石油运输过程中爆炸对岩石的破坏

Rafail Mehdiev, Alekber Mehdiyev Rafail Mehdiev, Alekber Mehdiyev, Vurgun Gakhramanov Vurgun Gakhramanov
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引用次数: 0

摘要

当油气井准备运行时,在井底进行钻探以与地层建立联系时,人们认为岩石的破碎程度与施加载荷的速度成正比。由于其产生的应力,破碎程度较高。文章建议在计算公式中使用一些经验系数来考虑必要岩石的破碎质量。在流体力学假设的基础上,对岩石分散过程的动力学进行了研究。在此,根据质量、能量和动量守恒定律给出了微分方程系的解法。根据山岩的强度特性,在整个环境的连续性中发现了破碎线,这决定了岩石破碎的最终效果。然而,关于岩石不可压缩性和爆炸冲力传递到直接环境的公认假设大大降低了结果的实用价值。应该注意的是,在直接临近荷载的附近区域,山岩受到不均匀的体积压缩。在这种情况下,最大的切向应力主要发生在与径向方向成 450 角的平面上。因此,螺旋滑动线系统将岩石分成小块。在这一区域之外,由于岩块的膨胀,形成了径向裂缝系统。当气穴中的压力减小,岩块向载荷方向后移时,就会出现切向裂缝。体积压缩区和到达区的组合构成了受控破碎区。当压缩波到达裸露表面时,就变成了应力波。当应力波从表面到达负载处时,会形成跳跃裂缝系统。具有足够爆炸能量的爆炸性气体的高爆炸效应会导致这种破碎岩石的释放。显然,这一概念对于山岩爆炸崩解理论的发展非常重要。因为岩石的溶解性质与声学硬度之间没有明确的关系。最早明确描述冲击波形成机理及其在引爆达到装药腔边界时转化为更具爆炸性的地震波的人之一。在岩石中,冲击波是在气穴膨胀的整个过程中形成的。关键词:岩石强度;恒定材料;尺度效应;岩石;破坏概率;断裂;鲁棒性理论;微裂缝;矿物;经验常数;缺陷密度;位移;压缩。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
DESTRUCTION OF ROCKS BY EXPLOSION DURING OIL TRANSPORTATION
When oil and gas wells are ready for operation, when drilling is carried out at the bottom of the well to establish contact with the formation, it is considered that the degree of crushing of the rocks is proportional to the speed of application of the load. As a result of the stresses created by them, the degree of fragmentation is higher. In the article, it is proposed to take into account the quality of crushing of the necessary rock by using some empirical coefficients in the calculation formulas. The dynamics of the rock dispersion process is studied on the basis of the hydrodynamic hypothesis. Here, the solution of the system of differential equations is given based on the fundamental laws of conservation of mass, energy and momentum. Based on the strength properties of mountain rocks, broken lines are found in the continuum of the whole environment, which determines the final effect of rock crushing. However, the accepted assumptions about the incompressibility of the rock and the transfer of the explosive impulse to the immediate environment significantly reduce the practical value of the results. It should be noted that in the immediate area directly adjacent to the load, the mountain rock is under uneven volume compression. In this case, the largest tangential stresses occur mainly in planes oriented at an angle of 450 to the radial direction. Thanks to this, a system of spiral sliding lines breaks the rock into small blocks. Outside this zone, a system of radial cracks is formed as a result of the expansion of the massif. When the pressure in the gas cavity decreases and the mass moves back in the direction of the load, tangential cracks appear. The combination of the volume compression zone and the reach zone constitutes the controlled crushing area. When the compression wave reaches the bare surface, it becomes a stress wave. As this wave travels from the surface to the load, it forms a system of jump cracks. The high explosive effect of explosive gases with sufficient explosion energy causes the release of such shattered rock. Obviously, this concept is very important for the development of the theory of explosive disintegration of mountain rocks. Because there is no unequivocal relationship between the nature of the dissolution of the rock and the acoustic hardness. One of the first to clearly describe the mechanism of shock wave formation and its transformation into a more explosive and seismic wave when detonation reaches the boundary of the charge cavity. In rocks, shock waves are formed during the entire time of expansion of the gas cavity. It explains in detail the mechanism of cracking phenomena by considering the cracks as a source of multiple reflections of the stress wave. Keywords: rock strength, constant material, scale effect, rocks, destruction probability, fractured, robustness theory, microcrack, mineral, experience constant, density of defects, displacement, compression.
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