JPH0141685B2 - - Google Patents
Info
- Publication number
- JPH0141685B2 JPH0141685B2 JP6867085A JP6867085A JPH0141685B2 JP H0141685 B2 JPH0141685 B2 JP H0141685B2 JP 6867085 A JP6867085 A JP 6867085A JP 6867085 A JP6867085 A JP 6867085A JP H0141685 B2 JPH0141685 B2 JP H0141685B2
- Authority
- JP
- Japan
- Prior art keywords
- torch
- arc
- plasma torch
- remelt
- speed
- 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
Links
- 239000000463 material Substances 0.000 claims description 12
- 238000003672 processing method Methods 0.000 claims 1
- 239000010410 layer Substances 0.000 description 11
- 238000000034 method Methods 0.000 description 7
- 239000007789 gas Substances 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 239000002184 metal Substances 0.000 description 4
- 229910052751 metal Inorganic materials 0.000 description 4
- 239000000654 additive Substances 0.000 description 3
- 230000000996 additive effect Effects 0.000 description 3
- 239000000843 powder Substances 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 229910001018 Cast iron Inorganic materials 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000002344 surface layer Substances 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 239000010953 base metal Substances 0.000 description 1
- 239000011261 inert gas Substances 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
Landscapes
- Heat Treatment Of Articles (AREA)
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明はカムシヤフト等のリメルト処理方法に
関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for remelting camshafts and the like.
(従来の技術)
カムシヤフトのカム部表面、ロツカアームのチ
ツプ部等の鋳鉄部材の表層部の一部は他の部材と
の摺接面となるため、当該部分は他の部分に比
べ、耐摩耗性、耐ピツチング性等の特性に優れて
いることが要求される。このためこれら鋳鉄部材
の表面にはリメルト処理が行われる。(Prior art) Parts of the surface layer of cast iron parts, such as the surface of the cam part of a camshaft and the tip part of a rocker arm, come into sliding contact with other parts, so these parts have better wear resistance than other parts. , excellent properties such as pitting resistance are required. For this reason, the surfaces of these cast iron members are subjected to remelting treatment.
斯かるリメルト処理は例えば第4図に示す如
く、鋳鉄部材であるカムシヤフト9のカム部10
と所定間隙離間してプラズマトーチ11を配設
し、カムシヤフト9を回転させると共にプラズマ
トーチ11をカム面10aの幅内において複数回
往復振動させ、これによつてカム面10aにおい
て舵行軌跡12を描きながらカム面10aを再溶
融せしめるようにしていた。 Such remelting treatment is performed, for example, as shown in FIG.
A plasma torch 11 is disposed at a predetermined distance from the camshaft 9 and the plasma torch 11 is reciprocated several times within the width of the cam surface 10a. The cam surface 10a was remelted while drawing.
(発明が解決しようとする問題点)
ところで従来、このプラズマトーチ11に供給
されるアーク電流には直流電流が使用され、この
ためカム部10の表面に供給されるプラズマアー
クのエネルギーは時間的に一定となつている。(Problems to be Solved by the Invention) Conventionally, DC current has been used as the arc current supplied to the plasma torch 11, and therefore the energy of the plasma arc supplied to the surface of the cam portion 10 varies over time. It has become constant.
ところが前記プラズマトーチ11の往復振動に
おける折り返し点13,…あるいはその近傍に於
いてはプラズマトーチの慣性力や駆動系の制御速
度の応答時間の限界等のため速度が遅くなり、カ
ム部表面上におけるプラズマトーチ11の舵行運
動速度が遅くなる。このためプラズマトーチの折
り返し点13,…及びその近傍においてはカム部
表面10aの単位面積当りに与えられるプラズマ
アークのエネルギーは他の部分(例えば中央部1
4,…)に比べて過大となり、リメルト層が深く
なり、均一な深さを有するリメルト層を得ること
ができない。 However, at or near the turning point 13 of the reciprocating vibration of the plasma torch 11, the speed becomes slow due to the inertia of the plasma torch and the limit of the response time of the control speed of the drive system. The steering movement speed of the plasma torch 11 becomes slower. Therefore, at the turning points 13 of the plasma torch and in the vicinity thereof, the energy of the plasma arc given per unit area of the cam part surface 10a is transferred to other parts (for example, the central part
4,...), the remelt layer becomes deeper, and a remelt layer having a uniform depth cannot be obtained.
第3図は以上の関係を夫々図示したものでA,
Bは横軸に時間を、縦軸に夫々舵行速度及びアー
ク電流をとつて示したもので時間T3プラズマト
ーチの往復動の半週期を、T1は半周期において
プラズマトーチが加速され一定速度になるまでの
時間を、T2からT3まではプラズマトーチが減
速され折り返し点に達するまでの時間を示す。C
はこのプラズマトーチの半周期の移動(距離L)
により得られたリメルト層の断面を示したもの
で、リメルト処理層15はその両端部15a,1
5aすなわちプラズマトーチの折り返し点及びそ
の近傍において他より深くなる。 Figure 3 illustrates the above relationships, respectively.A,
B shows time on the horizontal axis and steering speed and arc current on the vertical axis, respectively. Time T3 is the half-week period of the reciprocating motion of the plasma torch, and T1 is the half-cycle in which the plasma torch is accelerated to a constant speed. From T2 to T3 indicates the time required for the plasma torch to decelerate and reach the turning point. C
is the half-cycle movement of this plasma torch (distance L)
This figure shows a cross section of the remelt layer obtained by
5a, that is, the turning point of the plasma torch and its vicinity are deeper than the others.
このように従来のリメルト処理方法において
は、得られるリメルト処理層の深さは均一となら
ず、その表面の硬度が場所によつて不均一になる
という不具合を生じていた。 As described above, in the conventional remelt treatment method, the depth of the obtained remelt treatment layer is not uniform, and the hardness of the surface thereof is not uniform depending on the location.
そこで本発明の目的とする処は、均一な深さの
リメルト処理層が得られ、もつてリメルト処理部
材表面の硬度が均一となるリメルト処理方法を提
供するにある。 SUMMARY OF THE INVENTION Accordingly, it is an object of the present invention to provide a remelt treatment method in which a remelt treatment layer having a uniform depth can be obtained and the hardness of the surface of a remelt treatment member can be uniform.
(問題点を解決するための手段)
上記問題点を解決するため、本発明はトーチ1
と母材2の間にアークを発生させてリメルト処理
を行うに際し、トーチ1と母材2の相対移動速度
に対応させて相対移動速度が小さいときには1サ
イクル当りのパルス幅の小さい、相対移動速度が
大きいときには1サイクル当りのパルス幅の大き
いパルス電流を発生させ、これを直流アーク電流
に重畳(第2図B)させることにより相対移動速
度の大きさにかかわらず母材2の単位面積当りに
略々一定のアークエネルギーを与えるようにして
なる。(Means for Solving the Problems) In order to solve the above problems, the present invention provides a torch 1
When performing remelt processing by generating an arc between the torch 1 and the base material 2, when the relative movement speed is small, the relative movement speed is such that the pulse width per cycle is small, corresponding to the relative movement speed of the torch 1 and the base material 2. When is large, a pulse current with a large pulse width per cycle is generated, and this is superimposed on the DC arc current (Fig. 2B). Approximately constant arc energy is given.
(作用)
上記手段は次のように作用する。即ち母材の単
位面積に与えられるアークエネルギーは母材とト
ーチの相対移動速度に無関係に一定となり、処理
部材の表面に均一な深さのリメルト処理層8が得
られ、処理部材全域に渡り均一な硬度を得ること
ができる。(Operation) The above means operates as follows. In other words, the arc energy given to a unit area of the base material is constant regardless of the relative movement speed between the base material and the torch, and the remelt treatment layer 8 with a uniform depth is obtained on the surface of the processing member, which is uniform over the entire area of the processing member. hardness can be obtained.
(実施例)
以下に本発明の好適一実施例を添付図面に基づ
いて説明する。(Embodiment) A preferred embodiment of the present invention will be described below based on the accompanying drawings.
第1図は本発明に係る方法を実施するための構
成を簡略的に示した図である。第1図において符
号1は所定の駆動装置により矢印方向に回転せ
しめられる母材であるカム部材2にそのノズル部
1aを対向させ所定間隙離間して配設されたプラ
ズマトーチであり、このプラズマトーチ1は駆動
装置3により水平方向に距離Lに渡り往復移動
(母材2に対し矢印G,H方向)せしめられる。
そしてこのプラズマトーチ1のノズル部1aには
図示しないタングステン等の電極が内蔵されると
ともにその適所には不活性ガス等のシールドガ
ス、アルゴンガス等の作動ガス、そして添加金属
粉末の噴出口等を備える。 FIG. 1 is a diagram schematically showing a configuration for implementing the method according to the present invention. In FIG. 1, reference numeral 1 denotes a plasma torch, which is disposed with its nozzle portion 1a facing a cam member 2, which is a base material, and is spaced apart from it by a predetermined gap, and which is rotated in the direction of the arrow by a predetermined drive device. 1 is caused to reciprocate horizontally over a distance L (in the direction of arrows G and H with respect to the base material 2) by a drive device 3.
The nozzle portion 1a of the plasma torch 1 has an electrode (not shown) made of tungsten or the like built-in, and a shield gas such as an inert gas, a working gas such as argon gas, an ejection port for additive metal powder, etc. are provided at appropriate locations. Be prepared.
斯かる構成においてカム部材2を他方の電極と
し、シールドガス中でトーチ電極と母材2間でア
ークを発生せしめるとともに作動ガス及び添加金
属粉末を噴出させると作動ガスがプラズマ化し高
温高速のプラズマアークとなりカム部材2の表層
部に吹付けられ、この部分に溶融池を形成する。
そしてこの溶融池に添加金属粉末が溶け込み、チ
ル化することによりカム部材2表面にリメルト処
理が施されることになる。 In such a configuration, when the cam member 2 is used as the other electrode and an arc is generated between the torch electrode and the base material 2 in the shielding gas, and the working gas and additive metal powder are ejected, the working gas becomes plasma and a high-temperature, high-speed plasma arc is generated. The molten metal is sprayed onto the surface layer of the cam member 2, forming a molten pool in this area.
The additive metal powder is melted into this molten pool and chilled, so that the surface of the cam member 2 is subjected to remelt treatment.
ところで符号4はこのプラズマトーチ1の電極
に直流アーク電流を供給して電極と母材間にアー
クを発生せしめる直流用のアーク電流供給源であ
る。一方符号5は前記プラズマトーチ1の駆動装
置3に接続され、プラズマトーチ1の速度を検出
する速度検出器(例えばタコ・ジエネレータ)で
あり、この出力信号はパルス電流発生装置6に伝
達される。このパルス電流発生装置6は速度検出
器5の出力信号、即ちプラズマトーチ1の速度に
対応してプラズマトーチ1の速度が小さいときに
は1サイクル当りのパルス幅の小さい、速度が大
きいときには1サイクル当りのパルス幅の大きい
パルス電流を発生する。そしてこのパルス電流発
生装置6からのパルス電流は重畳器7により、ア
ーク電流供給源4からの直流アーク電流に重畳さ
れてプラズマトーチ1に供給される。 Incidentally, reference numeral 4 denotes a DC arc current supply source that supplies a DC arc current to the electrode of the plasma torch 1 to generate an arc between the electrode and the base metal. On the other hand, reference numeral 5 denotes a speed detector (for example, a tacho generator) connected to the drive device 3 of the plasma torch 1 to detect the speed of the plasma torch 1, and its output signal is transmitted to the pulse current generator 6. This pulse current generating device 6 corresponds to the output signal of the speed detector 5, that is, the pulse width per cycle is small when the speed of the plasma torch 1 is small, and the pulse width per cycle is small when the speed is large. Generates a pulse current with a large pulse width. The pulse current from the pulse current generator 6 is superimposed on the DC arc current from the arc current supply source 4 by a superimposer 7 and supplied to the plasma torch 1.
第2図はパルス電流発生装置の周波数を一定と
した場合の以上の関係を夫々第3図(従来例で示
した)と同様に図示したものでA,Bは横軸に時
間を、縦軸に夫々トーチ速度及びトーチ1に供給
されるアーク電流をとつて示したもので時間T3
はプラズマトーチの往復動の半周期を、T1は半
周期においてプラズマトーチが加速され一定速度
になるまでの時間を、T2からT3まではプラズ
マトーチが減速され折り返し点に達するまでの時
間を示す。A,Bより明らかなようにプラズマト
ーチ1の速度が小さいときには、幅の小さいパル
スが、大きいときには幅の大きいパルスが、カム
部材2の単位面積当りに加えられるアークエネル
ギーが略々一定となるように受畳されている。C
はこのプラズマトーチの半周期の移動(距離L)
により得られたリメルト層の断面を示したもの
で、リメルト層8の深さはその距離Lに渡つて
略々一定となる。 Figure 2 shows the above relationships when the frequency of the pulse current generator is constant, in the same way as Figure 3 (shown in the conventional example). are shown by taking the torch speed and the arc current supplied to torch 1, respectively, at time T3.
represents a half cycle of the reciprocating motion of the plasma torch, T1 represents the time it takes for the plasma torch to accelerate during the half cycle until it reaches a constant speed, and T2 to T3 represents the time it takes for the plasma torch to decelerate and reach the turning point. As is clear from A and B, when the speed of the plasma torch 1 is low, a pulse with a small width is applied, and when the speed of the plasma torch 1 is high, a pulse with a large width is applied so that the arc energy applied per unit area of the cam member 2 becomes approximately constant. It is tatami mated to. C
is the half-cycle movement of this plasma torch (distance L)
This figure shows a cross section of the remelt layer obtained by the method, and the depth of the remelt layer 8 is approximately constant over the distance L thereof.
また、パルス電流発生装置のパルス幅を一定と
した場合にトーチの速度が小さいときにはパルス
周波数を低く、トーチの速度が大きいときには、
パルス周波数を高くすることによつても同様な効
果が得られる。 Furthermore, when the pulse width of the pulse current generator is constant, when the torch speed is low, the pulse frequency is low, and when the torch speed is high, the pulse frequency is low.
A similar effect can be obtained by increasing the pulse frequency.
尚、本発明は本実施例に限定されるものではな
く、例えばプラズマトーチに対しテイグトーチな
どによるリメルト処理に使用してもよく、又、第
1図に示した構成もこれに限定されるものではな
い。 It should be noted that the present invention is not limited to this embodiment, and for example, a plasma torch may be used for remelting treatment using a Teigue torch, etc., and the configuration shown in FIG. 1 is not limited to this. do not have.
(発明の効果)
以上の説明より明らかな如く本発明に係るリメ
ルト処理方法によれば、母材の単位面積に与えら
れるアークエネルギーは母材とトーチの相対移動
速度に無関係に一定となり、処理部材の表面に均
一な深さのリメルト処理層8が得られ、処理部材
全域に渡り均一な硬度を得ることができる。(Effects of the Invention) As is clear from the above explanation, according to the remelt treatment method of the present invention, the arc energy given to the unit area of the base material is constant regardless of the relative movement speed of the base material and the torch, and the treated member A remelt treated layer 8 of uniform depth can be obtained on the surface of the treated member, and uniform hardness can be obtained over the entire area of the treated member.
第1図は本発明に係る一実施例の構成を簡略的
に示した図、第2図A,B,Cは夫々トーチ速
度、トーチに供給されるアーク電流、これらによ
り得られたリメルト層を示す図、第3図は第2図
と同様にして従来例を示した図、第4図は従来の
リメルト処理の一例を示した図である。そして図
面中、1はプラズマトーチ(トーチ)、2は母材
であるカム部材、3は駆動装置、4はアーク電流
供給源、5は速度検出器、6はパルス発生装置、
7は重畳器、8はリメルト処理層である。
Fig. 1 is a diagram schematically showing the configuration of an embodiment of the present invention, and Fig. 2 A, B, and C show the torch speed, the arc current supplied to the torch, and the remelt layer obtained by these, respectively. FIG. 3 is a diagram showing a conventional example similar to FIG. 2, and FIG. 4 is a diagram showing an example of a conventional remelting process. In the drawing, 1 is a plasma torch (torch), 2 is a cam member that is a base material, 3 is a drive device, 4 is an arc current supply source, 5 is a speed detector, 6 is a pulse generator,
7 is a superimposing device, and 8 is a remelt processing layer.
Claims (1)
ルト処理を行うに際し、トーチと母材の相対移動
速度に対応させて相対移動速度が小さいときには
1サイクル当りのパルス幅の小さい、相対移動速
度が大きいときには1サイクル当りのパルス幅の
大きいパルス電流を発生させ、これを直流アーク
電流に重畳させることにより相対移動速度の大き
さにかかわらず母材の単位面積当りに略々一定の
アークエネルギーを与えるようにしたことを特徴
とするリメルト処理方法。1 When performing remelt treatment by generating an arc between the torch and the base material, if the relative movement speed is small, the pulse width per cycle is small, and the relative movement speed is When it is large, a pulse current with a large pulse width per cycle is generated, and this is superimposed on the DC arc current to give approximately constant arc energy per unit area of the base material regardless of the relative movement speed. A remelt processing method characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6867085A JPS61227124A (en) | 1985-04-01 | 1985-04-01 | Remelt processing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6867085A JPS61227124A (en) | 1985-04-01 | 1985-04-01 | Remelt processing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61227124A JPS61227124A (en) | 1986-10-09 |
| JPH0141685B2 true JPH0141685B2 (en) | 1989-09-07 |
Family
ID=13380380
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6867085A Granted JPS61227124A (en) | 1985-04-01 | 1985-04-01 | Remelt processing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61227124A (en) |
-
1985
- 1985-04-01 JP JP6867085A patent/JPS61227124A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61227124A (en) | 1986-10-09 |
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