Research Article  Open Access
Xiaowei Li, Chenglin Jiang, Jun Tang, Yujia Chen, Dingding Yang, Zixian Chen, "A Fisher’s CriterionBased Linear Discriminant Analysis for Predicting the Critical Values of Coal and Gas Outbursts Using the Initial Gas Flow in a Borehole", Mathematical Problems in Engineering, vol. 2017, Article ID 7189803, 11 pages, 2017. https://doi.org/10.1155/2017/7189803
A Fisher’s CriterionBased Linear Discriminant Analysis for Predicting the Critical Values of Coal and Gas Outbursts Using the Initial Gas Flow in a Borehole
Abstract
The risk of coal and gas outbursts can be predicted using a method that is linear and continuous and based on the initial gas flow in the borehole (IGFB); this method is significantly superior to the traditional point prediction method. Acquiring accurate critical values is the key to ensuring accurate predictions. Based on ideal rock crosscut coal uncovering model, the IGFB measurement device was developed. The present study measured the data of the initial gas flow over 3 min in a 1 m long borehole with a diameter of 42 mm in the laboratory. A total of 48 sets of data were obtained. These data were fuzzy and chaotic. Fisher’s discrimination method was able to transform these spatial data, which were multidimensional due to the factors influencing the IGFB, into a onedimensional function and determine its critical value. Then, by processing the data into a normal distribution, the critical values of the outbursts were analyzed using linear discriminant analysis with Fisher’s criterion. The weak and strong outbursts had critical values of 36.63 L and 80.85 L, respectively, and the accuracy of the backdiscriminant analysis for the weak and strong outbursts was 94.74% and 92.86%, respectively. Eight outburst tests were simulated in the laboratory, the reverse verification accuracy was 100%, and the accuracy of the critical value was verified.
1. Introduction
Coal is the main nonrenewable energy resource consumed in China. Due to the advancement of coal mining in recent years, mining depths have reached 1,300 m and are estimated to reach 1,500 m within the next 20 years [1, 2]. As mining depth increases, ground stress as well as the pressure and content of gas in coal seams will increase, causing a corresponding increase in the outburst risk in coal seams. Outburst prediction is an important aspect of outburst coal seam mining to prevent accidents. For example, a serious accident occurred in 2011 in Sizhuang coal mine of Yunnan in China; the accident resulted in 43 deaths. Therefore, seammining countries around the world have all conducted extensive studies on outburst prediction. Outburst prediction methods can be divided into two categories: a single or comprehensive index and applying a statistical mathematical model.
In terms of the single or comprehensive index, the former Soviet Union proposed a based comprehensive index method and a based comprehensive index method [3] that were applied successively. Later, the Chinese researcher Wang [4] proposed a fourfactor comprehensive index method involving the value. Based on this method, the Fushun Institute of Coal Science [5, 6] of China proposed a comprehensive [6] index method involving the and values. Subsequently, the coal research and development institutes in China proposed a method involving the drill cutting desorption indexes and . Jiang [7, 8] proposed a method based on the initial gas expansion energy released (IGEER). In addition, other countries have used index methods involving [9] and [10]. All of the aforementioned methods measure the outburst risk at a certain point and use one point to represent the whole coal mass; in other words, they assume that the outburst risk in the predicted area is consistent with the outburst risk at the measured point. However, a coal mass is not a homogeneous body, making point prediction greatly limited.
Many factors can influence outburst prediction. Some researchers have used mathematical models to improve the accuracy of outburst prediction. Hao and Yuan [11], Tian and Zhou [12], and Qu et al. [13] studied the neural network model of outburst prediction. These methods are trained to capture the correlation between the outburst factors and the prominent outburst. To improve the accuracy of outburst prediction, Zhu et al. [14] combined principal component analysis (PCA) with the neural network. Zhang and Li [15] studied pattern recognition and the possibility prediction of coal and gas outbursts. With eight factors as the main discriminant, the pattern recognition method was used to perform possibility prediction of coal outbursts. Wang [16] studied the coal and gas outburst prediction based on fuzzy matterelement analysis. Guo et al. [17] studied the prediction method of coal and gas outbursts using the analytic hierarchy process and fuzzy comprehensive evaluation. The prediction of coal and gas outbursts was also studied using the analytic hierarchy process (AHP) and fuzzy comprehensive evaluation. In the prediction method, AHP was used to confirm the weights of the coal and gas outburst factors; the judgment matrix of each factor was constructed by membership functions; and the prediction model of coal and gas outbursts was established using the fuzzy comprehensive evaluation method. Zhao and Tan [18] studied the premonitory time series prediction of coal and gas outbursts based on chaos theory. According to the chaos characteristic of outburst prediction data, the outburst prediction model was established using the method of chaotic prediction. In addition, Peng and Wang [19] studied the improved analytic hierarchy process for coal and gas outburst prediction. Because the initial gas flow in the borehole (IGFB) is affected by many factors, and some of these factors are connected with each other while others are relatively independent, the IGFB are fuzzy and chaotic. These studies can be used as valuable references. However, the critical value of an outburst is usually measured under the simplest conditions. In the same way, research on the IGFB has discarded some minor factors. The fuzziness and chaos are relatively less. In addition, these methods are based on the results of point predictions and share the same disadvantages. Therefore, there are differences between research into the IGFB and the references.
The method established in the present study, which is based on the IGFB, is a linear prediction method. The mechanism of this method is as follows: during drilling, the volume of gas released from the borehole is continuously measured. Through data processing, the measured volume is converted to the total volume of gas released from a 1 m long borehole with a diameter of 42 mm within 3 min. The larger this flow is, the higher the outburst risk of the coal seam is. This method can continuously predict the outburst risk of coal seams passed during the drilling process. Therefore, this is a neoteric prediction method.
Wang and Yu [20–22] first analyzed such indexes in terms of the volume of drill cuttings and the volume of gas emitted from the borehole and found that the measured volume of gas emitted from the borehole exhibited fractal dimension characteristics. Based on Wang and Yu’s study, Han [23], Qin et al. [24], Nie [25, 26], and Yuan [27] studied the borehole wall and the emission pattern of coal cuttings and gas during the drilling process. Based on the aforementioned studies, Wu [28] completed comprehensive laboratory and field application studies on the outburst risk prediction during the tunneling of soft coal seams and roadways using the continuous flow method; however, because of the complexity of field studies on outbursts, Wu obtained only the safety value of IGFB (32.30 L).
These studies show that IGFB is influenced by many factors, such as the degree of coal deformation, the gas permeability coefficient, the borehole diameter, the gas pressure, and the radius in front of the drill bit. Therefore, IGFB also has the characteristics of fuzziness and chaos. However, in studying the critical value of IGFB, we can change some influencing factors to build a research model under the most dangerous conditions. This model is an ideal rock crosscut coal uncovering model. The effect of coal weight is neglected in this model. If the barrier layer is assumed to be dense and hard rock, then the amount of gas in the soft coal that leaks through the barrier into the tunnel is approximately zero. Then, the gas pressure in various locations in the soft coal remains at the initial pressure. Thus, regardless of the length of the driving cycle footage, the surface gas pressure in the exposed coal body after uncovering is equal to the initial gas pressure, and the outburst risk is at its highest level. Ideal rock crosscut coal uncovering occurs under this condition, as shown in Figure 1. This condition also has the highest probability of outburst; using this outburst risk as the basis for prediction, the conditions are more stringent, thus achieving a higher safety margin. All of the tests in this study were conducted with this condition.
The model fully considers the mechanical properties of coal, the in situ stress of the coal seam, and the gas bearing. Therefore, the critical values obtained from this model are credible. Thus, the present study obtained sufficient sample data by establishing a stricter laboratory simulation system. The study also obtained critical values of weak and strong outbursts of IGFB using linear discriminant analysis based on Fisher’s criterion. In addition, the present study also performed backdiscriminant analysis and verification to determine the accuracy of the results.
2. Measurement of IGFB
The apparatus for measuring IGFB mainly consists of two parts: an oblong outburst coal seam simulation device and a flow measurement device. Figure 2 shows the mechanism used in the apparatus.
The experimental apparatus shown in Figure 2 contains three gas outflow channels: a flow sensor channel (channel 1), a sealed coal chamber channel (channel 2), and a discharge channel for coal cuttings (channel 3). During the drilling process, the volume of gas emitted from the borehole that passes through channel 1 must be maximized and measured, while the volume of gas that passes through channel 2 and channel 3 must be minimized. Through experimentation, Wang et al. [29] demonstrated that the leakage of channel 2 and channel 3 is less than 1% and is negligible under the following conditions: the rotation speed is less than 425 r/min, channel 3 has a diameter of less than 60 mm and a length greater than 650 mm, and channel 2 is filled with coal cuttings with a diameter of less than 1 mm. The present study used a twist drill with a diameter of 42 mm for drilling and an electric coal drill with a rotation speed of 425 r/min to provide power; the length of channel 3 was set to 700 mm. Figure 3 shows the experimental configuration.
Coal samples from five coal mines in China were selected in the present study. A total of 48 sets of data were obtained, of which 23 sets were obtained under CO_{2} conditions and 25 sets were obtained under N_{2} conditions.
3. Analysis of the Range of IGFB Critical Values
After the data were collected, the IGEER from the coal samples was measured to determine the corresponding outburst risk. The IGEER is a comprehensive index for predicting coal seam outbursts [30, 31]. This index has been used to determine the outburst risk of 867 coal seams in 476 pairs of mine pits in China and has predicted the outburst risk of the coal seams with relative accuracy. Weak and strong outbursts have critical values of 42.98 mJ/g and 103.8 mJ/g, respectively. These critical values were used to determine the outburst risk of the simulated coal seams; Table 1 lists the results, and Figure 4 shows their distribution.
 
A: nonoutburst; B: weak outburst; C: strong outburst; resorted according to types A, B, and C. 
Figure 4 shows that a boundary exists between the nonoutburst samples and the weak outburst samples as well as between the weak outburst samples and the strong outburst samples. Based on the intervals between the boundaries, the critical values of the weak outbursts range from 35.28 to 38.26 L, and the critical values of the strong outbursts range from 77.56 to 86.94 L. To obtain accurate critical values, an accurate discriminant analysis must be performed. Figure 3 shows that the boundaries are linear; therefore, the critical values can be determined using linear discriminant analysis based on Fisher’s criterion.
4. Linear Discrimination Based on Fisher’s Criterion
Fisher’s discrimination method is commonly used in multivariate statistical discriminant analysis. The basic idea of Fisher’s discrimination method is projection. Assume that and are two ensembles, samples are taken from , and samples are taken from . Then, discriminant indexes are measured for the samples taken from and the samples taken from . A linear discriminant function, , that can reduce the data to a onedimensional numerical value is determined:where are the coefficients to be determined and are the measured values of the indexes.
Then, the linear function is used to transform the samples of the known class and the class of knowledge into onedimensional data in dimension . According to the degree of affinity, it is possible to identify the attribution of unknown samples. This linear function transforms all the points in dimensional space into onedimensional numerical values. It can not only reduce the difference between samples of the same class but also maximize the difference between sample points in different categories, which results in a higher discriminant efficiency. The calculation procedure is as follows.
First, the mean value and the covariance of the samples from group and group are calculated:
Let , and . Based on , the coefficient matrix, , is calculated to obtain the discriminant function. Then, and are calculated using type samples and type samples, respectively:
Finally, the weighted average of and is used as the critical value of the discriminant function:
Each sample that fulfills belongs to type ; otherwise, the sample belongs to type .
This discriminant analysis assumes that the two groups of samples are taken from different ensembles. If the difference in the mean value is insignificant, then the discrimination is of no value. Therefore, it is necessary to test whether there is a significant difference between the two ensembles. The test statistic is constructed based on the Mahalanobis distance ():where
The statistic follows the distribution with and degrees of freedom, that is, . The test value of statistic is obtained from (5). Using the distribution table, is obtained, where represents the test significance level ( or 0.01). The value of is compared with the value of to determine whether there is a significant difference between the two ensembles.
5. Linear Discriminant Analysis of the Critical Values of Outbursts Predicted Using IGFB
5.1. Normal Transformation of the Statistic
When statistic is used for the discriminant analysis of two types of samples, the samples must follow a normal distribution. The histogram method is the most visual method for determining whether samples follow a normal distribution. The number of small statistic intervals in a histogram is generally determined using the following equation [32]:where is the number of small statistic intervals and is the number of data points or samples.
Normalization was required for both of the sample combinations measured in the present study. A cubic root transformation was applied to the original data. Based on Table 1 and (7), there were 38 nonoutburst and weak outburst samples (the number of small intervals was set to 8) and 28 weak and strong outburst samples (the number of small intervals was set to 7). Based on these results, histograms were plotted, as shown in Figure 5. After transformation, the data approximately followed a normal distribution and thus could be used for discriminant analysis.
(a)
(b)
5.2. Discriminant Calculation and the Test of the Critical Values of the Outbursts
The number of nonoutburst samples and the number of weak outburst samples were and , respectively, and their mean values were and , respectively. The sum of the covariances of the two sets of samples was , and . The coefficient of the discriminant function was , and the critical value determined based on the discriminant function was
Because the IGFB was the only prediction index, . The discriminant function is , where . Therefore, the critical value of the weak outbursts obtained was as follows: L. Thus, there was no outburst risk when the flow was less than 36.63 L; otherwise, there was a weak outburst risk or a strong outburst risk. When , we obtained
The statistic used for examination was
Through calculation, the test value of the statistic was determined to be . Using the distribution table, we obtained
Because coal and gas outbursts are very dangerous, the prediction error will cause serious consequences. Therefore, a higher degree of confidence value should be selected; was used for a confidence level of the sample of 99%. Because , there was a significant difference between the mean values of the two sets of variables, and the discrimination was valid.
Similarly, the number of weak outburst samples and the number of strong outburst samples were and , respectively, and the mean value was . The sum of the covariances of the two sets of samples was . Additionally, . The coefficient of the discriminant function was . Therefore, the critical value of the strong outbursts was 80.85 L.
Through calculations, the test value of the statistic was determined to be . Using the distribution table, we obtained
Because , there was a significant difference between the mean values of the two sets of variables, and the discrimination was valid.
5.3. BackDiscriminant Analysis of the Critical Values
The backdiscriminant analysis of the discriminant analysis results was performed according to the following process: the critical values (i.e., 36.63 L and 80.85 L) were used to determine the outburst risk. In addition, the index method involving the IGEER index was also used to determine the outburst risk. If the two determination results were consistent, the sample point was classified as a normal point; otherwise, the sample point was classified as an anomalous point, and the backdiscrimination was erroneous. Figure 6 shows the backdiscrimination results.
In Figure 6, the critical values divided the 48 samples into three sections. The sample points within the dotted line boxes were anomalous points. There was one anomalous point in the nonoutburst section ABCD (4, 28.70 L); one anomalous point in the weak outburst section CDEF (14, 42.46 L); and two anomalous points in the strong outburst section EFGH (3, 98.18 L) and (14, 103.33 L). Therefore, the outburst and weak outburst samples were backdiscriminated 38 times, and the backdiscrimination was erroneous twice (correct backdiscrimination rate: 94.74%). The weak and strong outburst samples were backdiscriminated 28 times, and the backdiscrimination was erroneous two times (correct backdiscrimination rate: 92.86%). The correct backdiscrimination rates were all above 90%. The high rates of correct backdiscrimination indicate that the critical values obtained from the discriminant analysis were accurate.
6. Verification of the IGFB Critical Values in the Laboratory
Because of the rarity of outbursts, field verification of the above critical values is challenging. Therefore, to verify the accuracy of the above results, outburst simulation tests were conducted in the laboratory. Figure 7 shows the experimental device.
Each coal seam was compressed five times during the simulation process. After compression, each coal seam was subjected to vacuum pumping for 12 h and then filled with gas. Prior to filling each coal seam with gas, the initial gas flow and the gas pressure in the borehole were fitted, and the fitting function was obtained. Figure 8 shows the resulting fitting curves. By substituting the critical values (i.e., 36.63 L and 80.85 L) into the fitting curves, the gas filling pressure () was obtained. The gas filling process was performed for more than 48 h to attain adsorption equilibrium. However, because the adsorption process was relatively complex, it could not be guaranteed that the gas filling pressure was equal to the critical value. Therefore, the flow was indirectly calculated based on the equilibrium pressure during the determination process.
(a)
(b)
The gas dynamic phenomena were classified into three types in the outburst simulation: nonoutbursts, weak outbursts, and strong outbursts. For the nonoutbursts, the percentage of the volume of the collapsed coal in the total volume of the coal (referred to as the “throwout ratio”) was 0–5%. For the weak outbursts, the coal wall was damaged, and the throwout rate was 5–40%. For the strong outbursts, there was an intense gas dynamic phenomenon, and the throwout rate was more than 40%. Eight simulation tests were conducted (Table 2); Figure 9 shows a photograph of some of the tests.

(a)
(b)
In each of the eight simulation tests, the actual dynamic phenomenon of the coal seam was consistent with the outburst type determined based on the critical value of IGFB. This consistency indicates that the determined critical value was reliable.
7. Conclusions
(1)The initial gas flow released within 3 min from a 1 m long borehole with a diameter of 42 mm was measured in the laboratory; a total of 48 sets of data were obtained. The outburst risk corresponding to the IGFB was classified based on the critical values of the IGEER; 20 sets of nonoutburst data, 18 sets of weak outburst data, and 10 sets of strong outburst data were obtained.(2)A linear discriminant analysis based on Fisher’s criterion was established for IGFB. Through data normalization and analysis, the critical values of the weak and strong outburst risks were predicted using the method based on IGFB (36.63 L and 80.85 L, resp.). Furthermore, backdiscriminant analysis was performed, and the accuracy was 94.74% and 92.86%, respectively.(3)Eight simulation tests were conducted in the laboratory. The test results verified the accuracy of the critical values of the outbursts obtained using the method based on IGFB.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
Acknowledgments
This paper was supported by the Natural Science Foundation of Jiangsu Province, China (Grants nos. BK20150195, BK20150180, and BK20150181), the Graduate Research and Innovation Projects of Jiangsu Province, China (Grant no. KYLX151431), and financial support from the Project Funded by the Priority Academic Program Development of Jiangsu Higher Education Institutions (PAPD).
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Copyright © 2017 Xiaowei Li et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.