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Incorporating Uncertainty into Backward Erosion Piping Risk Assessments

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Backward erosion piping (BEP) is a type of internal erosion that typically involves the erosion of foundation materials beneath an embankment. BEP has been shown, historically, to be the cause of approximately one third of all internal erosion related failures. As such, the probability of BEP is commonly evaluated as part of routine risk assessments for dams and levees in the United States. Currently, average gradient methods are predominantly used to perform these assessments, supported by mean trends of critical gradient observed in laboratory flume tests. Significant uncertainty exists surrounding the mean trends of critical gradient used in practice. To quantify this uncertainty, over 100 laboratory-piping tests were compiled and analysed to assess the variability of laboratory measurements of horizontal critical gradient. Results of these analyses indicate a large amount of uncertainty surrounding critical gradient measurements for all soils, with increasing uncertainty as soils become less uniform.
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a Corresponding author: Bryant.A.Robbins@usace.army.mil
Incorporating Uncertainty into Backward Erosion Piping Risk
Assessments
Bryant A. Robbins1,a, Michael K. Sharp1
1U.S. Army Engineer Research and Development Center, Vicksburg, MS, USA
Abstract. Backward erosion piping (BEP) is a type of internal erosion that typically involves the erosion of
foundation materials beneath an embankment. BEP has been shown, historically, to be the cause of approximately
one third of all internal erosion related failures. As such, the probability of BEP is commonly evaluated as part of
routine risk assessments for dams and levees in the United States. Currently, average gradient methods are
predominantly used to perform these assessments, supported by mean trends of critical gradient observed in
laboratory flume tests. Significant uncertainty exists surrounding the mean trends of critical gradient used in practice.
To quantify this uncertainty, over 100 laboratory-piping tests were compiled and analysed to assess the variability of
laboratory measurements of horizontal critical gradient. Results of these analyses indicate a large amount of
uncertainty surrounding critical gradient measurements for all soils, with increasing uncertainty as soils become less
uniform.
1 Introduction
Internal erosion refers to various processes that cause
erosion of soil material from within or beneath a water
retention structure such as a dam or levee. With regard to
flood risk, internal erosion is an issue of significant
concern. Approximately half of all historical dam failures
have been attributed to internal erosion [1]. While
internal erosion risk can be reduced through the use of
well-designed filters and drains, modifying the entirety of
existing infrastructure to meet modern filter standards is
not economically feasible. Therefore, it is of utmost
importance to be able to assess the likelihood of internal
erosion occurring on existing infrastructure such as dams,
levees, and canals.
Internal erosion processes can be subdivided into four
broad categories: concentrated leak erosion, backward
erosion piping (BEP), internal instability, and contact
erosion [2]. This paper will discuss solely BEP, which
accounts for approximately one third of all internal
erosion related dam failures [1], [3]. For discussion on
the other types of internal erosion, the authors suggest
reviewing Bonelli et al. [4].
The process of BEP is illustrated in Figure 1. For
BEP to occur, it is necessary to have an unfiltered
seepage exit through which soil can begin eroding. As
filters and drains are rare along levee systems in the
United States, the seepage exit condition is usually
unfiltered. This is evident by the numerous sand boils that
occur along the U.S. levee systems during each flood [5].
A sand boil is a small cone of deposited soil that occurs
concentrically around a concentrated seepage exit, as
shown in Figure 1. The presence of sand boils indicates
that the process of BEP has initiated at a particular site.
Whether the BEP process continues, ultimately leading to
structural failure, depends upon numerous conditions
being met (roof support, sufficient hydraulic gradients for
erosion propagation, and unsuccessful human
intervention). Estimation of the probability of failure due
to BEP should consider all of these factors, as well as the
uncertainty surrounding them. The focus of this paper is
on improving how uncertainty regarding critical gradients
for BEP is incorporated into risk assessments, with
particular emphasis on methods used in the U.S. While
the work reported is a simple extension of the
groundbreaking work of Schmertmann and Sellmeijer
([6] & [7]), the authors hope that the simple portrayal of
uncertainty presented leads to the objective quantification
of uncertainty in BEP risk assessments.
Figure 1. Illustration of BEP progressing beneath a levee.
DOI: 10.1051/
03007 (2016)
,
6E3S We b of Conferences e3sconf/201
FLOODrisk 2016 - 3rd European Conference on Flood Risk Management
7
0703007
© The Authors, published by EDP Sciences. This is an open access article distributed under the terms of the Creative
Commons Attribution
License 4.0 (http://creativecommons.org/licenses/by/4.0/).
2 Literature Review
       
   
       

       
 
2.1 BEP Assessment Methods
 !"
          
!"#$%!"&'()*+ ',)

   -.     
   #      
/ 0          
        

  
       
   1  
  / 2     
     
      &  
'34)  5 '33)  6     
        
      
234
/       
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      2 

Ψ 5
Ψ 7
Ψ $78
Ψ 7*
Ψ !
Ψ 
Figure 2. Simplified event tree for BEP evaluation.
 2
2

        
   2    
      
        -'30)
'39). :  "1 -';) '3<). 
"'=)
          
    1    
1
 /      

'3>)
2.2 Critical Gradients and Uncertainty
8     
     
" '=)      
      
  -.       
 
-+.
? ? ? ? @? A? ? ? B?
2        
     C+  $+ 
'3=)  
       
1"1  '3<)    
       "
'3;) &D'3()
       
   "1    
  8    
     
   
!"
 ???B????????
       
       
        
      
      
 " '=)  /    
 
!"
3 Estimating Critical Point Gradients
3.1 Current Practice
" '=)    
  / 9       
 +
 -   . 

       
        
   "   
       
  + 
    / 9   
/ 2     & 
     '3,) '04)  '03) 
   $  3>     43>0   
    / 9    
3< 
 +      
  '=)   
      
 -   
   +   
 .  3    

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Figure 3. Suggested relationship for determining the critical
point gradient as a function of Cu (from [6]). Points represent
study averages of critical point gradient.


"C 3>0
CE 494
C5 494
*"+-34. 404
FGF3>
&E
=4H
"
4
&1
-'=)
.
When using Figure 3 (or the equivalent figure from
[6]), to estimate critical point gradients, it is necessary to
correct for all factors described by Schmertmann using
the reference values in Table 1 to arrive at comparable
point gradient values. Neglecting to adjust the values to
equivalent point gradients will yield erroneous results;
the magnitude of these errors has been shown to be as
large as 100 percent for factors related to soil density and
problem geometry [15].
3.2 Quantifying Uncertainty
While Figure 3 is quite useful, it is difficult to
estimate the uncertainty in the critical point gradient
because study averages are presented. In order to
examine the uncertainty in greater detail, the individual
laboratory test results from each experimental series must
be examined. The authors have compiled all of the
laboratory test results from [19][25]. It was difficult to
establish the exact number of tests in each experimental
series from references [22] and [23]. However, [26] has
provided a very thorough overview of the experiments
conducted by de Wit and Silvis. This overview was used
to determine the individual tests conducted for each
experimental series conducted by de Wit and Silvis.
Mueller-Kirchenbauer conducted more tests than
documented in [25]. However, for the sake of
consistency with [6], only the single test reported in [25]
was considered. In total, 110 laboratory piping tests were
found in the references previously mentioned. Of these,
9 of the piping tests were right censored (did not fail) [19,
21]. For all of the tests, the test results were corrected
using the correction factors provided in [6] to correct the
individual test results to the common reference values in
Table 1.
The corrected, individual laboratory critical point
gradients obtained from the 110 tests found in the
literature are plotted in Figure 4. For comparison
purposes, the no-test default line proposed by
Schmertmann and the best-fit median line are plotted as
well. From visual observation, it is seen that the no-test
default line (dashed) proposed by Schmertmann [6] more
closely approximates a lower bound than an average
trend for low values of uniformity coefficient.
Figure 4. Suggested relationship for determining the critical
point gradient compared to the best fit, median line of all test
results. Points represent individual laboratory tests.
Visual observation of Figure 4 also indicates that the
individual laboratory test points exhibit increasing
variance as the uniformity coefficient increases. This
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non-constant variance, called heteroscedasticity, indicates
that ordinary least squares (OLS) linear regression is not
a suitable means of estimating the uncertainty
surrounding the expected value (mean trend). OLS will
not capture the heteroscedasticity due to the constant
variance, Gaussian residual models typically associated
with linear regression. Transformations (e.g. log
transforms when dealing with exponential data) are
commonly used to transform the data to a distribution of
a particular form such that OLS regression techniques can
be used to estimate the conditional probability
distribution of the dependent variable. Another approach
to capturing the heteroscedasticity is the use of
generalized linear regression models, which attempt to
model the changing variance across the range of
covariates. In order to keep the results as simple and as
visual as possible, the data quantiles were used as
estimates of the conditional probability distribution.
The nth quantile of a sample of data is the value in the
data set for which the proportion n of the sample is lower,
and the proportion (1-n) is higher. As the size of the
sample increases, such that the empirical probability
density function (PDF) of the data more closely
approximates the underlying probability distribution, the
nth quantile approaches the nth percentile of the underlying
probability distribution. For small samples, the empirical
quantiles will exhibit less variance than the equivalent
percentiles due to the influence of the sample size. For
this particular application, the consequences of this are
minor compared to the influence of the many correction
factors used in arriving at the estimates of critical point
gradients for each test. For this reason, the authors
consider the quantiles to be an adequate estimate of the
conditional probability distribution of critical point
gradients.
To estimate the quantiles of the individual laboratory
test data, first order quantile regression was performed. In
other words, a linear equation was fit through the data
such that, for each nth quantile, an nth fraction of the data
lies below the line and a (1-n) fraction of the data lies
above the line. For an excellent (and quite humorous)
introduction to quantiles and quantile regression, the
authors recommend reviewing [27]. Quantile regression
was used to estimate each quantile between the 10th and
the 90th quantiles in increments of 10 percent. While
statistically incorrect to include the censored observations
in the regression, inclusion results in a conservative bias
and still provides useful information. For this reason, and
given the sparse data at high values of uniformity
coefficient, the censored data was included in the
regression analyses. The resulting quantiles are plotted in
comparison to the data in Figure 5. The 6 observations
obtained from [24] are distinguished from the rest of the
data as these observations were obtained from a different
testing configuration and exhibit more variability than the
other test series. While these observations were included
to provide a direct comparison to [6], they should be
carefully evaluated when using the results of this study.
From the linear quantiles plotted in Figure 5, it is
readily seen that the variance in the conditional
distribution of the critical point gradient increases with
increasing uniformity coefficient. It is also observed that
the spread in the data is quite large. At a uniformity
coefficient of 2, the difference between the  90th and
10th percentiles is 0.26. At a uniformity coefficient of 6,
the difference is 0.82. In both cases, the spread in the
distribution is large and should be considered in risk
assessments. Figure 5 can readily be used to inform
estimates of the conditional distribution of critical point
gradients for estimating the probability of BEP
progression in the appropriate node of an event tree
analysis.
Figure 5. Critical point gradients from individual laboratory
tests and best fit quantile regression lines for the 10th to 90th
quantiles. Open points are from a different testing configuration
[24] than other points.
4 Discussion
#        

     / >  


      

  '=)        
        3
5     
/>
#  2      
      / 
      
      43=    
    / >     
   + 
      3  #
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4
        
     403  1  
        
         0  /
/>2
   04     
   #  04    
2    2 
      04    

       

 '=)        
40>       I
/0 
2 I  
409!
        
-403.9(  
        I

D
        

 '=)     
2
5 Conclusions
A compilation of laboratory measurements of
critical point gradients for backward erosion piping is
presented. The probability distribution of critical point
gradients is characterized as a function of uniformity
coefficient through first order quantile regression on the
sample of 110 laboratory test results. Results of these
analyses indicate a large amount of uncertainty
surrounding critical gradient measurements for all soils,
with increasing uncertainty as soils become less uniform.
The results of this study can be used in risk assessments
to estimate the probability of progression for backward
erosion piping.
6 Acknowledgements
        
       
   6 " 
      
        
       
     * F+
:""?JBCA?? ?

      E
*"C
7 References
'3) :K?/A?&K?/A??:K?"A?L?

AM?9;34
3444N340<0444
'0) $JCEA?L?OPQ?I
2
R37
???AM?STOUK
'9) FK?"K?&??FK?&K?&A?L$?
??????AM?
==<9(3N
<406044;
'<) "
D86!"#76
5%"0439
'>) :K?K?*??6K?FK?F+A?L??
#::&
CII#:-"044<
&?STOTVAM?RA?STTQK
'=) 6K?DK?"A?L?8I//
"?#???"AM??
/"6
F+1#"$
0444=>N399
';) 6"1 !
"E!
3,((
'() !"#$??!"&A?L??AM??
!#$ 
0430E$J0430
',) K?*+A?L????
AM?
3>,9>N,<(
0434
'34) 6E&??CK?A?L&I

IAM?
0430
'33) /5%& '
R:"!"#!"#
&E$
3,,<
'30) K?5K?CA?L"?I
AM?(
"3443309>N30;03,9>
'39) 5K?*K?A?LEA?????
?AM?#=<0=
;4(N;343,34
'3<) D"16CW+E$+R:
DFA?L/I
I
I?61?2AM?
3>(339,N33><
0433
'3>) #&?RK?:K??A?L?
7#
AM??""
" &8JC#!"#043>3N04
'3=) 6C+$+$
"A?L$??
DOI: 10.1051/
03007 (2016)
,
6E3S We b of Conferences e3sconf/201
FLOODrisk 2016 - 3rd European Conference on Flood Risk Management
7
0703007
5
???8AM??
"&#$
" &0433>(;N>,>
'3;) "#!
)*&
E!043<
'3() FK?&??#K?DA?L???
??AM??+,
  "
!%%&3043>
'3,) 6D"#-( 
!" ./,"3,,>
'04) /6D"6C
6K?A??XK?5K?5A?L#?#??
2Y
????"AM?*A?/CA?
3,(3
'03) /6I:"&
' !-
 "*/C3,(=
'00) 6:5##"
(E83,(<
'09) 6K?51??6K?"1A?L#????
??AM?-
.&9<,N9>>3,,9
'0<) F:8A??XK?A?LC?

AM?0",0
>>N;=3,(;
'0>) D:IF:&$
"+A?L:????
???AM??-
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DOI: 10.1051/
03007 (2016)
,
6E3S We b of Conferences e3sconf/201
FLOODrisk 2016 - 3rd European Conference on Flood Risk Management
7
0703007
6
... BEP is recognized as one of the major causes of severe damage or even failure of flood defenses worldwide (e.g., Richards and Reddy 2007;Robbins and Sharp 2016). In Italy, a total of 130 sand boils of remarkable size (Fig. 2) have been catalogued in recent years along the major Italian watercourse, the Po River (Aielli et al. 2019). ...
Article
The article presents a three-dimensional (3D) finite element (FE) model of the groundwater flow beneath a river embankment, aimed at developing a simple and reliable numerical strategy for the identification of hydraulic conditions that cause the reactivation of sand boils in flood defense systems prone to recurrent backward erosion piping. The seepage model is calibrated on a cross section of the Po River, where a large natural sand boil has been periodically observed during past high-water events. Monitored river water levels, piezometric measurements, and geotechnical testing data have been used for the calibration study. The numerical analysis proposes a suitable way to simulate a preexisting eroded zone, identifies the key parameters to be collected in the field, and discusses the criteria for the assessment of piping reactivation. The sensitivity analysis proposed herein enables one to identify the set of model parameters capable of capturing field evidence.
Thesis
Full-text available
Backward erosion piping (BEP) is a type of internal erosion that has caused the failure of many dams and levees and continues to threaten the safety of existing infrastructure. To manage this threat, failure risks are regularly evaluated to prioritize risk reduction measures. Unfortunately, current practice for assessing BEP is limited to simple calculation rules that have large uncertainty and error. While numerical models have been developed for simulating BEP, ambiguity regarding the erosion constitutive model, inconsistencies in the assumed physics, and lack of laboratory tests for measuring model parameters have made it difficult to validate tools for use in practice. No validated, widely accepted model for BEP exists today. This thesis develops and validates an approach for finite element modeling of BEP by introducing the concept of the critical secant gradient function (CSGF). The CSGF provides a spatial function of the hydraulic gradient upstream of the pipe tip. An analytical expression for the CSGF and a laboratory test for measuring the CSGF are developed. A steady-state finite element model for simulating BEP progression is then developed for both two- and three-dimensional domains. The model and CSGF concept are validated through hindcasting of BEP experiments. Remarkable agreement was obtained between the finite element predictions and the experiments despite the experiments having different scale, configurations, and boundary conditions. These results indicate that the CSGF may provide the needed link between theory, lab testing, and numerical models to reliably predict BEP progression in practice. Additionally, the results indicate that the steady state finite element algorithm proposed is capable of adequately describing the BEP process, and more complex models may not be necessary. After developing and validating an approach for finite element modeling of BEP progression, the remainder of the thesis demonstrates techniques that can be used to simulate BEP in practice. The use of adaptive meshing is demonstrated in two-dimensions as a means of efficiently simulating BEP progression for field scale problems. Additionally, the random finite element method is applied to demonstrate how to incorporate spatial variability in soil properties into BEP predictions. The results of this study demonstrate how both techniques, in conjunction with the CSGF, offer the potential for transformative improvements in the engineering practice of risk assessment of dams and levees susceptible to BEP progression.
Article
Sand boils are the surface manifestation of an erosion process, known as backward erosion piping, which may take place beneath river embankments during high-water events. The risk of embankment failure greatly increases in locations affected by sand boils. Numerous studies have been carried out, mainly at the laboratory scale, providing significant advancements in this field. Nonetheless, there is still a gap between research and practice that needs to be filled. This study presents a set of field measurements carried out on a large sand boil reactivated near the toe of an embankment along the river Po (Italy). Hydraulic heads, velocity and discharge, concentration and pipe geometry were measured as a function of the water level in the river during the November 2018 flood. The collected data are compared to predictions of a theoretical model which provides the head loss in the vertical pipe. Furthermore, the local exit gradients, as deduced from measurements, are discussed, together with the operational critical gradients adopted in current design practice. The collected data provide important input parameters for the calibration of analytical and numerical models, typically implemented to investigate the sand boil evolution and then to assess the backward erosion piping risk at real scale.
Article
Backward erosion piping (BEP) is one of the major causes of seepage failures in levees. Seepage fields dictate the BEP behaviors and are influenced by the heterogeneity of soil properties. To investigate the effects of the heterogeneity on the seepage failures, we develop a numerical algorithm and conduct simulations to study BEP progressions in geologic media with spatially stochastic parameters. Specifically, the void ratio e, the hydraulic conductivity k, and the ratio of the particle contents r of the media are represented as the stochastic variables. They are characterized by means and variances, the spatial correlation structures, and the cross-correlation between variables. Results of the simulations reveal that the heterogeneity accelerates the development of preferential flow paths, which profoundly increase the likelihood of seepage failures. To account for unknown heterogeneity, we define the probability of the seepage instability (PI) to evaluate the failure potential of a given site. Using Monte-Carlo simulation (MCS), we demonstrate that the PI value is significantly influenced by the mean and the variance of lnk and its spatial correlation scales. While the other parameters, such as means and variances of e and r, and their cross-correlation, have minor impacts. Based on PI analyses, we introduce a risk rating system to classify the field into different regions according to risk levels. This rating system is useful for seepage failures prevention and assists decision making when BEP occurs.
Article
Full-text available
New insights into the failure mechanism piping (under-seepage) regarding the physical process as well as reliability aspects have led to a revision of the Dutch design and safety assessment rules for dikes. This paper describes how the required factor of safety for piping is derived from a top level requirements formulated in terms of an acceptable probability of flooding. The main steps herein are (a) to account for the length-effect to translate requirements on dike ring (system) level to admissible probabilities of failure on dike section (element) level and (b) the calibration of safety factors as a function of the (element) target reliability.
Article
Full-text available
As floodwaters rise against the riverside slope of a levee, hydrostatic pressure builds within the foundation and the embankment soils. Conventional underseepage analyses include the estimation of hydrostatic pressures within these soils to permit the incorporation of prevention methods, such as relief wells on the land side of the levee, to reduce the potential for piping. This study explores the use of an empirical model that uses traditional design variables in addition to previous levee performance and river geomorphology to identify locations most susceptible to piping during flood events. The study focused on levees of the Prairie Du Rocher and Fort Charles Levee Districts of Southwestern Illinois. Observation of excessive seepage or piping incidents made by personnel present during the 1973, 1993, and 1995 flood events were used in the modeling as an indicator of levee performance. Among the variables that proved to be significant in building the empirical model were the confining layer thickness on the land side of the levee, the effective aquifer grain size parameter, a variable designed to reflect the geomorphologic conditions, and an indicator variable designating the location of previous excessive underseepage conditions along the levee. Evidence of previous piping locations was shown to be the best indicator of piping conditions in future floods. This finding demonstrates the value of consistent and thorough record keeping during flood fights. In addition, it suggests that the piping process progressively deteriorates the ability of the subsurface to withstand flow, making a particular location increasingly susceptible to further piping.
Article
Full-text available
This paper presents a comprehensive review of published literature on soil piping phenomena. The first tools to design earth dams to resist piping were developed during 1910-1935. Filter criteria for dispersive soils was refined in the 1970's. Piping phenomena are generally defined as: (1) heave, (2) internal erosion, (3) backwards erosion, although other modes are possible. Recent work on piping highlights the limitations of the occurrence of piping and the role that design and construction may play in a large percentage of piping failures. Standardized laboratory procedures are available to assess piping potential in cohesive materials, but no such methods exist for non-cohesive soils. However, methods are available for evaluation of self-filtration potential. Recent advances in computer technology have facilitated the evaluation of seepage and deformation in embankments but computational methods for evaluation of piping potential are currently limited.
Book
Erosion is the most common cause of failures at earth-dams, dikes and levees, whether through overtopping and overflowing, or internal erosion and piping. This book is dedicated to the phenomenon of internal erosion and piping. It is not intended to be exhaustive on the subject, but brings together some of the latest international research and advances. Emphasis is placed on physical processes, how they can be studied in the laboratory, and how test results can be applied to levees and dams. The results from several research projects in Australia, France, the Netherlands and the United States are covered by the authors. Our aim has been to share our most recent findings with students, researchers and practitioners. Understanding the failure of an earth-dam or a levee by erosion in a unified framework, whether internal erosion or surface erosion, requires continuous research in this field. We hope that the reader will gain knowledge from this book that leads to further progress in the challenging field of the safety of levees and dams. Contents. 1. State of The Art on the Likelihood of Internal Erosion of Dams and Levees by Means of Testing, Robin Fell and Jean-Jacques Fry. 2. Contact Erosion, Pierre Philippe, Rémi Beguin and Yves-Henri Faure. 3. Backward Erosion Piping, Vera Van Beek, Adam Bezuijen and Hans Sellmeijer. 4. Concentrated Leak Erosion, Stéphane Bonelli, Robin Fell and Nadia Benahmed. 5. Relationship between the Erosion Properties of Soils and Other Parameters, Robin Fell, Gregory Hanson, Gontran Herrier, Didier Marot and Tony Wahl. About the Authors. Stéphane Bonelli is a Research Professor at Irstea (French Environmental Sciences and Technologies Research Institute) in Aix-en-Provence, France. He has over 20 years of teaching and research experience, and has been a member of the ICOLD (International Commission on Large Dams) European Working Group on Internal Erosion since 2005. He has participated in 19 large dam reviews in France (visual inspection, monitoring data analysis and numerical modeling). His current activities include research, teaching and consultancy, focusing on soil erosion and the processes of levee breach.
Article
Progressive internal erosion by piping still presents a major failure threat to dams built with and/or over cohesionless soils. A new test-based design method for determining the factor of safety and reliability vs. piping at any point in a trial piping path in cohesionless soils is presented. When using filters for safety vs. piping, the new method provides redundancy. The method uses the simplifying concept that very low effective stresses and the vertical seepage gradients at the advancing end of a pipe determine its advance, and that the pre-pipe gradients at any point in the pipepath have an important effect on the degree of safety at that point.
Article
Present methods for assessing the potential for unsatisfactory levee performance because of underseepage consist of deterministic seepage analyses and simplified reliabilitymethods. Deterministic methods consist of calculating factors of safety based on the ratio of the critical gradients of the soil and hydraulic exit gradients without taking into account high levels of uncertainty in soil properties and subsurface geometry that are inherent to many levee analyses. The most common simplified reliability approaches currently being used to analyze levees against underseepage apply the first-order second-moment Taylor series method, using the U.S. Army Corps of Engineers blanket theory equations as the performance functions. In many cases, these methods do not realistically reflect the geometry of the levee's foundation soils and the uncertainty associated with their performance. This study proposes a new application for the response surface method that allows modeling the initiation of erosion process with more accurate failure mechanisms and more complex subsurface geometry. The response surface-Monte Carlo (RSMC) simulation method uses finite-element analyses to develop a series of equations that define the relationship between the variables and the factor of safety (F). Using these equations, probability density functions (PDF) for variables, and the computer program @Risk, a Monte Carlo simulation is performed to calculate the conditional probability of unsatisfactory performance because of underseepage for a given river flood level. Two examples are presented to illustrate the proposed procedure. Multiple regression analyses are performed to assess the relative effect that changes in the input variables have on the F for the various analyses. The results suggest that uncertainty in the levee geometry has the greatest effect on the variation of the F for the cases studied.
Article
The paper describes the results of a statistical analysis of failures and accidents of embankment dams, specifically concentrating on those incidents involving piping and slope instability. The compilation of dam incidents includes details on the characteristics of the dams, including dam zoning, filters, core soil types, compaction, foundation cutoff, and foundation geology. An assessment of the characteristics of the world population of dams was also carried out. By comparing the characteristics of the dams which have experienced failures and accidents to those of the population of dams, it was possible to assess the relative influence of particular factors on the likelihood of piping and slope instability.Key words: dams, failures, piping, instability database.
Article
A semi-theoretical model is available to estimate the effect of backward erosion piping by underseepage in a dike by computing the critical head. The model accounts for the groundwater flow through the subsoil, pipe flow through the erosion channel and a limited particle equilibrium at the bottom of the channel. This model is extended and updated with the results of a wide range of tests presented in the paper of (Van Beek et al., 2011). The small- scale tests are analyzed by means of a multivariate regression in order to identify the level of influence of each variable. The regression outcome for the permeability corresponds precisely with the outcome of the prediction rule. The effect of relative density, uniformity and particle roundness is empirically dealt with. The role of the particle size is adapted in the new empirical formulation.
Article
Quantile regression, as introduced by Koenker and Bassett (1978), may be viewed as an extension of classical least squares estimation of conditional mean models to the estimation of an ensemble of models for several conditional quantile functions. The central special case is the median regression estimator which minimizes a sum of absolute errors. Other conditional quantile functions are estimated by minimizing an asymmetrically weighted sum of absolute errors. Quantile regression methods are illustrated with applications to models for CEO pay, food expenditure, and infant birthweight.