1. Introduction
A rock burst is a sudden and violent expulsion of rock from the surrounding rock mass. Rock burst is considered a dynamic instability phenomenon of surrounding rock mass of un-derground space in high geostatic stress and caused by the violent release of strain energy stored in the rock mass. Rock burst occurs during excavating underground space in the form of a stripe of rock slices or rock fall or throwing of rock fragments, sometimes accompanied by crack sound. Rock bursts are related to the fracture of rock in place and require two conditions for their occurrence: stress in the rock mass sufficiently high to exceed its strength, and physical characteristics of the rock which enable it to store energy up to the threshold value for sudden rupture. Rocks which yield gradually in plastic strain under load usually do not generate rock bursts. The likelihood of rock bursts occurring increases as the depth of the mine increases. Rock bursts are also affected by the size of excavation, becoming more likely if the excavation size is around 180m and above. Induced seismicity such as faulty methods of mining can trigger rock bursts. Other causes of rock bursts are the presence of faults, dikes, or joints (Dong et al., 2013).
Because rock burst occurs suddenly and intensely, it usually causes injury including death to workers, damage to equipment, and even substantial disruption and economic loss of under-ground space excavation. Therefore, there is a need for the development of suitable computa-tional methods for the prediction and control of rock bursts particularly for a safe and economic underground excavation for construction or mining in the burst-prone ground. For this case, numerous related research works, concerning about the mechanism, characteristics or type, the cause of formation, the critical conditions and preventive methods of rock burst have been con-ducted by many researchers. Many researchers have suggested various theories, many predic-tion methods, and empirical correlation, such as fuzzy-base evaluation method (Wang et al., 1998; Amoussou et al., 2013), distance discriminant analysis (Wang et al., 2009; Wang et al., 2017), support vector machine (SVM) (Zhao, 2005; Zhou et al., 2012, extension-theory-based method (Xiong et al., 2007), rough-set-based method (Yang, 2010), unascertained measurement method(Shi et al., 2010), numerical simulation (Zhen & Gao, 2017; Zhu et al., 2010) and case study (Mansurov, 2001).
These studies offered new ideas and approaches for rock burst prediction. However, each method discussed above has its advantages and disadvantages, and understanding, predicting and controlling the rock bursts still pose a considerable challenge for underground engineering.
As an important means, the ANN-based method for prediction of rock burst has been adopted by many researchers gradually in recent years (Bai et al., 2002; Zhang et al., 2012). Ar-tificial neural network technique is considered the most effective and reliable artificial intelli-gence methods for solving classification, prediction and recognition problems.
Currently, back propagation (BP) and radial basis function (RBF) networks are used in the field of prediction of robust classification. However, for network training, they are all easily trapped in local minimum values. Probabilistic neural network (PNN), on the other hand, is a feedforward neural network. It is derived from the Bayesian network and a statistical algorithm called kernel Fisher discriminant analysis. It was introduced by Specht and Donald(1990). Be-cause PNN has the advantages of low training complexity, high stability, quick convergence, and simple construction, it has a wide range of application in model classification, identification, prediction, as well as fault diagnosis and other fields(Adeli and Panakkat, 2009; Song et al., 2007; Ataa et al., 2017; Rutkowski, 2004 ). In this work, according to the practice of complicat-ed problems of the rock burst prediction, the PNN is applied to predicting rock burst classifica-tion.
2. Material and Methods
2.1. Criteria and indexes of rock burst and rock burst classification
2.1.1. Criteria considering stress in surrounding rock
The criteria listed in Table 1 were proposed early, and only considered the stress level in surrounding rock. Furthermore, different scholars chose different parameters as an evaluation index of criterion for rock burst, and the classification of rock burst intensity also differed from each other. So it is difficult to use these criteria in the construction of underground engineering.
Note: σ n is the maximum tangential stress of surrounding rock, MPa; σ is the axial stress of surrounding rock, MPa; σ 1 , is the maximum in si-tu stress of engineering area, MPa; σ 1 is the uniaxial compressive strength of rock, MPa;
2.1.2. Comprehension criteria considering stress, properties of surrounding rock and energy
1) The following criterion is presented with rock burst tendency index and energy condition of surrounding rock (Dong et al, 2013).
where W qχ is the rock burst tendency index; σ 1 and σ 2 are the major and middle principal stress in surrounding rock, respectively; μ is the Poisson ratio.
2) It is stipulated that rock burst could occur if σ θ / σ c ≤ K s in which the value of K related to σ t / σ c criterion.
3) Kidybinski (1981) proposed an elastic energy index We t No rock burst activity, moderate rock burst activity and strong rock burst activity, meet the conditions W et <2.0, 2.0≤ W et ≤5.0, and W et >5.0, respectively.
2.1.3 Input characteristic vector for PNN
The indexes of criterion should reflect the main factors of rock burst -the properties and stress of surrounding rock. At the same time, they should be obtained easily and can be compared with each other for different cases. In this work, the compressive rock strength σ c , tensile strength σ t , elastic energy index W et and the maximum tangential stress σ θ are chosen as the indexes of criterion. Compressive rock strength σ t , tensile strength σ t , and elastic energy index W et can indicate the properties of surrounding rock, and the tangential stress σ θ can reflect the virgin geostatic stress condition and the influence of the shape and dimension of the underground space on rock burst. In this work, σ θ , σ c , σ t and W et are selected as the input index for PNN model to predict the degree of rock burst activity. Hence, the input characteristic vector for PNN is [σ θ , σ c , σ t , W et ].
2.1.4 Classification for intensities of rock burst
According to the extent and intensity of the characteristics of the rock burst phenomenon in the underground openings, the grade of rock burst is divided into four degrees, namely none rock burst, light rock burst, moderate rock burst, strong rock burst, respectively. So the PNN model output is rock burst degree, output = [none rock burst, light rock burst, moderate rock burst, strong rock burst]. Also, the division of rock burst degree can be described in Table 2 (Wang et al., 1998; Zhou et al., 2012; Zhang et al., 2004)
2.2. PNN-based Rock burst Prediction Model
2.2.1 Outline of PNN
Probability neural networks are a tool for handling uncertainty for improving learning per-formance. Probability uncertainty and fuzziness uncertainty processing play a key role in boost-ing classification systems including extreme learning machines and decision trees (Wang et al., 2015; Lu et al., 2015). PNN is essentially a classifier that places the Bayes estimate in a feed-forward neural network. The central concept of Bayes criterion classification is the minimal ''predictable risk'' of the Bayes decision. The Bayes decision is based on the non-parametric estimation of the probability density function; accordingly, it obtains the classification results. Based on its advantages, such as rapid training time, a stable and simple neural structure, and good convergence, it is suitable for use in defect recognition.
For a multi-class problem with σ 1 , σ2, , σ q ,, σ s ,, we apply to the above issues two types of classification problems in Bayes decision classification. For p-dimensional vector X = {x 1 , x 2 , , x p } based on the Bayes decision rule, we determine the status of θЄθ with its measurement set,
In the Equation (5), h q represents the priori probability of θ = θ q , d(x) as the Bayes decision of test vector X , h k is the priori probability of θ = θ k , and l q and l k are incorrectly classified into other categories of losses. The latter should belong to θ q and θ k Besides, f q (x) and f q (x) are probability density function of θ q and θ k respectively.
where X is a sample of the input vector to be classified, p is the dimension of sample vectors, x qj is the j-th sample of the category θ q and m q is the sample number of category θ q . Additionally, σ is the smoothing parameter.
Figure 1 depicts a schematic diagram of the multi-class classification PNN. X is a vector to be classified as the neurons in the input layer. It is passed to the corresponding neurons in the hidden layer with no change. The hidden layer then transmits each neuron in the accumulated layers. At this point, the output obtained by the accumulation layer is the estimation of the probability density function of each pattern for the test vectors. Accordingly, the category of the occurrence of the maximum probability of the current test vector is the one that corresponds to the largest probability density function. This function is the output of the accumulation layer. The neuron output with the probability density maximum is 1; the corresponding category is the one to which h belongs.
2.2.2 PNN modeling for prediction of rock burst
The number of input layer neurons of PNN is the same as the dimensionality of the input characteristic vector. Based on discussed above, σ e , σ c , σ t , and W, are selected as the input characteristic vector for PNN model and the input vector of PNN = [σ θ , σ c , σ t , W et ]. Hence, the number of input layer neurons of PNN is 4.
The number of output neurons of PNN is the same as the number of classification of rock burst activity. According to the section 2.4, the grade of rock burst is divided into four degrees, and the PNN model output is rock burst degree and the output vector = [none rock burst, light rock burst, moderate rock burst, strong rock burst]. So the number of output layer neurons is 4.
The number of hidden layer neurons is determined by the training data set. The number of hidden layer neurons is equal to the sum of the number of each category of training sample
The number of accumulation layer neurons is the same as the number of classification of rock burst activity. Here, the number of accumulation layer neurons is 4.
The design of PNN modeling for prediction of rock burst includes the following aspects: a collection of data sets, data preprocessing, build a PNN, network model, training PNN, testing PNN etc. The design process is shown in Figure 2.
3. Results
Rock burst samples which come from underground rock projects in domestic and abroad are collected as training data set (Show in Table 3) and testing data set (Show in Table 4) to verify the rationality of our posed method.
The relationship among the indexes of criteria, the occurrence of rock burst and its intensity is very complicated. For the sake of the capability of PNN for pattern recognition, we attempt to predict the rock burst activity by using PNN.
Four degrees of rock burst activity, including none rock burst, light rock burst, moderate rock burst and strong rock burst are indicated by 1, 2, 3 and 4, respectively.
PNN model and criterion are obtained through training data sets of rock burst samples which come from underground rock projects in domestic and abroad. The training effect and the training error are shown in Figure 3. It is noted from Figure 3 that the misjudgment ratios of training samples using PNN model is 0, which prove that the PNN has a good learning performance. Figure 4 is the perdition results of testing samples. From the Figure 4, we can find that the prediction accuracy of PNN model is 100%. The results show that the prediction results agree well with the practical records, which prove the PNN-based rock burst model is useful and available and can be applied to the prediction for the possibility and classification of rock burst in underground engineering.
The results of the PNN-based method are compared with that SVM-based method, BP-based method, and LVQ-based method. The calculated results of PNN, SVM, BP and LVQ are listed in Table 3. From Table 3, we can find that the misjudgment ratios of tested samples using SVM, BP, LVQ, and PNN are 10%, 20%, 20% and 0, respectively. The compared predicted results show that it is feasible and appropriate to use PNN model for rock burst prediction.
To study the effectiveness and feasibility in engineering practice applications, two real-world examples are analyzed by using our posed PNN-based rock burst prediction method.
Case 1: Tongyu tunnel engineering
Tongyu Tunnel is currently one of the most deep-lying and longest tunnels in Chongqing, China. Its geological conditions are incredibly complex. The measured data of rock burst in depth 900m at a cross section of K21+680 of Tongyu tunnel are listed in Table 6 (He et al., 2008). Applying our proposed prediction model to rock burst prediction of this engineering, the result of prediction is light rock burst activity. The results agree well with the practical records.
Case 2: Qinnling tunnel engineering
The QingLing tunnel is the longest railway tunnel in China and takes the third place in the world at present. Reference (Thaldiri et al., 2017; Li and Wang, 2009) provides rock burst measured data for of QingLing tunnel engineering. Some measured data listed in Table 7. Table 7 compared the performance of the proposed method with existing BP-based method (Bai et al., 2002) and unascertained measurement method(Shi et al., 2010). From the Table 7, the result of prediction is same as the results of existing BP-based method and unascertained measurement method, just same as what happened in the scene. This case further confirms that the PNN-based method is effective and practical in the application of prediction of rock burst. On the other hand, PNN-based method has the advantages of low training complexity, high stability, quick convergence, and simple construction.
4. Discussion
In this paper, a novel PNN-based rock burst prediction model is proposed to determine whether rock burst will happen in the underground rock projects and how much the intensity of rock burst is. PNN model is obtained through training data sets of rock burst samples which come from underground rock project in domestic and abroad. Other samples are tested with the model. The testing results agree with the practical records. At the same time, two real-world applications are used to verify the proposed method. The results of prediction are same as the results of existing methods, just same as what happened in the scene, which verifies the effectiveness and applicability of our proposed work.
5. Conclusions
Because PNN has the advantages of low training complexity, high stability, quick convergence, and simple construction, it can be well applied in the prediction of rock burst. In this work, a PNN-based prediction model of rock burst is presented. According to the mechanism of rock burst, rocks' maximum tangential stress σθ, rocks' uniaxial compressive strength σ, rocks' uniaxial tensile strength σ and elastic energy index W et are defined as the criterion indices for rock burst prediction in the proposed PNN-model. Some collected rock burst samples which come from underground rock projects in domestic and abroad and two real-world engineering in China are used to verify the new model. The prediction results demonstrated that the developed PNN-based prediction model is effective and efficient approach to predict rock burst potential grade.