Next Article in Journal
Dissolution Behavior of Sodium Phosphate in a Na3PO4–Na2WO4–NaOH Solution System
Next Article in Special Issue
Effects of Accumulated Damage on the Dynamic Properties of Coal Measures Sandstone
Previous Article in Journal
Effects of Recycled Sponge Iron on Phosphorus Recovery from Polluted Water
Previous Article in Special Issue
Study on the Stress Variation Law of Inclined Surrounding Rock Roadway under the Influence of Mining
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Assessment of Machine Learning Models for the Prediction of Rate-Dependent Compressive Strength of Rocks

1
School of Civil Engineering and Architecture, Wuhan University of Technology, Wuhan 430070, China
2
School of Civil Engineering, Xinyang College, Xinyang 464000, China
3
School of Civil Engineering, Southeast University, Nanjing 211189, China
*
Author to whom correspondence should be addressed.
Minerals 2022, 12(6), 731; https://doi.org/10.3390/min12060731
Submission received: 17 April 2022 / Revised: 3 June 2022 / Accepted: 5 June 2022 / Published: 8 June 2022
(This article belongs to the Special Issue Failure Characteristics of Deep Rocks)

Abstract

:
The prediction of rate-dependent compressive strength of rocks in dynamic compression experiments is still a notable challenge. Four machine learning models were introduced and employed on a dataset of 164 experiments to achieve an accurate prediction of the rate-dependent compressive strength of rocks. Then, the relative importance of the seven input features was analyzed. The results showed that compared with the extreme learning machine (ELM), random forest (RF), and the original support vector regression (SVR) models, the correlation coefficient R2 of prediction results with the hybrid model that combines the particle swarm optimization (PSO) algorithm and SVR was highest in both the training set and the test set, both exceeding 0.98. The PSO-SVR model obtained a higher prediction accuracy and a smaller prediction error than the other three models in terms of evaluation metrics, which showed the possibility of the model as a rate-dependent compressive strength prediction tool. Additionally, besides the static compressive strength, the stress rate is the most important influence factor on the rate-dependent compressive strength of the rock among the listed input parameters. Moreover, the strain rate has a positive effect on the rock strength.

1. Introduction

Strain rate is one of the most important factors affecting the dynamic properties of rocks [1]. Especially for engineering projects involving blasting and excavation, the stress waves generated by blasting are different from the static loads acting on rocks and are complex dynamic processes. In the blasting analysis of rock tunnels, the dynamic properties of rocks show obvious strain rate dependence, and the effect of strain rate should be further considered [2,3,4]. Many studies have shown that the mechanical properties of rock materials change significantly as the strain rate increases [5,6]. Therefore, it is of great theoretical and practical importance to study the compressive strength of rocks under different strain rate conditions. Moreover, understanding the rate dependence of rock strength is of great importance to rock engineering design and construction [7,8].
As a key indicator of the mechanical properties of rocks, the current methods for determining the compressive strength of rocks rely on laboratory tests such as static compression tests and the Split Hopkinson Pressure Bar (SHPB) test [9,10]. These test methods investigate the rate dependence of the compressive strength of rocks at low and high strain rates, respectively. However, these methods are cumbersome and time-consuming to operate. Moreover, it is difficult to use these test methods to directly study the compressive strength of rocks at moderate strain rates. The study of the mechanical properties of rocks at moderate strain rates can be of great help in understanding the mechanism of excavation-induced geohazards (e.g., rock bursts) [11,12,13]. Some scholars have attempted to modify the test setup to control the intermediate strain rate [14], but it remains a challenging task. This is because there are many influencing factors, and these factors are complexly coupled with each other. Although numerical simulations have been applied in this area [15,16,17], the accurate prediction of rock strength depends on a reasonable intrinsic model and reliable model calibration. Therefore, there is an urgent need for a simple, fast, and reliable intelligent method to predict the compressive strength of rocks at different strain rates and to facilitate understanding of the rate dependence of rock strength.
With the development of artificial intelligence, some intelligent methods such as machine learning have been used to solve some complex engineering problems. In recent years, machine learning techniques such as artificial neural network (ANN), support vector machine (SVM), random forest (RF), extreme learning machine (ELM), and other models have been employed to predict concrete compressive strength and have achieved good prediction behavior [18,19,20,21,22,23,24,25]. Similarly, some intelligent models have been introduced to predict the mechanical properties and stability of rocks, with significant progress being made by numerous scholars [26,27,28,29,30,31,32,33,34]. For example, Ebrahim, et al. [35] developed a model tree approach to predict the uniaxial compressive strength and elastic modulus of carbonate rocks, which provided better prediction results. Li, et al. [36] utilized the Least squares support vector machine model to predict the compressive strength and shear strength of rocks, and the correlation coefficient R2 of the predicted results exceeded 0.99. Yılmaz, et al. [37] employed an ANN to predict the compressive strength and elastic modulus of rocks. Compared with the conventional statistical model, the ANN network obtained a higher prediction accuracy. Ehsan, et al. [38] proposed a particle swarm optimization (PSO) algorithm-based ANN model with four input parameters including point load index, Schmidt hammer rebound number, P-wave velocity, and dry density, to predict the uniaxial compressive strength of rocks. Compared with the conventional ANN, the hybrid optimized model reached higher prediction accuracy with R2 = 0.97. Gupta et al. [39] employed five machine learning models on 170 samples to predict rock strength, and the proposed density-weighted least squares twin support vector regression (SVR) model showed the best predictive performance compared with the other four models in terms of evaluation indicators. Hany et al. [40] developed two models, random forest and functional network, to predict the unconstrained compressive strength of rocks using six parameters: drilling torque, weight on bit, mud pumping rate, stand-pipe pressure, drill string rotating speed, and the rate of penetration. The model results showed that the developed RF and functional network models can provide accurate uniaxial compression strength estimations from drilling data in real-time. The application of the model saves time and costs and provides data support and guidance to improve well stability.
Although many successful applications have been achieved using methods such as empirical formulas [41] and intelligent models to estimate the compressive strength of rocks [42,43], it is undeniable that the relevant research has mainly focused on static compressive strength, less research has been performed on the rate-independent compressive strength of rocks, and more research is needed to improve the understanding of this problem. In particular, further analysis is required to understand the compressive strength of rocks under rate independence to improve the ability to predict the rate dependence of rock strength. Fortunately, these successful applications provide a research base and important guidance for the further extension of machine learning model applications to rock dynamics. To this end, this paper attempts to propose a hybrid model which combines a PSO algorithm and SVR to predict the rate-independent compressive strength of rocks. In addition, a comparative analysis with three other models (ELM, random forest, and SVR) is performed, providing new insights into the rate-dependence of rock strength.

2. Method and Models

2.1. Extreme Learning Machine

ELM is an algorithm based on a single hidden layer feedforward neural network, in which the input weights and biases are randomly assigned, and the output weights are calculated using the Moore–Penrose generalized inverse within the framework of the least-squares criterion [44,45,46]. Therefore, ELM has the advantage of fast convergence and is less likely to fall into local extremes than traditional neural networks based on gradient descent learning theory [47,48]. The network architecture of ELM is shown in Figure 1. Given a dataset containing N arbitrary samples (xi, ti), the number of nodes in the input layer is n and the number of nodes in the output layer is m, where x i = x i 1 , x i 2 , , x i n R n , t i = t i 1 , t i 2 , , t i m R m . For a neural network with an activation function g(x) and a single hidden layer with K hidden nodes, the expression is shown below.
i = 1 K β i g w i , x i + b i = o j   j = 1 , 2 , , N
where w i = [ w i 1 , w i 2 , , w i n ] T is the weight vector between the ith hidden node and the input node; β i = [ β i 1 , β i 2 , , β i n ] T is the weight vector between the ith hidden node and the output node; bi is the bias of the ith hidden node; w i , x i is the inner product of wi and x; oj is the output value.
It is known that the learning goal of a single hidden layer neural network is to minimize the error in the output, i.e., there exists βi, wi, and bi satisfying the following conditions.
i = 1 K β i g w i , x i + b i = t j   j = 1 , 2 , , N
Equation (2) is expressed in matrix form as follows.
H β = T

2.2. Random Forest

Random forest is a variant of the bagging integration algorithm to improve the model. The random forest uses decision trees as the base learner and builds a random forest model by integrating several decision trees, while the random forest introduces a random selection of feature attributes in the training process of the decision trees [49,50]. Based on this mechanism, random forest inherits the advantages of sample perturbation from the bagging integration algorithm and improves on it by introducing the perturbation strategy of a random selection of attributes. Therefore, for the same data set, the double randomness of the random forest provides a better generalization ability and overfitting resistance. As shown in Figure 2, the algorithm principle of random forest can be expressed as follows.
Y = 1 N i = 1 N F i X
where X is the input feature vector, Y is the prediction result, and N is the number of regression tree models built.

2.3. Support Vector Regression

Support vector machines can effectively solve classification and complex nonlinear regression problems [52]. When they are applied to regression problems, the basic idea is to find an optimal classification surface that minimizes the error of all training samples from that classification surface [53,54,55]. Assuming that there is a set of training samples x i , y i , i = 1 , 2 , , l R n × R , a linear regression function is established in the high-dimensional feature space as follows.
f x = w ϕ x + b
where ϕ x is a nonlinear mapping function. By finding w as well as b according to the structural risk minimization principle, the problem of solving the regression function is transformed into the optimization problem of the function [56,57].
min 1 2 w 2 + C i = 1 l ( ξ i + ξ i * ) s . t . y i w ϕ ( x ) b ε + ξ i y i + w ϕ ( x ) + b ε + ξ i * ξ i , ξ i * 0
where C is the penalty factor. A larger C indicates a larger penalty for samples with a training error greater than ε; ε specifies the error requirement of the regression function, and a smaller ε indicates a smaller error of the regression function. ξ i and ξ i * are slack variables.
This optimization problem can be solved by introducing the Lagrange function and transforming it into a pairwise form. The regression function can eventually be expressed as:
f x = i = 1 l α i α i * K x i , x + b
where K x i , x = ϕ x i ϕ x is the kernel function. In this paper, the radial basis function (RBF) with a wide convergence domain is selected as the kernel function.

2.4. Support Vector Regression with Particle Swarm Optimization

For the SVR model with RBF function, the combined values of C and g have a significant effect on the predictive ability of the model. Some intelligent algorithms such as grid search, genetic algorithm, and PSO algorithm, are used to optimize the model. Considering the advantages of the PSO algorithm with fewer parameters and higher efficiency, a PSO-based SVR model is proposed to improve the model performance of the original SVR. The PSO algorithm can be represented as follows. In addition, the training and testing process of the hybrid model is shown in Figure 3.
v i k + 1 = ω · v i k + c 1 r 1 ( p b e s t i k x i k ) + c 2 r 2 ( g b e s t i k x i k ) x i k + 1 = x i k + v i k + 1
where ω is the initial weight, k is the number of iterations, v i k and x i k are the velocity and position vectors of the particle, respectively, c1 and c2 are the learning factors, r1 and r2 are arbitrary values between [0, 1], p b e s t i k is the best position passed by the i-th particle, and g b e s t i k is the global best position.

3. Dataset Description

A total of 164 datasets were collected from the literature [5]. Each data set consists of seven input parameters which include length, diameter, grain size, bulk density, P-wave velocity, strain rate, and static compressive strength (SCS). The output is the rate-dependent compressive strength (CS) of the rocks. The distribution between each input parameter and output parameter is shown in Figure 4. To further understand the characteristics of the input parameters, the distribution characteristics of these parameters are listed in Table 1. For model training and testing, 131 sets of data were randomly selected for the training of the model, and the remaining data set was used as the test set. For comparison purposes, the training set and test set will be fixed after the training set has been randomly selected by the first model. In this way, the training and test sets of the four models are identical. The model training phase used 10-fold cross-validation.
In addition, three evaluation metrics are introduced for quantification when assessing and comparing the predictive performance of the models. The definitions of these evaluation metrics are listed in Table 2 [58,59,60,61].
Where Oe and Op are the true and predicted result of the rate-dependent compressive strength, respectively.

4. Model Performance Comparison

After training and testing, the prediction results of the four models are shown in Figure 5. Moreover, a linear fitting was performed between the predicted results and the actual values. According to the correlation coefficient R2 provided in Figure 5, it can be seen that among the four models, the PSO-SVR model achieves the best prediction performance, followed by the random forest, SVR, and ELM model. Specifically, the PSO-SVR model presents the best prediction results both in the training and testing phases. For both the training and test sets, the correlation coefficient R2 of the models exceeded 0.98.
The box line plots of the relative prediction errors for the testing samples are shown in Figure 6. Compared with the ELM model, the mean prediction relative errors of the other three models were within 10%. For the PSO-SVR model, the mean value of the prediction error reached a minimum of 7.944%. To facilitate further comparison of the prediction performance of different models, Table 3 lists the evaluation metrics for the training and testing phases of each model. For the PSO-SVR model, the correlation coefficient R2 is the highest and is close to 1. The other two error metrics are smaller than the other three models, which confirm the high accuracy, reliability, and generalization ability of the PSO-SVR model in predicting the rate-dependence compressive strength of rocks.

5. Relative Importance of Input Parameters

Analyzing the influence degree and relative importance of each influencing parameter on the output results is important for the prediction of the results. In particular, it is important to understand the positive or negative effect of each influencing parameter on the output. Figure 7 shows the relative importance of each influence parameter on the output results. It can be seen that among the seven influence parameters listed, the static compressive strength is the most important parameter, with a relative importance of more than 75%. It is followed by the strain rate, whose relative importance is about 15%. The remaining five parameters have a smaller degree of influence on the output results. Further, the effect of each influencing parameter on the output results is analyzed in detail and presented in Figure 8. Each scatter in Figure 8 represents a rock sample in the data set. The red color indicates that the parameter is positive for the output, while the blue color indicates that it is negative for the output. It can be observed that the three parameters, static compressive strength, strain rate, and bulk density, have a significant positive effect on the rate-independent compressive strength of rocks. Their increase leads to an increase in compressive strength.

6. Conclusions

In this work, four intelligent machine learning models were introduced to predict the rate-independent compressive strength of rocks. The main findings are summarized below.
(1)
All four machine learning models presented in this paper can effectively achieve a fast and rough estimation of the rate-independent compressive strength of rocks for a given combination of input parameters. Compared with ELM, the average relative prediction errors of the random forest, SVR, and PSO-SVR models were all within 10%, while the PSO-SVR model reached a minimum average relative error of 7.944% for the test set.
(2)
The PSO-SVR model could capture the complex nonlinear mapping between multiple inputs and outputs more accurately than the other two models in terms of the evaluation metrics, and its prediction performance is superior to the other three methods.
(3)
Among the seven input parameters mentioned, the static compressive strength and the strain rate are the two most important variables for the rate-independent compressive strength of rocks. The three parameters, static compressive strength, strain rate, and bulk density, have significant positive effects on the rate-independent compressive strength of rocks. Their increase leads to an increase in compressive strength.

Author Contributions

Z.Y.: Writing revised manuscript, writing response to comments; Y.W.: methodology, writing—original draft, conceptualization, formal analysis; Y.Z.: data curation, resources; H.T.: validation, data curation; S.F.: funding acquisition, visualization. All authors have read and agreed to the published version of the manuscript.

Funding

Key Scientific and Technological Research Projects of Henan Province (222102210306).

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Zaid, M.; Sadique, M.R.; Samanta, M. Effect of unconfined compressive strength of rock on dynamic response of shallow unlined tunnel. SN Appl. Sci. 2020, 2, 2131. [Google Scholar] [CrossRef]
  2. Zaid, M.; Sadique, M.R. A Simple Approximate Simulation Using Coupled Eulerian–Lagrangian (CEL) Simulation in Investigating Effects of Internal Blast in Rock Tunnel. Indian Geotech. J. 2021, 51, 1038–1055. [Google Scholar] [CrossRef]
  3. Zaid, M.; Shah, I.A. Numerical Analysis of Himalayan Rock Tunnels under Static and Blast Loading. Geotech. Geol. Eng. 2021, 39, 5063–5083. [Google Scholar] [CrossRef]
  4. Zaid, M.; Sadique, M.R.; Alam, M.M. Blast analysis of tunnels in Manhattan-Schist and Quartz-Schist using coupled-Eulerian–Lagrangian method. Innov. Infrastruct. Solut. 2021, 6, 69. [Google Scholar] [CrossRef]
  5. Wei, M.; Meng, W.; Dai, F.; Wu, W. Application of machine learning in predicting the rate-dependent compressive strength of rocks. J. Rock Mech. Geotech. Eng. 2022; in press. [Google Scholar] [CrossRef]
  6. Yang, L.; Wang, G.; Zhao, G.-F.; Shen, L. A rate- and pressure-dependent damage-plasticity constitutive model for rock. Int. J. Rock Mech. Min. Sci. 2020, 133, 104394. [Google Scholar] [CrossRef]
  7. Xie, S.J.; Han, Z.Y.; Chen, Y.F.; Wang, Y.X.; Zhao, Y.L.; Lin, H. Constitutive modeling of rock materials considering the void compaction characteristics. Arch. Civ. Mech. Eng. 2022, 22, 60. [Google Scholar] [CrossRef]
  8. Xie, S.J.; Lin, H.; Chen, Y.F.; Yong, R.; Xiong, W.; Du, S.G. A damage constitutive model for shear behavior of joints based on determination of the yield point. Int. J. Rock Mech. Min. Sci. 2020, 128, 104269. [Google Scholar] [CrossRef]
  9. Bieniawski, Z.T.; Bernede, M.J. Suggested methods for determining the uniaxial compressive strength and deformability of rock materials: Part 1. Suggested method for determining deformability of rock materials in uniaxial compression. Int. J. Rock Mech. Min. Sci. Geomech. Abstr. 1979, 16, 138–140. [Google Scholar] [CrossRef]
  10. Han, Z.; Li, D.; Li, X. Experimental study on the dynamic behavior of sandstone with coplanar elliptical flaws from macro, meso, and micro viewpoints. Theor. Appl. Fract. Mec. 2022, 120, 103400. [Google Scholar] [CrossRef]
  11. Zhong, K.; Zhao, W.; Qin, C.; Gao, H.; Chen, W. Mechanical Properties of Roof Rocks under Superimposed Static and Dynamic Loads with Medium Strain Rates in Coal Mines. Appl. Sci. 2021, 11, 8973. [Google Scholar] [CrossRef]
  12. Duan, K.; Ji, Y.; Wu, W.; Kwok, C.Y. Unloading-induced failure of brittle rock and implications for excavation-induced strain burst. Tunn. Undergr. Space Technol. 2019, 84, 495–506. [Google Scholar] [CrossRef]
  13. Xie, S.; Han, Z.; Hu, H.; Lin, H. Application of a novel constitutive model to evaluate the shear deformation of discontinuity. Eng. Geol. 2022, 304, 106693. [Google Scholar] [CrossRef]
  14. Whittington, W.R.; Oppedal, A.L.; Francis, D.K.; Horstemeyer, M.F. A novel intermediate strain rate testing device: The serpentine transmitted bar. Int. J. Impact Eng. 2015, 81, 1–7. [Google Scholar] [CrossRef]
  15. Du, H.-b.; Dai, F.; Xu, Y.; Liu, Y.; Xu, H.-n. Numerical investigation on the dynamic strength and failure behavior of rocks under hydrostatic confinement in SHPB testing. Int. J. Rock Mech. Min. Sci. 2018, 108, 43–57. [Google Scholar] [CrossRef]
  16. Huang, X.; Qi, S.; Xia, K.; Shi, X. Particle Crushing of a Filled Fracture during Compression and Its Effect on Stress Wave Propagation. J. Geophys. Res. Solid Earth 2018, 123, 5559–5587. [Google Scholar] [CrossRef]
  17. Duan, K.; Li, Y.; Wang, L.; Zhao, G.; Wu, W. Dynamic responses and failure modes of stratified sedimentary rocks. Int. J. Rock Mech. Min. Sci. 2019, 122, 104060. [Google Scholar] [CrossRef]
  18. Wu, Y.; Zhou, Y. Hybrid machine learning model and Shapley additive explanations for compressive strength of sustainable concrete. Constr. Build. Mater. 2022, 330, 127298. [Google Scholar] [CrossRef]
  19. Ahmad, A.; Ahmad, W.; Aslam, F.; Joyklad, P. Compressive strength prediction of fly ash-based geopolymer concrete via advanced machine learning techniques. Case Stud. Constr. Mater. 2022, 16, e00840. [Google Scholar] [CrossRef]
  20. Güçlüer, K.; Özbeyaz, A.; Göymen, S.; Günaydın, O. A comparative investigation using machine learning methods for concrete compressive strength estimation. Mater. Today Commun. 2021, 27, 102278. [Google Scholar] [CrossRef]
  21. Tang, F.; Wu, Y.; Zhou, Y. Hybridizing Grid Search and Support Vector Regression to Predict the Compressive Strength of Fly Ash Concrete. Adv. Civ. Eng. 2022, 2022, 3601914. [Google Scholar] [CrossRef]
  22. Ray, S.; Haque, M.; Rahman, M.M.; Sakib, M.N.; Al Rakib, K. Experimental investigation and SVM-based prediction of compressive and splitting tensile strength of ceramic waste aggregate concrete. J. King Saud Univ.-Eng. Sci. 2021; in press. [Google Scholar] [CrossRef]
  23. Ahmad, W.; Ahmad, A.; Ostrowski, K.A.; Aslam, F.; Joyklad, P.; Zajdel, P. Application of Advanced Machine Learning Approaches to Predict the Compressive Strength of Concrete Containing Supplementary Cementitious Materials. Materials 2021, 14, 5762. [Google Scholar] [CrossRef] [PubMed]
  24. Sonebi, M.; Cevik, A.; Grünewald, S.; Walraven, J. Modelling the fresh properties of self-compacting concrete using support vector machine approach. Constr. Build. Mater. 2016, 106, 55–64. [Google Scholar] [CrossRef]
  25. Saha, P.; Debnath, P.; Thomas, P. Prediction of fresh and hardened properties of self-compacting concrete using support vector regression approach. Neural Comput. Appl. 2020, 32, 7995–8010. [Google Scholar] [CrossRef]
  26. Meng, F.; Jing, S.; Sun, X.; Wang, C.; Liang, Y.; Pang, D. A New Approach of Disaster Forecasting Based on Least Square Optimized Neural Network. Geofluids 2020, 2020, 8882241. [Google Scholar] [CrossRef]
  27. Acar, M.C.; Kaya, B. Models to estimate the elastic modulus of weak rocks based on least square support vector machine. Arab. J. Geosci. 2020, 13, 590. [Google Scholar] [CrossRef]
  28. Ceryan, N.; Okkan, U.; Kesimal, A. Prediction of unconfined compressive strength of carbonate rocks using artificial neural networks. Environ. Earth Sci. 2013, 68, 807–819. [Google Scholar] [CrossRef]
  29. Ceryan, N.; Okkan, U.; Samui, P.; Ceryan, S. Modeling of tensile strength of rocks materials based on support vector machines approaches. Int. J. Numer. Anal. Methods Geomech. 2013, 37, 2655–2670. [Google Scholar] [CrossRef]
  30. Fattahi, H. Application of improved support vector regression model for prediction of deformation modulus of a rock mass. Eng. Comput. 2016, 32, 567–580. [Google Scholar] [CrossRef]
  31. Mohamad, E.T.; Armaghani, D.J.; Momeni, E.; Abad, S.V.A.N.K. Prediction of the unconfined compressive strength of soft rocks: A PSO-based ANN approach. Bull. Eng. Geol. Environ. 2015, 74, 745–757. [Google Scholar] [CrossRef]
  32. Rezaei, M.; Majdi, A.; Monjezi, M. An intelligent approach to predict unconfined compressive strength of rock surrounding access tunnels in longwall coal mining. Neural Comput. Appl. 2014, 24, 233–241. [Google Scholar] [CrossRef]
  33. Yagiz, S. Predicting uniaxial compressive strength, modulus of elasticity and index properties of rocks using the Schmidt hammer. Bull. Eng. Geol. Environ. 2009, 68, 55–63. [Google Scholar] [CrossRef]
  34. Armaghani, D.J.; Mohamad, E.T.; Momeni, E.; Monjezi, M.; Narayanasamy, M.S. Prediction of the strength and elasticity modulus of granite through an expert artificial neural network. Arab. J. Geosci. 2015, 9, 48. [Google Scholar] [CrossRef]
  35. Ghasemi, E.; Kalhori, H.; Bagherpour, R.; Yagiz, S. Model tree approach for predicting uniaxial compressive strength and Young’s modulus of carbonate rocks. Bull. Eng. Geol. Environ. 2018, 77, 331–343. [Google Scholar] [CrossRef]
  36. Li, W.; Tan, Z. Research on Rock Strength Prediction Based on Least Squares Support Vector Machine. Geotech. Geol. Eng. 2017, 35, 385–393. [Google Scholar] [CrossRef]
  37. Yılmaz, I.; Yuksek, A.G. An Example of Artificial Neural Network (ANN) Application for Indirect Estimation of Rock Parameters. Rock Mech. Rock Eng. 2008, 41, 781–795. [Google Scholar] [CrossRef]
  38. Momeni, E.; Armaghani, D.J.; Hajihassani, M.; Amin, M.F.M. Prediction of uniaxial compressive strength of rock samples using hybrid particle swarm optimization-based artificial neural networks. Measurement 2015, 60, 50–63. [Google Scholar] [CrossRef]
  39. Gupta, D.; Natarajan, N. Prediction of uniaxial compressive strength of rock samples using density weighted least squares twin support vector regression. Neural Comput. Appl. 2021, 33, 15843–15850. [Google Scholar] [CrossRef]
  40. Gamal, H.; Alsaihati, A.; Elkatatny, S.; Haidary, S.; Abdulraheem, A. Rock Strength Prediction in Real-Time While Drilling Employing Random Forest and Functional Network Techniques. J. Energy Resour. Technol. 2021, 143, 093004. [Google Scholar] [CrossRef]
  41. Xie, S.J.; Lin, H.; Chen, Y.F.; Wang, Y.X. A new nonlinear empirical strength criterion for rocks under conventional triaxial compression. J. Cent. South Univ. 2021, 28, 1448–1458. [Google Scholar] [CrossRef]
  42. Farhadian, A.; Ghasemi, E.; Hoseinie, S.H.; Bagherpour, R. Prediction of Rock Abrasivity Index (RAI) and Uniaxial Compressive Strength (UCS) of Granite Building Stones Using Nondestructive Tests. Geotech. Geol. Eng. 2022, 40, 3343–3356. [Google Scholar] [CrossRef]
  43. Amirkiyaei, V.; Ghasemi, E.; Faramarzi, L. Estimating uniaxial compressive strength of carbonate building stones based on some intact stone properties after deterioration by freeze–thaw. Environ. Earth Sci. 2021, 80, 352. [Google Scholar] [CrossRef]
  44. Liang, N.; Huang, G.; Saratchandran, P.; Sundararajan, N. A Fast and Accurate Online Sequential Learning Algorithm for Feedforward Networks. IEEE Trans. Neural Netw. 2006, 17, 1411–1423. [Google Scholar] [CrossRef]
  45. Guang-Bin, H. Learning capability and storage capacity of two-hidden-layer feedforward networks. IEEE Trans. Neural Netw. 2003, 14, 274–281. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  46. Ding, S.; Zhao, H.; Zhang, Y.; Xu, X.; Nie, R. Extreme learning machine: Algorithm, theory and applications. Artif. Intell. Rev. 2015, 44, 103–115. [Google Scholar] [CrossRef]
  47. Tran, V.Q. Machine learning approach for investigating chloride diffusion coefficient of concrete containing supplementary cementitious materials. Constr. Build. Mater. 2022, 328, 127103. [Google Scholar] [CrossRef]
  48. Wan, D. Research on Extreme Learning of Neural Networks. Chin. J. Comput. 2010, 33, 279–287. [Google Scholar]
  49. Han, Q.; Gui, C.; Xu, J.; Lacidogna, G. A generalized method to predict the compressive strength of high-performance concrete by improved random forest algorithm. Constr. Build. Mater. 2019, 226, 734–742. [Google Scholar] [CrossRef]
  50. Li, H.; Lin, J.; Lei, X.; Wei, T. Compressive strength prediction of basalt fiber reinforced concrete via random forest algorithm. Mater. Today Commun. 2022, 30, 103117. [Google Scholar] [CrossRef]
  51. He, B.; Lai, S.H.; Mohammed, A.S.; Sabri, M.M.; Ulrikh, D.V. Estimation of Blast-Induced Peak Particle Velocity through the Improved Weighted Random Forest Technique. Appl. Sci. 2022, 12, 5019. [Google Scholar] [CrossRef]
  52. Wu, Y.; Li, S. Damage degree evaluation of masonry using optimized SVM-based acoustic emission monitoring and rate process theory. Measurement 2022, 190, 110729. [Google Scholar] [CrossRef]
  53. Li, N.; Nguyen, H.; Rostami, J.; Zhang, W.; Bui, X.-N.; Pradhan, B. Predicting rock displacement in underground mines using improved machine learning-based models. Measurement 2022, 188, 110552. [Google Scholar] [CrossRef]
  54. Bardhan, A.; Kardani, N.; GuhaRay, A.; Burman, A.; Samui, P.; Zhang, Y. Hybrid ensemble soft computing approach for predicting penetration rate of tunnel boring machine in a rock environment. J. Rock Mech. Geotech. Eng. 2021, 13, 1398–1412. [Google Scholar] [CrossRef]
  55. Liu, B.; Wang, R.; Guan, Z.; Li, J.; Xu, Z.; Guo, X.; Wang, Y. Improved support vector regression models for predicting rock mass parameters using tunnel boring machine driving data. Tunn. Undergr. Space Technol. 2019, 91, 102958. [Google Scholar] [CrossRef]
  56. Jueyendah, S.; Lezgy-Nazargah, M.; Eskandari-Naddaf, H.; Emamian, S.A. Predicting the mechanical properties of cement mortar using the support vector machine approach. Constr. Build. Mater. 2021, 291, 123396. [Google Scholar] [CrossRef]
  57. Wu, Y.; Zhou, Y. Prediction and feature analysis of punching shear strength of two-way reinforced concrete slabs using optimized machine learning algorithm and Shapley additive explanations. Mech. Adv. Mater. Struct. 2022, 1–11. [Google Scholar] [CrossRef]
  58. Song, H.; Ahmad, A.; Farooq, F.; Ostrowski, K.A.; Maślak, M.; Czarnecki, S.; Aslam, F. Predicting the compressive strength of concrete with fly ash admixture using machine learning algorithms. Constr. Build. Mater. 2021, 308, 125021. [Google Scholar] [CrossRef]
  59. Chen, H.; Li, X.; Wu, Y.; Zuo, L.; Lu, M.; Zhou, Y. Compressive Strength Prediction of High-Strength Concrete Using Long Short-Term Memory and Machine Learning Algorithms. Buildings 2022, 12, 302. [Google Scholar] [CrossRef]
  60. Farooq, F.; Amin, M.N.; Khan, K.; Sadiq, M.R.; Javed, M.F.; Aslam, F.; Alyousef, R. A Comparative Study of Random Forest and Genetic Engineering Programming for the Prediction of Compressive Strength of High Strength Concrete (HSC). Appl. Sci. 2020, 10, 7330. [Google Scholar] [CrossRef]
  61. Nafees, A.; Javed, M.F.; Khan, S.; Nazir, K.; Farooq, F.; Aslam, F.; Musarat, M.A.; Vatin, N.I. Predictive Modeling of Mechanical Properties of Silica Fume-Based Green Concrete Using Artificial Intelligence Approaches: MLPNN, ANFIS, and GEP. Materials 2021, 14, 7531. [Google Scholar] [CrossRef] [PubMed]
Figure 1. Extreme Learning Machine Network Structure.
Figure 1. Extreme Learning Machine Network Structure.
Minerals 12 00731 g001
Figure 2. Schematic diagram of random forest model [51].
Figure 2. Schematic diagram of random forest model [51].
Minerals 12 00731 g002
Figure 3. Flowchart of the proposed hybrid model.
Figure 3. Flowchart of the proposed hybrid model.
Minerals 12 00731 g003
Figure 4. Scatterplot and histogram of the distribution of the input and output parameters.
Figure 4. Scatterplot and histogram of the distribution of the input and output parameters.
Minerals 12 00731 g004aMinerals 12 00731 g004b
Figure 5. Prediction results of three models. (a) ELM model prediction results; (b) RF model prediction results; (c) SVR model prediction results; (d) PSO-SVR model prediction results.
Figure 5. Prediction results of three models. (a) ELM model prediction results; (b) RF model prediction results; (c) SVR model prediction results; (d) PSO-SVR model prediction results.
Minerals 12 00731 g005aMinerals 12 00731 g005b
Figure 6. Relative error of model prediction results for the test set.
Figure 6. Relative error of model prediction results for the test set.
Minerals 12 00731 g006
Figure 7. Three-dimensional pie chart of the relative importance of parameters to output.
Figure 7. Three-dimensional pie chart of the relative importance of parameters to output.
Minerals 12 00731 g007
Figure 8. SHAP summary plot of compressive strength.
Figure 8. SHAP summary plot of compressive strength.
Minerals 12 00731 g008
Table 1. Distribution characteristics of the parameters.
Table 1. Distribution characteristics of the parameters.
ParameterLengthDiameterGrain SizeBulk DensityP-Wave VelocityStrain RateSCSCS
Unitmmmmmmkg/m3m/ss−1MPaMPa
Max70703.528506651223212352.71
Min102.50.03227824370.00000528.630.03
Mean40.4341.950.752479.683542.9959.4887.55128.14
Median49.7749.500.232384.003031.0056.0071.91101.42
Standard deviation15.8118.151.07186.211231.8946.8556.3980.23
Coefficient of variation0.390.431.430.080.350.790.640.63
Kurtosis−0.74−0.551.76−1.040.121.16−0.81−0.32
Skewness−0.76−0.621.750.591.330.900.750.91
Pearson correlation coefficient−0.220.130.540.710.780.160.891
Table 2. Definitions of evaluation indexes.
Table 2. Definitions of evaluation indexes.
Evaluation MetricsDefinition
Correlation coefficient R 2 = ( n i = 1 n ( O e O p ) i = 1 n O e i = 1 n O p ) 2 [ n ( i = 1 n O e 2 ) ( i = 1 n O e ) 2 ] [ n ( i = 1 n O p 2 ) ( i = 1 n O p ) 2 ]
Mean absolute error M A E = 1 n i = 1 n O e O p
Mean absolute percentage error M A P E = 1 n i = 1 n O e O p O e × 100 %
Table 3. Evaluation indicators of four models.
Table 3. Evaluation indicators of four models.
ModelMAEMAPE/%R2
ELM training12.53110.6200.947
ELM test15.57312.6640.946
RF training9.4298.4110.972
RF test10.3129.0070.979
SVR training10.2189.8710.969
SVR test11.041459.2788410.972
PSO-SVR training4.95114.7180.992
PSO-SVR test10.0527.9440.980
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Yang, Z.; Wu, Y.; Zhou, Y.; Tang, H.; Fu, S. Assessment of Machine Learning Models for the Prediction of Rate-Dependent Compressive Strength of Rocks. Minerals 2022, 12, 731. https://doi.org/10.3390/min12060731

AMA Style

Yang Z, Wu Y, Zhou Y, Tang H, Fu S. Assessment of Machine Learning Models for the Prediction of Rate-Dependent Compressive Strength of Rocks. Minerals. 2022; 12(6):731. https://doi.org/10.3390/min12060731

Chicago/Turabian Style

Yang, Ziquan, Yanqi Wu, Yisong Zhou, Hui Tang, and Shanchun Fu. 2022. "Assessment of Machine Learning Models for the Prediction of Rate-Dependent Compressive Strength of Rocks" Minerals 12, no. 6: 731. https://doi.org/10.3390/min12060731

APA Style

Yang, Z., Wu, Y., Zhou, Y., Tang, H., & Fu, S. (2022). Assessment of Machine Learning Models for the Prediction of Rate-Dependent Compressive Strength of Rocks. Minerals, 12(6), 731. https://doi.org/10.3390/min12060731

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