<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">GEP</journal-id><journal-title-group><journal-title>Journal of Geoscience and Environment Protection</journal-title></journal-title-group><issn pub-type="epub">2327-4336</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/gep.2016.46004</article-id><article-id pub-id-type="publisher-id">GEP-67271</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Assessment of the Internal Instability for Granular Soils Subjected to Seepage
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Marx</surname><given-names>Ferdinand Ahlinhan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Marius</surname><given-names>Bocco Koube</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Codjo</surname><given-names>Edmond Adjovi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Ecole des Sciences et Techniques du Batiment et de la Route (ESTBR), Université Polytechnique d’Abomey (UPA), Abomey, Benin</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>ahlinhan@yahoo.fr(MFA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>06</month><year>2016</year></pub-date><volume>04</volume><issue>06</issue><fpage>46</fpage><lpage>55</lpage><history><date date-type="received"><day>18</day>	<month>April</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>10</month>	<year>June</year>	</date><date date-type="accepted"><day>13</day>	<month>June</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The knowledge of the internal stability of granular soils is a key factor for the design of granular and filter for the geotechnical infrastructures such as dykes, barrages, weirs and roads embankment. To evaluate the internal instability of granular soils different criteria are generally used in the practice. However, the results of these criteria on the same soil may lead to different evaluations of the internal instability. In this paper the common criteria used for the internal instability have been presented and compared as far as possible. It was found that the most internal instability criteria define a limit value for the secant slope of the grain size distribution curve of the granular soils. Based on this finding an own criterion for the evaluation of the internal instability of granular soil has been developed and compared to the common criteria. A very good agreement between some criteria was found. Furthermore, a site specific assessment for the evaluation of the internal instability of granular soil has been proposed in order to get more confidence in this evaluation.
 
</p></abstract><kwd-group><kwd>Internal Instability</kwd><kwd> Granular Soils</kwd><kwd> Seepage</kwd><kwd> Dams</kwd><kwd> Dykes</kwd><kwd> Site Specific Assessment</kwd><kwd> Instability Index</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Internal instability or suffusion is a failure mode of the soil subjected to seepage. This failure mode is characterized by the wash out of the fine fraction through the pore matrix of the coarse fraction of the soil. The results are segregation in soil, a modification of the drainage properties, possible increase of the soil permeability of the porosity of the bulk density, and of the pore pressure. As consequence the resistance of the soil against external load decreases and the settlement increases.</p><p>Likewise, all drainage solutions become inefficient with the time due to migration of fine grains also internal instability or piping, Chapuis (1992) [<xref ref-type="bibr" rid="scirp.67271-ref1">1</xref>] . Therefore, the internal instability of soil is an essential problem for the long term stability of earth structures (dykes, dams, weirs, road embankment) subjected to seepage. According to Foster et al. (2000) [<xref ref-type="bibr" rid="scirp.67271-ref2">2</xref>] internal erosion and piping are a significant cause of failure and accidents affecting embankment dams.</p><p>To assess whether internal instability or suffusion is possible, two criteria i.e. the geometric criterion and the hydraulic criterion have to be fulfilled. For the geometric criterion, the proof consists to check whether it is possible that fine grains are able to pass through the smallest constrictions along the relevant pore path of coarse soil fraction without clogging. For that, the geometry of the pore channels has to be considered. Since the pore channel geometry cannot be exactly measured, the assessment is generally based on the curve of the grain size distribution, which is related to the pore channel geometry.</p><p>When the geometric criterion shows that the migration of fine fraction of the soil is possible, it has to be checked whether the hydrodynamic load in the pore structure provides a critical energy to mobilize and to transport fines grains (hydraulic criteria). Only the geometric criteria have been dealt in this paper, for the hydraulic criteria reference is made to Ahlinhan (2011) [<xref ref-type="bibr" rid="scirp.67271-ref3">3</xref>] and Ahlinhan et al. (2010) [<xref ref-type="bibr" rid="scirp.67271-ref4">4</xref>] .</p><p>The geometric criteria for the internal instability can be classified in three categories as follows:</p><p> the geometric criteria based on the pore constriction size</p><p> the geometric criteria based on filter rules, and</p><p> the geometric criteria based on comparison between the curve of the grain size distribution of the soil concerned and the curves of the grain size distribution of theoretical stable soils.</p><p>The above mentioned criteria are presented (Section 2 to Section 4) and compared (Section 5). Then, a resultant geometric criterion is developed in Section 6. Moreover a site specific assessment for the internal instability is proposed in Section 7.</p></sec><sec id="s2"><title>2. Criteria Based on the Pore Constriction Size</title><p>A simple geometric criterion for the internal stability of granular soils is the requirement that the pore diameter d<sub>p</sub> shall be smaller than the smallest grain diameter d<sub>min</sub>.</p><disp-formula id="scirp.67271-formula618"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x7.png"  xlink:type="simple"/></disp-formula><p>Kovacs (1981) [<xref ref-type="bibr" rid="scirp.67271-ref5">5</xref>] proposed a geometric criterion for the internal stability given in Equations (2) and (3), which were based on the capillary tubes model. The capillary tubes model supposes a hydraulic similarity between the network of the pore channel and the capillary tubes. The conduits of the pore channels are supposed to be parallel to the seepage direction as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><disp-formula id="scirp.67271-formula619"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x8.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Capillary tubes model as per Kovacs (1981) [<xref ref-type="bibr" rid="scirp.67271-ref5">5</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x9.png"/></fig><p>or</p><disp-formula id="scirp.67271-formula620"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x10.png"  xlink:type="simple"/></disp-formula><p>Here, n is the porosity, d<sub>h</sub> is the effective grain diameter, α is the shape factor and d<sub>0</sub> is the mean diameter of the channels. Equations (2) and (3) show that the quotient of two grains diameters arbitrary of a grain size distribution curve e.g. d<sub>h</sub>/d<sub>min</sub> shall be smaller than a value depending on the porosity of the soil concerned.</p><p>Based on this approach, Istomina (1957)―cited in Busch et al. (1993) [<xref ref-type="bibr" rid="scirp.67271-ref6">6</xref>] ―developed a geometric criterion for the suffusion considering the coefficient of uniformity U. For the suffusion stable soil the coefficient of uniformity U shall be smaller than 10, for the suffusion unstable soil the coefficient of uniformity U shall be larger than 20. Soil in transition zone fulfills following requirement: 10&lt; U ≤ 20.</p></sec><sec id="s3"><title>3. Criteria Based on the Filter Rules</title><p>The internal instability criteria based on the filter rules compare the ratio of mass percent for two grain diameters with a constant value. As explained above, internal stability is the detachment, and the transport of the fine grains of a soil through the grain skeleton formed by the coarse parts. It can be considered as a contact erosion process (i.e. the wash-out of a fine soil through the pores of an adjacent coarse soil layer) between the fine and coarse parts of the soil. Based on this consideration, Kezdi (1979) [<xref ref-type="bibr" rid="scirp.67271-ref7">7</xref>] proposed splitting up the grain size distribution of a soil into two grain size distributions, i.e. the fine and coarse parts, and assessing the stability by Terzaghi’s well-known filter criterion applied to the two curves of the grain size distributions. This criterion, also known as Terzaghi’s filter rule, is formulated as follows:</p><disp-formula id="scirp.67271-formula621"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x11.png"  xlink:type="simple"/></disp-formula><p>Here, d<sub>15F</sub> is grain diameter for which 15% of the grains by weight of the coarse soil are smaller and d<sub>85b</sub> is grain diameter for which 85% of the grains by weight of the fine soil are smaller.</p><p>The filter rule according to Sherard (1979) [<xref ref-type="bibr" rid="scirp.67271-ref8">8</xref>] is formulated as follows:</p><disp-formula id="scirp.67271-formula622"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x12.png"  xlink:type="simple"/></disp-formula><p>However, the Terzaghi criterion is valid only for poorly graded soil. To avoid this limitation, in the German guideline BAW (1989) [<xref ref-type="bibr" rid="scirp.67271-ref9">9</xref>] the splitting method is recommended in combination with the Cistin and Ziems contact erosion criterion (see Ahlinhan et al. 2010 [<xref ref-type="bibr" rid="scirp.67271-ref4">4</xref>] ), which is also applicable to non-uniform soils. In general, the grain size distribution curve has to be split up at several points and the resulting fine and coarse soils have to be assessed with the contact erosion criterion given in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Filter criterion according to Cistin and Ziems (1968) in [<xref ref-type="bibr" rid="scirp.67271-ref9">9</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x13.png"/></fig><p>Burenkova (1993) [<xref ref-type="bibr" rid="scirp.67271-ref10">10</xref>] proposed a method based on results of laboratory tests on 22 granular soils of maximum size up to 100 mm and coefficient of uniformity U up to 200. Based on the three fractions d<sub>15</sub>, d<sub>60</sub> and d<sub>90</sub>, the internal stability of the soil was described by two ratios called conditional factors of uniformity d<sub>90</sub>/d<sub>60</sub> and d<sub>90</sub>/d<sub>15</sub>. With these two factors of uniformity, Burenkova (1993) [<xref ref-type="bibr" rid="scirp.67271-ref10">10</xref>] presented boundaries between the suffusive soils and the non-suffusive soils as shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. Zone I and III represent suffusive granular soils, Zone II represents non-suffusive granular soils and Zone IV represents artificial soils. The zone for non-suffusive granular soils can approximately be expressed in function of the defined conditional factors of uniformity as follows:</p><disp-formula id="scirp.67271-formula623"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x14.png"  xlink:type="simple"/></disp-formula><p>In addition to the criterion for suffusion, an approximate diameter d<sub>d</sub> dividing the suffusive and non-suffusive portion is also defined as follows:</p><disp-formula id="scirp.67271-formula624"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x15.png"  xlink:type="simple"/></disp-formula><p>Wan and Fell (2008) [<xref ref-type="bibr" rid="scirp.67271-ref11">11</xref>] performed laboratory tests regarding internal instability of silt-sand-gravel and clay- silt-sand-gravel soils. Based on the results of these tests and of tests by others researchers, Wan and Fell (2008) [<xref ref-type="bibr" rid="scirp.67271-ref11">11</xref>] described a method for assessing the potential, the probability of internal instability and a criterion of internal instability, which is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Suffusion criterion according to Burenkova (1993) [<xref ref-type="bibr" rid="scirp.67271-ref10">10</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x16.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Alternative method for assessing internal instability of broadly graded silt-sand-gravel [<xref ref-type="bibr" rid="scirp.67271-ref16">16</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x17.png"/></fig></sec><sec id="s4"><title>4. Criteria Based on the Comparison with Theoretical Stable Soils</title><p>Lubochkov (1965)―cited in Kovacs (1981) [<xref ref-type="bibr" rid="scirp.67271-ref5">5</xref>] ―carried out laboratory tests regarding the suffusion and derived an analytical and graphical method for the proof of the internal instability. Grain size distributions lying between the borderlines given in <xref ref-type="fig" rid="fig5">Figure 5</xref> can be considered as geometric stable soils regarding suffusion. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows also the well-known theoretical stable Fuller curve, which is generally applied for the formulation of granular for concrete. It can be seen that the Fuller curve lies in the middle of the borderlines.</p><p>Based on the laboratory tests Lubochkov (1965)―cited in Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref12">12</xref>] ―established that the grading curve of a suffusion stable soil can be expressed as follows:</p><disp-formula id="scirp.67271-formula625"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x18.png"  xlink:type="simple"/></disp-formula><p>Here, d<sub>60</sub> is the particle size for 60% mass percent, d is an arbitrary particle size between d<sub>0</sub> and d<sub>100</sub>, and F is the masse percent of particles smaller than d.</p><p>Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] transformed the Equation (8) as follows:</p><disp-formula id="scirp.67271-formula626"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x19.png"  xlink:type="simple"/></disp-formula><p>Here, H is the masse fraction between d and 4d.</p><p>There was a particular reason for choosing the interval between d and 4d. The size of the relevant constriction in a void network of a filter is approximately equal to one quarter of the size of particles for the filter, Kenney et al. (1985) [<xref ref-type="bibr" rid="scirp.67271-ref14">14</xref>] and Kenney et al. (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] . This means that particles of size d can migrate through constrictions in a filter formed by particles of size 4d or larger. To prevent such transport these constrictions would have to be clogged by particles larger than d. The value H, mass fraction of particles between sizes d and 4d, provides some measure of the number of particles in a soil material that would form constrictions sufficiently small to prevent the passage of particles size d. For particles of size d to be removed by seepage there must be a deficiency in the number of particles in the size range between d and 4d, but if H were sufficiently large, particles of size d would not be transported.</p><p>The results of the laboratory tests performed by Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] confirmed the Equation (9). Therefore, Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] proposed transforming the grain size distribution curve to F-H diagram. Here F is the mass percentage of grains with diameters less than a diameter d and H is the mass percentage of grains with diameters between d and 4d (<xref ref-type="fig" rid="fig6">Figure 6</xref>). A portion F ≤ 0.20 of the grain size distribution has to be investigated for a widely graded soil, whereas a portion F ≤ 0.30 of the grain size distribution is required for a narrowly graded soil. In Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] H/F ≥ 1.3 was proposed as geometric internal stability criterion. In a following publication (Kenney and Lau 1986 [<xref ref-type="bibr" rid="scirp.67271-ref12">12</xref>] ) based on the discussion by Milligan (1986) [<xref ref-type="bibr" rid="scirp.67271-ref15">15</xref>] and Sherard and Dunnigan (1986) [<xref ref-type="bibr" rid="scirp.67271-ref16">16</xref>] , the less conservative requirement H/F ≥ 1.0 was recommended for use.</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Borderlines for non-suffusive soils according to Lubochkov (1965)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x20.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Geometric criterion for the internal stability according to Kenney et Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x21.png"/></fig></sec><sec id="s5"><title>5. Comparison between the Criteria of Internal Instability</title><p>Chapuis (1992) [<xref ref-type="bibr" rid="scirp.67271-ref1">1</xref>] demonstrated a mathematical similarity between the criteria for the internal instability. Here, these criteria for the internal instability were expressed as similar slope criteria. The slope of the grain size distribution curve at any point has been approximated by the slope of the secant line. Then, the secant slope of the grain size distribution curve indicates the risk of the internal stability.</p><p>Let us call I the point at which the grain size distribution curve is divided in fine and coarse fraction (<xref ref-type="fig" rid="fig7">Figure 7</xref>).</p><p>The mass percentage for particle size smaller than the size d<sub>I</sub> is called y<sub>I</sub>. In the fine portion, the abscise of the point J is x<sub>J</sub> = logd<sub>85b</sub> and its masse percentage is y<sub>J</sub> = 0.85y<sub>I</sub>. In the coarse portion, the abscise of the point K is to x<sub>K</sub> = logd<sub>15F</sub> and its mass percentage is:</p><disp-formula id="scirp.67271-formula627"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x22.png"  xlink:type="simple"/></disp-formula><p>The secant slope s<sub>JK</sub> between the points J and K can be expressed as:</p><disp-formula id="scirp.67271-formula628"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x23.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67271-formula629"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x24.png"  xlink:type="simple"/></disp-formula><p>Equation (4) in Equation (12) can be expressed as follows:</p><disp-formula id="scirp.67271-formula630"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x25.png"  xlink:type="simple"/></disp-formula><p>In a similar way the Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] criterion can be expressed as follows:</p><disp-formula id="scirp.67271-formula631"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x26.png"  xlink:type="simple"/></disp-formula><p>Therefore, the Kezdi (1979) [<xref ref-type="bibr" rid="scirp.67271-ref7">7</xref>] criterion is equivalent to the following: if a soil has in its grain size distribution curve a slope larger than 24.91% per cycle, it will be able to stabilize its own particles finer than the grain size at which such slope occurs (see equation 13). Likewise, the Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] method is equivalent to the following: at a particle size d<sub>y</sub> (y ≤ 20%), the slope per cycle of the grain size distribution curve must be larger than 1.66∙H to have internal stability.</p><p>The criteria based on the filter rules compare the slope of the grain size distribution curve with a constant value 24.91% by the Kezdi (1979) [<xref ref-type="bibr" rid="scirp.67271-ref7">7</xref>] criterion and 21.45% by Sherard (1979) [<xref ref-type="bibr" rid="scirp.67271-ref8">8</xref>] criterion, whereas the criteria based on the Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref13">13</xref>] criterion compares the slope of the grain size distribution curve with a value which depends on the mass percentage.</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Illustration for the determination of the mass percentage of d<sub>85b</sub> and d<sub>15F</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x27.png"/></fig></sec><sec id="s6"><title>6. Proposed Approach to Assess the Internal Instability of Granular Soil</title><p>Theoretical considerations were made in order to define the point at which the split-up of the curve of the grain size distribution should be carried out. In general, the grain size distribution might be split at several points. For the illustration of the splitting up approach in <xref ref-type="fig" rid="fig8">Figure 8</xref> two points T<sub>1</sub> and T<sub>2</sub> have been exemplary considered. The steeper the grading curve, the smaller is the distance b between fine and coarse fraction obtained from the splitting up of the grain size distribution curve at a point T (<xref ref-type="fig" rid="fig8">Figure 8</xref>). A maximum distance b between the fine fraction (base) and the coarse fraction (filter) represents the worst case scenario for the geometric stability of the soil. The secant slope β between a horizontal axis and the grading curve at the split-off point T can be expressed as follows:</p><disp-formula id="scirp.67271-formula632"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2170202x28.png"  xlink:type="simple"/></disp-formula><p>Here, d is the particle diameter at the split-off point T, F the mass fraction of particles smaller than d and H the mass fraction of particles between d and 4d. If b is maximal, β is minimal, and then H also becomes minimal. Therefore, it is proposed to split the grading curve at (H/F)<sub>min</sub>. The associated filter quotient is denoted as a modified filter or instability index (d<sub>15f</sub>/d<sub>85b</sub>)<sub>mod</sub>. The point (H/F)<sub>min</sub> represents a “weak point” for the soils and is therefore relevant for the assessment of its geometric stability. For internal stable soil the instability index (d<sub>15f</sub>/d<sub>85b</sub>)<sub>mod</sub> shall be smaller than 4, Ahlinhan [<xref ref-type="bibr" rid="scirp.67271-ref3">3</xref>] .</p><p>The above mentioned criteria for the internal stability cannot generally be compared with each other except the criteria based on filter rules and the Kenney and Lau (1986) criterion [<xref ref-type="bibr" rid="scirp.67271-ref12">12</xref>] . Therefore, five (5) granular soils with grain size distribution curves shown in <xref ref-type="fig" rid="fig9">Figure 9</xref> have been selected and analyzed regarding the internal instability criteria. The geometric parameters such as H, F, and d<sub>x</sub><sub>%</sub> can be derived from the grain size distribution curves.</p><p>The geometric criteria after Kezdi (1979) [<xref ref-type="bibr" rid="scirp.67271-ref7">7</xref>] and Kenney and Lau (1985) [<xref ref-type="bibr" rid="scirp.67271-ref12">12</xref>] are depicted in <xref ref-type="fig" rid="fig1">Figure 1</xref>0, our own test results and the test results of several authors regarding the internal stability of soils are presented [<xref ref-type="bibr" rid="scirp.67271-ref3">3</xref>] . <xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows that all soils with points lying above the Kenney and Lau (1986) line are stable and all soils with points lying below the Kezdi (1979) line are unstable. Soils with points lying in the transition zone (H &gt; F &lt; 0.15 and 0.15 &lt; H &lt; F) can obviously be either stable or unstable depending on the hydrodynamic energy.</p><p><xref ref-type="table" rid="table1">Table 1</xref> summarizes the results of the internal instability analysis for the reference soils. The results of the confrontation of internal stability criteria in <xref ref-type="table" rid="table1">Table 1</xref> show a general good agreement between the here proposed criterion and the criteria as per Lubochkov (1965), Kenney and Lau (1986) and BAM MSD (1989). However, these four criteria do not lead to the same prediction of the internal instability for the soil E1. This could be explained by the specific limit of boundary for each criterion, which has to be considered in a framework of the assessment of internal stability.</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Illustration for the determination of the mass percentage of d<sub>85b</sub> and d<sub>15F</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x29.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Grain size distribution curves of the reference soils</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x30.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Compilation of the test results regarding internal instability of granular soil [<xref ref-type="bibr" rid="scirp.67271-ref3">3</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2170202x31.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Evaluation results of the geometric internal stability for the reference soils</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Parameters/criteria</th><th align="center" valign="middle"  colspan="5"  >Reference soils</th></tr></thead><tr><td align="center" valign="middle" >A1</td><td align="center" valign="middle" >A2</td><td align="center" valign="middle" >E1</td><td align="center" valign="middle" >E2</td><td align="center" valign="middle" >E5</td></tr><tr><td align="center" valign="middle" >Coefficient of uniformity U</td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >3.00</td><td align="center" valign="middle" >6.80</td><td align="center" valign="middle" >13.50</td><td align="center" valign="middle" >23.40</td></tr><tr><td align="center" valign="middle" >Ratio (H/F)<sub>min</sub></td><td align="center" valign="middle" >2.92</td><td align="center" valign="middle" >3.23</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.03</td></tr><tr><td align="center" valign="middle" >(d<sub>15F</sub>/d<sub>85b</sub>)<sub>mod</sub></td><td align="center" valign="middle" >1.21</td><td align="center" valign="middle" >1.41</td><td align="center" valign="middle" >3.80</td><td align="center" valign="middle" >7.20</td><td align="center" valign="middle" >13.84</td></tr><tr><td align="center" valign="middle" >Istomina (1957)</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S/U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >Cistin (1965)</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >Lubochkov (1965)</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >Kezdi (1979) @ (H/F)<sub>min</sub></td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >Sherard (1979) @ (H/F)<sub>min</sub></td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >De Mello (1975) @ (H/F)<sub>min</sub></td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >Kenney et Lau (1986)</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >BAW MSD (1989) @ (H/F)<sub>min</sub></td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr><tr><td align="center" valign="middle" >Proposed method</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >S/U</td><td align="center" valign="middle" >U</td><td align="center" valign="middle" >U</td></tr></tbody></table></table-wrap><p>Legend: S for geometric Stable; U for geometric Unstable; S/U geometric Stable or Unstable (transition zone).</p></sec><sec id="s7"><title>7. Site Specific Assessment (SSA) for the Internal Instability</title><p>A site specific assessment regarding internal stability is recommended for the construction or the rehabilitation of dykes, barrages, weirs, road embankment, etc. To carry the site specific assessment the environmental data such as water depth, seepage condition, seepage velocity, hydraulic gradient are required. These environmental data are the effect of action. Moreover the site specific geotechnical data, which are the resistance, must be considered. The type and amount of the geotechnical data required will depend on the particular circumstances such as the type of the geotechnical infrastructure (dykes, barrages, weirs, road embankment, etc.) and previous experience of the site, or nearby or similar sites, for which the assessment is being performed. Such geotechnical information includes shallow seismic survey, coring data, cone penetrometer tests, side-scan sonar, magnetometer survey and diver’s survey. The environmental and geotechnical data have to be considered for the evaluation of the internal stability of the soil as follows:</p><p>1) Carry out analysis regarding the susceptibility to internal stability by applying relevant criteria, e.g. Ahlinhan et al. (2011) [<xref ref-type="bibr" rid="scirp.67271-ref3">3</xref>] , Kenney and Lau (1986) [<xref ref-type="bibr" rid="scirp.67271-ref12">12</xref>] Kezdi (1979) [<xref ref-type="bibr" rid="scirp.67271-ref7">7</xref>] and Lubochkov (1965) [<xref ref-type="bibr" rid="scirp.67271-ref5">5</xref>] . The Interpretation of the results of this analysis has to be performed with sound engineering judgment.</p><p>2) Take reasonably into account the complex soil structure, its variability its non-homogeneity (layered soils, soils variability, etc.) for some laboratory tests regarding the internal instability.</p><p>3) Compare the results from (1) and (2) in order to get more confidence for the assessment of the internal stability.</p><p>For economic reason the unstable soils may be used in the practice. For that, it has to be proved that hydrodynamic energy i.e. the hydraulic gradient and the velocity of the seepage will not reach the critical one.</p></sec><sec id="s8"><title>8. Conclusions</title><p>The main criteria for the internal instability of the granular soil subjected to seepage have been presented and compared. These main criteria can be classified in three categories, i.e. the criteria based on the pore distribution or constriction size, the criteria based on filter rules, and the criteria based on the comparison of the grain size distribution curve with the grain size distribution curve of a theoretical stable soil. The comparison shows that the criteria based of filter rules (e.g. Sherard (1979) [<xref ref-type="bibr" rid="scirp.67271-ref8">8</xref>] , and Kezdi (1979) [<xref ref-type="bibr" rid="scirp.67271-ref7">7</xref>] ) and the criteria based the criteria based on the comparison of the grain size distribution curve with the grain size distribution curve of a theoretical stable soil (e.g. Lubochkov (1969) in [<xref ref-type="bibr" rid="scirp.67271-ref5">5</xref>] , Kenney et Lau (1986) [<xref ref-type="bibr" rid="scirp.67271-ref12">12</xref>] ) can be replaced by minimum value for the secant slope of the grain size distribution curve. The criteria based on the filter rules compare the secant slope of the grain size distribution curve with a constant value (24.91% by the Kezdi (1979) [<xref ref-type="bibr" rid="scirp.67271-ref7">7</xref>] criterion and 21.45% by Sherard (1979) [<xref ref-type="bibr" rid="scirp.67271-ref8">8</xref>] criterion. But the criteria based on the comparison of the grain size distribution curve of the soil concerned with the grain size distribution of theoretical stable soil compare the secant slope of the grain size distribution curve with a value which depends on the mass percentage. A good agreement between the proposed criterion and the common criteria has been observed for the splitting of the grain size distribution curve at (H/F)<sub>min</sub>. It should be noted that these geometric criteria are based on the resistance that means the pore distribution or the constriction size or the grain size distribution curve of the soil, but not the effect of action or the loading that means the seepage velocity, the hydraulic gradient. Therefore, combined geometric and hydraulic criteria will be an economical design approach, since unstable soils are often used in the practice, when the hydrodynamic energy, the hydraulic gradient, and the seepage velocity are lower than the critical one.</p><p>Moreover, a site specific assessment regarding the internal stability has been proposed for engineering practice. Hence, this paper presents a practical approach to analyze the geometric internal instability. However, a development of a software tool which would consider the grain size distribution curve (resistance) and the hydrodynamic energy (effect of action), would be very helpful for the design and analysis with respect to the internal instability.</p></sec><sec id="s9"><title>Acknowledgements</title><p>This research was partially supported by the Germany Ministry of Education and Research through IPSWaT (International Postgraduate Studies in Water Technologies). This support is gratefully acknowledged.</p></sec><sec id="s10"><title>Cite this paper</title><p>Marx Ferdinand Ahlinhan,Marius Bocco Koube,Codjo Edmond Adjovi, (2016) Assessment of the Internal Instability for Granular Soils Subjected to Seepage. Journal of Geoscience and Environment Protection,04,46-55. doi: 10.4236/gep.2016.46004</p></sec><sec id="s11"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.67271-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Chapuis, R.P. (1992) Similarity of Internal Stability Criteria for Granular Soils. Canadian Geotechnical Journal, 29, 711-713. http://dx.doi.org/10.1139/t92-078</mixed-citation></ref><ref id="scirp.67271-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Foster, M., et al. (2000) A Method for Assessing the Relative Likelihood of Failure of Embankment Dams by Piping. Canadian Geotechnical Journal, 37, 1025-1061. http://dx.doi.org/10.1139/t00-029</mixed-citation></ref><ref id="scirp.67271-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Ahlinhan, M.F. (2011) Investigation of the Internal Stability of Non-Cohesive Soils. 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