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Article

Effects of Weak Structural Planes on Roadway Deformation Failure in Coastal Mines

1
State Key Laboratory of Lithospheric and Environmental Coevolution, Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing 100029, China
2
Institutions of Earth Science, Chinese Academy of Sciences, Beijing 100029, China
*
Author to whom correspondence should be addressed.
Water 2025, 17(15), 2257; https://doi.org/10.3390/w17152257
Submission received: 1 July 2025 / Revised: 26 July 2025 / Accepted: 27 July 2025 / Published: 29 July 2025

Abstract

Roadway deformation failure is often related to the presence of weak structural planes (WSPs) in the surrounding rock mass. Especially in coastal mining environments, WSP-induced deformation can create pathways that connect faults with seawater, accelerating groundwater seepage and inrush hazards. This study employs an optimized Finite–Discrete Element Method (Y-Mat) to simulate WSP-driven fracture evolution, introducing an elastoplastic failure criterion and enhanced contact force calculations. The results show that the farther the WSP is from the roadway, the lower its influence; its existence alters the shape of the plastic zone by lengthening the failure zone along the fault direction, while its angle changes the shape and location of the failure zone and deflects fracture directions, with the surrounding rock between the roadway and WSP suffering the most severe failure. The deformation failure of roadway surrounding rock is influenced by WSPs. Excavation unloading reduces the normal stress and shear strength in the weak structural plane of surrounding rock, resulting in slip and deformation. Additionally, WSP-induced fractures act as groundwater influx conduits, especially in fault-proximal roadways or where crack angles align with hydraulic gradients, so mitigation in water-rich mining environments should prioritize sealing these pathways. The results provide a theoretical basis for roadway excavation and support engineering under the influence of WSPs.

1. Introduction

In mining engineering, roadways are necessary for transporting materials, ores, and workers, so their stability is critical for security and sustainable production [1,2]. Geological rock mass always contains different types of weak structural planes (WSPs) such as faults, cracks, and joints, and the existence of these structural planes destroys the integrity of the rock mass and greatly damages its stability [3,4,5,6]. With the increase in mining depth, increasingly complex engineering geological environments will be faced for resource exploitation, so the effect of WSPs on deformation failure in deep roadways needs to be further explored. Moreover, in coastal mines, deformation along WSPs may hydraulically connect fault networks with overlying aquifers or seawater, posing catastrophic water-inrush risks. Quantifying WSP-controlled failure zones is thus critical for predicting preferential flow paths.
In recent years, rock mechanics has made unprecedented progress in numerical simulation methods, and various new methods and models have emerged [7,8]. Due to their low cost and repeatability, these methods have become increasingly significant in solving practical engineering issues [9,10,11]. Currently, numerical investigations into the mining-induced deformation failure of surrounding rock employ various simulation software, such as PFC (Particle Flow Code), UDEC (Universal Distinct Element Code), RFPA (Rock Failure Process Analysis), and FLAC (Fast Lagrangian Analysis of Continua). These tools are based on methods such as DEM (Discrete Element Method) and FEM (Finite Element Method) [12,13,14]. Bahaaddini et al. used PFC to simulate the deformation and instability process of joint surrounding rock, and compared the results with previous physical tests, proving that PFC can accurately simulate the mechanical characteristics and instability mechanisms of discontinuous jointed rock mass [15,16,17,18]. Based on RFPA, Tang et al. conducted numerical analysis on the deformation and nonlinear progressive failure characteristics of a circular roadway in deep rock mass, and studied the displacement and acoustic emission characteristics of the roadway under mining stress [19,20,21,22,23]. Shen et al. used UDEC to build a model of rocks containing two sets of vertical joints. By changing parameters such as joint spacing, boundary conditions, ground stress, and joint direction, the influence radius on the unloading zone of tunnel excavation was explored [24]. Through an open source DEM code ESyS-Particle, Yan et al. studied the significant influence of joint geometry on the mechanical properties and failure behavior of rock models with discontinuous joints under uniaxial compression, revealing the microscopic energy evolution characteristics and progressive failure behavior of rock models with multi-joints under uniaxial compression [25,26,27].
Based on previous research, this study proposes an FDEM (Finite–Discrete Element Method) by enhancing a contact force calculation method, introducing slip rate parameters, and incorporating an elastic–plastic failure criterion. Consequently, an improved algorithm suite is proposed, and a corresponding program named Y-Mat is developed using Matlab. Then, the deformation failure of roadway surrounding rock under the influence of WSPs is simulated and analyzed based on the program. Finally, the control effects of structural plane distance and dip angle on roadway deformation failure are explored, providing a reference for the stability analysis of roadways under the influence of WSPs.

2. Background

Sanshandao Gold Mine, located in Laizhou City, Yantai, Shandong Province, China, is the only remaining operational undersea mine in the country (Figure 1a) [28]. The geographical coordinates of the mining area lie between 37°24′01″ N and 37°24′44″ N, and between 119°56′54″ E and 119°57′20″ E. Situated on the coastal plain along the southern coast of the Bohai Sea, the region is surrounded by the sea to the north, west, and south, with land to the east. The mining area has a low-lying and relatively flat terrain, with an elevation ranging from 1.2 to 6 m above sea level, and features a continental climate in the northern warm temperate monsoon zone. Its surface water systems are well-developed: two seasonal rivers, the Wang River and the Zhuqiao River, traverse the entire study area. Both rivers are short in length, close to their sources, and have shallow water levels during autumn and winter (Figure 1b).
The area is characterized by well-developed brittle fracture structures, with primary strikes in the northeast and northwest directions, forming the basic structural framework of the region. The northeast-trending fracture structures are represented by the Sanshandao fault zone (F1), which is the most developed first-order fracture structure in the area (Figure 1c). This fault zone controls a series of large and super-large gold deposits, including those in Sanshandao, Cangshang, Xinli, Xiling, and the northern sea area of Sanshandao. In this region, the ore deposits are generally distributed below the main fracture surface (Figure 1d).
As a common WSP in underground engineering, faults are a decisive factor controlling the deformation and stability of surrounding rock, which has a great influence on the characteristics of stress and displacement distribution. In the field investigation, it was found that when the roadway axis was parallel to the fault strike or intersected at a small angle and the roadway did not cross the fault zone, and the deformation and failure of the roadway were asymmetrical [29]. Figure 2 shows two roadways affected by faults. In Figure 2a, the roadway was 220 m away from the fault. Concrete spraying was extruded from the south and west side, and the floor heave was obvious, with a variation of 6 cm in the first month. The roadway in Figure 1b was 70 m away from the fault. It can be seen that the side wall was squeezed, and there was water seeping out. The variation in the roadway in the first month reached 23 cm, and the average daily variation was close to 1 cm [28,29].
Under excavation conditions, the roadway was biased when it was close to the fault. The side of the roadway close to the fault was more seriously damaged than the side far away from the fault. Moreover, when the roadway was close to the fault, the deformation of the surrounding rock was not only large but also occurred rapidly. The excavation destroyed the balanced state of the WSP, reduced the positive pressure of the plane, and decreased the shear strength. Under certain conditions, fault slip activation can be induced, posing a greater threat to the safety of roadway use. Therefore, the effect of WSPs on roadway deformation failure needs to be further explored.

3. Methodology

3.1. Y-Mat Program

The Finite–Discrete Element Method (FDEM), initially proposed by Munjiza et al., exhibits limitations in computational efficiency and the characterization of mechanical behaviors of rock [30,31]. Hence, a Y-Mat program is proposed in this study to address these shortcomings.
  • According to the contact force algorithm based on the penalty function originally proposed by Munjiza, the contact force is calculated according to the length of the invading edge and the potential of the center of the invading part, which simplifies the calculation process and greatly improves the calculation efficiency [32].
  • Referring to the definition of static and dynamic loading in the laboratory, the concept of slip change rate in numerical simulation is proposed, and a calculation method for the contact tangential force considering static and dynamic friction and their mutual conversion is introduced [33,34].
  • Combined with the elastoplastic deformation of rock mass, and referring to the relevant theories in FLAC, the Mohr–Coulomb constitutive model and the maximum tensile stress criterion are introduced to correct the deformation force of the element after yield [35].
Details regarding the specific optimization principles of the Y-Mat program are available in Reference [36].

3.2. Numerical Model

To verify the feasibility of the program in the tunnel excavation simulation, a numerical calculation model was established, as shown in Figure 3. The size of the model was 40 m × 40 m, and the roadway was located at the center of the model with a radius of 2 m. The monitoring zones recorded the stress evolution process of the elements in the area. The physical and mechanical parameters measured in Sanshandao Gold Mine were adopted for the model unit, and the numerical model parameters used are shown in Table 1 [28,29,36]. The boundary conditions of the model were as follows: both sides limited the displacement in the horizontal direction, and the top and bottom boundaries limited the displacement in the vertical direction.

3.3. Verification of Model Reliability

The theoretical solution of the rock mechanics of secondary stress in the elastic zone of a circular roadway is as follows:
σ r = 1 2 ( p x + p y ) ( 1 r 2 x 2 ) + 1 2 ( p x p y ) ( 1 4 r 2 x 2 + 3 r 4 x 4 ) cos 2 φ σ φ = 1 2 ( p x + p y ) ( 1 + r 2 x 2 ) 1 2 ( p x p y ) ( 1 + 3 r 4 x 4 ) cos 2 φ
where σr is radial stress; σφ is tangential stress; px is horizontal geostress; py is vertical geostress; φ is the angle between the line passing through the point and the center of the circle and the horizontal direction; x is the distance from the point to the circle center; and r is the radius.
According to Formula (1), the radial stress on the top and right sides of the roadway is 0, and the tangential stresses are 3 × (pxpy) and 3 × (pypx), respectively. The boundary conditions, with a horizontal ground stress of 2 MPa and a vertical stress of 1 MPa, were entered into the formula and numerical model, respectively, and stress curves of the surrounding rock were drawn from the calculated results, as shown in Figure 4.
The stress distribution curves demonstrate close alignment between the simulated and analytical results in the elastic zone, where both radial and tangential stresses follow theoretical predictions. Beyond the elastic limit, plastic behavior manifests as irregular stress fluctuations. Notably, stresses converge to far-field values at sufficient distance from the roadway, validating the optimized program’s physical realism. Quantitative analysis confirms the analytical solutions achieve exceptional accuracy (≤3% relative error, maximum deviation 2.5%) and precision (standard deviation <0.08 MPa, R2 ≈ 0.994) when benchmarked against numerical results. This agreement establishes the reliability of the Y-Mat model.

3.4. Scheme Design

To investigate the impact of the distance and angle of WSPs on roadway deformation failure, 8 simulation tests were designed, as shown in Figure 5. The first 4 schemes studied the influence of the distance between the WSP and the center point of the roadway, with distances of 2 m, 4 m, 6 m, and 8 m. The last 4 schemes studied the influence of the WSP angle, with angles of 0°, 30°, 60°, and 90°. All calculations were performed using a plane strain model, with a horizontal stress of 10 MPa and a vertical stress of 5 MPa.

4. Results

4.1. Effect of Distance Between WSP and Roadway

The surrounding rock cracks and plastic zones of test 1–4 are presented in Figure 6. The plastic zone is defined as the regions exceeding the Mohr–Coulomb yield criterion. As can be seen from the figure, the distance had a significant impact on the failure of surrounding rock. When the WSP was close to the roadway, the surrounding rock between the two was more serious, and shear cracks and tensile yields mainly occurred. When the fracture was far away from the roadway, the surrounding rock between them still had shear cracks and tensile yield, but the failure range in the horizontal direction decreased. The existence of the WSP affected the failure direction of the roadway. From the perspective of its failure mode, the roadway was prone to shear cracks, which was consistent with the simulation results of other scholars on roadway excavation [37,38,39]. In addition, shear cracks constitute nearly 70% of all fractures in the plastic zone, while tensile cracks concentrate at the excavation boundary and contribute to spalling; both mechanisms are critical in the design of supports. The damage shapes were trapezoidal, and the local shape was related to the location and expansion direction of the crack. In relation to the failure direction, the fractures mainly spread in the vertical direction, opposite to the direction of the large deformation.
The horizontal and vertical stresses are illustrated in Figure 7 and Figure 8, respectively. As observed from these two figures, the distance had a significant influence on the horizontal and vertical stress fields of the roadway. The closer the distance was, the more obvious the surrounding rock stress drop. Because the strike of the crack was parallel to the vertical stress, the crack had a significant effect on the vertical stress field. In addition, shear cracks along WSPs create anisotropic permeability, potentially channeling groundwater toward roadways.

4.2. Effect of WSP Dipping Angle

The surrounding rock crack and plastic zone of test 5–8 are shown in Figure 9. Fracture angle exerted a significant influence on the roadway failure, with its effects manifested in both the failure direction and location. The change in inclination angle caused the fracture direction to be deflected, and the damage to the surrounding rock between the roadway and the fracture was more serious. Under the condition of differential stress, the expansion direction of the crack was mainly upward and downward. Due to the existence of a horizontal crack, the upward expansion of the cracks was cut off, and the extension distance of the crack in this direction was shortened.
The horizontal and vertical stresses are shown in Figure 10 and Figure 11. The WSP angle had a significant influence on the roadway deformation failure. Variations in the fracture angle altered both the direction and shape of the stress reduction zone, accompanied by significant stress differentiation. Moreover, the degree of stress differentiation was closely related to the crack angle (the angle between the maximum principal stress and the composition of the crack). Moreover, angled WSPs deflect fractures toward vertical stress directions, increasing risks of intersecting overlying aquifers.

5. Discussion

In the process of mine construction, a large number of roadways need to be excavated and maintained; here, the resulting deformation failure of the surrounding rock is often controlled by the WSPs. The distribution and characteristics of the plane are the internal factors of the rock mass stability, and they determine the failure modes, scales, and characteristics.
The distribution characteristics of WSPs in the surrounding rock of underground caverns and the structural trace in the rock mass medium will affect the physical and mechanical behavior of the rock mass. The strength of these discontinuities is always low, and the deformation resistance and modulus are also several orders of magnitude lower than those of rock materials. Therefore, such rock mass will show strong heterogeneity, anisotropy, and discontinuity. The existence of WSP reduces the macroscopic strength of the rock mass obviously, and the roadway failure is mainly controlled by the strength of the WSP. That is, the deformation failure of the surrounding rock first occurs around the weak structural face with low strength when other conditions are similar. Additionally, under low confining pressure, cracks, slippage, and deformation occur around the WSP. The failure of the WSP will cause a change in the relationship between the WSP and the adjacent rock mass, which will aggravate the deformation failure of the surrounding rock mass in other parts of the roadway and generate permeable channels. In coastal mines, this process may connect faults to seawater via fractures, triggering water inrush when hydraulic gradients exceed critical thresholds.
When excavating near a WSP, the surrounding rock close to the plane is damaged more seriously. Due to the influence of WSPs, roadways often experience local rapid falls, whole collapse, bedding slips, and so on. If the axial direction of the roadway is consistent with the strike of the fault, it is easy for shear slip to occur along the fault surface and cause fault activation, resulting in collapse. It can be seen that the WSP has an important impact on the overall safety of the surrounding rock of the roadway. Fully understanding the effect of WSPs in underground engineering is significant for guiding the construction of underground engineering and preventing disasters.

6. Conclusions

1.
By introducing slip change rate and maximum static friction to solve the tangential contact force in the process of dynamic and static transformation, an elastoplastic failure criterion was adopted to describe the yield behavior of rock mass during deformation, and an optimized Y-Mat program was established. The mechanical response of surrounding rock after roadway excavation under differential stress was calculated, and the simulated stress results were compared with the corresponding analytical solutions to verify the rationality of the program.
2.
The farther the WSP was from the roadway, the less influence it had on the roadway. At the same time, the existence of the WSP changed the shape of the plastic zone, lengthening the failure zone along the fault direction. The WSP angle can change the shape and location of the failure zone of the surrounding rock, and it also leads to a deflection of the fracture direction. The surrounding rock between the roadway and the WSP is the most serious failure zone.
3.
The deformation failure of roadway surrounding rock first occurred at the weak structural face with low strength, caused by the WSP effect. Excavation reduced the normal stress and shear strength of the WSP in surrounding rock, resulting in relative slip and deformation. As time passed, the rock mass in other parts of the roadway also produced damage along the primary or new fracture surface, which intensified the roadway deformation failure and even caused a disaster.
4.
WSP-induced fractures serve as conduits for groundwater influx, especially in fault-proximal roadways or where crack angles align with hydraulic gradients. Mitigation strategies should prioritize sealing these pathways in water-rich mining environments.

Author Contributions

Data curation, G.L.; formal analysis, G.L. and J.G.; methodology, J.G. and G.L.; software, G.L. and J.G.; writing—original draft, J.G.; writing—review and editing, G.L. and F.M. All authors have read and agreed to the published version of the manuscript.

Funding

This research was supported by the National Science Foundation of China (Grant No. 42072305) and the Second Tibetan Plateau Scientific Expedition and Research Program (Grant No. 2019QZKK0904).

Data Availability Statement

All the relevant data are included in the paper.

Acknowledgments

The authors are grateful to the assigned editors and anonymous reviewers for their enthusiastic help and valuable comments, which have greatly improved this paper.

Conflicts of Interest

The authors declared that they have no conflicts of interest regarding this study. We declare that we do not have any commercial or associative interests that represent a conflict of interest in connection with the paper submitted.

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Figure 1. Engineering geological map: (a) geographical location of the study area within China; (b) simplified geological map illustrating the Sanshandao fault and other relevant features; (c) geological map of the Xinli gold deposit area; (d) cross-section of underground workings.
Figure 1. Engineering geological map: (a) geographical location of the study area within China; (b) simplified geological map illustrating the Sanshandao fault and other relevant features; (c) geological map of the Xinli gold deposit area; (d) cross-section of underground workings.
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Figure 2. Deformation failure of roadway surrounding rock under the influence of faults: (a) the roadway 220 m from the fault; (b) water inrush induced by the fault.
Figure 2. Deformation failure of roadway surrounding rock under the influence of faults: (a) the roadway 220 m from the fault; (b) water inrush induced by the fault.
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Figure 3. The numerical model.
Figure 3. The numerical model.
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Figure 4. Stress curves: (a) analytical solution; (b) simulation solution.
Figure 4. Stress curves: (a) analytical solution; (b) simulation solution.
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Figure 5. Scheme design: (a) the distance between the WSP and the center point of the roadway; (b) the WSP angle.
Figure 5. Scheme design: (a) the distance between the WSP and the center point of the roadway; (b) the WSP angle.
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Figure 6. Distribution of surrounding rock fractures and plastic zones caused by excavation: (a) test 1; (b) test 2; (c) test 3; (d) test 4.
Figure 6. Distribution of surrounding rock fractures and plastic zones caused by excavation: (a) test 1; (b) test 2; (c) test 3; (d) test 4.
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Figure 7. Horizontal stress of surrounding rock caused by excavation: (a) test 1; (b) test 2; (c) test 3; (d) test 4.
Figure 7. Horizontal stress of surrounding rock caused by excavation: (a) test 1; (b) test 2; (c) test 3; (d) test 4.
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Figure 8. Vertical stress of surrounding rock caused by excavation: (a) test 1; (b) test 2; (c) test 3; (d) test 4.
Figure 8. Vertical stress of surrounding rock caused by excavation: (a) test 1; (b) test 2; (c) test 3; (d) test 4.
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Figure 9. Distribution of surrounding rock fractures and plastic zone caused by excavation: (a) test 5; (b) test 6; (c) test 7; (d) test 8.
Figure 9. Distribution of surrounding rock fractures and plastic zone caused by excavation: (a) test 5; (b) test 6; (c) test 7; (d) test 8.
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Figure 10. Horizontal stress of surrounding rock caused by excavation: (a) test 5; (b) test 6; (c) test 7; (d) test 8.
Figure 10. Horizontal stress of surrounding rock caused by excavation: (a) test 5; (b) test 6; (c) test 7; (d) test 8.
Water 17 02257 g010
Figure 11. Vertical stress of surrounding rock caused by excavation: (a) test 5; (b) test 6; (c) test 7; (d) test 8.
Figure 11. Vertical stress of surrounding rock caused by excavation: (a) test 5; (b) test 6; (c) test 7; (d) test 8.
Water 17 02257 g011
Table 1. Numerical model parameters.
Table 1. Numerical model parameters.
ParameterRock MassWSP
Cohesion (MPa)110.014
Static frictional angle (°)4812
Sliding frictional angle (°)4610
Residual frictional angle (°)205
Tensile strength (MPa)8.120.007
Fracture energy release rate of type I (N/m)101
Fracture energy release rate of type II (N/m)10010
Penalty function (Pa)8.75 × 10108.75 × 109
Normal contact penalty function (Pa)1.75 × 10111.75 × 1010
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Guo, J.; Li, G.; Ma, F. Effects of Weak Structural Planes on Roadway Deformation Failure in Coastal Mines. Water 2025, 17, 2257. https://doi.org/10.3390/w17152257

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Guo J, Li G, Ma F. Effects of Weak Structural Planes on Roadway Deformation Failure in Coastal Mines. Water. 2025; 17(15):2257. https://doi.org/10.3390/w17152257

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Guo, Jie, Guang Li, and Fengshan Ma. 2025. "Effects of Weak Structural Planes on Roadway Deformation Failure in Coastal Mines" Water 17, no. 15: 2257. https://doi.org/10.3390/w17152257

APA Style

Guo, J., Li, G., & Ma, F. (2025). Effects of Weak Structural Planes on Roadway Deformation Failure in Coastal Mines. Water, 17(15), 2257. https://doi.org/10.3390/w17152257

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