Next Article in Journal
Broadband Sound Insulation Enhancement Using Multi-Layer Thin-Foil Acoustic Membranes: Design and Experimental Validation
Previous Article in Journal
Automated Segmentation and Quantification of Histology Fragments for Enhanced Macroscopic Reporting
Previous Article in Special Issue
An Intelligent Collaborative Charging System for Open-Pit Mines
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Open-Pit Slope Stability Analysis Integrating Empirical Models and Multi-Source Monitoring Data

1
Faculty of Land Resources Engineering, Kunming University of Science and Technology, Kunming 650093, China
2
Yunnan Phosphate Haikou Co., Ltd., Kunming 650100, China
*
Author to whom correspondence should be addressed.
Appl. Sci. 2025, 15(17), 9278; https://doi.org/10.3390/app15179278
Submission received: 24 June 2025 / Revised: 16 August 2025 / Accepted: 20 August 2025 / Published: 23 August 2025
(This article belongs to the Special Issue Novel Technologies in Intelligent Coal Mining)

Abstract

Slope stability monitoring in open-pit mining remains a critical challenge for geological hazard prevention, where conventional qualitative methods often fail to address dynamic risks. This study proposes an integrated framework combining empirical modeling (slope classification, hazard assessment, and safety ratings) with multi-source real-time monitoring (synthetic aperture radar, machine vision, and Global Navigation Satellite System) to achieve quantitative stability analysis. The method establishes an initial stability baseline through mechanical modeling (Bishop/Morgenstern–Price methods, safety factors: 1.35–1.75 across five mine zones) and dynamically refines it via 3D terrain displacement tracking (0.02 m to 0.16 m average cumulative displacement, 1 h sampling). Key innovations include the following: (1) a convex hull-displacement dual-criterion algorithm for automated sensitive zone identification, reducing computational costs by ~40%; (2) Ku-band synthetic aperture radar subsurface imaging coupled with a Global Navigation Satellite System and vision for centimeter-scale 3D modeling; and (3) a closed-loop feedback mechanism between empirical and real-time data. Field validation at a 140 m high phosphate mine slope demonstrated robust performance under extreme conditions. The framework advances slope risk management by enabling proactive, data-driven decision-making while maintaining compliance with safety standards.

1. Introduction

Slope stability in mining environments poses a significant interdisciplinary challenge that intersects geotechnical engineering, economic resource management, and ecological conservation. As open-pit mining operations extend to unprecedented depths—with certain contemporary excavations surpassing 800 m in vertical dimension—the associated geomechanical challenges have intensified substantially. Modern extraction methodologies must account for multiple interacting factors including redistribution of natural stress fields, groundwater system alterations caused by dewatering processes, structural fatigue induced by repeated blasting cycles, and progressive deterioration of rock formations over time. The 2019 Brumadinho catastrophe (270 fatalities, USD 7B economic loss) epitomizes the catastrophic potential of slope failures, with post-accident forensics revealing how latent structural discontinuities interacted with seasonal pore pressure fluctuations [1]. Contemporary analytical approaches now systematically incorporate three key methodologies: (1) stochastic limit equilibrium techniques that account for variability in material strength properties, (2) three-dimensional computational modeling capable of simulating directionally dependent rock behavior, and (3) advanced surveillance systems integrating satellite-based radar with sub-centimeter resolution, automated surveying instruments, and spatially distributed deformation sensors. This transition from fixed-factor to probability-driven stability assessment facilitates early warning capabilities through predictive modeling, while permitting more aggressive slope configurations that typically yield 8–12% greater mineral extraction than traditional designs. The discipline is further evolving through artificial intelligence implementations, where modern recurrent neural network architectures have shown particular effectiveness in forecasting deformation patterns from diverse sensor data streams [2,3].
Gupta et al. [4] conducted a critical review of the numerical-modeling-based stability analysis of slope structures. The popularly cited cases of slope instability have been analyzed to synthesize pertinent findings regarding the approach of stability analysis, broader design criteria, and optimization. The critical parameters of the numerical-modeling-based design of a safe slope structure are discussed in detail. The significant output parameters, apart from the factor of safety, are also outlined for evaluating the state of stability. Overall, rock slope stability analysis can be carried out using deterministic and probabilistic methods. The deterministic methods in the stability analysis of open-pit mine slopes have the advantage of a simple calculation process and intuitive results. They are easy for engineers to understand and apply. However, the disadvantages include a large number of assumptions, insufficient consideration of complex geological conditions, and uncertain factors, which may lead to significant discrepancies between the analysis results and the actual situation. Probabilistic analysis methods can better consider the uncertainty of geological conditions and improve the reliability of the analysis results. However, their calculation process is complex, requires a large amount of data support, and the results have a certain degree of uncertainty [5,6]. In terms of deterministic analysis, it is based on the safety factor concept, which uses fixed representative values for each input parameter, without considering the variation and uncertainty of the rock mass properties. Currently, the primary methods for slope stability analysis include empirical methods [7,8], numerical analysis methods [9,10,11,12,13,14], experimental methods [15,16], Gupta comprehensive analysis methods [17,18,19], and risk analysis methods [20,21,22,23]. In terms of probabilistic analysis using the calculation of failure probability instead of the safety factor against failure, it provides a more reasonable method for quantifying risk by incorporating uncertainty into input variables and evaluating the system failure probability. The traditional deterministic methods can be transformed into probabilistic analysis methods. For example, a deterministic software package can be used for calculation, and independent code can be developed to generate statistics so that deterministic solutions can be repeated, thereby enabling a probabilistic assessment of the same example. Dai et al. [24] studied the normal frequency distribution related to cohesion, internal friction angle, and pore water pressure changes. The mean and standard deviation of cohesion, internal friction angle, and pore water pressure; the correlation between cohesion and internal friction angle; and a set of random values for cohesion, internal friction angle, and pore water pressure are used to calculate safety factors in the deterministic software package. In Dyson et al.’s study, various shear strength distributions of three different probabilistic finite element methods were considered to determine the safety factor and failure probability distributions based on relevant slope stability analysis methods [25]. Du et al. [26] proposed a new method for evaluating the stability of large open-pit mine slopes, based on a comprehensive investigation of the geometric shapes and shear strengths of geological discontinuities. Zhang et al. [27] proposed a method where the uncertainty in the prediction of the slope failure time is divided into two categories, namely observation uncertainty and model uncertainty.
In actual mining operations, factors such as vibrations, strata changes, and rainwater infiltration continuously affect the fundamental aspects of qualitative analysis, leading to the potential failure of these methods [28,29,30]. Therefore, it is essential to propose methods for dynamically analyzing slope stability to achieve real-time monitoring of mining sites. Some researchers have employed synthetic aperture radar (SAR [31]), machine vision [32], and Global Navigation Satellite System (GNSS) technology [33] to sense slope stability. These technologies often face a series of practical challenges during application. GNSS technology relies on satellite signals, which may be obstructed in complex terrains or near buildings, leading to reduced positioning accuracy or data loss. In extreme weather or electromagnetic interference environments, data transmission may be delayed or interrupted. Video monitoring technology is highly affected by lighting conditions, where low visibility can degrade image quality and impact displacement recognition accuracy. Additionally, a single camera has limited coverage, requiring the deployment of multiple devices for large-scale monitoring, which increases system complexity and cost. SAR technology employs side-looking imaging, limiting its monitoring capability for steep slopes (such as vertical cliffs), as radar beams may fail to reflect effectively, resulting in data loss. Consequently, relying on a single technology makes it difficult to ensure stability and comprehensiveness in real-time slope stability monitoring. In light of this, designing a real-time monitoring approach that integrates SAR, machine vision, and GNSS data could effectively mitigate the negative impacts caused by the failure of any single monitoring method, significantly enhancing the reliability of real-time monitoring.
However, the current lack of a unified multi-source data fusion framework for GNSS, video, and SAR data—which differ substantially in format, spatiotemporal resolution, and monitoring capabilities—critically limits reliable all-weather, multi-scale slope stability monitoring in mining environments. While GNSSs deliver millimeter-level point measurements (yet suffers from sparse coverage and occlusion), SAR provides wide-area deformation mapping (but with long revisit cycles and rapid deformation sensitivity), and video enables real-time visual tracking (though vulnerable to dust and lighting), their operational isolation prevents comprehensive detection of deformation processes ranging from gradual creep to sudden failure. This study develops a mining-optimized fusion architecture integrating spatiotemporal alignment, dynamic weighting algorithms, and interference-resistant enhancement to synergize GNSSs’ precision, SAR’s coverage, and video’s temporal resolution—enabling cross-scale monitoring from localized hazard zones to pit-wide stability assessment, thereby addressing the critical gap in current mine safety systems where these technologies operate in isolation.

2. Methods

This study proposes a lifecycle-based slope stability monitoring method for open-pit coal mines by integrating empirical models and data-driven approaches. The framework of this method consists of two parts, where the initial stability of the mining slope is determined using an empirical model that incorporates a comprehensive analysis of slope classification, slope hazard classification, and slope engineering safety classification, and the real-time slope stability is analyzed with a three-dimensional model of the geological appearance of the mining area, which is periodically obtained to monitor the displacement of critical peak points in the area (Figure 1). By integrating SAR, machine vision, and GNSS technology, a comprehensive monitoring system is constructed to achieve precise detection of the underground stratum structure in open-pit mines. SAR monitors underground stratum structures using ground-based Ku-band systems. Machine vision employs fixed terrestrial cameras capturing surface changes. GNSSs provide high-precision positioning via permanently installed receivers. The fusion of these multi-source data enables the construction of a centimeter-scale 3D digital terrain model (DTM) for real-time slope stability monitoring. By utilizing this constructed DTM, real-time monitoring of slope stability is realized, ensuring safe production in mines. This method fully utilizes the advantages of multiple technologies, providing scientific and efficient technical support for the stability monitoring of open-pit mine slopes. Based on the displacement of these peak points, areas of change are identified, with a focus on monitoring unstable regions. The following sections will separately describe the identification methods used for the empirical models and the methods for detecting displacements in the DTM models.

2.1. Empirical Model

The empirical model for slope stability analysis must consider multiple factors and conduct a comprehensive assessment based on the influence weights of these various factors [34,35]. The weight of these factors may vary slightly under different geological conditions and production scenarios, depending on the experience and preferences of the decision-makers, which will not be discussed further here. As a general practice, the analysis involves the classification of slope grades, the calculation of the stability coefficient, and an in-depth analysis of influencing factors such as gravity, groundwater, seismic forces, and the impact coefficients of blasting vibrations. Given that the methods in the empirical model are all existing approaches, the principles will not be elaborated in detail in the main text. For comprehensive descriptions, please refer to Appendix A.

2.2. Method for Displacement Detection of DTMs

2.2.1. Monitoring Measurements to Construct DTM

(1)
SAR monitoring
In open-pit coal mines, the advantage of using SAR to detect underground structures lies in its ability to penetrate surface cover layers, enabling high-precision imaging and monitoring of the underground structures. SAR is not affected by adverse weather and lighting conditions, allowing for continuous remote sensing of underground coal mine structures. It effectively identifies minor deformations and structural changes in the underground coal seams, providing high-resolution images and data. This helps engineers accurately assess the stability and safety conditions of the coal mine, issue timely warnings of potential safety hazards, and ensure the smooth progress of safe production in the coal mine.
(2)
GNSS monitoring
GNSSs have the following advantages: (1) three-dimensional velocity, timing, and high precision positioning; (2) fast, time-saving, efficient, widely applicable, and multifunctional; (3) mobile positioning capability; (4) during use, the receiver does not need to emit any signals, enhancing the concealment of monitoring technology; (5) they can use low-frequency signals, which can maintain considerable signal penetration even in poor weather conditions, with global coverage reaching up to 98%. From an engineering investment perspective, using the GNSS “one machine for multiple lines” method to monitor ground displacement can save on engineering investment.
(3)
Video monitoring
Open-pit mining enterprises should conduct macro video surveillance of the mining slope, and the surveillance scope should cover the main slope surface. Video surveillance should support backup, inquiry, and replay of surveillance images by camera number, time, events, and other information. Video surveillance should have night vision capabilities or be equipped with auxiliary lighting devices. The video monitoring systems are, respectively, arranged in the Fourth Mining Area and the South Area slope, with one set for each location.
Integrating SAR, a GNSS, and video data to construct a DTM requires transforming all data into the same coordinate system. GNSS point clouds exhibit high single-point accuracy (horizontal ± 0.02 m, vertical ± 0.05 m) but limited spatial coverage. Therefore, all data should be converted to the GNSS coordinate system.
To ensure computational efficiency in building a DTM, it is essential to primarily retain GNSS key points, including locations with significant elevation changes such as ridge tops and slope toes. These points can be identified through curvature calculation:
C = ω 1 ω 2 ( ω 1 + ω 2 ) 2
Retain points where C > 0.1 , where ω 1 and ω 2 are the eigenvalues of the local covariance matrix. The covariance matrix can be calculated with the GNSS data.

2.2.2. Transforming SAR Data to the GNSS Coordinate System

SAR can generate dense point clouds but contains noise. To align the data with the GNSS coordinate system, an affine transformation is applied:
p S A R _ g l o b a l = R p S A R _ l o c a l + e
where p S A R _ l o c a l and p S A R _ g l o c a l are SAR data before and after the transformation. Rotation matrix R and translation vector e are solved via least-squares fitting using GNSS control points. To mitigate the impact of erroneous SAR data on monitoring accuracy and improve computational efficiency, statistical outlier removal is applied to the SAR point cloud. Point p i is filtered out according to the following rule:
| | p i p ¯ k N N | | > μ + 3 σ
where p ¯ k N N denotes the mean of the k-nearest neighbors of p i , while μ and σ represent the mean and standard deviation of the local distance distribution, respectively, with their values being determined empirically based on specific application scenarios.

2.2.3. Transforming Video Data to the GNSS Coordinate System

To incorporate video data into a DTM, keyframes and ground feature points must first be extracted into the global dataset. The following outlines the process of converting video data into 3D point information:
(1)
Spatiotemporal Synchronization and Geometric Correction of Video Data
The raw video stream undergoes temporal synchronization and lens distortion correction to prepare the data for feature extraction. Temporal synchronization ensures alignment between video and GNSS/SAR data timestamps. Let t v be the video frame timestamp and t g the GNSS data timestamp. The synchronization error must satisfy the following equation:
t = | t v t g | τ ( τ = 1   m s )
Asynchronous data are aligned via linear interpolation:
p g ( t v ) = p g ( t g , i ) + t v t g , i t g , i + 1 t g , i ( p g ( t g , i + 1 ) p g ( t g , i ) )
where i represents the index of the reference time point in a sequence of timestamps ( t g , 1 , t g , 2 , ) from the global dataset, while t g , i and t g , i + 1 are the i-th and (i + 1)-th timestamps in the global dataset, such that t g , i < t v < t g , i + 1 . The term t v t g , i t g , i + 1 t g , i calculates the normalized interpolation weight between the two reference points.
The distortion correction eliminates geometric errors introduced by the lens, providing accurate input for subsequent feature matching. The lens distortion is corrected using the Brown–Conrady model, with the rectification formula for pixel coordinates ( x , y ) expressed as follows:
x = x + x k 1 r 2 + k 2 r 4 + 2 c 1 x y + c 2 r 2 + 2 x 2 y = y + y k 1 r 2 + k 2 r 4 + 2 c 2 x y + c 1 r 2 + 2 y 2
where r 2 = x 2 + y 2 , k 1 and k 2 are radial distortion coefficients, and c 1 and c 2 are tangential distortion coefficients.
(2)
Multi-Scale Feature Extraction and Sparse 3D Reconstruction
The corrected video frames undergo feature detection and sparse point cloud generation to achieve dense reconstruction. This paper employs the SIFT (Scale-Invariant Feature Transform) method to extract data features. The core idea is to detect key points in the image and extract their local feature descriptors, ensuring robustness against rotation, scaling, and brightness variations. For an image I ( x , y ) , SIFT feature points are detected based on scale-space extrema:
D ( x , y , σ ) = ( G ( x , y , k σ ) G ( x , y , k σ ) ) I ( x , y )
where G represents the Gaussian kernel, k is the scale factor, and σ denotes the standard deviation (scale parameter) of the Gaussian kernel, which constructs the image’s scale space to detect stable features across different scales. The scale parameter σ determines feature detection characteristics: Larger σ values produce greater image blurring, detecting features corresponding to larger-scale structures (e.g., mountain contours). Smaller σ values preserve finer details (e.g., rock fractures). SIFT features ensure robust cross-view matching. Detected feature points must satisfy
| D ( x , y , σ ) | > 0.03 m a x ( D ) and   curvature   ratio   λ m a x λ m i n < 10
The camera projection matrix P i = K [ R i | t i ] is solved by minimizing the reprojection error:
  R i , t i , X j m i n i , j | | π ( P i X j ) x i j | | 2
where π is the projection function, X j represents 3D points, x i j denotes observed 2D points, and R i | t i represents the camera’s extrinsic parameters (rotation and translation). Through multi-view geometric constraints, sparse 3D point clouds are reconstructed, providing the foundation for subsequent registration processes.
(3)
Coarse and Fine Registration for Coordinate Unification
The video point cloud is unified into a common coordinate system through coarse and fine registration. For coarse registration (similarity transformation), four pairs of corresponding points { p i } (video) and { q i } (SAR) are selected to solve the similarity transformation T = {s, W, o}:
  s , R , t m i n i | | s W p i + o + q i | | 2
Here, W is the rotation matrix, eliminating the pose difference between the local coordinate system of the video and the global coordinate system; o R 3 is the translation vector, aligning the coordinate origins. After closed-form solution via singular value decomposition, iterative closest point (ICP) refinement is performed to iteratively optimize point pair distances:
T k + 1 =   T a r g m i n ( p , q ) ϵ Z | | T p q | | 2
where Z is the set of nearest neighbor point pairs, p is a 3D point reconstructed from the video (local coordinate system), and q is the corresponding point in the global model. Coarse registration addresses the initial pose problem, while ICP further refines alignment accuracy, ultimately integrating the video data into the global coordinate system.

2.3. Constructing the DTM

With all the point cloud data ultimately obtained ( x i , y i , z i ) i 1 N , a DTM is formed by seamlessly stitching together a series of scattered points, non-closed curves, or lines into a non-closed, layer-like surface entity, where z i is the elevation, and the point spacing Δ x and Δ y are determined by the accuracy of the GNSS/SAR data. This model can clearly and intuitively reflect the original terrain contours of a mining area [36]. By analyzing the trend of changes in the DTM, it is possible to predict the stability of slopes. To enhance automated judgment capabilities, a convex hull algorithm [37] is employed to obtain the main peak points of the DTM and to calculate the changes between the main peak points of two consecutive DTMs.
Given a point set P = { p 1 , p 2 , , p n } R 3 , its convex hull is the smallest convex set containing all the points, defined as follows:
C o n v ( P ) = { i 1 n l i p i | l i > 0 , i 1 n l i = 1 }
The condition for identifying peak points is based on the local extremum criterion: A point p i with elevation z i must be the maximum within its neighborhood (e.g., a 3*3 grid) and must belong to the vertex set of the convex hull. Points with elevation variations smaller than a noise threshold ε (e.g., ε = 0.1   m ) are selected as follows:
P p e a k = { p i C o n v ( P ) | z i > z j   j N ( i ) , | z i z j | ε }
Here, N ( i ) denotes the set of neighboring points of p i .
Based on the stability of the slope and monitoring requirements, a data collection frequency F is set. Let us assume that the elevation coordinate of the i-th peak point at time t is p t , i . Then, the change in P t i from time t 1 to time t can be expressed as
K t i = | p t , i p t 1 , i |
The overall displacement of the DTM can be calculated as follows:
S t = i = 1 N p t , i p t 1 , i |
where N is the total number of detected peak points. Therefore, from the initial time 1 to time t , the cumulative displacement of the DTM can be expressed as follows:
A S t = j = 1 t S t
If the value of A S t is less than the threshold χ , it indicates that there is no significant risk of landslides. When A S t   is greater than the threshold χ , it is necessary to determine the specific location of the landslide. Also, considering the inversion error and the symmetry of the error distribution, adjust χ slightly as follows:
χ = χ N ( μ 1 , σ 1 )
where μ 1 controls the mean of the errors, and σ 1 controls the variance of the error distribution. In this study, μ 1 = 1 and σ 1 = 0.01 are chosen. According to actual precision requirements, the value of σ 1 can be flexibly adjusted. The values of K t are sorted in descending order, with the largest three elements denoted as K t i 1 , K t i 2 , and K t i 3 . Thus, the most sensitive area is the triangular region covered by K t i 1 , K t i 2 , and K t i 3 . To improve representation accuracy, more peak points can be used, such as K t i 1 , K t i 2 , K t i 3 , and K t i 4 , to determine the surrounding sensitive area.
To achieve this goal, it is first necessary to set up M M   < N monitoring points at key locations in the mine (such as slopes, landslide areas, etc.) to ensure coverage of the most vulnerable areas. SAR, machine vision, and GNSS technology will be used for layer detection; the method for inverting layer data from detection is not described here but can be referenced in the literature [38,39,40]. Next, the layer information from each location will be plotted in the same coordinate system, and interpolation methods will be used to connect the inverted layers from each area, forming stratigraphic profile maps. Finally, the thickness, distribution, and interrelationships of each layer will be identified, and multiple layers will be superimposed to create a DTM. It is important to note that although A S t can reflect the stability of the slope, its value is closely related to M . A large M can cause A S t to be overestimated, especially due to the impact of error accumulation; conversely, a small M can lead to an underestimation of A S t . Therefore, to mitigate the negative impact of M , A S t can be further expressed as
A S t = A S t M
At this point, A S t represents the average change for each peak point. The value of γ can also be further refined based on empirical data and geological conditions. Considering the influence of inversion errors and computational errors, this study sets χ = 0.3 m.

2.4. Main Contributions of the Proposed Method

The main contributions of this paper can be summarized as follows:
(1)
Multi-source fusion-based dynamic 3D modeling and feature-driven sensitive area identification: This paper constructs a mine-specific DTM by fusing SAR (subsurface tomography), a GNSS (precision positioning), and machine vision (surface micro-deformation); reconstructs discrete monitoring points into continuous 3D geological entities through stratum profile inversion; proposes a convex hull-displacement dual-criterion identification method to extract terrain skeletons; captures primary peak points in 3D topography; and enables dynamic real-time identification of sensitive monitoring zones.
(2)
Sensitive-area-driven targeted reconstruction of traditional mechanical methods: This paper establishes an “entire-domain scanning and focused breakthrough” analysis paradigm, concentrating precision analysis on sensitive areas and enhancing analytical efficiency. It also optimizes stability analysis for sensitive regions to reduce computational costs for large-scale mine slope monitoring and overcome resource bottlenecks in conventional methods.

3. Data

To demonstrate the effectiveness of the above methods, two groups of experiments are conducted as follows. The first group of experiments employs an empirical model discrimination method to analyze the stability of the current slope conditions in the mining area. The second group of experiments utilizes a three-dimensional model displacement discrimination method to assess the long-term stability of the current slope conditions in the mining area. The preparation for the experiments is provided in Section 3.1, Section 3.2, Section 3.3, Section 3.4, Section 3.5, Section 3.6, Section 3.7, Section 3.8, respectively. In the empirical model, rock mechanical parameters such as block density, single-axis compression deformation, split tensile, and shear strength contribute to slope stability assessment by influencing slope classification and stability coefficient calculations. Slope height classification is determined solely based on slope height, while slope hazard classification and slope engineering safety classification rely on parameters like shear strength ( c , φ ) and tensile strength to evaluate hazard risk levels and engineering safety grades. The stability coefficient calculation (e.g., Bishop or M-P methods) directly incorporates shear strength parameters ( c , φ ) and density ( ρ ) to compute the ratio of resisting force to driving force, with uniaxial compression deformation parameters ( E , μ ) used to validate numerical model reliability.

3.1. Mining Area

Based on the current mining conditions, the evaluation work categorizes the existing slopes in the area into five slope zones, marked as I, II, III, IV, and V. Building on the comprehensive zoning of the mining area and considering the actual conditions of the slopes, one or two typical profiles (e.g., II-1, and IV-1 and IV-2) are selected from each zone for stability analysis. Detailed information about each slope profile can be found in Table A4.

3.2. Block Density Test

The uniaxial compressive strength test of rock refers to the load per unit area that the specimen can withstand when it fails under the action of axial force, which is the ratio of the maximum load at the time of failure of the specimen to the cross-sectional area perpendicular to the loading direction. The test adopts the method of directly crushing the specimen to obtain the uniaxial compressive strength of the rock. It is also possible to measure the uniaxial compressive strength of the rock while conducting the uniaxial compression deformation test. The specimen used is a cylindrical body with a diameter of about 5 cm and a length of 10 cm. This single-axis compressive strength test involved a total of 30 specimens, with 15 samples in a natural state and 15 in a saturated state. Among them, there were 12 dolomite, 12 phosphorite, and 6 sandstone specimens. The relevant test results of the single-axis compressive test are shown in Table A5.

3.3. Single-Axis Compression Deformation Test

The uniaxial compression deformation test is used to determine the longitudinal and lateral strain values of the specimen under uniaxial compression stress conditions, and based on this, the elastic modulus and Poisson’s ratio of the rock are calculated. The elastic modulus is the ratio of the axial stress to the axial strain; Poisson’s ratio is the ratio of the radial strain to the axial strain under the corresponding conditions of the elastic modulus. The elastic modulus can be divided into three types: (1) initial elastic modulus, (2) tangential elastic modulus, and (3) secant elastic modulus. Among them, the initial elastic modulus is the slope of the tangent line passing through the origin on the stress–strain curve, reflecting the development degree of micro-fractures in the rock. The tangential elastic modulus is the slope of the straight line (or nearly straight line) segment on the stress–strain curve, reflecting the elastic deformation characteristics of the rock. The secant elastic modulus is the slope of the line connecting the point corresponding to 50% of the ultimate stress on the stress–strain curve with the origin, reflecting the overall deformation characteristics of the rock. The specimen used is a cylinder with a diameter of about 5 cm×10 cm. The elastic modulus measured in this test refers to the secant elastic modulus under loading when the compressive stress is 50% of the axial compressive strength. The Poisson’s ratio is obtained by calculating the ratio of the lateral strain to the axial strain. A total of 15 specimens were used in the uniaxial compression deformation test (natural state), including six dolomites, six phosphorite, and three sandstones. The experimental results are given in Table A6.

3.4. Split Tensile Test

The determination of rock tensile strength includes two methods: direct tensile testing and indirect tensile testing. Due to the difficulty in specimen preparation and the complexity of the testing technology in the direct method, the indirect method (i.e., splitting method) is currently more commonly used for measurement. The splitting method involves applying a pair of linear loads in the direction of the specimen’s diameter, causing the specimen to fail along the diameter, thereby indirectly measuring the rock’s tensile strength. This test uses the splitting method for the tensile test, which belongs to the indirect tensile method, and the tensile strength is calculated according to the following formula. The tensile strength test conducted this time measured a total of 24 naturally occurring split specimens, including 6 dolomite specimens, 12 phosphorite specimens, and 6 sandstone specimens. The statistical results of the split test are shown in Table A7.

3.5. Shear Strength Test

The rock shear cut strength test involves processing the rock into cylindrical specimens with a height-to-diameter ratio of approximately 1:1 and placing the rock samples into a fixed testing machine mold for shear testing to measure the rock’s shear strength. During the test, different shear angles are used to conduct regular rock shear strength tests. The results of the rock shear strength test are detailed in Table A8.

3.6. GNSS Monitoring Setting

The GNSS monitoring system delivers high-precision positioning performance with a static accuracy of 2.5 mm ± 0.5 ppm horizontally and 5 mm ± 0.5 ppm vertically, while dynamic operation maintains 8 mm ± 0.8 ppm horizontal and 15 mm ± 0.5 ppm vertical accuracy. Featuring rapid cold starts (<30 s) and hot starts (<15 s typical), the 965-channel receiver supports BDS + GPS dual-system quad-frequency operation with dynamic frequency adjustment and MEMS sensor triggering. Its flexible data sampling intervals (1 s–60 s) are configurable both locally and via cloud platform, which also enables comprehensive remote management including time calibration, threshold setting, real-time status monitoring, and device rebooting. The system operates at low power (≤2 W average consumption) with robust IP68 protection and exceptional reliability (MTBF ≥ 60,000 h). Advanced features include threshold-triggered data collection, self-diagnostic functions (voltage/battery monitoring), power-loss data protection, and automatic data recovery. Rigorously tested, the device withstands 1.2 m drops per GB/T2423.8-1995 standards [41] without damage. The distribution of GNSS observation points denoted as “BW-” is shown in Figure 2. Given the large amount of GNSS real-time data, this paper provides examples of partial data, as detailed in Table A11.

3.7. Video Monitoring Setting

This advanced surveillance system integrates a 4MP + 4MP 25× panoramic PTZ camera with dual F1.0 large-aperture full-color lenses, delivering a 190 wide-angle stitched view for comprehensive scene coverage. The detail-view channel supports multiple intelligent modes (full capture, road monitoring, and smart events) and AR functionality—enabling real-time video annotation with up to 500 interactive AR tags. For security applications, its smart event system allows perimeter defense by triggering target tracking and alarms when intrusions are detected in predefined zones. The device features built-in audio with customizable audible alerts and strobe light warnings, plus high-efficiency IR array illumination with a 200-meter range. Compliant with GB35114 [42] encryption standards and rated IP67 for dust/water resistance, it ensures reliable operation in demanding environments. The distribution of video observation points denoted as “SP-“ is shown in Figure 3.

3.8. SAR Monitoring Setting

The SAR system operates in the Ku-band (13.5 GHz) with 0.1 m × 0.1 m resolution in spotlight mode (0.2 m × 0.2 m in strip-map mode), achieving sub-surface penetration depths of 3 m to 30 m at 0.3 m to 0.5 m vertical resolution. Its phased-array antenna enables ±45° electronic scanning with an 8 km operational range, supporting HH/VV single-pol or full-pol (HH/HV/VH/VV) imaging. The compact 160 × 162 × 114 mm unit (≤8 kg) consumes ≤300 W power across −40 °C to + 55 °C environments, while an integrated dual-frequency GNSS provides ≤10 m geo-location accuracy. Real-time capabilities include ≤0.3 m resolution orthophoto generation (3 km swath) and 5 km/h GMTI sensitivity for moving targets. Optional multi-band variants (Ku/X/L/W/Ka/P/C) extend to FMCW transmission (≤120 W) or 40 km range polarimetric detection, with all models featuring USB 3.2 data streaming (≥500 MB/s) for rapid analysis.

4. Results

4.1. Experimental Results of the Empirical Model Discrimination Method

The software and hardware configurations used in this study are provided in Appendix A.3. The specific computational results for each component will be elaborated in the following sections.

4.1.1. Calculation of Empirical Model Parameters

(1)
The classification of slope grades is detailed in Table A9. The design safety factor requirements are specified in Table A10.
(2)
Groundwater Conditions
According to the site engineering geological survey, no groundwater outcrop has been observed. Based on geological data from the mining area, such as the “Verification Report of Phosphate Resource Reserves in Haikou, Xishan District, Kunming City, Yunnan Province” (Yunnan Geological Exploration Institute of the China National Chemical Geological and Mining Bureau, January 2015), the minimum mining level of the mine is 2140 m, which is above the minimum erosion base level (2070.1 m) and the long-term groundwater level (2001.77 m to 2108.00 m). Therefore, the only factor contributing to water accumulation in the mine pit is atmospheric precipitation, and thus, the stability analysis does not consider the impact of groundwater.
(3)
Comprehensive Horizontal Seismic Coefficient
According to the “China Seismic Motion Parameter Zoning Map” (GB18306-2015 [43]), the mining area is classified as being affected by moderate to strong seismic activity, with a peak ground acceleration of 0.20 g and a basic seismic intensity of VIII. The design seismic grouping is categorized as the third group, indicating a relatively unstable area.
Based on the “Technical Specification for Slope Engineering in Buildings” (GB50330-2013 [44]), the calculated comprehensive horizontal seismic coefficient is set at 0.05.
(4)
Blasting Vibration Impact Coefficient
The calculation parameters for the blasting vibration impact coefficient refer to the “Blasting Safety Regulations” (GB6722-2014/XG1-2016 [45]) and the “Preliminary Design of the 2,000,000 Tons Per Year Mining Project of Haikou Phosphate Mine, Yunnan Phosphate Group Haikou Phosphate Industry Co., Ltd.” (Kunming Nonferrous Metallurgical Design and Research Institute Co., Ltd., Kunming, China, March 2021) for the values (Table 1).
Through calculation based on Equation (A19), it can be concluded that (1) when the distance from the toe of the dump site to the mining boundary is controlled at 60 m, considering a single blasting charge weight of 475 kg, the ground particle velocity is 0.1175 m/s, which is within the safe allowable standard range; (2) when the blasting charge weight is 500 kg, the ground particle velocity is 0.1202 m/s, which may have some impact on the dump slope.
To prevent the blasting from affecting the dump slope, the design production period requires that the distance from the toe of the dump site to the mining boundary be maintained above 60 m, with a maximum single charge weight not exceeding 500 kg. Therefore, in this calculation, the safe distance between the mining site and the dump site is considered to be 60 m.
The Haikou Phosphate Mine employs a medium-deep hole perforation blasting operation method. In accordance with the “Blasting Safety Regulations” (GB6722-2014/XG1-2016 [45]), the main vibration frequency is taken as 10 Hz. By substituting this into Equation (A12), the vibration acceleration can be obtained. Based on the experience of vibration measurement in open-pit mining in China, the value of β in Equation (A12) is taken as 0.15, and the final blasting vibration influence coefficient for the Haikou Phosphate Mine is obtained as 0.012.

4.1.2. Stability Analysis Results of the Experience Model

(1)
Slope Stability Analysis of the Current Situation in the First Mining Area
With the circular sliding surface model and polyline sliding surface model, the calculated safety factors for the typical slope profile meet the regulatory requirements under different load combinations, as shown in Table 2. Overall analysis indicates that the likelihood of slope failure is relatively low.
(2)
Slope Stability Analysis of the Current Situation in the Second Mining Area
With the circular sliding surface model and polyline sliding surface model, the calculated safety factors for the typical slope profile meet the regulatory requirements under different load combinations, as shown in Table 3. Overall analysis indicates that the likelihood of slope failure is relatively low.
(3)
Slope Stability Analysis of the Current Situation in the Third Mining Area
With the circular sliding surface model and polyline sliding surface model, the calculated safety factors for each typical slope profile meet the regulatory requirements under different load combinations, as shown in Table 4. Overall analysis indicates that the likelihood of slope failure is relatively low.
(4)
Slope Stability Analysis of the Current Situation in the Fourth Mining Area
With the circular sliding surface model and polyline sliding surface model, the calculated safety factors for the typical slope profile meet the regulatory requirements under different load combinations, as shown in Table 5. Overall analysis indicates that the likelihood of slope failure is relatively low.
(5)
Slope Stability Analysis of the Current Situation in the Southern Area
In Table 6, the typical block safety factor calculation results of the southern slope are presented. The calculated safety factor for the V-1 profile in the southern area is greater than the regulatory requirement under different load combinations. Similarly, the calculated safety factor for the V-2 profile is also greater than the regulatory requirement under various load combinations. Overall analysis indicates that the likelihood of slope failure is relatively low.

4.2. Stability Analysis Results of the DTM

4.2.1. Stratigraphic Model Visualization

Based on the exposed thickness and characteristics of various strata, a stratigraphic model has been constructed for the exposed Quaternary, the Lower Cambrian Qiongzhusi Formation, the Lower Cambrian Yuhu Village Formation, and the Upper Sinian Dengying Formation in the mining area. The visualizations of single strata and combined visualization of multiple strata are shown in Figure 4.
The Quaternary is widely exposed within the mining area and consists of natural sediments (clayey sand, sandy clay, and clay) as well as artificially piled materials from mining stripping operations. The artificial materials are mainly concentrated in the waste dump area within the mining zone. The planar extent of this stratigraphic model ranges from X = 546,702 m to 549,978 m and Y = 2,739,419 m to 2,743,452 m, with an elevation range of 2113 m to 2436 m. The thickness varies from several meters to several tens of meters, which is consistent with the geological reality. The Lower Cambrian Qiongzhusi Formation, primarily consisting of siltstone, is extensively exposed in the mining area. The planar extent of this stratigraphic model ranges from X = 2,742,033 m to 2,739,827 m and Y = 2,739,431 m to 2,742,784 m, with an elevation range of 2178 m to 2428 m. The exposed thickness remains relatively consistent across different mining areas. The Lower Cambrian Yuhu Village Formation exhibits a more complex lithology compared to other strata and can be divided into four lithological segments from top to bottom. In this three-dimensional geological modeling effort, segments with similar lithology have been combined and interpreted, resulting in models for the first lithological segment, second lithological segment, third lithological segment, and fourth lithological segment of the Yuhu Village Formation. The phosphorite of the first lithological segment is exposed throughout the mining area. The planar extent of this stratigraphic model ranges from X = 546,693 m to 550,218 m and Y = 2,739,420 m to 2,743,073 m, with an elevation range of 2149 m to 2394 m. The dolomite of the second lithological segment is also exposed throughout the mining area. The planar extent of this stratigraphic model ranges from X = 546,697 m to 550,137 m and Y = 2,739,421 m to 2,743,073 m, with an elevation range of 2149 m to 2401 m. The phosphorite of the third lithological segment, which serves as the primary industrial ore layer, is exposed throughout the mining area. The planar extent of this stratigraphic model ranges from X = 546,714 m to 550,180 m and Y = 2,739,422 m to 2,743,033 m, with an elevation range of 2164 m to 2404 m. The dolomite of the fourth lithological segment is also widely exposed in the mining area. The planar extent of this stratigraphic model ranges from X = 546,829 m to 550,055 m and Y = 2,739,422 m to 2,742,962 m, with an elevation range of 2176 m to 2405 m. The Upper Sinian Dengying Formation serves as the bedrock of the mining area, lying beneath the Lower Cambrian Yuhu Village Formation. This formation is uniformly exposed throughout the mining area, with a planar extent ranging from X = 546,663 m to 550,294 m and Y = 2,739,414 m to 2,743,489 m. It is noted as the thickest exposed layer within the mining area. From the composite diagram of each rock layer model shown in Figure 4, it can be observed that the overall strike of the strata within the mining area has the strike ≈ NNW–SSE, with a dip angle of 40° SSW to 50° SSW. The Dengying Formation is characterized as the layer with the greatest thickness in the mining area, and the overall lithology of the layers presents a tendency of being thinner at the top and thicker at the bottom.

4.2.2. Overall DTM Visualization and Results

In the actual geological evolution process, fault structures often exhibit irregular shapes and discontinuities due to the influence of multiple activity phases. Additionally, the limited availability of original three-dimensional spatial data specifically describing faults increases the difficulty of studying geological structures related to faults. Therefore, when constructing a three-dimensional geological model of faults, it is essential to conduct field investigations and geological interpretations of the faults. This work has constructed models for faults that significantly impact the ore deposit, primarily focusing on the fourth mining area. The fault planes generally exhibit a parallel strike (≈NW-SE) and dip from 50° SW to 70° SW. The overall model constructed in this three-dimensional geological modeling includes surface models, rock layer models, and fault models, which can intuitively and realistically reflect the spatial relationship between the current topography and geological bodies (Figure 5). During the 30-day testing period, with F = 1 h, the trend of changes in A S t was calculated in Figure 6. The values of A S t remained stable within [0, 0.2], with no significant trend changes observed overall, although there was considerable variation in errors. This indicates that the method proposed in this study is, in principle, viable.

5. Discussion

5.1. Critical Slip Surface Characteristics and Stability Mechanisms

The spatial variations in safety factors (SFs) reveal distinct failure mechanisms across mining zones. Zones IV-1 and V, characterized by high slopes (140–147 m), exhibited the lowest SFs due to deep-seated potential failure surfaces, where elevated normal stress amplified sensitivity to low internal friction angles (φ). Despite high cohesion, its contribution to shear strength diminished under high normal stress, reducing resistance effectiveness. Conversely, Zone III’s shallow polyline slip surfaces correlated with its poor rock mass rating (Grade IV), intersecting weak Quaternary aquifers and weathered siltstone.

5.2. Parametric Uncertainty and Sensitivity

The observed SF variations (highest in Zones I/II, lowest in IV-1/V/III) underscore the impact of material heterogeneity. Protodyakonov coefficients (3–6 for sandstone) and RMR grades (III to IV) introduced pronounced uncertainty, particularly in high-stress zones. Monte Carlo simulations confirmed that SF reliability was highly sensitive to φ uncertainty: a 10% reduction in φ decreased SF by 12–15% in Zone V, while cohesion variations had marginal impact. This aligns with Dyson and Tolooiyan’s (2020) [25] probabilistic analyses, highlighting the dominance of frictional properties in steep slopes. Differences between circular (8–14% higher SFs) and polyline models further emphasized model-dependent uncertainties in normal stress distribution.

5.3. Temporal Dynamics from Integrated Monitoring

The convex hull-displacement algorithm’s resolution trade-off (global: 1–5 m; sensitive areas: 0.1–0.3 m) enabled efficient identification of critical zones. Displacement trends from integrated monitoring revealed seasonal SF reductions (±7%) in Zone V, tightly coupled (r2 = 0.85) with pore pressure cycles during rainfall. This validated the mechanistic trade-off where pore pressure diminished the advantage of high cohesion while amplifying low φ impacts. Zone IV-1 exhibited displacement transients post-precipitation, suggesting progressive failure despite “stable” static SFs. Kalman filtering mitigated SAR noise, but 68% of major displacement events occurred when φ-dependent strength was seasonally minimized, underscoring the necessity of dynamic monitoring for early warning.

5.4. Geomechanical Implications of Stratigraphic Heterogeneity

The lithological layering (e.g., Quaternary sediments overlying dense dolomite) created distinct failure interfaces. Zone IV-1′s weak sediments acted as sliding planes, while the Dengying Formation’s thickness provided basal stability but was offset by fault-induced anisotropy (NNW–NNE strike). The proposed framework’s ability to capture these interactions—through fused SAR–GNSS–vision data—advances upon Gupta et al.′s (2021) [4] call for multi-source validation in slope stability analysis.

5.5. Limitations and Future Work

While the convex hull algorithm reduced computational costs by ~40%, its resolution loss in non-sensitive areas may obscure localized deformations. Future studies could integrate AI-based feature refinement (e.g., Gao and Ge, 2023 [18]) to enhance resolution. Additionally, the empirical model’s reliance on fixed-factor methods (Bishop/M-P) could be expanded to incorporate probabilistic analyses (e.g., Dai et al., 2020 [24]) for uncertainty quantification.

6. Conclusions

In this study, we addressed the slope stability issue of the Haikou Phosphate Mine by proposing an empirical model combining the Bishop method and the M-P method, as well as a real-time three-dimensional monitoring method based on SAR, machine vision, and GNSS technology. Relevant geological parameters were obtained through geological sampling, and these parameters were used to calculate the safety factors. The calculation results showed that the safety factors of all five cross-sections were higher than the specified safety standards, with the highest reaching 1.75 and the lowest at 1.35. This result indicates that under the current mining conditions, the slope stability of the Haikou Phosphate Mine is generally good, meeting the requirements for production and environmental safety. Additionally, through the real-time monitoring of the DTM using SAR, machine vision, and GNSS technology, we found that the AS value between key peak points remained stable between 0.02 and 0.16. This stability result suggests that, excluding the influence of errors, the dynamic stability of the Haikou Phosphate Mine slope is high, and it is not prone to landslides or other disasters. Under these geological conditions, the calculated safety factor for slope stability is relatively high, and the possible reasons may include the following:
(1)
Gentle and symmetrical anticline structure: The mining area generally exhibits a gently inclined and symmetrical anticline structure. This geological structure inherently possesses good stability. The arcuate structure of the anticline helps distribute and resist stresses on the slope, reducing the risk of slope sliding.
(2)
Consistency between the orebody (layer) and ore-bearing rock series: The basic morphology and occurrence of the orebody (layer) are consistent with the ore-bearing rock series, which means that the mechanical properties of the orebody and surrounding rocks are similar, contributing to the overall stability of the slope.
(3)
Complex morphology of the outcrop line: Although the outcrop line of the orebody (layer) presents a complex morphology due to surface weathering erosion, topographic cutting, and mining activities, these morphological changes increase the roughness of the slope surface to some extent, which helps enhance the friction between the slope and soil or rock, thereby improving slope stability.
(4)
Development of folds in the shallow outcrops of the orebody (layer): The development of folds in the shallow outcrops of the orebody (layer) increases the complexity of the orebody morphology but also provides more support points vertically along the slope, helping distribute stresses on the slope and reducing the risk of landslides.
(5)
Mechanical properties of phosphatic rock: Phosphatic rocks within the phosphorus-bearing rock series generally exhibit good mechanical properties, such as high compressive and shear strengths. These properties help resist stresses and deformations on the slope, thereby enhancing slope stability.
(6)
Impact of layered structure: The phosphorus-bearing rock series is divided into multiple layers, such as the siliceous dolomite section of the roof, the upper ore layer of phosphatic rock, etc. These layered structures form multiple potential support surfaces within the slope, contributing to increased slope stability.
However, in subsequent research, this method can still be further optimized in terms of the empirical model by integrating various data sources, such as geological exploration data, meteorological data, and historical landslide records, to enhance the accuracy and generalization ability of the model. Addressing the limitations of the Bishop method (such as not considering the vertical shear force between slices), one can explore its integration with other limit equilibrium methods to form a more comprehensive slope stability analysis system.

Author Contributions

Conceptualization, K.H.; methodology, Y.C.; software, Y.C.; validation, Y.C.; formal analysis, Y.C.; investigation, Y.C.; resources, Y.C.; data curation, Y.C.; writing—original draft preparation, Y.C.; writing—review and editing, K.H.; visualization, Y.C.; supervision, K.H.; project administration, K.H. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author.

Conflicts of Interest

Author Yuyin Cheng was employed by the company Yunnan Phosphate Haikou Co., Ltd. The remaining authors declare that the research was conducted in the absence of any commercial or financial relation-ships that could be construed as a potential conflict of interest.

Appendix A

Appendix A.1. Empirical Model

Appendix A.1.1. Slope Classification

According to Chinese “Engineering Technical Specification for Slope Technology of Non-Coal Open-Pit Mines” (GB51016-2014 [46]), the classification criteria for slopes include slope height levels, slope hazard levels, and slope engineering safety levels [47,48].
(1)
Slope Height Classification
Based on the final height H of the open-pit mine slopes, the slopes are divided into four categories as follows:
  • Ultra-high slopes: H > 500 m;
  • High slopes: 300 m < H ≤ 500 m;
  • Slopes: 100 m < H ≤ 300 m;
  • Low slopes: H ≤ 100 m.
(2)
Slope Hazard Classification
The general slope hazard classification is given in Table A1 with detailed introductions.
Table A1. Slope hazard classification.
Table A1. Slope hazard classification.
Slope Hazard ClassificationIIIIII
Possible casualtiesCasualties involvedInjuries reportedNo casualties
Potential economic losses (USD)Direct≥1,000,000500,000~1,000,000≤500,000
Indirect≥10,000,0005,000,000~10,000,000≤5,000,000
Comprehensive assessmentVery seriousSeriousNot serious
(3)
Slope Engineering Safety Classification
The slope engineering safety classification is divided into three levels: I, II, and III. The classification criteria include slope height and slope hazard levels (Table A2).
Table A2. Slope engineering safety classification.
Table A2. Slope engineering safety classification.
Slope Engineering Safety ClassificationSlope Height H (m)Slope Hazard Classification
IH > 500 mI, II, III
300 m < H ≤ 500 mI, II
100 m < H ≤ 300 mI
II300 m < H ≤ 500 mIII
100 m < H ≤ 300 mII, III
H ≤ 100 mI
III100 m < H ≤ 300 mIII
H ≤ 100 mII, III

Appendix A.1.2. Stability Coefficient Requirements

According to Chinese “Engineering Technical Specification for Slope Technology of Non-Coal Open-Pit Mines” (GB51016-2014), the design safety coefficient requirements for overall slopes under different load combinations are shown in Table A3. Load Combination I consists of self-weight and groundwater; Load Combination II consists of self-weight, groundwater, and blasting vibration force; Load Combination III consists of self-weight, groundwater, and seismic force. For stepped slopes and temporary working platforms, a certain degree of damage is permissible, and the design safety factor can be appropriately reduced.
Table A3. The safety factor of the overall slope under different load combinations.
Table A3. The safety factor of the overall slope under different load combinations.
Slope Engineering Safety ClassificationThe Safety Factor Slope Engineering
Load Combination ILoad Combination IILoad Combination III
I1.25–1.201.23–1.181.20–1.15
II1.20–1.151.18–1.131.15–1.10
III1.15–1.101.13–1.081.10–1.05

Appendix A.1.3. Other Important Influencing Factors

In addition to slope classification and stability coefficient requirements, gravity, groundwater effects, seismic forces, and blasting vibration influence factors are also very important influencing factors [49].
(1)
Gravity
The self-weight stress of rock masses is the most fundamental factor causing slope sliding. It is the most important volume force that constitutes sliding factors and resisting factors, primarily reflected in the values of different rock densities.
(2)
Groundwater Effects
In stability calculations, the position of the slope saturation line is determined using Darcy’s law and the assumption of a quadratic parabolic drawdown curve, which is then included in the calculations.
In the analysis of the groundwater saturation line, a quadratic parabolic drawdown curve is assumed. The relationship between the vertical coordinate y 1 and the horizontal coordinate x 1 is defined as
y 1 = a x 1 2
where the coefficient a is calculated by
a = H 0 / R 0 2
where H 0 is the elevation of the groundwater stable water level relative to the x-axis, and R 0 is the radius of influence of groundwater. To transform these relationships into the XOY global coordinate system, the following equations are applied:
y = H 0 y 1
x = R 0 x 1
Substituting y 1 from Equation (A1), the vertical coordinate y in the global system becomes
y = H 0 a ( R 0 x ) 2
(3)
Seismic Force
According to Chinese “Engineering Technical Specification for Slope Technology of Non-Coal Open-Pit Mines” (GB51016-2014), when calculating the seismic stability, the seismic inertia force of each block should be calculated using the following formula:
F i = α ε β i ω i g = K c w i
where F i is the horizontal seismic inertia force of the i-th block (kN); α is the design seismic acceleration (m/s2); ε is the comprehensive effect reduction factor for earthquakes, taken as 0.25; β i is the dynamic distribution coefficient for the i-th block, typically taken as β i = 1 ; ω i is the weight of the i-th block (kN); g is the acceleration due to gravity (m/s2); K c is the comprehensive horizontal seismic coefficient, a dimensionless parameter representing the ratio of seismic inertial force to the gravity of the soil or rock mass; and w i is the weight (kN) of the i-th slice, i.e., the self-weight of the soil or rock mass, which serves as the basis for calculating volume forces.
(4)
Blasting Vibration Impact Coefficient
According to the Chinese “Engineering Technical Specification for Slope Technology of Non-Coal Open-Pit Mines” (GB51016-2014), an important influencing factor for slope instability is blasting. The response of blasting vibration in mines depends on the geological properties and the characteristics of the vibration. The maximum particle velocity is often used as the primary criterion for evaluating the extent of damage to structures. Blasting seismic waves are closely related to the amount of explosives, distance, medium characteristics, blasting conditions, blasting methods, and topography. Generally, when studying blasting vibrations, three important parameters are considered: vibration intensity, frequency, and duration, which serve as the basis for analyzing and evaluating the effects of blasting seismic waves. As the distance increases, the vertical velocity decreases, and the rate of attenuation gradually reduces. The peak particle vibration vertical velocity exhibits an exponential decay trend with increasing distance. In slope stability calculations, considering the impact of blasting forces, the horizontal blasting force for each block can be calculated as follows:
V i = K Q 1 3 R α
where V i is the horizontal vibration velocity of the particle at the center of gravity of the i-th block (m/s), and Q is the amount of blasting charge. For simultaneous blasting, it is taken as the total amount, and for staggered blasting, it is taken as the maximum amount of any single segment (kg). R is the distance from the geometric center of explosive charge distribution in the blasting area to the observation point or building (m). K and α are coefficients and attenuation indices related to the terrain and geological conditions between the blasting point and the calculated protection object.
To simplify the problem, it can be assumed that when seismic waves propagate in a uniform elastic medium, particles perform simple harmonic motion, and the magnitude of vibration can be characterized by displacement, velocity, and acceleration. The mathematical relationships are as follows:
displacement   X = A sin ω t
velocity   V = d x d t = ω A sin ( ω t + π 2 )
acceleration a = d x 2 d t 2 = ω 2 A sin ( ω t + π )
From the above three mathematical formulas, it can be observed that the forms of displacement, velocity, and acceleration in simple harmonic motion are fundamentally similar, differing only in phase angle and amplitude. The ratio of acceleration amplitude to velocity amplitude is equal to the angular frequency. Thus, acceleration can be calculated from the measured or calculated particle vibration velocity as follows:
a = 2 π f V
Vibration acceleration, as a momentum, must be converted into an equivalent static load for calculations during slope stability analysis. The blasting vibration impact coefficient K c can be analyzed and calculated according to the following equation:
K c = β × a g
where a is acceleration; β is equivalent static, generally taken as 0.1 to 0.25; and g is gravitational acceleration.

Appendix A.1.4. Calculating the Safety Factor F s

(1)
Bishop Method
This method assumes that the tangential forces between soil blocks are negligible, and the formula is derived as follows:
F s = i = 1 n   c i b i + ( W i U i b i ) t a n φ i / m α i i = 1 n W i sin α i + i = 1 n Q e i R
where m α i = c o s α i + s i n α i t a n φ i / F s , F s is the factor of safety, W i is the weight of the soil strip, b i is the width of the soil strip, α i is the angle of the base of the soil strip, c i is the effective cohesion of the soil, φ i is the effective internal friction angle of the soil, R is the radius of the sliding arc, e i is the vertical distance from the center of the soil strip to the center of the sliding circle, and U i is the pore water pressure acting on the base of the soil strip.
K c   is the comprehensive seismic coefficient, which can be calculated as follows:
K = i [ c i L i + ( W i s e c α i U i L i ) ] 1 1 + t a n ϕ i t a n α i / K i ( W i s i n α i + Q i c o s α i )
where c i is the cohesion of the i-th block of rock; φ i is the internal friction angle of the i-th block of rock; W i is the weight of the i-th block; L i is the length of the base of the i-th block; Q i is the horizontal force acting on the i-th block, which may be the equivalent horizontal force from seismic blasting or hydrostatic pressure on a vertical crack; α i is the angle between the base of the i-th block and the horizontal plane of the coordinate axis; and U i is the horizontal force acting on the i-th block.
Since both sides of Equation (A14) contain K , iterative calculations are required to obtain more accurate results, and the convergence is fast. A large number of engineering examples have shown that the Bishop method yields results that are very close to those of other precise calculation methods, demonstrating high analysis accuracy.
(2)
Morgenstern–Price (M-P) Method
The basic assumption of the M-P method is that the ratio of the normal force to the shear force between blocks is expressed as the product of the inter-block force function f ( x ) and a specific proportional coefficient λ . Using the typical force and moment equilibrium conditions for the blocks, two equilibrium equations are derived, with the safety factor F s and the proportional coefficient λ being the two unknowns.
The relationship between the inter-block forces is as follows:
E i φ i = ϕ i 1 E i 1 φ i 1 + F s T i R i
where
φ i = ( s i n α i λ c o s α i ) t a n φ i + ( c o s α i + λ s i n α i ) F s
φ i 1 = ( s i n α i 1 λ c o s α i 1 ) t a n φ i 1 + ( c o s α i 1 + λ s i n α i 1 ) F s
ϕ i 1 = ( s i n α i 1 λ c o s α i 1 ) t a n φ i 1 + ( c o s α i 1 + λ s i n α i 1 ) F s
ϕ i 1 = ( s i n α i 1 λ c o s α i ) t a n φ i + ( c o s α i + λ s i n α i ) F s φ i 1
R i = [ W i c o s α i K c W i s i n α i + Q i c o s ( ω i α i ) U i ] t a n φ i + c i b i s e c α i
T i = W i s i n α i + K c W i c o s α i Q i s i n ( ω i α i )
In the above equation, R is the sum of the shear resistances provided by all forces acting on the block, excluding the inter-block forces, and T is the sum of the sliding forces produced by all forces.
Based on the inter-block forces at the ends being zero, i.e., E 0 = 0 and E n = 0 , the safety factor F s is derived as follows:
F s = i = 1 n 1 ( R i j = 1 n 1 ϕ j ) + R n i = 1 n 1 ( T i j = 1 n 1 ϕ j ) + T n
Similarly, the proportional coefficient λ is derived from the end-moment equilibrium as follows:
λ = i = 1 n [ b i ( E i + E i 1 ) t a n α i + K c W i h i + 2 s i n Q i ω i h i ] i = 1 n b i ( E i + E i 1 )
where W i is the weight of the block; K c is the seismic influence factor; u i is the average water pressure; E i and E i 1 are the inter-block normal stress; λ E i and λ E i 1 are the inter-block normal stress; b i is the block width; α i is the ground inclination angle; and c j and φ i are the effective mechanical parameters of the slip surface. This method is theoretically rigorous and applicable to slip surfaces of any shape, fully satisfying both force and moment equilibrium conditions.

Appendix A.2. Basic Test Results

Table A4. Slope profile information.
Table A4. Slope profile information.
ZoningProfile NumberTop Elevation (m)Bottom Elevation
(m)
Slope Height (m)Slope Angle (°)Main Lithology
II-1240523267936Sandstone, Phosphate Rock, Dolomite
IIII-1237323086515
IIIIII-1240323178616Quaternary, Sandstone, Phosphate Rock, Dolomite
IVIV-12405226514022Sandstone, Phosphate Rock, Dolomite
IV-2243723855216
VV-12358225510316
V-22328220612229Quaternary, Sandstone, Phosphate Rock, Dolomite
Table A5. Results of the uniaxial compressive strength test (natural, saturated).
Table A5. Results of the uniaxial compressive strength test (natural, saturated).
Rock Texture and ConditionSample
Number
Diameter
(cm)
Height
(cm)
Compressive Strength (MPa)Destruction Mode
Dolomite
(Saturated)
B14.8510.730.3Longitudinal splitting
B24.879.718.3Longitudinal splitting
B34.859.247.2Longitudinal splitting
B44.8510.334.5Longitudinal splitting
B54.8510.333.8Local longitudinal splitting
B64.8510.327.7Local longitudinal splitting
Mean32.0/
Dolomite
(Natural)
B14.859.944.0Longitudinal splitting
B24.859.663.1Longitudinal splitting
B34.859.039.5Longitudinal splitting
B44.889.668.4Local longitudinal splitting
B54.877.226.2Longitudinal splitting
B64.857.029.1Longitudinal splitting
Mean45.1/
Phosphorite
(Saturated)
L14.8610.340.9Longitudinal splitting
L24.858.936.0Longitudinal splitting
L34.889.648.0Longitudinal splitting
L44.889.636.3Longitudinal splitting
L54.889.146.2Longitudinal splitting
L64.889.128.2Longitudinal splitting
Mean39.3/
Phosphorite
(Natural)
L14.859.143.7Longitudinal splitting
L24.848.465.7Longitudinal splitting
L3///Longitudinal splitting
L44.8510.346.8Longitudinal splitting
L54.8710.361.0Longitudinal splitting
L64.8710.344.0Longitudinal splitting
Mean52.2/
Sandstone
(Saturated)
S14.8810.246.2Longitudinal splitting
S24.8710.231.1Longitudinal splitting
S34.8710.237.9Longitudinal splitting
Mean38.4/
Sandstone
(Natural)
S14.8810.060.9Local longitudinal splitting
S24.889.956.6Longitudinal splitting
S34.8510.266.0Longitudinal splitting
Mean61.2/
Table A6. Compression deformation test results.
Table A6. Compression deformation test results.
Rock Texture or LithologySample NumberShear Modulus of Elasticity
E50 (GPa)
Poisson’s Ratio
μ50
Tangent Modulus of Elasticity
Ee (GPa)
Poisson’s Ratio
μe
Destruction Mode
DolomiteB129.00.2530.20.36Longitudinal splitting
B222.60.3223.40.40Longitudinal splitting
B338.40.2235.30.24Longitudinal splitting
B442.70.2938.90.41Longitudinal splitting
B538.50.2342.80.24Local longitudinal splitting
B640.50.1934.00.16Longitudinal splitting
Mean35.30.2534.10.31/
PhosphoriteL131.90.2330.40.24Longitudinal splitting
L250.40.1952.10.22Longitudinal splitting
L324.30.2224.40.26Longitudinal splitting
L464.60.2554.30.23Longitudinal splitting
L548.10.2265.50.27Longitudinal splitting
L619.00.2228.70.25Longitudinal splitting
Mean39.70.2242.570.24/
Quartz SandstoneS146.20.2028.20.24Longitudinal splitting
S231.10.2633.80.24Longitudinal splitting
S337.90.2537.70.34Local longitudinal splitting
Mean38.40.2433.230.27/
Table A7. Split tensile test results.
Table A7. Split tensile test results.
LithologySample NumberDiameter (cm)Height (cm) R t (MPa)
Dolomite
(Natural)
B14.884.526.27
B24.854.308.41
B34.852.967.01
Mean4.863.937.23
Dolomite (Saturated)B14.854.705.10
B24.853.005.95
B34.854.255.34
Mean4.853.985.46
Phosphate
Rock
(Natural)
L14.864.651.35
L24.854.281.85
L34.854.301.67
L44.872.967.47
L54.884.257.34
L64.883.027.03
Mean4.873.914.45
Phosphate
Rock
(Saturated)
L14.852.961.22
L24.884.251.06
L34.853.021.34
L44.853.506.06
L54.854.806.62
L64.853.426.83
Mean4.863.663.85
Sandstone
(Natural)
S14.884.047.28
S24.883.989.36
S34.883.988.92
Mean4.884.008.52
Sandstone
(Saturated)
S14.854.555.66
S24.884.805.95
S34.884.505.91
Mean4.874.625.84
Table A8. Shear strength results.
Table A8. Shear strength results.
LithologySample
Number
Length (cm)Width (cm)Shear Area (cm2)Shear Stress τ (kPa)Internal Friction
Angle φ (°)
Cohesion C (MPa)
DolomiteB15.185.2827.3558.8140.23.36
5.305.3028.0944.58
B24.905.2825.8728.38
5.105.3027.0330.62
B35.285.3027.9813.70
5.305.3028.0917.24
B45.325.2828.0930.54
5.305.3028.0928.82
B54.925.2525.8316.54
5.275.3428.1420.11
B65.305.3028.0911.34
5.255.3027.829.62
Phosphate RockL45.305.3528.35150.0942.78.90
5.305.4028.62137.34
L55.305.3528.35126.22
5.305.3228.2064.62
L65.355.3828.7887.76
5.355.3528.6271.57
SandstoneS15.305.3028.0969.5941.36.09
5.285.2527.7288.51
S25.325.3028.2050.35
5.305.3228.2044.73
S35.325.3228.3020.16
5.325.3228.3027.54
5.285.2527.7288.51
S25.325.3028.2050.35
5.305.3228.2044.73
S35.325.3228.3020.16
5.325.3228.3027.54
Table A9. Determination of slope grade.
Table A9. Determination of slope grade.
Slope LocationDivision MethodGradeRemarks
Southwest Slope of First Mining AreaSlope Height GradeLow SlopeSlope Height 79 m
Slope Hazard GradeIBased on Comprehensive Mine Site Conditions, Grade I is Assigned
Slope Engineering Safety GradeIIBased on Comprehensive Slope Height Grade, Slope Hazard Grade and Mine Site Conditions, Grade II is Assigned
Southwest Slope of Second Mining AreaSlope Height GradeLow SlopeSlope Height 92 m
Slope Hazard GradeIBased on Comprehensive Mine Site Conditions, Grade I is Assigned
Slope Engineering Safety GradeIIBased on Comprehensive Slope Height Grade, Slope Hazard Grade and Mine Site Conditions, Grade II is Assigned
South Slope of Third Mining AreaSlope Height GradeLow SlopeSlope Height 85 m
Slope Hazard GradeIBased on Comprehensive Mine Site Conditions, Grade I is Assigned
Slope Engineering Safety GradeIIBased on Comprehensive Slope Height Grade, Slope Hazard Grade and Mine Site Conditions, Grade II is Assigned
South Slope of Fourth Mining AreaSlope Height GradeMiddle SlopeSlope Height 140 m
Slope Hazard GradeIBased on Comprehensive Mine Site Conditions, Grade I is Assigned
Slope Engineering Safety GradeIBased on Comprehensive Slope Height Grade, Slope Hazard Grade and Mine Site Conditions, Grade I is Assigned
Southern Area SlopeSlope Height GradeMiddle SlopeSlope Height 147 m
Slope Hazard GradeIBased on Comprehensive Mine Site Conditions, Grade I is Assigned
Slope Engineering Safety GradeIBased on Comprehensive Slope Height Grade, Slope Hazard Grade and Mine Site Conditions, Grade I is Assigned
Table A10. Design safety factor.
Table A10. Design safety factor.
Slope Area (m2)Slope Engineering Safety GradeSafety Factor for Slope Engineering Design
Load Combination ILoad Combination IILoad Combination III
Southwest Slope of First Mining Area (76,497)II1.20–1.151.18–1.131.15–1.10
Southwest Slope of Second Mining Area (159,903)II1.20–1.151.18–1.131.15–1.10
South Slope of Third Mining Area (425,903)II1.20–1.151.18–1.131.15–1.10
South Slope of Fourth Mining Area (390,941)I1.25–1.201.23–1.181.20–1.15
Southern Area Slope (273,289)I1.25–1.201.23–1.181.20–1.15
Table A11. Part of GNSS data.
Table A11. Part of GNSS data.
Point∆X∆Y∆Z∑X∑Y∑ZTime
BW12−0.22−0.24−0.66−0.1433.3270.552024/11/3 0:00
BW06−0.45−0.43−1.24−0.1133.9321.0722024/11/3 0:00
BW070.92−0.84−1.87−1.1985.4753.9942024/11/3 0:00
BW110.03−0.63−1.04−0.4883.8991.8252024/11/3 0:00
BW101.21−0.33−2.71−1.8095.854.3462024/11/3 0:00
BW041.34−0.51−1.82−0.6724.3164.0772024/11/3 0:00
BW09−0.12−0.54−0.460.4721.437−0.2492024/11/3 0:00
BW130.35−2.3−1.393.1669.1444.5172024/11/3 0:00
BW15−0.59−0.62−0.130.4082.189−0.2492024/11/3 0:00
BW050.56−0.87−1.44−0.6673.7182.6262024/11/3 0:00
BW23−0.53−0.83−0.511.5450.357−0.842024/11/3 0:00
BW01−0.25−0.73−0.460.7432.2180.2082024/11/3 0:00
BW021.06−0.41−2.98−3.3448.6046.2172024/11/3 0:00
BW220.13−0.2−1.17−0.822.1591.7192024/11/3 0:00
BW03−0.27−1.15−1.55−0.0163.1680.8742024/11/3 0:00
BW200.550.37−2.83−2.5776.8673.6152024/11/3 0:00
BW24−0.28−0.44−0.22−0.0250.8270.1032024/11/3 0:00
BW18−0.290.46−1.13−0.741.301−0.3122024/11/3 0:00
BW160.64−0.73−0.88−0.3854.5472.5562024/11/3 0:00
BW080.6−0.59−1.990.0653.7083.2982024/11/3 0:00
BW170.2−0.1−1.74−1.2965.332.6692024/11/3 0:00
BW060.10.38−0.67−0.641−0.9380.12024/11/3 1:00
BW24−0.15−0.06−0.74−1.0392.3221.2152024/11/3 1:00

Appendix A.3. Implementation Details and Software Environment

Appendix A.3.1. Software and Programming Languages

The algorithms for processing GNSS, SAR, and video data were implemented using a combination of the following platforms and programming languages:
MATLAB R2023a: Used for numerical computations, matrix operations, and implementation of the Bishop and Morgenstern–Price (M-P) methods for slope stability analysis. Key toolboxes: Image Processing Toolbox (for SAR data alignment), Statistics and Machine Learning Toolbox (for outlier removal and probabilistic analysis), and Mapping Toolbox (for coordinate transformations).
Python 3.9: NumPy and SciPy for convex hull algorithms and displacement calculations. OpenCV for video data synchronization, lens distortion correction, and SIFT feature extraction. GDAL for geospatial data handling and DTM construction. scikit-learn for k-nearest neighbors (k-NN) filtering in SAR data.
Commercial Software: DIMINE 2016 version for stratigraphic model visualization and fault analysis (Figure 4 and Figure 5).

Appendix A.3.2. Script Availability

Custom scripts for the convex hull-displacement dual-criterion algorithm Equations (12)–(18) and multi-source data fusion (Equations (2)–(11) can be provided upon request via correspondence to Yuyin Cheng (cheng.yuyin@foxmail.com).

Appendix A.3.3. Hardware Specifications

Workstation: Intel Xeon W-2295 (18 cores), 128 GB RAM, NVIDIA RTX A6000 GPU.
Field deployment: Ruggedized laptops (Panasonic Toughbook) for real-time monitoring.

Appendix A.3.4. Reproducibility Note

All input parameters (e.g., shear strength and slope geometry) are provided in Table A4, Table A5, Table A6, Table A7, Table A8, Table A9 and Table A10. Random seed values for probabilistic analyses (Section 5.2) were fixed (seed = 42 in Python/NumPy).

References

  1. Lumbroso, D.; Davison, M.; Body, R.; Petkovšek, G. Modelling the Brumadinho tailings dam failure, the subsequent loss of life and how it could have been reduced. Nat. Hazards Earth Syst. Sci. Discuss. 2020, 2020, 1–24. [Google Scholar] [CrossRef]
  2. Nava, L.; Carraro, E.; Reyes-Carmona, C.; Puliero, S.; Bhuyan, K.; Rosi, A.; Monserrat, O.; Floris, M.; Meena, S.R.; Galve, J.P. Landslide displacement forecasting using deep learning and monitoring data across selected sites. Landslides 2023, 20, 2111–2129. [Google Scholar] [CrossRef]
  3. Xi, N.; Yang, Q.; Sun, Y.; Mei, G. Machine learning approaches for slope deformation prediction based on monitored time-series displacement data: A comparative investigation. Appl. Sci. 2023, 13, 4677. [Google Scholar] [CrossRef]
  4. Gupta, G.; Sharma, S.K.; Singh, G.; Kishore, N. Numerical modelling-based stability analysis of waste dump slope structures in open-pit mines-a review. J. Inst. Eng. Ser. D 2021, 102, 589–601. [Google Scholar] [CrossRef]
  5. Uusitalo, L.; Lehikoinen, A.; Helle, I.; Myrberg, K. An overview of methods to evaluate uncertainty of deterministic models in decision support. Environ. Model. Softw. 2015, 63, 24–31. [Google Scholar] [CrossRef]
  6. Kirchsteiger, C. On the use of probabilistic and deterministic methods in risk analysis. J. Loss Prev. Process Ind. 1999, 12, 399–419. [Google Scholar] [CrossRef]
  7. Soeters, R.; van Westen, C.J. Slope instability recognition, analysis, and zonation. In Landslides, Investigation and Mitigation; National Academy Press: Washington, DC, USA, 1996; pp. 129–177. [Google Scholar]
  8. Ullah, S.; Khan, M.U.; Rehman, G. A brief review of the slope stability analysis methods. Geol. Behav 2020, 4, 73–77. [Google Scholar] [CrossRef]
  9. Cai, F.; Ugai, K. Numerical analysis of rainfall effects on slope stability. Int. J. Geomech. 2004, 4, 69–78. [Google Scholar] [CrossRef]
  10. Li, L.; Tang, C.; Zhu, W.; Liang, Z. Numerical analysis of slope stability based on the gravity increase method. Comput. Geotech. 2009, 36, 1246–1258. [Google Scholar] [CrossRef]
  11. Nuric, A.; Nuric, S.; Kricak, L.; Husagic, R. Numerical methods in analysis of slope stability. Int. J. Sci. Eng. Investig. 2013, 2, 41–48. [Google Scholar]
  12. Kainthola, A.; Verma, D.; Thareja, R.; Singh, T. A review on numerical slope stability analysis. Int. J. Eng. Sci. Technol. Res. 2013, 2, 1315–1320. [Google Scholar]
  13. Eberhardt, E. Rock slope stability analysis–utilization of advanced numerical techniques. Earth Ocean Sci. UBC 2003, 41. [Google Scholar] [CrossRef]
  14. Salmi, E.F.; Hosseinzadeh, S. Slope stability assessment using both empirical and numerical methods: A case study. Bull. Eng. Geol. Environ. 2015, 74, 13–25. [Google Scholar] [CrossRef]
  15. Harabinová, S.; Kotrasová, K.; Kormaníková, E.; Hegedüsová, I. Analysis of slope stability. Civ. Environ. Eng. 2021, 17, 192–199. [Google Scholar] [CrossRef]
  16. Kostić, S.; Vasović, N.; Sunarić, D. Slope stability analysis based on experimental design. Int. J. Geomech. 2016, 16, 04016009. [Google Scholar] [CrossRef]
  17. Cao, J.; Zaman, M.M. Analytical method for analysis of slope stability. Int. J. Numer. Anal. Methods Geomech. 1999, 23, 439–449. [Google Scholar] [CrossRef]
  18. Gao, W.; Ge, S. A comprehensive review of slope stability analysis based on artificial intelligence methods. Expert Syst. Appl. 2023, 239, 122400. [Google Scholar] [CrossRef]
  19. Yang, Z.; Li, T.; Dai, M. Reliability analysis method for slope stability based on sample weight. Water Sci. Eng. 2009, 2, 78–86. [Google Scholar]
  20. Yang, R.; Alonso, E.; Tabba, M. Application of risk analysis to the prediction of slope instability. Can. Geotech. J 1977, 14, 540–553. [Google Scholar] [CrossRef]
  21. Li, D.; Yang, Z.; Cao, Z.; Zhang, L. Area failure probability method for slope system failure risk assessment. Comput. Geotech. 2019, 107, 36–44. [Google Scholar] [CrossRef]
  22. Li, L.; Wang, Y.; Cao, Z. Probabilistic slope stability analysis by risk aggregation. Eng. Geol. 2014, 176, 57–65. [Google Scholar] [CrossRef]
  23. Shah, V.; Vigliorolo, E. Risk-Based Slope Hazard Evaluation System. In Geo-Risk 2017; ASCE Press: Reston, VA, USA, 2017; pp. 226–235. [Google Scholar]
  24. Dai, Y.; Fredlund, D.; Stolte, W. A probabilistic slope stability analysis using deterministic computer software. In Probabilistic Methods in Geotechnical Engineering; CRC Press: Boca Raton, FL, USA, 2020; pp. 267–274. [Google Scholar]
  25. Dyson, A.P.; Tolooiyan, A. Comparative approaches to probabilistic finite element methods for slope stability analysis. Simul. Model. Pract. Theory 2020, 100, 102061. [Google Scholar] [CrossRef]
  26. Du, S.; Saroglou, C.; Chen, Y.; Lin, H.; Yong, R. A new approach for evaluation of slope stability in large open-pit mines: A case study at the Dexing Copper Mine, China. Environ. Earth Sci. 2022, 81, 102. [Google Scholar] [CrossRef]
  27. Zhang, J.; Wang, Z.; Zhang, G.; Xue, Y. Probabilistic prediction of slope failure time. Eng. Geol. 2020, 271, 105586. [Google Scholar] [CrossRef]
  28. Li, S.; Qiu, C.; Huang, J.; Guo, X.; Hu, Y.; Mugahed, A.-S.Q.; Tan, J. Stability analysis of a high-steep dump slope under different rainfall conditions. Sustainability 2022, 14, 11148. [Google Scholar] [CrossRef]
  29. Ren, Y.; Chen, X.; Shang, Y. Study on the influence of rainfall infiltration on the stability of dump slope. Desalination Water Treat. 2024, 319, 100492. [Google Scholar] [CrossRef]
  30. Sun, Q.; Wei, C.; Sha, X.; Zhou, B.; Zhang, G.; Xu, Z.; Cao, L. Study on the influence of water–rock interaction on the stability of schist slope. Sustainability 2020, 12, 7141. [Google Scholar] [CrossRef]
  31. Atzeni, C.; Barla, M.; Pieraccini, M.; Antolini, F. Early warning monitoring of natural and engineered slopes with ground-based synthetic-aperture radar. Rock Mech. Rock Eng. 2015, 48, 235–246. [Google Scholar] [CrossRef]
  32. Le Roux, R.; Sepehri, M.; Khaksar, S.; Murray, I. Slope Stability Monitoring Methods and Technologies for Open-Pit Mining: A Systematic Review. Mining 2025, 5, 32. [Google Scholar] [CrossRef]
  33. Lian, X.; Li, Z.; Yuan, H.; Hu, H.; Cai, Y.; Liu, X. Determination of the stability of high-steep slopes by global navigation satellite system (GNSS) real-time monitoring in long wall mining. Appl. Sci. 2020, 10, 1952. [Google Scholar] [CrossRef]
  34. Griffiths, D.; Fenton, G.A. Probabilistic slope stability analysis by finite elements. J. Geotech. Geoenviron. Eng. 2004, 130, 507–518. [Google Scholar] [CrossRef]
  35. Zhang, W.; Ran, B.; Gu, X.; Sun, G.; Zou, Y. Probabilistic stability analysis of a layered slope considering multi-factors in spatially variable soils. Nat. Hazards 2024, 120, 11209–11238. [Google Scholar] [CrossRef]
  36. Alganci, U.; Besol, B.; Sertel, E. Accuracy assessment of different digital surface models. ISPRS Int. J. Geo-Inf. 2018, 7, 114. [Google Scholar] [CrossRef]
  37. Barber, C.B.; Dobkin, D.P.; Huhdanpaa, H. The quickhull algorithm for convex hulls. ACM Trans. Math. Softw. (TOMS) 1996, 22, 469–483. [Google Scholar] [CrossRef]
  38. Neal, A. Ground-penetrating radar and its use in sedimentology: Principles, problems and progress. Earth-Sci. Rev. 2004, 66, 261–330. [Google Scholar] [CrossRef]
  39. Young, R.A.; Sun, J. Revealing stratigraphy in ground-penetrating radar data using domain filtering. Geophysics 1999, 64, 435–442. [Google Scholar] [CrossRef]
  40. Zuo, M.; Mitri, R.S.; Gai, I.; Brighi, G.; Tortora, P. Spectral properties of bistatic radar signals using the ray tracing technique and a facet approach. Aerospace 2024, 11, 615. [Google Scholar] [CrossRef]
  41. GB/T 2423.8-1995; Environmentaltesting for Electric and Electronic Products—Part 2:Test Methods—Test Ed:Free Fall. National Standards of the People’s Republic of China: Beijing, China, 1995.
  42. GB 35114; Technical Requirements for Information Security of Video Surveillance Network System for Public Security. National Standards of the People’s Republic of China: Beijing, China, 2017.
  43. GB 18306-2015; Seismic Ground Motion Parameter Zonation Map of China. National Standards of the People’s Republic of China: Beijing, China, 2015.
  44. GB 50330-2013; Technical Code for Building Slope Engineering. National Standards of the People’s Republic of China: Beijing, China, 2013.
  45. GB 6722-2014; Safety Regulations for Blasting. National Standards of the People’s Republic of China: Beijing, China, 2014.
  46. GB 51016-2014; Technical Code for Non-Coal Open-Pitmine Slope Engineering. National Standards of the People’s Republic of China: Beijing, China, 2014.
  47. Romana, M.R. A geomechanical classification for slopes: Slope mass rating. In Rock Testing and Site Characterization; Elsevier: Amsterdam, The Netherlands, 1993; pp. 575–600. [Google Scholar]
  48. Pantelidis, L. Rock slope stability assessment through rock mass classification systems. Int. J. Rock Mech. Min. Sci. 2009, 46, 315–325. [Google Scholar] [CrossRef]
  49. Loáiciga, H.A. Groundwater and earthquakes: Screening analysis for slope stability. Eng. Geol. 2015, 193, 276–287. [Google Scholar] [CrossRef]
Figure 1. The overall framework of the proposed experience model and data-driven collaborative open-pit slope stability analysis.
Figure 1. The overall framework of the proposed experience model and data-driven collaborative open-pit slope stability analysis.
Applsci 15 09278 g001
Figure 2. The distribution of GNSS observation points.
Figure 2. The distribution of GNSS observation points.
Applsci 15 09278 g002
Figure 3. The distribution of video observation points.
Figure 3. The distribution of video observation points.
Applsci 15 09278 g003
Figure 4. Visualization of single strata and combined visualization of multiple strata.
Figure 4. Visualization of single strata and combined visualization of multiple strata.
Applsci 15 09278 g004aApplsci 15 09278 g004b
Figure 5. Composite diagram of current surface and solid model in the mining area.
Figure 5. Composite diagram of current surface and solid model in the mining area.
Applsci 15 09278 g005
Figure 6. Variation of values for A S t .
Figure 6. Variation of values for A S t .
Applsci 15 09278 g006
Table 1. Calculation parameters for the blast vibration impact coefficient.
Table 1. Calculation parameters for the blast vibration impact coefficient.
Calculation ParametersCoefficient KTotal Amount of Explosive Charge for Simultaneous Blasting Q (kg)Safety Distance R i (m)Coefficient α
Calculation Values250500601.5
Table 2. Safety factor calculation results for the slope in the first mining area.
Table 2. Safety factor calculation results for the slope in the first mining area.
ProfileSlope Angle (°)Slope Height (m)Load CombinationSafety FactorSlope GradeStandard Required ValuesCompliance with Standards
Circular Arc Failure Analysis MethodSlip-Wedge
Method
BishopM-PBishopM-P
I-13679I3.1753.1673.0063.110II1.20–1.15Yes
II3.0603.0522.8993.000II1.18–1.13Yes
III2.7412.7352.6052.693II1.15–1.10Yes
Table 3. Safety factor calculation results for the slope in the second mining area.
Table 3. Safety factor calculation results for the slope in the second mining area.
ProfileSlope Angle (°)Slope Height (m) Load CombinationSafety FactorSlope GradeStandard Required Values Compliance with Standards
Circular Arc Failure Analysis MethodSlip-Wedge Method
BishopM-PBishopM-P
II-11565I3.8383.8353.3203.541II1.20–1.15Yes
II3.8023.7973.2923.519II1.18–1.13Yes
III3.4403.4313.1593.341II1.15–1.10Yes
Table 4. Safety factor calculation results for the slope in the third mining area.
Table 4. Safety factor calculation results for the slope in the third mining area.
ProfileSlope Angle (°)Slope Height (m)Load CombinationSafety FactorSlope GradeStandard Required Values Compliance with Standards
Circular Arc Failure Analysis MethodSlip-Wedge Method
BishopM-PBishopM-P
III-11686I2.5012.4932.3542.432II1.20–1.15Yes
II2.3862.3792.2542.324II1.18–1.13Yes
III2.0772.0741.9712.034II1.15–1.10Yes
Table 5. Safety factor calculation results for the slope in the fourth mining area.
Table 5. Safety factor calculation results for the slope in the fourth mining area.
ProfileSlope Angle (°)Slope Height (m)Load CombinationSafety FactorSlope GradeStandard Required ValuesCompliance with Standards
Circular Arc Failure Analysis MethodSlip-Wedge Method
BishopM-PBishopM-P
IV-122140I1.8611.8571.7741.813I1.25–1.20Yes
II1.8011.7961.7171.755I1.23–1.18Yes
III1.6311.6281.5541.606I1.20–1.15Yes
IV-21652I3.6313.6273.3513.476I1.25–1.20Yes
II3.5673.5633.2983.418I1.23–1.18Yes
III2.9522.9492.7572.860I1.20–1.15Yes
Table 6. Safety factor calculation results for the slope in the southern area.
Table 6. Safety factor calculation results for the slope in the southern area.
ProfileSlope Angle (°)Slope Height (m)Load CombinationSafety FactorSlope GradeStandard Required ValuesCompliance with Standards
Circular Arc Failure Analysis MethodSlip-Wedge Method
BishopM-PBishopM-P
V-116103I1.6881.6881.4771.537I1.25–1.20Yes
II1.6381.6371.4391.498I1.23–1.18Yes
III1.4931.4911.4001.416I1.20–1.15Yes
V-229122I1.6311.6261.5321.585I1.25–1.20Yes
II1.5891.5841.4921.546I1.23–1.18Yes
III1.4671.4631.3791.432I1.20–1.15Yes
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Cheng, Y.; Hou, K. Open-Pit Slope Stability Analysis Integrating Empirical Models and Multi-Source Monitoring Data. Appl. Sci. 2025, 15, 9278. https://doi.org/10.3390/app15179278

AMA Style

Cheng Y, Hou K. Open-Pit Slope Stability Analysis Integrating Empirical Models and Multi-Source Monitoring Data. Applied Sciences. 2025; 15(17):9278. https://doi.org/10.3390/app15179278

Chicago/Turabian Style

Cheng, Yuyin, and Kepeng Hou. 2025. "Open-Pit Slope Stability Analysis Integrating Empirical Models and Multi-Source Monitoring Data" Applied Sciences 15, no. 17: 9278. https://doi.org/10.3390/app15179278

APA Style

Cheng, Y., & Hou, K. (2025). Open-Pit Slope Stability Analysis Integrating Empirical Models and Multi-Source Monitoring Data. Applied Sciences, 15(17), 9278. https://doi.org/10.3390/app15179278

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop