轴向分布式药包激发地震波场模型

徐谦; 王仲琦

doi:10.11883/bzycj-2020-0236

轴向分布式药包激发地震波场模型

doi: 10.11883/bzycj-2020-0236

徐谦,
王仲琦^,

北京理工大学爆炸科学与技术国家重点实验室，北京 100081

基金项目: 国家科技重大专项（2016ZX05006-002）

详细信息

作者简介:
徐　谦（1993－　），男，博士研究生，chinaxuqian@126.com

通讯作者:
王仲琦（1972－　），男，博士，副教授，czqwang@bit.edu.cn

中图分类号: O382.2
计量
- 文章访问数: 435
- HTML全文浏览量: 324
- PDF下载量: 46
- 被引次数: 0
出版历程
- 收稿日期: 2020-07-03
- 修回日期: 2020-09-07
- 网络出版日期: 2021-07-05
- 刊出日期: 2021-07-05

Model of seismic wave field excited by axially distributed explosive

XU Qian,
WANG Zhongqi^,

State Key Laboratory of Explosion Science and Technology, Beijing Institute of Technology, Beijing 100081, China

摘要

摘要: 炸药震源激发地震波场幅频特性直接影响地震勘探精度，本文通过计算研究轴向分布式药包激发地震波场幅频特征规律：以球形空腔震源模型为基础，采用叠加方法获得轴向分布式药包激发地震波场计算方法，并与数值模拟结果进行对比。研究表明：该方法误差在7%以内；在爆心距大于药柱总长度9.8倍时轴向分布式药包所激发地震波速度场与球形药包基本一致，但地震波的频率更高。
- 地震波 /
- 地震勘探 /
- 炸药震源 /
- 轴向分布式药包
Abstract: The amplitude-frequency characters of the seismic wave excited by the explosive source directly affect the seismic exploration accuracy. In order to reveal the characteristic law of the amplitude and frequency of the seismic wave field excited by an axially distributed explosive, the study on the calculation method of the seismic wave field of the axially distributed explosive was proposed. Based on the spherical cavity source model, the calculation method of the seismic wave field excited by the axially distributed explosive source was obtained by using the superposition method, and the seismic wave field model excited by the axially distributed charge was established. This model can describe the characteristics of the seismic wave field of distributed explosive sources in seismic exploration. Comparison with numerical simulation shows that the error between the theoretical model and the numerical model is within 5% in the radial direction, and the error between the theoretical model and the numerical model is within 3.4% in the axial direction. Compared with the field experiment results, the theoretical model seismic wave vibration velocity error is within 10% when the blast center distance is greater than 14 m. The calculation accuracy increases with the increase of the distance, and the error is less than 6% when the distance is greater than 24 m. When the blast center distance is the same, the vibration speed in the axial direction is greater than the vibration speed in the radial direction. The difference between the two decreases with the increase of the blast center distance. When the blast center distance is 9.8 times the total length of the charge, the axial direction is the vibration speed difference in the radial direction is within 5%, and the frequency of the seismic wave is higher. The research shows that the model can accurately describe the amplitude-frequency character of the seismic wave excited by the axially-distributed explosive.
- seismic wave /
- seismic exploration /
- explosive source /
- axially distributed explosive

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图 1 轴向分布式药包在岩土介质中爆炸分区

Figure 1. Explosive zoning of an axially distributed charge in geotechnical media

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图 2 轴向分布式激发方案

Figure 2. Axial distributed excitation

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图 3 轴向分布式药包最大振动速度

Figure 3. Maximum vibration velocity at different locations of axial distributed excitation:

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图 4 传感器布置

Figure 4. Sensor layout

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图 5 不同激发方案地震波的峰值粒子振动速度衰减规律

Figure 5. Peak particle vibration velocities of seismic waves with different excitation schemes

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图 6 球形药包和轴向分布式药包地震波场

Figure 6. Seismic wave field of spherical explosive and axially-distributed explosive

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图 7 相同质点振动速度时球形药包距离与柱形药包轴向、径向距离对比

Figure 7. Comparison of the distance between spherical explosives and different directions of axially distributed cylindrical explosives at the same particle vibration velocity

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图 8 轴向分布式柱形药包和球形药包形成地震波主频对比

Figure 8. Comparison of frequency of spherical charge and axially distributed charge

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表 1 轴向分布式炸药激发方案

Table 1. Excitation scheme of axially distributed explosives

方案	药柱数量	单药柱质量/kg	药柱间隔/mm	总药量/kg	延迟时间/s	激发方向
3 kg×2	2	3	400	6	0.3	由上而下
2 kg×3	3	2	400	6	0.3	由上而下
1.5 kg×4	4	1.5	400	6	0.3	由上而下

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表 2 土介质参数

Table 2. Parameters of soil

$ {\sigma }_{\mathrm{c}} $/MPa	$ {\sigma }_{\mathrm{t}} $/MPa	$G$/GPa	$ \alpha $	$ \varphi /\mathrm{k}\mathrm{P}\mathrm{a} $	$ {\rho }_{\mathrm{s}} $/($ \mathrm{k}\mathrm{g} \cdot {\mathrm{m}}^{3} $)	k/MPa	G/MPa	$ {\sigma }_{\mathrm{y}} $/MPa
13	2	0.147	0.115	11.8	1840	245	147	22

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表 3 TNT炸药特性参数

Table 3. Parameters of TNT

C₁/GPa	C₂/GPa	R₁	R₂	ω	ρ_e/（kg·m⁻³）	D/（m·s⁻¹）	e/（J·m⁻³）	p_CJ/GPa	p₀/GPa
373.7	3.747	4.15	0.90	0.35	1650	6930	6.0$ \times {10}^{9} $	21	9.82

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表 4 检波器部分参数

Table 4. Parameters of sensors

量程/V	灵敏度/[V·（m·s⁻¹）⁻¹]	通频带/Hz	误差范围/%
10	7	1～100	＜0.05

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表 5 不同位置(x)处峰值粒子速度实验结果相与计算结果的相对误差

Table 5. Table 6 Relative error of experimental results of peak paritcle velocity to the calculational ones at different position x

炸药激发方案	误差/%
炸药激发方案	x=10 m	x=14 m	x=18 m	x=22 m	x=26 m	x=30 m
3 kg×2	4.52	4.84	4.77	4.32	3.92	4.12
2 kg×3	4.56	4.63	4.32	3.93	4.12	3.93
1.5 kg×4	8.01	6.82	6.51	7.25	8.80	9.44

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