WO1998021544A1 - Procede d'excavation par explosion - Google Patents
Procede d'excavation par explosion Download PDFInfo
- Publication number
- WO1998021544A1 WO1998021544A1 PCT/JP1997/004001 JP9704001W WO9821544A1 WO 1998021544 A1 WO1998021544 A1 WO 1998021544A1 JP 9704001 W JP9704001 W JP 9704001W WO 9821544 A1 WO9821544 A1 WO 9821544A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- blast
- blasting
- vibration
- time series
- sound
- Prior art date
Links
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F42—AMMUNITION; BLASTING
- F42D—BLASTING
- F42D1/00—Blasting methods or apparatus, e.g. loading or tamping
Definitions
- the present invention relates to a blasting method capable of reducing vibration and sound generated during blasting.
- multi-stage blasting using a step-down squib has been the most effective method used as a blasting method to reduce vibration and sound.
- the predominant frequency and the waveform of the single blast at the point where blast vibration is a problem are measured in advance, and based on this, the time interval of the multi-stage blast is determined, and the high-frequency using the Ic circuit is determined.
- a method of blasting using a second-time precision detonator is introduced in Japanese Patent Publication No. 7-122559 / Japanese Patent Laid-Open Publication No. Hei 1-285080.
- the vibration and sound waveforms generated by the blasting are greatly affected by the rock mass to be blasted.
- the predominant frequency of vibration and sound and the waveform of a single blast must be measured at each point of interest before each blast.
- the present invention performs step blasting at a specific place, and time-series data of vibration or sound generated at that time and the step of blasting.
- the explosion time series predicting the time series data of single blast vibration or sound in the blast, and based on the single blast prediction data obtained above, the step blast vibration or sound satisfying specific conditions.
- This is a blasting method characterized by calculating the step-and-explosion time series having the waveform shown in Fig. 4 and performing the next step-and-explosion using the calculated step-and-explosion time series.
- the present invention provides step blasting at a specific place, and performs time-series data of vibration or sound generated at that time and time-series data of step blasting of the blast, respectively, by performing Fourier transform, and corresponding spread spectrum.
- the spectrum corresponding to the time-series data of the single blast vibration or sound is predicted using these spectra, and the spectrum is subjected to a Fourier inverse transform to obtain the above-mentioned spectrum.
- This is a blasting method characterized by calculating the time series and carrying out the next step blasting in the calculated step blasting time series.
- the present invention also provides a step blast at a specific place, a cross-correlation function of time series data of vibration or sound generated at that time and the step blast time series data of the blast, From the autocorrelation function of the explosion time series data, it is considered that the time series data of the vibration or sound of the step blasting was formed by solving the Wiener's least squares theory using the Le V inson algorithm. The most probable single blast vibration or sound's time-series data is predicted, and the step blast vibration or sound waveform that satisfies specific conditions based on the single blast prediction data obtained above is used. This is a blasting method characterized by calculating the series and performing the next blasting in the calculated blasting time series.
- the current step blasting that is, a method using only the time series data of the vibration or sound of the latest step blasting and the time series of the step blasting of the blast
- Either a method using the vibrations of the past several times of blasting or a time series data of the sound and a method of using the time blasting and explosion of the blasting may be used.
- some examples of using only the current time series of vibration or sound of the blasting and the time series of the blasting and blasting will be described below for simplicity.
- a m and X m denotes the sampling point interval A t, the m-th data sampled at a sampling number N. Therefore, m takes the value of 0 ⁇ m ⁇ N-1.
- Is an integer obtained by dividing the i-th detonation time 1 ⁇ by m t, where L is the number of detonation, i takes the value of 0 ⁇ m ⁇ L-1.
- A is the time series data of the vibration or sound at a specific location due to the current step blast, and the timing of the step detonation of the blast, the number of the steps, and the ratio of the amplitude of each step ),
- the time series data of the vibration or sound of a single blast to be predicted is X, and the following relationship is recognized between the three time series data.
- step blast waveform A is represented by the single blast waveform X, and the convolution.
- each blast timing t t. , T ,,.
- X ⁇ f) A ( ⁇ ) ⁇ , and A) and ⁇ ) A are obtained from A)) and X)), so X) is obtained. Convert it to obtain the single-shot vibration or sound time-series data X) that you want to predict.
- Xt be the time series data of the vibration or sound of a single blast to be predicted. The following relationships are recognized in the above four time series data.
- the moving average, the use of a pass-pass filter, etc. can be used to obtain the SN of the time-series data at a specific location due to the current step blast.
- the ratio must be as good as possible.
- various methods can be considered as a method for calculating a step blast explosion time series that becomes a waveform of a step blast vibration or a sound that satisfies a specific condition based on the single blast prediction data obtained as described above.
- Tokuhei 7- A method of setting a detonation second time interval such that vibration waves interfere based on a dominant frequency, as disclosed in JP-A No. 1-258559, The method of predicting the vibration waveform of this blast based on the principle of superposition and selecting the optimal second time interval, the method using the M-sequence as disclosed in Japanese Patent Publication No. 8-144480, explosives
- an autocorrelation function and a cross-correlation function as shown in the academic journal, Vo 55, No. 4, 1994.
- the specific condition is to minimize the displacement amplitude, displacement velocity amplitude, displacement acceleration amplitude or the evaluation value of vibration level, vibration acceleration level, etc. in the case of vibration, and sound pressure amplitude or noise in the case of sound. It is to minimize the evaluation of the level.
- a specific condition may be used.
- time-series explosion time series is calculated, for example, the accuracy of the second-time accuracy known in Japanese Patent Application Laid-Open Nos. Sho 62-216900 and Hei 1 Blast in the sequence of the detonation with a good detonator.
- the vibration or sound caused by this blast is measured at a specific location, and is used again for predicting the time series data of the vibration or sound of the single blast of the next blast together with the time series of the blast. .
- the dominant frequency of the ground or the waveform of a single blast at a point where vibration or sound is a problem is measured at a specific place associated with the step blast without separately measuring before each blast. Vibration or sound can be controlled to a minimum.
- Fig. 1 shows two electric delay electric detonators with a detonation time set to 10 ms and 40 ms (detonation time interval of 30 ms) fitted with 100 g of hydrous explosives in water.
- Vertical ground vibration obtained at point A 3 shows a dynamic waveform.
- Figure 2 shows the results obtained at point A when an electric delay detonator with a detonation time set to 100 ms and 100 g of water-containing explosives was installed in water and detonated independently.
- the vertical vibration waveform of the ground is shown.
- Fig. 3-1 shows the single-shot blast vertical vibration waveform that constitutes the Fig. 1 waveform estimated from the waveform of Fig. 1 by the successive decomposition calculation method shown in the present invention
- Fig. 3-2 shows the waveform.
- the waveform of Fig. 1 was estimated by the Fourier transform method shown in the present invention, and the single-blast vertical vibration waveform composing the waveform in Fig. 1 was obtained.
- Fig. 1 shows the single-blast vertical vibration waveform composing the waveform shown in Fig. 1 estimated by the one-jon method.
- Fig. 4-1 shows the point A when two-stage blasting was performed at a detonation second time interval of 120 ms based on the principle of linear superposition using the waveform of Fig. 3-1.
- two-step blasting was performed using the waveforms shown in Fig. 4-2 and Fig. 4-2 based on the principle of linear superposition.
- the vertical vibration waveform predicted at the point A is shown in Fig. 4-13, using the waveform shown in Fig. 3-3, based on the principle of linear superposition, with two steps at a firing interval of 120 ms. This shows the vertical vibration waveform predicted at point A when blasting was performed.
- Figure 5 shows two electric delay electric detonators with a detonation time set to 10 ms and 130 ms (explosion time interval: 120 ms), with 100 g of water-containing explosives installed underwater. This is the vertical vibration waveform of the ground obtained at the point A when the detonation occurred.
- Figure 6 shows that the explosion time was set to 10 ms, 40 ms, 70 ms ⁇ 100 ms ⁇ 130 ms (explosion time interval 30 ms). Place the one with 100 g attached underwater,
- Figure 7-1 of Figure 7 shows the waveform of Figure 6 estimated from the waveform of Figure 6 by the sequential decomposition calculation method shown in the present invention.
- Fig. 7-2 shows the vertical vibration waveform of single blast, which is estimated from the waveform of Fig. 6 by the Fourier transform method shown in the present invention.
- FIG. 7-3 shows a single-blast vertical oscillating waveform constituting the waveform in FIG. 6, which is estimated from the waveform in FIG. 6 by the deconvolution method shown in the present invention.
- Fig. 8-1 shows the point A when 5-step blasting was performed at a 90 ms detonation time interval based on the principle of linear superposition using the waveforms in Fig. 7-1.
- Fig. 8-2 shows the vertical vibration waveform predicted by the above
- Fig. 7-2 shows the waveform in Fig. 7-2.
- Fig. 8-3 shows the vertical vibration waveform predicted at point A
- Fig. 7-3 shows the vertical vibration waveform at 90 ms detonation time interval based on the principle of linear superposition. This figure shows the vertical vibration waveform predicted at point A when step blasting was performed.
- Figure 9 shows the electrical delay when the detonation time was set to 10 ms, 100 ms, 190 ms, 280 ms, and 37 ms (explosion time interval 90 ms).
- the figure shows the vertical vibration waveform of the ground obtained at point A, with the explosive loaded with 100 g installed in water and detonated.
- the explosion time was set to 100 g with a water-containing explosive (trade name: Sambex) at a depth of 2 m near the center of the pond with a long side of 25 m, a short side of 25 m and a depth of 4 m.
- An electric delay detonator product name: EDD
- ground vibration normal direction X, tangential direction Y, vertical
- point A ground vibration
- FIG. 1 shows the vertical vibration waveform among the obtained waveforms.
- the ground vibration at point A was measured when an explosion time was set at 10 ms and an electric delay detonator equipped with 100 g of hydrous explosive was installed in water.
- Figure 2 shows the vertical vibration waveform among the results.
- FIGS. 3-1, 3-2, and 3-3 The waveforms obtained by the successive decomposition calculation method, the Fourier transform method, and the de-convolution method shown in the present invention are shown in FIGS. 3-1, 3-2, and 3-3.
- Fig. 3-1, Fig. 3-2, Fig. 3-3 the estimated waveforms
- various vertical vibration waveforms of the next blast are calculated. Predicting the detonation time interval, it was concluded that the maximum displacement velocity amplitude of the vertical vibration at point A was minimum at the detonation time interval of 120 ms.
- Fig. 4-1, Fig. 4-2, Fig. 4 _3 show the vertical vibration prediction results of 120 ms 2-stage blasting from the sequential decomposition calculation method, the Fourier transform method, and the de-convolution method.
- a single blast Fig. 2 and the single-shot waveforms predicted from the step blasting by the sequential decomposition calculation method, Fourier transform method, and de-convolution method of the present invention Fig. 3-1, Fig. 3_2, Fig. 3- Comparing Fig. 3, the waveforms are very similar, indicating that the successive decomposition calculation method, the Fourier transform method, and the de'convolution method are all effective single-shot waveform prediction methods. Furthermore, when the similarity between the two waveforms was evaluated using the cross-correlation coefficient, the correlation coefficients of Fig. 2 and Fig. 3-1, Fig. 3-2, and Fig. 3-3 were 0.88, 0.93, and 0, respectively. 9 6, which proves to be quantitatively similar.
- FIGS. 7-1, 7-2, and 7-3 The waveforms obtained by the successive decomposition calculation method, the Fourier transform method, and the de-convolution method shown in the present invention are shown in FIGS. 7-1, 7-2, and 7-3.
- various vertical vibration waveforms of the next blast are calculated. Predicting the detonation time interval, it was concluded that the maximum displacement velocity amplitude of the vertical vibration at point A was minimized at the detonation time interval of 90 ms.
- Figure 8-1, Figure 8-2, and Figure 8-3 show the results of vertical vibration prediction of 90 ms 5-stage blasting from the successive decomposition calculation method, Fourier transform method, and deconvolution method.
- the electric detonation time was set to 10 ms, 100 ms, 190 ms, 280 ms, and 370 ms (explosion time interval 90 ms).
- the one with 100 g of water-containing explosive was installed in water, detonated, and the ground vibration was measured at point A.
- Fig. 9 shows the vertical vibration waveform among the obtained waveforms.
- Fig. 2 obtained by a single blast and Fig. 7-1 shows a single-shot waveform predicted from the step blast by the successive decomposition calculation method, Fourier transform method, and de-convolution method of the present invention.
- Fig. 7-2 and Fig. 7_3 The data for the round blast using both methods is five rounds, but the results are very similar to those for the two rounds, and are stably obtained by the sequential decomposition calculation method and the Fourier transform. It can be seen that the deconvolution method is an effective single-shot waveform prediction method.
- the correlation coefficients between Fig.2 and Fig.7-1, Fig.7-2, and Fig.7-3 were 0.92, 0.96, 0.93.
- the blasting method of the present invention is useful for reducing vibration and sound generated during blasting.
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- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Geophysics And Detection Of Objects (AREA)
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
- Investigation Of Foundation Soil And Reinforcement Of Foundation Soil By Compacting Or Drainage (AREA)
Description
Claims
Priority Applications (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP52237398A JP3956237B2 (ja) | 1996-11-12 | 1997-11-04 | 発破工法 |
DE69728781T DE69728781T2 (de) | 1996-11-12 | 1997-11-04 | Ausschachtung durch sprengung |
AU47271/97A AU710306B2 (en) | 1996-11-12 | 1997-11-04 | Blasting method |
CA002265629A CA2265629C (en) | 1996-11-12 | 1997-11-04 | Blasting method |
US09/284,502 US6220167B1 (en) | 1996-11-12 | 1997-11-04 | Excavation method by blasting |
EP97909732A EP0939291B1 (en) | 1996-11-12 | 1997-11-04 | Excavation method by blasting |
Applications Claiming Priority (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30008696 | 1996-11-12 | ||
JP8/300086 | 1996-11-12 | ||
JP11242897 | 1997-04-30 | ||
JP9/112428 | 1997-04-30 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO1998021544A1 true WO1998021544A1 (fr) | 1998-05-22 |
Family
ID=26451589
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/JP1997/004001 WO1998021544A1 (fr) | 1996-11-12 | 1997-11-04 | Procede d'excavation par explosion |
Country Status (9)
Country | Link |
---|---|
US (1) | US6220167B1 (ja) |
EP (1) | EP0939291B1 (ja) |
JP (1) | JP3956237B2 (ja) |
KR (1) | KR100304229B1 (ja) |
CN (1) | CN1065954C (ja) |
AU (1) | AU710306B2 (ja) |
CA (1) | CA2265629C (ja) |
DE (1) | DE69728781T2 (ja) |
WO (1) | WO1998021544A1 (ja) |
Cited By (2)
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JP2015137788A (ja) * | 2014-01-21 | 2015-07-30 | 鹿島建設株式会社 | 発破工法 |
JP2016196970A (ja) * | 2015-04-03 | 2016-11-24 | 鹿島建設株式会社 | 振動予測方法 |
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EP1009967B3 (en) * | 1998-07-07 | 2009-12-16 | SMI Technology (Pty) Limited | Sequential detonation of explosive charges |
AUPR262801A0 (en) * | 2001-01-19 | 2001-02-15 | Orica Explosives Technology Pty Ltd | Method of blasting |
CA2564832C (en) * | 2004-06-22 | 2011-09-06 | Orica Explosives Technology Pty Ltd | Method of blasting |
CN100395509C (zh) * | 2004-12-08 | 2008-06-18 | 广东宏大爆破股份有限公司 | 电算精确延时干扰减震爆破方法 |
CN101988814B (zh) * | 2009-03-30 | 2013-01-09 | 中水东北勘测设计研究有限责任公司 | 控制爆破中毫秒延期时间的检验方法 |
CN102135445B (zh) * | 2010-06-30 | 2012-10-03 | 中国铁道科学研究院铁道建筑研究所 | 爆破振动预测方法 |
CN102095338A (zh) * | 2010-12-14 | 2011-06-15 | 中国建筑第八工程局有限公司 | 隧道电子雷管爆破施工方法 |
CN104297777A (zh) * | 2013-07-15 | 2015-01-21 | 中国石油化工股份有限公司 | 全自动地震勘探数字信号遥爆系统及其遥爆方法 |
CN103389015A (zh) * | 2013-08-09 | 2013-11-13 | 贵州新联爆破工程集团有限公司 | 一种爆破孔内分段毫秒微差爆破方法 |
JP6408388B2 (ja) * | 2015-01-23 | 2018-10-17 | 鹿島建設株式会社 | 発破工法 |
JP6998014B2 (ja) * | 2016-12-19 | 2022-01-18 | 西松建設株式会社 | 発破工法 |
CN107941104B (zh) * | 2017-11-03 | 2018-12-18 | 北京科技大学 | 基于多孔微差爆破振动合成计算的隧道掏槽药量设计方法 |
KR102120778B1 (ko) * | 2018-03-27 | 2020-06-09 | 한국해양과학기술원 | 수중 광역 발파 시스템 및 그 방법 |
CN112034006B (zh) * | 2020-09-09 | 2024-03-12 | 中国葛洲坝集团易普力股份有限公司 | 基于多目标控制的精确延时控制爆破延时参数设计方法 |
CN114646244A (zh) * | 2022-03-23 | 2022-06-21 | 中国五冶集团有限公司 | 降低隧道掘进爆破振动的方法 |
CN114739246B (zh) * | 2022-04-20 | 2023-08-29 | 北京大成国测科技有限公司 | 一种减小爆破振动的爆破方法及系统 |
CN114812312B (zh) * | 2022-04-29 | 2023-02-07 | 东北大学 | 一种监测岩体内部爆破振动波传播规律的装置及方法 |
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JPS62261900A (ja) | 1986-05-08 | 1987-11-14 | 旭化成株式会社 | 発破工法 |
JPH01285800A (ja) | 1988-05-11 | 1989-11-16 | Asahi Chem Ind Co Ltd | 発破工法 |
JPH07122559A (ja) | 1993-10-27 | 1995-05-12 | Fujitsu Ltd | はんだバンプ形成方法 |
JPH0814480A (ja) | 1994-06-24 | 1996-01-16 | Tabuchi:Kk | 防食スリーブ |
JPH0814480B2 (ja) * | 1989-05-17 | 1996-02-14 | 四一 安藤 | 発破方法 |
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EP0323687A1 (en) * | 1988-01-08 | 1989-07-12 | Shell Oil Company | Method of measuring, analysing, predicting and controlling vibrations induced by explosive blasting in earth formations |
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JP3147895B2 (ja) * | 1990-10-30 | 2001-03-19 | 靖二 中島 | 斉発穿孔発破における穿孔間隔長決定方法 |
US5765923A (en) * | 1992-06-05 | 1998-06-16 | Sunburst Excavation, Inc. | Cartridge for generating high-pressure gases in a drill hole |
US5359935A (en) * | 1993-01-13 | 1994-11-01 | Applied Energetic Systems, Inc. | Detonator device and method for making same |
US5388521A (en) * | 1993-10-18 | 1995-02-14 | Coursen Family Trust | Method of reducing ground vibration from delay blasting |
US5811741A (en) * | 1997-03-19 | 1998-09-22 | Coast Machinery, Inc. | Apparatus for placing geophones beneath the surface of the earth |
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1997
- 1997-11-04 EP EP97909732A patent/EP0939291B1/en not_active Expired - Lifetime
- 1997-11-04 AU AU47271/97A patent/AU710306B2/en not_active Ceased
- 1997-11-04 CN CN97199355A patent/CN1065954C/zh not_active Expired - Fee Related
- 1997-11-04 WO PCT/JP1997/004001 patent/WO1998021544A1/ja active IP Right Grant
- 1997-11-04 DE DE69728781T patent/DE69728781T2/de not_active Expired - Fee Related
- 1997-11-04 CA CA002265629A patent/CA2265629C/en not_active Expired - Fee Related
- 1997-11-04 US US09/284,502 patent/US6220167B1/en not_active Expired - Fee Related
- 1997-11-04 JP JP52237398A patent/JP3956237B2/ja not_active Expired - Fee Related
-
1999
- 1999-03-20 KR KR1019997002420A patent/KR100304229B1/ko not_active IP Right Cessation
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JPS62261900A (ja) | 1986-05-08 | 1987-11-14 | 旭化成株式会社 | 発破工法 |
JPH07122559B2 (ja) * | 1986-05-08 | 1995-12-25 | 旭化成工業株式会社 | 発破工法 |
JPH01285800A (ja) | 1988-05-11 | 1989-11-16 | Asahi Chem Ind Co Ltd | 発破工法 |
JPH0814480B2 (ja) * | 1989-05-17 | 1996-02-14 | 四一 安藤 | 発破方法 |
JPH07122559A (ja) | 1993-10-27 | 1995-05-12 | Fujitsu Ltd | はんだバンプ形成方法 |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2015137788A (ja) * | 2014-01-21 | 2015-07-30 | 鹿島建設株式会社 | 発破工法 |
JP2016196970A (ja) * | 2015-04-03 | 2016-11-24 | 鹿島建設株式会社 | 振動予測方法 |
Also Published As
Publication number | Publication date |
---|---|
AU4727197A (en) | 1998-06-03 |
CA2265629A1 (en) | 1998-05-22 |
CA2265629C (en) | 2002-07-23 |
EP0939291B1 (en) | 2004-04-21 |
CN1235669A (zh) | 1999-11-17 |
KR20000048516A (ko) | 2000-07-25 |
DE69728781D1 (de) | 2004-05-27 |
DE69728781T2 (de) | 2005-05-25 |
EP0939291A1 (en) | 1999-09-01 |
US6220167B1 (en) | 2001-04-24 |
KR100304229B1 (ko) | 2001-09-24 |
CN1065954C (zh) | 2001-05-16 |
JP3956237B2 (ja) | 2007-08-08 |
AU710306B2 (en) | 1999-09-16 |
EP0939291A4 (en) | 2001-04-18 |
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