JPH088094A - Electrode for generating plasma arc - Google Patents

Electrode for generating plasma arc

Info

Publication number
JPH088094A
JPH088094A JP6143660A JP14366094A JPH088094A JP H088094 A JPH088094 A JP H088094A JP 6143660 A JP6143660 A JP 6143660A JP 14366094 A JP14366094 A JP 14366094A JP H088094 A JPH088094 A JP H088094A
Authority
JP
Japan
Prior art keywords
electrode
plasma arc
plasma
circular cross
insertion electrode
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.)
Granted
Application number
JP6143660A
Other languages
Japanese (ja)
Other versions
JP3179656B2 (en
Inventor
Shunei Fujii
俊英 藤井
裕之 ▲せ▼畑
Hiroyuki Sehata
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tanaka Manufacturing Co Ltd
Original Assignee
Tanaka Manufacturing Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Tanaka Manufacturing Co Ltd filed Critical Tanaka Manufacturing Co Ltd
Priority to JP14366094A priority Critical patent/JP3179656B2/en
Publication of JPH088094A publication Critical patent/JPH088094A/en
Application granted granted Critical
Publication of JP3179656B2 publication Critical patent/JP3179656B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Arc Welding In General (AREA)
  • Plasma Technology (AREA)

Abstract

PURPOSE:To provide an inexpensive plasma-arc-generating electrode which extends life and is stable. CONSTITUTION:This plasma-arc-generating electrode has an electrode base 11 having a holed portion 13 of a circular cross section open to the outside of its end portion, and has an inserted electrode 12 of a circular cross section which is tightly fitted in place inside the holed portion 13 of the electrode base 11. The inserted electrode 12 has a recessed portion 15 which is located at the center of an exposed end face 14 and recesses in the direction of the axis of the inserted electrode 12. The recessed portion 15 creates a space of a circular cross section perpendicular to the axis and has a diameter 50 to 90% of that of the inserted electrode 12 and a depth of 0.3mm or more along its axis.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、先端部外方に向けて開
口する断面円形の穴部を有する電極基体と、この電極基
体の前記穴部内に密に嵌挿固定された断面円形の挿入電
極とを備えてなるプラズマアーク発生用電極に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electrode base having a hole having a circular cross section which is open to the outside of the tip end, and a circular cross section which is tightly fitted and fixed in the hole of the electrode base. And an electrode for generating a plasma arc comprising an electrode.

【0002】[0002]

【従来の技術】周知のようにプラズマ切断装置は、ノズ
ルに設けた電極とワークとの間にアークを発生させると
ともに、該ノズルから噴出された作動ガスをプラズマ化
させて該ワークの切断を行なうものである。このプラズ
マ切断装置に用いられる電極、すなわち酸素ガスや空気
などの酸化性雰囲気ガス中で使用されるプラズマアーク
発生用電極としては、図4に示すように、銅や銅合金等
でなる電極基体1の先端部外方に向けて開口する断面円
形の穴部2に、ハフニウムやジルコニウムで断面円形の
棒状に形成された挿入電極3がインサート成形され、こ
れらハフニウムやジルコニウムの先端部が外部に露出し
た構成のものが一般的である。このプラズマアーク発生
用電極は、図5に示すように、プラズマ切断装置の加工
ヘッド本体4内部に、前記挿入電極3が該加工ヘッド本
体4の先端開口部5方向に向けて配置され、加工ヘッド
本体4のプラズマアーク発生用電極外側に形成された作
動ガス通路6を介して加工ヘッド本体4内部に作動ガス
が供給された際に、前記挿入電極3先端部分が該作動ガ
スに包まれ、この状態でアークを発生することにより、
該作動ガスをプラズマ化するようになっている。またプ
ラズマアーク発生用電極は、使用に伴って挿入電極3が
溶損し、この溶損の進行に伴って、図6に示す状態に至
るようになっている。
2. Description of the Related Art As is well known, a plasma cutting apparatus cuts a work by generating an arc between an electrode provided on a nozzle and a work and turning a working gas ejected from the nozzle into a plasma. It is a thing. As shown in FIG. 4, an electrode substrate 1 made of copper or a copper alloy is used as an electrode used in this plasma cutting device, that is, an electrode for generating a plasma arc used in an oxidizing atmosphere gas such as oxygen gas or air. The insertion electrode 3 formed of hafnium or zirconium in the shape of a rod having a circular cross-section is insert-molded into the hole 2 having a circular cross-section that is open toward the outside of the tip, and the tips of these hafnium and zirconium are exposed to the outside. The thing of a structure is general. As shown in FIG. 5, this electrode for plasma arc generation has a processing head body 4 of a plasma cutting device in which the insertion electrode 3 is arranged toward the tip opening 5 of the processing head body 4, When the working gas is supplied to the inside of the processing head body 4 through the working gas passage 6 formed outside the plasma arc generating electrode of the body 4, the tip portion of the insertion electrode 3 is wrapped in the working gas. By generating an arc in the state,
The working gas is turned into plasma. The electrode for plasma arc generation has a structure in which the insertion electrode 3 is melted and damaged as it is used, and the state shown in FIG. 6 is reached as the melting and damage progresses.

【0003】[0003]

【発明が解決しようとする課題】ところで、前記プラズ
マアーク発生用電極には、挿入電極3の溶損の結果、電
極基体1が溶損することに起因して、以下のような問題
があった。すなわち、前記挿入電極3の溶損の結果、プ
ラズマ流Pが挿入電極3の溶損した内部に入り込み、場
合によっては、図6に示すように電極基体1の穴部2内
周面の露出部分から直接プラズマ流Pが発生して、この
プラズマエネルギーによって電極基体1が溶損する。プ
ラズマ流Pが電極基体1から直接発生する場合には、プ
ラズマ流Pが偏在するので、ワークの加工精度が低下す
る。前記挿入電極3の溶損および電極基体1の溶損の進
行は一様ではなく大概の場合ばらつきがあるが、この溶
損の進行のばらつきが作動ガスの流れを乱してプラズマ
乱流を形成し、ワークの加工能率および加工精度の低下
を招いていた。前記溶損の進行のばらつきは、溶損の進
行が早い部分が完全に溶損してしまえばプラズマアーク
発生用電極の寿命に大きな影響を与え、結果的にプラズ
マアーク発生用電極の寿命を短縮するとともに、一般的
には溶損の進行の早い部位が不確定であるためにプラズ
マアーク発生用電極の寿命が不安定であって、加工を中
断してプラズマアーク発生用電極の交換を余儀なくされ
るケースが発生して、製品の分留まり低下の原因となっ
ていた。また、挿入電極3の溶損の進行によって電極基
体1の内周面が露出すれば、電極基体1への入熱によっ
て電極基体1の挿入電極3に対する冷却作用が無くな
り、挿入電極3の溶損が促進される状況になるととも
に、入熱量が臨界状態を越えれば電極基体1が一気に溶
融して、プラズマアーク発生用電極の寿命短縮が促進さ
れる。
The plasma arc generating electrode, however, has the following problems due to the melting damage of the electrode base 1 as a result of the melting damage of the insertion electrode 3. That is, as a result of the erosion of the insertion electrode 3, the plasma flow P enters the erosion inside of the insertion electrode 3, and in some cases, the exposed portion of the inner peripheral surface of the hole 2 of the electrode base 1 as shown in FIG. A plasma flow P is generated directly from the electrode base 1, and the plasma energy causes the electrode substrate 1 to melt. When the plasma flow P is generated directly from the electrode substrate 1, the plasma flow P is unevenly distributed, so that the machining accuracy of the work is deteriorated. Although the progress of the melting loss of the insertion electrode 3 and the progress of the melting loss of the electrode substrate 1 are not uniform and generally vary, the variation in the progress of the melting loss disturbs the flow of the working gas to form plasma turbulence. However, the work efficiency and the work accuracy of the work are deteriorated. The variation of the progress of the melting loss has a great influence on the life of the plasma arc generating electrode if the portion where the progress of the melting loss progresses is completely melted, and as a result, the life of the plasma arc generating electrode is shortened. At the same time, the life of the plasma arc generation electrode is generally unstable because the part where the melting loss progresses is uncertain, and the processing is interrupted and the plasma arc generation electrode must be replaced. A case has occurred, which has been a cause of reduced retention of product. Further, if the inner peripheral surface of the electrode base 1 is exposed due to the progress of the melting damage of the insertion electrode 3, the cooling effect of the electrode base 1 on the insertion electrode 3 is lost by the heat input to the electrode base 1, and the melting damage of the insertion electrode 3 is lost. When the amount of heat input exceeds the critical state, the electrode base body 1 melts at once and the life of the plasma arc generating electrode is shortened.

【0004】前記問題に鑑みて、図4に示すように、挿
入電極3先端面に深さ0.05mm程度の円錐状の凹所
7を設ける技術が知られているが、この技術は、プラズ
マアーク発生用電極の使用初期状態においてのみプラズ
マ流Pの安定化や挿入電極3の一様な溶損に寄与する手
段であって、電極基体1の保護や溶損の安定といった面
ではその効果に不満があった。
In view of the above problem, as shown in FIG. 4, a technique is known in which a conical recess 7 having a depth of about 0.05 mm is provided on the distal end surface of the insertion electrode 3, but this technique uses plasma. It is a means that contributes to stabilization of the plasma flow P and uniform melting loss of the insertion electrode 3 only in the initial state of use of the arc generating electrode, and is effective in terms of protection of the electrode base 1 and stability of melting loss. I was dissatisfied.

【0005】一方、挿入電極3の溶損に対して電極基体
1内周面を保護してプラズマアーク発生用電極の寿命の
安定および延長を図る技術として、電極基体1と挿入電
極3との間に第3の物質を介装する技術も提案されてい
る。この技術は、前記第3の物質として金合金、銀合
金、アルミニウム合金等の熱伝導性および導電性に優れ
た材料を使用し、この第3の部材を筒状に形成した部材
として前記穴部2に挿入したり、電極基体1に拡散結合
させるが、材料が高価である上、作業に手間がかかるた
め、コスト上昇および製造能率の低下の原因になるとい
った問題がある。
On the other hand, as a technique for protecting the inner peripheral surface of the electrode base 1 against the melt damage of the insertion electrode 3 to stabilize and extend the life of the electrode for generating plasma arc, a technique between the electrode base 1 and the insertion electrode 3 is used. A technique of interposing a third substance is also proposed. This technique uses a material having excellent thermal conductivity and electrical conductivity such as a gold alloy, a silver alloy, and an aluminum alloy as the third substance, and uses the third member as a cylindrical member to form the hole portion. Although it is inserted into the electrode 2 or is diffusion-bonded to the electrode substrate 1, there is a problem that the material is expensive and the work is troublesome, which causes an increase in cost and a decrease in manufacturing efficiency.

【0006】本発明は、前述の課題に鑑みてなされたも
ので、寿命が延長しかつ安定する安価なプラズマアーク
発生用電極を提供することを目的とするものである。
The present invention has been made in view of the above-mentioned problems, and an object of the present invention is to provide an inexpensive plasma arc generating electrode having an extended life and stability.

【0007】[0007]

【課題を解決するための手段】請求項1記載の発明で
は、先端部外方に向けて開口する断面円形の穴部を有す
る電極基体と、この電極基体の前記穴部内に密に嵌挿固
定された断面円形の挿入電極とを備えてなり、前記挿入
電極の外部に露出する先端面にその中心部に位置させて
該挿入電極の軸線方向に凹む凹部が形成され、該挿入電
極の使用により、前記凹部が前記軸線方向へ深くなるよ
う消耗するプラズマアーク発生用電極において、前記凹
部は、前記軸線に対して直交する方向の断面が円形の空
間とされ、その径が、前記挿入電極の径の50〜95%
であることを特徴とするプラズマアーク発生用電極を前
記課題の解決手段とした。
According to a first aspect of the present invention, there is provided an electrode base having a hole having a circular cross section, which is open toward the outer end of the tip, and the electrode base is tightly fitted and fixed in the hole. The insertion electrode having a circular cross-section is formed, and a concave portion that is located in the center of the tip surface exposed to the outside of the insertion electrode and is recessed in the axial direction of the insertion electrode is formed. In the plasma arc generating electrode that is consumed so that the recess becomes deeper in the axial direction, the recess has a circular cross section in a direction orthogonal to the axis, and the diameter thereof is the diameter of the insertion electrode. 50-95% of
The electrode for plasma arc generation characterized in that

【0008】請求項2記載の発明では、前記凹部は軸線
方向に0.3mm以上の深さを有することを特徴とする
前記請求項1記載のプラズマアーク発生用電極を前記課
題の解決手段とした。
According to a second aspect of the present invention, the plasma arc generating electrode according to the first aspect is characterized in that the recess has a depth of 0.3 mm or more in the axial direction. .

【0009】[0009]

【作用】請求項1記載のプラズマアーク発生用電極によ
れば、プラズマアーク発生用電極の使用に伴って挿入電
極がその外周部を残しつつ軸線方向奥方に溶損する。
According to the plasma arc generating electrode of the first aspect, when the plasma arc generating electrode is used, the insertion electrode is melted and damaged in the axial direction while leaving the outer peripheral portion thereof.

【0010】請求項2記載のプラズマアーク発生用電極
によれば、挿入電極の溶損が進行した状態においても、
挿入電極がその外周部を残しつつ軸線方向奥方に溶損す
ることが安定して進行する。
According to the plasma arc generating electrode of the second aspect, even in the state in which the melting loss of the insertion electrode progresses,
The insertion electrode can be stably melted inward in the axial direction while leaving the outer peripheral portion thereof.

【0011】[0011]

【実施例】以下本発明の一実施例を、図1から図3を参
照して説明する。図1において、図中符号10は本発明
のプラズマアーク発生用電極、11は電極基体、12は
挿入電極である。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIGS. In FIG. 1, reference numeral 10 in the drawing is a plasma arc generating electrode of the present invention, 11 is an electrode substrate, and 12 is an insertion electrode.

【0012】前記プラズマアーク発生用電極10は、前
記図5の加工ヘッド本体4内に配置されるものであっ
て、先端部外方に向けて開口する断面円形の穴部13を
有する電極基体11と、この電極基体11の前記穴部1
3内に密に嵌挿固定された断面円形の挿入電極12とを
備えてなっている。前記電極基体11は銅または銅合金
製であって、前記穴部13が前記加工ヘッド本体4の開
口部5方向に向けられた状態で加工ヘッド本体4内に配
置される。前記挿入電極12は、ハフニウムまたはジル
コニウム製の部材であって、外部に露出する先端面14
にその中心部に位置させて該挿入電極12の軸線方向に
凹む凹部15が形成され、該挿入電極12の使用によ
り、前記凹部15が前記軸線方向へ深くなるよう消耗す
るようになっている。前記凹部15は、前記軸線に対し
て直交する方向の断面が円形で、その径が前記挿入電極
12の径の50〜95%であるとともに、軸線方向に
0.3mm以上の深さXを有する穴であって、電極基体
11と同軸状に形成されている。また、前記凹部15の
径寸法Yは、例えば、使用電流250A、挿入電極12
の径φが2.0mmの場合、1.0〜1.9mmに設定
する。
The plasma arc generating electrode 10 is arranged in the processing head body 4 shown in FIG. 5, and has an electrode base 11 having a hole 13 having a circular cross section which is open toward the outer end of the tip. And the hole 1 of the electrode substrate 11
3, and an insertion electrode 12 having a circular cross section which is tightly fitted and fixed. The electrode base body 11 is made of copper or a copper alloy, and is arranged in the processing head body 4 with the hole portion 13 being directed toward the opening 5 of the processing head body 4. The insertion electrode 12 is a member made of hafnium or zirconium and has a tip surface 14 exposed to the outside.
A recess 15 is formed at the center of the insertion electrode 12 and is recessed in the axial direction of the insertion electrode 12. By using the insertion electrode 12, the recess 15 is consumed so as to become deep in the axial direction. The recess 15 has a circular cross section in a direction orthogonal to the axis, has a diameter of 50 to 95% of the diameter of the insertion electrode 12, and has a depth X of 0.3 mm or more in the axis direction. It is a hole and is formed coaxially with the electrode base 11. Further, the diameter dimension Y of the recess 15 is, for example, 250 A of working current, the insertion electrode 12
When the diameter φ is 2.0 mm, it is set to 1.0 to 1.9 mm.

【0013】前記プラズマアーク発生用電極10は、プ
ラズマ切断等に使用した際には、図1に示すように、凹
部15の作用でプラズマ流Pが正常位置に安定に保持さ
れ、このプラズマ流Pを安定保持したまま、前記凹部1
5から挿入電極12の軸線方向奥方に向かって挿入電極
12の溶損が進行する。挿入電極12は、溶損が進行し
て、やがて図2に示すように、挿入電極12の外周部の
みを残して円筒状になる。この際、挿入電極12は、電
極基体11を露出させることなく電極基体11の穴部1
3の内周面全体を被うので、電極基体11から直接プラ
ズマ流Pが発生することがなく、溶損が相当進行した場
合においてもプラズマ流Pが安定保持される。
When the plasma arc generating electrode 10 is used for plasma cutting or the like, as shown in FIG. 1, the plasma flow P is stably held in a normal position by the action of the recess 15, and the plasma flow P is maintained. While holding the
The melting loss of the insertion electrode 12 progresses from 5 toward the inner side of the insertion electrode 12 in the axial direction. As the erosion progresses, the insertion electrode 12 eventually becomes a cylindrical shape, leaving only the outer peripheral portion of the insertion electrode 12, as shown in FIG. At this time, the insertion electrode 12 does not expose the electrode base 11 and the hole portion 1 of the electrode base 11 is not exposed.
Since the entire inner peripheral surface of 3 is covered, the plasma flow P is not directly generated from the electrode base 11, and the plasma flow P is stably maintained even when the melting loss progresses considerably.

【0014】したがって、本発明のプラズマアーク発生
用電極10は、挿入電極12の溶損が進行してもプラズ
マ流Pが常時安定保持されるので、ワークの加工精度お
よび加工能率が向上する。また、プラズマ流Pが常時安
定して発生するので、挿入電極12の局所的な溶損・消
耗が防止され、例えば、図3に示すように、同一条件に
おいてアーク発生回数に対する挿入電極の消耗深さの実
験結果を比較した場合、従来のプラズマアーク発生用電
極に比して寿命が大幅に延長することがわかる。
Therefore, in the plasma arc generating electrode 10 of the present invention, the plasma flow P is always maintained stably even when the insertion electrode 12 is melted and damaged, so that the machining accuracy and the machining efficiency of the work are improved. Further, since the plasma flow P is constantly generated, local melting loss and wear of the insertion electrode 12 are prevented, and for example, as shown in FIG. 3, the wear depth of the insertion electrode with respect to the number of arc occurrences under the same conditions. When the results of the experiments are compared, it can be seen that the life is greatly extended as compared with the conventional plasma arc generating electrode.

【0015】さらに、プラズマ流Pの安定によって、前
記プラズマアーク発生用電極10の寿命が安定するの
で、プラズマアーク発生用電極10の交換時期を予測す
ることができ、ワークの加工作業を効率良く行なうこと
ができる。前記プラズマアーク発生用電極10は、電極
基体11と挿入電極12との間への第3の物質の介装が
不要であり、しかも、前記凹部15は簡単に形成するこ
とができるので、安価に得られる。
Further, since the plasma flow P is stabilized and the life of the plasma arc generating electrode 10 is stabilized, the replacement time of the plasma arc generating electrode 10 can be predicted, and the work of the workpiece can be efficiently performed. be able to. The plasma arc generating electrode 10 does not require the interposition of the third substance between the electrode base 11 and the insertion electrode 12, and the recess 15 can be easily formed, so that the cost can be reduced. can get.

【0016】なお、前記凹部15の形状は、前記したも
のに限られず、全体または一部にテーパが付けられたも
のや、円錐状であってもよい。
The shape of the concave portion 15 is not limited to the above-mentioned shape, but may be a tapered shape in whole or in part, or a conical shape.

【0017】[0017]

【発明の効果】以上説明したように本発明のプラズマア
ーク発生用電極によれば、挿入電極が溶損した際に自身
の外周部のみを残して中央部のみが溶損して、挿入電極
の残った部分が電極基体を露出させることなく電極基体
の内周面全体を被うので、電極基体から直接プラズマ流
が発生することがなく、溶損が相当進行した場合におい
てもプラズマ流が安定保持され、ワークの加工精度およ
び加工能率が向上するとともに、プラズマ流の安定によ
って、前記プラズマアーク発生用電極の寿命が延長かつ
安定し、また、この寿命の安定によって、プラズマアー
ク発生用電極の交換時期が予測でき、ワークの加工作業
を効率良く行なうことができる。
As described above, according to the plasma arc generating electrode of the present invention, when the insertion electrode is melted, only the outer peripheral part of the electrode is left and only the central part is melted, and the insertion electrode remains. Since the exposed portion covers the entire inner peripheral surface of the electrode base without exposing the electrode base, the plasma flow is not directly generated from the electrode base, and the plasma flow is stably maintained even when the melting loss progresses considerably. In addition, the machining accuracy and the machining efficiency of the work are improved, and the plasma flow is stabilized, so that the life of the plasma arc generation electrode is extended and stabilized, and the stabilization of this life allows the replacement time of the plasma arc generation electrode. It can be predicted and the work of the workpiece can be efficiently performed.

【0018】請求項2記載のプラズマアーク発生用電極
によれば、挿入電極の溶損が進行した状態においても、
挿入電極がその外周部を残しつつ軸線方向奥方に溶損す
ることが安定して進行して、プラズマ流が安定に保持さ
れるので、一層の寿命の延長や電極交換時期の安定化と
いった優れた効果を奏する。
According to the plasma arc generating electrode of the second aspect, even in the state where the insertion electrode is melted and damaged,
The insertion electrode remains stable at the axial depth while leaving the outer periphery of the insertion electrode, and the plasma flow is stably maintained, resulting in an even longer life and stabilization of the electrode replacement period. Play.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の電極を示す側断面図である。FIG. 1 is a side sectional view showing an electrode of the present invention.

【図2】図1の電極の挿入電極溶損時のプラズマ発生状
態を示す側断面図である。
FIG. 2 is a side sectional view showing a plasma generation state when the insertion electrode melts in the electrode of FIG.

【図3】従来の挿入電極と本発明の挿入電極について、
同一条件におけるアーク発生回数に対する消耗深さの関
係を示すグラフである。
FIG. 3 shows a conventional insertion electrode and an insertion electrode of the present invention,
It is a graph which shows the relationship of the consumption depth with respect to the frequency | count of arc generation on the same conditions.

【図4】従来の電極を示す側断面図である。FIG. 4 is a side sectional view showing a conventional electrode.

【図5】加工ヘッド本体を示す側断面図である。FIG. 5 is a side sectional view showing a processing head body.

【図6】従来の電極の挿入電極の溶損を示す側断面図で
ある。
FIG. 6 is a side sectional view showing melting damage of an insertion electrode of a conventional electrode.

【符号の説明】[Explanation of symbols]

10 電極 11 電極基体 12 挿入電極 13 穴部 14 先端面 15 凹部 10 Electrode 11 Electrode Base 12 Insertion Electrode 13 Hole 14 Tip Surface 15 Recess

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 先端部外方に向けて開口する断面円形の
穴部を有する電極基体と、この電極基体の前記穴部内に
密に嵌挿固定された断面円形の挿入電極とを備えてな
り、前記挿入電極の外部に露出する先端面にその中心部
に位置させて該挿入電極の軸線方向に凹む凹部が形成さ
れ、該挿入電極の使用により、前記凹部が前記軸線方向
へ深くなるよう消耗するプラズマアーク発生用電極にお
いて、前記凹部は、前記軸線に対して直交する方向の断
面が円形の空間とされ、その径が、前記挿入電極の径の
50〜95%であることを特徴とするプラズマアーク発
生用電極。
1. An electrode base having a hole having a circular cross section that is open toward the outside of the tip, and an insertion electrode having a circular cross section that is closely fitted and fixed in the hole of the electrode base. , A concave portion is formed on the tip end surface exposed to the outside of the insertion electrode, the concave portion being located at the center of the insertion electrode and recessed in the axial direction of the insertion electrode. In the plasma arc generating electrode described above, the concave portion is a space having a circular cross section in a direction orthogonal to the axis, and the diameter thereof is 50 to 95% of the diameter of the insertion electrode. Electrode for plasma arc generation.
【請求項2】 前記凹部は軸線方向に0.3mm以上の
深さを有することを特徴とする前記請求項1記載のプラ
ズマアーク発生用電極。
2. The electrode for plasma arc generation according to claim 1, wherein the recess has a depth of 0.3 mm or more in the axial direction.
JP14366094A 1994-06-24 1994-06-24 Electrodes for plasma arc generation Expired - Fee Related JP3179656B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14366094A JP3179656B2 (en) 1994-06-24 1994-06-24 Electrodes for plasma arc generation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14366094A JP3179656B2 (en) 1994-06-24 1994-06-24 Electrodes for plasma arc generation

Publications (2)

Publication Number Publication Date
JPH088094A true JPH088094A (en) 1996-01-12
JP3179656B2 JP3179656B2 (en) 2001-06-25

Family

ID=15343970

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14366094A Expired - Fee Related JP3179656B2 (en) 1994-06-24 1994-06-24 Electrodes for plasma arc generation

Country Status (1)

Country Link
JP (1) JP3179656B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012512510A (en) * 2008-12-18 2012-05-31 シェルベリ フィンスターヴァルデ プラスマ ウント マシーネン ゲーエムベーハー Electrode for plasma torch

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012512510A (en) * 2008-12-18 2012-05-31 シェルベリ フィンスターヴァルデ プラスマ ウント マシーネン ゲーエムベーハー Electrode for plasma torch

Also Published As

Publication number Publication date
JP3179656B2 (en) 2001-06-25

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