EFFECT OF COMPACTION ON THE UNSATURATED SHEAR STRENGTH OF A COMPACTED TILL

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EFFECT OF COMPACTION ON THE UNSATURATED SHEAR STRENGTH OF A COMPACTED TILL Vanapalli, S.K., Pufahl, D.E., and Fredlund, D.G. (University of Saskatchewan, Saskatoon, SK., Canada, S7N 5A9) Abstract An experimental program was undertaken on compacted clay till at three different initial water contents to study the unsaturated shear strength under drained and undrained loading conditions. The three different initial moulding water contents (dry of optimum, optimum, and wet of optimum) induced differing soil structures to the compacted soil. The research study presented in this paper shows that the variation in suction in a soil that arises due to the influence of soil structure is a function of the initial compaction water content. The influence of soil structure on the drained and undrained shear strength parameters in unsaturated conditions is reflected through the shear strength contribution due to suction. Introduction Compacted fine-grained soils are commonly used in the construction of geotechnical and geo-environmental structures. Both drained and undrained shear strength analyses of compacted soils are of significance in dealing with these structures. The shear strength behavior of compacted soils in an unsaturated condition is significantly influenced by properties such as the initial moulding water content, stress state and soil structure. For example, a fine-grained soil compacted at various initial water contents and to various densities produce different soils from a soil mechanics behavioral standpoint even though their mineralogy, plasticity, and texture are the same. The engineering behavior will vary from one specimen to other due to differences in soil structure or aggregation which are related to the initial moulding water content. Limited information is available in the literature with respect to the influence of soil structure on the shear strength behavior of unsaturated soils in drained and undrained loading. An experimental program was undertaken on a compacted clay till to study the shear strength in drained and undrained loading. The initial water contents were chosen to represent dry of optimum, optimum, and wet of optimum conditions. The influence of soil structure on the drained and undrained shear strength parameters in unsaturated conditions and the contribution of shear strength due to suction is presented in this paper. Testing Program The clay till used for the study has the following properties: liquid limit, w L, equal to 35.5% and plastic limit, w P, equal to 16.8%. The percentages of sand, silt, and clay are 28, 42, and 3 respectively. The specific gravity of soil is 2.73. The soil is classified as a CL. The AASHTO standard compacted density is 1.8 Mg/m 3 with an optimum water content of 16.3%. Three initial water contents were selected for preparing the soil specimens representing dry of optimum (initial water content of 13% and γ d of 1.73 Mg/m 3 ), optimum (initial water content of 16.3% and γ d of 1.8 Mg/m 3 ), and wet of optimum (initial water content of 19.2% and γ d of 1.77 Mg/m 3 ). Statically compacted specimens were used for the study. The effective saturated shear strength parameters were determined using conventional direct shear equipment in single stage, multistage and residual shear tests. The unsaturated shear strength was determined in multistage testing using modified direct shear equipment designed by Gan and Fredlund (1988). The drained unsaturated shear strength behavior was determined under three net normal stresses: 25, 1, and 2 kpa for a suction range of to 5 kpa. Soil-water characteristics were determined using a pressure plate apparatus for the suction range of to 1,5 kpa. To attain the suction versus degree of saturation relationship beyond 1,5 kpa (i.e., 4,5 to 3, kpa), osmotic desiccators were used. The undrained shear strength characteristics were studied using conventional undrained triaxial tests both in unconfined and confined loading conditions. The details of sample preparation and testing procedures are available in Vanapalli (1994). Saturated Shear Strength Results

A narrow range of effective cohesion values were determined from the testing. This variation can be attributed to differences in strain rate, different direct shear equipment, type of testing procedures, and the possible variation in soil properties (Vanapalli 1994). The values of c' tended to zero with decreasing strain rates. The effective angle of shearing resistance, φ', is 23 o for all three different initial water contents and densities. Shear Strength of Unsaturated Soil in Drained Loading Conditions The shear strength mobilization with horizontal displacement in the modified direct shear tests for specimens tested with a net normal stress of 25 kpa at a suction value of 35 kpa is shown in Fig. 1. The strength increase is related to the initial water contents. A more comprehensive analysis with respect to shear strength is offered using the entire shear strength envelope shown in Fig. 2. Shear Stress (kpa) 15 12 9 6 3 and suction = 35 kpa.5 1 1.5 2 Displacement (mm) Dry of Wet of Fig. 1. Shear stress versus horizontal displacement relationship ( ) Shear Strength (kpa) 15 125 1 75 5 25 Wet of optimum Dry of optimum 1 2 3 4 5 Suction (kpa) Fig. 2. Shear strength versus suction for three initial water contents The variation of shear strength with respect to suction for the unsaturated soil specimens tested with three different initial water contents subjected to a net normal stress of 25 kpa is shown in Fig. 2. At any particular value of suction, the dry of optimum specimens have the lowest shear strengths. Specimens tested wet of optimum have the highest shear strength and the specimens tested at optimum water content lie in between that of dry and wet of optimum. Similar trends were observed for specimens tested with a net normal stress of 1 and 2 kpa for the three different initial water contents. The shear strength behavior under drained loading conditions can be explained using the soil-water characteristics. Figure 3 shows the soil-water characteristics with a net normal stress of 25 kpa for the three different initial water

contents. The macro pore structure present in the specimens dry of optimum facilitates easier drainage of water (i.e., desaturation) under an applied suction. In contrast to the dry of optimum specimens, the pore channels in the wet of optimum specimens are generally disconnected and offer greater resistance to water flow. The soil in this latter condition is more impervious since the micro structure dominates and provides resistance to the desaturation process. At any given value of suction, the specimens compacted wet of optimum have the highest degree of saturation while the specimens compacted dry of optimum have the lowest. In other words, the specimens tested at wet of optimum have more wetted interaggregate contact area in comparison to specimens that are dry of optimum. Suction as a stress state variable, transmits shearing stresses more effectively in specimens with greater water contents or higher degrees of saturation. Thus, the unsaturated shear strength in drained loading conditions is always higher in specimens at any given suction value in a specimen that has a higher degree of saturation or water content. The saturated shear strength as characterized by the shear strength parameters c' and φ' for all the specimens tested with three different initial water contents are the same. However, the shear strength in unsaturated conditions is different in each of the specimens due to the imparted soil structure (Fig. 1 and 2). The contribution of shear strength in unsaturated conditions due to the influence of soil structure is dependent on the value of φ b, which is the frictional angle associated with suction. Figure 4 shows the variation of φ b versus suction for specimens tested with different initial water contents with a net normal stress of 25 kpa. Similar trends were observed for specimens tested with net normal stresses of 1 kpa and 2 kpa with the three different initial water contents. 1 Degree of Saturation, S (%) 8 6 4 2, e =.514 Dry of optimum Initial void ratio, e =.59 Pressure plate tests Wet of optimum e =.54 Desiccator tests 1 1 1 1 1 1 1 Suction, (kpa) Fig. 3. Soil-water charatersistics for specimens compacted at three different initial water contents 25 Frictional Angle, φ b (deg) 2 15 1 5 Dry of optimum Wet of optimum 1 1 1 1 Suction (kpa) Fig. 4. Frictional angle, φ b, versus suction for 25 kpa net normal stress for specimens with different initial water contents

Shear Strength of Unsaturated Soil in Undrained Loading Conditions Figure 5 shows the confined compression test results of specimens with the three different initial water contents. The initial matric suction values of the dry of optimum, optimum, and wet of specimens were 368, 152, and 68 kpa, respectively. Figure 6 shows the variation of shear strength with the applied confining pressure for triaxial specimens tested with known initial suction values in confined and unconfined loading. Deviator Stress (kpa) 3 2 1 Dry of Initial void ratio, e =.58 Initial matric suction = 368 kpa Wet of e =.545 68 kpa 5 1 15 2 25 Strain (%) e =.52 152 kpa Confining Pressure = 2 kpa Fig. 5. Stress versus strain relationships of confined compression tests 6 Shear Strength (kpa) 5 4 3 2 1 Dry of optimum (water content = 13%) (w = 16.3%) Wet of optimum (w = 19.2%) 2 4 6 8 Confining Pressure (kpa) Fig. 6. Variation of shear strength with confining pressure The trend of results in Fig. 5 and 6 are opposite to that of drained test results shown in Fig. 1 and 2. The specimens tested with lower water contents had lower strengths in drained loading while the strengths were higher in undrained loading conditions. Such contradiction in behavior requires some discussion. In the research study as described in this paper, the densities and initial water contents are the same both in drained and undrained loading. A comparison of the contribution to strength due to suction both in drained and undrained loading is required to understand the influence of soil structure on the shear strength. Before the comparisons are undertaken the procedure for predicting the nonlinear variation of shear strength contribution due to suction is briefly detailed for one series of undrained test results obtained from specimens prepared at optimum initial water content and tested in confined and unconfined loading conditions. For this series of tests a horizontal failure envelope was obtained beyond a confining pressure of 4 kpa (Fig. 6). It can be inferred that the specimens were saturated and may have a suction value close to zero for the specimens tested with confining pressures higher than 4 kpa. The measured and predicted degrees of saturation using the theory of undrained pore pressure parameters for confining pressures higher than 4 kpa were close to 1% (Vanapalli 1994). The degree of saturation versus suction variation (i.e., the wetting soil-water characteristic curve) can be obtained from the undrained triaxial test results. The change in degree of saturation and suction in the undrained triaxial specimens due to the applied confining pressures can be computed from knowledge of the initial conditions of the soil using a

marching forward technique. This procedure is detailed in Fredlund and Rahardjo (1993). This technique is not required if the suction and degree of saturation are measured at failure conditions. The soil-water characteristic generated from the undrained tests along with the saturated shear strength parameters was used for predicting the shear strength of unsaturated soils under undrained loading conditions using either Eq. 1 or Eq. 2. These equations are described in the following section of this paper. There is a good correlation between the predicted and measured variation of shear strength with suction for the specimens compacted at optimum initial water contents. More details of the procedure and the test results are available in Vanapalli and Fredlund (1997). Figure 7 shows the variation of φ b versus suction for these test results. Frictional Angle, φ b, (deg) 25 2 15 1 5 5 1 15 2 Suction (kpa) Fig. 7. Variation of frictional angle, φ b, from undrained triaxial shear tests Comparison of shear strength contributions due to suction in drained and undrained loading conditions The shear strength of an unsaturated soil can be predicted using one of the following equations: [ c κ ( ua ) ] ( ua uw ) S ( τ = ' + σ tan φ' + tan φ' ) ( S τ = [ c+ ( σ u a ) φ ] + ( u a u Sr ) ' tan ' w ) ( tan φ' ) (2) ( 1 S r ) where: κ = fitting parameter S r = residual state of saturation The first part of each equation represents the saturated shear strength, when the pore-air pressure, u a, is equal to the pore-water pressure, u w. The second part of each equation is the shear strength contribution due to the soil suction. The information that is needed for predicting the unsaturated shear strength from [1] or [2] is the soil-water characteristic and the saturated shear strength parameters. The fitting parameter, κ, is required to obtain a correlation between the predicted and measured shear strength. The residual state of saturation, S r, can be estimated from the soil-water characteristic data using a graphical procedure. More details of these equations and procedures are available in Vanapalli et al. (1996) and Fredlund et al. (1996). The unsaturated shear strength of several soils including the clay till used in this study has been successfully predicted using these equations. The resulting structure or aggregation in a specimen is a function of initial water content and has a considerable influence on the nature of the interphase contact area (i.e., wetted area of contact) that develops in an unsaturated soil. The unsaturated shear strength both in drained and undrained loading is directly dependent on the interphase contact area that is available to transmit the suction as a stress state variable. The variation of this interphase contact area with respect to suction can be interpreted using the soil-water characteristic curve. The normalized wetted area of contact is represented as a dimensionless number, S κ, from [1] or {(S-S r )/(1-S r )} from [2]. The relationship for tan φ b / tan φ' versus {(S-S r )/(1-S r )} for specimens tested both in drained and undrained loading conditions is shown in Fig. 8. In spite of different soil structures resulting from different initial water contents and stress states there is a unique relationship between these two variables within the limitations of experimental errors. It seems apparent that the influence of soil structure is directly reflected in the suction values of compacted soils. A similar unique relationship will be obtained for tan φ b / tan φ' versus S κ relationship as {(S-S r )/(1-S r )} is equal to S κ. These unique relationships between tan φ b / tan φ' versus {(S-S r )/(1-S r )} or tan φ b / tan φ' versus S κ are useful for further simplifying the interpretations of shear strength of unsaturated soils. (1)

tan φ b / tan φ' 1.8.6.4 Dry of, Net Normal Stress = 25 kpa, 25 kpa Wet of, 25 kpa Dry of, 2 kpa, 2 kpa Wet of, 2 kpa, Undrained Test Results.2.2.4.6.8 1 (S-S r )/(1-S r ) Fig. 8. Variation of tan φ b / tan φ b versus (S-S r )/(1-S r ) relationship for drained and undrained shear test results for the clay till Summary and Conclusions The influence of soil structure on the drained and undrained shear strength characteristics of statically compacted clay till with three different initial water contents representing dry of optimum, optimum, and optimum water contents have been presented and discussed in this paper. The drained and undrained shear strengths and the soil-water characteristics are different due to the varying soil structures in the specimens. The results of this study support the contention that the resulting soil structure in a compacted soil is a function of initial compaction water content. The influence of soil structure on the drained and undrained shear strength parameters in unsaturated conditions is reflected in shear strength contribution due to suction (i.e., φ b values). In spite of varying soil structures resulting due to different initial water contents, there appears to be a unique relationship between tan φ b / tan φ' versus {(S-S r )/(1-S r )} or tan φ b / tan φ' versus S κ for the clay till tested. More studies are required on different compacted soils to verify these relationships. References [1] Gan, J.K.M. and Fredlund, D.G. Multistage direct shear testing of unsaturated soils. Geotechnical Testing Journal, 11 (2), (1988). 132-138. [2] Vanapalli, S.K.. Simple Test Procedures and their Interpretation in Evaluating the Shear Strength of Unsaturated Soils. Ph.D. thesis. University of Saskatchewan, Saskatoon, Canada. (1994), 35. [3] Fredlund, D.G. and Rahardjo, H., Soil Mechanics for Unsaturated Soils. John Wiley & Sons Inc., New York, NY (1993) [4] Vanapalli, S.K., and Fredlund, D.G.. Interpretation of undrained shear strength of unsaturated soils in terms of stress state variables, Proc. Nsat 97, (1997). 35-45. [5] Vanapalli, S.K., Fredlund, D.G., Pufahl, D.E., and Clifton, A.W. Model for prediction of shear strength with respect to soil suction. Can. Geotech. Journal., 33(3), (1996). 379-392. [6] Fredlund, D.G., Xing, A., Fredlund, M.D., and Barbour, S.L. (1996). The relationship of the unsaturated soil shear strength to the soil-water characteristic curve. Can. Geotech. Journal, 33(3), 44-448.