Open access peer-reviewed chapter

The Grading Entropy-Based Criteria for Structural Stability of Granular Materials and Filters

By János Lőrincz, Emöke Maria Imre and Vijay Pal Singh

Submitted: November 18th 2016Reviewed: April 12th 2017Published: September 6th 2017

DOI: 10.5772/intechopen.69167

Downloaded: 480

Abstract

Some rules for particle migration, filtering, and segregation were elaborated on the basis of some simple laboratory tests and data of well-designed, artificial mixtures of natural sand grains. Use was made of the knowledge available in the field and two pairs of grading entropy parameters. These parameters incorporate all information of the grading curve and are pseudo-metrics in the “space of the possible grading curves.”

Keywords

  • grading entropy
  • internal erosion
  • suffosion
  • filtering
  • segregation
  • piping

1. Introduction

The internal stability of compacted earth dam materials, granular filters, and soils on natural slopes is essential. The internal erosion involves loss of particles under seepage flow; the matrix of coarse soil particles may or may not be unstable [13]. The term “suffosion” is Russian in origin and is used to describe the process of removal and transport of small soil particles through pores [4, 5].

It is desirable that adjacent materials in earth dams or rockfill dams should act as filters for each other and the material should not segregate [614]. Broadly graded materials may segregate during the construction process where the particles are able to flow freely, such as tipping and spilling. The likelihood of backward erosion is greater for segregated soil than for non-segregated soil [7, 8].

The inherent stability or proneness to segregation is usually specified in terms of particular diameters Dx (or dx), which represent the particle diameter for which x% of grains (by weight) are smaller. The susceptibility to suffosion is assessed by the graphical approach [5], where a grain size distribution is compared with empirical upper- and lower-bound thresholds; the method is not valid for gap-graded grading. The filter rules—the compacted earth dam or core material should obey when associated with each other and with the dam base—are formulated in terms of pairs of grading curve points [915], which is “too simple” in case of broadly graded soils.

This chapter summarizes three grading entropy-based rules, on the basis of the original work of Lőrincz and some applications [1522]. The suggested rules differ from most existing rules in that the whole grading curve is used instead of some limited number of grading curve points, without any constraint on the shape of the grading curve. They were elaborated on the basis of the knowledge available, the measured data available in the literature, and data measured for well-designed sand mixtures by Lőrincz. The rules were verified by the examined cases [1922], an example included.

2. Grading curve characterization

The grading curve is a statistical distribution of logarithm of the diameter with respect to the dry weight. It is a discrete distribution curve with a non-uniform cell system in arithmetic scale. To characterize it, first of all, the statistical cell system—the so-called abstract fraction system—is defined and the space of the grading curve is introduced.

Then the two grading entropy parameter pairs are introduced. The first pair is related to the expected (log diameter) value of the grain size distribution, in non-normalized and normalized forms. The normalized version has a shift symmetry on the log d axis.

The second pair is the entropy arisen from the mixing of the fractions, in non-normalized and normalized forms. Its maximum for a fixed value of the first coordinate is related to a single grading curve with finite fractal distribution. The grading curves can be represented in terms of the two parameters in the entropy diagram.

2.1. The fractions

The fraction system is defined on the pattern of the classical sieve hole diameters (where measurements are made), by successive multiplication with a factor of 2, as follows. The diameter range for fraction j (j = 1, 2…, see Table 1):

Fraction number j12324
d [–]d0 to 2 d0222 d0 to 223 d0223 d0 to 224 d0
d [mm]2−22 to 2−211–22–4
S0j [–]12324

Table 1.

Definitions of fractions, based on the smallest particles likely to occur in nature.

2jd0d>2j1d0,E1

or the upper diameter range for fraction j:

dj=2dj1E2

Using log2 form results in an integer increment by each multiplication and fraction as follows:

log2dj=1+log2dj1E3

The variable d0 is the arbitrary smallest diameter, and assumingly a 2-power, d0 = 2−k. Its possible value is equal to the height of the SiO4 tetrahedron (d0 = 2−22 mm).

log2d1=1+22E4

The fraction serial number variable can be expressed by the diameter:

j=k+log2djE5

The integer j/j − 1 is a so-called abstract upper/lower diameter limit (log2 dj shifted by k).

2.2. The grading curve space

By the measurements of the fractions during sieving, the relative frequencies of the fractions xj (j = 1, 2, 3…N) can be determined. These fulfill the following equation of each grading curve:

j = 1xj=1,xj0E6

which can be rewritten as follows:

i=1Nxi=1,xi0,N1.E7

where i is a rescaled fraction serial number being equal to 1 at the finest non-zero fraction with original serial number jmin (see Table 1), the integer variable N is the number of the fractions between the finest jmin and coarsest jmax non-zero fractions:

N=jmaxjmin+1.E8

The space of the grading curves with N fractions can be identified with the N − 1-dimensional, closed simplex (which is the N − 1-dimensional analogy of the triangle or tetrahedron, the two- and three-dimensional instances, Figure 1) as follows. Each grading curve is related to a simplex point, the relative frequencies xi can be identified with the barycentric coordinates of the points of the N − 1-dimensional closed simplex.

Figure 1.

(a) Standard simplex images with dimension less than 4. (b) The lattice of the continuous sub-simplexes of the six-dimensional simplex.

2.3. The grading entropy coordinates of the grading curve

The grading entropy concept is an application of the statistical entropy to the grading curve [15, 23], by introducing a uniform cell system for the derivation besides the fractions. It condenses the information of the whole grading curve into two pairs of parameters. The grading entropy S is the sum of two “means” [15]:

S=S0+ΔSE9

which are called as base entropy S0 and entropy increment ΔS. The base entropy S0 is a weighted mean or expected value of the fraction serial number:

S0=i=iminimaxxiS0iE10

which depends linearly on the log2 diameter d (see Eq. (5)), S0i is the grading entropy of the ith fraction, being identical to the fraction serial number (see Table 1):

S0i=iE11

Any decrease in the base entropy S0 can be explained by the decrease of the mean grain diameter, for example, due to breakage. Any increase in the base entropy S0 can be explained by the increase of the mean grain diameter, for example, due to suffosion or segregation.

The relative base entropy A is defined as follows:

A=S0S0minS0maxS0minE12

where S0max and S0min are the entropies of the largest and the smallest fractions in the mixture, respectively.

The relative base entropy A varies between 0 and 1, its value is equal to 0.5 if all relative frequencies of the fractions xj (j = 1, 2, 3,…, N) are equal. It measures the distance of the mean log2 diameter and the smallest log2 diameter. Geometrically, the grading curves with the same A have the same sub-graph area. Since A is linear, the A = constant condition in addition means parallel hyperplanes in the N − 1-dimensional space generated by the simplex (Figure 2(a) and (b)).

Figure 2.

The constant A sections of the simplex and the optimal line (a) for a two-dimensional simplex and (b) for a three-dimensional simplex [16].

The entropy increment ΔS is the logarithm of the weighted generalized geometric mean of the relative frequencies of the fractions xj (j = 1, 2, 3,…, N):

ΔS=1ln2xi0xilnxi.E13

The entropy increment ΔS measures how much the soil behavior is really influenced by all of its N fractions. For those grading curves, in which all N fractions are well represented, the entropy increment is typically close to ln N/ln 2. The normalized entropy increment B is defined as follows:

B=ΔSlnNE14

Being a strictly concave function, the normalized entropy increment B has a unique maximum for each A = constant value, which is the following grading curve with finite fractal distribution (see the definition in [24]):

x1=1j=1Naj1=1a1aN,E15
xj=x1aj1E16

where parameter a is the root of the following equation:

y=j=1Naj1[j1A(N1)]=0.E17

As A varies between 0 and 1 (the extreme values represent the extreme fractions 1 and N), the positive root a varies between 0 and ∞ in the function of N. The optimal grading curve has finite fractal distribution with fractal dimension n given by:

a=2(3n)E18

The optimal grading curve is concave if A < 0.5, linear if A = 0.5, convex if A > 0.5 (see Figure 3). Having no inflexion points, the optimal grading curve has the shortest curve length out of the possible grading curves with a specified A. The optimal points of the simplex constitute a continuous line called optimal line which can be seen in Figure 2.

Figure 3.

Optimal grading curves with finite fractal distribution, (a) N = 7. A varies. (b) A = 2/3, N varies.

In the linear case, it has a unique maximum, being equal to 1/ln 2, in the center of the simplex where each relative frequencies xi are the same, in this case the “disorder” is maximal in the system. The disorder originated from mixing of the fractions can be measured by the entropy increment ΔS, which is the entropy of the fractions neglecting the fact that the width of the statistical cells in arithmetic scale is different

2.4. The entropy diagram

Four kinds of maps can be defined between the N − 1-dimensional simplex with fixed N, with fixed smallest fraction serial number imin and the two-dimensional space of the entropy coordinates: entropy map with coordinates [So, ΔS], the normalized entropy map with coordinates [A, B] and the two partly normalized entropy maps with a mixture of normalized and non-normalized coordinates, that is, [So, B] or [A, ΔS]. The optimal line of the simplex—between vertices 1 and N−

These maps are continuous on the closed simplex for fixed N. The image of the simplex—the entropy diagram—has a maximum and a minimum value for every possible value of A or So. The optimal line of the simplex maps into the maximum line, the map along the optimal line—maximum B line is one to one (see Figure 4(c) and (d)). The simplex edges and vertices map into the minimum line. The minimum and maximum diagram lines—illustrated in Figures 4 and 5—differ in scaling.

Figure 4.

The normalized entropy map and the inverse image for N = 3. (a) The two-dimensional simplex and its A = 0.5 hyperplane section. (b) The image of the simplex in the entropy diagram. (c) and (d) The inverse image of points A = 0.5, B = 1, 1.4 and Bmax = 1.44 in the simplex and in the space of the grading curves, respectively.

Figure 5.

Diagrams of simplexes with various N, the image of the optimal lines (“maximum lines”) and the image of the edges 1 – N, N = 2–7 (i.e., “minimum lines”). (a) The non-normalized diagram. (b) The normalized diagram.

In terms of the original entropy coordinates, the map is continuous if N is changing, and in terms of the normalized entropy coordinates, the map is not continuous if N is changing. The normalization with respect to a coordinate results in the range being fixed in that direction. The maximum B point is equal to l/ln 2 = 1.44 for any N, the maximum of the entropy increment ΔS is equal to ln N/ln 2.

The images of the optimal lines—the maximum B lines—will nearly coincide for any number of the fractions N (Figure 5(b)) in the normalized diagram but will separate in terms of the non-normalized coordinates [So, ΔS], reflecting the structure of the continuous sub-simplexes of a simplex. This is illustrated in Figures 1(b) and 5(a) for soils with up to seven fractions.

The inverse image of a regular normalized entropy diagram point [A,B] in the simplex is situated on the A = constant, N − 2-dimensional, affine hyperplane, with shape of an N − 3-dimensional “sphere,” centered to the optimal point, its “radius” depends on BmaxB. The related grading curves have the same sub-graph area and the deviation from the optimal grading curve depends on BmaxB.

3. The construction of the grading entropy-based rules

3.1. The methods

The particle migration (or internal stability) rule, the filter rule, and the segregation rule were constructed as follows. For each rule, simple soil testing programs were designed and executed by using artificial mixtures of natural sand grains [15]. Two variables were carefully constructed using the grading entropy concept [15] for each rule separately.

The entropy variables were used such that the experimental data were plotted on diagrams, differentiating points which exhibited different physical behavior so that domains of particular behaviors could be defined. In addition, some other information and existing data (e.g. the data base related to Ref. [7]) were used.

The additional information was as follows: one piece of information used was that there could be no more than two empty particle size fractions between the filter and the base soil, before the base soil cannot be retained by the filter [21]. This can be derived using Pure Geometry Theorems [21] and also by using the Terzaghi filter criterion (i.e., the finer is to be protected) as follows:

1Dd4E19

where D and d are the diameter of the filter and the base soil. Another piece of information was that the data of suffosion tests could be used for the filter rules, and vice versa, based on the following consideration which comes from the self-filtering theory of Kézdi [25, 26]. If the gap-graded grading curve (see eg. Figure 6) is cut into two parts, with the coarser part considered as the filter and the finer part as the base soil, and the base soil part being filtered, then there will be no suffosion within the soil.

Figure 6.

(a–h) Some grading curves of samples used by Lőrincz [15, 21] for suffosion tests. The inset shows the permeameter test arrangement used in the tests.

3.2. Particle migration rule

For the particle migration (internal stability-suffosion) rule, simple vertical flow tests were designed and executed using artificial mixtures of natural sand grains. The dimensions of the permeameter were 20 cm in height and 10 cm in diameter. It was closed at the bottom by a sieve which was permeable of grains smaller than 1.2 mm but which retained grains larger than 1.2 mm. The downward hydraulic gradient [i] was between four and five. The two parts of the permeameter were separated after the test, and the grading curves were determined. The grain movements were detected.

The results of the vertical water flow (suffosion) test were represented in the partly normalized entropy diagram, in terms of the relative base entropy and the entropy increment coordinates A and ΔS, as shown in Figure 7(a) and the rule was separately set up for each specified N value. The part of the diagram where the gap-graded grading curves resulted in self-suffosion was indicated by letter b. The simplified normalized diagram version is shown in Figure 7(b).

Figure 7.

(a) Particle migration zones in half of the partly normalized entropy diagram for mixtures with N = 6 fractions, the three digit numbers are related to the grading curves shown in Figure 6. (b) Particle migration zones in the simplified, normalized entropy diagram [21].

If A < 2/3 (zone I), the soil was internally unstable; if A = 2/3 and A < 2/3 (zones II, III), the soil was internally stable. In zone II, there were no particle movements: the larger particles retained the smaller particles and the smaller particles supported the larger ones. In zone III, the fines may have migrated in the presence of seepage flow (“suffosion”).

The internal stability zone III was separated by the 2/3 vertical line. The division curve between zones II and III connects the maximum entropy points of the mixtures with fraction number less than N, the shape of the curve between II and III is approximate in Figure 7(b).

The rule can be interpreted such that, in zone I (where A < 2/3), no structure of the larger grains is present, the coarse particles ?float? in the matrix of the fines and become destabilized when the fines are removed by piping. In the zone where A = 2/3 and A > 2/3 the coarse particles form a skeleton and total erosion cannot occur. In zone III, the structure of larger particles is inherently stable, the smaller particles may move by suffosion.

3.3. Filter rule

The filter rule was developed using three series of tests: the filter tests of Sherard [7], the filter tests of Lőrincz [15], and the suffosion tests of Lőrincz [15]. The grading of the soils tested by Sherard is shown in Figure 8 and the grading of the soils tested by Lőrincz is shown in Figures 6 and 9. In the filtering test, the filter and base soils are placed into the permeameter (20 cm in height and 10 cm in diameter) in series separated by a sieve. The downward hydraulic gradient [i] is between four and five. The suffosion tests of Lőrincz [15] were reanalyzed as follows. The gap-graded grading curves shown in Figure 6 were cut into two parts at the gap and one part was considered as the filter and the other part as the base soil. If suffosion occurred, then the filter was unsafe.

Figure 8.

(a) Filter test apparatus in [7, 21]; (b) and (c) Sherard-filter soils [7, 21]; (d) Sherard-base soils [7, 21].

Figure 9.

Some grading curves of soils used in the filter tests of Lőrincz [15, 21]. Note that the filters are identified by characters, and the base soils by numbers.

Two pseudo-metrics were constructed from the grading entropy parameters. The logarithm of the difference between base entropies of the filter and base soils, log(S0fS0b) described the distance between the mean log2 diameters of the filter and base soils. The sum of filter and base soil entropy increments ΔSf + ΔSb expressed the sum of the two “effective” fraction number or N values (i.e., the total number of important fractions in the two grading curves).

Plotting the test results in terms of the foregoing variables, the safe and unsafe areas were separated by a straight line: a layer acts as a filter for an adjacent layer (for the base soil) on the condition that:

ΔSf+ΔSb4ln(S0fS0b)4.39E20

where index f and b denote the filtering layer and the material being filtered (base soil), respectively. The domains defined by the Eq. (20) are shown in Figure 10. The point where ΔSf + ΔSb = 0 was defined on the basis of the assumption that in the limit state two empty size fractions do exist between the filtering fraction and the filtered fraction.

Figure 10.

The filter rule with the safe and unsafe areas. The soils are shown in Figures 8 and 9 [15, 21].

3.4. Segregation rule

For the segregation rule, the simple emax test was used in a modified form. In the emax tests, the soil is poured into a funnel and flow is allowed from the funnel into a cylinder (10 cm in height and 10 cm in diameter). The segregation test was made with about double the quantity that expectedly filled the 10 cm diameter, 10 cm high cylinder. The funnel is just rising above the soil surface.

The artificial mixtures of natural sand grains used for the segregation rule were partly continuous mixtures (A, B), partly gap-graded mixtures (C, D, E), as shown in Ref. [21]. The results are shown in Figure 11. The difference in the initial and the poured base entropy S0, entropy increment ΔS, and grading entropy S was represented in the function of the relative base entropy A. According to the results, some segregation was always measured, but it was with minor significance if the relative base entropy of the soil was within the following limits:

Figure 11.

Results of the segregation test, mixtures A–E are shown in [21].

0.4A0.7E21

The results showed that the base entropy difference S0 was negative and the entropy increment difference ΔS was positive above the lower limit A = 0.4. Physically, the proportion of the large grains and the mean log2 diameter is larger if the base entropy difference S0 is larger and vice versa. The value of ΔS is larger if the mixture is more uniform in terms of fraction relative frequencies.

3.5. Applications

3.5.1. Non-segregating mixtures

Minimal segregation occurs, and relatively uniformly textured body of soil is achieved for laboratory testing of granular materials or for the earth works, if a non-segregating mixture with 0.4 < A < 0.7 is used.

To construct continuous, non-segregating mixtures, some optimal limit curves can be determined. The optimal mixtures computed by a simple algorithm fulfilling Eqs. (15)–(17) for fixed N = 5 (where B is a maximum for a given A are for five fractions) are shown in Figure 12 and Table 2. Similar limit curves can be reproduced for any fraction number.

Figure 12.

Limit curves for non-segregating optimal 5-fraction mixtures [21].

A [–]a [–]x1 [–]ΔS/ln N [–]
0.501.000.201.44
0.561.130.151.43
0.601.230.131.41
2/31.420.091.34
0.701.540.071.29

Table 2.

Some non-segregating optimal 5-fraction mixtures.

However, it can be noted that soils with gap-graded grading curves can be non-segregating also. For example, in case of a two-fraction soil with gap-graded grading curve, the segregation is minimal if the quantity of the larger fraction varies between 0.4 and 0.7.

3.5.2. Testing the filter rules

The grading entropy-based filter law was compared with the existing filtering rules available in the literature. Summaries of well-known filter rules [7, 915] for uniformly graded filters and broadly graded filters are presented in Appendix A. These different filtering rules were tested by generating soils with the special-shaped grading curves [21] shown in Figure 13 and parameterized in Table 3.

Figure 13.

The theoretical grading curves used in the testing of existing filtering laws. (a) Mixtures for the Terzaghi’s criterion-T. (b) US Bureau simple filters-U. (c) US Bureau mixed filters-UM. (d) Mixtures for Bertram’s criterion-B.

D50/d50D15/d85D10/d60D15/d15S0bS0fΔSbΔSf
1B1-1I74.586.57.86131600
2B1-1II145.6722.59.71131701.585
3T1-1I10.004.174.447.141316.3501.44
4T1-1II42.423.14.14131500
5T1-1III6.894.173.17.141315.8500.61
6T1-1Iv11.115.176.38.861316.501
7UM1-1I13.97.30.8121316.800.722
8UM1-1II587.30.8121318.5102.07
9UM1-1III5825.52.6401319.01.585
10U1-1I5.553.023.134.571315.501
11U1-1II7.785.195.427.86131600
12U1-1III11.15.856.258.861316.501
13U1-1Iv15.510.1910.6315.43131700

Table 3.

The data of the theoretical grading curves used in evaluating the filtration rules, generated for this purpose [15] to four existing filter rules, as shown in Figure 13.

The 13 combinations listed in Table 3 were represented for the different filtering rules of the literature, some results are shown in Figure 14. If the rule from the literature predicted a successful filtering (i.e., safe behavior), it was plotted with an open circle; where it predicted a failure to filter (i.e., unsafe behavior), it was plotted with a full circle.

Figure 14.

Testing some filtering rules, using the theoretical grading curves of Figure 13 and Table 3. (a) The filter rule of USBR for uniform filters [12] is acceptable. (b) The filter rule of Terzaghi [11] is conservative.

The results indicated that (i) the Terzaghi?s filter rule is too conservative, (ii) the Bertram rule is conservative for mixed filters and not acceptable for uniform soils, (iii) the rule of United States Bureau of Reclamation (USBR) for uniform filters is acceptable, and (iv) for mixed filters is not acceptable.

4. Case study

Several applications of the entropy-based rules, by examining the reason of piping, softening, dispersive soil behavior, and the goodness of a leachate collection system, were previously presented [1922]. Here, a dam failure case study is summarized.

The 71 m high, Gouhou rockfill dam was founded on a sandy gravel base layer (Figure 15). The dam body consisted of the following parts: the upstream face was a thin layer of material with a design particle diameter of 100 mm, zone I was a transition zone with the maximum diameter of 400 mm, zones II and III were the main rockfill with maximum diameters d of 600 and 800 mm.

Figure 15.

The Gouhou dam failure. Cross section and failure mechanism.

The dam failed [22, 27, 28], killing 288 people, immediately after the first rising water level, and infiltrating the water into the dam body causing internal erosion, piping, and washout of material (see 1–6, Figure 15).

The relative base entropies of the soils in zones I, II, and III were 0.42, 0.55, 0.58, respectively, all less than 2/3 and non-segregating. This result explains why the rockfill material was incapable of forming a stable skeleton of coarse fragments. It follows that the grading entropy-based soil behavior rules would have been capable of predicting piping failure in the Gouhou dam.

5. Discussion and conclusion

5.1. Some comments on the entropy parameters

The grading entropy parameters are some kind of integrals of the whole grading curve. The same shaped grading curve has the same A, ΔS, or B value independent of the value of the minimum grain size. Therefore, these are well-defined parameters and have some physical contents, as follows.

The relative base entropy parameter A has a potential to be a grain structure stability measure possibly based on the simple physical fact that if enough large grains are present in a mixture, then these will form a skeleton.

The entropy increment ΔS measures how much the soil behavior is really influenced by all of its N fractions. For those grading curves, in which all N fractions are well represented, the entropy increment is typically close to ln N/ln 2.

The entropy parameters are pseudo-metrics. The difference between base entropies of the filter and base soils, S0fS0b describes the distance between the mean diameters. The sum of filter and base soil entropy increments ΔSf + ΔSb expresses the sum of the two “effective” N values (i.e., the total number of important fractions in the two grading curves).

5.2. Some comments on the rules

The overall soil stability—according to the experimental results—is described by the criterion that A > 2/3. In soils which meet this criterion, the matrix of coarser soil particles is stable and able to form a resistant skeleton, even though suffosion may occur.

Some questions arise, for example, in regard to the stability of a single fraction which does not lie in a unique position on the entropy diagram. Since the change due to degradation is the appearance of smalls, which causes an increase in the A value [29], the one fraction case is likely on the safe side.

Another question is related to the probability that an arbitrary N-fraction soil is stable. This can be characterized by the relative size of the grading curve space separated with the A = 2/3 hyperplane on condition that the probability is the same in the whole simplex. This number is decreasing with the fraction number (e.g., for N = 2, the 1/3 part of the grading curve space is safe, for N = 3, the 2/9 part of the possible grading curves are safe, for N =18, less than the 0.01 part of the possible grading curves are safe).

Significant segregation is unlikely to occur, if the relative base entropy A is between the limits of 0.4 and 0.7. It is important to note that the same parameter—the relative base entropy A—is responsible for overall soil stability. Soils which meet both criteria may constitute very small part of the grading curve space and may need careful design in case of broadly graded soils.

The filtration problems are safely solved in the literature for uniform filters and bases (i.e., soils to be protected by the filters). The suggested filter rule can be used to design broadly graded filters (e.g., for clay cores or for leachate collection systems). However, the rule was estimated on the basis of one data point only at the range of very large N and ?S values.

The testing of the existing rules known from the literature was possible on the basis of the suggested filter rule and using some theoretical grading curves. According to the results, the Terzaghi filter rule is too conservative. The filtering rule of USBR for uniform filters is acceptable. The mixed filter rule of the USBR is not conservative and is not acceptable. The Bertram rule is be conservative for mixed filters and not acceptable for uniform soil.

5.3. The importance, use, and implementation of the rules

Applications of the derived entropy-based rules were presented by examining the reason of a dam piping failure, dike piping, dispersive soils, leachate collection system case studies [1922], a dam example is presented here only. On the basis of the case study, it is apparent that the grading entropy-based soil behavior rules would have been capable of predicting piping failure in the Gouhou dam.

The grading entropy-based criteria can easily be implemented into any laboratory test evaluation software. A basic requirement for the use is that the grading curve information is reliable. The simple soil tests presented here were made on coarse material and the rules apply for soils where the solid fraction is composed of non-clay minerals.

For clay minerals, the same criteria may be valid if the grading curve information is reliable and the appropriate degree of particle agglomeration is reflected in the measurements [3033]. The first results indicate that the same criteria may be valid for silty soils if the grading curve information is reliable (see e.g., the dispersive soil case studies [20]).

Acknowledgments

The chapter is related to the work of the Research Project OTKA 1457/86 on river dykes and of the Research Project NKFP B1 2006 08 on MSW landfills.

Rules for uniform filters

U.S. Bureau of Reclamation [12]:

D50d50=510E22

Sichard [9]:

D50d50=34.5E23

Sherard et al. [7]:

D15d85<9E24

where D and d denote the filter and the base soil, respectively.

Rules for broadly graded soils

Terzaghi’s [10, 11]:

D15d854,D15d154E25

US Bureau of Reclamation [12]:

D50d50=1258,D15d15=124E26

Bertram [13]:

D15d855,D15d15=59E27

Cistin [14]:

D10d60<5,UD=D60D10<5E28

where D and d are diameters of the filter soil and the base soil.

© 2017 The Author(s). Licensee IntechOpen. This chapter is distributed under the terms of the Creative Commons Attribution 3.0 License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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János Lőrincz, Emöke Maria Imre and Vijay Pal Singh (September 6th 2017). The Grading Entropy-Based Criteria for Structural Stability of Granular Materials and Filters, Granular Materials, Michael Sakellariou, IntechOpen, DOI: 10.5772/intechopen.69167. Available from:

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