WO2022051890A1 - Vibration reduction method based on blast vibration prediction technology - Google Patents

Vibration reduction method based on blast vibration prediction technology Download PDF

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WO2022051890A1
WO2022051890A1 PCT/CN2020/113937 CN2020113937W WO2022051890A1 WO 2022051890 A1 WO2022051890 A1 WO 2022051890A1 CN 2020113937 W CN2020113937 W CN 2020113937W WO 2022051890 A1 WO2022051890 A1 WO 2022051890A1
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blasting
vibration
hole
blast
measuring point
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PCT/CN2020/113937
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French (fr)
Chinese (zh)
Inventor
林飞
张志刚
姜德义
李勇
于魏清
王继峰
周晓红
赵彭
李强
张阳光
耿宏银
厉建兴
叶鑫
马传坤
韩廷亮
张计璨
王德玲
徐海峰
杨宗玲
夏光
吴竞
王召锋
潘先峰
刘治兵
金富
黄嵩
翟清翠
Original Assignee
中煤科工集团淮北爆破技术研究院有限公司
重庆大学
永嘉县住房和城乡建设局
福建海峡科化富兴建设工程有限公司
安徽雷鸣矿业有限责任公司
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Application filed by 中煤科工集团淮北爆破技术研究院有限公司, 重庆大学, 永嘉县住房和城乡建设局, 福建海峡科化富兴建设工程有限公司, 安徽雷鸣矿业有限责任公司 filed Critical 中煤科工集团淮北爆破技术研究院有限公司
Priority to PCT/CN2020/113937 priority Critical patent/WO2022051890A1/en
Publication of WO2022051890A1 publication Critical patent/WO2022051890A1/en

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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F42AMMUNITION; BLASTING
    • F42DBLASTING
    • F42D3/00Particular applications of blasting techniques
    • F42D3/04Particular applications of blasting techniques for rock blasting

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  • the invention relates to the technical field of blasting vibration safety, in particular to a vibration reduction method based on blasting vibration prediction technology.
  • Deep hole step blasting is large in scale and has a wide range of influence. It is very necessary to effectively predict the blasting vibration intensity in the design stage.
  • physical quantities such as acceleration, velocity or displacement can be used.
  • a large number of research experiments show that the velocity index can better reflect the relationship between the building and the degree of damage caused by blasting vibration, and is little affected by the thickness of the cover layer of the transmission medium.
  • A-vibration intensity (displacement, velocity, acceleration, etc.); Q-one-time priming charge or single-stage maximum priming charge (kg); ⁇ -charge index; R-distance from detonation source to measuring point (m) ; K, ⁇ - coefficients related to geological conditions, reflecting the attenuation degree of seismic waves to a certain extent.
  • the long-distance group-hole charge can be approximately regarded as a concentrated charge, which satisfies the basic assumption of Sadowski's formula.
  • the prediction error of the vibration peak value of the measuring point can reach 200%-300%, and the result is not satisfactory. This is obviously unfavorable for knowing and evaluating the impact degree of blasting vibration in advance in blasting construction of adjacent structures and buildings.
  • the present invention proposes a vibration reduction method based on blasting vibration prediction technology.
  • the vibration waveform of group-hole blasting predicted by the vibration waveform of single-hole blasting is basically consistent with the variation law of the measured blasting vibration waveform. Compared with the traditional blasting vibration waveform The formula plus empirical prediction method is more effective and reliable.
  • the vibration reduction method based on blasting vibration prediction technology proposed by the present invention the method steps are as follows:
  • S2 Select several measuring points on the periphery of the reference blasting hole, and arrange the vibrometer in the radial direction of the reference blasting hole and the measuring points;
  • S4 Use the Matlab software to analyze the collected vibration data of the reference blasting hole, input the differential time of the group hole blasting under the n segment, and predict the complete blasting vibration waveform of the measuring point and the maximum blasting vibration velocity of the particle; the details are: Use the xlsread function of Matlab software to read the single-hole blasting vibration signal in the specified path of the document, select the maximum blasting vibration velocity in the three channels (vertical, radial, tangential) of the measured single-hole blasting vibration signal, and set the number of overlapping segments n (the number of blasting holes in the group hole) and the differential time ⁇ t, and the total duration of the group hole waveform is determined by the number of superpositions. Under the for loop, the n-segment group hole blasting waveform superimposed by the channel waveform under the set differential time is realized. At the same time, the maximum blasting vibration velocity of the particle is predicted.
  • S5 Use Matlab software to fit the relationship curve between different differential time and the maximum blasting vibration velocity of the particle, and the relationship between different differential time and vibration reduction rate. Specifically: on the basis of the S4 prediction program, determine the sampling frequency of the vibration measuring instrument, set the differential time range (1-100ms), and perform n superimposition cycles on the single-hole blasting vibration signal at different differential times. Cycle to determine a maximum blasting vibration velocity, thereby obtaining the relationship curve between the maximum blasting vibration velocity and the particle under the differential time.
  • the reference blasting hole is the last blasting hole in the group of holes, and the delay time interval between the blasting of the last blasting hole and the adjacent blasting hole is not less than 500ms.
  • the vibrometers are arranged on the bedrock or wedged into the ground with vibrometers.
  • the blasting parameters include the position of the blasting hole, the distance between the measuring points, the depth of the hole, the propagation medium, the charge per hole, the distance between the holes and the blasting network.
  • the expression of the complete blasting vibration waveform in the S4 is:
  • S(T) is the total blasting vibration velocity of the measuring point, T is a certain moment in the whole process of blasting vibration; K i is the charge coefficient of the ith segment, when the charge amount of each segment, explosive When the blasting parameters such as the type are the same, and the topographic and geological conditions from the blast source to the measuring point are not much different, take 1; S(t i ) is the vibration velocity of the particle generated after the explosion of the ith subsection explosive; t i is the ith The time for the seismic wave to travel from the source to the measuring point after the explosion of a segmented explosive; n is the number of segments; ⁇ (t) is the unit step signal.
  • the expression is:
  • the present invention uses Matlab program numerical simulation, and the group hole blasting vibration waveform predicted by the single hole blasting vibration waveform is basically consistent with the variation law of the measured blasting vibration waveform, and the group hole blasting vibration peak velocity error rate is within 16%. It is more effective and reliable than the traditional formula plus empirical prediction method.
  • the micro-difference time to reduce the blasting vibration effect of blasting is not in half the main vibration waveform period. In the period of 0-100ms, the vibration reduction rate of blasting vibration intensity in the interval of 16ms-20ms is particularly obvious. When it reaches more than 60ms, the group The hole vibration signal acts independently of the single hole blasting vibration signal.
  • Fig. 1 is the blast hole and measuring point arrangement diagram of the embodiment proposed by the present invention
  • Fig. 2 is the reference blasting hole blasting vibration waveform measured by the measuring point M1 of the embodiment proposed by the present invention
  • Fig. 3 is the reference blasting hole blasting vibration waveform measured by the measuring point M2 of the embodiment proposed by the present invention
  • Fig. 4 is the reference blasting hole blasting vibration waveform measured by the measuring point M3 of the embodiment proposed by the present invention.
  • Fig. 5 is the measurement point M1 simulation and actual measurement group hole blasting vibration waveform of the embodiment proposed by the present invention.
  • Fig. 6 is the measurement point M2 simulation and actual measurement group hole blasting vibration waveform of the embodiment proposed by the present invention.
  • Fig. 7 is the differential time of the embodiment proposed by the present invention and the maximum blasting vibration velocity relationship curve of the particle;
  • Fig. 8 is the relationship curve of differential time and vibration reduction rate of the embodiment proposed by the present invention.
  • Fig. 9 is the damping law of blasting vibration velocity of S1 measuring point under different differential time of the verification example proposed by the present invention.
  • Fig. 10 is the vibration velocity peak value of each measuring point under different differential time of the verification example proposed by the present invention.
  • FIG. 11 is the main frequency of each measuring point under different differential time of the verification example proposed by the present invention.
  • the single-hole blasting hole (reference blasting hole) is selected as the final blasting hole for group blasting, and the delay time interval between single-hole blasting and the penultimate blasting hole for group blasting is set to 500ms, and the positions of blasting holes and measuring points are as follows: Figure 1.
  • Figure 2-4 is the single-hole blasting vibration data record of the three measuring points M1, M2 and M3.
  • Table 1 shows the single-hole blasting parameters and the measured single-hole blasting true poison velocity peak value.
  • the single-hole vibration waveform with the largest vibration velocity among the three channels is retrieved, and the prediction program of the present application is used to carry out 10 superimposed groups at a differential time of 22ms.
  • the hole blasting vibration waveform was numerically simulated, and compared with the measured group hole blasting vibration data after blasting.
  • the waveform of measuring point 3 is distorted, and the simulated and measured vibration waveforms of group hole blasting at measuring points 1 and 2 are shown in Figure 5-6.
  • the predicted blasting vibration waveform at two different positions is basically the same as the actual blasting vibration waveform (by measuring the vibration data of group hole blasting to determine the actual blasting vibration waveform).
  • the occurrence times of enhancement and weakening are also close, and the blasting vibration waveform predicted in this study basically reflects the variation trend of blasting vibration at each measuring point. From Table 2, it can be found that the measured vibration velocity peak value v a of the two vibration measuring points is close to the predicted vibration velocity peak value v p , and the error rate does not exceed 16%, which is much lower than the regression prediction analysis method using the Sadowsky formula.
  • the method of blasting vibration velocity peak prediction is effective and reliable.
  • the intensity of blasting vibration is mainly reflected by the maximum blasting vibration velocity when the main vibration frequency is similar, so the relationship curve between different differential time and the maximum blasting vibration velocity of the particle can be fitted.
  • vibration reduction rate is used to describe the degree to which the maximum vibration velocity is weakened after n times of single-hole blasting vibration signals are superimposed.
  • the ratio of the difference to the burst vibration velocity is used to measure the vibration reduction rate, that is,
  • v 0 is the maximum blasting vibration velocity of the homogeneous blasting particle
  • v i is the maximum blasting vibration velocity of the particle under the n segments with different differential times.
  • the variation law of the superimposed group hole blasting vibration signal with the differential time is as follows.
  • the peak value of the superimposed signal decreases rapidly with the generation of the differential time, and the drop rate reaches the maximum at 18ms, reaching 92.5%.
  • the vibration reduction rate of group hole blasting vibration signal in the interval of 16ms-20ms is particularly obvious, reaching more than 91.5%.
  • the differential time is more than 60ms, the vibration reduction rate of the group-hole blasting vibration signal is close to a straight line, and the peak value of the blasting vibration is close to the peak value of the single-hole blasting vibration signal, indicating that the mutual interference and superposition of the main vibration of each single-hole vibration signal has been eliminated.
  • the group-hole vibration signal at this time is the result of the independent action of the single-hole blasting vibration signal.
  • the blasting parameters of the group hole and the single hole are the same.
  • the blasting hole diameter is 120mm
  • the hole depth is 10.0m
  • the hole mesh parameter is 5m ⁇ 4m
  • the single hole charge is 49kg
  • a total of 10 holes the total blasting charge is 490kg
  • there is no spaced coupling charge. install 1 digital electronic detonator per hole.
  • Digital electronic detonators are used in the 4 groups of experimental rows to form a differential detonation network with differential times of 18ms, 22ms, 27ms and 50ms.
  • three monitoring points are arranged from the near and far radial directions, which are recorded as S1, S2 and S3, the measured peak value of blasting vibration velocity of group holes is shown in Table 3, and the attenuation law of blasting vibration velocity of S1 measuring point in the four monitoring is shown in Figure 9.
  • the main vibration frequency of blasting vibration of each measuring point is basically kept within 9-20HZ, and the influence of differential time on the main vibration frequency is not obvious.
  • the peak value of the minimum blasting vibration velocity measured at the S1 measuring point is 0.701cm/s
  • the minimum blasting vibration velocity peak value measured at the S1 measuring point is 0.477cm /s
  • the minimum blasting vibration velocity peak measured at the S1 measuring point is 0.305cm/s
  • the peak value of blasting vibration velocity decreases continuously with the increase of blasting center distance; the main frequency of blasting vibration basically lasts in the same interval, and only a few measuring points change the main frequency.
  • the peak value of blasting vibration velocity decreases to different degrees, and the main vibration frequency of blasting vibration does not change significantly; It can be reduced by 69.7%; in the middle and far areas of the blasting area, the vibration reduction effect is general with the change of the differential time, and the optimal differential time for the vibration reduction effect is 18ms.
  • the vibration reduction effect is not obvious, the main vibration frequency of blasting vibration is significantly increased, which It has a certain protective effect on structures (the own frequency is generally lower than 10Hz).

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  • General Engineering & Computer Science (AREA)
  • Geophysics And Detection Of Objects (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Abstract

A vibration reduction method based on a blast vibration prediction technology, comprising the following steps: S1: selecting a blast hole as a reference blasting hole in multiple holes of a blasting area; S2: selecting a plurality of measuring points on the periphery of the reference blasting hole, and arranging a vibration measuring instrument in the radial direction of the reference blasting hole and the measuring points; S3: collecting vibration data of the reference blasting hole and other blast holes, and recording blasting parameters; S4: analyzing the collected vibration data of the reference blasting hole by using Matlab software, inputting millisecond times of multi-hole blasting in n segments, and predicting a complete blasting vibration waveform of the measuring points and the maximum multi-hole blasting vibration speed; S5: using Matlab software to fit a relationship curve between different millisecond times and a particle maximum blasting vibration speed and a relationship curve between different millisecond times and a vibration reduction rate. According to the method, the change rule of a multi-hole blasting vibration waveform predicted by a single-hole blasting vibration waveform is basically consistent with that of an actually measured blasting vibration waveform, and compared with a conventional formula plus experience prediction method, the method is more effective and reliable.

Description

基于爆破振动预测技术的降振方法Vibration reduction method based on blasting vibration prediction technology 技术领域technical field
本发明涉及爆破振动安全技术领域,尤其涉及基于爆破振动预测技术的降振方法。The invention relates to the technical field of blasting vibration safety, in particular to a vibration reduction method based on blasting vibration prediction technology.
背景技术Background technique
深孔台阶爆破规模较大,影响范围较广,在设计阶段对爆破振动强度进行有效的预测是十分必要的。对振动强度进行描述,可以用加速度、速度或位移等物理量。大量的研究试验表明,速度指标可以较好地反映建筑物与爆破震动破坏程度的关系,受传播介质覆盖层厚度的影响很小。Deep hole step blasting is large in scale and has a wide range of influence. It is very necessary to effectively predict the blasting vibration intensity in the design stage. To describe the vibration intensity, physical quantities such as acceleration, velocity or displacement can be used. A large number of research experiments show that the velocity index can better reflect the relationship between the building and the degree of damage caused by blasting vibration, and is little affected by the thickness of the cover layer of the transmission medium.
公式经验法预测爆破振动速度峰值基于大量的工程实践,总结得出若干对爆破振动强度影响较大的因素,通过量纲分析,再根据现场不同的爆破条件对振动强度计算公式进行不断修正。截止目前,各个国家和地区的爆破工作者根据各自试验条件,得出不同的经验计算公式,总体来说,均可以概括成如下数学表达式:The formula empirical method for predicting the peak value of blasting vibration velocity is based on a large number of engineering practices. Several factors that have a greater impact on blasting vibration intensity are summarized. Through dimensional analysis, the calculation formula of vibration intensity is continuously revised according to different blasting conditions on site. Up to now, blasting workers in various countries and regions have obtained different empirical calculation formulas according to their own test conditions. Generally speaking, they can be summarized into the following mathematical expressions:
Figure PCTCN2020113937-appb-000001
Figure PCTCN2020113937-appb-000001
式中:A-振动强度(位移、速度、加速度等);Q-一次起爆药量或单段最大起爆药量(kg);β-药量指数;R-爆源到测点距离(m);K、α-与地质条件有关的系数,一定程度反映了地震波的衰减程度。In the formula: A-vibration intensity (displacement, velocity, acceleration, etc.); Q-one-time priming charge or single-stage maximum priming charge (kg); β-charge index; R-distance from detonation source to measuring point (m) ; K, α - coefficients related to geological conditions, reflecting the attenuation degree of seismic waves to a certain extent.
中国采用的萨道夫斯基公式:The Sadowski formula used in China:
Figure PCTCN2020113937-appb-000002
Figure PCTCN2020113937-appb-000002
美国矿业局的经验公式:The empirical formula of the US Bureau of Mines:
Figure PCTCN2020113937-appb-000003
Figure PCTCN2020113937-appb-000003
日本的经验公式:Japanese empirical formula:
Figure PCTCN2020113937-appb-000004
Figure PCTCN2020113937-appb-000004
关于爆破振动的安全判据,中国国家《爆破安全规程》(GB 6722-2014)规定对地面建筑物采用振速和频率作为综合判别标准,以振速为主,频率作为修正 参考的依据,仍沿用前苏联M.A萨道夫斯基公式。萨道夫斯基公式的推导是在集中药包酮室爆破的基础上,通过量纲分析得到的,具有明确的物理意义和使用条件。若将其应用到深孔台阶爆破中,势必会出现诸多问题。然而,爆破工作者在大量的工程实践中发现,萨道夫斯基公式对于中远区爆破振动的预测,仍然能够满足工程要求。Regarding the safety criteria of blasting vibration, China's National "Blasting Safety Regulations" (GB 6722-2014) stipulates that the vibration speed and frequency are used as the comprehensive judgment criteria for ground buildings. Follow the former Soviet MA Sadowski formula. The derivation of Sadowski's formula is obtained by dimensional analysis on the basis of the blasting of the ketone chamber in the concentrated charge, and has clear physical meaning and usage conditions. If it is applied to deep hole step blasting, many problems are bound to occur. However, blasting workers have found in a large number of engineering practices that the Sadowski formula can still meet the engineering requirements for the prediction of blasting vibration in the middle and far-reaching areas.
原因是当爆心距相对于爆区分布范围来说足够大时,可将远距离群孔药包近似看成集中药包,满足萨道夫斯基公式的基本假设。但在爆破近区,测点振动峰值的预测误差可以达到200%-300%,结果差强人意。这对于临近结构及建筑物的爆破施工中,预先了解和评估爆破震动的影响程度,显然是不利的。The reason is that when the blast center distance is large enough relative to the distribution range of the blast area, the long-distance group-hole charge can be approximately regarded as a concentrated charge, which satisfies the basic assumption of Sadowski's formula. However, in the blasting near area, the prediction error of the vibration peak value of the measuring point can reach 200%-300%, and the result is not satisfactory. This is obviously unfavorable for knowing and evaluating the impact degree of blasting vibration in advance in blasting construction of adjacent structures and buildings.
发明内容SUMMARY OF THE INVENTION
基于背景技术存在的技术问题,本发明提出了基于爆破振动预测技术的降振方法,通过单孔爆破振动波形预测的群孔爆破振动波形,与实测爆破振动波形的变化规律基本一致,相比传统的公式加经验的预测方法更有效可靠。Based on the technical problems existing in the background technology, the present invention proposes a vibration reduction method based on blasting vibration prediction technology. The vibration waveform of group-hole blasting predicted by the vibration waveform of single-hole blasting is basically consistent with the variation law of the measured blasting vibration waveform. Compared with the traditional blasting vibration waveform The formula plus empirical prediction method is more effective and reliable.
本发明提出的基于爆破振动预测技术的降振方法,方法步骤如下:The vibration reduction method based on blasting vibration prediction technology proposed by the present invention, the method steps are as follows:
S1:在爆破区域的群孔中选择一炮孔作为基准爆破孔;S1: Select a blast hole as the reference blast hole in the group of holes in the blasting area;
S2:在基准爆破孔外围选取若干测点,并在基准爆破孔和测点的径向方向上布置测振仪;S2: Select several measuring points on the periphery of the reference blasting hole, and arrange the vibrometer in the radial direction of the reference blasting hole and the measuring points;
S3:采集基准爆破孔的振动数据,并记录爆破参数;S3: Collect the vibration data of the reference blasting hole, and record the blasting parameters;
S4:利用Matlab软件对采集到的基准爆破孔的振动数据进行分析,输入n分段下群孔爆破的微差时间,预测出测点完整的爆破振动波形及质点最大爆破振动速度;具体为:利用Matlab软件的xlsread函数读取文档指定路径下的单孔爆破振动信号,选取已测单孔爆破振动信号三个通道(垂直、径向、切向)中最大爆破振动速度,设置叠加分段次数n(群孔爆破孔数)和微差时间Δt,并通过叠加次数确定群孔波形总时长,在for循环下实现该通道波形在设定微差时间下叠加的n分段群孔爆破波形,同时预测质点最大爆破振动速度。S4: Use the Matlab software to analyze the collected vibration data of the reference blasting hole, input the differential time of the group hole blasting under the n segment, and predict the complete blasting vibration waveform of the measuring point and the maximum blasting vibration velocity of the particle; the details are: Use the xlsread function of Matlab software to read the single-hole blasting vibration signal in the specified path of the document, select the maximum blasting vibration velocity in the three channels (vertical, radial, tangential) of the measured single-hole blasting vibration signal, and set the number of overlapping segments n (the number of blasting holes in the group hole) and the differential time Δt, and the total duration of the group hole waveform is determined by the number of superpositions. Under the for loop, the n-segment group hole blasting waveform superimposed by the channel waveform under the set differential time is realized. At the same time, the maximum blasting vibration velocity of the particle is predicted.
S5:利用Matlab软件,拟合不同微差时间与质点最大爆破振动速度关系曲线和不同微差时间与降振率关系曲线。具体为:在S4预测程序的基础上,确定测振仪器采样频率,设定微差时间范围(1-100ms),对单孔爆破振动信号在不同微差时间下进行n次叠加循环,每一个循环,确定一个最大爆破振动速度,从而 得到微差时间下与质点最大爆破振动速度关系曲线。S5: Use Matlab software to fit the relationship curve between different differential time and the maximum blasting vibration velocity of the particle, and the relationship between different differential time and vibration reduction rate. Specifically: on the basis of the S4 prediction program, determine the sampling frequency of the vibration measuring instrument, set the differential time range (1-100ms), and perform n superimposition cycles on the single-hole blasting vibration signal at different differential times. Cycle to determine a maximum blasting vibration velocity, thereby obtaining the relationship curve between the maximum blasting vibration velocity and the particle under the differential time.
优选地,所述基准爆破孔为群孔中的末位爆破孔,且该末位爆破孔与相邻的爆破孔爆破的延期时间间隔不小于500ms。Preferably, the reference blasting hole is the last blasting hole in the group of holes, and the delay time interval between the blasting of the last blasting hole and the adjacent blasting hole is not less than 500ms.
优选地,所述测振仪不少于3台,且所述测振仪布置于基岩或利用测振振子楔入地面。Preferably, there are no less than three vibrometers, and the vibrometers are arranged on the bedrock or wedged into the ground with vibrometers.
优选地,所述爆破参数包括炮孔位置、测点距离、孔深、传播介质、单孔药量、孔排距和爆破网络。Preferably, the blasting parameters include the position of the blasting hole, the distance between the measuring points, the depth of the hole, the propagation medium, the charge per hole, the distance between the holes and the blasting network.
优选地,所述S4中完整的爆破振动波形的表达式为:Preferably, the expression of the complete blasting vibration waveform in the S4 is:
Figure PCTCN2020113937-appb-000005
Figure PCTCN2020113937-appb-000005
式中:S(T)为测点总的爆破振动速度,T为爆破振动全过程中某一时刻;K i为第i个分段的药量系数,当每个分段装药量、炸药品种等爆破参数相同,且爆源至测点的地形、地质条件相差不大时,取1;S(t-t i)为第i个分段炸药爆炸后产生的质点振动速度;t i为第i个分段炸药爆炸后地震波由震源传到测点的时间;n为分段数量;δ(t)为单位阶跃信号表达式为: In the formula: S(T) is the total blasting vibration velocity of the measuring point, T is a certain moment in the whole process of blasting vibration; K i is the charge coefficient of the ith segment, when the charge amount of each segment, explosive When the blasting parameters such as the type are the same, and the topographic and geological conditions from the blast source to the measuring point are not much different, take 1; S(t i ) is the vibration velocity of the particle generated after the explosion of the ith subsection explosive; t i is the ith The time for the seismic wave to travel from the source to the measuring point after the explosion of a segmented explosive; n is the number of segments; δ(t) is the unit step signal. The expression is:
Figure PCTCN2020113937-appb-000006
Figure PCTCN2020113937-appb-000006
与现有技术相比,本发明的有益技术效果:Compared with the prior art, the beneficial technical effects of the present invention:
(1)本发明利用Matlab程序数值模拟,通过单孔爆破振动波形预测的群孔爆破振动波形,与实测爆破振动波形的变化规律基本一致,群孔爆破振动峰值速度误差率在16%以内,相比传统的公式加经验的预测方法更加有效可靠。(1) The present invention uses Matlab program numerical simulation, and the group hole blasting vibration waveform predicted by the single hole blasting vibration waveform is basically consistent with the variation law of the measured blasting vibration waveform, and the group hole blasting vibration peak velocity error rate is within 16%. It is more effective and reliable than the traditional formula plus empirical prediction method.
(2)降低爆破爆破振动效应的微差时间并非在半个主振波形周期,在0-100ms周期内,爆破振动强度在16ms-20ms区间内的降振率尤其明显,达到60ms以上时,群孔振动信号是以单孔爆破振动信号独立作用。(2) The micro-difference time to reduce the blasting vibration effect of blasting is not in half the main vibration waveform period. In the period of 0-100ms, the vibration reduction rate of blasting vibration intensity in the interval of 16ms-20ms is particularly obvious. When it reaches more than 60ms, the group The hole vibration signal acts independently of the single hole blasting vibration signal.
(3)应用高精度数码电子雷管改变微差时间可以实现各炮孔爆破振动信号的干扰叠加,在爆破区域近区,微差时间对降振有明显作用,最大可降低69.7%;在爆破区域中远区,微差时间降振效果一般,在爆破施工前利用本发明预测程序最优降振效果微差时间,在不同距离都可以有效地控制爆破振动强度。(3) The application of high-precision digital electronic detonators to change the differential time can realize the interference and superposition of the blasting vibration signals of each blasting area. In the mid-to-far area, the vibration reduction effect of the differential time is general. Before the blasting construction, the invention predicts the optimal vibration reduction effect of the program by the micro-difference time, and the blasting vibration intensity can be effectively controlled at different distances.
(4)本发明微差时间对露天矿山爆破振动效应的影响,采用控制爆破的方式来降低地震波的危害效应,工程可行性更强,便于在实际工程中推广。(4) The influence of the differential time on the blasting vibration effect of the open-pit mine of the present invention adopts the method of controlled blasting to reduce the harmful effect of the seismic wave, and the engineering feasibility is stronger, which is convenient for promotion in practical engineering.
附图说明Description of drawings
图1为本发明提出的实施例的炮孔和测点布置图;Fig. 1 is the blast hole and measuring point arrangement diagram of the embodiment proposed by the present invention;
图2为本发明提出的实施例的测点M1测定的基准爆破孔爆破振动波形;Fig. 2 is the reference blasting hole blasting vibration waveform measured by the measuring point M1 of the embodiment proposed by the present invention;
图3为本发明提出的实施例的测点M2测定的基准爆破孔爆破振动波形;Fig. 3 is the reference blasting hole blasting vibration waveform measured by the measuring point M2 of the embodiment proposed by the present invention;
图4为本发明提出的实施例的测点M3测定的基准爆破孔爆破振动波形;Fig. 4 is the reference blasting hole blasting vibration waveform measured by the measuring point M3 of the embodiment proposed by the present invention;
图5为本发明提出的实施例的测点M1模拟与实测群孔爆破振动波形;Fig. 5 is the measurement point M1 simulation and actual measurement group hole blasting vibration waveform of the embodiment proposed by the present invention;
图6为本发明提出的实施例的测点M2模拟与实测群孔爆破振动波形;Fig. 6 is the measurement point M2 simulation and actual measurement group hole blasting vibration waveform of the embodiment proposed by the present invention;
图7为本发明提出的实施例的微差时间与质点最大爆破振动速度关系曲线;Fig. 7 is the differential time of the embodiment proposed by the present invention and the maximum blasting vibration velocity relationship curve of the particle;
图8为本发明提出的实施例的微差时间与降振率关系曲线;Fig. 8 is the relationship curve of differential time and vibration reduction rate of the embodiment proposed by the present invention;
图9为本发明提出的验证例的不同微差时间下S1测点爆破振动速度衰减规律;Fig. 9 is the damping law of blasting vibration velocity of S1 measuring point under different differential time of the verification example proposed by the present invention;
图10为本发明提出的验证例的不同微差时间下各测点振速峰值;Fig. 10 is the vibration velocity peak value of each measuring point under different differential time of the verification example proposed by the present invention;
图11为本发明提出的验证例的不同微差时间下各测点主频。FIG. 11 is the main frequency of each measuring point under different differential time of the verification example proposed by the present invention.
具体实施方式detailed description
下面结合具体实施例对本发明作进一步解说。The present invention will be further explained below in conjunction with specific embodiments.
实施例Example
按照试验实施步骤,单孔爆破孔(基准爆破孔)选取群孔爆破的末炮孔,单孔爆破孔与群孔爆破倒数第二炮孔延期时间间隔设置为500ms,炮孔和测点位置如图1所示。According to the test implementation steps, the single-hole blasting hole (reference blasting hole) is selected as the final blasting hole for group blasting, and the delay time interval between single-hole blasting and the penultimate blasting hole for group blasting is set to 500ms, and the positions of blasting holes and measuring points are as follows: Figure 1.
图2-4是M1、M2和M3三个测点的单孔爆破振动数据记录,表1为单孔爆破参数及实测单孔爆破真毒速度峰值。Figure 2-4 is the single-hole blasting vibration data record of the three measuring points M1, M2 and M3. Table 1 shows the single-hole blasting parameters and the measured single-hole blasting true poison velocity peak value.
表1单孔爆破参数及峰值振速Table 1 Single-hole blasting parameters and peak vibration velocity
Figure PCTCN2020113937-appb-000007
Figure PCTCN2020113937-appb-000007
在进行群组炮孔爆破前,根据已有的爆破设计参数,调取三个通道中振速最大的单孔振动波形,采用本申请的预测程序在22ms微差时间下进行10次叠加的群孔爆破振动波形数值模拟,并在爆破后与实测群孔爆破振动数据进行比对。测点3波形失真,测点1、2的模拟与实测群孔爆破振动波形如图5-6所示。Before carrying out group blasting, according to the existing blasting design parameters, the single-hole vibration waveform with the largest vibration velocity among the three channels is retrieved, and the prediction program of the present application is used to carry out 10 superimposed groups at a differential time of 22ms. The hole blasting vibration waveform was numerically simulated, and compared with the measured group hole blasting vibration data after blasting. The waveform of measuring point 3 is distorted, and the simulated and measured vibration waveforms of group hole blasting at measuring points 1 and 2 are shown in Figure 5-6.
从图5-6可以看出,在2个不同位置预测的爆破振动波形,与实测爆破振动波形(通过对群孔爆破的振动数据进行测定,确定实际爆破振动波形)的变化规律基本一致,振动增强和减弱的发生时间也接近,本研究预测得到的爆破振动波形基本反映了爆破振动在各测点的波形振动变化趋势。通过表2可以发现,2个测振点实测振动速度峰值v a与预测振动速度峰值v p接近,其误差率不超过16%,远低于采用萨道夫斯基公式回归预测分析方法,可以说明爆破振动速度峰值预测的方法是有效可靠的。 It can be seen from Figure 5-6 that the predicted blasting vibration waveform at two different positions is basically the same as the actual blasting vibration waveform (by measuring the vibration data of group hole blasting to determine the actual blasting vibration waveform). The occurrence times of enhancement and weakening are also close, and the blasting vibration waveform predicted in this study basically reflects the variation trend of blasting vibration at each measuring point. From Table 2, it can be found that the measured vibration velocity peak value v a of the two vibration measuring points is close to the predicted vibration velocity peak value v p , and the error rate does not exceed 16%, which is much lower than the regression prediction analysis method using the Sadowsky formula. The method of blasting vibration velocity peak prediction is effective and reliable.
表2模拟与实测群孔爆破振动数据对比Table 2 Comparison of simulated and measured group blasting vibration data
测点Measuring point L/mL/m v a v a v p v p |Δv||Δv| 误差率/%Error rate/%
M1M1 6565 1.2461.246 1.05361.0536 0.19240.1924 15.415.4
M2M2 9595 0.7470.747 0.65650.6565 0.09050.0905 12.112.1
M3M3 125125 -- -- -- --
爆破振动的强度在主振频率相似情况下,主要由最大爆破振动速度来体现,故可以拟合不同微差时间与质点最大爆破振动速度关系曲线。The intensity of blasting vibration is mainly reflected by the maximum blasting vibration velocity when the main vibration frequency is similar, so the relationship curve between different differential time and the maximum blasting vibration velocity of the particle can be fitted.
利用“降振率”来描述单孔爆破振动信号n次叠加后最大振动速度减弱的程度,计算利用齐爆(微差时间为0ms)与不同微差时间叠加后的最大振动速度之差,利用差值与齐爆振动速度比值衡量降振率,即The "vibration reduction rate" is used to describe the degree to which the maximum vibration velocity is weakened after n times of single-hole blasting vibration signals are superimposed. The ratio of the difference to the burst vibration velocity is used to measure the vibration reduction rate, that is,
Figure PCTCN2020113937-appb-000008
Figure PCTCN2020113937-appb-000008
式中:v 0为齐爆质点最大爆破振速度动;v i为不同微差时间在n分段下的质点最大爆破振动速度。编制式(3)计算程序即可得到降振率随微差时间的变化曲线。 In the formula: v 0 is the maximum blasting vibration velocity of the homogeneous blasting particle; v i is the maximum blasting vibration velocity of the particle under the n segments with different differential times. By compiling the calculation program of formula (3), the variation curve of the vibration reduction rate with the differential time can be obtained.
如图7所示,在整个微差时间段0-100ms内,群孔爆破爆破叠加信号峰值随微差时间的存在不同程度的增强和减弱,在18ms处为最大降振率,相比齐爆降振率达到92.5%,这并不符合“Δt=T/2”(25ms)时半个主振波形周期相减的干 扰降震理论,这是由于爆破振动信号为一种典型的非平稳随机信号,具有短时、突变快的特征。As shown in Figure 7, in the entire differential time period of 0-100ms, the peak value of the superimposed signal of group hole blasting increases and decreases to varying degrees with the existence of the differential time, and the maximum vibration reduction rate is at 18ms. The vibration reduction rate reaches 92.5%, which is not in line with the interference vibration reduction theory that half of the main vibration waveform period is subtracted when "Δt=T/2" (25ms). This is because the blasting vibration signal is a typical non-stationary random The signal has the characteristics of short duration and rapid mutation.
如图8所示,叠加群孔爆破振动信号的随微差时间的变化规律如下,叠加信号峰值随着微差时间的产生迅速降低,且在18ms时差点上降幅率达到最大,达到了92.5%以上,群孔爆破振动信号在16ms-20ms区间内的降振率尤其明显,达到了91.5%以上。当微差时间在60ms以上时,群孔爆破振动信号降振率接近为一条直线,其爆破振动峰值接近单孔爆破振动信号峰值,说明各个单孔振动信号的主振相互干扰叠加作用已消除,此时的群孔振动信号是由单孔爆破振动信号独立作用的结果。As shown in Figure 8, the variation law of the superimposed group hole blasting vibration signal with the differential time is as follows. The peak value of the superimposed signal decreases rapidly with the generation of the differential time, and the drop rate reaches the maximum at 18ms, reaching 92.5%. Above, the vibration reduction rate of group hole blasting vibration signal in the interval of 16ms-20ms is particularly obvious, reaching more than 91.5%. When the differential time is more than 60ms, the vibration reduction rate of the group-hole blasting vibration signal is close to a straight line, and the peak value of the blasting vibration is close to the peak value of the single-hole blasting vibration signal, indicating that the mutual interference and superposition of the main vibration of each single-hole vibration signal has been eliminated. The group-hole vibration signal at this time is the result of the independent action of the single-hole blasting vibration signal.
验证例Verification example
在杭州某石灰岩采场进行4组群孔爆破试验,现场实验仪器有四川拓普的NUBOX-8016、GPS测量仪,通过爆破试验的实测不同微差时间下爆破振动速度峰值,验证预测的爆破振动微差时间准确性。群孔与单孔爆破参数保持一致,爆破炮孔直径120mm,孔深10.0m,孔网参数为5m×4m,单孔药量49kg,共10孔,爆破总药量490kg,无间隔耦合装药,每孔安装1发数码电子雷管。4组实验排间选用数码电子雷管,组成微差时间为18ms、22ms、27ms和50ms的微差起爆网路,在每次测振区域由近及远径向布置3个监测点,分别记为S1、S2和S3,实测群孔爆破振动速度峰值见表3,4次监测中S1测点爆破振动速度衰减规律和如图9所示。Four groups of hole blasting tests were carried out in a limestone stope in Hangzhou. The on-site experimental instruments were NUBOX-8016 and GPS measuring instrument from Sichuan Tuopu. Through the actual measurement of blasting vibration velocity peaks at different differential times in blasting tests, the predicted blasting vibration was verified. Differential time accuracy. The blasting parameters of the group hole and the single hole are the same. The blasting hole diameter is 120mm, the hole depth is 10.0m, the hole mesh parameter is 5m×4m, the single hole charge is 49kg, a total of 10 holes, the total blasting charge is 490kg, and there is no spaced coupling charge. , install 1 digital electronic detonator per hole. Digital electronic detonators are used in the 4 groups of experimental rows to form a differential detonation network with differential times of 18ms, 22ms, 27ms and 50ms. In each vibration measurement area, three monitoring points are arranged from the near and far radial directions, which are recorded as S1, S2 and S3, the measured peak value of blasting vibration velocity of group holes is shown in Table 3, and the attenuation law of blasting vibration velocity of S1 measuring point in the four monitoring is shown in Figure 9.
表3不同微差时间下各测点爆破振动速度数据Table 3 Blasting vibration velocity data of each measuring point under different differential time
Figure PCTCN2020113937-appb-000009
Figure PCTCN2020113937-appb-000009
Figure PCTCN2020113937-appb-000010
Figure PCTCN2020113937-appb-000010
通过对4组微差试爆区12个测点测得的振动速度峰值分析发现:各测点爆破振动的主振频率基本保持在9-20HZ内,微差时间对主振频率的影响不明显。在65m处,微差时间选取18ms时,S1测点测得最小爆破振动速度峰值为0.701cm/s;在95m处,微差时间选取18ms时,S1测点测得最小爆破振动速度峰值0.477cm/s;在125m处,微差时间选取18ms时,S1测点测得最小爆破振动速度峰0.305cm/s;Through the analysis of the peak vibration velocity measured at 12 measuring points in 4 groups of differential test blasting areas, it is found that the main vibration frequency of blasting vibration of each measuring point is basically kept within 9-20HZ, and the influence of differential time on the main vibration frequency is not obvious. . At 65m, when the differential time is selected as 18ms, the peak value of the minimum blasting vibration velocity measured at the S1 measuring point is 0.701cm/s; at 95m, when the differential time is selected as 18ms, the minimum blasting vibration velocity peak value measured at the S1 measuring point is 0.477cm /s; at 125m, when the differential time is 18ms, the minimum blasting vibration velocity peak measured at the S1 measuring point is 0.305cm/s;
试验结果显示,选取18ms的进行微差逐孔爆破时,各测点爆破振动速度峰值低于其他三种情况,可证实通过本研究进行的单孔爆破振动叠加预测方法与实际相符。The test results show that when 18ms is selected for differential hole-by-hole blasting, the peak value of blasting vibration velocity at each measuring point is lower than the other three cases, which confirms that the single-hole blasting vibration superposition prediction method carried out in this study is consistent with reality.
由图10-11可知,爆破地震波传播过程中,随着爆心距的增加爆破振动速度峰值不断衰减;爆破振动主频基本持续在一个区间,只有少数测点主频发生突变。同一测点随着微差时间的改变,爆破振动速度峰值在出现不同程度降低,爆破振动的主振频率变化不明显;在爆破区域近区,随微差时间的改变有明显降振效果,最大可降低69.7%;在爆破区域中远区,随微差时间的改变降振效果一般,对于降振效果最优微差时间18ms,虽然降振效果不明显,但爆破振动主振频率明显提高,这对于构筑物(自有频率一般低于10Hz)起到了一定的保护作用。It can be seen from Fig. 10-11 that in the process of blasting seismic wave propagation, the peak value of blasting vibration velocity decreases continuously with the increase of blasting center distance; the main frequency of blasting vibration basically lasts in the same interval, and only a few measuring points change the main frequency. With the change of the differential time at the same measuring point, the peak value of blasting vibration velocity decreases to different degrees, and the main vibration frequency of blasting vibration does not change significantly; It can be reduced by 69.7%; in the middle and far areas of the blasting area, the vibration reduction effect is general with the change of the differential time, and the optimal differential time for the vibration reduction effect is 18ms. Although the vibration reduction effect is not obvious, the main vibration frequency of blasting vibration is significantly increased, which It has a certain protective effect on structures (the own frequency is generally lower than 10Hz).
以上所述,仅为本发明较佳的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明揭露的技术范围内,根据本发明的技术方案及其发明构思加以等同替换或改变,都应涵盖在本发明的保护范围之内。The above description is only a preferred embodiment of the present invention, but the protection scope of the present invention is not limited to this. The equivalent replacement or change of the inventive concept thereof shall be included within the protection scope of the present invention.

Claims (5)

  1. 基于爆破振动预测技术的降振方法,其特征在于,方法步骤如下:The vibration reduction method based on blasting vibration prediction technology is characterized in that the method steps are as follows:
    S1:在爆破区域的群孔中选择一炮孔作为基准爆破孔;S1: Select a blast hole as the reference blast hole in the group of holes in the blasting area;
    S2:在基准爆破孔外围选取若干测点,并在基准爆破孔和测点的径向方向上布置测振仪;S2: Select several measuring points on the periphery of the reference blasting hole, and arrange the vibrometer in the radial direction of the reference blasting hole and the measuring points;
    S3:采集基准爆破孔的振动数据,并记录爆破参数;S3: Collect the vibration data of the reference blasting hole, and record the blasting parameters;
    S4:利用Matlab软件对采集到的基准爆破孔的振动数据进行分析,输入n分段下群孔爆破的微差时间,预测出测点完整的爆破振动波形及群孔最大爆破振动速度;S4: Use the Matlab software to analyze the collected vibration data of the reference blasting hole, input the differential time of the group hole blasting under the n segment, and predict the complete blasting vibration waveform of the measuring point and the maximum blasting vibration speed of the group hole;
    S5:利用Matlab软件,拟合不同微差时间与质点最大爆破振动速度关系曲线和不同微差时间与降振率关系曲线。S5: Use Matlab software to fit the relationship curve between different differential time and the maximum blasting vibration velocity of the particle, and the relationship between different differential time and vibration reduction rate.
  2. 根据权利要求1所述的基于爆破振动预测技术的降振方法,其特征在于,所述基准爆破孔为群孔中的末位爆破孔,且该末位爆破孔与相邻的爆破孔爆破的延期时间间隔不小于500ms。The vibration reduction method based on blasting vibration prediction technology according to claim 1, wherein the reference blasting hole is the last blasting hole in the group of holes, and the delay time of blasting between the last blasting hole and the adjacent blasting hole The interval is not less than 500ms.
  3. 根据权利要求1所述的基于爆破振动预测技术的降振方法,其特征在于,所述测振仪不少于3台,且所述测振仪布置于基岩或利用测振振子楔入地面。The vibration reduction method based on blasting vibration prediction technology according to claim 1, characterized in that there are no less than three vibrometers, and the vibrometers are arranged on the bedrock or wedged into the ground with vibrators .
  4. 根据权利要求1所述的基于爆破振动预测技术的降振方法,其特征在于,所述爆破参数包括炮孔位置、测点距离、孔深、传播介质、单孔药量、孔排距和爆破网络。The vibration reduction method based on blasting vibration prediction technology according to claim 1, wherein the blasting parameters include blasting hole position, measuring point distance, hole depth, propagation medium, single hole charge, hole row spacing and blasting The internet.
  5. 根据权利要求1所述的基于爆破振动预测技术的降振方法,其特征在于,所述S4中完整的爆破振动波形的表达式为:The vibration reduction method based on blasting vibration prediction technology according to claim 1, is characterized in that, the expression of complete blasting vibration waveform in described S4 is:
    Figure PCTCN2020113937-appb-100001
    Figure PCTCN2020113937-appb-100001
    式中:S(T)为测点总的爆破振动速度,T为爆破振动全过程中某一时刻;K i为第i个分段的药量系数,当每个分段装药量、炸药品种等爆破参数相同,且爆源至测点的地形、地质条件相差不大时,取1;S(t-t i)为第i个分段炸药爆炸后产生的质点振动速度;t i为第i个分段炸药爆炸后地震波由震源传到测点的时间;n为分段数量;δ(t)为单位阶跃信号表达式为: In the formula: S(T) is the total blasting vibration velocity of the measuring point, T is a certain moment in the whole process of blasting vibration; K i is the charge coefficient of the ith segment, when the charge amount of each segment, explosive When the blasting parameters such as the type are the same, and the topographic and geological conditions from the blast source to the measuring point are not much different, take 1; S(t i ) is the vibration velocity of the particle generated after the explosion of the ith subsection explosive; t i is the ith The time for the seismic wave to travel from the source to the measuring point after the explosion of a segmented explosive; n is the number of segments; δ(t) is the unit step signal. The expression is:
    Figure PCTCN2020113937-appb-100002
    Figure PCTCN2020113937-appb-100002
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CN117053639B (en) * 2023-08-15 2024-01-30 广东中人集团建设有限公司 Bridge blasting parameter regulation and control method based on real-time monitoring data
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