Research Article  Open Access
T. Yang, Q. S. Ye, "Elastoplastic Analysis of Circular Opening Based on a New StrainSoftening Constitutive Model and Its Engineering Application in Hydraulic Fracturing", Advances in Civil Engineering, vol. 2018, Article ID 2806489, 12 pages, 2018. https://doi.org/10.1155/2018/2806489
Elastoplastic Analysis of Circular Opening Based on a New StrainSoftening Constitutive Model and Its Engineering Application in Hydraulic Fracturing
Abstract
Constitutive effect is extremely important for the research of the mechanical behavior of surrounding rock in hydraulic fracturing engineering. In this paper, based on the triaxial test results, a new elasticpeak plasticsofteningfracture constitutive model (EPSFM) is proposed by considering the plastic bearing behavior of the rock mass. Then, the closedform solution of a circular opening is deduced with the nonassociated flow rule under the cavity expansion state. Meanwhile, the parameters of the loadbearing coefficient and brittles coefficient are introduced to describe the plastic bearing capacity and strainsoftening degrees of rock masses. When the above two parameters take different values, the new solution of EPSFM can be transformed into a series of traditional solutions obtained based on the elasticperfectly plastic model (EPM), elasticbrittle plastic model (EBM), elasticstrainsoftening model (ESM), and elasticpeak plasticbrittle plastic model (EPBM). Therefore, it can be applied to a wider range of rock masses. In addition, the correctness of the solution is validated by comparing with the traditional solutions. The effect of constitutive relation and parameters on the mechanical response of rock mass is also discussed in detail. The research results show that the fracture zone radii of circular opening presents the characteristic of EBM > EPBM > ESM > EPSFM; otherwise, it is on the contrast for the critical hydraulic pressure at the softeningfracture zone interface; the postpeak failure radii show a linear decrease with the increase of loadbearing coefficients or a nonlinear increase with the increasing brittleness coefficient. This study indicates that the rock mass with a certain plastic bearing capacity is more difficult to be cracked by hydraulic fracturing; the higher the strainsoftening degree of rock mass is, the easier it is to be cracked. From a practical point of view, it provides very important theoretical values for determining the fracture range of the borehole and providing a design value of the minimum pumping pressure in hydraulic fracturing engineering.
1. Introduction
The stresses and plastic zone distribution of the circular opening are extremely important for evaluating the tunnel stability and hydraulic fracturing effect in underground engineering. However, the mechanical response of the surrounding rock is closely related to rock mass lithology. In fact, the constitutive relation of different lithology rock masses generally shows obviously diversity and complexity under the effect of internal fissures, joints, components, and external environment. Therefore, it is difficult to choose a certain simplified constitutive equation to study this problem [1–4]. In the early stage, the elastoplastic analysis of the circular opening was firstly investigated by Fenner and then corrected by Kastner. However, they regarded the rock mass as the elasticperfectly plastic material (EPM). It is obviously not reasonable for the brittle plastic and strainsoftening rock masses. In recent years, as shown in Figure 1, many studies have been carried out by using the elasticbrittle plastic model (EBM), elasticstrainsoftening model (ESM), and elasticpeak plasticbrittle plastic model (EPBM) with the associated and nonassociated flow rule [5–9]. Nevertheless, each constitutive model has its own application scope. The EBM applies only to the poorquality rock mass, while ESM is suitable for averagequality rock mass and EPM for highquality rock mass [10–15]. In addition, EPBM is suitable for the brittle rock masses with a certain plastic bearing capacity [16–18]. In fact, many strainsoftening rock masses also show a certain plastic bearing behavior after load peak.
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As shown in Figure 2, the silty mudstone and marble were, respectively, taken from the Yangzhuang coal mine, Wushan, and Ya’an area of China. A large number of rock masses firstly showed the strainsoftening characteristics after the peak plastic zone and then entered the fracture stage. Therefore, according to the total stressstrain curve, the rock mass approximately experienced four stages in the process of the triaxial test. That is elastic, peak plastic, softening, and fracture stages. Then, the elasticpeak plasticsofteningfacture constitutive model (EPSFM) was proposed in this paper and then applied to the engineering practice.
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Most of the above investigations focus on the compression problems of the circular opening. However, the problems of cavity expansion have also attracted much attention in geotechnical engineering with the application to wellbore instability, coalgas exploration, and hydraulic fracturing [3, 4, 19, 20]. Actually, the circular opening expansion is mainly applied in the hydraulic fracturing, which has been widely used in the hard roof fracturing, coalbed methane extraction, and in situ stress measurement.
Since the early 1950s, numerous analytical solutions to the circular opening expansion have been studied in materials and geotechnical engineering. For instance, Gibson and Anderson applied the cavity expansion theory to in situ measurement of soil properties with the pressure meter test [19]. Li et al. obtained the closedform solution for the hydraulic fracturing borehole, which was only applied to hard rock, depending on the elastic fracture theory [20]. Bishop and Mott derived the quasistatic expansion equations of cylindrical cavities in an infinite medium and applied it to the materials processing [21]. Cheng discussed the errors arising from the assumption of small displacement around the cavity with no volume change in the plastic zone and modified Kastner’s formula for cylindrical cavity contraction and expansion in the Mohr–Coulomb rock masses [22]. Li et al. derived the stresses and plastic zone radii of the circular borehole excavated in the strainsoftening coal seam by considering contraction and expansion problems [23].
In this paper, based on the triaxial test results, a new elasticpeak plasticsofteningfracture constitutive model (EPSFM) is firstly proposed and then used to study the borehole expansion problems in underground engineering. Furthermore, the validity of this solution is verified by comparing with a series of traditional solutions based on EBM, EPM, ESM, and EPBM. Finally, the influences of the parameters and constitutive models on the mechanic responses of rock mass are discussed in detail.
2. Problem Description
2.1. Establishment of EPSFM
As shown in Figure 3, a borehole with the inner radius drilled in an infinite, isotropic, and homogeneous EPSFM rock masses is subjected to an inner hydraulic pressure at and hydrostatic pressure at infinite boundary. Originally, the surrounding rock is in the elastic state. As gradually increase, the peak plastic firstly occurs around the borehole when is more than the initial yield stresses. The stage is not an infinite extension whose range should be restricted by some factors. In this paper, assuming the plastic shear strain increment of the peak plastic zone reaches a certain value, the surrounding rock of the borehole will enter the softening stage in which the strength parameters gradually decrease. Until a residual value is reached, the surrounding rocks start to enter the fracture stage. Finally, it will have four zones around the borehole that is elastic zone, peak plastic zone, softening zone, and fracture zone. Meanwhile, the radius of peak plastic, softening, and fracture zones are, respectively, denoted as , , and . The mechanical model should satisfy the following assumption conditions:(i)The borehole is drilled in an infinite geological body, so the problem can be regarded as a plane strain problem(ii)The total strain of the postpeak failure zone only consists of plastic strain and the effect of elastic strain is ignored
For axisymmetric plane strain problems, when , the hoop stress and radial stress are, respectively, the minimum and maximum principal stresses; and are the minimum and maximum principal strains, respectively [20, 21]. Supposing that the rock mass satisfies the linear Mohr–Coulomb yield criteria, the stressstrain relation at any postpeak stages can be expressed as follows [22, 23]:where and are, respectively, the initial uniaxial compressive strength and residual compressive strength, , ; and are, respectively, initial and residual cohesion of rock mass; and is a constant which is related to the strength parameter , .
2.2. Basic Equations and Boundary Condition
For the axisymmetric plane strain problems, the equilibrium differential equation in the “” zone can be expressed as follows (ignoring the body force) [7, 9]:where and are the radial and hoop stresses in the “” zone, respectively. The subscript symbol “” represents different zones of surrounding rock, which can be replaced by the numbers “0, 1, 2, and 3.”
Based on the supposition of small deformation, the geometric equation for the axisymmetric plane strain problem can be denoted as [12, 13]where and are the radial and hoop strains in the “” zone, respectively, and represents the radial displacement.
Supposing that the volume of rock mass is changing, the relationship between hoop strain and radial strain can be established by adopting a nonassociated flow rule and small strain theory as follows [22, 23]:where and is the dilatancy angle.
Both the radial stress and radial displacement should be continuous at the elasticpeak plastic, peak plasticsoftening, and softeningfracture zone interfaces. Therefore, the boundary conditions around the borehole can be summarized as
3. ClosedForm Solution of EPSFM
3.1. Stresses and Displacement of Elastic Zone
Based on the elasticity theory, the solution of a thickwalled cylinder under hydrostatic pressure can be easily obtained. The stresses and displacement for the elastic zone can be expressed as [18, 23]where is the minimum critical inner hydraulic pressure at elasticpeak plastic zone interface; ; and and are Young’s modulus and Poisson’s ratio.
For the borehole expansion problem, both radial and circumferential stresses satisfy the Mohr–Coulomb yield criteria at the elasticpeak plastic zone interface. Hence, the parameters can be easily deduced by substituting equations (8) and (9) into equation (1) as follows:
Considering the boundary condition by equation (7), the radial displacement and strains in the postpeak failure zones can be easily deduced based on the small deformation supposition and volume expansion assumption by substituting equation (5) into equation (6). The calculation results are shown in Table 1.

3.2. Stresses Distribution of Peak Plastic and Fracture Zones
When the inner hydraulic pressure remains at a certain value, the surrounding rock of the borehole is in the stress equilibrium state in the peak plastic and fracture zones. Therefore, the principal stresses should satisfy the equations (1) and (4) in the peak plastic zone or equations (3) and (4) in the fracture zone.
In the above two zones, the equilibrium differential equation can be rewritten by substituting equation (1) or equation (3) into equation (4) as follows:where equals to in the peak plastic zone or equals to in the fracture zone.
Solving equation (12), the stresses in the peak plastic zone can be obtained by combining with the boundary condition :
Meanwhile, the stresses in the fracture zone can be also easily deduced by considering :
3.3. Stresses Distribution of Softening Zone
By considering the condition at and , the compressive strength in the softening zone can be obtained aswhere , which can be defined as a brittleness coefficient and represents the strainsoftening degree of rock mass and may be called the strainsoftening modulus.
Introducing equations (2) and (15) into equation (4), the equilibrium differential equation in the softening zone can be deduced as
The radial stress at the peak plasticsoftening interface must be coincided; thus it can be obtained by solving equation (16) and considering the boundary condition at :
Then, by introducing equations (15) and (17) into equation (2), the hoop stress is
3.4. Radius (, , ) of Postpeak Failure Zones
As the inner hydraulic pressure gradually increasing, the surrounding rock of the borehole will experience four stages. That is elastic stage, elasticpeak plastic stage, elasticpeak plasticsoftening stage, and elasticpeak plasticsofteningfracture stage.
3.4.1. ElasticPeak Plastic Stage
In this stage, the surrounding rock of the borehole only consists of elastic and peak plastic zones. The range of the peak plastic zone gradually increases with the increase of the inner hydraulic pressure. As shown in Figure 3, when the plastic shear strain increment of the peak plastic zone increases to a particular value, the rock mass will reach the maximum peak plastic state in which the softening zone is just not arisen. Hence, we can define a loadbearing coefficient which can be calculated by the difference of the plastic shear strain in section “AB” of Figure 3 to describe the plastic bearing capacity of rock mass. The parameter can be expressed as follows:where and represent the plastic shear strain at points “B” and “A,” respectively. They can easily be determined by the experiment. Hence, the radius of the peak plastic zone can be obtained as
Presently, the middle critical inner hydraulic pressure at the peak plasticsoftening zone interface can be solved by introducing equation (20) into equation (13):
3.4.2. ElasticPeak PlasticSoftening Stage
When , the softening zone appears. If assuming that the surrounding rock is in the critical state where the fracture zone is not yet arisen, equation (20) can be rewritten as
By integrating equation (15), according to at , the relationship between and can be obtained as follows:
Then, by substituting equation (22) into equation (23), the softening zone radii can be expressed as
At this state, introducing equations (22) and (24) into equation (17), the maximum critical inner hydraulic pressure can be calculated as follows:
3.4.3. ElasticPeak PlasticSofteningFracture Stage
When , it means that the rock mass has entered into the fracture stage. According to equations (22) and (24), the relationship of is easily deduced. In addition, the radial stress should be consistent at the softeningfracture zone interface. Therefore, we can obtain
Integrating equation (26), the fracture zone radius can be obtained as follows:
Then, the radius of peak plastic and softening zones can also be calculated by introducing equation (27) into .
3.5. Discussion and Transformation with Traditional Model
The new closedform solution based on the EPSFM can be degenerated for different traditional solutions based on the EPM, EBM, ESM, and EPBM in a particular situation. For instance, only when , the results of EPSFM can be translated into the results of ESM [23]; when , , the EPSFM converts to the EBM; if assuming that and , the EPSFM solution degenerates for EPM solution [22]; only when , the EPSFM solution changes to the EPBM solution. It includes not only the traditional results but also a series of new results compared with the traditional ones. Hence, it can be regarded as a unified analytical solution. In other words, the new closedform solution can generate a broad range of theoretical and practical values in circular opening expansion engineering, especially in the hydraulic fracturing.
When loadbearing coefficient and brittleness coefficient take special values, the new analytical solution will degenerate for a series of traditional solutions. It mainly includes four different cases.
Case 1. When and , the peak plastic zone will disappear, and then the EPSFM degenerates into the elasticstrainsoftening model.
In this state, the softening and fracture zones radius can be obtained by solving equation (27):When , equations (28) and (29) are the solutions obtained by Li et al. [23] for the circular opening expansion.
Then, integrating equation (25), the maximum critical inner hydraulic pressure at can be rewritten as follows:
Case 2. When , , , and , the EPSFM converts to the elasticbrittle plastic model. The stress at the elasticfracture zone interface presents instantaneous dropping characteristics. However, the radius of the fracture zone cannot be given directly. The fracture zone radius can be deduced by considering the boundary condition as follows:
Case 3. When and , the softening zone will disappear. Thus, the EPSFM degenerates into the elasticpeak plasticbrittle plastic model. Meanwhile, the maximum principal stress between peak plastic and fracture zones shows obvious drop characteristics. In this state, the radius of peak plastic and fracture zones can be deduced by integrating equations (22) and (27):
Case 4. When , , , and , the surrounding rock is only composed of the elastic and peak plastic zones. Therefore, the EPSFM becomes the elasticperfectly plastic model. The radius of the peak plastic zone can also be deduced by considering the boundary condition :The analytical solution of equation (33) is the same with reference results (Cheng [22]).
4. Case Studies
4.1. Case I: Comparative Analysis
Constitutive effect is extremely important for researching the mechanics and deformation behavior of rock mass. To validate the developed model in this paper and study the influence of constitutive relation on the mechanics response of the rock mass, the geometrical and physical parameters of a circular opening are shown in Table 2. Moreover, the loadbearing coefficient is assumed as 0.004.

The circular opening expansion theory is mainly applied to hydraulic fracturing in underground engineering. The stresses distribution law under different constitutive models is shown in Figure 4. In addition, Table 3 presents the maximum inner hydraulic pressure at the softeningfracture zone interface. It can be seen from Figure 4 and Table 3 that the maximum critical pressure shows the characteristics of EBM < EPBM < ESM < EPSFM. By comparing with the EBM, EPBM, and ESM rock masses, the maximum critical pressure of EPSFM increases by 9.895 MPa, 7.752 MPa, and 1.286 MPa, respectively. It means that the EPSFM rock mass is the hardest to be cracked, whereas the EBM rock mass is the easiest in the process of hydraulic fracturing.
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The influence of constitutive relation on the postpeak failure radii is shown in Figure 5. When the inner hydraulic pressure is equal to 40 MPa, the radii of show the characteristics of EBM > EPBM > ESM > EPSFM. Therefore, the above results indicate that the rock mass with a certain plastic bearing capacity is more difficult to be cracked in hydraulic fracturing engineering. In other words, the design of hydraulic fracturing pressure should take full account of the influence of lithology to achieve the best crack effect.
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4.2. Case II: Parameter Analysis
A case of hydraulic fracturing in coal seam is used to study the mechanical response of rock masses with the change of hydraulic pressure. The influence of parameters on the surrounding rock state is also discussed. The hydraulic fracturing case was implemented in No. 7601 coal seam with high gas in Wuyang Coal Mine of China for improved gas extraction. The coalbed was buried at about 480 m underground. The average value of hydrostatic pressure is 7.16 MPa; the radius of the borehole is 0.1 m; Young’s modulus and Poisson’s ratio are 3.0 GPa and 0.28, respectively; the initial cohesion and the internal friction angle are 1.5 MPa and 30°; and and are, respectively, about 5.2 MPa and 1.2 MPa. Moreover, the loadbearing coefficient and brittleness coefficient are 0.0006 and 1.2, respectively. It should be noted that the influence of the dilatancy coefficient is ignored () in order to avoid the errors arising from the volume change of postpeak rock mass.
4.2.1. Stresses and Postpeak Failure Radii Evolution Law
Figure 6 shows the stress evolution law with the change of the critical hydraulic pressure. In the present example, it can be seen that there is only elastic zone around the borehole when (Figure 6(a)). There are elastic and peak plastic zones when (Figure 6(b)). Then, the surrounding rock of the borehole is composed of elastic, peak plastic, and softening zones if (Figure 6(c)). Finally, the surrounding rock consists of four zones if (Figure 6(d)). In addition, is commonly found in Figure 6 for the borehole expansion.
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The radius of the postpeak failure zone is also significantly important for evaluating the hydraulic fracturing effect and optimizing the layout of the boreholes. The radius of the peak plastic, softening, and fracture zones evolution law under different hydraulic pressures are shown in Figure 7. It is clear that there is no postpeak failure zone when . The radius gradually increases with the increasing of the hydraulic pressure in the range for the circular opening expansion. Figure 7 is of great practical significance because the threshold of the critical hydraulic pressure has an important theoretical value for providing a design value of the minimum pumping pressure compared with the traditional empiricism [23]. In this case, the threshold of calculation is 14.917 MPa and is in good accordance with the field test results (14.54 MPa).
4.2.2. Influence of LoadBearing Coefficient
The loadbearing coefficient reflects the plastic bearing capacity of rock mass and is extremely important for determining the fracture range and the critical hydraulic pressure in the process of hydraulic fracturing. The radii of the postpeak failure zone evolution law are shown in Figure 8. It can be seen that the postpeak failure radii obviously decrease with the increase of the loadbearing coefficient. However, the decreasing rate of softening zone radii is the maximum. For instance, when transforms from to , the radii , , and , respectively, decrease by 15.8 mm, 25.9 mm, and 1.8 mm. It means that the greater the is, the stronger the plastic bearing capacity of the rock mass and the smaller the fracture range of the drill hole are. Here, the inner hydraulic pressure is set at 20 MPa (>15.986 MPa) (Table 4) in order to make the rock mass enter the residual state.

In addition, the loadbearing coefficient also has a very important effect on the critical hydraulic pressure. As shown in Table 4, and , respectively, decrease by 1.987 MPa and 1.525 MPa with the loadbearing coefficient decreasing from to . The conclusion can provide exceedingly important reference for determining the threshold of maximum critical hydraulic pressure in hydraulic fracturing engineering.
4.2.3. Influence of Brittleness Coefficient
Figure 9 shows the influence of brittleness coefficients () on the postpeak failure radii. With the parameter () increasing, the postpeak failure radii show a nonlinear increase characteristic. However, the increase rate is gradually decreasing. For instance, when changes from 0.6 to 2, the radii , , and , respectively, increase by 35.6 mm, 6.7 mm, and 7.2 mm. In addition, as shown in Table 5, the maximum critical hydraulic pressure is negatively correlated with the brittleness coefficient (). The above result shows that the higher the strainsoftening degree of rock mass is, the easier it is to be cracked by hydraulic fracturing.

5. Conclusions
Based on the triaxial test results, a new elasticpeak plasticsofteningfracture constitutive model (EPSFM) is proposed by considering the plastic bearing behavior of the silty mudstone. Then, the closedform solution of a circular opening based on the new proposed constitutive model is deduced with the nonassociated flow rule under the cavity expansion state. The correctness of the solution is also verified by comparing with the traditional solutions. The effect of the constitutive relation and parameters on the mechanical response of rock mass is also discussed in detail. The primary conclusions can be summarized as follows:(1)The new closedform solution based on EPSFM, considering the effect of plastic bearing capacity of rock masses, can be regarded as a uniform solution compared with the traditional research results. Only when the loadbearing coefficient is equal to zero, the calculated results of the EPSFM can be converted to the ESM’s solution; only when the brittleness coefficient is large enough or zero, the EPSFM’s solution turned to the result by EPBM or EPM. Meanwhile, when the loadbearing coefficient is zero and the brittleness coefficient is large enough, the calculated results of the EPSFM was found to be in accordance with the closedform solution of the EBM.(2)In hydraulic fracturing engineering, when the hydraulic pressure remains at a certain values, the fracture zone radii of circular opening present the characteristic of EBM > EPBM > ESM > EPSFM; otherwise, it is on the contrast for the critical hydraulic pressure at the softeningfracture zone interface. Therefore, the EPSFM rock mass is hardest to be cracked, whereas the EBM rock mass is easiest in the process of hydraulic fracturing.(3)The postpeak failure radii show obviously a linear decrease with the increase of loadbearing coefficients or a nonlinear increase with the increasing brittleness coefficient. It means that, for the best fracturing effects, the design of hydraulic fracturing pressure should take full account of the influence of rock mass lithology, loadbearing coefficient, and brittleness coefficient.
Data Availability
The article data used to support the findings of this study are included within the article.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
Acknowledgments
The authors would like to thank the financial support from the National Natural Science Foundation for Young Scientists of China (51604116), State Key Laboratory of Coal Resources and Safe Mining (China University of Mining and Technology) (SKLCRSM16KFB10), Fundamental Research Funds for the Central Universities (3142018028), Natural Science Foundation of Hebei Province (E2016508036), and State Key Laboratory Cultivation Base for Gas Geology and Gas Control (Henan Polytechnic University) (WS2017B07).
References
 L. Placidi and E. Barchiesi, “Energy approach to brittle fracture in straingradient modelling,” Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences, vol. 474, no. 2212, Article ID 20170878, 2018. View at: Publisher Site  Google Scholar
 A. H. Wilson, “A method of estimating the closure and strength of lining required in drivages surrounded by a yield zone,” International Journal of Rock Mechanics and Mining Sciences and Geomechanics Abstracts, vol. 17, no. 6, pp. 349–355, 1980. View at: Publisher Site  Google Scholar
 Y. J. Ning, J. Yang, and P. W. Chen, “Numerical simulation of rock blasting in jointed rock mass by DDA method,” Rock & Soil Mechanics, vol. 31, no. 7, pp. 2259–2263, 2010. View at: Google Scholar
 J. F. Zou, W. Q. Tong, and J. Zhao, “Energy dissipation of cavity expansion based on generalized nonlinear failure criterion under high stresses,” Journal of Central South University, vol. 19, no. 5, pp. 1419–1424, 2012. View at: Publisher Site  Google Scholar
 H. Zhang, Z. Wan, D. Ma, Y. Zhang, J. Cheng, and Q. Zhang, “Experimental investigation on the strength and failure behavior of coal and synthetic materials under planestrain biaxial compression,” Energies, vol. 10, no. 4, p. 500, 2017. View at: Publisher Site  Google Scholar
 E. Hoek and E. T. Brown, “Practical estimates of rock mass strength,” International Journal of Rock Mechanics and Mining Science & Geomechanics Abstracts, vol. 34, no. 8, pp. 1165–1186, 1997. View at: Publisher Site  Google Scholar
 K. H. Park, B. Tontavanich, and J. G. Lee, “A simple procedure for ground response curve of circular tunnel in elasticstrain softening rock masses,” Tunnelling and Underground Space Technology, vol. 23, no. 2, pp. 151–159, 2008. View at: Publisher Site  Google Scholar
 Y. K. Lee and S. Pietruszczak, “A new numerical procedure for elastoplastic analysis of a circular opening excavated in a strainsoftening rock mass,” Tunnelling and Underground Space Technology, vol. 23, no. 5, pp. 588–599, 2008. View at: Publisher Site  Google Scholar
 Q. Zhang, B. S. Jiang, S. L. Wang, X. R. Ge, and H. Q. Zhang, “Elastoplastic analysis of a circular opening in strainsoftening rock mass,” International Journal of Rock Mechanics and Mining Sciences, vol. 50, no. 1, pp. 38–46, 2012b. View at: Publisher Site  Google Scholar
 S. L. Wang, H. Zheng, C. G. Li, and X. R. Ge, “A finite element implementation of strainsoftening rock mass,” International Journal of Rock Mechanics and Mining Sciences, vol. 48, no. 1, pp. 67–76, 2011. View at: Publisher Site  Google Scholar
 S. K. Sharan, “Exact and approximate solutions for displacements around circular openings in elasticbrittleplastic HoekBrown rock,” International Journal of Rock Mechanics and Mining Sciences, vol. 42, no. 4, pp. 542–549, 2005. View at: Publisher Site  Google Scholar
 K. H. Park and Y. J. Kim, “Analytical solution for a circular opening in an elasticbrittleplastic rock,” International Journal of Rock Mechanics and Mining Sciences, vol. 43, no. 4, pp. 616–622, 2006. View at: Publisher Site  Google Scholar
 Q. Zhang, B. S. Jiang, X. S. Wu, H. Q. Zhang, and L. J. Han, “Elastoplastic coupling analysis of circular openings in elastobrittleplastic rock mass,” Theoretical and Applied Fracture Mechanics, vol. 60, no. 1, pp. 60–67, 2012a. View at: Publisher Site  Google Scholar
 S. L. Wang, X. T. Yin, H. Tang, and X. Ge, “A new approach for analyzing circular tunnel in strainsoftening rock masses,” International Journal of Rock Mechanics and Mining Sciences, vol. 47, no. 1, pp. 170–178, 2010. View at: Publisher Site  Google Scholar
 Q. Zhang, B. S. Jiang, and H. J. Lv, “Analytical solution for a circular opening in a rock mass obeying a threestage stressstrain curve,” International Journal of Rock Mechanics and Mining Sciences, vol. 86, pp. 16–22, 2016. View at: Publisher Site  Google Scholar
 B. S. Jiang, Q. Zhang, Y. N. He et al., “Elastioplastic analysis of cracked surrounding rocks in deep circular openings,” Chinese Journal of Rock Mechanics and Engineering, vol. 26, no. 5, pp. 982–986, 2007, in Chinese. View at: Google Scholar
 M. H. Yu, S. Y. Yang, S. C. Fan, and G. W. Ma, “Unified elastoplastic associated and nonassociated constitutive model and its engineering applications,” Computers and Structures, vol. 71, no. 6, pp. 627–636, 1999. View at: Publisher Site  Google Scholar
 C. G. Zhang, J. F. Wang, and J. H. Zhao, “Unified solutions for stresses and displacements around circular tunnels using the unified strength theory,” Science China Technological Sciences, vol. 53, no. 6, pp. 1694–1699, 2010. View at: Publisher Site  Google Scholar
 R. E. Gibson and W. F. Anderson, “Insitu measurement of soil properties with the pressuremeter,” Civil Engineering and Public Works Review, vol. 56, pp. 615–618, 1961. View at: Google Scholar
 Y. Li, N. Fantuzzi, and N. Tornabene, “On mixed mode crack initiation and direction in shafts: strain energy density factor and maximum tangential stress criteria,” Engineering Fracture Mechanics, vol. 109, no. 1, pp. 273–289, 2013. View at: Publisher Site  Google Scholar
 R. F. Bishop and N. F. Mott, “The theory of indentation and hardness,” Proceedings of the Physical Society, vol. 57, no. 3, pp. 147–159, 1945. View at: Publisher Site  Google Scholar
 Y. M. Cheng, “Modified Kastner formula for cylindrical cavity contraction in MohrCoulomb medium for circular tunnel in isotropic medium,” Journal of Mechanics, vol. 28, no. 1, pp. 163–169, 2012. View at: Publisher Site  Google Scholar
 Y. Li, S. G. Cao, F. Nicholas, and Y. Liu, “Elastoplastic analysis of a circular borehole in elasticstrain softening coal seams,” International Journal of Rock Mechanics and Mining Sciences, vol. 80, pp. 316–324, 2015. View at: Publisher Site  Google Scholar
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Copyright © 2018 T. Yang and Q. S. Ye. 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.