MONITORING MICROSEISMIC OF âMOâ UNDERGROUND MINING USING PHASENET, GAMMA, AND NONLINLOC PROGRAMS
The increase of seismicity in seismic areas and the emergence of seismicity in aseismic areas is a result of underground mining. Tunneling and block caving are mining activities to access and extract mineral resources. Tunneling and block caving can pose accident risks, such as tunnel collapse, r...
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Format: | Final Project |
Language: | Indonesia |
Online Access: | https://digilib.itb.ac.id/gdl/view/76588 |
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Institution: | Institut Teknologi Bandung |
Language: | Indonesia |
Summary: | The increase of seismicity in seismic areas and the emergence of seismicity in
aseismic areas is a result of underground mining. Tunneling and block caving are
mining activities to access and extract mineral resources. Tunneling and block
caving can pose accident risks, such as tunnel collapse, rock bursts, slope
instability in open pit mines, and seismic hazards. Seismic activity in mining areas
varies widely from small to large-scale earthquakes associated with damage from
seismic events. Microseismic is seismic wave activity that has a small size and is
not necessarily felt by humans. Therefore, microseismic monitoring is needed in
underground mining areas to minimize losses both in material and casualties. In
this study, the data used are 50 microseismic events of the underground mine "MO"
for the period November-December 2022. At the initial stage of the study, the phase
selection of P and S waves was carried out using the algorithm of the PhaseNet
program. The PhaseNet program shows good performance in determining the
arrival times P and S waves. PhaseNet is also able to determine the arrival time of
P and S waves in poor waveforms data. However, the PhaseNet program also has
limitations, namely the existence of multiple picking. The existence of multiple
picking can affect the accuracy and quality of the picking results, so event
associations using GaMMA are needed. In this study, 4 experiments were
conducted with the dbscan parameters used in the association were 0.1; 0.2; 0.5;
and 1.0. And the most optimal result is 0.5. This is because the events that can be
used at DBSCAN 0.5 are 41 events with an average difference in arrival time of
0.691 seconds. The 41 events used in NonLinLoc have differences in latitude,
longitude, and depth that are quite far for microseismic cases, namely 0.420 km,
0.604 km, and 0.765 km. The differences in P and S wave arrival times and locations
between the "MO" mine catalog data and the PhaseNet and GaMMA data are
caused by problems in extracting waveforms and the assumed homogeneous
velocity model. |
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