Microseismic Temporal-Spatial Precursory Characteristics and Early Warning Method of Rockburst in Steeply Inclined and Extremely Thick Coal Seam
Abstract
:1. Introduction
2. Precursor Characteristic Parameters and Early Warning Method
2.1. Precursor Characteristic Parameters for Temporal Pre-Warning of Rockburst
2.2. Precursor Characteristic Parameter for Spatial Pre-Warning of Rockburst
2.2.1. Energy Density Index of MS
2.2.2. Velocity and Velocity Anomaly
2.3. Temporal-Spatial Comprehensive Early Warning Method
3. Case Study
3.1. Basic Conditions of the Field
3.2. Temporal Early Warning Results and Analysis
3.2.1. Variation of Energy and Event Count
3.2.2. Variation of Energy and Event Count Deviation
3.2.3. “Critical Value + Trend” Temporal Early Warning Method of Rockburst Hazard
3.3. Spatial Early Warning Results and Analysis
3.3.1. Evolution Law of EDIM and Discussion
3.3.2. Passive Tomographic Results and Discussion
4. Effectiveness and Field Application
4.1. Effectiveness Test Method
4.2. Early Warning Capability of “Critical Value + Trend” Early Warning Method
4.3. Comparative Study on the Early Warning Effectiveness of “Critical Value” and “Critical Value + Trend” Early Warning Method
4.4. Field Application of Temporal-Spatial Comprehensive Early Warning Method
5. Conclusions
- Three new spatial/temporal quantification parameters (energy deviation, event count deviation, and EDIM) were proposed. The temporal precursor characteristic parameters of rockburst and high energy tremor, including daily total energy Ed, event count P, energy deviation DE, event count deviation DP were used to comprehensively early warn rockburst risk in time series. The sharp-rise-sharp-drop variation in total daily energy and event count, DE ≥ 20, DP ≥ 1, could be regarded as a precursor to rockburst and high energy tremor occurrence. Laboratory AE experiment revealed that using the precursor characteristics obtained from this study could be feasibly used to warn of rockburst risk.
- A “critical value + trend” early warning method of SIETCS was proposed by combining MS energy, trend, and quantitative precursor characteristics. Firstly, based on the MS energy value E, a critical value early warning was used to determine the initial rockburst risk level. Then, the trend and quantitative precursor characteristics were used to correct the initial risk level and to determine the final rockburst risk level. The trend and quantitative precursor characteristics could play a very good supplementary role to the critical value of early warning, thus enhancing early warning level and improving early warning accuracy.
- The high EDIM, velocity, and velocity anomaly areas were observed to be mainly distributed within the rock pillar and roof around the working surface. The fracturing of rock pillar and roof was the main inducing factor of rockbursts. The spatial distribution of both EDIM and passive velocity tomography could compensate for the shortcomings of the “critical value + trend” early warning method, specifically to determine the rockburst risk area and to guide the accurate implementation of the pressure relief engineering.
- While the early warning capability of the “critical value” warning method had R = 0.23, the early warning capability of the “critical value + trend” temporal early warning method had R = 0.83, which was 3.6 times the “critical value” early warning method. The “critical value + trend” early warning method had marked significance for the warning of the rockburst risk in SIETCS.
- This study could improve MS monitoring and provide a reference for rockburst early warning in SIETCSs. Most importantly, it should be emphasized that warning of a rockburst must use the comprehensive warning method, including both temporal early warning method (both qualitative and quantitative analysis of microseismicity evolution) and spatial early warning method (spatial evolution law of EDIM, velocity, and velocity anomaly), as well as some traditional detection methods. The spatio-temporal comprehensive early warning method not only identified the possibility of rockburst occurrence but also early warned stress concentration areas and rockburst risk areas. Furthermore, field application in this study showed that this method could help to reduce the probability of rockburst.
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Acknowledgments
Conflicts of Interest
References
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Name | Basic Equations | Key References |
---|---|---|
Number of events | Total number of MS events in a given time window | Srinivasan et al. (1997); Tan et al. (2015); Li et al. (2018) |
Amount of energy | Total amount of MS energy in a given time window | |
b value | Gutenberg and Richter (1944); Li et al. (2017); Cao et al. (2018) | |
N(M) is the cumulative number of MS events having a magnitude larger than M, and a and b are constants. It has been shown in laboratory studies, field observations, and numerical simulations that the slope of this distribution curve depends on stress conditions | ||
A(b) value | Wu and Cao (1983) | |
b is the b value, and Mi is the magnitude of the MS event. | ||
Seismicity degree SD | Gu and Wei (1987) | |
N is the total number of MS events, and Mmax is the maximum magnitude | ||
Lack of shock bL | Aki (1965) | |
Mmean is the mean magnitude and Mmin is the minimum magnitude of given MS events | ||
Fault total area | Lu et al. (2015) | |
k0 is the lower limit of the statistical MS energy level, and k is the energy level of each event. N(k) is the event count of MS energy level k | ||
(correspondingly, the energy is 10k–10k+1 J) | ||
Z value | Lu et al. (2015) | |
is the arithmetic mean magnitude of all MS events in the entire monitoring period, which is a relatively stable amount to manifest background characteristics. is the arithmetic mean magnitude of MS events over the time window. N and n are the quantities of MS events used for calculating and , respectively, and σM and σm are their standard deviations accordingly | ||
Source concentration degree | Cai et al. (2014) | |
λ1, λ2, and λ3 are standard orthogonal eigenvectors of the covariance matrix of MS hypocentre parameters x, y, z | ||
Seismic diffusivity | Mendecki (1996) | |
is the mean distance between consecutive events and is the mean time between events | ||
Fractal dimension | Xie and Pariseau (1993); | |
C(r) is the correlation integral of the energy or number of MS events, and r is the energy or spatial radio scale | Feng et al. (2016) | |
Algorithm complexity AC | Lv and Lu | |
n is the number of magnitudes of MS events over the time window; MAC = Mmax − Mmin + 1, and Mmax and Mmin here are the maximum and minimum magnitudes, respectively | (1993) | |
Apparent stress/volume | , | Mendecki (1996); Tang and |
μ is the shear rigidity modulus, EA is the MS energy, and M0 is the MS moment | Xia (2010) | |
Energy index | Mendecki (1996); Tang et al. (2010); Xu et al. (2011) | |
is the average energy released by events of the same MS moment | ||
Time information entropy Qt | Zhu and Wang | |
where pi = (ti + 1−ti)/(tN−t1), with value from 0 to 1, and ti is the occurrence time of the ith MS event. | (1988) | |
Energy ratio | Ratio of the S- and P-wave energies (ES/EP) | Gibowicz and Kijko (1994) |
Rockburst Risk Index | Stress Concentration Degree | Velocity Anomaly An, % |
---|---|---|
0 | None | <5 |
1 | Weak | 5–15 |
2 | Middle | 15–25 |
3 | Strong | >25 |
Early Warning Result | ||||
No Rockburst or High Energy Tremor | Rockburst or High Energy Tremor | |||
Actual situation | No rockburst or high energy tremor | N0 | ||
Rockburst or high energy tremor | N1 | |||
N0 | N1 | N |
Early Warning Result | Total Number of Times | |||
---|---|---|---|---|
No Rockburst or High Energy Tremor | Rockburst or High Energy Tremor | |||
Actual situation | No rockburst or high energy tremor | |||
161 | 7 | 168 | ||
Rockburst or high energy tremor | ||||
1 | 7 | 8 |
Early Warning Result | Total Number of Times | |||
---|---|---|---|---|
No Rockburst or High Energy Tremor | No Rockburst or High Energy Tremor | |||
Actual situation | No rockburst or high energy tremor | |||
165 | 3 | 168 | ||
Rockburst or high energy tremor | ||||
6 | 2 | 8 |
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Li, Z.; He, S.; Song, D.; He, X.; Dou, L.; Chen, J.; Liu, X.; Feng, P. Microseismic Temporal-Spatial Precursory Characteristics and Early Warning Method of Rockburst in Steeply Inclined and Extremely Thick Coal Seam. Energies 2021, 14, 1186. https://doi.org/10.3390/en14041186
Li Z, He S, Song D, He X, Dou L, Chen J, Liu X, Feng P. Microseismic Temporal-Spatial Precursory Characteristics and Early Warning Method of Rockburst in Steeply Inclined and Extremely Thick Coal Seam. Energies. 2021; 14(4):1186. https://doi.org/10.3390/en14041186
Chicago/Turabian StyleLi, Zhenlei, Shengquan He, Dazhao Song, Xueqiu He, Linming Dou, Jianqiang Chen, Xudong Liu, and Panfei Feng. 2021. "Microseismic Temporal-Spatial Precursory Characteristics and Early Warning Method of Rockburst in Steeply Inclined and Extremely Thick Coal Seam" Energies 14, no. 4: 1186. https://doi.org/10.3390/en14041186
APA StyleLi, Z., He, S., Song, D., He, X., Dou, L., Chen, J., Liu, X., & Feng, P. (2021). Microseismic Temporal-Spatial Precursory Characteristics and Early Warning Method of Rockburst in Steeply Inclined and Extremely Thick Coal Seam. Energies, 14(4), 1186. https://doi.org/10.3390/en14041186