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 Research

Risk assessment for geohazards

Seismic hazard, risk and loss

Stability of rock slopes

Geomechanical modelling

Offshore geohazards

Slope instability assessment and hazard zonation

Slide dynamics

Tsunamis

Monitoring, remote sensing and early warning systems

Geophysics for geohazards

Application of GIT to geohazards

Mitigation and risk

GeoExtreme     
 

 News

Simulations of the Samoa tsunami 2009

IYPE projects related to ICG

www.snoskred.no
Norwegian snow avalanche website

2nd ICG Phd seminar
 Download presentations

Positive midway evaluation of ICG
 

 IGCP 511

Submarine Mass Movements and Their Consequences
 

 Conferences

4th International Symposium
on Submarine Mass Movements and Their Consequences,
Austin Texas, 2009

EGU 2009

OTC Geohazard Session
 Download abstracts
 

 Reports

Debris flow and river flooding 23 Aug 2005 in Paznauner Valley, Tirol, Austria

BAM Earthquake of 26th of December 2004

ECI Conference: Geohazards - Technical, Economical and Social Risk Evaluation

2nd International conference on Submarine Mass Movement and Their Consequences 2005

International Workshop 27th of September 2004 - Natural Disaster Hotspot

 

 ICG Partners







 
Project 2: Risk assessment for geohazards
Project Manager:
Unni Eidsvig (NGI)

Subproject 2: Case studies

The following case studies and applications of the Integrated Risk Assessment Framework are presented here:

Case study 1: Rock slopes

Case study 2: Slopes in clays

Case study 3: Snow avalanches

Case study 4: Tsunamis
 

Case study 1: Rock Slopes

When the Integrated Risk Assessment Framework is implemented for rock slopes it takes the form illustrated here. 

Integ_risk_assessmt_schematic_SL_21062006

Figure 1 Risk assessment framework for rock slopes

Data collection
Data collection involves obtaining relevant data for geology, geometry, strength, groundwater condition, dynamic loads and elements at risk.  

Hazard assessment
Hazards assessment is composed of the following consecutive stages:

  1. Kinematic analysis: The basic aim of this stage is to determine discontinuity sets which governs the slope instability
  2. Numerical modeling: This stage is for understanding the possible failure mechanism and better determination of failure surface and slope geometry. Continuum models are more appropriate for weak rock conditions while discontinuum models are more suitable for competent rock situations. The outputs of this stage are volume of rock mass to slide, geometry of slip surface and depth of slide for weak rock and number of blocks to slide and volume of sliding rock for competent rock.
  3. Sensitivity analysis: This stage is for evaluation of model’s sensitivity to input parameters. Here the sensitivity of Mohr-Coulomb and/or Barton-Bandis failure criteria which are most frequently used failure criteria for rock slopes can also be compared.
  4. Uncertainty analysis: Prior to probabilistic modeling, uncertainty analysis is essential in order to obtain more realistic slope failure probabilities. The uncertainties associated with most sensitive parameters are quantified and analyzed in this stage.
  5. Probabilistic modeling: Failure probability for the considered rock slope can be evaluated based on Monte Carlo simulation (MCS) or First Order Reliability Method (FORM).
  6. Evaluation of slide magnitude: The magnitude of the hazard can be assessed by constructing probability of failure (Pf) versus possible rock block volumes.

Vulnerability assessment
The vulnerability assessment in this case diminishes to 2-dimension as the scale is small scale. Then vulnerability can be assessed in a (n x m) matrix, where n is the type of elements at risk and m is number of rock blocks to slide. 

Risk assessment
Risk assessment starts with the computation of total and specific risk. 

 

Case study 2: Slopes in clay

The zone assessed in this study is located in an urban area on the Southern coast of Norway, extending about 1 km along the banks of a river in the vicinity of a fjord.

The quaternary geology description indicates that the soils in the area are nor­mally consolidated. Typical soil profiles display river sand layer at the surface with marine deposits down to bedrock. The transition from marine deposits to sand/gravel deposits is lower than the river water level, which means that the clay deposits are exposed to river erosion. The sensitivity tests of the clay, indicates “quick clay” behaviour. 

Figure 2 Model of the area under investigation

Hazard assessment

To quantify hazard, a scenario-based second-moment probabilistic limit equilibrium approach is implemented. The spatial variability of undrained shear strength is accounted for in the slope stability analyses. Spatial variability of soil strength, river water level and river bed erosion were shown to influence hazard and expected risk levels significantly.

Probabaility distributions of calculated 3-D factor of safety for "01yr" scenarios

Vulnerability assessment
Vulnerability and elements at risk are estimated with a second-moment approach. Values for vulnerability are obtained from published data and engineering judgement. Categories of elements at risk are considered in the study.

Risk assessment
Risk estimates are obtained based on hazard, vulnerability and the potential loss associated with the elements at risk. The uncertainty in risk estimates is quantified using first-order second-moment approximation.

 

Case study 3: Snow avalanches

Figure 4

Avalanches constitute a considerable natural hazard in snow-covered mountain areas. They are fast moving masses of snow and debris on (steep) mountain slopes, which can cause catastrophic destruction. During precipitation and/or storm periods, snow accumulates on slopes. When the snow amount increases, snow weight may exceed the shear resistance at some critical snow depth and a slide will be released. In addition, external loads can contribute to the release of a slab, like a skier or loading by explosives as done for temporal mitigation. Also the reduction of the strength, for example due to rapid warming or rain, can cause an avalanche release. During their descent, avalanches may reach veloc­ity up to 100 m s-1; the flowing density is thought to range typically between 30 to 300 kg m-3. Thus, impact pressures can be as high as several hundred kPa.

Two case studies for avalanches have been performed where hazard, vulnerability and risk are estimated:

1)      A case regarding the risk to a building in an avalanche path

2)      A study concerning the risk to traffic on a major mountain road.

Here the first of these case studies is presented. 

Risk to a building in an avalanche path
A farm is located at the foot of an avalanche path at about 30 masl. 

Hazard assessment

The hazard is comprised of two parts: the probability for release and the probability for run-out of a snow avalanche.
Input parameters are:

  1. Meteorology parameter: precipitation,
  2. Slide release parameters, see table below
     

Random variable

Distribution

Thickness (or height) of slab, D

Beta

Slope angle, y

Lognormal

Shear strength of sliding plane, ts

Lognormal

Width of slide, B

Normal

Length of slide, L

Normal

Density of snow, r

Lognormal

Additional load Wext

 

 In the hazard  assessment, the following models for release and run-out are used:

1. Release model: A simple snow slab avalanche model is used for predicting the release, see figure below. The release probability is denoted P release. The probability of sliding, Pslide is found by integrating Prelease over all snowdepths.

 

fig1

               Figure 5  Snow-slab avalanche definitions, coordinate system and acting forces (Lackinger, 1989).

2. Run-out model: An energy line approach combined with Monte Carlo simulation is used for run-out prediction. Based on simple energy considerations, the energy line approach allows to determine the run out length and to give an estimate on the velocity along the track:

Kinetic energy = loss of potential energy – energy loss due to friction

The run out probability is denoted Ptravel

The avalanche hazard at farm location is given by the probability of the avalanche occurrence times the probability that the avalanche actually reaches the location:

H = Pslide∙Ptravel

Vulnerability assessment
Vulnerability curves for both constant flow density and velocity dependent density are given in the figure below. 

Bleie_19940127_press_PDF_CDF_rho_masonary

Figure 6 Cumulative vulnerability curve versus avalanche speed (red solid line velocity dependent density; red dashed line constant flow density). The blue lines show corresponding specific loss curve for a monumental buildings.

The vulnerability of a building is defined by integrating the probability of a specific loss over all speeds.

Risk assessment

Building
The risk to a building is given by the product of hazard and the vulnerability of the specific building

Inhabitants
The individual risk to a person is given by the product of hazard, vulnerability and the exposure of the respective person.

The risk estimation process is illustrated in the figure below.

Figure 7 llustration of the steps in the risk assessment

Case study 4: Tsunamis

The scope of the study is to quantify the risk associated with a rock slide at Åknes, which has the potential to generate a tsunami. The Åknes rock slope is located in Storfjorden in Western Norway. The area has been subject to a large number of rockslides during post glacial time. In 1934 a rock slide hit the fjord near Tafjord, also in the Storfjorden area, and caused a disastrous tsunami which killed 41 people.

Data collection
Data has been collected from available literature about historical rockslides in the Storfjorden area. Data for vulnerability has been collected from sources containing fatality rates from tsunamis in western Norway, from the December 2004 Indian Ocean tsunami and from the July 2006 Java tsunami.

Hazard assessment
The Åknes threat is not the rockslide itself but its tsunamigenic potential. This means that the hazard is comprised of two parts:

  • The probability of a rockslide at Åknes.
  • The probability of generating a tsunami caused by the Åknes rockslide.

The probability is calculated from frequency of previous rockslides in the Storfjorden area and from expert judgement.

Figure 1 The diagram shows the number of rock-avalanche events and the volume distribution in the entire Storfjorden, Blikra et al. (2005).

The tsunami generated by the rockslide is calculated by numerical simulation using the linear shallow water equations. Several rock volumes are considered in the analysis. Corresponding run-up heights are calculated for four different locations.

Vulnerability assessment
In this study vulnerability to people is studied.
The quantitative vulnerability models for people are based on historic data from statistics of previous tsunami disasters. This is obtained in two steps:

  1. A review of life’s losses caused by earlier tsunamis.
  2. A formulation of a continuous model relating inundation height with life’s losses.

Vulnerability curves are proposed for vulnerability as a function of inundation height, these curves, are shown in the figure below.

Figure 2 Empirical quantification of vulnerability as a function of inundation height

Risk assessment
Two approaches are proposed for quantifying risk at the prescribed locations in Storfjorden. An ‘implicit’ approach I, based on the principle that the expected risk value equals the product of the expected value of hazard, vulnerability and losses, including an implicit relaxation on the dependencies between multi-threats; and the Bayesian network approach BN, which relates the causal dependencies between the threats and other relevant risk factors.

 

International Centre for Geohazards (ICG), PoBox 3930 Ullevaal Stadion, N-0806 Oslo, Norway. Phone: +47-22023000, fax: +47-22230448