The Effect of Temperature on Dynamic Characteristics of Frozen Clay under Principal Stress Rotation

Zhang, Bin-Long; Wang, Da-Yan; Zhou, Zhi-Wei; Ma, Wei; Lei, Le-Le

doi:https://doi.org/10.1155/2021/3127253

Advances in Materials Science and Engineering

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Abstract Introduction Methods Discussion Conclusions Data Availability Conflicts of Interest Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2021 | Article ID 3127253 | https://doi.org/10.1155/2021/3127253

The Effect of Temperature on Dynamic Characteristics of Frozen Clay under Principal Stress Rotation

Bin-Long Zhang,^1,2Da-Yan Wang ,¹Zhi-Wei Zhou,¹Wei Ma,¹and Le-Le Lei³

Academic Editor: Hossein Moayedi

Received10 Aug 2021

Revised06 Oct 2021

Accepted23 Nov 2021

Published20 Dec 2021

Abstract

The foundation soil is always subjected to complex stress, including continuous rotation of the principal stress caused by traffic and earthquake loads. To comprehend the dynamic characteristics of frozen clay under complex stress sate, including continuous rotation of the principal stress, this study investigates the effect of temperature on the dynamic characteristics of frozen clay under principal stress rotation using a frozen hollow cylinder apparatus (FHCA-300). The test results reveal that the cumulative plastic strain of frozen clay samples exponentially increases with the rising of temperature under principal stress rotation. The influence of temperature is more profound with a high cyclic stress ratio (CSR). A decrease in temperature can improve the stiffness of the frozen clay, reduces its energy dissipation, and enhances its ability to resist dynamic loading. However, the principal stress rotation phenomenon may aggravate the damage of frozen clay and increase the energy dissipation and reduces its ability to resist dynamic loading. Based on the experimental data, an empirical expression was proposed to describe the coupling influence of CSRs and temperature on the axial resilient modulus of frozen clay, which can predict the development of axial resilient modulus under different thermal-mechanical conditions.

1. Introduction

Frozen soils are compound materials composed of solid mineral particles, polycrystalline ice, unfrozen water, and gaseous inclusions. They are widely distributed in cold regions or artificial ground freezing projects [1, 2]. With the rapid development of the society, projects increasingly have been built on frozen soil in the cold region. Furthermore, the artificial ground freezing (AGF) method, which is widely used in large-scale cross-sea and river-crossing projects in coastal areas, is an effective underground engineering support technology [3]. In these projects, frozen soils as a foundation or supporting wall are subjected to dynamic loads such as those from waves, traffic, and earthquakes. Such dynamic loads may impact the stability of projects, reducing their service lifetime and increasing maintenance costs [4]. Therefore, it is crucial to study dynamic characteristics of frozen soil for engineering design in cold regions and artificial ground freezing projects.

In the past few decades, much attention had been paid to investigate the dynamic properties of frozen soils through triaxial dynamic loading, and many meaningful results were obtained. For example, the effects of temperature, confining pressure, freeze-thaw cycles, initial compaction degree, and initial water content on the dynamic shear modulus and damping ratio of various frozen soils were also investigated under multistage cyclic loading by using a triaxial apparatus [5–8]. The corresponding empirical models of maximum dynamic shear modulus were proposed. Furthermore, experimental studies on the residual deformation and stiffness of frozen soils have been conducted under long-term cyclic loadings to investigate the effect of variables, such as soil type, cyclic amplitude, frequency, water content, temperature, initial deviatoric stress ratio, and confining pressure [9–19]. The results obtained from tests showed that the residual deformation increases significantly with the increase of cycles, cyclic stress ratio, temperature, freeze-thaw cycles, and cyclic amplitude but decreases with that of frequency, water content, and confining pressure. Additionally, some results reported that the stiffness decreases at the initial stage and then tends to stabilize, whereas some other results suggested that the stiffness increases as the number of cycles increases. All the previously mentioned research plays a great role in understanding the dynamic properties of frozen soils. However, on the one hand, consensus regarding stiffness change has not been reached. On the other hand, most research efforts were dedicated to cyclic triaxial loadings without the rotation of principal stress, and limited attention was paid to the characterization of dynamic behavior with rotation of principal stress axes.

In actual engineering, the stress path of soil foundation is complex, and the amplitude of principal stress acting on the geotechnical structures constantly changes under dynamic loadings; meanwhile, principal stress axes constantly rotate [20–22]. However, it is difficult to investigate the characteristics of soil under principal stress rotation due to the intrinsic disadvantages of triaxial apparatuses. Hence, the hollow cylinder apparatuses (HCA) have been developed to explore the characteristics of soil under principal stress rotation and complex stress paths [23–32]. Nakata et al. [23] and Tong et al. [24] reported that an increase in pore pressure and strain could be solely triggered by continuous rotation of the principal stress axis, although the magnitude of the principal stresses remains constant. Erken and Ulker [25] and Huang et al. [26] found that the rotation of the principal stress axis can reduce dynamic strength. Mamou et al. [27] and Wang et al. [28] demonstrated that the principal stress rotation reduces the resilient modulus of the soil without changes in the magnitude of the principal stresses. Besides, Cai et al. [29] and Qian et al. [30] indicated that cyclic principal stress rotation accelerates the accumulative permanent deformation. Wang et al. [31] and Sun et al. [32] obtained similar results. Although these lines of evidence confirm that the principal stress rotation significantly influences the mechanical behaviors of soil, the investigations on the influence of principal stress rotation on the cyclic response of frozen soil remain scarce.

This paper aims to expand the current understanding of frozen soil behavior by investigating the effect of temperature on the dynamic characteristics of frozen clay under the principal stress rotation. A series of dynamic loading tests were conducted using FHCA-300 to assess the evolution of the dynamic strain, stress-strain hysteresis curve, resilient modulus, and damping ratio with number of cycles under principal stress rotation. The results provide a significant guidance for the design and operation of frozen soil engineering.

2. Test Material and Methods

2.1. Test Device, Material, and Specimen Preparation

The frozen hollow cylinder apparatus, as shown in Figure 1, was jointly developed by the State Key Laboratory of Frozen Soil Engineering and GCTS firms. It was employed to perform the cyclic loading tests on frozen soil specimens. Compared with the triaxial apparatus, it was the main instrument for studying the mechanical properties of frozen soil under complex stress paths involving the principal stress rotation that can exert axial force, torque, and internal and outer confining pressure on the installed specimen at a stable negative temperature. The maximum loading frequency of the instrument is 20 Hz; the temperature of the pressure chamber ranges from −40°C to 80°C with a precision of ±0.1°C; the axial stress loading varies from −100 to 100 kN; the torque loading range is −1000-1000 Nm; the maximum confining pressure is 22 MPa; the confining pressure oil used is dimethyl silicone with viscosity of 50 CS. Additionally, parallel tests under different conditions have been carried out to prove the reliability of the test and the repeatability of this apparatus. As detailed description of this instrument and parameters were provided by Guo et al. [33] and Lei et al. [34], correspondingly, according to the stress of the thin-walled element of the hollow cylindrical specimen, the conversion relationship between the loading parameters of the test apparatus and the stress of the specimen is expressed in Table 1 [35].

We have that represents the axial load; represents the torque; represents the outer confining pressure; represents the inner confining pressure; represents the outer radius; represents the inner radius; , , and represent the height, outer diameter, and inner diameter strain, respectively, while is the torsional angle.

The test soil was taken from the cold region of Qinghai-Tibet Plateau, China, where the Qinghai-Tibet Railway, Laluo Dam, and other projects have been built. The liquid and plasticity limits of the tested soil are 27.7% and 17.6%, respectively. Based on the Unified Soil Classification System (ASTM, 2011), the tested soil can be classified as the low liquid limit clay (LC). The maximum dry density is 1.77 g/cm³, and the saturated moisture content is 19.8%. The particle gradation of the soil is shown in Figure 2.

In this study, a standard routine preparation procedure of specimens was adopted to guarantee the uniformity of the specimens. First, the air-dried and crushed soil was sieved by a 2 mm screen. The soil with a moisture content of 19.8% was added and mixed uniformly by hands, after which the wet soil was stored in a sealed bag for 24 hours for the even distribution of water. Then, a certain amount of clay was put layer-by-layer into a self-made sample mold with the same thickness (5 layers) and compacted at a certain speed using a sample-making machine. Finally, a hollow cylindrical sample with a height of 200 mm, an outer diameter of 100 mm, and an inner diameter of 60 mm was obtained with a dry density of 1.77 g/cm³ (Figure 3(a)). The prepared hollow cylindrical specimen was placed into the pressure chamber of the FHCA-300 apparatus and was quickly frozen at the temperature of −30°C to prevent frost heave and moisture migration. Then, the temperature was set at the desired temperature for 10 hours to ensure the even distribution of the sample temperature (Figure 3(b)). At last, a hollow cylindrical sample of frozen soil was obtained.

2.2. Test Program

Ishihara and Towhata [35] proved that it is possible to use a hollow cylinder apparatus to achieve circular stress paths in the plane through coupled dynamic loading of axial force and torque under principal stress rotation. Under principal stress rotation, the stress is composed of deviator stress and shear stress. To simultaneously reflect the influence of deviator stress and shear stress on the test, the CSR was defined [36–38]:where is the maximum shear stress peak value and is the confining pressure; , where is the shear stress, is the axial stress, and is the tangential stress.

This test aims to investigate the influence of temperature on the dynamic characteristics of frozen clay with the rotation of the principal stress axis under different CSRs. The frequency was selected as 0.2 Hz during the cyclic loading test. This is because the frequency between 0.05 and 1 Hz has little effect on its dynamic characteristics [26]. Additionally, the internal pressure and external pressure were set at 2.5 MPa, and the test temperatures of −8, −10, −13, and −15°C were selected to study the dynamic characteristics of frozen soil undergoing the cryogenic process. Previous studies [16, 39] provided a reference to determine the amplitudes of cyclic shear stress which were chosen as 1.125 MPa, 1.5 MPa, 1.875 MPa, and 2.25 MPa corresponding to the CSRs of 0.225, 0.300, 0.375, and 0.45 in the experiments. The details of the testing plans are shown in Table 2. The initial static deviating stress and confining pressure were applied on the specimens to reach a stable stress condition for the dynamic test. Then, cyclic loading of axial stress and torque was carried out on frozen samples, where the representative loading waveforms and stress path are shown in Figure 4. During the test, a total of 50 points’ data were recorded for each loading cycle. The specimens were loaded to 250 cycles, or the axial strain reached the failure limit of 20%. The operating procedures of hollow cylinder torsional shear tests are shown in Figure 5.

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2.3. Determination of Resilient Modulus and Damping Ratio

During the test, a hysteresis loop can be obtained under cyclic loadings, as shown in Figure 6, from which the resilient modulus and the damping ratio can be derived. The secant modulus determined from the hysteresis loop is considered as the resilient modulus that can be calculated as follows:where is the maximum axial stress, is the minimum axial stress, is the maximum axial strain, and is the minimum axial strain.

The damping ratio is an important parameter to reflect the energy consumption of frozen clays under cyclic loadings; its formulation for frozen soil can be expressed as follows:where is the area of the hysteresis loop and is the area of the triangle.

3. Test Result and Discussion

3.1. Cumulative Plastic Strain

Figure 7 presents the evolution of the cumulative plastic strain versus the number of cycles under the different conditions of temperature and CSR. When CSR = 0.225, the cumulative plastic strain increases slightly with the increase of the number of cycles at low temperatures (−15°C and −13°C, as shown in Figure 7(a)), while the cumulative plastic strain increases rapidly as the number of cycles increases at the higher temperatures at −10°C and −8°C. Clearly, the cumulative plastic strain increases significantly as the temperature increases from T = −15°C to T = −8°C at the same number of cycles. For the cases of CSR = 0.300, 0.375, and 0.450 presented in Figures 7(b)–7(d), it is clear that the evolution of the cumulative plastic strain is similar to that of CSR = 0.225, but the value and rate of the cumulative plastic strain increase with the increasing of CSR. To further exhibit the effect of temperature on the cumulative plastic strain, the relationship between the final cumulative plastic strain () and temperature under four CSRs is plotted in Figure 8. In general, the final cumulative plastic strain exponentially increases with the increase of the temperature at a certain CSR. The greater CSR means a more significant growth rate. The results imply that the cyclic deformation behaviors of frozen soil are sensitive to temperature changes. There is static friction between solid particles and the cementing force between ice and soil in frozen soil [40–42]. The mechanism of frozen soils is different from that of unfrozen soil. The cementing force between ice and soil in frozen soil decreases with the increase of the temperature, decreasing the strength of the frozen specimens [43]. Therefore, the cumulative plastic strain increases sharply with the rising temperature at a given CSR. The effect of temperature seems to be more profound on cumulative plastic strain at a high CSR.

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3.2. Axial Resilient Modulus and Damping Ratio

Figure 9 depicts the evolution of representative axial stress strain versus the number of cycles at four temperatures as CSR = 0.375. As shown in Figure 9(a), the area of the hysteresis loop is large in the initial cycles, and, with the increase of number of cycles, the cumulative plastic strain and the area of the hysteresis loop decrease. In contrast, the slope of the hysteresis loop is small in the initial cycles, and, with the increase of the number of cycles, the slope of the hysteresis loop increases. The results show that as the number of cycles increases, the stiffness of frozen samples will be enhanced, while the recoverable strain and the amount of dissipated energy decrease with the increase of the number of cycles at high temperatures. Comparing Figures 9(a)–9(d) reveals that, at a lower temperature, the shape of the hysteresis loop changes slightly with the increase of the number of cycles. To further highlight the effect of temperatures on axial stress strain, the typical axial stress-strain hysteresis hoops at a different temperature under N = 50 and 200 are plotted in Figure 10. Clearly, when the temperature decreases, the plastic strain and the area of the hysteresis loop decrease sharply at the initial stage and then decrease slowly, while the slope of the hysteresis loop increases (see Figure 10). These results imply that the stiffness of frozen soil samples is enhanced with the decrease in temperature, while amount of energy dissipation decreases.

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Resilient modulus is a key parameter for engineering design and performance evaluation. Figure 11 depicts the evolution of the axial resilient modulus versus the number of cycles at different temperatures and CSRs. In Figures 11(a)–11(d), when CSR = 0.225 and T = −15°C, the resilient modulus rapidly decreases at the beginning of the loading stage and then fluctuates around a steady value as the loading cycles increase. For the case of CSR = 0.225 and T = −8°C, the resilient modulus decreases slightly at the beginning of the loading stage and then increases significantly as the loading cycles increase. Interestingly, the evolution characteristics of axial resilient modulus in this paper differ from those obtained in the cyclic triaxial test of frozen soil [16–19]. In this study, the axial resilient modulus decreases at the initial loading stage and then increases. That is because the inherent anisotropic structure in frozen soil is more significant, and the particles tend to rotate to support the rotation of principal stress during the first few cycles. Then, the frozen samples achieve stable structure after continuous orientation, realignment, and rearrangement [44–46]. Furthermore, Figures 11(a)–11(d) show that as the temperature increases from −15 to −8°C, the axial resilient modulus decreases significantly at a given number of cycles. Thus, the temperature has a significant impact on the variation of resilient modulus. The strength increases with the decrease of the temperature. Therefore, its stiffness and resilient modulus increase. However, the results from Ling et al. [14] show that the decrease of temperature has little influence on the stiffness of frozen soil between 0°C and −1.5°C. That may imply that the stiffness of frozen soil can be improved only when the temperature is lower than the freezing point.

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To better analyze the influence of temperature and CSR energy dissipation, Figure 12 illustrates the evolution of the axial damping ratio versus the number of cycles at different temperatures and CSRs. For the case of CSR = 0.225 and CSR = 0.300, as shown in Figures 12(a) and 12(b), on the whole, the damping ratio of specimens reduces gradually at the initial stage and subsequently reaches a relatively steady value. For the case of CSR = 0.375 and CSR = 0.450, as shown in Figures 12(c) and 12(d), when T = −15°C and −13°C, the damping ratio of specimens also decreases rapidly at the initial stage and then tends to stabilize as the number of cycles increases. The evolution of the damping ratio indicates that energy dissipation gradually decreases with increase of the number of cycles due to a more stable structure formation at lower temperatures [17]. When T = −10°C and −8°C, the damping ratio of specimens decreases at the initial stage and then increases gradually as the number of cycles increases. This is possible because the effect of torsional stress on the structural damage of frozen samples becomes more significant at a higher temperature and CSR, leading to the significant microfracturing phenomenon. Furthermore, it can be seen that the damping ratio of all specimens increases as the temperature rises. That is because the cementing force of ice decreases as the temperature rises. Thus, the strength of the specimens is reduced, and the obvious cumulative plastic strain occurs, increasing the energy dissipation.

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3.3. Torsional Resilient Modulus and Damping Ratio

To analyze the effect of temperature on the torsional stress-strain relationship, the representative torsional stress-strain responses with the number of cycles at four temperatures as CSR = 0.375 are shown in Figure 13. It can be found that hysteresis loops obtained from torsional stress strain move to the left, and the distance between the hysteresis loops decreases as the number of cycles increases. At the end of cyclic loading, the curves of hysteresis loops nearly overlap because the plastic strain gradually tends to stabilize. Moreover, the area of hysteresis loops decreases with increasing the number of cycles, while the hysteresis loops gradually lean toward to the torsional stress axial (vertical axial) with increase in the number of cycles. Figure 14 illustrates the representative torsional stress-strain responses at a given number of cycles and different temperatures. It can be observed that the hysteresis loops from torsional stress-strain responses move to the right, and the area of hysteresis loops increases as the temperature rises. Furthermore, the hysteresis loops gradually lean toward to the torsional axial strain (horizontal axial) as the temperature rises, which implies that the stiffness of frozen clay decreases with the increasing of the temperature. However, it should be noted that the stiffness and energy dissipation of frozen clay vary slightly as the temperature changes from −10°C to −8°C, showing that there may be a critical temperature for a given CSR. That needs further exploration in the future.

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The study on torsional resilient modulus of frozen soil has been relatively scarce until now. Figure 15 depicts the evolution of the torsional resilient modulus versus the number of cycles at different temperatures and CSRs. Figures 15(a)–15(d) show that the evolution laws of the torsional resilient modulus can be divided into three types at different temperatures. For the case of T = −15°C, the torsional resilient modulus decreases rapidly at the initial cyclic loading stage and then reaches a relatively steady value. In the case of T = −13°C and T = −10°C, it decreases slightly at the initial cyclic loading stage and then increases slightly with the increasing of the number of cycles. For the case of T = −8°C, it significantly increases with the increasing number of cycles, and its growth rate gradually reduces. Obviously, the evolution characteristics of torsional modulus versus number of cycles mostly depend on the changes in temperature. Furthermore, the results show that the evolution of the torsional shear modulus is similar to that of the axial resilient modulus. However, the value of the torsional shear modulus is smaller than that of the axial resilient modulus. The torsional shear modulus evolution rules of frozen samples are inconsistent with those derived from previous studies of unfrozen soil [28, 44]. The unfrozen soil specimen is softened by the accumulation of pore water pressure under cyclic loading. In contrast, the frozen soil sample is hardened under cyclic loading because of the cementation of ice [28, 44]. Besides, the temperature has a significant impact on the torsional resilient modulus. For specimens with low temperatures, the torsional resilient modulus is large. The comparison between axial resilient modulus and torsional resilient modulus (Figures 11 and 15) shows that the axial resilient modulus is about four times the torsional resilient modulus.

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Figure 16 depicts the evolution of the torsional damping ratio versus the number of cycles under different temperatures. The torsional damping ratio decreases rapidly at the beginning of the cyclic loading stage. After that, the decrease rate of the torsional damping ratio becomes slower than before, mainly because stress acting on specimens along the axial direction is higher than that along the torsional direction, causing the cyclic densification of samples and increasing torsional strength. Therefore, the torsional damping ratio gradually decreases with the increase of the number of cycles. However, the change of torsional damping ratio for the case of CSR = 0.375 and T = −10°C shown in Figure 16(c) is different from others, which may be due to the sample inhomogeneity. Additionally, the increase in temperature also promotes the torsional energy dissipation of the sample to increase, with the increasing of the torsional damping ratio. What is more, it could be seen from Figures 12 and 16 that the axial damping ratio is greater than the torsional damping ratio.

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4. Prediction Model of Axial Resilient Modulus

The resilient properties of soils have been extensively investigated by many researchers, and lots of empirical models were established to predict the resilient modulus under different conditions [42–46]. The most well-known and commonly used resilient modulus predicted models in existing literatures are presented in Table 3. Based on the existing empirical models for resilient modulus, it should be noted that the influences of shear stress and bulk stress are regularly considered, and few prediction models are expressed as a function with considering the temperature. Actually, a remarkable finding of this research is that the axial resilient modulus is uniquely related to temperature and CSR. Consequently, the introduction of CSR and temperature in frozen soil axial resilient modulus prediction model is helpful for mechanistic-empirical design of engineering for cold regions or artificial ground freezing projects.

The prediction model proposed by Fu and Dafalias [45] is widely used, as it not only takes 3D stress state into consideration but also overcomes problems of the undefined resilient modulus values when confining pressure and shear stresses approach 0. In this study, a prediction model of axial resilient modulus including (Equation (3)) the influences of CSR and temperature is proposed when confining pressure is held constant, based on the modified universal model established by Fu and Dafalias [45].where k1, k2, and k3 are regression coefficients, CSR is cyclic shear stress ratio, Tref is the reference temperature of −15°C, T is experimental temperature, and Pfa is the reference pressure of 100 MPa.

After that, to obtain the parameter of the modified prediction model, Equation (3) is applied to fit the mean values of axial resilient modulus determined by the mean value of axial resilient modulus in all 240 cycles. Because the experimental data of the average axial resilient modulus at −10°C are relatively scattered, where the data of −8°C, −13°C, and −15°C are used to fit the model parameters, a comparison of optimal fitting curves and measured average axial resilient modulus is shown in Figure 16, and the corresponding regression parameters and R2 for the axial resilient modulus prediction model are listed in Table 4. As shown in Figure 17 and Table 4, the fitting curves of the prediction model are relatively intimate to the measured data, indicating that the proposed model is feasible. However, it should be pointed out that some factors have not be taken in this prediction model, such as the confining pressure and frequency. Additionally, the modified model needs more experimental data to verify.

5. Conclusions

In this research, a series of FHCA tests were performed to investigate the effect of temperature on dynamic characteristics of frozen clay under complex stress path involving principal stress rotation. The evolutions of cumulative plastic strain, hysteresis loop, resilient modulus, and damping ratio were analyzed. Based on test results, the following main conclusions can be obtained from this study:(1)The temperature has a significant influence on the generalized cumulative plastic. The cumulative plastic strain rate is greater with the temperature increase, resulting in greater final cumulative plastic strain. The effect of temperature seems to be more profound with a high CSR.(2)Axial resilient modulus decreases at the initial stage and then increases with the increased number of cycles under different temperatures. The phenomenon of rearrangement on the particles and cyclic densification is obvious under principal stress rotation. As the number of cycles increases, axial damping ratio gradually decreases at low temperature and small CSR. However, due to the microfracturing phenomenon, the axial damping ratio first decreases and then increases at high temperatures and high CSRs. The high temperature leads to the small axial resilient modulus and large axial damping ratio.(3)The evolution characteristic of torsional resilient versus the number of cycles mostly depends on temperature. According to the different temperatures, the evolution of torsional resilient modulus can be classified into three categories: the torsional resilient modulus gradually decreases and tends to stabilize, the torsional resilient modulus decreases at the initial cycles and then gradually increases, and the torsional resilient modulus gradually increases and tends to stabilize. The torsional damping ratio decreases with the increase of the number of cycles. The high temperature results in the small torsional resilient modulus and large torsional damping ratio.(4)Based on the test results, an improved axial resilient modulus prediction model is established with considering the influences of cyclic shear stress ratios and temperatures. The new model has been proven to have high fitting accuracy through comparison with the measured values.

The above conclusions provide a better understanding of the long-term dynamic engineering geological characteristics of frozen clay under complex stress path involving principal stress rotation, which could potentially be used for engineering design and contribute to ensuring the service life of frozen soil infrastructures.

Data Availability

The experimental data used in this research are included within the paper.

Conflicts of Interest

The authors declare that they have no conflicts of interest or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgments

The authors appreciate the help of Zhi-Wei Zhou in revising the paper. The work presented in this paper was supported by the National Natural Science Foundation of China under Grants nos. 41671069 and 41871054. This ﬁnancial support is gratefully acknowledged.

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Copyright © 2021 Bin-Long Zhang et al. 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.

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