<?xml version="1.0" encoding="utf-8"?>
<!DOCTYPE article
  PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Publishing DTD v1.0 20120330//EN" "http://jats.nlm.nih.gov/publishing/1.0/JATS-journalpublishing1.dtd">
<article article-type="research-article" dtd-version="1.0" specific-use="sps-1.6" xml:lang="en" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
	<front>
		<journal-meta>
			<journal-id journal-id-type="publisher-id">dyna</journal-id>
			<journal-title-group>
				<journal-title>DYNA</journal-title>
				<abbrev-journal-title abbrev-type="publisher">Dyna rev.fac.nac.minas</abbrev-journal-title>
			</journal-title-group>
			<issn pub-type="ppub">0012-7353</issn>
			<publisher>
				<publisher-name>Universidad Nacional de Colombia</publisher-name>
			</publisher>
		</journal-meta>
		<article-meta>
			<article-id pub-id-type="doi">10.15446/dyna.v84n202.60627</article-id>
			<article-categories>
				<subj-group subj-group-type="heading">
					<subject>Artículos</subject>
				</subj-group>
			</article-categories>
			<title-group>
				<article-title>Probabilistic analysis of the active earth pressure on retaining wall for  <italic>c</italic>  -φ soil backfill under seismic loading conditions</article-title>
				<trans-title-group xml:lang="es">
					<trans-title>Análisis probabilístico del empuje activo en muros de retención con relleno cohesivo-friccionante bajo condiciones de carga sísmica</trans-title>
				</trans-title-group>
			</title-group>
			<contrib-group>
				<contrib contrib-type="author">
					<name>
						<surname>Brasil-Cavalcante</surname>
						<given-names>André Luís</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>
 <italic>a</italic>
</sup> </xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Rodriguez-Rebolledo</surname>
						<given-names>Juan Felix</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>
 <italic>a</italic>
</sup> </xref>
				</contrib>
				<aff id="aff1">
					<label>a</label>
					<institution content-type="original"> Department of Civil &amp; Environmental Engineering, University of Brasilia, Brazil. abrasil@unb.br, jrodriguezr72@unb.br</institution>
					<institution content-type="normalized">Universidade de Brasília</institution>
					<institution content-type="orgdiv1">Department of Civil &amp; Environmental Engineering</institution>
					<institution content-type="orgname">University of Brasilia</institution>
					<country country="BR">Brazil</country>
					<email>abrasil@unb.br</email>
					<email>jrodriguezr72@unb.br</email>
				</aff>
			</contrib-group>
			<pub-date pub-type="epub-ppub">
				<season>Jul-Sep</season>
				<year>2017</year>
			</pub-date>
			<volume>84</volume>
			<issue>202</issue>
			<fpage>9</fpage>
			<lpage>15</lpage>
			<history>
				<date date-type="received">
					<day>20</day>
					<month>10</month>
					<year>2016</year>
				</date>
				<date date-type="rev-recd">
					<day>23</day>
					<month>05</month>
					<year>2017</year>
				</date>
				<date date-type="accepted">
					<day>07</day>
					<month>06</month>
					<year>2017</year>
				</date>
			</history>
			<permissions>
				<license license-type="open-access" xlink:href="http://creativecommons.org/licenses/by-nc-nd/4.0/" xml:lang="en">
					<license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution License</license-p>
				</license>
			</permissions>
			<abstract>
				<title>Abstract</title>
				<p>This paper describes a methodology based on the Rosenblueth point estimate method to analyze the active earth pressure developed on retaining walls for c-φ soil backfill under seismic loading conditions. The fundamentals of this methodology are to use two point estimates to examine a variable in the safety analysis: the mean value and the standard deviation. When the horizontal seismic acceleration coefficient increases, the overturning factor of safety decreases, whereas the probability of failure increases, particularly for coefficients greater than 0.2. In addition, the mean factor of safety increases when the vertical seismic acceleration coefficient increases, but the probability of failure remains practically identical for the considered critical factor of safety (1.15).</p>
			</abstract>
			<trans-abstract xml:lang="es">
				<title>Resumen</title>
				<p>En este artículo se describe una metodología basada en el método de estimación puntual de Rosenblueth para el análisis del empuje activo desarrollado en un muro de retención con relleno cohesivo-friccionante bajo condiciones de carga sísmica. El principio básico de esta metodología es usar dos estimaciones puntales, <italic>i.e.</italic>, la desviación estándar y el valor medio, para examinar una variable en el análisis de seguridad. Es posible mostrar que aumentando el valor del coeficiente de aceleración sísmica horizontal, el factor de seguridad por volteo decrece y la probabilidad de falla aumenta, especialmente para coeficientes mayores que 0.2. Por otro lado, es observado que el valor medio del factor de seguridad crece cuando aumenta el coeficiente de aceleración sísmica vertical, sin embargo la probabilidad de falla se mantiene prácticamente igual para el valor del factor de seguridad considerado como crítico (1.15). </p>
			</trans-abstract>
			<kwd-group xml:lang="en">
				<title>Keywords:</title>
				<kwd>probabilistic analysis</kwd>
				<kwd>point estimate method</kwd>
				<kwd>retaining wall</kwd>
				<kwd>seismic loading</kwd>
				<kwd>factor of safety</kwd>
				<kwd>probability of failure.</kwd>
			</kwd-group>
			<kwd-group xml:lang="es">
				<title>Palabras clave:</title>
				<kwd>análisis probabilístico</kwd>
				<kwd>método de estimación puntual</kwd>
				<kwd>muro de retención</kwd>
				<kwd>carga sísmica</kwd>
				<kwd>factor de seguridad</kwd>
				<kwd>probabilidad de falla.</kwd>
			</kwd-group>
			<counts>
				<fig-count count="7"/>
				<table-count count="7"/>
				<equation-count count="28"/>
				<ref-count count="27"/>
				<page-count count="7"/>
			</counts>
		</article-meta>
	</front>
	<body>
		<sec sec-type="intro">
			<title>1. Introduction</title>
			<p>Retaining walls are structures that are usually constructed to form roads, stabilize trenches and soil slopes, and support unstable structures. From the last century until now, works have been performed on the reliability-based design of earth retaining walls, such as [<xref ref-type="bibr" rid="B1">1</xref>,<xref ref-type="bibr" rid="B3">3</xref>,<xref ref-type="bibr" rid="B4">4</xref>,<xref ref-type="bibr" rid="B8">8</xref>,<xref ref-type="bibr" rid="B18">18</xref>,<xref ref-type="bibr" rid="B22">22</xref>-<xref ref-type="bibr" rid="B27">27</xref>].</p>
			<p>Their design must satisfy two major requirements: internal stability, which is ensured by sufficient resistance against bending moments and shear forces, and external stability, which indicates that except for small movements necessary to mobilize the earth pressures, the wall must be in equilibrium under external forces [<xref ref-type="bibr" rid="B15">15</xref>]. These structures are designed to withstand the lateral earth and water pressures, effects of surcharge loads, self-weight of the wall, and earthquake loads in particular cases. Four failures modes can be considered in the design of a gravity retaining wall: (1) overturning of the wall about its toe, (2) sliding along its base, (3) bearing capacity failure of the foundation soil, and (4) overall failure.</p>
			<p>The reliability of a geotechnical design depends on the safety factor, methods of analysis, calculation models, definition of the factor of safety, reliability of the geological model, assessment of the appropriate geotechnical parameters and construction quality. Because of these characteristics, in addition to the common factor of safety analysis, a probabilistic analysis has been used in this paper to illustrate an application of the design of retaining walls. </p>
			<p>This paper presents a Mathematica code [<xref ref-type="bibr" rid="B21">21</xref>], which was developed for the Rosenblueth point estimate approach [<xref ref-type="bibr" rid="B16">16</xref>]. The authors successfully verified the code by computing the overturning failure probability of a retaining wall under static and seismic loading conditions. Based on these results, a design analysis was evaluated.</p>
		</sec>
		<sec>
			<title>2. Factor of safety under seismic conditions</title>
			<p>The existing deterministic approach evaluates the factor of safety against overturning failure about the wall’s toe as follows [<xref ref-type="bibr" rid="B19">19</xref>,<xref ref-type="bibr" rid="B2">2</xref>] (<xref ref-type="fig" rid="f1">Fig. 1</xref>):</p>
			<p>
				<disp-formula id="e1">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e1.jpg"/>
				</disp-formula>
			</p>
			<p>where M<sub>resisting</sub> [ML<sup>2</sup>T<sup>-2</sup>] is the actual resisting moment, and M<sup>overturning</sup> [ML<sup>2</sup>T<sup>-2</sup>] is the overturning moment. The actual resisting moment is given by:</p>
			<p>
				<disp-formula id="e2">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e2.jpg"/>
				</disp-formula>
			</p>
			<p>with:</p>
			<p>
				<disp-formula id="e3">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e3.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e4">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e4.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e5">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e5.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e6">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e6.jpg"/>
				</disp-formula>
			</p>
			<p>where <sub>
 <sup>
 <italic>W1</italic>
</sup> 
</sub> and <sub>
 <sup>
 <italic>W2</italic>
</sup> 
</sub> [MLT<sup>-2</sup>] are the component weights of the retaining wall with horizontal lever distances <sub>
 <sup>
 <italic>Arm1</italic>
</sup> 
</sub> and <sub>
 <sup>
 <italic>Arm2</italic>
</sup> 
</sub> [L], respectively, which are measured from the toe of the wall; γ<sub>wall</sub> [ML<sup>-2</sup>T<sup>-2</sup>] is the unit weight of the retaining wall concrete; (<italic>a</italic> + <italic>b</italic>) [L] is the width of the base of the wall, and <italic>H</italic> [L] is the height of the wall. </p>
			<p>
				<fig id="f1">
					<label>Figure 1</label>
					<caption>
						<title>Geometry of the analyzed retaining wall. </title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gf1.jpg"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>Under seismic loading conditions, the overturning moments is (according to [<xref ref-type="bibr" rid="B18">18</xref>]):</p>
			<p>
				<disp-formula id="e7">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e7.jpg"/>
				</disp-formula>
			</p>
			<p>with:</p>
			<p>
				<disp-formula id="e8">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e8.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e9">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e9.jpg"/>
				</disp-formula>
			</p>
			<p>where <sub>
 <sup>
 <italic>Pae</italic>
</sup> 
</sub> [MLT<sup>-2</sup>] is the seismic active earth thrust with a vertical lever distance <sub>
 <sup>
 <italic>H0e</italic>
</sup> 
</sub> [L]; <sub>
 <sup>
 <italic>Kaec</italic>
</sup> 
</sub> and <sub>
 <sup>
 <italic>Kae</italic>
</sup> 
</sub> 
 <sub>γ</sub> are the seismic active earth pressure coefficients:</p>
			<p>
				<disp-formula id="e10">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e10.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e11">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e11.jpg"/>
				</disp-formula>
			</p>
			<p>with:</p>
			<p>
				<disp-formula id="e12">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e12.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e13">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e13.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e14">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e14.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e15">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e15.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e16">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e16.jpg"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e17">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e17.png"/>
				</disp-formula>
			</p>
			<p>where <sub>
 <sup>
 <italic>ah</italic>
</sup> 
</sub> is the horizontal component of the earthquake acceleration (LT<sup>-2</sup>), <sub>
 <sup>
 <italic>av</italic>
</sup> 
</sub> is the vertical component of the earthquake acceleration (LT<sup>-2</sup>), and <italic>g</italic> is the acceleration due to gravity (LT<sup>-2</sup>).</p>
			<p>Seismic forces that are applied to the mass of the slope are based on a horizontal seismic acceleration coefficient <sub>
 <sup>
 <italic>kh</italic>
</sup> 
</sub> (<xref ref-type="table" rid="t1">Table 1</xref>). The vertical seismic acceleration coefficient <sub>
 <sup>
 <italic>kv</italic>
</sup> 
</sub> is considered equal to zero.</p>
			<p>The minimum factor of safety against overturning failure under seismic loading is 75% of the minimum factor of safety against overturning failure under static loading. The minimum factor of safety against overturning failure under seismic loading is 1.15 [<xref ref-type="bibr" rid="B17">17</xref>].</p>
			<p>
				<table-wrap id="t1">
					<label>Table 1</label>
					<caption>
						<title>Recommended horizontal seismic coefficients. </title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gt1.jpg"/>
					<table-wrap-foot>
						<fn id="TFN1">
							<p><bold>Source:</bold> The authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
		</sec>
		<sec>
			<title>3. Deterministic approach analysis</title>
			<p>A parametric evaluation was conducted to evaluate the factor of safety against overturning failure about the wall’s toe under a seismic loading condition (<xref ref-type="fig" rid="f1">Fig. 1</xref>) using the deterministic approach in Eqs. (1)-(17). <xref ref-type="table" rid="t2">Table 2</xref> describes the parameters in this evaluation. The parameters and properties in this assessment are assumed to be estimated based on a limited number of data or expert opinion.</p>
			<p>
				<table-wrap id="t2">
					<label>Table 2</label>
					<caption>
						<title>Geometry parameters and material properties</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gt2.jpg"/>
					<table-wrap-foot>
						<fn id="TFN2">
							<p><bold>Source:</bold> The authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>The first case was evaluated to describe the effect of the strength properties of the backfill in the overturning stability of the retaining wall under seismic loading conditions. <xref ref-type="fig" rid="f2">Fig. 2</xref> shows that the overturning factor of safety increases with the increase in internal friction angle of the backfill when the parameters <italic>H</italic>, <italic>a</italic>, <italic>b</italic>, γ<sub>wall</sub>, γ<sub>soil</sub>, <italic>c,</italic> and <sub>
 <sup>
 <italic>kv</italic>
</sup> 
</sub> remain constants. <xref ref-type="fig" rid="f2">Fig. 2</xref> also shows that for stability conditions (<sub>
 <sup>
 <italic>FSseismic</italic>
</sup> 
</sub> ≥1.15), the value of <sub>
 <sup>
 <italic>kh</italic>
</sup> 
</sub> must be less than 0.3.</p>
			<p>
				<fig id="f2">
					<label>Figure 2</label>
					<caption>
						<title>Effect of the strength properties of the backfill in the overturning stability of the retaining wall under seismic conditions.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gf2.jpg"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>The second case was evaluated to describe the effect of the geometrical parameters of the wall for the overturning stability of the retaining wall under seismic conditions. <xref ref-type="fig" rid="f3">Fig. 3</xref> shows that the overturning factor of safety decreases with the increase in height of the wall when the parameters <italic>a</italic>, <italic>b</italic>, γ<sub>wall</sub>, γ<sub>soil</sub>, <italic>c</italic>, φ and <sub>
 <sup>
 <italic>kv</italic>
</sup> 
</sub> remain constants. This figure shows that the <sub>
 <sup>
 <italic>kh</italic>
</sup> 
</sub> coefficient has more effect on the lower walls (<italic>H</italic>&lt;6.5m) because the other walls are unstable even under static conditions.</p>
			<p>
				<fig id="f3">
					<label>Figure 3</label>
					<caption>
						<title>Effect of the geometrical parameters of the wall in its overturning stability under seismic conditions.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gf3.jpg"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>The third case was evaluated to describe the effect of the unit weight of the concrete in the overtopping stability of the retaining wall under a seismic condition. <xref ref-type="fig" rid="f4">Fig. 4</xref> shows that the overturning factor of safety increases with the increase in unit weight of concrete in the retaining wall when the parameters <italic>H</italic>, <italic>a</italic>, <italic>b</italic>, γ<sub>soil</sub>, <italic>c</italic>, φ and <sub>
 <sup>
 <italic>kv</italic>
</sup> 
</sub> remain constants. In this case, for stability conditions, the value of <sub>
 <sup>
 <italic>kh</italic>
</sup> 
</sub> must be less than 0.24.</p>
			<p>
				<fig id="f4">
					<label>Figure 4</label>
					<caption>
						<title>Effect of the unit weight of the concrete in the overturning stability of the retaining wall under seismic conditions.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gf4.jpg"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
		</sec>
		<sec sec-type="methods">
			<title>4. Rosenblueth point estimate method</title>
			<p>The probability of failure can be defined as the probability that the factor of safety can be less than 1.5 considering the adverse values of the variables in its calculation. The reliability is the complement of the probability of failure. For example, if there is a 1% probability that the factor of safety against overturning failure is less than 1.5, the reliability is 99%.</p>
			<p>The Rosenblueth point estimate method [<xref ref-type="bibr" rid="B16">16</xref>,<xref ref-type="bibr" rid="B8">8</xref>] can be used to evaluate the structural reliability of the retaining wall against overturning failure. The essence of the Rosenblueth point estimated method is to compute the mean value (μ) and standard deviation (σ) of the factor of safety (<italic>FS</italic>). This methodology selects two point estimates as μ ± σ for a variable, where μ + σ and μ - σ are the positive and negative point estimates, respectively. The result is a total of <sub>
 <sup>
 <italic>2n</italic>
</sup> 
</sub> combinations in point estimates if there are <italic>n</italic> variables in the governing expression of the <italic>FS</italic>. Accordingly, each combination determines <sub>
 <sup>
 <italic>2n</italic>
</sup> 
</sub> 
 <italic>FS</italic>s, from which the mean (μ<sub>
 <italic>FS</italic>
</sub> ) and standard deviation (σ<sub>
 <italic>FS</italic>
</sub> ) of the <italic>FS</italic> are governed by the following mathematical expressions:</p>
			<p>
				<disp-formula id="e18">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e18.png"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e19">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e19.png"/>
				</disp-formula>
			</p>
			<p>where <sub>
 <sup>
 <italic>fi</italic>
</sup> 
</sub> and <sub>
 <sup>
 <italic>wi</italic>
</sup> 
</sub> are the <italic>FS</italic> and weight in the <sub>
 <sup>
 <italic>ith</italic>
</sup> 
</sub> trial, respectively. The mathematical expression of <sub>
 <sup>
 <italic>wi</italic>
</sup> 
</sub> is:</p>
			<p>
				<disp-formula id="e20">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e20.jpg"/>
				</disp-formula>
			</p>
			<p>where ρ<sub>
 <italic>jk</italic>
</sub> is the correlation (-1 to 1) between two variables. <italic>A</italic> is the determinant and equal to 1 or -1. For a given analysis, when the two variables use both positive or negative point estimates, <italic>A</italic> is equal to 1; otherwise, it is -1. Following the computations in μ<sub>
 <italic>FS</italic>
</sub> and σ<sub>
 <italic>FS</italic>
</sub> of the <italic>FS</italic>, the probability of failure can be computed. </p>
			<p>According to the Rosenblueth approach, the factor of safety follows a normal distribution. The normal distribution of <italic>FS</italic> with μ<sub>
 <italic>FS</italic>
</sub> and σ<sub>
 <italic>FS</italic>
</sub> is described by a probability density function (PDF):</p>
			<p>
				<disp-formula id="e21">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e21.jpg"/>
				</disp-formula>
			</p>
			<p>Since the values of the parameters of the probability density function change for each possible combination of μ<sub>
 <italic>FS</italic>
</sub> and σ<sub>
 <italic>FS</italic>
</sub> , the area under the normal distribution curve must be calculated every time the probabilities are calculated. This area is related to the distributions of any mean and standard deviation of the standard normal distribution (μ<sub>
 <italic>FS</italic>
</sub> =0 and σ<sub>
 <italic>FS</italic>
</sub> =1), which is given by:</p>
			<p>
				<disp-formula id="e22">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e22.jpg"/>
				</disp-formula>
			</p>
			<p>with</p>
			<p>
				<disp-formula id="e23">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e23.png"/>
				</disp-formula>
			</p>
			<p>Consequently, the standard normal distribution can be integrated to calculate the area between two limits. The risk of overturning failure of a retaining wall is directly related to the probability of failure, which is obtained by integrating Eq. (24) from <sub>
 <sup>
 <italic>zmin</italic>
</sup> 
</sub> =-∞ to <sub>
 <sup>
 <italic>zmax</italic>
</sup> 
</sub> =β: </p>
			<p>
				<disp-formula id="e24">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e24.jpg"/>
				</disp-formula>
			</p>
			<p>β is the reliability index and corresponds to the number of standard deviations between the most likely value of the factor of safety and the minimum factor of safety against overturning, <italic>i.e.</italic>:</p>
			<p>
				<disp-formula id="e25">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e25.png"/>
				</disp-formula>
			</p>
			<p>where <sub>
 <sup>
 <italic>FSc</italic>
</sup> 
</sub> is the minimum factor of safety against overturning. </p>
			<p>The integral in Eq. (24) can be expressed in a simple closed formula:</p>
			<p>
				<disp-formula id="e26">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e26.png"/>
				</disp-formula>
			</p>
			<p>where erfc(<italic>x</italic>) is the complementary error function.</p>
			<p>As a result, when <sub>
 <sup>
 <italic>fi</italic>
</sup> 
</sub> follows a normal distribution, the probability of failure (<sub>
 <sup>
 <italic>Pf</italic>
</sup> 
</sub> ) is estimated as:</p>
			<p>
				<disp-formula id="e27">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e27.jpg"/>
				</disp-formula>
			</p>
			<p>Finally, the structural reliability of the retaining wall is:</p>
			<p>
				<disp-formula id="e28">
					<graphic xlink:href="0012-7353-dyna-84-202-00009-e28.png"/>
				</disp-formula>
			</p>
		</sec>
		<sec>
			<title>5. Probabilistic analysis</title>
			<p>The factors that contribute to the variability of geotechnical parameters are the anisotropy and heterogeneity of the soil, soil sampling methods, and test methods. The coefficient of variation of cohesion is subject to considerable variation. In this analysis, it is 0.1-0.4. The coefficient of variation of internal friction angle is 0.02-0.13. In contrast, the coefficient of variation of unit weight is practically considered a determined value [<xref ref-type="bibr" rid="B9">9</xref>,<xref ref-type="bibr" rid="B11">11</xref>] and is 0.03-0.07.</p>
			<p>In addition to the variability of geotechnical parameters (<italic>c</italic>, φ and γ), the seismic loading condition considers the variability of the horizontal seismic acceleration coefficient. The coefficient of variation of horizontal seismic acceleration, which is subject to considerable variation, is 0.26-0.34 [<xref ref-type="bibr" rid="B13">13</xref>].</p>
			<p>In this analysis, the deterministic parameters <italic>H</italic>, <italic>a</italic>, <italic>b</italic>, γ<sub>wall,</sub> and <sub>
 <sup>
 <italic>kv</italic>
</sup> 
</sub> are assumed to be constants. They are listed as follows: <italic>H</italic>=5.5 m, <italic>a</italic>=0.4 m, <italic>b</italic>=1.4 m, γ<sub>wall</sub>=24 kN/m<sup>3</sup> and <sub>
 <sup>
 <italic>kv</italic>
</sup> 
</sub> =0. <xref ref-type="table" rid="t3">Table 3</xref> shows the mean, standard deviation, and coefficient of variation of the other parameters.</p>
			<p>
				<table-wrap id="t3">
					<label>Table 3</label>
					<caption>
						<title>Ranges of the backfill property variability</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gt3.jpg"/>
					<table-wrap-foot>
						<fn id="TFN3">
							<p><bold>Source:</bold> The authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>The governing expression of <italic>FS</italic> (Eq. 1) has four variables (<italic>c</italic>, φ, γ<sub>soil</sub>, <sub>
 <sup>
 <italic>kh</italic>
</sup> 
</sub> ), which results in 16 point-estimate combinations. <xref ref-type="table" rid="t4">Table 4</xref> provides these possibilities.</p>
			<p>
				<table-wrap id="t4">
					<label>Table 4</label>
					<caption>
						<title>Overturning factors of safety for point estimates</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gt4.jpg"/>
					<table-wrap-foot>
						<fn id="TFN4">
							<p><bold>Source:</bold> The authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>The mean and standard deviation of the overturning factor of safety can be computed using Eqs. (18) and (19), respectively. <xref ref-type="table" rid="t5">Table 5</xref> shows the calculated values considering the variables <italic>c</italic>, φ, γ<sub>soil</sub> and <sub>
 <sup>
 <italic>kh</italic>
</sup> 
</sub> as independent (<italic>i.e.</italic>, ρ<sub>jk</sub>=0).</p>
			<p>
				<table-wrap id="t5">
					<label>Table 5</label>
					<caption>
						<title>Mean, standard deviation, coefficient of variation and z-value of the Factor of Safety</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gt5.jpg"/>
					<table-wrap-foot>
						<fn id="TFN5">
							<p><bold>Source:</bold> The authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>The probability that the value of <italic>FS</italic> is less than 1.15 is 0.11 (11%). Thus, the structural reliability of this wall against overturning failure about the wall’s toe is 89%.</p>
			<p>Thus, considering the horizontal seismic coefficients in <xref ref-type="table" rid="t1">Table 1</xref>, a seismic analysis for different earthquake intensities was conducted, as shown in <xref ref-type="table" rid="t6">Table 6</xref>.</p>
			<p>
				<table-wrap id="t6">
					<label>Table 6</label>
					<caption>
						<title>Results of the seismic analysis of different earthquake intensities</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gt6.jpg"/>
					<table-wrap-foot>
						<fn id="TFN6">
							<p><bold>Source:</bold> The authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>
				<xref ref-type="fig" rid="f5">Fig. 5</xref> illustrates the probability of failure for different earthquake intensities. This analysis shows that when the horizontal seismic acceleration coefficient increases, the overturning factor of safety decreases, and the probability of failure increases. The probability of failure also dramatically increases from an acceleration coefficient of 0.2 (medium intensity, <sub>
 <sup>
 <italic>Pf</italic>
</sup> 
</sub> =6%) to 0.3 (high intensity, <sub>
 <sup>
 <italic>Pf</italic>
</sup> 
</sub> =28%) and 0.4 (very high intensity, <sub>
 <sup>
 <italic>Pf</italic>
</sup> 
</sub> =62%). In the interpretation of these results, it is important to clarify that this example does not consider the probability of occurrence of a certain level of seismic intensity [<xref ref-type="bibr" rid="B4">4</xref>].</p>
			<p>
				<fig id="f5">
					<label>Figure 5</label>
					<caption>
						<title>Probability of failure versus horizontal seismic acceleration coefficient.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gf5.jpg"/>
					<attrib><bold>Source:</bold> The authors</attrib>
				</fig>
			</p>
			<p>
				<xref ref-type="fig" rid="f6">Fig. 6</xref> illustrates the normal distribution for μ<sub>
 <italic>FS</italic>
</sub> and σ<sub>
 <italic>FS</italic>
</sub> as described in <xref ref-type="table" rid="t5">Table 5</xref> for different vertical seismic acceleration coefficients when the unit weight of the concrete wall is 24 kN/m<sup>3</sup>. The mean overturning factor of safety increases when the vertical seismic acceleration coefficient increases, and the critical factor of safety (<sub>
 <sup>
 <italic>FSc</italic>
</sup> 
</sub> =1.15) for the overturning analysis was reached for all values of vertical seismic acceleration coefficient. Nevertheless, for the cumulative density functions (<xref ref-type="fig" rid="f7">Fig. 7</xref>), the computation of β values for each case shows that the obtained overturning probability of failure (<xref ref-type="table" rid="t7">Table 7</xref>) is practically identical for the three <sub>
 <sup>
 <italic>kv</italic>
</sup> 
</sub> values (8-11%).</p>
			<p>
				<fig id="f6">
					<label>Figure 6</label>
					<caption>
						<title>Normal distribution of μ<sub>
 <italic>FS</italic>
</sub> and σ<sub>
 <italic>FS</italic>
</sub> for different vertical seismic acceleration coefficients.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gf6.jpg"/>
					<attrib><bold>Source:</bold> The authors</attrib>
				</fig>
			</p>
			<p>
				<fig id="f7">
					<label>Figure 7</label>
					<caption>
						<title>Probability of failure for μ<sub>
 <italic>FS</italic>
</sub> and σ<sub>
 <italic>FS</italic>
</sub> for different vertical seismic acceleration coefficients.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gf7.jpg"/>
					<attrib><bold>Source:</bold> The authors</attrib>
				</fig>
			</p>
			<p>
				<table-wrap id="t7">
					<label>Table 7</label>
					<caption>
						<title>Mean, standard deviation, coefficient of variation, probability of failure and structural reliability of the Factor of Safety</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-202-00009-gt7.jpg"/>
					<table-wrap-foot>
						<fn id="TFN7">
							<p><bold>Source:</bold> The authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>There is some theoretical justification for the normal distribution of the factor of safety. The central limit theorem indicates that the sum of many distributions approaches to the normal distribution when the number approaches infinity. However, the use of the normal or any other theoretical distribution to form generalizations about the distributions of data is an assumption, which are made partly because they are considered reasonable approximations of reality and convenient for the calculations of probability and reliability. [<xref ref-type="bibr" rid="B14">14</xref>] provides a complete discussion of the use of the normal distribution.</p>
		</sec>
		<sec sec-type="conclusions">
			<title>6. Conclusions</title>
			<p>In this work, a deterministic approach is proposed to evaluate the factor of safety against the overturning failure of a retaining wall for c-φ soil backfill under seismic loading conditions.</p>
			<p>A Mathematica code was implemented to compute the overturning failure probability of the wall using the deterministic approach and Rosenblueth point estimate method.</p>
			<p>The main conclusions of the deterministic approach analysis are as follows: </p>
			<p>
				<list list-type="alpha-lower">
					<list-item>
						<p>As expected, the overturning factor of safety increases with the increase in internal friction angle of the backfill, and for stability conditions (FS<sub>seismic</sub>≥ .15), the horizontal seismic acceleration coefficient must be less than 0.3.</p>
					</list-item>
					<list-item>
						<p>The horizontal seismic acceleration coefficient has more effect on lower walls (H&lt;6.5 m) because the other walls are unstable even under static conditions.</p>
					</list-item>
					<list-item>
						<p>The overturning factor of safety increases with the increase in unit weight of concrete in the retaining wall. In this case, for stability conditions, the horizontal seismic acceleration coefficient must be less than 0.24.</p>
					</list-item>
					<list-item>
						<p>The main conclusions of the probabilistic analysis are as follows:</p>
					</list-item>
					<list-item>
						<p>When the horizontal seismic acceleration coefficient increases, the overturning factor of safety decreases, and the probability of failure increases, particularly for coefficients greater than 0.2 (medium earthquake intensity). </p>
					</list-item>
					<list-item>
						<p>The probability of failure (not considering the probability of occurrence) dramatically increases from medium to high earthquake intensity (from 6 to 28%) and from high to very high intensity (from 28 to 62%).</p>
					</list-item>
					<list-item>
						<p>The mean factor of safety increases with the increase in vertical seismic acceleration coefficient. Nevertheless, for the considered value of the critical factor of safety (1.15), the probability of failure remains practically identical when the acceleration coefficient increases.</p>
					</list-item>
				</list>
			</p>
			<p>The paper illustrates a specific application, but the Mathematica code can be easily modified for other conditions such as when water pressures or surcharge loads are considered. The methodology in this work appears to be a good framework for designers to make decisions about the security and costs of a retaining wall project.</p>
		</sec>
		<sec>
			<title>Acknowledgements</title>
			<p>The authors acknowledge the support of the following institutions: the Brazilian National Council for Scientific and Technological Development (CNPq-Project 30449420127), the Coordination for the Improvement of Higher Level Personnel (CAPES-Project 1431/14-5), and the University of Brasilia for funding this research.</p>
		</sec>
	</body>
	<back>
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				<p><bold>How to cite:</bold> Brasil-Cavalcante, A.L. and Rodriguez-Rebolledo, J.F., Probabilistic analysis of the active earth pressure on retaining wall for c-φ soil backfill under seismic loading conditions DYNA, 84(202), pp. 9-15, September, 2017.</p>
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