The working face often encounters faults as the coal mining process moves to complex geological regions. In this case, when using conventional mining methods with coal pillar and the gob-side entry retaining, the stress on the protective pillar and the roadside filling near the fault increased because the roof transfer path was not changed and the pressure on the roof was not relieved. If the bearing capacity limit of the protective pillar and the roadside filling is exceeded, rock burst or other disasters may occur. However, GEFRCPR was able to successfully avoid these disasters under complex geological conditions owing to its none coal pillar and pressure release characteristics. The diagram in Fig. 2 shows the principle of GEFRCPR passing through the fault.
Figure 2.
Based on a number of academic researches on normal fault (Wang et al. 2014), it is found that the stress increase was most prominent as the working face of the hanging wall is moving to normal fault. As a result, the mining process from the working face of the hanging wall to the normal fault was taken as the key area of our study, and the mechanical model was constructed as is shown in Fig. 3. When the working face moved from the hanging wall to the footwall, the basic roof in the upper gob side was broken to form the hinge structure, as is shown in Fig. 3. At this point, the load on the basic roof was shared by the footwall of the fault, the pillars in the fault, and the gob-side gangues. Half of the load from rotating broken blocks on the basic roof above the gob side was shared by the gob-side gangues, and the other half was transferred to the pillars in the fault and the footwall of the fault by squeezing broken blocks.
Figure 3.
At the fault, the fault surface transferred the load above the pillars in the fault and the load on the basic roof above the gob side to the footwall by a certain pressure transfer factor.
The load above the pillars in the fault is qL
The load on the basic roof above the gob side is qL
The mining load that was transferred through the fault to the footwall can be expressed as
$$Q{\text{=}}K\left( {qL+\frac{{{Q_{\text{1}}}}}{{\text{2}}}} \right){\text{=}}K\left( {qL+\frac{{qL}}{2}} \right)=\frac{{3KqL}}{2}$$
1
where Q in MN/m stands for the load transferred from hanging wall to footwall of normal fault; Q1 in MN/m represents the load on the basic roof above the gob side and Q1 = qL; K is the load transfer factor from hanging wall to footwall of normal fault and 0 ≤ K ≤ 1; q in MN/m2 is the load on broken pieces of the basic roof above the pillar per unit area and q = γh; γ in N/m3 is the average volume weight of the layer under load and the current layer of the basic roof above the pillar; h in m stands for the total thickness of strata above the coal seam; L in m is the length of the rotating broken pieces of the gob-side basic roof transferred to the basic broken pieces of the basic roof above the pillar and is calculated by periodic weighting pace.
The load that was not transferred to the footwall of the fault was borne by the pillars on the working face, which mainly included the load on the broken pieces of the basic roof above the pillars in the fault, the load on the broken pieces of the roof above the gob side that were not transferred to the footwall of the fault, and the load on strata of the basic roof above the pillar in the fault.
The load that is not transferred to the footwall of the fault is \(\left( {{\text{1-}}K} \right)\left( {{\text{qL+}}\frac{{{\text{q}}L}}{{\text{2}}}} \right)=\frac{{3\left( {1 - K} \right)qL}}{2}\)
The load on strata of the basic roof above the pillar in the fault is \({\gamma _z}{h_z}\left( {\frac{{{h_z}\tan \alpha }}{2}+B+D} \right)\)
The load on the pillars in the fault is
$${Q_d}=\frac{{3\left( {1 - K} \right)qL}}{2}+{\gamma _z}{h_z}\left( {\frac{{{h_z}\tan \alpha }}{2}+B+D} \right)$$
2
The load intensity on the pillars in the fault is obtained from Eq. (2):
$${q_d}=\frac{{3\left( {1 - K} \right)qL+{\gamma _z}{h_z}^{2}\tan \alpha +2{\gamma _z}{h_z}D}}{{2B}}+{\gamma _z}{h_z}+\gamma h$$
3
where Qd in MN/m is the load on the pillars in the fault; qd in MN/m stands for the intensity of load on the pillars in the fault; γz in N/m3 is the volume weight of strata on the immediate roof; hz in m is the thickness of strata on the immediate roof; α in ° is the dip angle of fault; B in m is the width of the pillars in the fault; D in m is the distance from the coal seam on the working face to the gob.
According to the Eq. (3), when the working face gradually moved to the normal fault, the pillars in the fault decreased, namely B in Eq. (3) decreased, while other factors remained the same, then the load intensity qd above the pillars in the fault became larger. When the working face came closer to the normal fault, the cutting effect of the fault made the overlying strata on the working face of the hanging wall on the pillars in the fault an inverted wedge rock. As the working face approached the normal fault, the effect arising from the inverted wedge which overlaid the strata tended to be more prominent and led to greater stress on the pillars in the fault. Under the combined above effects, the closer the working face was to the normal fault, the greater the stress on the pillars in the fault of the working face would be. When reaching the bearing capacity limit, the pillars on the working face were subjected to plastic failure, the stress on the pillars in the fault was transferred to two ends of the working face until it reached the solid coal at both sides of the working face. As a result, as the working face came closer to the normal fault, the stress on the solid coal side at both sides of the working face gradually increased. In other words, when the working face gradually came closer to the normal fault, as the stress on the roof and at the solid coal side was greater, reinforced support should be provided to ensure the effect and stability of the entry retaining.