Influence of different casing materials on borehole wall pressure of high-energy gas-generating agents
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摘要: 深部煤岩爆破风险高、水力压裂受限,亟需可控破岩技术。高能产气剂作为一种先进高能气体压裂技术,以其卓越性能在破岩领域展现出显著优势,为煤炭高效安全开采提供了有力技术支撑。试验以高能产气剂外壳材料为突破口,研究不同外壳材料对煤岩破岩孔壁压力的影响,构建了全过程压力监测系统,选用PVC(polyvinyl chloride)透明、PVC白色和牛皮纸管3种外壳材料,进行孔壁压力试验,以衰减指数和可信度最为评价指标,对比得到材料物理性质对孔壁压力的影响。结果表明,启动剂点火后产生应力波和少量气体,应力波到达第1个峰值后,气体扩散致压力下降,应力波反射与气体膨胀波叠加形成第2个峰值,气体膨胀变化形成第3个峰值。因无主药剂,启动剂组压力峰值最小,升压时间最短,加载率最低,能量释放少,传递效率低。含主药剂的3组试验在距离高能产气剂 10 cm处达到压力峰值,约为200 MPa,升压时间控制在 20 ms附近。3组不同外壳材料的压力峰值衰减系数从大到小依次为:PVC透明外壳材料、PVC白色外壳材料、牛皮纸管。升压时间衰减系数从大到小依次为:PVC透明外壳材料、牛皮纸管、PVC白色外壳材料。加载率衰减系数从大到小依次为:PVC白色外壳材料、PVC透明外壳材料、牛皮纸管。PVC白色外壳材料因高弹性模量和低泊松比,在靠近高能产气剂位置的压力峰值、升压时间和加载率方面表现最佳,能量传递效率最高。PVC透明外壳材料在靠近高能产气剂位置的压力峰值和加载率高于纸管,但在远距离处低于纸管,表现出较强的方向性和集中性。纸管外壳材料能量分布均匀,但整体能量集中能力弱,升压时间和加载率均最低。研究结果为优化高能产气剂设计、提高破岩效果提供了理论依据。Abstract: Deep coal rock blasting poses high risks, and hydraulic fracturing faces limitations, necessitating the development of controllable rock-breaking technologies. As an advanced high-energy gas fracturing technique, high-energy gas-generating agents demonstrate remarkable advantages in rock fragmentation, providing robust technical support for efficient and safe coal mining. This study focuses on the casing materials of high-energy gas-generating agents, investigating their impact on borehole wall pressure during coal rock fracturing. A comprehensive pressure monitoring system was established, employing three casing materials—transparent PVC, white PVC, and kraft paper tubes—for borehole wall pressure experiments. Attenuation indices and reliability were selected as evaluation metrics to analyze the influence of material physical properties on borehole wall pressure. Results indicate that the initiator, upon ignition, generates stress waves and a small amount of gas. The stress wave induces the first pressure peak, followed by a decline due to gas diffusion. The superposition of reflected stress waves and gas expansion waves forms the second peak, while gas expansion variations produce the third peak. Without the main agent, the initiator group exhibits the lowest pressure peak, shortest pressure rise time, minimal loading rate, limited energy release, and low transmission efficiency. For the three groups containing the main agent, pressure peaks near the high-energy gas-generating agent (10 cm away) approximate 200 MPa, with pressure rise times around 20 ms. The attenuation coefficients of pressure peaks for the three casing materials from the biggest to the smallest follow the order: transparent PVC, white PVC, and kraft paper tube. The attenuation coefficients of pressure rise times from the biggest to the smallest rank as: transparent PVC, kraft paper tube, and white PVC. For loading rate attenuation coefficients, the sequence from the biggest to the smallest is: white PVC, transparent PVC, and kraft paper tube. Because of its high elastic modulus and low Poisson’s ratio, white PVC casing demonstrates optimal performance in pressure peak, rise time, and loading rate near the high-energy gas-generating agent, achieving the highest energy transmission efficiency. Transparent PVC casing exhibits higher pressure peaks and loading rates than the paper tube near the agent but underperforms at longer distances, indicating strong directionality and concentration. The kraft paper tube ensures uniform energy distribution but exhibits the weakest overall energy concentration, along with the longest rise times and lowest loading rates. These findings provide a theoretical foundation for optimizing high-energy gas-generating agent designs and enhancing rock-breaking efficacy.
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Key words:
- borehole wall pressure /
- casing material /
- high-energy gas /
- rock-breaking efficacy
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表 1 材料的物理性质
Table 1. Physical properties of materials
剂壳类型 弹性模量/GPa 泊松比 PVC透明 3.16 0.42 PVC白色 3.63 0.37 纸管 2.32 0.29 表 2 待爆品试验
Table 2. Products for testing before explosion
组别 启动剂 外壳材料 A组 40 mm启动剂 无 B组 PVC透明 C组 PVC白色 D组 纸管 表 3 孔壁压力参数
Table 3. Hole wall pressure parameter
组别 监测点 压力峰值/MPa 升压时间/ms 加载率/(MPa·ms−1) A组 测点1 15.54 22.61 0.69 测点2 92.88 17.11 5.43 测点3 94.53 17.91 5.28 B组 测点1 19.30 25.44 0.76 测点2 271.89 22.49 12.09 测点3 178.76 21.84 8.18 C组 测点1 28.91 25.50 1.13 测点2 282.16 21.10 13.37 测点3 165.92 19.20 8.64 D组 测点1 23.00 28.07 0.82 测点2 246.21 24.67 9.98 测点3 170.43 24.42 6.98 表 4 不对称指数
Table 4. Asymmetric index
组别 峰值差值/MPa 时间差值/ms 不对称指数/(MPa·ms−1) A组 1.65 0.80 1.32 B组 93.13 0.65 60.53 C组 116.24 1.90 220.86 D组 75.78 0.25 18.95 表 5 压力峰值衰减指数
Table 5. Pressure peak attenuation index
组别 p2,peak/
MPap3,peak/
>MPa(p2,peak−p3,peak)/
MPa压力峰值衰减系数
β1/(MPa·cm−1)可信度δ A组 93.71 15.54 78.17 7.82 0.283 B组 225.33 19.30 206.03 20.60 0.256 C组 224.04 28.91 195.13 19.51 0.249 D组 208.32 23.00 185.32 18.53 0.272 表 6 升压时间衰减指数
Table 6. Attenuation index of boost time
组别 t2,peak/
mst3,peak/
ms(t2,peak−t3,peak)/
ms升压时间衰减
系数β2/
(ms·cm−1)可信度δ A组 17.51 22.61 5.10 0.51 0.283 B组 22.17 25.44 3.27 0.33 0.256 C组 20.15 25.50 5.35 0.54 0.249 D组 24.55 28.07 3.52 0.35 0.272 表 7 加载率衰减指数
Table 7. Loading rate attenuation index
组别 a2,peak/
(MPa·ms−1)a3,peak/
(MPa·ms−1)(a2,peak−a3,peak)/
(MPa·ms−1)加载率衰减
系数β3/
(MPa·ms−1·cm−1)可信度δ A组 5.36 0.69 4.67 0.48 0.283 B组 10.14 0.76 9.38 0.94 0.256 C组 11.01 1.13 9.88 0.99 0.249 D组 8.48 0.82 7.66 0.77 0.272 -
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