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![]() Advances in Ma terials Physics and Che mist ry, 2012, 2, 102-105 doi:10.4236/ampc.2012.24B028 Published Online December 2012 (htt p://www.SciRP.org/journal/ampc) Copyright © 2012 SciRes. AMPC Influence of Humidity on Yiel d Stress Determi nation by Sl um p Test of Sl i p-P rone Clayey Soils and Their Relation with the Chemical Properties Arturo F. Méndez-Sánchez, Ana M. Paniag ua-Mercado1, Karen E. Nieto-Zepe da, Leonor Pérez-Trejo, Elvia Diaz Valdés, Concepción Mejía García Escuela Superior de Física y Matemáticas, Instituto Politécnico Nacional, Edif. Unidad Profesional Adolfo López Mateos, Col. Lindavista, México Email: ampani@esfm.ipn.mx Received 2012 ABSTRACT In this work, the yield stress evaluation as a function of water content for slip-prone clayey soils is studied in order to understand how yield st ress decreases as water conten t increases, an d their relatio n with the chemical pro perties. The clayey soil samples were t aken from the region of Teziutlán-Puebla-Mexico. Yield stress was calculated using the slump test in cylindrical geometry. Results show three zo nes . The first on e sho ws an exp o nen tial d ecrement o n yield stres s du e to lower water content in accord with clayey soils with high content of illita, foll owed by a second region where yield st ress decreases d ramaticall y at a cer tain crit ical water concen tration, and the third one where yield stress dependence is not well-defined since the clayey soil flow is seen. Finally, it is discussed how yield st r es s var iation due to the water incr ement in fluences the landslide risk in crement. Keywords: Clayey Soil; Yield Stress; Slump Test; Microstructure; Illita 1. Introduction There are a few studies focused to analyze the modified physi- cal parameters before a landslide occurrence [1-3]. Reference [1] implemented a debris-flow monitoring system employing real-time rain gauge data. The pre-warning for the time of landslide triggering derives from the critical rainfall peak ob- tained from historical events, involving regional rainfall pat- terns and geological conditions. Reference [2] proposed equa- tions of state of soil prone to slum-type settlement, which take into account the degree of wetting in the initial stage. These equations were developed using models of deformation of the continuous and experimental results of cohesion and the angu- lar coefficient of internal friction as well as the bulk compres- sion and shear modulus. Those authors proposed a plasticity function that decreases exponentially when the wetting content in the soil is increased. It is clear that plasticity function is one of the most important modified parameters before o f a land slid e occurr ence by rainfall . Hence, l andsl ides can take place b ecause of load excess generated by a water saturated soil overcoming yield stress [ 4-6], as well as, infiltrated water excess in the soil (decrement of the pore pressure) produces a yield stress decre- ment and the internal load overcomes the decremented yield stress. In this work, the yield stress evaluation as a function of water content for slip-prone clayey soils due rainfall is studied in order to understand how yield stress is decremented by the water content. Yield stress was calculated for several water concentrations using the slump test in cylindrical geometry. Particularly, samples of the region of Teziutlán-Puebla-Mexico were tested and the results were analyzed and compared with the historical daily rain data of October 1999, when a landslide occurred in the zone. In addition, a comparison of the chemical microstructure and the compound determination using Energy Dispersive Spectroscopy by X-ray dispersion was performed. As well, clayey soils were characterized by SEM observation and X-ray diffraction . 2. Exp erimenta l Pro cedu r e The studied clay corresponds to high risk zone located in the Aurora neighborhood in Teziutlán-Pu e bla-Mexico, where a landslide took place due to high rainfall in October 1999 [7]. The zone where the sample was taken corresponds to a transi- tion zone of two physiographic units-the transversal volcanic belt and oriental mountain chain. Andosol is the predominant soil d erived from volcan ic materials; als o, there are ign imbrites and cl ayey soils. Th is kind o f soil is charact erized b y a variable high capacity of acquiring water and humidi ty. Micro anal yses of chemic al co mpo sit ion were performed with an energy dispersive spectroscopy technique (EDS) attach ed to a scanning electron microscope FEI, Sirion. In addition, X-ray diffraction exp eri ments were c arri ed o ut emplo yin g a MM A, GBC diffractometer in order to determine the clayey compounds, by using CoKα radiation (λ = 1.789Å) in the 2θ range of 5-120 degrees with a 0.02 step and 0.5s as step width and step count- ing time resp ectively. The samples were sifted with a standard mesh No. 8 (2.36 mm) mesh in order to eliminate larger debris. Samples of 0.3 kg of clay were p rep ared at 3 0-40 wt% of water concentration, and slump test experiments were carried out [8]. The method con- sists of filling a cylindrical frustum with the material to be tested in the specified way; lifting the frustum off and allowing the material to collapse under its own weight (Figure 1). The ![]() A. F. MÉNDEZ-SÁNCHEZ ET AL. Copyright © 2012 SciRes. AMPC 103 height of the final slumped material is measured and the differ- ence between the initial and final heights is called the slump height (s). Figure 1 outlines the experimental procedure. Yield stress value ( τy) was calculated by the equation of Pa- shias and coworkers, expression 1. 11 . 22 y s gH H τρ = − (1) where ρ is the material density, g is the gravity, s is the slump height, and H is the frustum height. In this case, the slump height was measured at room temperature, after 40 seconds lifting the frustum off, as was suggested in a previous work [9,10]. 3. Results and Discussion Figure 2 shows SEM micrographs of clayey soil. It can be Figure 1. Slump test diagram, a) frustum filling, b) frustum lifting, c) collapsed materia l, and d) slump height measurement. (a) (b) Fi gur e 2. SEM images at a) 500x and b) 1000x, granular shape with fiber con f ormation. observed a granular shape with a fibrous surface of individual particles. Table 1 shows the chemical composition determined by EDS analysis. High contents of aluminum and silicon were detected as expected for this type of material. Besides, a low cont ent of Iron and Titanium was observed in this material. Figure 3 shows the particle size distribution. It can be seen that 60% of the p articl e sizes are i n the ran ge between 3 0 0 and 1250 microns, the 10% are in the interval 1250- 2360 microns, and the rest 30% of the particle size is shorter than 200 microns. The X -ray diffraction analysis of clayey soil shows the pres- ence of compounds, such as illite (39.79%), gibbsite (33.74%) and cristobalite (26.47%). The peak identification is shown in Figure 4 and the Percentage of mineralogical phases is shown in Tabl e 2. Figure 5 shows the plot of yield stress, τy, versu s water con- centration expressed in weight percentage. In the case of con- tents lower than 35.5 wt%, the yield stress decreases exponen- tially with concentration. The regression equation is also shown. These results are in agreement with Sultanov and Khusanov’s model [2], as well as with that reported by Sánchez-Crúz [9]. Tabl e 1. Chemical compo si t ion o f c l ayey soil. Element Wt% Int. Error O 49.09 0.55 Al 18.17 0.59 Si 23.1 0.55 Ti 1.42 3.3 7 Fe 8.23 1.46 Total 100 20 40 60 80 100 0.1 1 0 5 10 15 20 25 30 35 Finus Particle size distribution Gauss fit Frequency (%) Particle size (mm) Cum ulative frequency Cum ulative frequency Sigmoidal fit Figure 3. Particle size distrib u t ion of th e clayey soil . Tabl e 2. Percentage of mineralogical phases. Element Percenta ge % SiO2 39.79 KAl2(SiAlO10)(OH)2 33.74 Al2O3H2O 26.47 Total 100.00 ![]() A. F. MÉNDEZ-SÁNCHEZ ET AL. Copyright © 2012 SciRes. AMPC 104 020 40 60 80100120 0 100 200 300 400 500 600 700 3 3 1 3 1 1 3 3 (2) 2 11 11 1 3 2 1 22 2 Counts Degrees 2-Theta 1) SiO 2 2) K Al 2 (Si 3 Al O 10 )(OH) 2 3) Al 2 O 3 ! 3 3H 2 O Figure 4. X-ray diffraction pattern of the clayey soil. 30 32 34 36 38 40 0 50 100 150 200 250 300 350 21.0 21.5 22.0 22.5 23.0 23.5 24.0 24.5 25.0 Y ield stress (Pa) Water concentration (%) Y ield stress measurements τ y =170.7157e -.08397 *C R a in fall milimet e rs ( m m) Figure 5. Y i eld st ress ve rsu s w at er p erc en t a ge con cen t r at i on . These authors studied a clayey soil with the presence of illite, which showed a similar behavior. In the case of contents be- tween 35.5 wt% and 36 wt%, the yield stress shows an abnor- mal behavi or and it decreases substan tially, up to 50 percent of its initial value. At this point, it is possible to elucidate an in- crement in the landslide risk, since the sample has changed from solid-plastic to solid-viscous behavior. It is important to mention that this decrease in yield stress was not predicted by the Sultanov and Khusanov’s model, in spite of having in- cluded the plastic and the viscous behavior in their model. For higher water concentrations (>36 wt %), a non-linear d ecr ement on yield stress is seen and it differs from the exponential or power-law behavior. We believe that this response is due to a combination of non-Newtonian behavior and yield stress and this is not possible to separate them in the slump test. Additionally, upper horizontal axis in Figure 5 shows the variation of yield stress versus equivalent millimeters of rainfall. In this case, it was supposed that all of the water was absorbed by the clayey soil. Millimeters of rainfall (h) were calculated b y using the expression 2. . w V hA = (2) where VW is the water volume in the frustum, and A is the fr us- tum c r oss section . Under this assumption, it can be seen that only 23 mm of water are enough for the soil to start to flow. However, this value is lower in comparison with the historical rainfall data obtained in the studied geographical zone [7], where the maxi- mum rainfall peak was reached (360 mm of water) the day before the landslide and considering that in the previous ten days, an unusual accumulated rainfall reached 908 mm (com- pared with the medium annual rain 1593 mm). This difference arises from the small quantity of the rainfall absorbed by the soil ( natur e’s soil ) and by the f act th at most o f the water moves down due to the region´s inclination (23 degrees). In order to clarify this, it would be necessary to carry out the yield stress determination immediately after the occurrence of a landslide and measure the absorbed rainfall water. 4. Conclusions Yield stress determination as function of water content by a slump test for a clayey soil from a Teziutlán-Puebl a -Mexico zone was performed. The results showed an exponential decrement of yield stress followed by an abrupt reduction of it with the increase in water concentration. From this value, an increment of the risk of landslide was revealed. At high water content (36%), a decrease in yield stress was observed, and a more complex behavior was exhibited. Finally, a correlation of yield stress with rainfall was done, but results were below the values reported in the literatur e. 5. Acknowledgements The authors thank to Professor V. M. López-Hirata by his use- ful commen ts. REFERENCES [1] C . Ch ien -Yuan, C . Ti en -Chen, C. Y. Fan-Chieh, Y. Wen-Hui, T. Chun-Chieh, “Rainfall duration and debris-flow initiated studies for real-time monitoring,” Environment Geology, vol. 47, p.p. 715–724, 2005. [2] K. S. Sultanov, B. E. Khusanov, “Stat e equation s for soils p rone to slump-type settlement with allowance for degree of wetting,” Soil Mec hanics and Foundation s Engineering, vol. 38, No. 3, p.p. 80-86, 2001. [3] I.A. Caldiño-Villagómez, I. Bonola-Alonso, G. Salgado-Maldonado, “Estudio experimental del esfuerzo de cedencia con relación al flujo de lodos y debris,” Asociación Internacional de Ingeniería e Investigaciones Hidro-Ambientales vol. 8, [Memorias del XXII Congreso Latinoamericano de Hidráu lica, Guayana, Ven ezuela]. [4] D. F. Van Dine, R. F. Rodman, P. Jordan , J. Dupas, “Kusk onook Creek, an example of a debris flow analysis,” Lanslides vol. 2, p.p. 2 57-265, 200 5. [5] R. M. Iverson, “The physics of debris flows,” Reviews of Geo- physi cs, vol. 35, No. 3, p.p. 245–296, 1997. [6] R . P .Den linger, R . M. Iverson, “Flow of variably fluidized gra- ![]() A. F. MÉNDEZ-SÁNCHEZ ET AL. Copyright © 2012 SciRes. AMPC 105 nular masses across three-dimensional terrain 2. Numerical predictions and experimental tests,” Journal of Geophysical Researc h, vol. 106, No. b1 , p. p. 553–566, 200 1. [7] P. Flores Lorenzo, I. Alcántara Ayala, “Cartografía morfogenética e identificación de procesos de ladera en Teziutlán, Puebla,” Investigaciones geográficas Boletín, vol. 49, p.p. 7-26, 2002. [8] N. Pashias, J. Boger, D.V. Summers, D. J. Glenister, “A fifty cent rheometer for yield stress measuremen t,” Jou rnal of Rheol- ogy, vol. 4 0, No. 6, p.p. 1179-1189, 1996. [9] P. Sánchez Crúz, “Análisis del esfuerzo de cedencia de suelos arcillosos como posible indicador de un derrumbe,” Bachelor Thesis, ESFM, Instituto Politécnico Nacional, Mexico, 2008. [10] A. F. M én d ez-Sánchez, L. P ére z-Trejo, A. M. Paniagua Mercado, “Dete rmi na ción del esfu erzo de c eden cia para s uelos vuln erab les a deslizamientos originados por lluvias,” Boletín de la Sociedad Geológica Mexicana, vol. 63,No 2, p.p. 345-352, 2011. |