JP3103021B2 - Discharge hydraulic pressure breakdown method - Google Patents
Discharge hydraulic pressure breakdown methodInfo
- Publication number
- JP3103021B2 JP3103021B2 JP07194413A JP19441395A JP3103021B2 JP 3103021 B2 JP3103021 B2 JP 3103021B2 JP 07194413 A JP07194413 A JP 07194413A JP 19441395 A JP19441395 A JP 19441395A JP 3103021 B2 JP3103021 B2 JP 3103021B2
- Authority
- JP
- Japan
- Prior art keywords
- fracture
- discharge
- breaking
- holes
- hydraulic pressure
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
Landscapes
- Processing Of Stones Or Stones Resemblance Materials (AREA)
- Drilling And Exploitation, And Mining Machines And Methods (AREA)
- Perforating, Stamping-Out Or Severing By Means Other Than Cutting (AREA)
Description
【0001】[0001]
【発明の属する技術分野】本発明は、自由面が1面であ
る被破壊物、たとえばトンネルや宅地造成地の岩盤、コ
ンクリート構造物、水中の岩盤やコンクリート構造物を
破壊するための放電液圧破壊工法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a discharge pressure for destroying an object to be destroyed having one free surface, for example, a rock, a concrete structure, an underwater rock or a concrete structure in a tunnel or a residential land development site. Related to the destruction method.
【0002】[0002]
【従来の技術】コンデンサに充電蓄積された電気エネル
ギーを極めて短時間で金属細線に放電供給して、これに
より金属細線自身および周囲の破壊用液体の急激な気化
による衝撃力で周囲の被破壊物を破壊する放電液圧破壊
工法は、周辺温度や装填後の経過時間などに左右され
ず、電圧を印加しないかぎり爆発しないため、極めて安
全性が高く、かつ破壊力を容易に調節できるため、老朽
化したビルなどのコンクリート構造物の破壊に利用され
ている。2. Description of the Related Art An electric energy charged and stored in a capacitor is discharged and supplied to a thin metal wire in a very short time. The liquid pressure destruction method, which destroys the air, does not depend on the ambient temperature or the elapsed time after loading, does not explode unless voltage is applied, and is extremely safe. It is used to destroy concrete structures such as converted buildings.
【0003】[0003]
【発明が解決しようとする課題】従来に放電液圧破壊工
法が採用される被破壊物は、通常回りが全て自由面であ
るコンクリート塊などであり、岩盤などのように自由面
が1面の被破壊物に適用されていなかった。The objects to be destroyed to which the electric discharge hydraulic rupture method is conventionally employed are concrete blocks or the like, all of which are usually free surfaces, and have one free surface such as rock. Not applicable to destroyables.
【0004】本発明は、自由面が1面の被破壊物をより
効果的に破壊できる放電液圧破壊工法を提供することを
目的とする。[0004] It is an object of the present invention to provide a discharge hydraulic fracturing method capable of more effectively destroying an object having one free surface.
【0005】[0005]
【課題を解決するための手段】上記目的を達成するため
に本発明の請求項1記載の発明は、コンデンサに充電蓄
積した電気エネルギーを金属細線に極めて短時間に供給
することにより、金属細線およびその周囲の液体の急激
な気化、体積膨張により発生する衝撃力を利用する放電
液圧破壊具を使用して、自由面が1面である被破壊物を
破壊するに際し、まず自由面に形成されて破壊中心とな
る先行溝の、奥部中心から外側に広がる破壊面に沿っ
て、複数箇所に傾斜破壊孔を形成し、この破壊孔内にそ
れぞれ放電液圧破壊具を装填し、コンデンサから電気エ
ネルギーを各放電液圧破壊具に短時間で同時に供給して
被破壊物を放電破壊することにより、先行溝をくり抜い
て第2の自由面を形成し、この先行溝の周囲に複数の破
壊孔を形成して、それぞれの破壊孔に装填された放電液
圧破壊具により放電破壊して先行溝を拡大し被破壊物を
放電破壊するものである。In order to achieve the above object, the invention according to claim 1 of the present invention provides an electric energy charged and stored in a capacitor to a metal wire in a very short time, so that the metal wire and When the object to be destroyed, which has one free surface, is first formed on the free surface by using a discharge hydraulic pressure destroyer utilizing an impact force generated by rapid vaporization and volume expansion of the surrounding liquid, Be the center of destruction
A plurality of inclined fracture holes are formed along the fracture surface extending outward from the center of the back of the leading groove, and a discharge hydraulic pressure breaker is loaded in each of the fracture holes, and electric energy is discharged from the capacitor to each discharge hole. By simultaneously supplying the hydraulic pressure breaking tool in a short time to discharge-break the object to be destroyed, the preceding groove is cut out to form a second free surface, and a plurality of breaking holes are formed around the preceding groove. In this method, the discharge is destroyed by the discharge hydraulic pressure destroyer loaded in each of the breaking holes, the leading groove is enlarged, and the object to be destroyed is discharged.
【0006】上記工法によれば、自由面の先行溝を、中
心から外側に広がる両破壊面に沿って先端部が互いに交
差または接近するように形成された傾斜破壊孔を形成
し、これら傾斜破壊孔に放電液圧破壊具を装填して放電
破壊し、先行溝を効果的にくり抜いて第2の自由面を形
成することができ、次いでこの第2の自由面を利用して
効果的に被破壊物を破壊することができる。[0006] According to the above method, the leading groove of the free surface is formed with oblique fracture holes formed so that the tips cross each other or approach each other along both fracture surfaces extending outward from the center. A discharge hydraulic pressure breaker is loaded in the hole to cause a discharge breakdown, and the leading groove can be effectively cut out to form a second free surface, and then the second free surface can be effectively used. Destruction can be destroyed.
【0007】[0007]
【発明の実施の形態】ここで、本発明に係る放電液圧破
壊工法の実施の形態を図1〜図10に基づいて説明す
る。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of a discharge hydraulic pressure breaking method according to the present invention will be described with reference to FIGS.
【0008】まず、放電液圧破壊設備について説明す
る。図7に示すように、被破壊物1に穿設された傾斜破
壊孔または破壊孔2に装填される放電液圧破壊具である
放電プルーブ3は、たとえば水などからなる破壊用液4
が充填された合成ゴムや防水処理紙性の破壊容器5と、
この容器5の天板5aを貫通して破壊用液4中に延び、
スペーサ6により互いに平行に保持された一対の電極棒
7と、電極棒7の先端部間に連結された金属細線8とで
構成され、被破壊物1から離れて配置された大容量のコ
ンデンサ10aを有するエネルギー供給回路10と電極
棒7とが、放電スイッチ9aを有するリード線9により
接続されている。このエネルギー供給回路10は、コン
デンサ10aに電気エネルギーを充電蓄積する直流高電
圧電源10bを備え、コンデンサ10aと直流高電圧電
源10bとが充電スイッチ10cが介在された接続線1
0dにより互いに接続されている。First, the discharge hydraulic pressure destruction equipment will be described. As shown in FIG. 7, a discharge probe 3 which is a discharge hydraulic pressure breaking tool loaded in an inclined breaking hole or a breaking hole 2 drilled in the object to be broken 1 comprises a breaking liquid 4 made of, for example, water.
A destruction container 5 made of synthetic rubber or waterproof paper filled with
It penetrates through the top plate 5a of the container 5 and extends into the breaking liquid 4,
A large-capacity capacitor 10a, which is composed of a pair of electrode rods 7 held in parallel with each other by a spacer 6 and a thin metal wire 8 connected between the tip ends of the electrode rods 7 and is disposed apart from the object 1 to be destroyed Is connected to the electrode rod 7 by a lead wire 9 having a discharge switch 9a. The energy supply circuit 10 includes a DC high-voltage power supply 10b for charging and accumulating electric energy in a capacitor 10a, and the capacitor 10a and the DC high-voltage power supply 10b are connected to a connection line 1 via a charging switch 10c.
0d are connected to each other.
【0009】このエネルギー供給回路10のコンデンサ
10aの充電電圧Vcと、放電プルーブ3の放電衝撃力
Fの関係は、図9のF−Vc特性を示すグラフのよう
に、比例関係にある。ところで、垂直に形成された破壊
孔2に装填された放電プルーブ3による破壊状態は、図
8に示すように、内部の直接破壊領域の幅Liと表面の
直接破壊領域の幅Laとは異なる。そして、放電衝撃力
Fと直接破壊領域の幅Li,Laの関係Fは図10およ
び式に示すように、充電電圧Vc(ボルト)と直接破
壊領域の幅L(cm)の比例関係として導かれる。The relationship between the charging voltage Vc of the capacitor 10a of the energy supply circuit 10 and the discharge impact force F of the discharge probe 3 is in a proportional relationship as shown in a graph showing the F-Vc characteristic in FIG. By the way, as shown in FIG. 8, the state of the breakdown caused by the discharge probe 3 loaded in the vertically formed breakdown hole 2 is different from the width Li of the internal direct breakdown region and the width La of the surface direct breakdown region. The relationship F between the discharge impact force F and the widths Li and La of the direct breakdown region is derived as a proportional relationship between the charging voltage Vc (volts) and the width L (cm) of the direct breakdown region, as shown in FIG. .
【0010】 |Vc|/120≧L≧|Vc|/1200…式 図10で、表面の直接破壊両域Laは式の|Vc|/
120に対応し、内部の直接破壊両域Liは式の|V
c|/1200に対応する。| Vc | / 120 ≧ L ≧ | Vc | / 1200... In FIG. 10, both direct destruction regions La on the surface are represented by | Vc | /
120, the internal direct destruction region Li is expressed by the equation | V
c | / 1200.
【0011】次に放電液圧破壊工法の実施の第1の形態
を図1,図2を参照して説明する。この工法により破壊
される被破壊物1は岩盤やコンクリート基礎、コンクリ
ート床などの自由面が1面F1のものである。a.ま
ず、図1に示すように、穿孔装置等を使用して、第1の
自由面F1に形成されて破壊中心となる先行溝11の中
心奥部から両外側表面に傾斜する2つの破壊面11a,
11bに沿って、平面視で開口部が千鳥状に配置された
複数本の傾斜破壊孔12A,12Bを横断面に沿って形
成するとともに、両辺の傾斜破壊孔12A,12Bの先
端部12bをそれぞれ破壊面11a,11bの交差線P
に達するように形成する。Next, a first embodiment of the discharge hydraulic pressure breaking method will be described with reference to FIGS. The object 1 to be destroyed by this method has one free surface F1 such as a bedrock, a concrete foundation, and a concrete floor. a. First, as shown in FIG. 1, using a perforation device or the like, two fracture surfaces 11 a inclined from the deep portion of the center of the preceding groove 11 formed on the first free surface F <b> 1 and serving as a fracture center to both outer surfaces. ,
A plurality of inclined breaking holes 12A, 12B whose openings are arranged in a staggered manner in plan view are formed along the cross section along 11b, and the tip portions 12b of the inclined breaking holes 12A, 12B on both sides are respectively formed. Intersecting line P between fracture surfaces 11a and 11b
Is formed to reach.
【0012】ここで同一の破壊面11a,11bに形成
され隣接する傾斜破壊孔12A,12Bの基端開口部1
2a間の距離XA1 と、先端部12b間の距離XA
2 は、放電プルーブ3による直接破壊領域13の幅L
(実際はLaとLi)とすると、 XA1 ≦2×L XA2 ≦2×L すなわちそれぞれLの2倍以下に設定される。Here, the base opening 1 of the adjacent inclined breaking holes 12A, 12B formed on the same breaking surfaces 11a, 11b.
A distance XA 1 between 2a, the distance between the tip 12b XA
2 is the width L of the direct breakdown region 13 by the discharge probe 3
(Actually La and Li), XA 1 ≦ 2 × L XA 2 ≦ 2 × L, that is, each is set to twice or less of L.
【0013】またこの直接破壊領域13aの幅Lは、
式の範囲を満足するものである。 b.この傾斜破壊孔12A,12Bにそれぞれ放電プル
ーブ3を装填し、放電スイッチ9aがオンされてコンデ
ンサ10aから高電圧が極めて短時間に全ての放電プル
ーブ3に供給され金属細線8に印加される。これによ
り、金属細線8とその回りの破壊用液4が瞬間的に気化
されてその衝撃力が周囲の被破壊物1に伝達され直接破
壊領域13が破壊される。これにより、先行溝11がく
り抜かれて第2の自由面F2が形成される。The width L of the direct destruction region 13a is
This satisfies the range of the expression. b. The discharge probes 3 are loaded into the inclined breaking holes 12A and 12B, respectively, and the discharge switch 9a is turned on. A high voltage is supplied from the capacitor 10a to all the discharge probes 3 in a very short time and applied to the thin metal wires 8. As a result, the thin metal wire 8 and the breaking liquid 4 around the thin metal wire 8 are instantaneously vaporized, and the impact force is transmitted to the surrounding object 1 to be broken, thereby directly breaking the breaking area 13. Thereby, the preceding groove 11 is hollowed out, and the second free surface F2 is formed.
【0014】なお、ここで対向する破壊面11a,11
bの間で最も近い傾斜破壊孔12A,12Bの先端部1
2bの中心間距離YB 2 を、YB 2 ≦2×L と設定することにより、図6に示すように、先行溝11
の開口面全体を完全に破壊して、自由面が1つの被破壊
物1に先行溝11を完全にくり抜き状に放電破壊するこ
とができる。Here, the opposing destruction surfaces 11a, 11
b, the tip 1 of the inclined breaking holes 12A and 12B closest to each other.
Center distance YB 2 of 2b Is set as YB 2 ≦ 2 × L, as shown in FIG.
Completely destroy the entire open surface of the fracture free surface is one
The preceding groove 11 can be completely broken in the object 1 by electric discharge.
【0015】c.先行溝11の周囲に、放電プルーブ3
の直接破壊領域に応じて破壊孔1が形成され、破壊孔に
放電プルーブ3が装填されて、順次または同時に被破壊
物が破壊されて先行溝11が拡大され、これが繰り返さ
れて被破壊物1が破壊される。C. Around the leading groove 11, a discharge probe 3
Is formed in accordance with the direct destruction area, and the discharge probe 3 is loaded in the destruction hole, and the object to be destroyed is sequentially or simultaneously destroyed, and the preceding groove 11 is enlarged. Is destroyed.
【0016】次に第2の実施の形態を図3〜図5を参照
して説明する。a.まず、図3に示すように、穿孔装置
等を使用して、第1の自由面F1に形成しようとする先
行溝21の中心奥部から両外側表面に傾斜する2つの破
壊面21a,21bに沿って、互いに対向する位置に複
数本の傾斜破壊孔22A,22Bを横断面上に形成す
る。Next, a second embodiment will be described with reference to FIGS. a. First, as shown in FIG. 3, using a perforation device or the like, two fracture surfaces inclined from the center deep portion of the preceding groove 21 to be formed on the first free surface F1 to both outer surfaces. A plurality of oblique breaking holes 22A and 22B are formed on the cross section at positions facing each other along 21a and 21b.
【0017】ここで同一の破壊面21a,21bに形成
されて隣接する傾斜破壊孔22A,22Bの基端開口部
22a間の距離XB1 と、先端部22b間の距離XB2
は、放電プルーブ3による直接破壊領域23の幅L(実
際はLaとLi)とすると、 XB1 ≦2×L XB2 ≦2×L すなわちそれぞれLの2倍以下に設定される。また同一
横断面上の傾斜破壊孔22A,22Bの先端部22b間
の距離YB2 は、傾斜破壊孔22A,22Bにそれぞれ
装填された放電プルーブ3による直接破壊領域23の幅
L(実際はLi)が互いに接するか重なるように設定さ
れて、先行溝21の底部で直接破壊領域23を連続させ
るように設定される。Here, a distance XB 1 between the base openings 22 a of the adjacent inclined breaking holes 22 A, 22 B formed on the same breaking surfaces 21 a, 21 b and a distance XB 2 between the front ends 22 b.
Is defined as XB 1 ≦ 2 × L XB 2 ≦ 2 × L, where L is the width of the direct breakdown region 23 due to the discharge probe 3 (actually, La and Li). The distance YB 2 between the same inclined destroy holes 22A on the cross section, 22B of tip portion 22b, inclined destroy holes 22A, the width L of the direct destroy region 23 by the discharge probe 3 is loaded respectively 22B (actually Li) is They are set so as to be in contact with or overlap with each other, and are set so that the destruction area 23 is directly continuous at the bottom of the preceding groove 21.
【0018】すなわち、傾斜破壊孔22A,22Bの第
1の自由面F1に対する傾斜角をθとすると、図5の斜
線の直角三角形において、YB 2 /2≦Lcos (90°−θ) ∴YB 2 ×Lcos (90°−θ)に設定される。[0018] That is, the inclined destroy holes 22A, when the inclination angle with respect to the first free surface F1 of 22B and theta, in the shaded right triangle in Fig. 5, YB 2/2 ≦ Lcos (90 ° -θ) ∴ YB 2 × Lcos (90 ° −θ).
【0019】これにより、先行溝21の底部で直接破壊
領域23が連続され、先行溝21をくり抜くことができ
る。もし、YB 2 >2Lcos (90°−θ)であると、
底部で直接破壊領域23が繋がらないために、先行溝2
1をくり抜くことができない。As a result, the rupture region 23 is directly continuous at the bottom of the preceding groove 21, and the preceding groove 21 can be hollowed out. If YB 2 > 2L cos (90 ° −θ),
Since the fracture region 23 is not directly connected at the bottom, the leading groove 2
1 cannot be cut out.
【0020】b.この傾斜破壊孔22A,22Bにそれ
ぞれ放電プルーブ3を装填し、放電スイッチ9aがオン
されてコンデンサ10aから高電圧が極めて短時間に全
ての放電プルーブ3に供給され金属細線8に印加され
る。これにより、金属細線8とその回りの破壊用液4が
瞬間的に気化されてその衝撃力が周囲の被破壊物1に伝
達され直接破壊領域23が繋がった状態で放電破壊され
る。これにより、逆台形状の先行溝21がくり抜かれて
第2の自由面F2が形成される。B. The discharge probes 3 are loaded into the inclined breaking holes 22A and 22B, respectively, and the discharge switch 9a is turned on. A high voltage is supplied from the capacitor 10a to all the discharge probes 3 in a very short time and applied to the thin metal wires 8. As a result, the thin metal wire 8 and the surrounding liquid 4 are instantaneously vaporized, and the impact force is transmitted to the surrounding object 1 to be destroyed by discharge in a state where the destroyed area 23 is directly connected. Thus, the inverted trapezoidal leading groove 21 is hollowed out to form the second free surface F2.
【0021】[0021]
【0022】c.先行溝21の周囲に、放電プルーブ3
の直接破壊領域に応じて破壊孔1が形成され、破壊孔1
に放電プルーブ3が装填されて、順次または同時に被破
壊物が破壊されて先行溝21が拡大され、これが繰り返
されて被破壊物1が破壊される。C. Around the leading groove 21, a discharge probe 3
The fracture hole 1 is formed in accordance with the direct fracture area of
Is charged with the discharge probe 3 and the object to be destroyed is sequentially or simultaneously destroyed, and the preceding groove 21 is enlarged. This is repeated, and the object to be destroyed 1 is destroyed.
【0023】尚、上記実施の各形態で先行溝11,21
をそれぞれ直線状としたが、曲線状であってもよい。In each of the above embodiments, the leading grooves 11, 21
Are linear, but may be curved.
【0024】[0024]
【発明の効果】以上に述べたごとく、請求項1記載の発
明によれば、自由面の先行溝を、中心から外側に広がる
両破壊面に沿って先端部が互いに交差または接近するよ
うに形成された傾斜破壊孔を形成し、これら傾斜破壊孔
に放電液圧破壊具を装填して放電破壊し、先行溝を効果
的にくり抜いて第2の自由面を形成することができ、次
いでこの第2の自由面を利用して効果的に被破壊物を破
壊することができる。As described above, according to the first aspect of the present invention, the leading groove of the free surface is formed so that the tips cross each other or approach each other along both fracture surfaces extending outward from the center. The inclined fracture holes are formed, a discharge hydraulic pressure breaker is loaded in these inclined fracture holes, discharge breakdown occurs, the preceding groove is effectively cut out, and a second free surface can be formed. The object to be destroyed can be effectively destroyed by utilizing the second free surface.
【図1】本発明に係る放電液圧破壊工法の実施の第1の
形態を示す一部切欠き斜視図である。FIG. 1 is a partially cutaway perspective view showing a first embodiment of a discharge hydraulic rupture method according to the present invention.
【図2】同被破壊物の横断面図である。FIG. 2 is a cross-sectional view of the object to be destroyed.
【図3】本発明に係る放電液圧破壊工法の実施の第2の
形態を示す一部切欠き斜視図である。FIG. 3 is a partially cutaway perspective view showing a second embodiment of the discharge hydraulic pressure breaking method according to the present invention.
【図4】同被破壊物の横断面図である。FIG. 4 is a cross-sectional view of the object to be destroyed.
【図5】同被破壊物断面の説明図である。FIG. 5 is an explanatory view of a cross section of the object to be destroyed.
【図6】同放電液圧破壊工法による破壊された先行溝の
斜視図である。FIG. 6 is a perspective view of a preceding groove broken by the discharge hydraulic pressure breaking method.
【図7】同静電液圧破壊設備を示す構成図である。FIG. 7 is a configuration diagram showing the same electrostatic hydraulic destruction equipment.
【図8】同静電液圧破壊設備による被破壊物の破壊状態
を示す断面図である。FIG. 8 is a cross-sectional view showing a destruction state of an object to be destroyed by the electrostatic hydraulic destruction equipment.
【図9】同放電液圧破壊工法における放電衝撃力と充電
電圧の関係を示すグラフである。FIG. 9 is a graph showing a relationship between a discharge impact force and a charging voltage in the discharge hydraulic pressure breaking method.
【図10】同放電液圧破壊工法における直接破壊領域と
充電電圧の関係を示すグラフである。FIG. 10 is a graph showing a relationship between a direct breakdown region and a charging voltage in the discharge hydraulic pressure breakdown method.
1 被破壊物 3 放電プルーブ 4 破壊用液 8 金属細線 10 エネルギー供給回路 11,21 先行溝 12A,12B,22A,22B 傾斜破壊孔 13,23 直接破壊領域 L 直接破壊領域の幅 Vc 充電電圧 F1 第1の自由面 F2 第2の自由面 DESCRIPTION OF SYMBOLS 1 Destruction object 3 Discharge probe 4 Breaking liquid 8 Thin metal wire 10 Energy supply circuit 11, 21 Leading groove 12A, 12B, 22A, 22B Inclined breaking hole 13, 23 Direct breaking region L Direct breaking region width Vc Charging voltage F1 1 free surface F2 2nd free surface
フロントページの続き (56)参考文献 特開 平7−145698(JP,A) (58)調査した分野(Int.Cl.7,DB名) E21C 37/18 F42D 1/045 - 1/06 F42D 3/04 E04G 23/00 - 23/08 B26F 3/00 B28D 1/00 - 7/04 Continuation of the front page (56) References JP-A-7-145698 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) E21C 37/18 F42D 1/045-1/06 F42D 3 / 04 E04G 23/00-23/08 B26F 3/00 B28D 1/00-7/04
Claims (4)
を金属細線に極めて短時間に供給することにより、金属
細線およびその周囲の液体の急激な気化、体積膨張によ
り発生する衝撃力を利用する放電液圧破壊具を使用し
て、自由面が1面である被破壊物を破壊するに際し、 まず自由面に形成されて破壊中心となる先行溝の、奥部
中心から外側に広がる破壊面に沿って、複数箇所に傾斜
破壊孔を形成し、この破壊孔内にそれぞれ放電液圧破壊
具を装填し、コンデンサから電気エネルギーを各放電液
圧破壊具に短時間で同時に供給して被破壊物を放電破壊
することにより、先行溝をくり抜いて第2の自由面を形
成し、この先行溝の周囲に複数の破壊孔を形成して、そ
れぞれの破壊孔に装填された放電液圧破壊具により放電
破壊して先行溝を拡大し被破壊物を放電破壊することを
特徴とする放電液圧破壊工法。A discharge pressure utilizing an impact force generated by rapid vaporization and volume expansion of a thin metal wire and its surroundings by supplying electric energy charged and stored in a capacitor to the thin metal wire in a very short time. When using a breaking tool to break an object to be destroyed having one free surface, first, along the breaking surface that extends outward from the center of the back of the preceding groove that is formed on the free surface and becomes the breaking center , An inclined fracture hole is formed at a plurality of locations, and a discharge hydraulic pressure destroyer is loaded into each of the fracture holes, and electric energy is simultaneously supplied from a capacitor to each discharge hydraulic pressure destroyer in a short time to discharge-break the object to be destroyed. As a result, a second free surface is formed by hollowing out the preceding groove, a plurality of breaking holes are formed around the preceding groove, and the discharge is destroyed by the discharge hydraulic pressure breaker loaded in each breaking hole. To expand the leading groove A discharge hydraulic pressure destruction method characterized in that an object to be destroyed is discharged.
面に沿って千鳥状に配置されるとともに、両辺の傾斜破
壊孔の先端部が破壊面の交差線に達するように形成し、 同一破壊面上で隣接する傾斜破壊孔の開口部間の距離X
A1 と、傾斜破壊孔の先端部間の距離XA2 は、放電液
圧破壊具による直接破壊領域の幅をLとすると、 XA1 ≦2×L、XA2 ≦2×Lの範囲にあり、また両破壊面間で隣接する傾斜破壊孔の開口部間の距離
Y 2 は、 Y 2 ≦2×Lの範囲にある ことを特徴とする請求項1記
載の放電液圧破壊工法。2. The opening of the plurality of inclined breaking holes is broken in plan view.
Are arranged in a zigzag pattern along the plane, and formed so that the tips of the inclined fracture holes on both sides reach the intersection line of the fracture plane, and the distance X between the openings of adjacent inclined fracture holes on the same fracture plane
And A 1, the distance XA 2 between the tip portion of the inclined destroy holes, and the width of the direct destroy region due to discharge pressure destroying tool is L, there XA 1 ≦ 2 × L, the range of XA 2 ≦ 2 × L And the distance between the openings of adjacent inclined fracture holes between the fracture surfaces
2. The method according to claim 1 , wherein Y 2 is in the range of Y 2 ≦ 2 × L.
対向する位置に形成し、 同一破壊面上で隣接する傾斜破壊孔の基端開口部間の距
離XB1 と、傾斜破壊孔の先端間の距離XB2 は、放電
液圧破壊具による直接破壊領域の幅をLとすると、 XB1 ≦2×L、XB2 ≦2×Lの範囲にあり、 また対向する傾斜破壊孔の先端部間の距離YB2 は、第
1の自由面に対する傾斜破壊孔の傾斜角をθとすると、 YB2 ≦2×Lcos (90°−θ)の範囲にあることを
特徴とする請求項1記載の放電液圧破壊工法。3. A plurality of oblique fracture holes are formed at positions facing each other along a fracture surface, a distance XB 1 between base openings of adjacent oblique fracture holes on the same fracture surface, and The distance XB 2 between the tips is in the range of XB 1 ≦ 2 × L and XB 2 ≦ 2 × L, where L is the width of the direct breaking area by the discharge hydraulic pressure breaking tool. distance YB 2 between parts, when the inclination angle of the inclined destroy holes with respect to the first free surface and theta, according to claim 1, characterized in that the range of YB 2 ≦ 2 × Lcos (90 ° -θ) Discharge hydraulic breakdown method.
充電電圧をVc(ボルト)とすると、直接破壊領域の幅
L(cm)は、 |Vc|/120≧L≧|Vc|/1200 の範囲にあることを特徴とする請求項2または3記載の
放電液圧破壊工法。Assuming that the charging voltage of the capacitor supplied to the discharge hydraulic pressure destroyer is Vc (volt), the width L (cm) of the direct breakdown region is: | Vc | / 120 ≧ L ≧ | Vc | / 1200 The method according to claim 2 or 3, wherein the method is in the range of:
Priority Applications (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP07194413A JP3103021B2 (en) | 1995-07-31 | 1995-07-31 | Discharge hydraulic pressure breakdown method |
RU98103872A RU2139990C1 (en) | 1995-07-31 | 1996-07-29 | Method for destruction of object by electric-discharge hydraulic pressure |
PCT/JP1996/002140 WO1997004934A1 (en) | 1995-07-31 | 1996-07-29 | Discharge hydraulic pressure destroying method |
CN96195794A CN1075430C (en) | 1995-07-31 | 1996-07-29 | Discharge hydraulic pressure destroying method |
EP96925129A EP0885703A4 (en) | 1995-07-31 | 1996-07-29 | Discharge hydraulic pressure destroying method |
KR1019980700326A KR19990029023A (en) | 1995-07-31 | 1996-07-29 | Discharge pressure breakdown method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP07194413A JP3103021B2 (en) | 1995-07-31 | 1995-07-31 | Discharge hydraulic pressure breakdown method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0938953A JPH0938953A (en) | 1997-02-10 |
JP3103021B2 true JP3103021B2 (en) | 2000-10-23 |
Family
ID=16324196
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP07194413A Expired - Fee Related JP3103021B2 (en) | 1995-07-31 | 1995-07-31 | Discharge hydraulic pressure breakdown method |
Country Status (1)
Country | Link |
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JP (1) | JP3103021B2 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP6411031B2 (en) * | 2014-01-20 | 2018-10-24 | 鹿島建設株式会社 | Dismantling method |
WO2015108098A1 (en) * | 2014-01-20 | 2015-07-23 | 鹿島建設株式会社 | Dismantling method |
-
1995
- 1995-07-31 JP JP07194413A patent/JP3103021B2/en not_active Expired - Fee Related
Also Published As
Publication number | Publication date |
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JPH0938953A (en) | 1997-02-10 |
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