Research Article  Open Access
Suman Manandhar, Noriyuki Yasufuku, "Analytical Model for the EndBearing Capacity of Tapered Piles Using Cavity Expansion Theory", Advances in Civil Engineering, vol. 2012, Article ID 749540, 9 pages, 2012. https://doi.org/10.1155/2012/749540
Analytical Model for the EndBearing Capacity of Tapered Piles Using Cavity Expansion Theory
Abstract
On the basis of evidence from model tests on increasing the endbearing behavior of tapered piles at the loadsettlement curve, this paper proposes an analytical spherical cavity expansion theory to evaluate the endbearing capacity. The angle of tapering is inserted in the proposed model to evaluate the endbearing capacity. The test results of the proposed model in different types of sands and different relative densities show good effects compared to conventional straight piles. The endbearing capacity increases with increases in the tapering angle. The paper then propounds a model for prototypes and realtype pile tests which predicts and validates to evaluate the endbearing capacity.
1. Introduction
The pile endbearing capacity in sands is not only affected by the compressibility of soil, shear stiffness, and strength, but also by the angle of tapering of the pile. Very few researchers have noticed the effects of tapering angle in endbearing resistance when penetrated downward in a frictional mode [1]. The shape of the pile type changes from a straightsided cylindrical shape to a conical type, while the weight and volume of the pile appendages to the ground and mechanism also change. Therefore, the tapering effects must be taken into consideration when evaluating the endbearing capacity of tapered piles [2, 3]. There are two main methods to evaluate the endbearing capacity: a semiempirical method using SPTN values and a theoretical approach based on geomechanical considerations. Out of all the theoretical methods of geomechanics, the cavity expansion theory is particularly popular among geotech experts [4–6]. Yasufuku et al. derived successfully an evaluation technique for the endbearing capacity in nondisplacement straight cylindrical piles using a spherical cavity expansion theory for closed solutions [7, 8]. This research asserts the use of the spherical cavity expansion theory as a way of evaluating the endbearing capacity of tapered piles based on axial cylindrical model tests. The tapering angle is inserted in the analytical model to evaluate the ultimate endbearing capacity of the spherical cavity expansion theory previously postulated by Yasufuku et al. [7, 8]. The proposed model then referred to predict and validate other prototypes and realtype pile reference data to estimate the endbearing capacity.
2. Methodology and Evidence from Test Results
Chromiumplated three steel piles—one straight (S) and two tapershaped (T1 and T2)—were used for model tests (Table 1) on modeled ground, having relative densities of 60% and 80%, respectively (Table 2). The model piles have equal lengths and the same tip diameters. The model chamber has dimensions of 1000 mm height and a diameter of 750 mm, as shown by Figure 1(a).
 
Note: : length of pile; : diameter at the pile head; : pile tip diameter; FRP: fiberreinforced polymer; : angle of tapering; na: not applicable. 

(a)
(b)
Japanese Industrial System (JIS A 1224) and Japanese Geotechnical Standards (JGS 0161) [9] were used to determine the maximum and minimum dry densities of sands so as to determine the relative densities (Table 2). A multiple sieving technique was used to prepare model ground at an appropriate relative density by height of fall and nozzle diameter. Changes in nozzle area and/or diameter of multiple sievings determine the relative density of the ground when particles fall at a specific height and vice versa [10]. In this method, the height of falling was determined by keeping a constant nozzle area. Then, two sands, K7 and Toyoura (TO) sands, were allowed to fall through multiple sievings from the heights of 1400 mm and 700 mm, respectively. The pile was installed at a height of 710 mm from the bottom, and soil was further poured in up to a height of 930 mm, as shown by Figure 1(b). Following this, an overburden pressure () of 50 kPa was furnished vertically through the upper plate, and the pile was installed up to 200 mm at a rate of 5 mm/min to facilitate in castinplace pile condition. A minimum of fifteen hours is required for stress relaxation after installation. Afterwards, a pile loading test was performed up to 0.4 settlement ratio. In the loading test, load cells were installed inside the pile tip and at the pile head, which were connected with the cord. During loading, the load cell at the pile tip can measure directly the endbearing capacity of the pile.
Figure 2 shows evidence obtained from model test results of straight and tapered piles of K7 and TO sands. These tests show that when the tapering angle increases, the pile tip resistance increases for both sands at a normalized settlement ratio. Here, and are considered as settlement and the pile tip diameter, respectively. The normalized total endbearing capacity has been plotted by dividing mean effective stress which is the mean of lateral and vertical stresses (i.e., ). For normally consolidated soil, the lateral stress can be determined by selecting a 0.5value in the relation between lateral and overburden stresses (i.e., ), where is the coefficient of earth pressure at rest relating with dry unit weight of the ground and its depth. Figure 3 shows the normalized total endbearing capacity of sands at different relative densities. The result adds tapering effects to the endbearing mechanism by increasing the tapering angle. This evidence obtained through small model tests explains the merits over tapered piles. Given this, it is necessary to develop an analytical model for evaluating the endbearing capacity, and it is imperative to check the validity and liability of verifying with prototypes and real pile references, which will be discussed in the next section.
3. Analytical Model to Evaluate EndBearing Capacity
The compressibility of soil, shear stiffness, and strength all affect the pile endbearing capacity in sands. Compressibility is believed to differ greatly, ranging from incompressible silica sands to highly compressible carbonate sands for different types of soils. A spherical cavity expansion solution has been incorporated to estimate the endbearing capacity of cylindrical straight piles in closed forms by Yasufuku et al. [7, 8]. On the basis of this estimation technique, this model is advanced by introducing the angle of tapering to evaluate the endbearing capacity of tapered piles. Figures 4(a) and 4(b) explain a modified failure mechanism using a spherical cavity expansion theory which was initially postulated by Yasufuku et al. [7, 8] for frictional soils with cavity expansion pressure proposed by Vesic [4] to determine the ultimate bearing capacity . In the modified mechanism of tapered piles, it is assumed that a rigid cone of soil exists beneath the pile tip with the angle and that outside the conical region, the zone is subjected to isotropic stress which is equal to the cavity expansion pressure . In addition, the active earth pressure conditions are considered to exist immediately beneath the pile tip along AC plane. Then, at point B, the moment is created as shown by Figure 4 for the cavity expansion pressure , ultimate endbearing pressure , and the active earth pressure [3]. Then, the ultimate bearing capacity of the tapered pile can be addressed with the formula
(a)
(b)
The cavity expansion pressure on the basis of Vesic theory [4] can be written as where where , , and are known as dimensionless spherical cavity expansion factors, reduced rigidity index, and rigidity index, respectively, which are associated with friction angle , shear stiffness , and average volumetric strain for the plastic zone around a cavity, with the coefficient of earth pressure at rest and overburden pressure . provides a ratio of shear stiffness to strength, and is a parameter in lieu of the soil compressibility, in which shear stiffness, shear strength, and average volumetric strain are combined. Proceeding, is basically calculated as an averaged unit weight . On the basis of the theoretical relation to plastic equilibrium, Ochiai [11] derived the critical state friction angle as
Asserting is effective and rational in practical applications as a strength parameter [12–15], the friction angle guarantees the minimum shear strength under the same initial conditions and soil density, with initial fabric and confining pressure considered to be independent. The value of of sands is almost equal to the maximum friction angle under the high confining stress, which will be mobilized below the pile tip [16, 17]. Therefore, the is recommended for estimating the pile endbearing capacity of sands. At the same time, an empirical equation is used to predict the value in the strain level of 10^{−3} from the measured value [18], in MPa. The penetration resistance is presumed to increase with the square of the relative density and to be directly proportional to the effective overburden pressure and inversely proportional to the void ratios [19] such that where is relative density and and are maximum and minimum void ratios. Rearranging values of from (5), the empirical correlation can be expressed as
The empirical equation is a function of in a simple manner [6]. Rearranging from (3), a function of , , , and can be written in this form
Equation (7) measures the average volumetric stain for a plastic zone around a cavity, which increases with increasing overburden pressure in the ground. The rearrangement of this equation addresses the evaluation of the ultimate pile endbearing capacity as follows: where
The Kondner types of hyperbolic curves are useful for predicting the load settlement curves of nondisplacement piles in virgin loading [20–22]. A simple hyperbolic function is assumed for estimating the relationship between the applied pile tip stress, , and the corresponding normalized pile tip settlement, , as where and are experimental parameters corresponding to the inverse values of suitable initial shear stiffness and ultimate pile stress, respectively.
When introducing reference displacement , presented by Hirayama [22], which is empirically derived for nondisplacement piles in sands, expressed as the normalized settlement required to mobilize the half of the ultimate endbearing capacity , the inverse of the initial shear stiffness is expressed such that
Validity of the Model
The validity of the model was checked after verifying it with a small model and prototype pile materials, including with different sources of data. The parameters of TO sand K7 sand and pile materials have been taken from Manandhar et al. [1] and Fanshawe brick sand from Sakr et al. [23–25]. This research employs a cylindrical fiberreinforced polymer (FRP) FC pile and a threetapered FRP composite tapered pile, which is an offtheshelf pipe with an average diameter of 162.4 mm and a ply angle of 55°. These fabricated FRP tapered piles using six layers of glass filament wound (GFW) were placed at ply angles 0° (parallel to pile axis) and 90° (hoop layer) [23] (Table 1). The pile installation of Fanshawe brick sand is confined to a low pressure (LP) with an initial radial stress of 30 kPa and a vertical pressure of 60 kPa, as well as a high pressure (HP) with an initial radial stress of 60 kPa and a vertical pressure of 120 kPa at different depths and mobilized up to 0.4 normalized settlement ratios. The fundamental geotechnical properties of sand are set out in Table 2. The vertical pressure can be obtained by using the simple formula discussed in the previous section. Figure 5 shows there is increase in total endbearing capacity when increasing the tapering angles in the closed form cavity expansion solution. Larger total endbearing resistance is reflected by high density ground. Similarly, high endbearing capacity has been obtained at a high radial stress at the same density ground, as shown by Figure 6.
Further, the total endbearing capacity measured in kN is where is the radius of the pile tip at the middle point of the embedded pile section.
The following arrangement can be obtained by substituting the value of using (1), (2), (10), and (11) into (10):
Assume for the total endbearing capacity of straight piles. When the total endbearing capacity of tapered piles is normalized with the total endbearing capacity of straight piles by taking ratios between them, the following relation is obtained:
This equation shows the relationship between the angle of internal friction at a critical state and tapering angle as the interdependent function for evaluating the total endbearing capacity of tapered piles. This verifies that the endbearing capacity depends on the angle of internal friction at the critical state condition and the tapering angle of piles only. When there is a change in the angle of tapering, the endbearing capacity will also change independently of overburden pressure, confining pressure, and the shear modulus of soil. Hence, Figures 7, 8, and 9 were plotted to verify this mechanism of normalized ratios of total endbearing capacity for different sands. There is a clear increase in the total endbearing capacity at 0.1 settlement ratios for all types of soils and pile materials.
Further, different tapering angles were asserted to understand the behavior of endbearing capacity in sands. This study employed model tests, the prototype test described by Sakr et al. [23–25] and the real type Rybnikov [26] pile. Rybnikov carried out tests in the Irtysh Pavlodar region of the former Soviet Union and used bored castinplace tapered piles. The holes for the piles were drilled with endless screws. Seven different piles were consummated having lengths of 4.5 m each, constituting five tapered piles and two cylindrical piles to comprehend the behavior of tapered piles with respect to straight piles. In this study, only the geometry of pile materials is considered for the analyses, with the assumption of soil properties obtained by TO sand as shown by Table 2.
Figure 10 represents the effects of the tapering angle in four different types of pile materials and soils by dividing the total endbearing capacity of straight piles to tapered piles. The results show an increase in the endbearing capacity of almost 10% for the maximum tapered angle, indicating that the endbearing capacity is affected by the angle of tapering and angle of internal friction only.
Afterwards, the measured and calculated results of the end bearing capacity were plotted to verify the model. The model was verified with the addition of various reference data. The measured and predicted data for the endbearing capacity, measured in kPa, are shown in Tables 3 and 4, respectively. Figure 11 shows how the proposed model fits remarkably well and that it is valid for evaluating endbearing capacity when various data have been obtained. The measured and calculated results were plotted in a 1 : 1 ratio and proved the validity of the model with the parameters used with different types of pile geometry and sands.

 
Note: *FS: Fanshawe brick sand. 
Conclusions
The benefits of tapered piles obtained through evidence from small model tests in the laboratory lead to the development of an analytical model for the estimation of the endbearing capacity of tapered piles. The assertion of tapering angle in the analytical spherical cavity expansion theory was successfully evaluated for the endbearing capacity of tapered piles. The proposed models have been validated through the verification of model tests, prototype tests and real type pile tests. The main conclusions drawn using the various proposed models are summarized as follows.(1)Parametric studies with the key variable of the tapering angle show that the proposed model effectively sustains the general behavior of tapered piles in evaluating the endbearing. (2)The total endbearing capacity of tapered piles confines to restrain the failure mode, which increases the endbearing capacity, and the model is supported by the measured data.
Acknowledgments
The authors would like to extend their gratitude to Professor Kiyoshi Omine for his invaluable advice. In addition, heartfelt thanks go to laboratory assistant Mr. Michio Nakashima and colleague Mr. Tohio Ishimoto for their continued support.
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Copyright
Copyright © 2012 Suman Manandhar and Noriyuki Yasufuku. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.