and</strong> Chini ridges <strong>and</strong> 2 slumps. However, the debris slides <strong>and</strong> small<br />

rock slides observed by Moeyersons et al. (2008) are too small to be recognized by the aerial<br />

photographs.<br />

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Figure 3.1 L<strong>and</strong>slide Inventory map<br />

Details on the slides are shown in Figure 3.2. (A) l<strong>and</strong>slide in Tsilli ridge, (B) May Antebteb debris flow, (C) L<strong>and</strong>slide belt around<br />

Medayk ridge, (D) Melka Maryam debris flow, <strong>and</strong> (E) Upper Tankwa river valley (Tsatsen ridge)<br />

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Figure 3.2 Photographic views of some slides (Source: Online database of Royal Central<br />

Africa museum <strong>and</strong> Moeyersons et al., 2008)<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 17<br />

3.1.1 Mechanism of failures<br />

A. Debris flow affecting plateau layers<br />

Figure 3.3 L<strong>and</strong>slide mechanism 1 (Source: Moeyersons et al., 2008)<br />

Geologic layers resting over Amba Aradom s<strong>and</strong>stone which are the Upper basaltic layer, the<br />

whitish s<strong>and</strong>y clay lacustrine deposit, the lower basaltic series <strong>and</strong> the weathering product of<br />

the basalts i.e. swelling clays start flowing as a massive surge from a nearly horizontal Amba<br />

Aradom structural surface <strong>and</strong> descend down the valleys. Amba Aradom s<strong>and</strong>stone is an<br />

aquicludes/ aquitard which could sufficiently block the passage of water (Tesfaye <strong>and</strong><br />

Gebretsadik, 1982). The increase in water content of the upper layers can mobilize the<br />

l<strong>and</strong>slides in two ways: (1) By destroying the natural anchorage between particles <strong>and</strong><br />

decreasing the shear strength of the materials (2) By developing pore water pressure <strong>and</strong><br />

increasing the shear stress acting on the plateau layers. The above Figure indicates that the<br />

flows are sometimes mixed with detached fragments of Antalo limestone <strong>and</strong> Amba Aradom<br />

s<strong>and</strong>stone.<br />

B. L<strong>and</strong>slides affecting the Antalo supersequence.<br />

Most l<strong>and</strong>slide failures in Ethiopia are rainfall triggered. The l<strong>and</strong>slides affecting Antalo<br />

limestone are also related with pore water pressure built up above massive/ hard layers acting<br />

as an aquicludes or aquitard. Figure 3.4 shows the mechanism by which failure occurs.<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 18<br />

Figure 3.4 L<strong>and</strong>slide mechanism 2<br />

The first massive formation recognized as an aquitard or aquiclude is the Adiwerat layer (Van<br />

de Wauw et al., 2008). It is a massive shale layer on the top of which l<strong>and</strong>slides of Agula<br />

shale would be mobilized. Following these movements the cliffs resting over the Agula shale<br />

will start sliding. Thus, these flows are characterized with s<strong>and</strong>stone <strong>and</strong> basalt inclusions<br />

(Van de Wauw et al., 2008). The second aquitard is the upper shale or marl layer which is also<br />

called May Ba’ati aquitard (Moeyersons et al., 2008). It has a low small hydraulic<br />

conductivity <strong>and</strong> water can hardly move to lower layers. However, the carbonate layer resting<br />

over the shale, Storamatoporoid bed, has a considerable vertically permeability resulting from<br />

cracks. Thus water is allowed to st<strong>and</strong> in the cracks. When the water table is increased to a<br />

level higher than the Storamatoporoid layer, pore water pressure will be built up in the upper<br />

Anatalo limestone <strong>and</strong> will mobilize the l<strong>and</strong>slides. The third aquitard is the lower shale/ marl<br />

layer under carbonate cliffs of stromatoporoid layer. The mechanism of failure is similar to<br />

what is explained for the upper series.<br />

C. L<strong>and</strong>slides around Imba Degua <strong>and</strong> chini<br />

The geologic composition of the Imba Degua <strong>and</strong> Chini ridge is quite different from what has<br />

been observed in the rest of the study area. Most part of the ridge is composed of dolerites.<br />

Unlike other places, the l<strong>and</strong>slides around this ridge are not characterized by structural<br />

topography but are composed of fresh dolerite boulders resting over corestone weathering<br />

profiles. These slides are huge enough that the lobes are clearly identified by aerial<br />

photographs. However, field observations reveal that the area is not characterized by rugged<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 19<br />

topography (Moeyersons et al., 2008). The l<strong>and</strong>slide depletion areas are not completely<br />

identifiable with aerial photograph interpretation. Some erosional belts visibly start from the<br />

steepest parts of the ridges while other lack morphological justification to delineate the zones.<br />

However, Moeyersons et al. (2008) state a field recognition result with a significant difference<br />

in size <strong>and</strong> freshness of dolerite boulders with the weathering profiles. Thus the erosional<br />

belts are considered to start from the steepest parts of the ridges.<br />

D. Rock falls<br />

A l<strong>and</strong>slide analysis in Hagere Selam area will not be complete without including the effect of<br />

rock falls. The failure mechanism is believed to be detachment <strong>and</strong> toppling of boulders from<br />

rocky cliffs after every rainy season. In addition, a secondary movement of the rocks has to be<br />

considered. Creep effects are not easily realized in short period of time, but are very<br />

devastating as the attachment between the rocks particles will get removed with time. From<br />

1998 to 2001, slopes below Amba Aradom s<strong>and</strong>stone have been investigated twice a year, at<br />

the end of the rainy season <strong>and</strong> mid of the dry season (Nyssen et al., 2006). The investigation<br />

includes identification of down slope scars of damaged vegetation, freshly fallen boulders <strong>and</strong><br />

information of local shepherds. For creep considerations, theodolite measurements have been<br />

collected (Nyssen et al., 2006).<br />

For this study, we identified the cliffs using the topographic map <strong>and</strong> the DEM. It is intended<br />

to apply infinite slope <strong>and</strong> statistical models for the l<strong>and</strong>slide identification. However, the<br />

Mohr – Coulomb criterion cannot be used because of the extremely high cohesion of<br />

consolidated or cemented rocks as compared to soft materials. So, the shear strength<br />

parameters of weathered rocks will be treated. L<strong>and</strong>slides can be detected in cliffs due to<br />

their large slope angles; despite they have very large shear strength. As a first approximation,<br />

the infinite slope analysis will be applied. Alternatively, Statistical models are expected to<br />

yield reliable results to identify rock falls, as their consideration is causative not inherent soil<br />

properties or particular failure plane assumption.<br />

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3.2 Geotechnical parameters<br />

In slope stability analysis, evaluation of variables such as soil stratification <strong>and</strong> in situ shear<br />

strength parameters may prove to be a formidable task especially when the analysis concerns<br />

to be spatial. The inherent soil parameters would be difficult to obtain on a detailed scale in<br />

regional basis. In that instance, grouping of adjacent soil units having homogeneous<br />

properties would be practical. Direct measurement of the parameters would then be made in a<br />

representative number of times for each unit. In case when direct measurements do not exist,<br />

range of literature values could be tried <strong>and</strong> a reasonable decision would be taken. Most of the<br />

time, results of laboratory analysis do not happen to be better than literature values.<br />

There were two possible ways to obtain the geotechnical parameters of the study area: (1)<br />

considering the FAO soil map 1998, (2) considering the lithology. As The FAO soil map<br />

1998 on the study area is compiled with a large scale <strong>and</strong> would give a rough approximation,<br />

it is concluded to use the lithology as the base for major soil properties. The areal distribution<br />

of the geologic formations is shown in Figure 3.5.<br />

Entcho S<strong>and</strong>stone<br />

Endaga Arbi Glacial<br />

Alluvium<br />

Adigrat S<strong>and</strong>stone<br />

Marl Limestone<br />

Shale Marl Limestone<br />

Dolerite Sill<br />

Shale<br />

Amba Aradom S<strong>and</strong>stone<br />

Limestone Marl<br />

Trap basalt<br />

Areal distribution of geologic layers(%)<br />

0 5 10 15 20 25<br />

Figure 3.5 Areal distribution of geologic layers<br />

The geologic properties of these formations are described, in short, here below:<br />

1. Trap basalts: are represented by dark colored, fine to coarse grained, basic igneous<br />

rocks that are associated with soft sediments (volcanic ash <strong>and</strong>/or lacustrine deposits)<br />

as discontinuous interbeds.<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 21<br />

2. Horizontal/sub-horizontal flow structures form rock sequences of variable<br />

characteristics which range from well developed columnar joints to less fractured <strong>and</strong><br />

massive layers. The majority of soils derived from basalt flows are grouped into CH,<br />

inorganic clays of high plasticity, SC-clayey s<strong>and</strong>, <strong>and</strong> MH-inorganic silts<br />

(Woldaregay et al., 2006).<br />

3. Antalo limestone: It is represented by yellow to white, slightly to moderately jointed<br />

limestone with intercalations of calcareous clay (Marl). Limestone to marl ratio is not<br />

constant throughout the area. The marl interbedding is greatest at escarpments,<br />

decreasing considerably both to the east <strong>and</strong> west.<br />

4. Amba Aradom s<strong>and</strong>stone: It is characterized by fine to medium grained, white to pink<br />

colored, thickly bedded, slightly to moderately weathered s<strong>and</strong>stone, which is<br />

interbedded with thin layers of siltstone/ claystone. Vertical/sub-vertical joints <strong>and</strong><br />

horizontal/sub horizontal bedding planes are characteristic of these rocks.<br />

5. Agula shale: is dominated by gray, green <strong>and</strong> black, thinly bedded, moderately to<br />

highly weathered shale (marly), which is interlaminated with thin limestone beds.<br />

Soils derived from Agula shale range from CH, inorganic clays of high plasticity, to<br />

ML, inorganic silts <strong>and</strong> very fine s<strong>and</strong>s with slight plasticity.<br />

6. Dolerites (resting on a typical corestone weathering profile): These rocks include a<br />

variety of intrusive bodies which form isolated peaks <strong>and</strong> ridges. In steep terrains they<br />

are affected by vertical/sub-vertical tensional fractures (Twidale, 1982).<br />

7. Adigrat s<strong>and</strong>stone: Is a medium to coarse grained cliff forming s<strong>and</strong>stone with some<br />

shale <strong>and</strong> laterite intercalations. It is characterized by red to brown, slightly to<br />

moderately weathered, horizontally bedded, jointed s<strong>and</strong>stone. These rocks are<br />

associated with vertical/ sub-vertical joints <strong>and</strong> horizontal/sub horizontal bedding<br />

planes. In many cases s<strong>and</strong>stone cliffs are associated with open tensional fractures<br />

(Woldaregay et al., 2006).<br />

8. Alluvium: are unconsolidated deposits overlying the different rocks.<br />

9. Edaga Arbi glacial: The glacial are mainly composed of clay <strong>and</strong> silt <strong>and</strong> act like an<br />

aquicludes.<br />

10. Enticho s<strong>and</strong>stone: It is a white fine to medium grained s<strong>and</strong>stone with calcareous,<br />

locally siliceous, cement which is leached at the surface. The s<strong>and</strong>stone shows<br />

variations in grain size, sorting <strong>and</strong> degree of cementation. It contains clay <strong>and</strong> lithic<br />

materials.<br />

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The lower part of the s<strong>and</strong>stone is massive while the upper is cross-bedded (Tesfaye &<br />

Gebretsadik, 1982).<br />

Nyssen et al. (2002) explain the shear strength measurements conducted in the laboratory,<br />

using a manual monoaxial shear strength measuring device (M&O, Montrouge, France).<br />

Disturbed soil samples taken from toe <strong>and</strong> sides of the lobes are first saturated with water <strong>and</strong><br />

then consolidated under a normal pressure of 59 kN/ m² in an attempt to simulate a soil depth<br />

of +3 m, which is similar to the thickness of the May Ntebteb flow where it leaves the Amba<br />

Aradam s<strong>and</strong>stone cliff. Water is allowed to be absorbed by the soil samples till field capacity<br />

was reached in equilibrium with the attained state of consolidation. The samples are then<br />

submitted to shear tests at normal stresses of approximately 60, 40, 20 <strong>and</strong> 0 kN/m². Slow<br />

tests with a shear stress increase of 981 N /m² in 3 min have been conducted in order to assure<br />

a drained test<br />

Table 3.1 Shear strength parameters<br />

θ field<br />

Site Composition capacity γ field capacity (kN/m³) Cohesion(kPa) Friction angle(°)<br />

May Ntebteb Swelling clays 0.471 15.77 6.18 24<br />

Amba Raeset Weathered Marl 0.263 17.67 11.58 20<br />

The dry unit weight can be calculated by<br />

γ =<br />

γ<br />

1 + w<br />

(3.1)<br />

Where γ d = dry unit weight<br />

w = water content (weight of water per weight of solid material)<br />

γ = unit weight at a water content of w<br />

Woldearegay et al. (2006) also performed measurements on the shear strength of weathered<br />

Basalt <strong>and</strong> Agula shale. The result is reported in Table 3.2.<br />

Table 3.2 Range of shear strength parameters for weathered formations<br />

Formation Cohesion (kPa) Friction angle (°) γ sat (kN/m³)<br />

Weathered Basalt 5 to 32 16 to 28 17 to 22<br />

Weathered Agula Shale 16 to 37 15 to 27 16 to 23<br />

The analysis of slope stability could not be realistic, if performed on a particular value of<br />

cohesion, friction angle or unit weight.<br />

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Those soil parameters are highly variable with space <strong>and</strong> time. Yet the range of the values<br />

remains, almost, reasonably known. One of the particular capabilities of <strong>GIS</strong> is its ease to<br />

change the parameters <strong>and</strong> check different combinations. Thus this study is intended to be<br />

performed using different values in the range <strong>and</strong> come up with a reasonable approximation.<br />

The parameters for l<strong>and</strong>slide mechanisms 1 <strong>and</strong> 2, described before, are reasonably available.<br />

These flows involve basaltic, marly limestone <strong>and</strong> shale materials. For other formations,<br />

l<strong>and</strong>slides will occur at joints <strong>and</strong> fractured zones. Thus, ranges of strength parameters are<br />

looked for from different literatures. Franklin & Dusseault, (1989), <strong>and</strong> Jaeger & Cook,<br />

(1977) compile friction angle for rock joints <strong>and</strong> fillings. Barton, (1973), <strong>and</strong> Hoek & Bray,<br />

(1977) also give range of friction angle values for residual soils. The values are complied in<br />

Table 3.3. Other literatures also give values related to weathered formations (Sloane, 1991;<br />

Hudson et al., 1997; Hoek et al., 1998; Văn et al., 2001; Kentli & Topal, 2004).<br />

Table 3.3 Friction angle values for rocks at joints<br />

Franklin & Dusseault (1989),<br />

<strong>and</strong> Jaeger & Cook (1977)<br />

Barton (1973), <strong>and</strong> Hoek &<br />

Bray (1977)<br />

Jointed rocks φ' (°) Jointed rocks φ' (°)<br />

Porous limestone 32-48 Basalt 31-38<br />

S<strong>and</strong>stone 24-35 Limestone 33-40<br />

Clay shale 22-37 S<strong>and</strong>stone 25-35<br />

Dolerite 33-43 Shale 27<br />

Another approach for these lithologic layers is to consider the shear strength parameters of<br />

their weathering products, soils derived from the formations. Lambe & Whitman, (1979) give<br />

typical values as described in Table 3.4 <strong>and</strong> 3.5.<br />

Table 3.4 Angle of friction <strong>and</strong> unit weight values of soils derived from geologic layers<br />

Soil type Friction angle (°) γ sat (kN/m³) γdry(kN/m³)<br />

S<strong>and</strong>y loam 34 20.2 17.3<br />

Loam 33 18.6 14.9<br />

Clay 28 19.9 16.5<br />

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Table 3.5 Cohesion <strong>and</strong> friction angle values of soils derived from geologic layers<br />

Soil Cohesion (kPa) Friction angle (°)<br />

Silt (non plastic) 0 26-30<br />

Uniform fine to<br />

medium s<strong>and</strong> 0 26-30<br />

Well graded s<strong>and</strong> 0 30 -34<br />

S<strong>and</strong> <strong>and</strong> Gravel 0 32 -36<br />

Roughly equal to non<br />

Predominantly clayey 4.8-24 consolidated soil<br />

Driscoll, (1979), cited by Deoja, (1991) also state some shear strength parameter values as given<br />

in Table 3.6.<br />

Table 3.6 Cohesion <strong>and</strong> friction angle values of soils<br />

Soil type Symbol Cohesion (kN/m²) Friction (°)<br />

Well Graded Gravel GW 0 >38<br />

Poorly Graded Gravel GP 0 >37<br />

Gravel with Silts GM - >34<br />

Gravel with Clay GC - >31<br />

Well Graded S<strong>and</strong> SW 0 38<br />

Poorly Graded S<strong>and</strong> SP 0 37<br />

S<strong>and</strong> with Silts SM 2 to 5 34<br />

S<strong>and</strong> with Clay SC 1 to 7.5 31<br />

Mixture of s<strong>and</strong>s with silts<br />

<strong>and</strong> s<strong>and</strong>s with clay<br />

SM-SC 1.5 to 5 33<br />

Inorganic Silts ML 1 to7.0 32<br />

Inorganic Clay CL 1.5 to 9 28<br />

Mixture of inorganic silts <strong>and</strong><br />

inorganic clay<br />

ML-CL 2 to 6.5 32<br />

Organic Silts OL - -<br />

Inorganic Silts MH 2.1 to 7.5 25<br />

Inorganic Clay CH 1 to 10 19<br />

For this study, we concluded to try different combinations of values using the laboratory<br />

results as well as literature values. The one yielding the most unstable condition will be<br />

considered to be governing. Thus we come up with a final compilation of shear strength<br />

parameters which is given in Table 3.7.<br />

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Table 3.7 Final compiled shear strength parameters<br />

Weathered Formation<br />

Weathered Basalt<br />

(Swelling clays)<br />

Weathered Marl<br />

limestone<br />

Cohesion (kPa) Friction angle (°) γ sat γ dry<br />

C' φ' (kN/m³) (kN/m³)<br />

6.18 24 15.77 10.72<br />

11.58 20 17.67 13.99<br />

Remark<br />

On the study area by Nyssen<br />

et al. (2002)<br />

On the study area by Nyssen<br />

et al. (2002)<br />

Weathered S<strong>and</strong>stone 0 24 23 21<br />

Table 3.3 <strong>and</strong> Sloane,<br />

(1992), Hudson et al. (1997),<br />

Barton (1973)<br />

Weathered Shale<br />

4.4 19 18.2 15.1<br />

Table 3.2 <strong>and</strong> Văn et al.<br />

(2001)<br />

Weathered Dolerite 0 33 34 28.44 Table 3.3 <strong>and</strong> (Sloane, 1992)<br />

Weathered Shale -marl<br />

limestone<br />

5.79 21 20.84 18.84<br />

Alluvium 23 25 18 16<br />

Hoek et al. (1998), Kentli &<br />

Topal (2004)<br />

Table 3.4, 3.5, 3.6 <strong>and</strong> Văn<br />

et al. (2001)<br />

3.3 Soil depth<br />

Maps of the soil depth on steep hillsides are required for deterministic shallow l<strong>and</strong>slide<br />

models that include the effects of infiltration or soil cohesion. However, since collecting<br />

sufficient measurements to map soil thickness compatible with the scale of the DEMs is<br />

practically impossible; deterministic modeling efforts have typically relied on empirical or<br />

theoretical models to create soil depth maps (Dietrich et al., 1995; DeRose, 1996; Casadei et<br />

al., 2003).<br />

Ray & De Smedt (2009) determined the thickness of soil based on l<strong>and</strong> use <strong>and</strong> corrected it<br />

for slope angles, because depth of soil is inversely proportional with steepness of a terrain.<br />

Salciarini et al. (2006) also used an exponential function of topographic slope to map the soil<br />

depth in slope stability calculations.<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 26<br />

De Rose (1996) <strong>and</strong> Salciarini et al. (2006) estimate the depth to the lower boundary as:<br />

d 7.72* e<br />

0.04<br />

(3.2)<br />

lb<br />

Where d lb = depth to the lower boundary;<br />

β = slope angle;<br />

d lb is at a minimum of about 0.5 m on the steepest slopes, about 1.4 m on 40° slopes,<br />

<strong>and</strong> about 2.0 m on 30° slopes.<br />

Such approximations are expected to be used as a first estimate in slope stability calculations,<br />

<strong>and</strong> they are not considered to represent the actual site condition. The ideal investigation<br />

would be creating borehole locations <strong>and</strong> compiling geological, geotechnical <strong>and</strong> soil depth<br />

parameters. A site specific empirical relation is needed to be developed using topographical<br />

parameters <strong>and</strong> the borehole data.<br />

A shallow depth results in greater discharge volume <strong>and</strong> lower peak pore water pressure<br />

during major rainfall events, <strong>and</strong> consequently slope failure tends not to occur. However, a<br />

deeper material depth increases the weight of solids <strong>and</strong> the soil moisture in a slope <strong>and</strong> the<br />

pore water pressure. Hence it increases the likelihood of slope failure.<br />

Even though the thickness of the soil is an important parameter, it does not have an impact in<br />

granular soils. For cohesionless soils, the stability of slopes depends only on friction angle<br />

<strong>and</strong> slope angle in the dry conditions. And, for half saturated or saturated scenarios, the<br />

stability is controlled by unit weight, friction angle <strong>and</strong> slope angle values. This will be<br />

discussed in detail in chapter 4.<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 27<br />

3.4 Causative factor maps preparation<br />

3.4.1 <strong>Slope</strong> factor<br />

On steeper slopes, the tangential component of the weight of a mass <strong>and</strong> the shear stress<br />

increases while the perpendicular component of the weight decreases. The resistance to the<br />

down slope movement is favored by the frictional resistance <strong>and</strong> cohesion among the particles<br />

that make up the object. When the shear stress is greater than the combination of forces<br />

holding the object on a slope, the object will tend to move down-slope. Thus the slope of a<br />

terrain is a principal factor involving in the analysis of l<strong>and</strong>slides.<br />

The slope map of the study area is extracted using IDRISI <strong>GIS</strong> from the digital elevation<br />

model prepared using SRTM with pixel size of 90m. The minimum slope angle along flat<br />

sections is 0° while the maximum slope observed on nearly vertical cliffs is 57°.<br />

A slope category map is prepared for five categories: (1) Flat slopes (0-5°), (2) Rolling terrain<br />

(5-15°), (3) Mountainous, (15-25°), (4) Escarpments (25-45°), <strong>and</strong> (5) Cliffs (45-60°). The<br />

classification indicates that 52.42% of the study area is dominated by a rolling terrain, while<br />

Flat terrain amounts for 22.37%, 17.74% of the area is characterized by a Mountainous<br />

terrain, Escarpments occur on about 4.96% of the area <strong>and</strong> Cliffs occupy 0.1%.<br />

Figure 3.6 <strong>Slope</strong> map<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 28<br />

3.4.2 Geological factor<br />

The Distribution of l<strong>and</strong>slide is largely controlled by bedrock geology. Rock formations <strong>and</strong><br />

the type of soil present control the shear strength that can be provided, the weight of a mass<br />

that is involved, <strong>and</strong> the hydrologic characteristics of the regolith. The mechanical,<br />

mineralogical <strong>and</strong> hydrologic properties of the weathering products are directly dependent on<br />

the lithology.<br />

The geology of Hagere Selam area covers the north-western part of the Mekele outlier, which<br />

is composed of a nearly sub horizontal succession of the geological layers consisting of a<br />

lower s<strong>and</strong>stone unit, the Adigrat s<strong>and</strong>stone, an intermediate large carbonate unit, the Antalo<br />

limestone <strong>and</strong> Agula shale, <strong>and</strong> an upper s<strong>and</strong>stone unit, the Amba Aradam Formation<br />

(Bosellini et al., 1997). The Paleozoic Formation includes the Edaga Arbi glacial <strong>and</strong> Enticho<br />

s<strong>and</strong>stone which are found in North West part of the study area. Enticho s<strong>and</strong>stone, the metasedimentary<br />

Tembien Group <strong>and</strong> the meta-volcanics Tsaliet Group are equally significant in<br />

studying the geologic Formation of the study area. It is a white fine to medium grained<br />

s<strong>and</strong>stone with some calcareous cement (Tesfaye & Geberetsadik, 1982).<br />

The oldest geological formation, deep in the valley of the May Zegzeg, Tsaliet <strong>and</strong> upper<br />

Tankwa rivers is the Upper-Palaeozoic Adigrat s<strong>and</strong>stone. It is overlain by the marine Antalo<br />

limestones of Jurassic age, about 500 m thick (Moeyersons et al., 2008). Agula shales, which<br />

form the upper part of the Antalo supersequence (Bosellini et al., 1997) are present in a small<br />

belt around the Imba Degoa–Amba Raeset <strong>and</strong> on the elongated pass between the latter <strong>and</strong><br />

the Medayk Ridge (Moeyersons et al., 2008). Agula shales <strong>and</strong> Antalo limestones are<br />

truncated by a peneplanation disconformities (Dramis et al., 2002), overlain by Amba Aradam<br />

s<strong>and</strong>stone of Cretaceous age <strong>and</strong> by two series of Tertiary volcanic basalts. The basalts are<br />

intercalated with silicified lacustrine deposits (i.e. white silicified clays <strong>and</strong> marls with<br />

abundant cherts; Bosellini et al., 1997; Asrat, 2002). Tertiary basalts are believed to be more<br />

prone to mass wasting than the underlying formations (Moeyersons et al., 2008). As a result<br />

of contact metamorphism, the top of the Amba Aradam s<strong>and</strong>stone is resistant <strong>and</strong> impervious.<br />

A network of Mekelle dolerite sills <strong>and</strong> dykes are developed more or less contemporaneously<br />

with the plateau basalts (Dramis et al., 2002). The Imba Degoa Ridge is, for example, a feeder<br />

dyke of the Mekele dolerite sill (Van Den Eeckhaut et al., 2009).<br />

The geological map of Hagere Selam is derived from the geological map of the Mekele outlier<br />

on scale 1:100.000 (Russo et al., 1999), the geological map of Ethiopia, <strong>and</strong> SWIR images. It<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 29<br />

was recompiled <strong>and</strong> simplified to a <strong>GIS</strong> format for the purpose of l<strong>and</strong>slide susceptibility<br />

analysis. Figure 3.7 shows the simplified geological map of the study region.<br />

Figure 3.7 Geologic map<br />

3.4.3 Distance to faults factor<br />

Tectonics contributes to slope instability by fracturing, faulting, jointing <strong>and</strong> deforming<br />

foliation structures (Ibetsberger, 1996). Varnes (1984) concluded that the degree of fracturing<br />

<strong>and</strong> shearing plays an important role in determining slope stability. The Effect of faulting is<br />

detachment of soil grains resulting in decrease in shear strength.<br />

The distance to faults factor is obtained using the following procedures:<br />

The faults on the geological map of Mekele outlier on scale 1:100.000 (Russo et al.,<br />

1999) are digitized using IDRISI-<strong>GIS</strong>.<br />

Distance to those faults is calculated, <strong>and</strong> categorized into 6 groups: (1) Very close to<br />

faults (5000 m)<br />

Several faults cross the study area. SE-NW facing faults being are dominant.<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 30<br />

Figure 3.8 Distance to faults map<br />

3.4.4 Elevation factor<br />

The influence of elevation on the mechanism of l<strong>and</strong> sliding is often attributed to be indirect.<br />

Humidity, hydrate reactions, weathering processes, erosion <strong>and</strong> resulting weathering depths<br />

are affected by elevation. The more intense erosion <strong>and</strong> weathering, the more will be the<br />

influence of elevation on l<strong>and</strong>slides. Thus considering elevation as one of the causative<br />

factors is reasonable from the perspective of other elevation affected processes that control<br />

l<strong>and</strong>slides.<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 31<br />

The digital elevation model representing Hagere Selam area is obtained from SRTM DEM at<br />

a resolution of 90 m. An appropriate filtering operation is applied on IDRISI-<strong>GIS</strong> to obtain a<br />

smoothened output. The study area is characterized by high relief variability ranging to about<br />

1158m with the minimum elevation recorded being 1668 m in the north west part of Hagere<br />

Selam <strong>and</strong> the maximum elevation being 2826 m around the Medayk ridge.<br />

For l<strong>and</strong>slide susceptibility analysis, the elevation of the study area is categorized into five<br />

classes: (1) Low Elevation (


Chapter 3: Methodology <strong>and</strong> data preparation 32<br />

The effects of vegetation cover on the hydrological processes of shallow l<strong>and</strong> sliding can be<br />

subdivided into the loss of precipitation by interception, removal of soil moisture by<br />

evapotranspiration <strong>and</strong> the effects on hydraulic conductivity (Van Beek, 2002).<br />

For the study area, we are unable to find an already prepared l<strong>and</strong> use map. Compiling such a<br />

map requires precise imagery as well as field measurements. In fact, it is not under the scope<br />

of this study to produce a detailed l<strong>and</strong> use map. However, we are interested to investigate the<br />

effect of vegetation to slope stability. This can, roughly, be obtained using SRTM (Shuttle<br />

Radar Topography Mission) imagery. A false color composite is compiled using VNIR image<br />

b<strong>and</strong> 3, 2 <strong>and</strong> 1. A supervised classification is carried out controlled by training pixels<br />

obtained from Google earth. Identifying vegetation is rather easy on false color composite, but<br />

there are sometimes clear 'shading' effects that complicate the classification. In addition, there<br />

are rivers <strong>and</strong> other water bodies in the scene, which might have been recognized by their<br />

shape. However, they are difficult to be used as training sites as they are quite narrow at this<br />

resolution. Bare soils <strong>and</strong> S<strong>and</strong>y soils are also identifiable in the scene. There is no big city<br />

that can be assigned as urban class, <strong>and</strong> hence identified as such by using its spatial structure.<br />

However, Hagere Selam is included using manual delineation on the classified image. The<br />

classification employed is a maximum likelihood classification.<br />

Needless to say, what we presented in Figure 3.10 doesn’t represent the l<strong>and</strong> use map of the<br />

area but some l<strong>and</strong> use features that can be identified using the available data.<br />

Figure 3.10 L<strong>and</strong> use factor map<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 33<br />

3.4.6 <strong>Slope</strong> Shape<br />

Degree of saturation of a slope-forming material is another major factor controlling the<br />

occurrence of l<strong>and</strong>slides. Concave slopes favor pore water pressure build up than straight<br />

slopes (Dai & Lee, 2002). Easy flow of water on convex slopes attribute to its stability than<br />

other slope shapes. For the study area slope shape map is produced using IDRISI-<strong>GIS</strong>.<br />

Appropriate grouping is performed to classify the map in to 7 categories: (1) Peak <strong>and</strong> ridges,<br />

(2) Saddle, (3) <strong>Slope</strong> hill, (4) Convex, (5) Concave, (6) Gully, <strong>and</strong> (7) Other.<br />

3.4.7 Aspect<br />

The amount of precipitation received on a particular slope differs with respect to the various<br />

orientations it could have. Aspect related parameters such as exposure to sunlight, drying<br />

winds, rainfall (degree of saturation), <strong>and</strong> discontinuities may control the occurrence of<br />

l<strong>and</strong>slides (Dai & Lee, 2002). However, the direct relationship with aspect <strong>and</strong> l<strong>and</strong>slides is<br />

not yet clear (Van Westen et al., 2006). The aspect map of Hagere Selam area is, thus, derived<br />

from the DEM to account for the probable causative relationship between aspect <strong>and</strong> slope<br />

instability. The aspect map is classified into 10 groups: (1) Flat (-1°), (2) North (0°-22.5°), (3)<br />

North east (22.5°-67.5°), (4) East (67.5°-112.5°), (5) South east (112.5°-157.5°), (6) South<br />

(157.5°-202.5°), (7) South west (202.5°-247.5°), (8) West (247.5°-292.5°), (9) North west<br />

(292.5°-337.5°), <strong>and</strong> (10) North (337.5°-360°).<br />

Figure 3.11 <strong>Slope</strong> shape <strong>and</strong> Aspect<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 34<br />

3.4.8 Distance to streams<br />

An important parameter that controls the stability of a slope is the degree of saturation of the<br />

material on the slope. The closer the slope is to streams, the more likely will it get water <strong>and</strong><br />

develop pore pressure. Streams may adversely affect stability by eroding slopes or by<br />

saturating the lower part of the material which results an increase in ground water level.<br />

A map of distances to streams was calculated using the buffering algorithms of ILWIS<br />

software on the basis of rivers <strong>and</strong> streams available on the topographic map. The map is then<br />

classified into 6 categories: (1) Very close (


Chapter 3: Methodology <strong>and</strong> data preparation 35<br />

Figure 3.12 Distance to streams<br />

Figure 3.13 Distance to roads<br />

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Chapter 3: Methodology <strong>and</strong> data preparation 36<br />

3.4.10 Wetness index<br />

In order to express water condition, a DEM-based wetness index, otherwise known as<br />

compound topographic index was used to represent the spatial distribution of water flow<br />

across the study area. The wetness index represents a theoretical measure of the accumulation<br />

of flow at any point within a river basin <strong>and</strong> is calculated using the expression:<br />

w = ln( A tanβ<br />

) (3.3)<br />

Where w is the wetness index, As is the upstream catchment area <strong>and</strong> β is slope angle. This<br />

equation assumes steady-state conditions <strong>and</strong> uniform soil properties (i.e., transmissivity is<br />

constant throughout the catchment <strong>and</strong> equal to unity). This equation predicts zones of<br />

saturation where the upstream catchment area (As) is large (typically in converging segments<br />

of l<strong>and</strong>scapes), the slope (β) is small (at the base of concave slopes where slope gradient is<br />

reduced) <strong>and</strong> the transmissivity is minimal (on shallow soils). These conditions are usually<br />

encountered along drainage paths <strong>and</strong> in zones of water concentration in l<strong>and</strong>scapes (Wilson<br />

& Gallant, 2000). The topographic wetness index map of the study area is prepared using<br />

IDRISI-<strong>GIS</strong> <strong>and</strong> classified into 4 categories: (1) w


Chapter 4: Deterministic models<br />

4.1 Physical based models<br />

All limit equilibrium methods utilize the Mohr-Coulomb expression to determine the shear<br />

strength (τ ) along a sliding surface. According to Prasad (2006), a state of limit equilibrium<br />

exists when the mobilized shear stress (τ) is expressed as a fraction of the shear strength. At<br />

the moment of failure, the shear strength is fully mobilized along the failure surface when the<br />

critical state conditions are reached.<br />

4.1.1 <strong>Stability</strong> of infinite slopes<br />

Figure 4.1 (a) <strong>and</strong> (b) - infinite slope force diagrams<br />

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Chapter 4: Deterministic models 38<br />

Figure 4.1 shows an infinite slope with force diagrams. Assuming a seepage through the<br />

material <strong>and</strong> that the ground water table is at mH distance above the failure plane. The shear<br />

strength of the material is given by,<br />

τ<br />

f<br />

c' σ' tan'<br />

(4.1)<br />

Where c’ is the effective cohesion (kN/m²), σ’ is the effective normal stress (kN/m²) <strong>and</strong> ϕ’ is<br />

the angle of internal friction (°).<br />

To determine the factor of safety against failure along plane AB, we consider the slope<br />

element abcd. The forces that act on the vertical faces ab <strong>and</strong> cd are equal <strong>and</strong> opposite. The<br />

total weight of the slope element of unit length is,<br />

W<br />

L<br />

((1 m)<br />

<br />

dry<br />

m<br />

sat<br />

) H<br />

(4.2)<br />

cos <br />

where, γ sat = saturated unit weight of the material (kN/m³), γ dry = dry unit weight of the<br />

material (kN/m³), H is depth of the material above the failure surface (m), m = wetness index,<br />

L is length of slope element abcd (m), <strong>and</strong> β is the slope angle (°).<br />

The components of the weight in the directions normal <strong>and</strong> parallel to the plane AB are<br />

N a = Wcosβ = (( 1 m)<br />

m<br />

LH , T a = (( 1<br />

m)<br />

m<br />

) LH tan <br />

dry sat<br />

)<br />

dry<br />

<br />

sat<br />

<br />

N r =N a, T r = T a<br />

The normal stress is given by:<br />

The shear stress is given by:<br />

N ((1 m)<br />

<br />

dry<br />

m<br />

) LH<br />

r<br />

sat<br />

<br />

<br />

Area of the base L<br />

cos <br />

(( 1m)<br />

dry m<br />

sat ) H cos <br />

(4.3)<br />

T ((1 m)<br />

<br />

a<br />

<br />

<br />

Area of the base<br />

dry<br />

m<br />

sat<br />

L<br />

cos <br />

) LH tan <br />

(( 1<br />

m)<br />

m<br />

) H sin <br />

(4.4)<br />

dry<br />

<br />

sat<br />

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Chapter 4: Deterministic models 39<br />

The effective normal stress is given by:<br />

' u<br />

(4.5)<br />

where, u is the pore water pressure (kN/m²). Referring to Figure 4.1 (b), we find<br />

u<br />

w w<br />

= (height of piezometer head at f) * = h <br />

u = h <br />

w<br />

( ef<br />

w<br />

cos ) mH<br />

w<br />

cos <br />

Substituting the value of σ <strong>and</strong> u into εq 4.1,<br />

<br />

f<br />

c'<br />

(((1<br />

m)<br />

m<br />

) H cos mH cos ) tan '<br />

(4.6)<br />

dry<br />

sat<br />

w<br />

Expressing the factor of safety as a the ratio of stabilizing to destabilizing forces,<br />

F<br />

s<br />

<br />

f<br />

c'<br />

(((1<br />

m)<br />

<br />

dry<br />

m<br />

sat<br />

) H cos <br />

wmH<br />

cos ) tan '<br />

<br />

(4.7)<br />

<br />

((1 m)<br />

m<br />

) H sin <br />

dry<br />

sat<br />

Now, we introduce the effective unit weight of the material,<br />

( 1<br />

m)<br />

m<br />

e dry sat<br />

(4.8)<br />

Thus the factor of safety is written as,<br />

C'<br />

(<br />

m<br />

w<br />

) H cos tan '<br />

F<br />

e<br />

s<br />

<br />

H sin <br />

e<br />

C'<br />

<br />

w tan '<br />

Fs<br />

(1 m )<br />

H sin tan <br />

(4.9)<br />

e<br />

e<br />

The safety factor map calculated using Eq. 4.9 can be classified into categories describing<br />

degree of instability. In this study, the classification shown in Table 4.1 is adopted.<br />

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Chapter 4: Deterministic models 40<br />

Table 4.1 Classification of factor of safety values<br />

Criteria<br />

FS


Chapter 4: Deterministic models 41<br />

Figure 4.2 (a) saturated unit weight map, (b) dry unit weight map<br />

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Chapter 4: Deterministic models 42<br />

Figure 4.3 (a) cohesion map, (b) angle of internal friction map<br />

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Chapter 4: Deterministic models 43<br />

4.1.3 Critical depth<br />

The critical engineering depth is used as an indication of how a slope behaves without support<br />

<strong>and</strong> explains the ability of a slope to withst<strong>and</strong> instabilities. In addition, it guides the extent by<br />

which construction cuts <strong>and</strong> embankments can be accomplished. The Critical height map is of<br />

equal importance as factor of a safety map to engineers <strong>and</strong> planners. It is calculated for the<br />

factor of safety value of one. From equation 4.9, it can be derived as:<br />

H<br />

c<br />

C'<br />

<br />

2<br />

4.10<br />

sin cos ( m<br />

) cos tan '<br />

w<br />

H<br />

c<br />

C'<br />

<br />

2<br />

4.11<br />

cos ( (tan tan '<br />

) m<br />

tan '<br />

)<br />

w<br />

For granular material, the cohesion between particles is negligible <strong>and</strong> C’ = 0. From equation<br />

4.9, the factor of safety equals tanϕ’/ tanβ for dry conditions. Hence, the slope is stable as<br />

long as β < ϕ’. For half saturated <strong>and</strong> saturated scenarios, the factor of safety depends on unit<br />

weight, friction angle <strong>and</strong> slope angle. Therefore, the stability of an infinite slope in<br />

cohesionless material is independent of depth. The critical depth calculation is carried out<br />

only for non granular materials in the study area. Three steady state conditions, m = 0, m =<br />

0.5 <strong>and</strong> m = 1 are considered.<br />

4.1.3.1 Saturated critical depth<br />

The calculation of critical height with equation 4.11 results in negative values of the critical<br />

height when the term (tan β – tan ϕ’) becomes negative. This happens when the slope angle is<br />

less than the angle of internal friction. In this case, the negative value has to be considered as<br />

an infinite critical depth, because if the slope angle is less than the angle of internal friction,<br />

failure is unlikely to occur.<br />

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Chapter 4: Deterministic models 44<br />

Figure 4. 4 Critical depth to lower boundary under fully saturated condition<br />

The critical depth under fully saturated condition ranges from 0 to 20 m. Around 31% of the<br />

area has a slope angle smaller than the angle of internal friction resulting in a stable condition.<br />

An additional 22% of the area is characterized by negligible soil cohesion; hence, its stability<br />

is independent of depth of material above the failure plane. The depth of the slide plane is<br />

only less than 1.5 m for 16% of the area. A material thickness of less than 2.5 m shall be<br />

maintained over 27% of the area to attain stability. 41% of the area should have a depth to the<br />

lower boundary of less than 10 m under fully saturated condition. Figure 4.5 summarizes the<br />

areal distribution versus critical depth.<br />

4.1.3.2 Half saturated critical depth<br />

The critical height map under half saturated scenario is shown in Figure 4.5(a). 22% of the<br />

area is characterized by negligible cohesion, <strong>and</strong> hence its stability is independent of depth.<br />

56% of the area has a slope angle small enough to have a sufficient frictional resistance<br />

against shear failure. This Figure was 31% for fully saturated scenario. The larger the amount<br />

of water in the regolith, the lower will be the frictional resistance between particles <strong>and</strong> the<br />

more unstable the slope will become. In addition, a soil depth of less than 3.5m <strong>and</strong> 10m shall<br />

be maintained over 15% <strong>and</strong> 20% of the area, respectively, to prevent instability.<br />

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Chapter 4: Deterministic models 45<br />

4.1.3.3 Dry critical depth<br />

The dry scenario gives the most stable condition. 68% of the slope angles are small enough to have a sufficient frictional resistance against shear<br />

failure. 7.5% of the area shall have a depth to the failure plane of less than 10m to prevent instability.<br />

Figure 4.5 Critical depth to lower boundary, (a) under half saturated, (b) under dry conditions<br />

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Chapter 4: Deterministic models 46<br />

Figure 4.6 Areal distribution of critical depths under saturated, half sat <strong>and</strong> dry scenarios<br />

During dry condition, around 68% of the area has a slope angle sufficiently lower than the<br />

internal angle of friction to control instability. However, this decreases to 56% <strong>and</strong> 31% for<br />

half saturated <strong>and</strong> saturated scenarios. This is explained by the fact that the frictional<br />

resistance between particles is reduced due to the presence of water. Therefore, it can be said<br />

that slope angles that were significantly smaller than the internal angle of friction to control<br />

sliding would become susceptible with the increase in soil wetness.<br />

4.1.4 Factor of safety calculation<br />

4.1.4.1 Completely dry condition<br />

The stability of a slope under completely dry condition is governed by cohesion, angle of<br />

internal friction, slope angle <strong>and</strong> the depth of the material above the bedding plane. Since,<br />

there is no pore water pressure developed, this scenario gives the highest amount of area<br />

under stable condition. However, due to very steep slope <strong>and</strong> poor material strength in shear,<br />

the minimum safety factor for this situation is observed to be 0.03. In some flat parts of the<br />

study area the safety factor is observed to be over 4000. Under completely dry scenario,<br />

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Chapter 4: Deterministic models 47<br />

80.3% of the area is found to be stable, 8.4% is regarded as moderately stable, 6.4% <strong>and</strong> 4.9%<br />

are found to be quasi stable <strong>and</strong> unstable respectively.<br />

The safety factor map displaying the inventoried l<strong>and</strong>slides <strong>and</strong> rocky cliffs is shown in<br />

Figure 4.7.<br />

Figure 4.7 Classified factor of safety map under dry condition<br />

The next step is to check how many of the inventoried l<strong>and</strong>slides are indeed identified by the<br />

infinite slope model. For this, a cross operation is performed between the categorized factor of<br />

safety map under dry condition <strong>and</strong> the l<strong>and</strong>slide inventory using ILWIS-<strong>GIS</strong>. The result is<br />

shown in the Table 4.2.<br />

Table 4.2 Model validation under dry condition<br />

<strong>Stability</strong> class<br />

Observed l<strong>and</strong>slides<br />

(# of pixels) % of LS LS susceptibility class<br />

Unstable 965 19.02 Very high<br />

Quasi stable 987 19.46 High<br />

Moderately stable 944 18.61 Moderate<br />

Stable 2177 42.91 Low/Very low<br />

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Chapter 4: Deterministic models 48<br />

Under completely dry condition, 38% of the observed l<strong>and</strong>slides are identified in high <strong>and</strong><br />

very high l<strong>and</strong>slide susceptibility classes. An additional 19% of the failure units are in zones<br />

of moderate hazard. According to the infinite slope model, however, 43% of the l<strong>and</strong>slides<br />

will not be mobilized, if the soil remains dry.<br />

To investigate the stability condition with slope classes, a cross operation between slope<br />

categories <strong>and</strong> factor of safety classes is carried out. The result is shown in Table 4.3.<br />

Table 4.3 <strong>Stability</strong> vs slope classes<br />

<strong>Stability</strong> condition<br />

Flat Rolling Mountainous Escarpments Cliffs Remark<br />

(%) (%) (%) (%) (%)<br />

Unstable 0.00 0.01 8.83 57.40 81.82 Very high LS susc.<br />

Quasi stable 0.00 0.00 26.88 33.33 5.45 High LS susc.<br />

Moderately stable 0.00 3.22 35.11 9.26 12.73 Moderate LS susc.<br />

Stable 100.00 96.77 29.18 0.00 0.00 Low/Very low LS susc.<br />

In flat <strong>and</strong> rolling terrains, the slope is unlikely to fail under completely dry condition. 37% of<br />

areas with slope angle 15°-25° are regarded as high <strong>and</strong> very high l<strong>and</strong>slide susceptibility<br />

zones. 91% of the escarpments in the study area, with slope angle ranging from 25° to 45°, are<br />

likely to fail without the action of water. However, this Figure lowers to 87% for larger slope<br />

angles i.e. for cliffs (with slope angle between 45° to 60°). This is explained by the nature of<br />

the formations. If it weren’t for the hard <strong>and</strong> firm composition of such cliffs, a profile slope of<br />

over 45° would have never been attained. Therefore, such formations have large strength in<br />

shear that decreases the extent by which sliding occurs.<br />

The stability condition against geologic formations is assessed in Table 4.4.<br />

Table 4.4 <strong>Stability</strong> vs geologic formations<br />

<strong>Stability</strong> condition<br />

Trap<br />

basalt<br />

Limestone<br />

Marl<br />

Amba<br />

Aradom<br />

S<strong>and</strong>stone<br />

Shale Dolerite<br />

Sill<br />

Shale Marl<br />

Limestone<br />

Marl<br />

Limestone<br />

Endaga<br />

Adigrat<br />

S<strong>and</strong>stone Alluvium Arbi<br />

Glacial<br />

Entcho<br />

S<strong>and</strong>stone<br />

(%) (%) (%) (%) (%) (%) (%) (%) (%) (%) (%)<br />

Unstable 0.02 2.49 16.19 3.41 0.91 1.23 0.00 32.61 0.00 2.52 11.88<br />

Quasi stable 5.80 7.03 16.85 6.68 4.85 5.73 2.22 13.71 0.00 0.00 4.99<br />

Moderately stable 10.84 9.17 11.06 9.02 4.21 6.86 7.48 9.10 0.00 0.00 3.66<br />

Stable 83.34 81.31 55.89 80.89 90.04 86.18 90.29 44.57 100.00 97.48 79.47<br />

33% of Amba Aradom s<strong>and</strong>stone formation is likely to fail under completely dry scenario.<br />

46% of Adigrat s<strong>and</strong>stone is characterized by a factor of safety less than 1.25. Adigrat<br />

s<strong>and</strong>stone is a hard formation, however the slope angles of part of such cliffs (located around<br />

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Chapter 4: Deterministic models 49<br />

NW of the study area) is sufficiently large that mohr-coloumb criteria is not satisfied. 10% of<br />

shale, 10% of Limestone marl <strong>and</strong> 6% of trap basalts are located in high <strong>and</strong> very high<br />

l<strong>and</strong>slide susceptibility classes, even if the soil is kept dry. Failure in alluvium, Endaga Arbi<br />

glacial, dolerite sill <strong>and</strong> marl limestone is unlikely to occur in this situation.<br />

4.1.4.2 Half saturated condition<br />

The stability of a slope under half saturated condition is controlled by cohesion, angle of<br />

internal friction, slope angle, the thickness of the material above the bedding plane <strong>and</strong> pore<br />

water pressure. Half the thickness of the material is assumed to be saturated with water.<br />

21.67% of the area is found to be unstable, 12.85% is quasi stable while moderately stable <strong>and</strong><br />

stable classes constitute 13.02% <strong>and</strong> 52.46% respectively. Therefore, under half saturated<br />

scenario, 34% of the study area is defined to be high <strong>and</strong> very high l<strong>and</strong>slide susceptibility<br />

category. This value exceeds the area identified by the l<strong>and</strong>slide inventory by 14%.<br />

The safety factor map overlaid by the inventoried l<strong>and</strong>slides <strong>and</strong> rocky cliffs is shown in<br />

Figure 4.8. From Figure 4.8, it is observed that, infinite slope model identifies most of the<br />

rock falls under half saturated scenario. For l<strong>and</strong>slide bodies, the depletion areas are<br />

recognized to be quasi stable <strong>and</strong> unstable (FS < 1.25 <strong>and</strong> FS


Chapter 4: Deterministic models 50<br />

Figure 4.8 Classified factor of safety map for half saturated condition<br />

Table 4.5 Model validation under half saturated condition<br />

<strong>Stability</strong> class<br />

Observed<br />

l<strong>and</strong>slides<br />

(# of pixels) % of LS LS susceptibility class<br />

Unstable 3145 61.99 Very high<br />

Quasi stable 633 12.48 High<br />

Moderately stable 430 8.48 Moderate<br />

Stable 865 17.05 Low/Very<br />

Under half saturated scenario, 74% of the observed l<strong>and</strong>slides are identified in high <strong>and</strong> very<br />

high l<strong>and</strong>slide susceptibility classes. An additional 9% of the failure units are in zones of<br />

moderate hazard. In the study area, if slope evaluation is made using this model under semi<br />

saturated condition, 17% of failure zones won’t be recognized. However, this is not a bad<br />

Figure due to the following reasons:<br />

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Chapter 4: Deterministic models 51<br />

Part of those unrecognized l<strong>and</strong>slides could have been triggered by a rainfall incidence<br />

which might have saturated more than half the thickness of the material.<br />

In compiling the l<strong>and</strong>slide database, not all the erosional belts of the mass movements<br />

could be identified accurately. This is mainly due to the fact that only morphology of<br />

depositional bodies are clearly visible using aerial photographs, <strong>and</strong> the depletion<br />

zones had more difficult morphologies to be delineated accurately. So, there will be<br />

some pixels of depositional lobes in the database, which will turn out to be stable by<br />

the infinite slope model.<br />

To correlate the stability condition with slope classes, a cross operation between slope<br />

categories <strong>and</strong> factor of safety map is carried out. The result is shown in Table 4.6.<br />

Table 4.6 <strong>Stability</strong> vs slope classes under semi saturated condition<br />

<strong>Slope</strong> catagories<br />

<strong>Stability</strong> condition Flat Rolling Mountainous Escarpments Cliffs Remark<br />

(%) (%) (%) (%) (%)<br />

Unstable 0.00 3.53 80.80 100.00 100.00 Very high LS susc.<br />

Quasi stable 0.00 18.29 18.40 0.00 0.00 High LS susc.<br />

Moderately stable 0.00 24.57 0.78 0.00 0.00 Moderate LS susc.<br />

Stable 100.00 53.60 0.03 0.00 0.00 Low/Very low LS susc.<br />

In flat terrain, the slope is unlikely to fail under half saturated condition. Unlike the dry<br />

condition, instability starts to happen on slopes > 5°. Only 54% of the rolling terrain is<br />

assured to have low l<strong>and</strong>slide susceptibility. An additional 62% to the 37% of the<br />

mountainous areas that were defined to likely fail in dry condition will be regarded as zones<br />

of high <strong>and</strong> very high l<strong>and</strong>slide susceptibility classes. If half of the material depth is assumed<br />

to be saturated with water, all areas with slope angle 25-45° will possibly fail. The same is<br />

true for cliffs. The stability condition against geologic formations is looked into table 4.7.<br />

Table 4.7 <strong>Stability</strong> vs geologic formations under semi saturated scenario<br />

Amba<br />

Endaga<br />

<strong>Stability</strong> condition<br />

Limestone Aradom Dolerite Shale Marl Marl Adigrat<br />

Arbi Entcho<br />

Trap basalt Marl S<strong>and</strong>stone Shale Sill Limestone Limestone S<strong>and</strong>stone Alluvium Glacial S<strong>and</strong>stone<br />

(%) (%) (%) (%) (%) (%) (%) (%) (%) (%) (%)<br />

Unstable 24.46 16.44 43.79 21.83 7.88 13.44 11.58 55.20 0.00 2.52 20.25<br />

Quasi stable 14.73 17.18 13.67 17.30 6.87 10.74 12.74 10.24 0.00 0.00 4.85<br />

Moderately stable 13.82 14.80 13.30 17.84 8.20 13.93 13.17 8.20 5.48 0.59 4.92<br />

Stable 46.99 51.58 29.23 43.03 77.04 61.89 62.51 26.36 94.52 96.89 69.97<br />

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Chapter 4: Deterministic models 52<br />

57% of Amba Aradom s<strong>and</strong>stone formation is likely to fail under half saturated scenario. 65%<br />

of Adigrat s<strong>and</strong>stone is characterized by a factor of safety less than 1.25. Adigrat s<strong>and</strong>stone is<br />

a hard formation, however the slope angles of part of such cliffs (located around NW of the<br />

study area) is sufficiently large that mohr-coloumb criteria is not satisfied. Saturating half of<br />

the material depth is enough to mobilize an additional 33% of trap basalts than the 6%<br />

identified during the dry condition. 39% of shale <strong>and</strong> 34% of Limestone marl are recognized<br />

to be in high <strong>and</strong> very high l<strong>and</strong>slide susceptibility zones. It is observed that the highest effect<br />

of the developed pore-water pressure is felt in the basalts. This is explained by the nature of<br />

expansive clays resulting from the weathering of basalts. Moreover, failure in alluvium <strong>and</strong><br />

Endaga Arbi glacial is unlikely to occur in this situation.<br />

4.1.4.3 Full saturated condition<br />

The stability of a slope under fully saturated condition is controlled by cohesion, angle of<br />

internal friction, slope angle, depth to solid rock <strong>and</strong> pore water pressure. The ground water<br />

table is assumed to be parallel with the bedding plane <strong>and</strong> coincide with the ground surface.<br />

This scenario gives the worst instability that could exist owing to the considered parameters.<br />

The factor of safety map is shown in Figure 4.9. 39.34% of the area is characterized by a<br />

factor of safety of less than one, 13.65% is quasi stable while moderately stable <strong>and</strong> stable<br />

classes contribute to be 12.39% <strong>and</strong> 34.62% respectively. Hence, considering the parameters<br />

involved in this study, the worst situation that could happen is that 53% of the area will be<br />

under high <strong>and</strong> very high l<strong>and</strong>slide susceptibility zones. This is comparably very large as<br />

compared with the l<strong>and</strong>slide inventory which puts 20% of the area in l<strong>and</strong>slide zone. In<br />

comparison with the inventory, fully saturated scenario assigns an additional 1/3 of the study<br />

area i.e. 164km² under risk zone. If extreme rainfall situation permits full saturation, only 35%<br />

of the area will be resistant in shear.<br />

From Figure 4.9, it is observed that, infinite slope model identifies almost all rock falls under<br />

fully saturated scenario. The l<strong>and</strong>slide lobes are also significantly recognized; especially the<br />

depletion units are defined to have a FS < 1. Parts of the depositional lobes could reasonably<br />

have a FS > 1, as these areas are not the place where the l<strong>and</strong>slides get mobilized.<br />

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Chapter 4: Deterministic models 53<br />

To depict the extent by which the final output under full saturated scenario conform to the<br />

l<strong>and</strong>slide database, Table 4.8 shows a cross validation between the categorized factor of safety<br />

map <strong>and</strong> the l<strong>and</strong>slide inventory.<br />

Figure 4.9 Classified factor of safety map under full saturated condition<br />

Table 4.8 Model validation under fully saturated condition<br />

<strong>Stability</strong> class<br />

Observed<br />

l<strong>and</strong>slides<br />

(# of pixels) % of LS LS susceptibility class<br />

Unstable 4020 79.24 Very high LS susc.<br />

Quasi stable 369 7.27 High LS susc.<br />

Moderately stable 249 4.91 Moderate LS susc.<br />

Stable 435 8.57 Low/Very low LS susc.<br />

An infinite slope model based on completely saturated scenario identifies 86% of the<br />

observed l<strong>and</strong>slides in high <strong>and</strong> very high l<strong>and</strong>slide susceptibility classes. An additional 5% of<br />

the failure units are defined in zones of moderate hazard. On the study area, if slope stability<br />

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Chapter 4: Deterministic models 54<br />

analysis is performed using this model under full saturated condition, only 9% of actual<br />

failure zones wouldn’t be recognized.<br />

The stability condition is assessed with slope classes in Table 4.9.<br />

Table 4.9 <strong>Stability</strong> versus slope classes<br />

<strong>Slope</strong> catagories<br />

<strong>Stability</strong> condition Flat Rolling Mountainous Escarpments Cliffs Remark<br />

(%) (%) (%) (%) (%)<br />

Unstable 0.00 31.15 98.81 100.00 100.00 Very high LS susc.<br />

Quasi stable 0.00 25.66 1.13 0.00 0.00 High LS susc.<br />

Moderately stable 1.12 23.14 0.06 0.00 0.00 Moderate LS susc.<br />

Stable 98.88 20.05 0.00 0.00 0.00 Low/Very low LS susc.<br />

In flat terrain, the slope is unlikely to fail under full saturated condition. However unlike the<br />

other scenarios 1.12% of slopes < 5° are observed to have a FS < 1.5. Only 20% of the rolling<br />

terrain is assured to have low l<strong>and</strong>slide susceptibility, this Figure amounts to 10% of the study<br />

area. 56% of the area with slope angle between 5° to 15° is characterized by a FS < 1.25. If<br />

the weathered material is fully saturated, failure is eminent in slopes > 15°. The shear strength<br />

of 100% of areas with slope angles between 15° to 45° will be fully mobilized, <strong>and</strong> hence<br />

failure will likely occur. The same is true for cliffs. It could be deduced from the above table<br />

<strong>and</strong> areal distribution of the terrain classes that if the weathering products are allowed to fully<br />

saturate, only 35% of the study area will be stable. Therefore such a condition shall be<br />

considered for the long term estimation of stability. However, for short term modeling,<br />

assumption of full saturation is not realistic.<br />

The stability condition is assessed with the lithology in Table 4.10.<br />

Table 4.10 <strong>Stability</strong> vs geologic formations<br />

Amba<br />

Aradom<br />

S<strong>and</strong>stone<br />

Endaga<br />

Arbi<br />

Glacial<br />

<strong>Stability</strong> condition<br />

Limestone<br />

Dolerite Shale Marl Marl Adigrat<br />

Entcho<br />

Trap basalt Marl<br />

Shale Sill Limestone Limestone S<strong>and</strong>stone Alluvium S<strong>and</strong>stone<br />

(%) (%) (%) (%) (%) (%) (%) (%) (%) (%) (%)<br />

Unstable 50.69 34.17 60.88 50.87 12.57 26.49 26.03 68.22 0.00 2.61 26.09<br />

Quasi stable 14.39 15.27 14.04 16.30 8.36 15.77 14.53 7.61 1.37 1.09 5.91<br />

Moderately stable 11.21 13.04 11.06 11.16 8.26 16.27 15.93 5.99 17.81 3.36 6.12<br />

Stable 23.71 37.52 14.02 21.66 70.80 41.46 43.50 18.18 80.82 92.94 61.88<br />

74% of Amba Aradom s<strong>and</strong>stone formation is likely to fail under this scenario. Fully<br />

saturation of the soil develops a pore pressure that could mobilize an additional 59% of trap<br />

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Chapter 4: Deterministic models 55<br />

basalts than the 6% that was identified during the dry condition. 75% of Adigrat s<strong>and</strong>stone is<br />

characterized by a factor of safety less than 1.25. 67% of shale, 49% of Limestone marl, <strong>and</strong><br />

42% shale –marl limestone will have a factor of safety less than 1.25. It is observed that the<br />

highest effect of the developed pore-water pressure is felt in the basalts. Swelling clays are the<br />

weathering products of basalts in the study area. These clay minerals could increase twice in<br />

volume upon the entrance of water. The impact of water is two sided for slope stability; (1) it<br />

breaks the natural anchorage between the soil grains <strong>and</strong> decreases the strength the soil has in<br />

shear (2) it creates an uplift pressure which counterbalances the vertical component of the<br />

weight. Owing to the higher areal distribution covered by trap basalt in the study area,<br />

emphasis shall be given to instabilities occurring in the formation.<br />

4.1.4.5 <strong>Stability</strong> calculation by combining three steady state scenarios, dry,<br />

half saturated <strong>and</strong> fully saturated.<br />

Now, we will investigate the stability analysis by combining the three steady state scenarios,<br />

using the classification shown in Table 4.11.<br />

Table 4.11 Combined factor of safety classification<br />

Category<br />

Factor of safety criteria<br />

Saturated Half sat. Dry<br />

Unconditionally stable FS > 1.5 Stable in completely saturated condition<br />

Stable 1.25 < FS < 1.5<br />

Moderately stable 1 < FS < 1.25<br />

Criteria<br />

Moderately stable in completely saturated<br />

condition<br />

Quasi stable in completely saturated<br />

condition<br />

Moderately unstable FS < 1 FS > 1 FS > 1<br />

Unstable in completely saturated condition<br />

but not in half saturated <strong>and</strong> dry conditions<br />

Unstable FS < 1<br />

Unstable in half saturated condition but not<br />

FS > 1<br />

unstable in dry condition<br />

Unconditionally unstable<br />

FS < 1 unstable in dry condition<br />

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Chapter 4: Deterministic models 56<br />

Figure 4.10 <strong>Stability</strong> map based on three steady state scenarios<br />

40<br />

Percentage of area<br />

30<br />

20<br />

10<br />

0<br />

Unconditionally stable<br />

Stable<br />

Moderately stable<br />

Moderately unstable<br />

Unstable<br />

Unconditionally unstable<br />

<strong>Stability</strong> condition<br />

Figure 4.11 Areal distribution of stability classes under three steady state scenarios<br />

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Chapter 4: Deterministic models 57<br />

Figure 4.10 <strong>and</strong> 4.11 show the combined hazard map <strong>and</strong> areal distributions under the three<br />

steady state scenarios. Based on an infinite slope model <strong>and</strong> owing to the considered<br />

parameters, 34.6% of the study area is unconditionally stable, <strong>and</strong> will not fail under any<br />

circumstances unless major destabilizing activities occur. If extreme rainfall event leads to<br />

full soil saturation, 12.4% of the area will face instability under moderate destabilizing<br />

actions, 13.7% of the area will likely fail under minor destabilizing forces <strong>and</strong> 17.7% of the<br />

area needs stabilization methods to control instability. L<strong>and</strong>slides will be mobilized in about<br />

16.7% of the area, if the soil is half saturated. 4.93% of the area will likely fail under any<br />

condition, <strong>and</strong> hence stabilization techniques are recommended.<br />

We generalized from the three steady state scenarios that 21% of the area is under high <strong>and</strong><br />

very high l<strong>and</strong>slide susceptibility zone. An additional 17.67% of the area is categorized under<br />

instability zone with a moderate hazard. The result is quite coherent with the 20% that was<br />

identified with the l<strong>and</strong>slide inventory.<br />

To verify the model output, a cross operation is performed against the l<strong>and</strong>slide database. The<br />

result is summarized in Table 4.12.<br />

Table 4.12 Validation of the model (a) with the whole database (b) with validation group<br />

<strong>Stability</strong> class Observed l<strong>and</strong>slides % of LS <strong>Stability</strong> class Observed l<strong>and</strong>slides % of LS<br />

(# of pixels)<br />

(# of pixels)<br />

Unconditionally stable 435 8.57 Unconditionally stable 156.6 8.31<br />

Stable 249 4.91 Stable 104.58 5.55<br />

Moderately stable 369 7.27 Moderately stable 171 9.08<br />

Moderately unstable 875 17.25 Moderately unstable 360 19.11<br />

Unstable 2180 42.97 Unstable 764 40.56<br />

Unconditionally unstable 965 19.02 Unconditionally unstable 327.4 17.38<br />

On the study area, if slope stability analysis is performed using infinite slope model, 79% any<br />

l<strong>and</strong>slide incidences will be identified in high <strong>and</strong> very high l<strong>and</strong>slide susceptibility zones. An<br />

additional 7% of the failure zones might be regarded to be initiated in long term condition.<br />

However, the model fails to recognize 14% of mobilized l<strong>and</strong>slides under normal<br />

circumstances. Yet, the output obtained is still appreciable provided the following reasons:<br />

While compiling a l<strong>and</strong>slide database, not all l<strong>and</strong>slide depletion areas could be<br />

accurately identified. The reason is the morphology of some erosional belts is difficult<br />

to be interpreted by aerial photographs. On the other h<strong>and</strong>, depositional lobes could be<br />

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Chapter 4: Deterministic models 58<br />

clearly delineated. Therefore, in some instances, the l<strong>and</strong>slide inventory is expected to<br />

contain some depositional areas which will turn out to be stable in the model.<br />

The input data are obtained in different formats. The analysis is performed using three<br />

different softwares. Some data manipulation would be performed well using one<br />

software while other data format will not. So, the analysis is conjugated with data<br />

transformations <strong>and</strong> arrangements. Moreover, the l<strong>and</strong>slide data base is created using<br />

aerial photo interpretation <strong>and</strong> manual delineation on the topographic map using <strong>GIS</strong>.<br />

It is clear that allowable projection <strong>and</strong> consistency errors will be included.<br />

On the coming chapter, we will be dealing with statistical models. As these methods solely<br />

depend on the inventory, the l<strong>and</strong>slide data base will be divided in to two. (1) training mass<br />

movement bodies that will be used to built the model (2) validation l<strong>and</strong>slide bodies which<br />

will be used to check the accuracies. To compare infinite slope model with the statistical<br />

methods, we shall confirm it with the validation group.<br />

Table 4.12(b) shows the cross-checking with validation l<strong>and</strong>slides. The accuracy obtained in<br />

this case is 77% which is almost identical with the one found for the whole data base.<br />

Next step is assessing the combined stability against slope classes,<br />

Percentage<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

Flat Rolling Mountainous Escarpments Cliffs<br />

Unconditionally<br />

stable<br />

Stable<br />

Moderately stable<br />

Moderately unstable<br />

Unstable<br />

Unconditionally<br />

unstable<br />

Figure 4.12 <strong>Stability</strong> under three steady state scenarios vs slope classes<br />

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Chapter 4: Deterministic models 59<br />

Failure is unlikely to occur in any normal circumstance on slopes < 5°. 31% of the area with<br />

slope angle 5°-15° is unstable or moderately unstable, while 20% of it is unconditionally<br />

stable. 9% of mountainous terrain needs stabilization techniques, while 72% of it would likely<br />

fail under minor destabilizing forces when the soil is kept saturated. 57% of the escarpment<br />

<strong>and</strong> 82% of cliffs need stabilization approaches to mitigate slope failures. Well, the results<br />

prove that slopes > 15° are favorable for instability in the study area.<br />

The same assessment is done for geologic layers in Table 4.17.<br />

Table 4.13 <strong>Stability</strong> vs geologic formations<br />

<strong>Stability</strong> classes<br />

Trap Limestone<br />

basalt Marl<br />

Amba<br />

Aradom<br />

S<strong>and</strong>stone<br />

Shale Dolerite<br />

Sill<br />

Shale Marl<br />

Limestone<br />

Marl<br />

Limestone<br />

Endaga<br />

Adigrat<br />

S<strong>and</strong>stone Alluvium Arbi<br />

Glacial<br />

Entcho<br />

S<strong>and</strong>stone<br />

(%) (%) (%) (%) (%) (%) (%) (%) (%) (%) (%)<br />

Unconditionally stable 23.71 37.52 14.02 21.66 70.80 41.46 43.50 18.18 80.82 92.94 61.88<br />

Stable 11.21 13.04 11.06 11.16 8.26 16.27 15.93 5.99 17.81 3.36 6.12<br />

Moderately stable 14.39 15.27 14.04 16.30 8.36 15.77 14.53 7.61 1.37 1.09 5.91<br />

Moderately unstable 26.23 17.73 17.08 29.04 4.69 13.05 14.45 13.03 0.00 0.08 5.84<br />

Unstable 24.44 13.95 27.60 18.42 6.98 12.21 11.58 22.58 0.00 0.00 8.37<br />

Unconditionally unstable 0.02 2.49 16.19 3.41 0.91 1.23 0.00 32.61 0.00 2.52 11.88<br />

32.41% of Adigrat s<strong>and</strong>stone cliffs near NW of the study area will not satisfy mohr-coloumb<br />

criteria under any conditions. 27.6% of Amba Aradom s<strong>and</strong>stone <strong>and</strong> 24.44% of trap basalts<br />

are found to be unstable. 29% of shale <strong>and</strong> 26% of trap basalts are moderately unstable. Trap<br />

basalts contribute the highest areal coverage in the study area as compared with other<br />

formations. In addition, it is likely that the local people tend to settle on the basalts for search<br />

of fertile l<strong>and</strong>s. Therefore, it is concluded that the highest instability risk that would be<br />

considered is on trap basalt formation.<br />

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Chapter 5: Statistical <strong>Analysis</strong> approach<br />

5.1 General<br />

Statistical analysis of slope stability is often indirect. It depends mainly upon a relationship<br />

between past l<strong>and</strong>slides <strong>and</strong> causative factors. The first most important step is identifying<br />

factors whose combinations have led to past failures. This requires a precise observation on<br />

how the failures are triggered. Underst<strong>and</strong>ing the failure mechanisms helps in weighting the<br />

factors beforeh<strong>and</strong>. Quantitative prediction of instability is then made on areas that are free of<br />

l<strong>and</strong>slides but with similar characteristics, with respect to factors inducing l<strong>and</strong>slides. The<br />

second step is recognizing the extent by which different combinations of the factors yield<br />

unstable conditions. In our study, we investigated 10 causative factors: slope, lithology,<br />

elevation, l<strong>and</strong>use, distance to faults, distance to streams, slope shape, aspect, distance to<br />

roads, <strong>and</strong> topographic wetness index. Multiple perspectives of combining the factors are<br />

investigated. The worst scenario with the highest accuracy is then selected. We employed<br />

three combinations:<br />

1: Considering all the 10 factors.<br />

2: Considering the pre-estimated most governing <strong>and</strong> those which are not related to each other<br />

i.e. slope, lithology, distance to faults <strong>and</strong> l<strong>and</strong>use.<br />

3: Considering factors which prove to show a discernible causative relationship with<br />

l<strong>and</strong>slides in the study area, i.e. slope, lithology, l<strong>and</strong>use, aspect <strong>and</strong> slope shape.<br />

Statistical approaches are widely employed in hazard assessment studies. The prominent<br />

features of these methods are high efficiency, low cost, better <strong>and</strong> precise underst<strong>and</strong>ing<br />

between the spatial factors <strong>and</strong> instability. Moreover, inaccurate spatial representations of soil<br />

parameters <strong>and</strong> failure plane assumptions are removed. However, the methods lack<br />

consideration of l<strong>and</strong>slides that exist in areas which are not inventoried. Aerial photograph<br />

interpretation might identify those l<strong>and</strong>slides, but it still depends on the expertise of the<br />

investigator to recognize small scale morphologies. A reliable approach is combining field<br />

investigations <strong>and</strong> aerial photograph interpretation in building the l<strong>and</strong>slide database.<br />

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Chapter 5: Statistical models 61<br />

5.2 Bivariate statistical analysis<br />

The basic idea of bivariate statistical analysis is calculating the densities of l<strong>and</strong>slide<br />

occurrences for each causative factor <strong>and</strong> within its categories. The calculation is used to<br />

drive data driven weights for each factor to contribute to failure. Different combinations of the<br />

weights are applied to obtain a l<strong>and</strong>slide hazard map. In order to apply bivariate analyses,<br />

continuous parameter maps have to be converted into discrete (categorical) maps to compute<br />

the corresponding weight for each class. However, such conversions remain always unclear as<br />

most authors use their expert opinion in dividing the classes (Van Westen, 1993; Soeters <strong>and</strong><br />

Van Westen, 1996). Hence, it is reasonable to argue that the classification of the factors is<br />

rather subjective. But multiple trials of categorization can be considered until a reasonable<br />

causative relationship is attained.<br />

For a bivariate statistical approach, maps of medium scale are most appropriate, in the range<br />

of 1:25000 to 1:500000 (Van Westen et al., 1997), because the technique is not detailed<br />

enough to be applied on a larger scale. In bivariate statistical analysis, the occurrence of mass<br />

movements is related to each causative factor independently <strong>and</strong> the weights of the parameters<br />

are calculated separately. The method relies on the assumption that the relative importance of<br />

the inducing factors is identified by calculating the density of mass movements for each<br />

variable class. Integrating various parameter maps into a new map <strong>and</strong> cross checking with<br />

the l<strong>and</strong>slide data base gives densities per unique combinations.<br />

5.2.1 Statistical index method<br />

The Statistical index method is a bivariate statistical method introduced by Van Westen,<br />

(1997) for l<strong>and</strong>slide susceptibility analysis. A weight value for each categorical unit is defined<br />

as the natural logarithm of the l<strong>and</strong>slide density in the categorical unit divided by the l<strong>and</strong>slide<br />

density in the entire map. This method is based on the following formula (Van Westen, 1997):<br />

Where,<br />

∗<br />

A <br />

W = ln f <br />

f = ln ⎛ A <br />

⎞ ⎛ A ∗<br />

<br />

⎜ A<br />

∗⎟<br />

= ln A<br />

⎜<br />

∗ ⎞<br />

<br />

A <br />

⎟<br />

A<br />

A<br />

⎝ ⎠ ⎝ ⎠<br />

W ij = weight given to a certain class i of parameter j;<br />

f ij = l<strong>and</strong>slide density within class i of parameter j;<br />

(5.1)<br />

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Chapter 5: Statistical models 62<br />

f = l<strong>and</strong>slide density within the entire map;<br />

A ij * = Area of l<strong>and</strong>slides in a certain class i of parameter j;<br />

A ij = Area of a certain class i of parameter j;<br />

A* = Total area of l<strong>and</strong>slides in the entire map;<br />

A = Total area of the entire map.<br />

The weight value for each class is only calculated for those that have l<strong>and</strong>slide observations,<br />

either from field or aerial photograph interpretation. For those instances when no l<strong>and</strong>slide is<br />

identified, the weight will be assigned to zero (Van Westen, 1997). This means that a<br />

parameter class with no l<strong>and</strong>slide incidence will have no sufficient evidence in relation to<br />

future l<strong>and</strong>slide occurrence. Hence, its influence on the calculation of the l<strong>and</strong>slide<br />

susceptibility index will be zero. In this study, every parameter map is crossed with the<br />

l<strong>and</strong>slide map, <strong>and</strong> the density of the l<strong>and</strong>slides in each class is calculated. The distribution of<br />

l<strong>and</strong>slides for various data layers <strong>and</strong> weight values are performed with a script written using<br />

ILWIS – <strong>GIS</strong>. The results are shown in Table 5.1.<br />

We note from the calculation of the weights that:<br />

For slope classes there exists a clear causal relationship between steeper slope angles<br />

<strong>and</strong> l<strong>and</strong>slides. With increasing order of correlation, mountainous terrain, escarpments,<br />

<strong>and</strong> cliffs show a positive relationship with mass movements. Flat <strong>and</strong> rolling terrains<br />

prove to be unfavorable for l<strong>and</strong>slides. Thus, it is concluded that l<strong>and</strong>slides occur in<br />

the study area in areas with slope angle > 15°.<br />

Alluvium, Dolerite sill, Amba Aradom s<strong>and</strong>stone, Trap basalts <strong>and</strong> marl limestone<br />

prove to have properties favorable for instability. The highest area of l<strong>and</strong>slides is<br />

observed for Trap basalts <strong>and</strong> marl limestone. This observation is quite coherent with<br />

the l<strong>and</strong>slide mechanisms explained in chapter 3. The positive correlation attributed to<br />

Adigrat s<strong>and</strong>stone arises from cliff rock fall. However, Agula shale has a negative<br />

weight value. This contradicts with failure mechanism B. The possible reason for this<br />

is the wide area covered by the formation which lowers its l<strong>and</strong>slide density.<br />

According to failure mechanism B, there are l<strong>and</strong>slides mobilized in shale but the flow<br />

is also ascribed with l<strong>and</strong>slides mobilized in Antalo limestone. Considering the<br />

positive correlation of Marl limestone, Amba Aradom s<strong>and</strong>stone, Dolerite sill, <strong>and</strong><br />

trap basalts with instability, we conclude that the three governing l<strong>and</strong>slide<br />

mechanisms are well detected with the statistical index method.<br />

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Chapter 5: Statistical models 63<br />

Table 5.1 Weight assignment, statistical index method<br />

Area of<br />

Area of<br />

Class<br />

Area of observed Weight<br />

Area of observed Weight<br />

Class<br />

category l<strong>and</strong>slides<br />

category l<strong>and</strong>slides<br />

(# of pixels) (# of pixels) (# of pixels) (# of pixels)<br />

<strong>Slope</strong><br />

Flat 13448 1367 -0.73<br />

slope shape<br />

Peak <strong>and</strong> Ridges 11267 2156 -0.07<br />

Rolling 31512 5725 -0.15 Saddle 15745 3380 0.04<br />

Mountanious 10664 3289 0.38 <strong>Slope</strong> Hill 25 5 -0.03<br />

Escarpments 2979 1912 1.12 Convex 8738 1947 0.08<br />

Cliffs 61 51 1.38 Concave 8774 1973 0.09<br />

Total 58664 12344 Gully 13542 2595 -0.07<br />

Lithology<br />

Other 2021 288 -0.37<br />

Trap basalt 12766 3210 0.20 Total 60112 12344<br />

Limestone Marl 5291 611 -0.58 Distance to streams<br />

Amba Aradom S<strong>and</strong>stone 3489 1340 0.63 Very Close 7066 1381 -0.05<br />

Shale 6019 891 -0.33 Close 12703 2592 -0.01<br />

Dolerite Sill 1877 942 0.89 Moderate 11028 2321 0.02<br />

Shale Marl Limestone 10650 1102 -0.69 Fairly Moderate 12883 2784 0.05<br />

Marl Limestone 12093 2888 0.15 Far 12061 2534 0.02<br />

Adigrat S<strong>and</strong>stone 5243 1292 0.18 Very far 4371 732 -0.20<br />

Alluvium 73 49 1.18 Total 60112 12344<br />

Endaga Arbi Glacial 1189 0 0.00 Distance to roads<br />

Entcho S<strong>and</strong>stone 1422 19 -2.73 Close 3234 563 -0.17<br />

Total 60112 12344 Medium 2902 503 -0.17<br />

Elevation<br />

Fairly Far 2661 562 0.03<br />

Low 729 0 0.00 Very Far 51315 10716 0.02<br />

Moderate 2842 0 0.00 Total 60112 12344<br />

Fairly Moderate 17438 2358 -0.42 Aspect<br />

High 33827 8351 0.18 Flat 14 0 0.00<br />

Very High 5276 1634 0.41 N 4686 1118 0.15<br />

Total 60112 12343 NE 8815 1728 -0.05<br />

L<strong>and</strong>use<br />

E 8147 1052 -0.46<br />

Bare Soils 39356 8844 0.09 SE 7097 1354 -0.07<br />

S<strong>and</strong>y/Whitish Clay 3881 521 -0.43 S 8507 1612 -0.08<br />

Urban 0 0 0.00 SW 6647 1092 -0.22<br />

Vegtation 16563 2919 -0.15 W 6433 1540 0.15<br />

Total 59800 12284 NW 6263 1863 0.37<br />

Distance to faults<br />

N2 3436 983 0.33<br />

Very Close 15140 2599 -0.18 Total 60045 12342<br />

Close 12576 2480 -0.04 Wetness index<br />

Moderate 7851 1613 0.00 WI


Chapter 5: Statistical models 64<br />

fairly moderate elevation proves to be unfavorable, while high <strong>and</strong> very high elevation<br />

classes have positive correlations with mass movement.<br />

Concave slope shapes prove to be relatively highly correlated with l<strong>and</strong>slides than<br />

other shapes. Convex, <strong>and</strong> saddle shapes also yield small positive weights<br />

For distance to streams, fairly moderate class yields the highest matching index.<br />

However, all weights observed for distance to stream factor are close to zero. This<br />

means that there is not sufficient evidence to demonstrate a significant positive or<br />

negative relationship between distance to streams <strong>and</strong> l<strong>and</strong>slides.<br />

For distance to roads, our results depict an unclear causal association between this<br />

factor <strong>and</strong> instability.<br />

North, Northwest <strong>and</strong> West facing slopes prove to be positively related with mass<br />

movements in a decreasing order. On the other h<strong>and</strong>, those slopes which face opposite<br />

to the formers, East, Southwest, <strong>and</strong> South, turn out to be most unfavorable to<br />

l<strong>and</strong>slides.<br />

Bare soils are observed to be highly affected by l<strong>and</strong>slides. Moreover, the highest area<br />

of observed l<strong>and</strong>slides is in this category. While vegetation, as expected, proves to<br />

have a negative relationship with l<strong>and</strong>slides.<br />

For distance to fault, unlike to what was expected, the highest positive matching is<br />

observed for moderately far <strong>and</strong> far distances to faults, <strong>and</strong> the lowest correlation<br />

occur in very close <strong>and</strong> close categories. As distance to faults is one of the important<br />

factors inducing l<strong>and</strong>slides, this seems eccentric. First, to investigate if the discrepancy<br />

happens to be from the factor employed, another consideration is checked i.e. using<br />

fault density. The fault density is calculated to be the total length of fault over a<br />

r<strong>and</strong>om square unit of 300m x 300m. Another zoning is also tried for total fault length<br />

over each lithological unit. The results in both cases remain to be the same as to what<br />

we found for distance to faults. Therefore, the explanation is as follows: faults <strong>and</strong><br />

fractures affect the stability of earthen slopes by destroying the anchorage between<br />

soil grains. This decreases the shear strength of the soil. However, failure will only<br />

occur provided the mobilized shear stress is greater than the shear strength. If the<br />

intensity of fracturing is not strong enough to reduce the strength below the stress,<br />

failure will not occur. In addition, if the faulting activity has ceased then the shear<br />

strength is not expected to decrease any further. Also, there will be no effect of<br />

faulting, if the direction it occurs is opposite to the failure plane. Most of the very high<br />

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Chapter 5: Statistical models 65<br />

fault density zones exist in Adigrat s<strong>and</strong>stone formation which has a large shear<br />

strength. They also exist on flat <strong>and</strong> rolling terrains with quite low slope angles, which<br />

yield a small value for the mobilized shear stress. Hence, we conclude that though<br />

faulting is an important inducing factor for destabilizing slopes, it is not observed to<br />

significantly destabilize slopes in Hagere Selam.<br />

For the topographic wetness index, those localities with a TWI < 2.5 prove to be<br />

significantly affected by l<strong>and</strong>slides.<br />

The weights of the causative factors are summed to obtain a l<strong>and</strong>slide susceptibility map:<br />

Where:<br />

LSI: l<strong>and</strong>slide susceptibility index<br />

<br />

LSI = W <br />

<br />

(5.2)<br />

W ij : weight of class i in parameter j<br />

n: number of causative factors combined<br />

5.2.1.1 Considering all factors (SI model 1)<br />

The l<strong>and</strong>slide susceptibility index, LSI, is established in ILWIS software using formula 5.2.<br />

The minimum value obtained for the entire map is -5.28 while the maximum is 2.946. The<br />

Mean value is -0.58 <strong>and</strong> st<strong>and</strong>ard deviation is 1.67. To finalize the hazard zonation map, the<br />

LSI map is classified on the basis of the relationship between LSI values <strong>and</strong> observed<br />

l<strong>and</strong>slides. Usually, the LSI frequency diagram <strong>and</strong> l<strong>and</strong>slide occurrences are matched <strong>and</strong><br />

used for the l<strong>and</strong>slide hazard zonation. However, this is not straight forward as there are no<br />

statistical rules which can categorize continuous data automatically (Ayalew et al., 2004;<br />

Long, 2008). The problems of transforming a continuous data set into a categorical unit seem<br />

to be unclear, as most researchers employ subjective approaches. In this study, we adopted the<br />

manual classifier method to classify the LSI values into five different susceptibility zones.<br />

The l<strong>and</strong>slide susceptibility classes are: very low, low, moderate, high <strong>and</strong> very high.<br />

The l<strong>and</strong>slide database is divided in to two groups. The first group contains training pixels<br />

that are to be employed for classifying the LSI map <strong>and</strong> the second group containing<br />

validation pixels. The proportion of training <strong>and</strong> validation pixels is considered to be 60% <strong>and</strong><br />

40% respectively.<br />

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Chapter 5: Statistical models 66<br />

Normally, the classification procedure shall satisfy the principle that higher l<strong>and</strong>slide<br />

susceptibility classes should indicate more l<strong>and</strong>slide events than lower l<strong>and</strong>slide susceptibility<br />

classes. Therefore, it is assumed that the expected number of training pixels within a higher<br />

l<strong>and</strong>slide susceptibility class equals two times than that of the expected numbers in the next<br />

lower l<strong>and</strong>slide susceptibility class (Long, 2008). For instance, the expected number of<br />

training l<strong>and</strong>slide pixels in the low l<strong>and</strong>slide susceptibility class should equal two times the<br />

expected numbers in the very low l<strong>and</strong>slide susceptibility class, <strong>and</strong> so on. Thus, it can be<br />

shown that, if X is the percentage of training l<strong>and</strong>slide pixels in the very low l<strong>and</strong>slide hazard<br />

class:<br />

31X = 100%, ⤇ X = 3.225%<br />

Similarly, the percentages of training l<strong>and</strong>slide pixels in low, moderate, high <strong>and</strong> very high<br />

classes would be 6.45%, 12.9%, 25.8% <strong>and</strong> 51.6% respectively.<br />

The l<strong>and</strong>slide occurrence map is compared to the LSI values, <strong>and</strong> the cumulative percentage<br />

of training l<strong>and</strong>slide pixels against its LSI values is arranged in an ascending order. Four<br />

cutoff percentages of the cumulative percentage are used to identify the five l<strong>and</strong>slide hazard<br />

zones. The cutoff values are 3.225% for separating very low to low, 9.65% for separating the<br />

low from the moderate class, 22.55% for separating the moderate from high class, <strong>and</strong> finally<br />

48.35% for separating the high from the very high class. At the cutoff points, the<br />

corresponding LSI cutoff values are determined, <strong>and</strong> the map of l<strong>and</strong>slide susceptibility<br />

zonation is created from the LSI map using the respective LSI cutoff values. The procedure is<br />

shown in Figure 5.1.<br />

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Chapter 5: Statistical models 67<br />

Figure 5.1 Percentage of observed training l<strong>and</strong>slides versus LSI (SI model 1)<br />

The cutoff l<strong>and</strong>slide statistical index values are:<br />

‣ Very low l<strong>and</strong>slide susceptibility: LSI < -1.30<br />

‣ Low l<strong>and</strong>slide susceptibility: -1.30 ≤ LSI < -0.69<br />

‣ Moderate l<strong>and</strong>slide susceptibility: -0.69 ≤ LSI < -0.15<br />

‣ High l<strong>and</strong>slide susceptibility: -0.15 ≤ LSI < 0.45<br />

‣ Very high l<strong>and</strong>slide susceptibility: LSI ≥ 0.46<br />

The final hazard map <strong>and</strong> the areal distribution of each susceptibility classes are shown in<br />

Figure 5.2 <strong>and</strong> Figure 5.3 respectively. It is observed that very low, low, moderate, high <strong>and</strong><br />

very high susceptibility classes represent, 17%, 24%, 26%, 14% <strong>and</strong> 19% of the study area.<br />

The very high <strong>and</strong> high hazard classes are considered to be representative for future l<strong>and</strong>slide.<br />

While the total area of l<strong>and</strong>slides inventoried was about 20% of the study area, the total area<br />

of high <strong>and</strong> very high susceptibility classes comprise about 33%.<br />

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Figure 5.2 L<strong>and</strong>slide hazard map (SI model 1)<br />

30<br />

25<br />

20<br />

15<br />

10<br />

Area (%)<br />

5<br />

0<br />

Very low LSS Low LSS Moderate LSS High LSS Very high LSS<br />

Figure 5.3 Areal distribution of susceptibility classes (SI model 1)<br />

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Chapter 5: Statistical models 69<br />

To validate the final output, the hazard map is cross checked with validation l<strong>and</strong>slide bodies.<br />

To perform this, a cross operation is done between the validation l<strong>and</strong>slide pixels <strong>and</strong> the<br />

categorized susceptibility map, using ILWIS <strong>GIS</strong>. The result is shown in the Table 4.15.<br />

Table 5.2 Validation of SI model 1<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (pix) Percentage<br />

Very low 24 1.20<br />

Low 94 4.63<br />

Moderate 413 20.37<br />

High 362 17.83<br />

Very high 1135 55.97<br />

Total 2028.40 100.00<br />

Hence, considering all the 10 causative factors as equally important to failure <strong>and</strong> future<br />

l<strong>and</strong>sliding, the statistical index model 1 identifies the l<strong>and</strong>slide activities in the study area<br />

with 74% accuracy, as it assigns 56% <strong>and</strong> 18% of actual failure zones to the very high <strong>and</strong><br />

high susceptibility classes. 20% of the l<strong>and</strong>slide incidences are in the moderate hazard zone<br />

<strong>and</strong> 5.63% in the low <strong>and</strong> very low risk zones.<br />

5.2.1.2 Considering the pre-estimated most governing factors (SI model 2)<br />

<strong>Slope</strong>, lithology, distance to faults <strong>and</strong> l<strong>and</strong>use are pre-estimated to be most governing as<br />

compared to the other factors. In addition, those factors are not related to each other. Hence a<br />

LSI map is created using only those factors. The minimum value of LSI obtained is -3.54 <strong>and</strong><br />

the maximum is 2.29. The mean value is -0.19 <strong>and</strong> the st<strong>and</strong>ard deviation is 1.25. The LSI<br />

map is classified on the basis of the relationship between LSI values <strong>and</strong> training l<strong>and</strong>slide<br />

bodies, as explained before.<br />

The cutoff l<strong>and</strong>slide statistical index values are:<br />

‣ Very low l<strong>and</strong>slide susceptibility: LSI < -1.45<br />

‣ Low l<strong>and</strong>slide susceptibility: -1.45 ≤ LSI < -0.84<br />

‣ Moderate l<strong>and</strong>slide susceptibility: -0.84 ≤ LSI < 0.16<br />

‣ High l<strong>and</strong>slide susceptibility: 0.16 ≤ LSI < 0.42<br />

‣ Very high l<strong>and</strong>slide susceptibility: LSI ≥ 0.42<br />

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Chapter 5: Statistical models 70<br />

Figure 5.4 Percentage of observed training l<strong>and</strong>slides versus LSI (SI model 2)<br />

The final hazard map <strong>and</strong> the areal distribution of each susceptibility classes are shown in<br />

Figure 5.5 <strong>and</strong> 5.6 respectively. It is observed that very low, low, moderate, high <strong>and</strong> very<br />

high susceptibility categories constitute 25%, 12%, 32%, 12% <strong>and</strong> 19% of the study area. The<br />

total area of l<strong>and</strong>slides inventoried was about 20% of the study area. The statistical index<br />

method of analysis, model 2, predicts that 31% of the area is high or very high l<strong>and</strong>slide<br />

susceptibility class. Compared with model 1, this is only 2% less.<br />

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Chapter 5: Statistical models 71<br />

Figure 5.5 L<strong>and</strong>slide hazard map (SI model 2)<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

Area (%)<br />

5<br />

0<br />

Very low ls. s. Low ls. s. Moderate ls. s. High ls. s. Very high ls. s.<br />

Figure 5.6 Areal distribution of susceptibility classes (SI model 2)<br />

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Chapter 5: Statistical models 72<br />

To validate the final output, we made a cross operation between the validation l<strong>and</strong>slides<br />

pixels <strong>and</strong> the categorized hazard map of SI model 2. The result is shown in the Table 5.3.<br />

Table 5.3 Validation of SI model 2<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (pix) Percentage<br />

Very low 38 1.85<br />

Low 137 6.74<br />

Moderate 472 23.26<br />

High 300 14.78<br />

Very high 1083 53.36<br />

Total 2029 100.00<br />

Considering only slope, lithology, distance to faults <strong>and</strong> l<strong>and</strong>use as factors equally important<br />

to failure <strong>and</strong> future l<strong>and</strong>sliding, the statistical l<strong>and</strong>slide index model 2 envisages the l<strong>and</strong>slide<br />

activities in the study area with 69% accuracy. It designates 54% <strong>and</strong> 15% of the l<strong>and</strong>slide<br />

zones to the very high <strong>and</strong> high susceptibility classes. In addition, 23% of the unstable units<br />

are specified in the moderate risk zone, <strong>and</strong> about 9% in the low <strong>and</strong> very low susceptibility<br />

classes.<br />

5.2.1.3 Considering factors which show clear causative relationship with<br />

l<strong>and</strong>slides (SI model 3)<br />

During the statistical weight analysis, the causative factors slope, lithology, l<strong>and</strong>use, aspect<br />

<strong>and</strong> slope shape gave a reasonable causative association with the inventory compared to the<br />

other factors. Therefore, a LSI map is created using those factors. The minimum LSI value<br />

obtained is -4.19 while the maximum is 2.52. The mean value is -0.34 <strong>and</strong> the st<strong>and</strong>ard<br />

deviation is 1.29. The cutoff l<strong>and</strong>slide statistical index values are:<br />

‣ Very low l<strong>and</strong>slide susceptibility: LSI < -1.17<br />

‣ Low l<strong>and</strong>slide susceptibility: -1.17 ≤ LSI < -0.28<br />

‣ Moderate l<strong>and</strong>slide susceptibility: -0.28 ≤ LSI < 0.16<br />

‣ High l<strong>and</strong>slide susceptibility: 0.16 ≤ LSI < 0.32<br />

‣ Very high l<strong>and</strong>slide susceptibility: LSI ≥ 0.32<br />

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Chapter 5: Statistical models 73<br />

Figure 5.7 % of observed training l<strong>and</strong>slides VS LSI (SI model3)<br />

The areal distribution of each susceptibility class <strong>and</strong> the final hazard map are shown in<br />

Figure 5.8 <strong>and</strong> Figure 5.9 respectively. It is observed that very low, low, moderate, high <strong>and</strong><br />

very high susceptibility classes constitute 14.15%, 24.18%, 28.7%, 13.58% <strong>and</strong> 19.28% of the<br />

study area. With statistical index method of analysis, considering only the 5 factors which<br />

have a clear causative relationship with l<strong>and</strong>slides, the total area of high <strong>and</strong> very high<br />

susceptibility classes is 33%.<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

Area (%)<br />

5<br />

0<br />

Low ls. s. Very low ls. s. Moderate ls. s. High ls. s. Very high ls. s.<br />

Figure 5.8 Areal distribution of susceptibility classes (SI model 3)<br />

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Chapter 5: Statistical models 74<br />

Figure 5.9 L<strong>and</strong>slide hazard map (SI model 3)<br />

To validate the final output, the hazard map is cross checked with validation l<strong>and</strong>slide bodies.<br />

A cross operation is done between the validation l<strong>and</strong>slides <strong>and</strong> the categorized susceptibility<br />

map. The result is shown in the Table 5.4.<br />

Table 5.4 Validation SI model 3<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (Pix) Percentage<br />

Very low 20 0.97<br />

Low 103 5.07<br />

Moderate 412 20.33<br />

High 367 18.10<br />

Very high 1126 55.53<br />

Total 2028 100.00<br />

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Chapter 5: Statistical models 75<br />

The causative factors slope, lithology, L<strong>and</strong>use, aspect <strong>and</strong> slope shape gave a reasonable<br />

causative association with the inventory. A l<strong>and</strong>slide statistical index model performed<br />

considering only those factors as equally important to future instability detects the l<strong>and</strong>slide<br />

incidences with 74% accuracy. It designates 56% <strong>and</strong> 18% of mass movement zones to the<br />

very high <strong>and</strong> high susceptibility classes. 20% of unstable zones are allotted to zones of<br />

moderate risk. If a l<strong>and</strong>slide hazard analysis is performed using this model in Hagere Selam, it<br />

is highly probable that 6% of actual failure zones will not be recognized.<br />

5.2.2 Statistical weighting factor analysis<br />

The statistical index method considers each causative factor to be equally responsible for past<br />

l<strong>and</strong>slides. It assumes future failure estimates is based on equal consideration of the inducing<br />

factors. Practically, however, this hardly will be true. A closer look at the result obtained from<br />

the weight-factor relationship (Table 5.1) shows significant differences between the<br />

importances of causative factors in triggering l<strong>and</strong>slides. Statistical weighting factor analysis<br />

is a method that assigns data driven weights to each inducing parameter, so that the<br />

contribution of one parameter is different from the others (Cevik & Topal, 2003; Oztekin et<br />

al., 2005; Voogd, 1983). A weighting factor is calculated as:<br />

W =<br />

T − Min (T )<br />

Max (T ) − Min (T )<br />

(5.3)<br />

Where<br />

W = weighting factor calculated for layer, j.<br />

T = Total weighting index value of all l<strong>and</strong>slide cells for layer, j<br />

Min (T ) = Minimum T value<br />

Max (T ) =Maximum T value<br />

The W values are calculated using ILWIS-<strong>GIS</strong>. The procedures followed are:<br />

<br />

<br />

The l<strong>and</strong>slides database is cross multiplied with the w ij value map of each causative<br />

factor (parameter).<br />

The summed weight values of all cells within l<strong>and</strong>slide bodies are calculated for each<br />

parameter.<br />

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Chapter 5: Statistical models 76<br />

The resulting weighting factor values considering all the 10 inducing factors are given in<br />

Table 5.5.<br />

Table 5.5 Weighting factor values<br />

Causative factor (j) T j W fj<br />

<strong>Slope</strong> 1625.38 1.00<br />

Lithology 1609.95 0.99<br />

Elevation 1225.18 0.75<br />

<strong>Slope</strong> shape 51.14 0.02<br />

Distance to streams 23.00 0.00<br />

Distance to Road 17.50 0.00<br />

Aspect 367.33 0.22<br />

L<strong>and</strong> Use 125.30 0.07<br />

Distance to faults 96.40 0.05<br />

Wetness index 259.51 0.15<br />

From the weighting factor outputs, slope is the most influential factor to instability;<br />

lithology has nearly the same effect as slope.<br />

Elevation, aspect, wetness index <strong>and</strong> l<strong>and</strong>use have moderate but important<br />

contribution.<br />

Distances to road, <strong>and</strong> distance to stream have no significant contribution to<br />

l<strong>and</strong>slides in the study area.<br />

The l<strong>and</strong>slide susceptibility index is calculated using:<br />

<br />

LSI = W W <br />

<br />

(5.4)<br />

Where<br />

W = Weighting factor calculated for layer j.<br />

W ij = Weight of class i in parameter j<br />

n = number of causative factors combined<br />

5.2.2.1 SWF modeling results<br />

The procedure is similar to what was explained for the statistical index modeling, paragraph<br />

5.2.1, but the LSI map is calculated using equation 5.4.<br />

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Chapter 5: Statistical models 77<br />

Figure 5.10 Percentage of observed training l<strong>and</strong>slides versus LSI. Model 1 (A), Model 2 (B), <strong>and</strong> Model 3 (C)<br />

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Chapter 5: Statistical models 78<br />

Table 5.6 Parameters of LSI map <strong>and</strong> cutoff values<br />

SWF_ Model 1 SWF_ Model 2 SWF_ Model 3<br />

Mean LSI -0.21 0.10 -0.15<br />

Min LSI -3.79 -3.44 -3.55<br />

Max LSI 2.30 2.06 2.12<br />

St<strong>and</strong>ard deviation 0.95 1.03 1.06<br />

Cut off values<br />

Very low [-3.79, -0.90) [-3.44, -1.03) [-3.55, -1.20)<br />

Low [ -0.90, -0.55) [-1.03, -0.56) [-1.20, -0.58)<br />

Moderate [-0.55, -0.24) [-0.56, -0.32) [-0.58, -0.28)<br />

High [-0.24, 0.35) [-0.32, 0.07) [-0.28, 0.10)<br />

Very high [0.35, 2.30] [0.07, 2.06] [0.10, 2.12]<br />

Figure 5.10 presents the manual classification procedure to classify the numerical LSI values<br />

to a categorical map. Table 5.6 depicts the parameters of the entire LSI maps <strong>and</strong> boundary<br />

values used for the classification. The areal distribution of the l<strong>and</strong>slide categories is given in<br />

Figure 5.6.<br />

35<br />

30<br />

25<br />

Area (%)<br />

20<br />

15<br />

10<br />

5<br />

SWF_model 1<br />

SWF_model 2<br />

SWF_model 3<br />

0<br />

Low Very low Moderate High Very high.<br />

L<strong>and</strong>slide susceptibility category<br />

Figure 5.11 Areal distribution of susceptibility classes<br />

From Figure 5.11, it is apparent that there are slight differences between the three approaches<br />

followed. Considering all the 10 selected factors, <strong>and</strong> employing statistical weighting factor<br />

method of analysis, the area identified as high <strong>and</strong> very high hazard zone is 32%. An<br />

additional 28.65% is regarded as a zone of possible failure with a moderate hazard. It is<br />

recalled that the area of l<strong>and</strong>slides recognized during the inventory was about 20%.<br />

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Chapter 5: Statistical models 79<br />

If only slope, lithology, distance to faults <strong>and</strong> l<strong>and</strong>use were the only factors responsible for the<br />

instability, the prediction of high <strong>and</strong> very high l<strong>and</strong>slide susceptibility zones is 35.4%. In<br />

addition some 27% of the area, 135km², is a zone of possible failure with moderate hazard.<br />

If slope, lithology, l<strong>and</strong>use, aspect <strong>and</strong> slope shape are the only responsible factors for the<br />

mass movements in the study area, the high <strong>and</strong> very high hazard zone amounts to about 35%.<br />

In addition, the moderate l<strong>and</strong>slide susceptibility zone is about 27.38% of the area.<br />

SWF model 2 <strong>and</strong> SWF model 3 are comparatively identical. However, SWF model 1 gives<br />

somewhat a smaller value.<br />

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Chapter 5: Statistical models 80<br />

Figure 5.12 L<strong>and</strong>slide hazard map (a) SWF model 1, (b) SWF model 2<br />

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Chapter 5: Statistical models 81<br />

Figure 5.13 L<strong>and</strong>slide hazard map (a) SWF model 3<br />

The accuracy of the results obtained using SWF models are verified by a cross validation of<br />

the final hazard maps with the validation l<strong>and</strong>slides. Table 5.7 shows the results.<br />

Table 5.7 Validation of SWF models<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (npix) Percentage<br />

Very low 24 1.27<br />

Low 83 4.38<br />

Moderate 318 16.77<br />

High 335 17.67<br />

Very high 1136 59.92<br />

Total 1896 100.00<br />

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Chapter 5: Statistical models 82<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (npix) Percentage<br />

Very low 16 0.84<br />

Low 76 4.01<br />

Moderate 194 10.23<br />

High 396 20.89<br />

Very high 1214 64.03<br />

Total 1896 100.00<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (npix) Percentage<br />

Very low 15 0.79<br />

Low 81 4.27<br />

Moderate 234 12.34<br />

High 361 19.04<br />

Very high 1205 63.55<br />

Total 1896 100.00<br />

Hence, considering all the 10 causative factors being variably important to failure <strong>and</strong> future<br />

l<strong>and</strong>sliding, SWF model 1 recognizes the validation l<strong>and</strong>slides in the study area with 78%<br />

accuracy. It specifies 60% <strong>and</strong> 18% of the actual mass movement zones in the very high <strong>and</strong><br />

high susceptibility zones respectively. In addition, 17% of the incidences are regarded in the<br />

moderate hazard zone. The final method fails to identify 5% of the validation l<strong>and</strong>slides.<br />

SWF model 2 <strong>and</strong> model 3 predict the l<strong>and</strong>slide activities with 85% <strong>and</strong> 84% accuracies<br />

respectively. The failure to predict the validation l<strong>and</strong>slides is about 5% for both models.<br />

Therefore, we conclude that varying the triggering factors improves the accuracy as far as<br />

weighting factor method is concerned. A model based on all triggering factors is proved to be<br />

less efficient than models based on selected triggering factors.<br />

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5.2.3 Certainty factor analysis<br />

Among the commonly used <strong>GIS</strong> analysis models for l<strong>and</strong>slide hazard mapping, certainty<br />

factor model has been profoundly considered <strong>and</strong> experimentally investigated to be beneficial<br />

(Chung & Fabbri, 1993; Chung & Leclerc, 1994; Binaghi et al., 1998). The Certainty Factor<br />

(CF) approach is a favorability function that h<strong>and</strong>les the problem of combining many data<br />

layers, heterogeneity <strong>and</strong> uncertainty of input data (Chung & Fabbri, 1993). The Certainty<br />

Factor at each pixel p, denoted with CF k (p) is defined as the change in certainty that a<br />

proposition is true (i.e. an area is l<strong>and</strong>slide prone) from without the evidence to given the<br />

evidence at p for each data layer (Chung & Leclerc, 1994; Binaghi et al., 1998). ‘No<br />

evidence’ means prior probability of having a l<strong>and</strong>slide in a study area <strong>and</strong> ‘with evidence’<br />

means the conditional probability of having a l<strong>and</strong>slide given a certain class of a causative<br />

factor.<br />

Where:<br />

⎧ f − f<br />

⎪f (1 − f) if f ≥ f<br />

CF =<br />

⎨ f − f<br />

⎪<br />

⎩f(1 − f ) if f < f<br />

CF ij - certainty factor given to class i of parameter j;<br />

f ij - the l<strong>and</strong>slide density within the class i of parameter j;<br />

f - The l<strong>and</strong>slide density within the entire map.<br />

(5.5)<br />

Statistically, f ij is the conditional probability having a number of l<strong>and</strong>slide occurrence in class<br />

i of a causative factor j, <strong>and</strong> f is the prior probability of total number of l<strong>and</strong>slide occurrences<br />

in the study area.<br />

The range of values of the CF is [−1, 1] <strong>and</strong> positive values indicate an increase in certainty,<br />

after evidence is observed, while negative numbers imply a decrease in certainty. A value of -<br />

1 indicates a maximum disfavoring effect <strong>and</strong> +1 show the strongest causative link between<br />

the class considered <strong>and</strong> l<strong>and</strong>slides. A value close to 0 means that the prior probability is very<br />

similar to the conditional one, so it is not possible to give any indication about the certainty of<br />

the proposition.<br />

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Chapter 5: Statistical models 84<br />

Table 5.1 gives the l<strong>and</strong>slide densities for each category of the causative factors. <strong>Using</strong><br />

equation 5.5, the certainty factor values are calculated on the basis of the conditions set. The<br />

results are presented in Table 5.8.<br />

Table 5.8 Certainty factor values<br />

Class<br />

Area of<br />

catagory<br />

Area of<br />

observed<br />

l<strong>and</strong>slides f ij f CF<br />

(# of pixels) (# of pixels)<br />

<strong>Slope</strong><br />

Flat 13448 1367 0.10 0.21 -0.58<br />

Rolling 31512 5725 0.18 0.21 -0.17<br />

Mountanious 10664 3289 0.31 0.21 0.40<br />

Escarpments 2979 1912 0.64 0.21 0.85<br />

Cliffs 61 51 0.84 0.21 0.95<br />

Lithology<br />

Trap basalt 12766 3210 0.25 0.21 0.23<br />

Limestone Marl 5291 611 0.12 0.21 -0.49<br />

Amba Aradom S<strong>and</strong>stone 3489 1340 0.38 0.21 0.59<br />

Shale 6019 891 0.15 0.21 -0.33<br />

Dolerite Sill 1877 942 0.50 0.21 0.74<br />

Shale Marl Limestone 10650 1102 0.10 0.21 -0.55<br />

Marl Limestone 12093 2888 0.24 0.21 0.18<br />

Adigrat S<strong>and</strong>stone 5243 1292 0.25 0.21 0.21<br />

Alluvium 73 49 0.67 0.21 0.87<br />

Endaga Arbi Glacial 1189 0 0.00 0.21 -1.00<br />

Entcho S<strong>and</strong>stone 1422 19 0.01 0.21 -0.95<br />

Elevation<br />

Low 729 0 0.00 0.21 -1.00<br />

Moderate 2842 0 0.00 0.21 -1.00<br />

Fairly Moderate 17438 2358 0.14 0.21 -0.39<br />

High 33827 8351 0.25 0.21 0.21<br />

Very High 5276 1634 0.31 0.21 0.42<br />

<strong>Slope</strong> shape<br />

Peak <strong>and</strong> Ridges 11267 2156 0.19 0.21 -0.08<br />

Saddle 15745 3380 0.21 0.21 0.05<br />

<strong>Slope</strong> Hill 25 5 0.20 0.21 -0.03<br />

Convex 8738 1947 0.22 0.21 0.10<br />

Concave 8774 1973 0.22 0.21 0.11<br />

Gully 13542 2595 0.19 0.21 -0.08<br />

Other 2021 288 0.14 0.21 -0.36<br />

Topographic wetness index<br />

WI


Chapter 5: Statistical models 85<br />

Class<br />

Area of<br />

catagory<br />

Area of<br />

observed<br />

l<strong>and</strong>slides f ij f CF<br />

(# of pixels) (# of pixels)<br />

Distance to streams<br />

Very Close 7066 1381 0.20 0.21 -0.06<br />

Close 12703 2592 0.20 0.21 -0.01<br />

Moderate 11028 2321 0.21 0.21 0.03<br />

Fairly Moderate 12883 2784 0.22 0.21 0.06<br />

Far 12061 2534 0.21 0.21 0.03<br />

Very far 4371 732 0.17 0.21 -0.22<br />

Distance to road<br />

Close 3234 563 0.17 0.21 -0.18<br />

Medium 2902 503 0.17 0.21 -0.19<br />

Fairly Far 2661 562 0.21 0.21 0.03<br />

Very Far 51315 10716 0.21 0.21 0.02<br />

Aspect<br />

Flat 14 0 0.00 0.21 -1.00<br />

N 4686 1118 0.24 0.21 0.18<br />

NE 8815 1728 0.20 0.21 -0.06<br />

E 8147 1052 0.13 0.21 -0.43<br />

SE 7097 1354 0.19 0.21 -0.09<br />

S 8507 1612 0.19 0.21 -0.10<br />

SW 6647 1092 0.16 0.21 -0.24<br />

W 6433 1540 0.24 0.21 0.18<br />

NW 6263 1863 0.30 0.21 0.39<br />

N2 3436 983 0.29 0.21 0.36<br />

L<strong>and</strong>use factor<br />

Bare Soils 39356 8844 0.22 0.21 0.11<br />

S<strong>and</strong>y/Whitish Clay 3881 521 0.13 0.21 -0.40<br />

Urban 0 0 0.00 0.21 0.00<br />

Vegtation 16563 2919 0.18 0.21 -0.17<br />

Distance to faults<br />

Very Close 15140 2599 0.17 0.21 -0.20<br />

Close 12576 2480 0.20 0.21 -0.05<br />

Moderate 7851 1613 0.21 0.21 0.00<br />

Moderately far 5820 1410 0.24 0.21 0.19<br />

Far 7681 1958 0.25 0.21 0.24<br />

Very far 11044 2284 0.21 0.21 0.01<br />

From the results of the certainty factor calculation the following conclusions are drawn:<br />

The degree of certainty of a l<strong>and</strong>slide incidence is the highest for cliffs. <strong>Slope</strong> angles<br />

> 15° are likely to fail, while slope angles < 15° are less prone to instability.<br />

Alluvium shows the highest CF value (0.87). Therefore, it is highly prone to mass<br />

movements. Dolerite sill, Amba Aradom s<strong>and</strong>stone <strong>and</strong> trap basalts show also very<br />

high CF values, indicating their susceptibility to l<strong>and</strong>slides. Thus, failure mechanisms<br />

A <strong>and</strong> C, discussed in chapter 3, are well expressed by the analysis. Marl limestone<br />

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Chapter 5: Statistical models 86<br />

formation shows a CF value of 0.18; however shale indicates a negative certainty<br />

factor value of -0.33. This is a discrepancy as far as l<strong>and</strong>slide failure mechanism B is<br />

concerned. We believe, this has got to do with the large areal coverage of the shale<br />

formation. Though there are failures in this layer, there exist also equally many pixels<br />

with no l<strong>and</strong>slide incidence that make the favorability function become negative.<br />

Elevation proves to be a strong casual factor to instability. Areas with elevation ><br />

2200 m are highly prone to failure while areas with elevation < 2220 m are not<br />

favorable for l<strong>and</strong>slides.<br />

Concave slope shapes show a CF value of 0.11, thus are prone to failure. Convex<br />

shapes also have a positive contribution to mass movements. The other slope shapes<br />

indicate negative values close to zero. Therefore there is no indication that these<br />

shapes favor instability.<br />

Very far distance to a stream proves to be unlikely to failure. The other distance to<br />

stream classes do not have a strong casual link with l<strong>and</strong>slides.<br />

The CF values for distance to road factor clearly show a weak causal link between the<br />

factor <strong>and</strong> instability.<br />

For aspect, a distinct result is obtained. North, Northwest <strong>and</strong> West facing slopes<br />

prove to be highly prone to instability. Opposite facing slopes, East, Southwest <strong>and</strong><br />

South, are unfavorable for l<strong>and</strong>slides.<br />

For distance to faults, the same result as obtained with the statistical index analysis is<br />

observed here. Recalling the same reasoning that was given in section 5.1, it is<br />

concluded that we haven’t observed a sufficient evidence for the causal relationship<br />

between faulting <strong>and</strong> mass movements.<br />

For l<strong>and</strong>use, it can be said that there is a negative effect of the presence of vegetation<br />

to slope instability while bare soils are susceptible to sliding.<br />

The CF is calculated for each inducing factor. The layers are then combined pairwise. The<br />

combination of two CF’s, X <strong>and</strong> Y, due to two different layers of information, is expressed as<br />

Z in equation 5.6 (Long, 2008).<br />

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Chapter 5: Statistical models 87<br />

X + Y − XY if, X, Y ≥ 0<br />

⎧<br />

X + Y<br />

Z =<br />

if X ∗ Y < 0<br />

⎨1 − min(/X/,/Y/)<br />

⎩ X + Y + XY if X, Y < 0<br />

(5.6)<br />

The pairwise combination of causative factors is performed repeatedly using a script written<br />

in ILWIS <strong>GIS</strong> using the integration rule of equation (5.6). The triggering factors to be<br />

considered are different for the three models speculated, as discussed earlier.<br />

5.2.3.1 CF modeling results<br />

Table 5.9 Parameters of the CF map <strong>and</strong> cutoff values<br />

CF_ Model 1 CF_ Model 2 CF_ Model 3<br />

Mean CF 0.05 0.15 0.03<br />

Min CF -1.00 -1.00 -1.00<br />

Max CF 1.00 0.99 0.99<br />

St<strong>and</strong>ard deviation 0.81 0.74 0.74<br />

Cut off values<br />

Very low [-1, -0.856) [-1, -0.81) [-1, -0.74)<br />

Low [-0.86, -0.61) [-0.81, -0.61) [-0.74, -0.6)<br />

Moderate [-0.61, -0.03) [-0.61, -0.14) [-0.6, -0.26)<br />

Uncertain 0 0 0<br />

High [-0.03, 0.6) [-0.14, 0.4) [-0.26, 0.34)<br />

Very high [0.6, 1] [0.4, 0.99] [0.34, 0.99]<br />

The maximum CF value is 1, as obtained from CF model 1. Thus, the highest certainity for a<br />

l<strong>and</strong>slide occurance is obtained when all triggering factors are taken into account. Figure 5.14<br />

demonstrates the procedure adopted to classify the discrete CF maps to catagorical l<strong>and</strong>slide<br />

hazard maps. Figure 5.14D shows the areal distribution of the susceptibility classes. It is noted<br />

that CF_model 1 <strong>and</strong> model 2 predict over 40% of the area to be under l<strong>and</strong>slide risk. This<br />

value exceeds the inventoried area by 99km². On the other h<strong>and</strong> CF_model 3 estimates the<br />

unstable area to be about 31%, which exceeds the inventoried area by 54km². the reliability of<br />

a model is assesed by looking into the extent by which it identifies the inventoried l<strong>and</strong>slides.<br />

However, identifying the existing failures by itself is not a sufficient condition for the<br />

dependability of a model. This is because; an overestimated output could have a clean<br />

validation result. So, what we are looking for is a method that could efficiently identify the<br />

existing failures, <strong>and</strong> at the same time does not bring an overestimation to our results.<br />

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Chapter 5: Statistical models 88<br />

Figure 5.14 Percentage of observed training l<strong>and</strong>slides versus CF value: Model 1(A), Model 2(B), Model 3(c), <strong>and</strong> percentage area of susc. Classes (D)<br />

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Chapter 5: Statistical models 89<br />

Figure 5.15 L<strong>and</strong>slide hazard map (a) CF model 1, (b) CF model2<br />

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Chapter 5: Statistical models 90<br />

Figure 5.16 L<strong>and</strong>slide hazard map CF model 3<br />

The potential of the methods is judged by investigating the extent by which they can identify<br />

existing failures. Table 5.10 provides the results.<br />

Table 5.10 Validation of certainty factor method of analysis<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (npix) Percentage<br />

Very low 30 1.58<br />

Low 120 6.33<br />

Moderate 89 4.69<br />

Uncertain 1 0.05<br />

High 558 29.43<br />

Very high 1098 57.91<br />

Total 1896 100<br />

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Chapter 5: Statistical models 91<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (npix) Percentage<br />

Very low 22 1.16<br />

Low 128 6.75<br />

Moderate 142 7.49<br />

Uncertain 0 0.00<br />

High 523 27.58<br />

Very high 1081 57.01<br />

Total 1896 100<br />

L<strong>and</strong>slide susceptibility Area of validation l<strong>and</strong>slides (npix) Percentage<br />

Very low 16 0.84<br />

Low 82 4.32<br />

Moderate 318 16.77<br />

Uncertain 0 0.00<br />

High 530 27.95<br />

Very high 950 50.11<br />

Total 1896 100<br />

The highest accuracy is achieved when all triggering factors are considered. CF model 1 gives<br />

87.4% accuracy while CF model 2 <strong>and</strong> 3 yield 84.6% <strong>and</strong> 78.4% respectively. Hence,<br />

employing as many factors as possible gives a better potential to identify instabilities.<br />

5.2.4 L<strong>and</strong>slide susceptibility analysis<br />

L<strong>and</strong>slide susceptibility analysis is a method that is comparable to the l<strong>and</strong>slide statistical<br />

index method of analysis. Unlike the statistical index method, it doesn’t express the weight of<br />

the triggering factors as a logarithmic function; instead the density relationship is outlined in a<br />

range of 100. The weighting factors are calculated on the basis of a comparison made<br />

between densities in each category with the total l<strong>and</strong>slide density (Süzen & Doyuran, 2004):<br />

W = 100(f − f) (5.7)<br />

The result of the weight calculation is shown in Table 5.11. The l<strong>and</strong>slide susceptibility is the<br />

cumulative effect of the weights of the triggering factors combined:<br />

<br />

LSI = W <br />

<br />

(5.8)<br />

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Chapter 5: Statistical models 92<br />

Table 5.11 Weight values for the l<strong>and</strong>slide susceptibility method<br />

<strong>Slope</strong><br />

Class Wij Class Wij Class Wij<br />

Flat -10.88 Low -20.54 Close -3.13<br />

Rolling -2.87 Moderate -20.54 Medium -3.20<br />

Mountanious 9.80 Fairly Moderate -7.01 Fairly Far 0.58<br />

Escarpments 43.14 High 4.15 Very Far 0.35<br />

Cliffs 62.56 Very High 10.44<br />

Lithology<br />

Elevation<br />

<strong>Slope</strong> shape<br />

Class Wij Class Wij Class Wij<br />

Trap basalt 4.61 Peak <strong>and</strong> Ridges -1.40 Flat -20.54<br />

Limestone Marl -8.99 Saddle 0.93 N 3.32<br />

Amba Aradom S<strong>and</strong>stone 17.87 <strong>Slope</strong> Hill -0.54 NE -0.93<br />

Shale -5.73 Convex 1.75 E -7.62<br />

Dolerite Sill 29.65 Concave 1.95 SE -1.46<br />

Shale Marl Limestone -10.19 Gully -1.37 S -1.59<br />

Marl Limestone 3.35 Other -6.28 SW -4.11<br />

Adigrat S<strong>and</strong>stone 4.11 W 3.40<br />

Alluvium 46.59 Distance to streams<br />

NW 9.21<br />

Endaga Arbi Glacial -20.54 Class Wij N2 8.07<br />

Entcho S<strong>and</strong>stone -19.20 Very Close -0.99<br />

Close -0.13<br />

Topographic wetness index<br />

Moderate 0.51<br />

Class Wij Fairly Moderate 1.07<br />

WI


Chapter 5: Statistical models 93<br />

Figure 5.17 L<strong>and</strong>slide hazard map (a) LS (model 1), (b) LS (model2)<br />

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Chapter 5: Statistical models 94<br />

Figure 5.18 L<strong>and</strong>slide hazard map LS (model 3)<br />

35<br />

30<br />

25<br />

Area (%)<br />

20<br />

15<br />

10<br />

LS_model 1<br />

LS_model 2<br />

LS_model 3<br />

5<br />

0<br />

Low Very low Moderate High Very high.<br />

Figure 5.19 Areal distribution of the hazard classes, LS method<br />

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Chapter 5: Statistical models 95<br />

Table 5.12 presents the validation results of the predictions obtained with the LS<br />

susceptibility modeling. LS model 2 predicts 76% of the validation l<strong>and</strong>slides accurately,<br />

while LS model1 <strong>and</strong> LS model 3 estimates only 74% of the failure bodies correctly.<br />

Therefore, employing all triggering factors is not as reliable as the approach based on only<br />

pre-estimated governing factors.<br />

Table 5.12 Validation results for l<strong>and</strong>slide susceptibility method of analysis<br />

L<strong>and</strong>slide susceptibility<br />

Percentage area<br />

Ls_Model1 Ls_Model2 Ls_Model3<br />

Very low 0.95 0.58 0.63<br />

Low 6.06 6.43 4.64<br />

Moderate 18.87 17.82 20.88<br />

High 18.40 20.56 18.87<br />

Very high 55.72 54.61 54.98<br />

Total 100 100 100<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion<br />

Determining the l<strong>and</strong>slide susceptibility of Hagere Selam area is the main objective of this<br />

research. In addition, different l<strong>and</strong>slide models are tested to find the most suitable prediction<br />

method. In this chapter we will discuss:<br />

The comparison between the results of the employed methodologies <strong>and</strong> the inventory.<br />

A comparison between the accuracies of the models.<br />

Selection of a suitable physically based scenario.<br />

Selection of a suitable statistical model.<br />

Matching between statistical model outputs.<br />

Matching between the selected deterministic <strong>and</strong> statistical model results.<br />

Selection of the final representative hazard map.<br />

Identifying the responsible triggering factors.<br />

Discussing the final hazard map with respect to the inventory.<br />

Future work<br />

6.1 Comparison <strong>and</strong> discussion<br />

To compare the employed methodologies, the areal distribution of the assigned l<strong>and</strong>slide<br />

hazard zones is examined prior to validating the outcomes. The total area of mass movement<br />

zone identified by aerial photo interpretation is 20%. Table 6.1 summarizes the areal<br />

distributions of stability classes defined by using the various methods.<br />

Table 6.1 Areal distribution summary (M x = model x)<br />

<strong>Stability</strong> condition<br />

Physically based<br />

Statstical index<br />

Weighting factor<br />

<strong>Stability</strong> class LS susceptibility class Dry Half sat Sat M 1 M 2 M 3 M 1 M 2 M 3<br />

Unstable Very high 4.93 21.67 39.34 19.45 19.33 19.28 19.92 21.02 20.58<br />

Quasi stable High 6.42 12.85 13.65 13.51 12.07 13.58 10.53 14.34 14.66<br />

Moderately stable Moderate 8.39 13.02 12.39 25.93 31.51 28.7 29.74 27 27.38<br />

Stable Low/Very low 80.26 52.46 34.62 40.99 37.1 38.33 39.81 37.64 37.37<br />

<strong>Stability</strong> condition<br />

Certainity factor L<strong>and</strong>slide susceptibility<br />

<strong>Stability</strong> class LS susceptibility class M 1 M 2 M 3 M 1 M 2 M 3<br />

Unstable Very high 16.87 19.51 14.57 17.11 16.87 17.53<br />

Quasi stable High 22.55 21.61 17.36 12.07 14.09 13.09<br />

Moderately stable Moderate 15.63 19.59 30.5 29.83 30.62 31.91<br />

Stable Low/Very low 42.65 39.22 37.53 40.99 38.42 37.47<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 97<br />

Comparison of the l<strong>and</strong>slide inventory <strong>and</strong> the methods is equally valuable as validating the<br />

outputs. An approach showing the highest matching with the observed l<strong>and</strong>slides is not<br />

necessarily the best prediction method. An accuracy of close to 100% would be attained, if the<br />

hazard mapping overestimates the very high <strong>and</strong> high susceptibility zones. For instance, if the<br />

whole l<strong>and</strong>slide pixels were used to classify the LSI values, only 2-3% of the l<strong>and</strong>slides<br />

would have been unrecognized. However, it doesn’t mean that the output has 97-98%<br />

accuracy, rather it implies an overestimation. To prevent this, the classification is performed<br />

on training l<strong>and</strong>slides (around 60% of the database), <strong>and</strong> the validation is done with the<br />

remaining 40% of the database. Hence, two perspectives shall be considered:<br />

A representative hazard map is at least expected to recognize failure zones indicated<br />

by the inventory, <strong>and</strong> at most anticipated to detect units with similar properties but not<br />

necessarily inside the inventory.<br />

As 20% of the area is identified by the morphology of the mobilized mass movements,<br />

its extent of susceptibility is expected to be very high or high. This is because once the<br />

soil mass is displaced, the first-time movement of the material causes the shear<br />

strength to drop from the original to the residual strength along the failure plane<br />

(Lambe & Whitman, 1979).<br />

Figure 6.1 Comparison of instability classes with the inventory (Mx = model x)<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 98<br />

From Figure 6.1, it is inferred that:<br />

The dry scenario indicates only 11% of the area to be unstable, a 9% offset from the<br />

inventory. Therefore, a physical model based on dry scenario is regarded as less<br />

appropriate.<br />

The saturated scenario shows a significantly larger amount of area to be susceptible as<br />

compared with all the other models. Hence, it over estimates the hazard.<br />

For the high <strong>and</strong> very high susceptibly classes, the deterministic methods yield larger<br />

values than the statistical methods. But, statistical approaches show more area to be<br />

unstable, if the moderate susceptibility category is included.<br />

The results of the half saturated condition demonstrate to be analogous to the certainty<br />

factor <strong>and</strong> weighting factor approaches.<br />

The Statistical index <strong>and</strong> susceptibility analysis methods give essentially similar<br />

results.<br />

Next, we will compare the prediction accuracies obtained by the models. By prediction<br />

accuracy, we mean the matching between the validation l<strong>and</strong>slide set with the very high <strong>and</strong><br />

high susceptibility categories. The results are depicted in Figure 6.2.<br />

Figure 6.2 Comparison between the accuracies of the employed methodologies (Mx=model x)<br />

It is noted from Figure 6.2 that:<br />

The physical model with fully saturated scenario <strong>and</strong> certainty factor model 1 give the<br />

highest accuracy (87%). Because the fully saturated condition envisages most of the<br />

area to be unstable, its high accuracy is regarded to arise from over estimation.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 99<br />

On the other h<strong>and</strong>, the dry scenario gives the smallest matching with the database, an<br />

accuracy of 38%. Accordingly, its potential for slope stability analysis is judged to be<br />

limited. Still, it is critical in forecasting unconditionally unstable zones.<br />

The certainty factor <strong>and</strong> weighting factor approaches prove to be superior to the other<br />

statistical methods. The weighting factor model 2 <strong>and</strong> certainty factor model 2 give<br />

exactly the same accuracy (85%).<br />

The statistical index <strong>and</strong> l<strong>and</strong>slide susceptibility approaches have more or less<br />

comparable validation results.<br />

The half saturated scenario predicts as many l<strong>and</strong>slides as the statistical index <strong>and</strong><br />

l<strong>and</strong>slide susceptibility methods. Its accuracy is 74%. Owing to the fact that this<br />

approach is based on soil mechanics principles <strong>and</strong> that the half saturated condition<br />

represents practical field conditions, the result obtained is regarded to be highly<br />

appreciable.<br />

It is shown that for the weighting factor approach, the model based on the preestimated<br />

most governing factors give a better result than the model based on all the<br />

factors. On the contrary, for the certainty factor technique, the combination of all the<br />

factors proves to be better than the other combinations.<br />

The accuracies of the models tell how much of the l<strong>and</strong>slides are predicted in the high <strong>and</strong><br />

very high susceptibility categories. However, this is not adequate. The relative proportion of<br />

l<strong>and</strong>slide bodies with respect to the area of the susceptibility class in which they exist is also<br />

important. This is done by calculating posterior probabilities (Long, 2008). The posterior<br />

probability is the area of observed l<strong>and</strong>slides divided by the l<strong>and</strong>slide susceptibility class in<br />

which they occur. The l<strong>and</strong>slide prone zone identified by a certain method is regarded to be<br />

more accurately predicted, if its area of high <strong>and</strong> very high susceptibility class is small. If the<br />

posterior probability is small for low hazard zones, it means that the model has predicted large<br />

area to be a low risk zone <strong>and</strong> very few of the l<strong>and</strong>slide bodies exist in the zone. Therefore, a<br />

low posterior probability in the low hazard zones, <strong>and</strong> large posterior probability in the high<br />

hazard zones depict the strength of a model in predicting instabilities. Table 6.2 presents the<br />

results of probability values calculated for each model.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 100<br />

Table 6.2 Posterior probabilities of all methods<br />

Area<br />

(npix) (%)<br />

L<strong>and</strong>slide probability<br />

Deterministic<br />

Very low/low l<strong>and</strong>slide susceptibility 31532 52.46 0.017<br />

Moderate l<strong>and</strong>slide susceptibility 7827 13.02 0.048<br />

High l<strong>and</strong>slide susceptibility 7727 12.85 0.060<br />

Very high l<strong>and</strong>slide susceptibility 13026 21.67 0.083<br />

SI model 1<br />

Very low/low l<strong>and</strong>slide susceptibility 24640 40.99 0.007<br />

Moderate l<strong>and</strong>slide susceptibility 15589 25.93 0.040<br />

High l<strong>and</strong>slide susceptibility 8124 13.51 0.064<br />

Very high l<strong>and</strong>slide susceptibility 11692 19.45 0.097<br />

SI model 2<br />

Very low/low l<strong>and</strong>slide susceptibility 22301 37.1 0.005<br />

Moderate l<strong>and</strong>slide susceptibility 18939 31.51 0.049<br />

High l<strong>and</strong>slide susceptibility 7254 12.07 0.064<br />

Very high l<strong>and</strong>slide susceptibility 11618 19.33 0.082<br />

SI model 3<br />

Very low/low l<strong>and</strong>slide susceptibility 23041 38.33 0.011<br />

Moderate l<strong>and</strong>slide susceptibility 17253 28.7 0.039<br />

High l<strong>and</strong>slide susceptibility 8162 13.58 0.068<br />

Very high l<strong>and</strong>slide susceptibility 11589 19.28 0.085<br />

WF model 1<br />

Very low/low l<strong>and</strong>slide susceptibility 23934 39.81 0.006<br />

Moderate l<strong>and</strong>slide susceptibility 17878 29.74 0.036<br />

High l<strong>and</strong>slide susceptibility 6327 10.53 0.070<br />

Very high l<strong>and</strong>slide susceptibility 11973 19.92 0.102<br />

WF model 2<br />

Very low/low l<strong>and</strong>slide susceptibility 22626 37.64 0.008<br />

Moderate l<strong>and</strong>slide susceptibility 16232 27 0.023<br />

High l<strong>and</strong>slide susceptibility 8618 14.34 0.088<br />

Very high l<strong>and</strong>slide susceptibility 12636 21.02 0.090<br />

WF model 3<br />

Very low/low l<strong>and</strong>slide susceptibility 22469 37.37 0.010<br />

Moderate l<strong>and</strong>slide susceptibility 16458 27.38 0.028<br />

High l<strong>and</strong>slide susceptibility 8811 14.66 0.076<br />

Very high l<strong>and</strong>slide susceptibility 12374 20.58 0.090<br />

CF model 1<br />

Very low/low l<strong>and</strong>slide susceptibility 25636 42.65 0.005<br />

Moderate l<strong>and</strong>slide susceptibility 9509 15.82 0.019<br />

High l<strong>and</strong>slide susceptibility 13558 22.55 0.068<br />

Very high l<strong>and</strong>slide susceptibility 11342 18.87 0.107<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 101<br />

CF model 2<br />

Very low/low l<strong>and</strong>slide susceptibility 23573 39.22 0.005<br />

Moderate l<strong>and</strong>slide susceptibility 11821 19.67 0.027<br />

High l<strong>and</strong>slide susceptibility 12993 21.61 0.070<br />

Very high l<strong>and</strong>slide susceptibility 11725 19.51 0.094<br />

CF model 3<br />

Very low/low l<strong>and</strong>slide susceptibility 22557 37.53 0.010<br />

Moderate l<strong>and</strong>slide susceptibility 18318 30.47 0.039<br />

High l<strong>and</strong>slide susceptibility 10424 17.34 0.068<br />

Very high l<strong>and</strong>slide susceptibility 8746 14.55 0.092<br />

LS model 1<br />

Very low/low l<strong>and</strong>slide susceptibility 24640 40.99 0.010<br />

Moderate l<strong>and</strong>slide susceptibility 17934 29.83 0.041<br />

High l<strong>and</strong>slide susceptibility 7255 12.07 0.072<br />

Very high l<strong>and</strong>slide susceptibility 10283 17.11 0.092<br />

LS model 2<br />

Very low/low l<strong>and</strong>slide susceptibility 23098 38.42 0.009<br />

Moderate l<strong>and</strong>slide susceptibility 18405 30.62 0.047<br />

High l<strong>and</strong>slide susceptibility 8467 14.09 0.055<br />

Very high l<strong>and</strong>slide susceptibility 10142 16.87 0.091<br />

LS model 3<br />

Very low/low l<strong>and</strong>slide susceptibility 22521 37.47 0.015<br />

Moderate l<strong>and</strong>slide susceptibility 19182 31.91 0.037<br />

High l<strong>and</strong>slide susceptibility 7871 13.09 0.065<br />

Very high l<strong>and</strong>slide susceptibility 10538 17.53 0.085<br />

From Table 6.2, CF model 1 gives the highest posterior probability of l<strong>and</strong>slides in the very<br />

high susceptibility category (0.107). Therefore, it relatively predicts many l<strong>and</strong>slide bodies in<br />

the very high hazard zone which has smaller area. In the same way, it has the smallest<br />

probability of l<strong>and</strong>slide bodies in the low hazard zone (0.005). Such a comparison can also be<br />

made by drawing cumulative percentage of observed l<strong>and</strong>slides against cumulative area.<br />

Figure 6.3 depicts the comparison made between all the employed methodologies. It is shown<br />

that CF model 1 has the highest curvature i.e. its classification gives the highest areas in the<br />

very low, low <strong>and</strong> moderate susceptibility classes. Hence, it proves to be more precise in<br />

predicting instabilities.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 102<br />

Figure 6.3 Cumulative % of observed l<strong>and</strong>slides versus cumulative % area<br />

Now, we will discuss matching between the employed methodologies. Correlation between<br />

different results can be weak or strong, i.e. the relationship between the two sets may be<br />

significant or weak. Identifying the agreed areas between different hazard maps gives a hint<br />

about the most important triggering factors. First, we will analyze the agreement between<br />

each three models for each statistical approach. Then, we will compare the representative<br />

models of each statistical approach with one another. Table 6.3 presents the percentage of<br />

agreed areas among the three models used for statistical approach.<br />

Table 6.3 Agreed areas on stability classes using statistical index method<br />

(SI_M1) vs ( SI_M2) (SI_M1) vs ( SI_M3) (SI_M2) vs ( SI_M3)<br />

(%) (%) (%)<br />

Very low 15 13 13<br />

Low 7 17 7<br />

Moderate 16 20 18<br />

High LS susc 6 8 6<br />

Very high 16 17 17<br />

Total agreed area 60 75 61<br />

The output hazard maps correlate strongly. Around 60% of the area is agreed by<br />

SI_M1 <strong>and</strong> SI_M2, 75% by SI_M1 <strong>and</strong> SI_M3, <strong>and</strong> 61% by SI_M2 <strong>and</strong> SI_M3.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 103<br />

The correlations show the stability of the area controlled by factors common to the<br />

three models. It is agreed that 16-17% of the area is very high susceptibility class<br />

(VHLS), <strong>and</strong> 6-8% of the area is high susceptibility class (HLS). The areas defined by<br />

the combinations employed range between 19.28-19.45% for VHLS, <strong>and</strong> 12.07-<br />

13.58% for HLS. Thus, most of the failure zones are agreed. For instance, for SI_M1<br />

<strong>and</strong> SI_M3, the two out puts agree on about 90% of the l<strong>and</strong>slide susceptible zones.<br />

As the factors slope, lithology <strong>and</strong> l<strong>and</strong>use are common to the models, they are<br />

regarded to significantly control the l<strong>and</strong>slide mechanism in Hagere Selam.<br />

Table 6.4 gives the percentage of agreed areas among the three models of the statistical<br />

weighting factor approach.<br />

Table 6.4 Agreed areas on stability classes using statistical WF method<br />

(WF_M1) vs (WF_M2) (WF_M1) vs (WF_M3) (WF_M2) vs ( WF_M3)<br />

(%) (%) (%)<br />

Very low 15 12 13<br />

Low 13 15 20<br />

Moderate 20 22 21<br />

High LS susc 8 8 10<br />

Very high 19 19 20<br />

Total agreed area 75 76 84<br />

A l<strong>and</strong>slide hazard mapping performed using SWF method gives the same result for 75% of<br />

the study area, if all the 10 causative factors are considered or only slope, lithology, l<strong>and</strong>use<br />

<strong>and</strong> fault density are considered. 76% of the results obtained by model 1 <strong>and</strong> 3 are alike. The<br />

highest matching is observed between model 2 <strong>and</strong> model 3, about 84% of the study area.<br />

More than 92% of the very high l<strong>and</strong>slide susceptibility category is agreed by model 2 <strong>and</strong> 3.<br />

Therefore, we conclude that the triggering factors slope, lithology <strong>and</strong> l<strong>and</strong>use are indeed the<br />

most determining factors for instability.<br />

For the SWF approach, since the contribution of one parameter is different from the<br />

others, <strong>and</strong> data driven weights were given for all the factors, the final outputs match<br />

better than the other statistical methods.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 104<br />

Table 6.5 presents the percentage of agreed areas among the three models of the certainty<br />

factor approach.<br />

Table 6.5 Agreed areas on stability classes using statistical CF method<br />

(CF_M1) vs (CF_M2) (CF_M1) vs (CF_M3) (CF_M2) vs (CF_M3)<br />

(%) (%) (%)<br />

Very low 20 15 14<br />

Low 11 10 11<br />

Moderate 10 11 13<br />

High LS susc 15 10 10<br />

Very high 15 13 14<br />

Total agreed area 71 59 62<br />

The outputs obtained using the three combinations of causative factors match for about<br />

71% of the area for combination 1 <strong>and</strong> 2, 59% for combination 1 <strong>and</strong> 3, <strong>and</strong> 62% for<br />

combination 2 <strong>and</strong> 3. As compared to SI <strong>and</strong> WF methods, the correlation for CF maps<br />

is lower. This means that certainty analysis is affected by the considered factors. The<br />

very high hazard unit shown by CF_M1 is 16.87% while for CF_M2 this is 19.51%.<br />

The percentage of agreed area on the very high hazard zone is 15% of the study area.<br />

This means that around 89% of the very high hazard unit identified by CF_M1 is also<br />

identified by CF_M2. So certainty analysis performed by considering only slope,<br />

lithology, l<strong>and</strong>use <strong>and</strong> distance to faults is as efficient as the analysis based on 10<br />

factors.<br />

Next we will discuss the comparison between each bivariate statistical technique.<br />

Table 6.6 Agreed areas on stability classes by four bivariate methods<br />

SI with WF SI with CF SI with LS WF with CF WF with LS<br />

% % % % % %<br />

Very low 17 16 16 18 18 23<br />

Low 17 11 13 10 12 16<br />

Moderate 21 11 21 12 21 9<br />

High LS susc 7 12 10 6 6 11<br />

Very high 17 18 17 16 16 17<br />

Total agreed area 79 68 77 62 73 76<br />

CF with LS<br />

SI = Statistical index, WF = Weighting factor, CF = certainty factor, LS = L<strong>and</strong>slide<br />

susceptibility method<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 105<br />

Some remarks can be noted:<br />

A maximum agreement of 79% is attained between the results of SI <strong>and</strong> WF methods,<br />

while the minimum agreement is 62% for WF <strong>and</strong> CF approaches. As compared with<br />

the other bivariate techniques, the certainty factor analysis yields somewhat different<br />

result.<br />

All four methods agree on 16-18% of the area to be very high susceptibility, <strong>and</strong> 6-<br />

12% as high susceptibility. The highest disagreements are observed for moderate <strong>and</strong><br />

very low hazard zones. If we consider the areas agreed by all the statistical<br />

approaches, 22% of the area is likely to fail under normal circumstances or under<br />

minor destabilizing forces. An additional 9% is agreed by all the methods to be<br />

unstable under moderate destabilizing forces.<br />

To compare the agreement between physically based <strong>and</strong> statistical techniques, CF model 2<br />

<strong>and</strong> half saturated scenarios are selected. Table 6.7 shows the comparison.<br />

Table 6.7 Agreed areas on stability classes by physically based <strong>and</strong> certainty factor methods<br />

<strong>Stability</strong> condition<br />

Agreed area<br />

Physically based(half sat) Certainity factor (%)<br />

Unstable /Quasi stable Very high/high 20.98<br />

Moderately stable Moderate 4.86<br />

Stable Low/Very low 28.12<br />

Total agreement 53.96<br />

The deterministic <strong>and</strong> certainty factors approaches agree on 21% of the area to be unstable or<br />

quasi stable, <strong>and</strong> 28% to be stable. The disagreement is pronounced for the moderately stable<br />

category. Though the statistical methods match sufficiently with each other, the similarity<br />

between half saturated physically based model <strong>and</strong> certainty factor approaches is noticeably<br />

small. Apparently, the reason is the disparity between the core concepts the models are based<br />

up on. However, Figure 6.4 demonstrates that most of the l<strong>and</strong>slide source areas are in zones<br />

of agreement. Therefore, it can be said that there is no significant difference between the two<br />

methods as far as present l<strong>and</strong>sliding is concerned.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 106<br />

Figure 6.4 A map displaying matching between statistical <strong>and</strong> deterministic methods<br />

6.2 Conclusions<br />

For a long time, the existence of l<strong>and</strong>slides was not recognized, <strong>and</strong> l<strong>and</strong>sliding was not<br />

believed to be a significant hazard in the 497 km² study area in Hagere Selam, northern<br />

Ethiopia. However, during the last few years, slope instabilities were reported, <strong>and</strong> studies<br />

showed that many of the failures were reactivations of old deep-seated l<strong>and</strong>slides. Because<br />

slope instability problems are affecting human lives, infrastructures, agricultural l<strong>and</strong>, <strong>and</strong> the<br />

natural environment, a l<strong>and</strong>slide risk assessment study is deemed to be indispensable.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 107<br />

We developed a l<strong>and</strong>slide inventory of the study area consisting of cliffs associated with rock<br />

falls <strong>and</strong> l<strong>and</strong>slides zones associated with debris flows, debris slides, rock slides <strong>and</strong> slumps.<br />

30 debris flows, 7 l<strong>and</strong>slide belts, 4 l<strong>and</strong>slides in the Antalo supersequence, 12 l<strong>and</strong>slides in<br />

Imba Degua <strong>and</strong> Chini ridges, <strong>and</strong> 2 slumps were identified. The l<strong>and</strong>slide database amounts<br />

to about 20% of the study area.<br />

Four failure mechanisms are believed to be responsible for the l<strong>and</strong>sliding in the study area.<br />

The first mechanism consists of flow of geologic layers resting over the Amba Aradom<br />

s<strong>and</strong>stone; this is mainly the basaltic flows. Secondly, the l<strong>and</strong>slides affecting the Antalo<br />

limestone are related to pore water pressure built up resulting from the massive/ hard layers<br />

acting as an aquicludes or aquitard. Third, l<strong>and</strong>slides composed of fresh dolerite boulders<br />

resting over corestone weathering profiles. Lastly, rock falls arise from the detachment <strong>and</strong><br />

toppling of boulders from rocky cliffs after every rainy season.<br />

A deterministic approach for l<strong>and</strong>slide susceptibility mapping was applied. Infinite slope<br />

models including three steady state conditions assuming either dry, half saturated, or saturated<br />

conditions were analyzed. A comprehensive evaluation of the obtained l<strong>and</strong>slide susceptibility<br />

maps was done by model validation whereby the outputs are justified by comparing them with<br />

the l<strong>and</strong>slide database. The following conclusions are drawn:<br />

The fully saturated scenario model validation result is 88%, but is regarded to arise<br />

from an over-estimation of instability. Such a simulation is judged to be unpractical.<br />

Nonetheless, such slope stability analysis is essential, as it correctly delineates the<br />

unconditionally stable zones.<br />

As expected, the dry scenario demonstrated a low validation result, i.e. an under<br />

estimation to slope instability. However, it is crucial in identifying the unconditionally<br />

unstable zones.<br />

The half saturated scenario provides the best output among the physically based<br />

models. It correctly designates 75% of the inventoried l<strong>and</strong>slides. The total area of<br />

l<strong>and</strong>slide hazard zones defined by this model is 35%. It proved even to be better than<br />

some of the statistical models. Therefore, among the deterministic methods, it is<br />

believed to be the most suitable for the assessment of l<strong>and</strong>slide incidence in the study<br />

area.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 108<br />

A combined factor of safety map obtained from the three steady state scenarios is<br />

believed to be important, because each scenario has its particular importance as<br />

discussed above.<br />

The infinite slope model detected l<strong>and</strong>slides in the Amba Aradom s<strong>and</strong>stone, <strong>and</strong> rock<br />

falls in Adigrat s<strong>and</strong>stone taking place in the NW part of the study area. <strong>Slope</strong><br />

instability due to increase in soil moisture was markedly recognized in the basalts.<br />

The behavior of the expansive clays resulting from the weathering of basalts favor an<br />

enhanced pore-water pressure built up, which eventually leads to an increase in<br />

l<strong>and</strong>slides in the formation.<br />

In addition, 4 statistical approaches, statistical index, weighting factor, certainty factor <strong>and</strong><br />

l<strong>and</strong>slide susceptibility analysis, were applied. These methods depend mainly upon a<br />

relationship between past l<strong>and</strong>slides <strong>and</strong> causative factors. Ten triggering factors were<br />

selected. From the correlation between the observed l<strong>and</strong>slides <strong>and</strong> the factors, the following<br />

conclusions are drawn:<br />

<strong>Slope</strong> angle has a clear causal relationship with l<strong>and</strong>slides. It is concluded that<br />

l<strong>and</strong>slides occur in the study area in zones with slope angle > 15°.<br />

Alluvium, Dolerite sill, Amba Aradom s<strong>and</strong>stone, <strong>and</strong> Trap basalts have soil<br />

properties favorable for instability.<br />

Elevation proved to be a strong causal factor to instability. Areas with elevation ><br />

2200 m are highly prone to failure, while areas with elevation < 2220 m are not<br />

favorable for l<strong>and</strong>slides<br />

Concave slope shapes proved to be correlated with l<strong>and</strong>slides better than other shapes,<br />

though the correlation is weak. Therefore, the results obtained do not allow drawing<br />

any meaningful conclusion here.<br />

Distance to river factor does not have a strong causal link with l<strong>and</strong>slides. Hence,<br />

undercutting of the slope by a river was probably not the main triggering factor for the<br />

l<strong>and</strong>slides.<br />

Destabilizing of slopes by road construction is judged to be less significant in the<br />

study area.<br />

With aspect, a distinctive result is obtained. North, Northwest <strong>and</strong> West facing slopes<br />

proved to be highly prone to instability, <strong>and</strong> quite the opposite for slopes facing East,<br />

Southwest <strong>and</strong> South.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 109<br />

We believe that though faulting is an important inducing factor for destabilizing<br />

slopes, l<strong>and</strong>slides are generally not located in fault zones in the study area. Hence, it is<br />

concluded that there is no sufficient evidence for a causal relationship between<br />

faulting <strong>and</strong> mass movements.<br />

For l<strong>and</strong>use, there is a negative effect of the presence of vegetation to slope instability,<br />

while bare soils are susceptible to sliding.<br />

For the application of statistical methods, three different causative factor combinations were<br />

employed. Accordingly, the following conclusions are drawn:<br />

Certainty factor model 1 is selected to be the best model for predicting l<strong>and</strong>sliding in<br />

the study area. It is based on causal relationships between past l<strong>and</strong>sliding <strong>and</strong> 10<br />

selected triggering factors. It predicts 41% of the area to be under l<strong>and</strong>slide risk. The<br />

quality of the output is successfully tested by validating it with r<strong>and</strong>omly chosen<br />

l<strong>and</strong>slide grid cells. It correctly identifies 87% of the l<strong>and</strong>slide units.<br />

The hazard maps from the statistical index, weighting factor <strong>and</strong> l<strong>and</strong>slide<br />

susceptibility methods, are highly similar, as indicated by an average of 75% of the<br />

area being classified in the same susceptibility class.<br />

The statistical index <strong>and</strong> l<strong>and</strong>slide susceptibility methods confirm to be less powerful<br />

than the other statistical models.<br />

Altering factors involved in the combinations produces significantly different outputs.<br />

For SI <strong>and</strong> CF models, the combination based on the entire causative factors yield an<br />

enhanced recognition of the existing l<strong>and</strong>slides. On the contrary, for SWF <strong>and</strong> LSS<br />

methods the combination based on slope, lithology, l<strong>and</strong> use <strong>and</strong> fault density result in<br />

a better identification of the existing l<strong>and</strong>slides. Moreover, CF method yields<br />

relatively more disparate results for the employed three combinations.<br />

Finally, Figure 6.5 gives the selected hazard maps based on certainty factor model 1 <strong>and</strong> a<br />

combination of three steady state scenarios. Based on the CF model 1, it is concluded that<br />

41% of the area is under high <strong>and</strong> very high l<strong>and</strong>slide risk, 15% of the area is moderately<br />

susceptible, <strong>and</strong> 44% of the area is free from l<strong>and</strong>slide risk. Based on the combined steady<br />

state deterministic model, it is concluded that 34.6% of the study area is unconditionally<br />

stable, <strong>and</strong> will not fail under any circumstances unless major destabilizing activities occur. If<br />

extreme rainfall event leads to full soil saturation, 12.4% of the area will face instability under<br />

moderate destabilizing actions, 13.7% of the area will likely fail under minor destabilizing<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 110<br />

forces, <strong>and</strong> 17.7% of the area needs stabilization methods to control instability. L<strong>and</strong>slides<br />

will be mobilized in about 16.7% of the area, if the soil is half saturated; 4.93% of the area<br />

will likely fail under any condition, <strong>and</strong> hence stabilization techniques are recommended.<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 111<br />

Figure 6.5 Final Hazard maps based on (A) CF model 1, <strong>and</strong> (B) combined steady state deterministic methods<br />

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Chapter 6: Comparison <strong>and</strong> Conclusion 112<br />

6.3 Recommendations<br />

Our underst<strong>and</strong>ing of the geotechnical <strong>and</strong> geomorphologic mechanisms of slope instability<br />

would be enhanced, if the following points were thoroughly assessed:<br />

A detailed soil investigation including laboratory analyses.<br />

Circular stability calculations on typical sections by various methods.<br />

A compliment of other slope stability softwares together with <strong>GIS</strong>.<br />

A zoomed analysis on selected section to underst<strong>and</strong> the soil mechanics behind it.<br />

A consideration of soil wetness based on different return periods of rainfall.<br />

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References 113<br />

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Varnes, D.J., 1996. L<strong>and</strong>slide Types <strong>and</strong> Processes. In: Turner, A.K., <strong>and</strong> R.L. Schuster (eds),<br />

L<strong>and</strong>slides: Investigation <strong>and</strong> Mitigation, Transportation Research Board Special Report<br />

247, National Research Council, Wasington, D.C. National Academy Press.<br />

Verstappen, H.T., 1983. Applied geomorphology: geomorphological surveys for<br />

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Voogd, H., 1983. Multi-criteria evaluation for urban <strong>and</strong> regional planning. Pion, London.<br />

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<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> using <strong>GIS</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Modeling</strong> Techniques


Appendix 123<br />

Appendix<br />

Figure 1 VNIR image<br />

Figure 2 SI weight values<br />

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Appendix 124<br />

Figure 3 SI weight for geology category<br />

Table 1. Example of weight values with % of l<strong>and</strong>slides<br />

SI(model2) Total pix % of observed LS CF model 2 % of observed LS<br />

-2.754 1 0.02 -0.957 0.02<br />

-2.451 3 0.07 -0.946 0.07<br />

-2.251 20 0.44 -0.926 0.44<br />

-2.173 21 0.47 -0.916 0.47<br />

-2.142 22 0.49 -0.916 0.49<br />

-2.033 23 0.51 -0.9 0.93<br />

-2.027 24 0.53 -0.897 0.95<br />

-1.951 44 0.98 -0.895 1.04<br />

-1.933 46 1.02 -0.886 1.07<br />

-1.873 47 1.04 -0.877 1.09<br />

-1.87 51 1.13 -0.855 1.75<br />

-1.844 52 1.15 -0.852 1.8<br />

-1.67 82 1.82 -0.843 1.82<br />

-1.644 88 1.95 -0.836 2.37<br />

-1.594 89 1.98 -0.831 2.51<br />

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-1.561 114 2.53 -0.818 2.53<br />

-1.555 115 2.55 -0.803 4.77<br />

-1.446 121 2.69 -0.797 4.9<br />

-1.37 222 4.93 -0.795 4.95<br />

-1.344 239 5.30 -0.789 5.08<br />

-1.341 245 5.44 -0.778 5.7<br />

-1.314 247 5.48 -0.771 6.08<br />

-1.296 248 5.50 -0.761 6.1<br />

-1.261 276 6.13 -0.753 6.17<br />

-1.255 279 6.19 -0.726 6.24<br />

-1.2 282 6.26 -0.717 6.41<br />

-1.146 285 6.32 -0.712 6.48<br />

-1.141 306 6.79 -0.708 6.95<br />

-1.117 308 6.84 -0.706 6.97<br />

-1.114 316 7.01 -0.705 7.01<br />

-1.111 319 7.08 -0.677 7.23<br />

-1.094 320 7.10 -0.67 7.48<br />

-1.063 323 7.17 -0.66 7.52<br />

-1.032 334 7.41 -0.633 7.57<br />

-1.026 336 7.46 -0.617 8.23<br />

-0.996 346 7.68 -0.605 9.59<br />

-0.917 358 7.94 -0.603 9.61<br />

-0.915 360 7.99 -0.598 10.3<br />

-0.911 378 8.39 -0.593 10.56<br />

-0.841 439 9.74 -0.583 10.61<br />

-0.814 469 10.41 -0.554 11.07<br />

-0.784 470 10.43 -0.531 11.3<br />

-0.782 472 10.47 -0.53 11.52<br />

-0.733 503 11.16 -0.507 11.58<br />

-0.732 524 11.63 -0.504 11.7<br />

-0.726 529 11.74 -0.497 11.94<br />

-0.715 539 11.96 -0.467 11.96<br />

-0.66 549 12.18 -0.453 12.14<br />

-0.617 562 12.47 -0.449 12.43<br />

-0.611 570 12.65 -0.445 13.69<br />

-0.608 581 12.89 -0.435 14<br />

-0.605 582 12.92 -0.404 14.07<br />

-0.584 590 13.09 -0.365 14.6<br />

-0.533 647 14.36 -0.352 15.05<br />

-0.482 661 14.67 -0.32 15.45<br />

-0.46 681 15.11 -0.305 15.82<br />

-0.415 705 15.65 -0.278 15.93<br />

-0.408 729 16.18 -0.259 16.36<br />

-0.359 739 16.40 -0.248 20.88<br />

-0.305 744 16.51 -0.222 20.99<br />

-0.293 748 16.60 -0.215 21.22<br />

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-0.284 767 17.02 -0.192 21.53<br />

-0.253 769 17.07 -0.162 21.57<br />

-0.233 973 21.59 -0.122 24.28<br />

-0.204 987 21.90 -0.079 24.46<br />

-0.203 992 22.02 -0.078 24.81<br />

-0.186 994 22.06 -0.059 27.1<br />

-0.184 996 22.10 -0.059 27.14<br />

-0.161 1003 22.26 -0.012 27.43<br />

-0.16 1125 24.97 0.017 27.59<br />

-0.108 1251 27.76 0.044 27.83<br />

-0.082 1254 27.83 0.059 28.05<br />

-0.079 1270 28.18 0.069 29.36<br />

-0.059 1280 28.41 0.103 29.54<br />

-0.027 1293 28.70 0.119 29.69<br />

-0.024 1304 28.94 0.147 29.85<br />

-0.004 1312 29.12 0.208 29.87<br />

-0.003 1371 30.43 0.214 31.05<br />

0.015 1374 30.49 0.215 31.36<br />

0.047 1381 30.65 0.225 31.42<br />

0.107 1386 30.76 0.266 32.29<br />

0.114 1400 31.07 0.274 32.6<br />

0.116 1402 31.11 0.294 33.09<br />

0.121 1455 32.29 0.308 33.4<br />

0.139 1469 32.60 0.312 37.97<br />

0.17 1470 32.62 0.321 38.06<br />

0.173 1509 33.49 0.338 38.59<br />

0.176 1510 33.51 0.342 38.62<br />

0.199 1513 33.58 0.366 38.64<br />

0.22 1527 33.89 0.37 39.15<br />

0.276 1549 34.38 0.388 39.19<br />

0.296 1573 34.91 0.392 39.3<br />

0.297 1779 39.48 0.393 39.33<br />

0.315 1787 39.66 0.419 50.47<br />

0.373 1788 39.68 0.428 50.64<br />

0.407 1834 40.70 0.434 50.71<br />

0.42 1896 42.08 0.458 56.24<br />

0.421 2398 53.22 0.46 56.3<br />

0.45 2401 53.28 0.496 56.39<br />

0.47 2409 53.46 0.499 57.77<br />

0.473 2658 58.99 0.524 58.99<br />

0.48 2659 59.01 0.531 59.17<br />

0.488 2660 59.03 0.537 60.94<br />

0.499 2688 59.65 0.548 60.99<br />

0.502 2692 59.74 0.551 62.01<br />

0.505 2747 60.96 0.572 62.03<br />

0.526 2827 62.74 0.605 62.14<br />

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Appendix 127<br />

0.529 2834 62.89 0.606 62.16<br />

0.596 2839 63.00 0.609 62.92<br />

0.65 2873 63.76 0.609 62.98<br />

0.688 2907 64.51 0.616 63.23<br />

0.702 2928 64.98 0.63 66.91<br />

0.705 2929 65.00 0.635 67.38<br />

0.72 3095 68.69 0.648 68.89<br />

0.726 3106 68.93 0.656 68.95<br />

0.729 3108 68.97 0.658 71.68<br />

0.749 3111 69.04 0.69 72.44<br />

0.78 3119 69.22 0.692 72.59<br />

0.805 3187 70.73 0.703 72.61<br />

0.826 3310 73.46 0.708 73.86<br />

0.896 3366 74.70 0.711 75.9<br />

0.949 3396 75.37 0.711 76.52<br />

0.95 3488 77.41 0.73 79.21<br />

0.988 3718 82.51 0.751 79.87<br />

1.002 3839 85.20 0.771 84.98<br />

1.028 3842 85.26 0.777 85.02<br />

1.029 3859 85.64 0.781 85.2<br />

1.217 3860 85.66 0.816 86.62<br />

1.235 3862 85.71 0.835 87<br />

1.238 3968 88.06 0.846 87.02<br />

1.249 4032 89.48 0.855 87.33<br />

1.259 4073 90.39 0.856 87.39<br />

1.383 4109 91.19 0.875 87.44<br />

1.425 4123 91.50 0.882 89.79<br />

1.435 4131 91.68 0.885 90.7<br />

1.438 4133 91.72 0.886 92.83<br />

1.459 4138 91.83 0.902 92.88<br />

1.517 4234 93.96 0.903 93.68<br />

1.538 4342 96.36 0.905 93.79<br />

1.546 4343 96.38 0.909 93.96<br />

1.559 4375 97.09 0.912 96.36<br />

1.682 4387 97.36 0.915 97.07<br />

1.683 4439 98.51 0.928 98.22<br />

1.735 4485 99.53 0.933 99.25<br />

1.846 4491 99.67 0.938 99.51<br />

1.982 4498 99.82 0.954 99.67<br />

2.25 4506 100.00 0.969 99.69<br />

0.972 99.87<br />

0.977 100<br />

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<strong>Slope</strong> <strong>Stability</strong> <strong>Analysis</strong> <strong>Using</strong> <strong>GIS</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Modeling</strong> Techniques

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