3.1. Characteristics of U-δ Curves
Figure 4 shows the experimental curves between the uplift load
U and the displacement of pile top
δ for different curves, and
Figure 5 shows the time courses of
δ in the semi-logarithmic coordinate. According to the
U-δ curves, the uplift displacement of conventional piles (KB1) increases relatively slowly at the initial stage of loading. When the load increases to a certain level, the displacement increases suddenly, indicating a type of steep change. However, for the KB2 and KB7 piles, the uplift displacement increases slowly with the increasing load, showing a gradual change. According to the “Technical Specification for Testing of Building Foundation Piles” (JGJ106-2014), for the steeply deformed
U-δ curve (e.g., KB1), the load corresponding to the beginning of the sudden increase in displacement is taken as the ultimate bearing capacity of pile. For the slowly deformed
U-δ curves (e.g., KB2 and KB7), the load of the previous stage, where the slope of
δ-lg
t curve becomes steeper or the tail of the curve is obviously bent, can be taken as the pile’s ultimate bearing capacity. The experimental results of different piles are summarized in
Table 2.
Comparing the
U-δ curves of the KB1 type pile and KB2 type pile, when the load is less than the bearing capacity, the change rate of pile top displacement of the KB1 and KB2 piles is basically the same, and the pile top displacement increases relatively slowly. When the load exceeds the ultimate bearing capacity, the top displacement of the KB1-type pile increases sharply. According to the test results of piles (
Table 2), the average uplift bearing capacity of the KB1 pile is 12.0% greater than that of the KB2 test pile, while the uplift displacement corresponding to the bearing capacity is 29.6% larger than that of the KB2 pile. From the
U-δ curves, the vertical displacements of KB1 and KB2 type test piles under the same load have little difference, indicating that the uplift performance of the two types of piles is basically the same. On the whole, the uplift bearing capacity of both KB1 and KB2 piles reaches the estimated value and meets the design requirements.
Comparing the
U-δ curves of KB1 and KB7 piles, at the initial loading stage, the vertical displacement of the two types of piles changes basically the same as the uplift load, and both show a linear trend. This distribution characteristic is mainly caused by the elastic deformation of the pile at the initial stage of loading. The load applied in the initial test stage was relatively small. Under the action of a small load, the interfaces between the main reinforcement and concrete and between the pile and soil did not reach the ultimate stress state. The displacement of the pile top will be mainly controlled by the elastic deformation of the pile-soil interface, so their displacements basically show a linear increase with a similar slope with the increase of the load. With the further increase of the load, the change rate of vertical displacement increases gradually, showing an upward concave. However, the change rate of vertical displacement of KB1 type pile is faster than that of KB7 type pile, and the
U-δ curves of KB7 piles are always below that of KB1 piles. According to
Table 2, the uplift bearing capacity of the KB7-type pile is similar to that of the KB1-type test pile, while its corresponding uplift displacement is much (about 7.4 mm) smaller than that of the KB1-type test pile. The KB7 type piles have better uplift performance than the KB1 type pile.
In addition, the
U-δ curves of KB2 and KB7 piles have the same “slow change” characteristics. With the gradual increase of the load, the change rate of displacement of KB2 piles is greater than that of the KB7 pile. Under the load of 5520 kN, the vertical displacement of the KB7 type pile is about 55% of that of the KB2 type pile. According to the experimental results in
Table 2, the averaged uplift bearing capacity of the KB7 pile is about 550 kN larger than that of the KB2 pile, and its corresponding uplift displacement is about 2.9 mm smaller than that of the KB2 pile. This is because the KB7 pile adopts the hole-forming method of dry rotary drilling, which avoids the mud skin effect between the pile body and the soil.
In summary, the uplift performance of the KB1 and KB2 piles is basically the same; due to the absence of mud skin effect in the KB7 pile, its displacement is smaller than that of KB1 and KB2 piles, with similar or greater ultimate bearing capacity. Both the conventional pile (e.g., KB1) and the new pile (e.g., KB2 and KB7) can meet the designed uplift bearing capacity. The new pile has only four composite anchors as the main reinforcement, with a reinforcement ratio of 0.75%, while the reinforcement ratio of the KB1 pile is 3.84%. That is, compared with the conventional pile, the reinforcement ratio of the new-type composite-anchor pile is reduced by 80.54%, and the cost of the pile cage is reduced by about 47%.
3.2. Distribution of Axial Forces
Figure 6 shows the distribution of axial force along the piles. Since the results of the repeated tests for each pile type are basically the same, only one set of test results is illustrated for each pile type. It can be seen from the figure that the axial force in the KB1 pile decreases gradually from top to bottom, and the pile body is basically in a tension state. For the KB2 and KB7 type piles, the upper part of the pile body is in a state of compression due to the application of prestress. In the initial stage of loading, the prestress gradually cancels out, and with the increase of the vertical load, the pressure on the upper part of the pile body gradually decreases, and the axial force in the tension zone in the lower part of the pile gradually increases. Generally, the stress in the lower middle part of the pile body is the greatest, and it decreases rapidly towards the pile top and the pile bottom.
Table 3 shows the distribution of the pile’s lateral friction resistance under a load of 5520 kN. Comparing the distribution of axial force and lateral friction between the conventional uplift pile and the new prestressed uplift pile with semi-bonded composite anchor, the stressed area of the former is mainly concentrated at the elevation from −1 to −4 m, while the latter is mainly at the elevation from −11 to −18 m. The maximum lateral friction resistance of the new pile is 2.5 times that of the conventional uplift pile. In addition, the lateral friction resistance of the new piles at the elevation from −11 to −18 m is about 10 times that of the conventional piles, and the lateral friction resistance of the new piles at the elevation from −18 to −21.5 m is about five times that of the conventional uplift piles.
Comparing the lateral friction resistance of KB2 and KB7 piles, the stressed positions are mainly concentrated in the lower middle part of the pile body. At the most stressed position (i.e., from −11 to −18 m), the lateral friction of the KB7 pile is 1.0–1.1 times that of the KB2 type pile; at the location from −1 to −11 m, the lateral friction of the KB7 pile is about 25% that of the KB2 pile; and at the location from −18 to −21.5 m, the lateral friction of KB7 pile is about 90% of that of KB2 pile. The differences in the lateral friction between the KB2 and KB7 piles are mainly caused by the different hole forming methods of the two.
In summary, the conventional pile (i.e., KB1) is mainly stressed at the upper part of the pile body, and the new piles (i.e., KB2 and KB7) are mainly stressed at the lower middle part. As we know, the soil pressure on the pile side increases with increasing burial depth, so the lateral friction resistance of the lower middle part of the new pile can be exerted more effectively, and the uplift bearing capacity and the uplift resistance of the pile can be improved correspondingly.
3.3. Cracking Characteristics of Test Piles
Figure 7 shows the strain distribution of the KB1 and KB2 piles, which reflect the development of microcracks in the pile during loading. From
Figure 7a, it can be seen that no significant cracks appeared in the pile body of KB-1 during the first three loading stages throughout the loading process. With the increase in load, the pile strain gradually increases. Starting from the fourth loading stage (2200 kN), micro-cracks first start to appear in the area from 0 to 4 m at the top of the pile. As the load increases further, the cracking area gradually expands to the lower part of the pile body. When the pile is loaded to the maximum stage, the cracking area develops to a large range of 0–14.5 m from the top of the pile.
On the other hand,
Figure 7b shows the strain distribution of the KB2 pile throughout the loading process. No significant cracks were observed in the pile for the first seven loading stages. Similarly, the pile strain gradually increases with the increase of load. From the eighth loading stage (i.e., 4140 kN), cracks start to appear in the zone from 6.5 to 14 m, and the cracks in this area gradually become larger with the further increase of load.
Comparing the strain distribution of KB1 and KB2 piles, it can be seen that, (1) due to the prestressing applied to the KB2 pile, no cracks were generated in the first seven loading stages, while the KB1 test pile showed obvious micro-cracks after the third loading stage. (2) The cracks in KB2 pile were mainly distributed in the area from 6.5 to 14 m, while the cracks in KB1 pile were distributed in the range from 0 to 15 m from the top of the pile, and the cracking area in KB2 piles was only half of that in the KB1 pile. (3) The maximum crack width of KB1 pile under 5060 kN load is 0.075 mm and that of KB2 pile is about 0.036 mm, which is only 48% of the former, as integrated by the strain data.
In summary, compared with the conventional piles (KB1 type), the cracking situation of the new KB2 pile is significantly improved.
3.4. Discussions
3.4.1. Comparison between the Costs of Different Uplift Piles
As mentioned above, compared with the traditional uplift pile, although the reinforcement ratio of the newly developed pile has significantly been reduced, its comprehensive mechanical properties are greatly improved. In fact, another great advantage of the new pile is that its construction cost has been significantly reduced.
Based on the different structures of the newly developed piles and conventional piles, an estimate of their costs can be made easily. At first, the anchorage system of the new pile is only composed of four composite anchor cables, four three-hole anchorages, and two auxiliary bars, and its cost is about 1270 US dollars, accounting for 65.5% of the whole pile cost (i.e., $1940). However, the main reinforcement of the conventional pile is composed of 24 HRB400 steel bars with a diameter of 32 mm. Its cost is about $2260, which accounts for 77.7% of the total construction cost of the pile (i.e., $2920). That is to say, compared with the conventional uplift pile, the cost of the anchorage system of the new uplift pile is reduced by 43.8%, and the total cost of a single pile is reduced by 33.6%.
3.4.2. Phenomenon of Cracking in Uplift Piles
Concrete cracking is an important feature that distinguishes uplift piles from compression piles. Cracking will cause great harm to the pile body and will directly accelerate the corrosion of the steel bars in a pile. Especially in the presence of corrosive groundwater, the cracks will pose a great hidden danger to the bearing performance and durability of the uplift piles.
From the in-situ load test in this study, the conventional pile and the new pile formed cracks under the uplift load of 2200 kN and 4140 kN, respectively. As the load continued to increase, the cracking range of the pile body continued to develop. When the load reaches greater than 5000 kN, the cracking range of the conventional pile reaches 65.9% of the pile length, while the cracking range of the new type of pile is only 34.1% of the pile length, indicating that the crack resistance of the new piles has been greatly improved. Generally, compared with the conventional pile, the new pile’s cracking load is increased by 88.2%, and its crack range at the maximum load is reduced by 48.3%. The improved crack resistance will enhance the durability of the uplift pile. In addition, in the new type of pile, the multi-layer structure of the composite main bar makes the load-bearing steel strands isolated from the external environment under the protection of the grouting body and high-strength steel piles. As such, the new pile is expected to gain better durability than conventional piles.
In addition, the in-situ load tests show that the bearing capacity of the piles did not decrease significantly after cracking. However, cracking does have two adverse effects on the pile body. First, as mentioned above, the steel bars lose the protection of the concrete, and the rate of corrosion will increase. Especially in areas with a high water table, the corrosion rate of steel bars can be significant. Secondly, the cracking and fracture of the concrete will lead to the redistribution of the stress of steel bars and the concentration of stress on the steel bars, resulting in increased deformation. The accumulation of this increased deformation may likely increase the top displacement of uplift pile, thereby failing the pile. It is worth noting that, from the experimental results of side friction resistance and axial force after the occurrence of pile body crack, the side friction resistance of the cracked pile body is still being effectively exerted.
3.4.3. Mechanism and Simulation of Pile Cracking
Cracking is a discontinuous phenomenon in solid materials, which belongs to the category of material strength theory. For reinforced concrete, the stress on the weakest surface will reach the tensile strength when the concrete is about to crack. After cracking, the concrete stress at the fracture is reduced to 0, and the load is completely borne by the steel bar. In the bond region adjacent to the crack, the stress of the steel bar is partially transferred to the concrete through the bond between the steel bar and the concrete, and the bond stress in this region varies between 0 and a maximum value. In areas away from the cracks, the reinforcement and concrete deform cooperatively.
In uplift piles, there are different transfer mechanisms for the bond between the main reinforcement and the concrete. This section will take the pile with ribbed main reinforcements as an example for explanation. First, when the bonding stress is relatively small, it is mainly achieved through the bonding effect and the occlusal effect between the cement-based matrix, the aggregate, and the surface of the steel bar. As the load increases and the bond gradually fails, two new bond mechanisms are triggered between the reinforcement and the concrete, i.e., the friction and the compression between steel rib flange and concrete. Among them, the compressive effect between rib flange and concrete is the leading way to transmit the bonding stress under high stress. The compressive stress before the flange can radiate to the surrounding concrete, and the pressure can be decomposed into components parallel to and perpendicular to the reinforcement. The parallel component is numerically equal to the bond stress, and the perpendicular component causes a hoop tensile stress in the concrete, which can also lead to splitting bond failure unless there is sufficient restraint.
In the design and engineering application of uplift piles, a numerical method for predicting the cracking loads and simulating the cracking characteristics of uplift piles is required. This is important to aid in the design of such structures. As a matter of fact, although there are cracking load prediction methods for reinforced concrete structures at present, their accuracy is poor and they cannot be applied to uplift piles, especially to complex structures, such as the new anchor-cable uplift pile proposed in this study. In terms of numerical methods, with the continuous progress of numerical simulation methods, a variety of cracking analysis theories have been established. However, the cracking simulation of reinforced concrete uplift piles is still a difficult problem.
For homogeneous isotropic materials, the use of fracture mechanics theory and damage mechanics theory to solve the crack problem has been quite developed. For uplift piles, the application of relevant theories and numerical methods is far from practical. Uplift piles consist of main reinforcements, stirrups, and concrete. At first, the composition of concrete is complex, and the physical and chemical properties of each component vary widely. Secondly, the connection method of steel bars is relatively complicated. Finally, the surface of steel bars may have a complex ribbed structure. An irregular stress concentration causes a large number of micro-cracks, and the expansion of micro-cracks is affected by the resistance of pores, aggregates, and steel bars. The fracture or damage analysis of cracks is much more complicated than that of homogeneous materials, which brings great difficulties to the numerical simulation of cracking in uplift piles.
However, these theoretical and numerical studies have given us a lot of inspiration. For example, in recent years, scholars such as Thamburaja et al. [
29,
30] have successfully applied numerical methods to simulate the local cracking problem of concrete. If these numerical simulation methods are applied in this study to simulate the cracking phenomenon of the pile body accurately, it will bring great convenience to future research work on the new piles.
3.4.4. Possible Limitations of This Study
As mentioned above, a new type of prestressed uplift pile that adopts the semi-bonded composite anchor as the main reinforcement is developed for the first time in this study. Then, a site mainly containing sand and silt layers was selected to carry out static load tests to study the new pile’s deformation, stress, bearing capacity, and cracking characteristics. However, it should be further pointed out that this study was carried out under certain preconditions, so there are still some unavoidable limitations.
First of all, this paper only focuses on the uplift performance of the new pile under static loads, ignoring its performance under seismic loads. It is undeniable that the mechanical response of pile foundations under seismic load will be more complicated. Studies have pointed out that pile foundations can effectively resist the horizontal load generated by the seismic event and can solve the liquefaction problem of the foundation to a certain extent. However, the specific performance of the new pile under seismic load still needs to be further verified. At present, there are two main ways to study the seismic performance of pile foundations, one based on the shaking table test and the other based on the numerical simulation methods (e.g., finite element method). Both approaches can be used in our future research on this new type of pile.
Secondly, the site for load tests in this study is mainly composed of silt to sand layers. Whether the results of the load tests are applicable to clayey soils is another issue that needs to be further discussed. In fact, due to the huge differences in deformation, strength, and permeability characteristics between clay and coarse-grained soils, there may be considerable differences in the pile–soil interaction mechanisms under both static and seismic loads. For this problem, more load tests on sites with different soil properties and numerical simulations will be carried out in the future for targeted research.