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JPH0527490B2 - - Google Patents
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JPH0527490B2 - - Google Patents

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Publication number
JPH0527490B2
JPH0527490B2 JP17905487A JP17905487A JPH0527490B2 JP H0527490 B2 JPH0527490 B2 JP H0527490B2 JP 17905487 A JP17905487 A JP 17905487A JP 17905487 A JP17905487 A JP 17905487A JP H0527490 B2 JPH0527490 B2 JP H0527490B2
Authority
JP
Japan
Prior art keywords
pass
austenitic steel
temperature
metastable austenitic
passes
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 - Lifetime
Application number
JP17905487A
Other languages
Japanese (ja)
Other versions
JPS6422412A (en
Inventor
Chuzo Sudo
Takashi Tsukamoto
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.)
Nippon Steel Corp
Original Assignee
Sumitomo Metal Industries 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 Sumitomo Metal Industries Ltd filed Critical Sumitomo Metal Industries Ltd
Priority to JP17905487A priority Critical patent/JPS6422412A/en
Publication of JPS6422412A publication Critical patent/JPS6422412A/en
Publication of JPH0527490B2 publication Critical patent/JPH0527490B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

<産業上の利用分野> この発明は、磁気目盛素材等として好適な強磁
性化準安定オーステナイト鋼棒を経済性良く安定
して製造するための、低い引抜減面率でもつて十
分に加工誘起変態を促進させる準安定オーステナ
イト鋼の引抜方法に関するものである。 近年、例えばピストンロツド等の変位量や変位
速度等を測定するのに“磁気目盛”の採用が目立
つようになつてきた。 “磁気目盛”とは、金属材料等から成る基体表
面に線状又は帯状の磁気的変質部を規則的に配列
形成して目盛部となしたものであり、その表面部
に近接対峙させた磁気センサーにて上記目盛を読
み取ることによつて、前記基体と磁気センサーと
の相対変位を測定するためのものである。 <従来技術とその問題点> 従来の、このような“磁気目盛”として、強磁
性体から成る基体に空隙溝を削り出し、この空隙
溝を磁気変質部として活用するものが知られてい
た。 しかし、このようにして製作された“磁気目
盛”は磁気目盛特性が良くて高い出力を得られる
ものではあつたが、その構造上、ピストンロツド
や案内軸等のような摺動軸に使用するには溝を埋
めなければならず、製造コストや機械的強度上か
ら実用的でないと言う問題点があつた。 また、特開昭57−16309号公報にみられるよう
に、金属材料表面に高エネルギービームを照射し
て局部的に熱処理し、その部分を磁気的に変質さ
せて目盛付けすると言う手段で“磁気目盛”を製
作する方法も提案されたが、この場合には製作方
法自体は簡便ではあるものの母材部(基体部)と
熱処理部との磁気特性の差が小さい製品しか得ら
れる、使用に当つて高価な検出装置を必要とした
り、或いは製品の信頼性が今一つ十分でないとの
問題点があつた。もつとも、上記提案の中には磁
気特性向上対策についても触れられており、25%
Fe−75%Ni合金等の非常に高価な磁性材料を適
用する例が示されているが、このようにして得ら
れる製品は高価であるばかりではなく強度が耐摩
耗性の面でも余り高くは望めないことから用途上
の制約が多い上、磁気特性も完全とは言い難いも
のであつた。 即ち、“磁気目盛”においては、理論上、空隙
溝を形成することによりその部分で最大の磁気出
力が得られることは既に述べたが、“空隙溝”と
は、言い換えれば“非磁性体”を指すものであ
り、従つて上記事項は「強磁性体と非磁性体を組
み合わせたものが磁気目盛として最良である」こ
とを示しているものである。ところが、前記提案
のFe−Ni合金を使用した“磁気目盛”は、母材
部(基体部)及び熱処理部とも強磁性体であつ
て、単にそれらの透磁率の差によつてのみ目盛が
形成されているに過ぎないものであるから、磁気
特性上必ずしも理想的な製品とは言えないのであ
る。 更に、これ等とは別に、化学メツキにより金属
材の表面にNi及びPを主成分とする薄膜(0.2〜
0.3mm厚)を形成して基体とし、部分的な通電加
熱やレーザなどの粒子線による加熱によつて前記
基体上の薄膜に磁気的変質部を所定間隔で設けて
成る“磁気目盛”も提案されている(特開昭58−
7517号)。 しかしながら、上記の如き“Ni及びPを主成
分とするメツキ薄膜に部分加熱処理を施して変質
部を形成したもの”では、目盛の読み取り感度が
比較的低いためにS/N比が悪いと言う欠点があ
つて感度を高めるためには薄膜の厚さをかなり厚
くしなければならない等の経済的不利を避け得な
い上、磁気目盛表面に耐摩耗性が要求される場合
には更にクロムメツキ等の耐摩耗性被覆を施す必
要があつて加工工程が複雑になるとの問題点があ
り、また加熱処理されたメツキ薄膜にクラツク等
の損傷が発生する恐れもあつた。 このような状況の中で、本発明者等は、先に、
前記従来法が有する問題点をほぼ解決したところ
の『基体が冷間加工誘起変態によるマルテンサイ
ト組織を10%以上含む強磁性体のオーステナイト
鋼であり、目盛部が局部的な溶融処理による非磁
性のオーステナイト組織であることを特徴とする
磁気目盛』を提案した。 この本発明者等の提案になる上記磁気目盛は、
“準安定オーステナイト鋼を冷間加工して強磁性
化した基体にレーザ照射して局部的な非磁性化部
を形成し目盛としたもの”であり、極めて良好な
磁気特性を有するものであるが、それでも、準安
定オーステナイト鋼の強磁性化のために高加工度
の冷間加工を必要とし、従つて大型の引抜設備を
必要とするなど製造上の制約を余儀無くされるも
のであつた。 即ち、準安定オーステナイト鋼に積極的に加工
誘起変態を起こして強磁性化するが如き必要性が
無かつたこともあつて、従来、このような引抜手
段は確立されていなかつたのである。 なぜなら、準安定オーステナイト鋼は加工誘起
変態によりマルテンサイト組織が生じるので非常
に硬くなる性質があり、その引抜作業においては
“ダイスの焼付”や“断線”等のトラブルを発生
し易いからである。そのため、通常用途の準安定
オーステナイト鋼材料の引抜に際しては、従来、
“加工誘起変態をできるだけ抑制する”ことに主
眼がおかれ、一般的には第3図で示されるような
「温間にて必要な減面率を1パスで引抜くことで
加工誘起変態の抑制と高能率化を図る手段」が採
用されているに過ぎなかつた。なお、第3図にお
いて、符号1は引抜素材を、2は引抜ダイスをそ
れぞれ示している。 <問題点を解決するための手段> 本発明者等は、上述のような実情に鑑み、従来
は意図されることのなかつた“加工誘起変態をで
きるだけ促進して十分な強磁性化が達成されるよ
うな準安定オーステナイト鋼の強磁性化引抜法”
を確立すべく、特に 「準安定オーステナイト鋼の引抜加工に際して
冷間での減面率(加工率)を高くすれば加工誘起
変態が進行するのは当然であるが、減面率を大き
くすることは大型の引抜設備や付属設備の増強に
つながつて大幅なコスト上昇を招く上、作業トラ
ブルが増大するなどの工業的に決して好ましいも
のではない」 との認識の下に、「準安定オーステナイト鋼の引
抜において、引抜減面率を可能な限り低く抑えた
上で加工誘起変態をできるだけ促進させることの
可能性」を追求しつつ研究を重ねた結果、以下(a)
〜(d)に示される如き知見が得られたのである。即
ち、 (a) 例えば磁気目盛素材等として好適な、十分に
強磁性化された準安定オーステナイト鋼引抜棒
材を引抜加工によつて得る場合には、入口引抜
温度が140℃以下に抑制されている必要があり、
該引抜温度が特に140℃までに抑えられていれ
ば問題はないが、その温度を超えると十分な強
磁性化が達成されない。 (b) ところが、機器部材に要求される組織や強度
を備えた引抜棒製品を得るために適用される通
常径寸法の素材(十分な減面率が見込まれてい
る)から1パスで所要製品寸法にまで引抜を行
うと、加工熱のため準安定オーステナイト鋼棒
素材の引抜温度を140℃以下に抑えることは不
可能である上、変態による硬化のためにダイス
焼付や素材の切断等のトラブルが生じ易くな
る。 (c) しかし、引抜に際して引抜パス数を複数とし
て1パス当りの減面率を低くすると加工熱によ
る素材の温度上昇が抑制され、所要径寸法に仕
上がるまでの入口引抜温度を140℃以下に抑え
ることが十分可能になると共に、所要径寸法に
仕上がつた製品の強度も十分に高くなり、しか
もダイス焼付や素材の切断と言つたトラブルも
安定して防止される。 なお、このとき、各パス間での素材の放熱が
若干不足する場合にはパスを重ねる毎に素材温
度が上昇し、実際には最終パスにおいて140℃
を超えることもあり得るが、その場合でもそれ
以前のパスにおいて加工誘起変態が十分促進さ
れているので、強磁性化は十分に向上する。 (d) ただ、引抜作業能率を上げかつ十二分に安定
した強磁性化を達成するには各パス間で素材に
強制冷却を施すのが効果的であり、これにより
各パス間での自然放熱を待つことなく引抜温度
を安定して140℃以下に抑えることが可能とな
つて、“複数の引抜ダイスを直線上に配置する
と共に、最終ダイス出口に設けた1基のつかみ
装置で全パスを同時に引き抜く”と言う高能率
多重ダイス引抜の実施にも好都合となる。 この発明は、上記知見に基づいてなされたもの
であり、 「準安定オーステナイト鋼棒を引抜加工するに
際し、引抜パス数を複数として1パス当りの減面
率を小さくすることで各パスにおける引抜温度を
140℃以下に維持しつつ冷間引抜を行うか、或い
は引抜パス数を複数として1パス当りの減面率を
小さくすると共に、各パス通過前の中間素材を強
制冷却してその直前の引抜ダイス通過による温度
上昇を抑えることで各パスにおける引抜温度を
140℃以下に維持しつつ冷間引抜を行い、これに
よつて加工誘起変態を積極的に生ぜしめると共に
強度を向上させ、十分に高い強磁性と強度とを有
する準安定オーステナイト鋼棒を安定して製造し
得るようにした」点 に特徴を有するものである。 なお、上記“準安定オーステナイト鋼”とは、
例えばSUS301やSUS304ステンレス鋼等の如き
「溶体化処理を受けることによつて完全オーステ
ナイト組織となり非磁性を示すが、その後の冷間
加工により加工誘起変態を生じてマルテンサイト
組織となつて強磁性化し、更に再度の溶体化処理
で完全オーステナイト組織となつて非磁性となる
もの」として知られているが、この発明に適用す
るに当たつては、その種類が問われるものではな
い。 以下、この発明を更に詳細に説明する。 まず、この発明の方法において引抜パス数を複
数とすることは極めて重要なことであるが、これ
は、引抜製品を得るための所定減面率を達成する
のに“1パス”ではなく“2パス又はそれ以上”
にパスを分割することを意味しており、これによ
つてパス当りの加工発熱が減少するので加工誘起
変態を十分に促進できるのである。 ところで、一般の引抜加工において大きな減面
率を必要とする場合で、1パスでは材料の断線や
引抜機の容量の制約等から引抜が不可能なときに
は、パス数を複数に分けて引抜くこと従来からも
実施されていた手段である。しかしながら、この
場合の多パス引抜はあくまでも“作業上のトラブ
ルなく引抜作業を行う”との観点からのみ実施さ
れるものであつて、1パスでの引抜作業が不可能
なときにだけ採用されていた手段である。 これに対し、本発明の方法にあつては、引抜素
材として準安定オーステナイト鋼を対象にすると
共に、本来1パスで引抜くことが可能な減面率を
“加工熱によつて準安定オーステナイト鋼引抜素
材の加工誘起変態が阻まれる領域にまで温度上昇
しないようにするために1パス当りの減面率を抑
える”との観点から分割するものであり、引抜パ
スを複数に分割する目的が全く異なるものであ
る。つまり、本発明の方法においてパスを分割す
る狙いは引抜時の材料温度を低下することにあ
り、引抜温度は引抜の減面率を下げれば著しく低
下するので、それにより加工誘起変態が顕著に促
進されるのである。 従つて、本発明の方法を実施するに際して、1
パス(1ダイス)毎に引抜装置によつて引き抜く
ことが必要である前記“従来観点からの複数パス
引抜”では不可能であつたところの「引抜ライン
上の引抜ダイス数を増やして複数のダイスを直線
上に配列した状態にすると共に、全減面率を1つ
の引抜装置での1回の引抜動作でもつて一気に引
抜く方法(ここでは“多重ダイス法”と呼ぶ)」
の適用も可能であり、またそれで十分でもある。
なお、第1図は上記“多重ダイス法”の概念図で
あつて、直線上に複数の引抜ダイス2,2,…を
配置すると共に、一回の引抜動作でもつて一気に
所要減面率にまで引抜素材1を引抜く様子を示し
たものである。 そして、この“多重ダイス法”は一工程で加工
を完了できるので、従来の多パス引抜に比べると
優れた生産性が確保でき極めて好ましい手段であ
るが、生産性に重きを置かなければ従来の多パス
引抜法でも加工誘起変態促進の効果が得られるこ
とは言うまでもない。 なお、以前に公開された特開昭58−221611号公
報には、2個のダイスと1基の引抜装置を使用す
ると共に、これによつて引抜素材を一気に引抜く
方法が開示されているが、これはダイス間におい
て材料の表面疵を検査するに際し寸法精度とパス
センタを確保するために行うものであつて、本発
明の方法と本質的に異なつていることは断るまで
もない。 さて、上述のように、本発明の方法においては
入口引抜温度の管理が極めて重要であり、例えば
磁気目盛用素材等としての性能を決めるのに支配
的な役割を果たすものである。 入口引抜温度が140℃を超えると引抜製品の十
分な強磁性化が達成できず、磁気目盛等に適用す
る場合には強磁性特性が不足して満足できる製品
が得られない。従つて、入口引抜温度が140℃を
超えないように所定減面率となるまでの引抜パス
数を設定するか、或いはパス数を分割して引抜温
度上昇を軽減した上で、ダイス入口で引抜素材を
補助的に強制冷却する必要がある。 もつとも、特に前記多重ダイス法を適用した場
合には、ダイス間における冷却不足のためパスを
重ねる毎に素材の温度が上昇し、最終パスにおい
て140℃の上限を超えることも実際には考えられ
るが、前述した通り、このような場合でも基本的
に本発明法の如き対策がとられておればそれ以前
のパスにおいて加工誘起変態が十分促進されてい
るので、磁気特性は十分に向上する。 このため、実用上は常温の大気中での複数パス
による引抜作業で十分に所期の目的を達成できる
が、更に強力な温度上昇抑制を望む場合には液化
ガス等の室温以下の冷媒にてダイス通過前の素材
をダイス入口で冷却すれば良い。強制冷却によつ
て、それだけ強磁性化効果が向上する。 多重ダイス法にて強制冷却を実施する場合は、
具体的には、第2図に示す如く各ダイス2,2の
間で引抜素材1にガス又は液体の冷媒3をスプレ
ーにて吹き付ける方法や、引抜素材全体を冷却液
中に浸漬する方法等が採用できる。この場合、引
抜時に潤滑効果を発揮する冷却液を適用すると更
に好都合である。 ところで、従来、“直接冷却伸線法”と称され
るところの、ダイスを出た直後の材料を冷媒によ
つて直接冷却する方法が知られているが、これは
高炭素鋼線等で伸線温度による静的歪時効を抑制
するために適用されるものである。一方、加工誘
起変態はダイス内に材料があるうちに終了するた
め、直接冷却伸線法の場合のようにダイスを出た
後で準安定オーステナイト鋼素材を冷却しても無
意味であり、ダイス入口における温度を低下させ
ることが重要な課題となる。従つて、本発明法に
おいては最終ダイスの出口では強制冷却を行う必
要はない。 次に、この発明を実施例によつて具体的に説明
する。 <実施例> 実施例 1 まず、C:0.05%、Si:0.50%、Mn:1.40%、
Ni:6.81%、N:0.02%を含むと共に残部が実質
的にFeより成る準安定オーステナイト鋼を熱間
圧延により27mmφの棒材とし、これを1100℃に2
時間均熱して溶体化処理した後、その表面をピー
リングして25mmφの引抜素材棒とした。 次いで、これに弗素系樹脂皮膜処理を施して潤
滑下地皮膜とし、これを種々の条件で21.6mmφに
引抜いた。そして、引抜後の棒材を2ロール型の
回転曲げ矯正機に通し、真直度0.3〜0.5mm/mの
直棒を得た。 引抜条件は、第1表に示すように、引抜ダイス
を1〜4個とした1パス引抜又は多重ダイス引抜
で、中間冷却は自然放冷又は強制空冷、そして引
抜速度は最終ダイス出口で0.5m/分と設定した。
なお、各ダイス出口の材料温度は熱電対式接触温
度計で測定した。 このようにして得られた直棒から10mmφの試験
片を切り出し、直流磁化特性を測定して強磁性化
の尺度としての飽和磁束密度[Bs]を求めて、
その結果を第1表に併せて示した。 なお、強磁性化の評価に際しては、前述の磁気
目盛における位置検出精度が飽和磁束密度[Bs]
によつて支配され、「Bs≧5KG」で実用的な精度
を達成できることが本発明者等の別の研究により
判明しているので、それを評価の基準とした。 第1表に示される結果からも明らかなように、
1パス引抜では十分な強磁性化が達成できず、パ
ス回数を多くするほど良好な結果を得られること
が分かる。 また、第1表からは、強制空冷手段を適用した
場合には3〜8℃の冷却効果が認められ全体的に
は温度は下がつたものの、最終パスではむしろ1
<Industrial Application Field> The present invention is capable of sufficiently suppressing deformation-induced transformation even at a low drawing area reduction rate in order to economically and stably produce a ferromagnetized metastable austenitic steel bar suitable as a magnetic scale material, etc. The present invention relates to a method for drawing metastable austenitic steel that promotes . In recent years, the use of "magnetic scales" has become more prominent for measuring the amount of displacement, displacement speed, etc. of piston rods, etc. A "magnetic scale" is a scale formed by regularly arranging linear or band-shaped magnetically altered parts on the surface of a base made of a metal material, etc., and a magnetic scale placed close to and facing the surface of the scale. The sensor measures the relative displacement between the base and the magnetic sensor by reading the scale. <Prior Art and its Problems> As a conventional "magnetic scale" of this kind, one is known in which air gap grooves are carved out in a base made of a ferromagnetic material and the air gap grooves are utilized as magnetically altered parts. However, although the "magnetic scale" manufactured in this way had good magnetic scale characteristics and could obtain high output, its structure made it difficult to use it for sliding shafts such as piston rods and guide shafts. The problem was that the grooves had to be filled, making it impractical due to manufacturing costs and mechanical strength. In addition, as seen in Japanese Patent Application Laid-Open No. 57-16309, "magnetic A method of manufacturing "scale scales" was also proposed, but although the manufacturing method itself is simple, in this case, only a product with a small difference in magnetic properties between the base material (base part) and the heat-treated part can be obtained, and it is difficult to use. However, there are problems in that an expensive detection device is required or the reliability of the product is not sufficient. However, the above proposal also mentions measures to improve magnetic properties, and the 25%
Examples have been given of applying very expensive magnetic materials such as Fe-75%Ni alloy, but the products obtained in this way are not only expensive but also have poor strength and wear resistance. Not only that, but there are many limitations in terms of use, and the magnetic properties are also far from perfect. In other words, in the case of a "magnetic scale," it has already been mentioned that theoretically, by forming an air gap groove, the maximum magnetic output can be obtained at that part. Therefore, the above statement indicates that ``a combination of ferromagnetic material and non-magnetic material is the best magnetic scale.'' However, in the "magnetic scale" using the Fe-Ni alloy proposed above, both the base material (base part) and the heat-treated part are ferromagnetic, and the scale is formed simply by the difference in magnetic permeability between them. Therefore, it cannot necessarily be said that it is an ideal product in terms of magnetic properties. Furthermore, apart from these, a thin film (0.2~
We have also proposed a "magnetic scale" in which a thin film (0.3 mm thick) is formed as a base, and magnetically altered parts are created at predetermined intervals in a thin film on the base by partial electrical heating or heating with a particle beam such as a laser. (Unexamined Japanese Patent Publication No. 1983-
No. 7517). However, in the above-mentioned "thin plating film mainly composed of Ni and P that is partially heat-treated to form altered areas," the S/N ratio is said to be poor because the reading sensitivity of the scale is relatively low. However, in order to increase the sensitivity, the thickness of the thin film must be considerably thickened, which is an economic disadvantage, and if the surface of the magnetic scale is required to have wear resistance, it is necessary to use chrome plating, etc. There was a problem in that it was necessary to apply a wear-resistant coating, complicating the processing process, and there was also a risk that damage such as cracks would occur in the heat-treated plating thin film. Under these circumstances, the present inventors first
Most of the problems of the conventional method have been solved. proposed a magnetic scale characterized by an austenite structure. The above magnetic scale proposed by the present inventors is
It is a scale made by irradiating a base material made of metastable austenitic steel that has been cold-worked to become ferromagnetic to form localized non-magnetized areas, and has extremely good magnetic properties. However, in order to make the metastable austenitic steel ferromagnetic, a high degree of cold working is required, and therefore, manufacturing constraints are unavoidable, such as the need for large-scale drawing equipment. That is, there was no need to actively induce deformation-induced transformation in metastable austenitic steel to make it ferromagnetic, and thus such a drawing method had not been established in the past. This is because metastable austenitic steel has the property of becoming extremely hard due to the formation of a martensitic structure due to deformation-induced transformation, and problems such as "die seizure" and "wire breakage" are likely to occur during the drawing operation. Therefore, when drawing metastable austenitic steel materials for normal use, conventionally,
The main focus is on "suppressing deformation-induced transformation as much as possible," and generally speaking, as shown in Figure 3, "by drawing out the necessary area reduction in one pass in a warm process, deformation-induced transformation can be suppressed as much as possible.""Means to suppress and improve efficiency" were simply adopted. In addition, in FIG. 3, the reference numeral 1 indicates a drawing material, and the reference numeral 2 indicates a drawing die. <Means for Solving the Problems> In view of the above-mentioned circumstances, the present inventors have devised a method to achieve sufficient ferromagnetism by promoting deformation-induced transformation as much as possible, which was not previously intended. “Ferromagnetic drawing method for metastable austenitic steel”
In order to establish the Recognizing that this is not at all industrially desirable as it leads to the reinforcement of large drawing equipment and auxiliary equipment, which leads to a significant increase in costs and increases work troubles, we have developed As a result of repeated research in pursuit of the possibility of promoting deformation-induced transformation as much as possible while keeping the drawing area reduction rate as low as possible during drawing, we have found the following (a):
The findings shown in ~(d) were obtained. That is, (a) When obtaining a sufficiently ferromagnetic metastable austenitic steel drawn bar suitable as a material for magnetic scales by drawing, the inlet drawing temperature is suppressed to 140°C or less. need to be
There is no problem if the drawing temperature is kept particularly below 140°C, but if it exceeds that temperature, sufficient ferromagnetization will not be achieved. (b) However, in order to obtain a drawn rod product with the structure and strength required for equipment components, the required product can be obtained in one pass from a material with normal diameter dimensions (sufficient area reduction is expected). When drawing to the required dimensions, it is impossible to keep the drawing temperature of the metastable austenitic steel bar material below 140℃ due to processing heat, and problems such as die seizure and cutting of the material occur due to hardening due to transformation. becomes more likely to occur. (c) However, if the number of drawing passes is multiple during drawing to reduce the area reduction rate per pass, the rise in temperature of the material due to processing heat will be suppressed, and the inlet drawing temperature until the required diameter is finished will be kept below 140°C. At the same time, the strength of the finished product to the required diameter is sufficiently high, and troubles such as die seizure and cutting of the material can be stably prevented. In addition, at this time, if the heat dissipation of the material is slightly insufficient between each pass, the material temperature will increase with each pass, and in reality it will reach 140 degrees Celsius in the final pass.
However, even in that case, since the deformation-induced transformation is sufficiently promoted in the previous pass, ferromagnetization is sufficiently improved. (d) However, in order to increase the drawing efficiency and achieve sufficiently stable ferromagnetization, it is effective to forcefully cool the material between each pass. It is now possible to stably keep the drawing temperature below 140℃ without waiting for heat dissipation, and by arranging multiple drawing dies in a straight line, a single gripping device installed at the exit of the final die can handle all passes. It is also convenient for carrying out high-efficiency multiple die drawing, which involves simultaneously drawing out the dies. This invention was made based on the above knowledge, and it is based on the following: ``When drawing a metastable austenitic steel bar, by making a plurality of drawing passes and reducing the area reduction rate per pass, the drawing temperature in each pass can be reduced. of
Either perform cold drawing while maintaining the temperature at 140°C or less, or use multiple drawing passes to reduce the area reduction rate per pass, and forcefully cool the intermediate material before each pass to remove the drawing die immediately before it. By suppressing the temperature rise due to passage, the drawing temperature in each pass can be reduced.
Cold drawing is carried out while maintaining the temperature below 140℃, thereby actively causing deformation-induced transformation and improving the strength, resulting in a stable metastable austenitic steel bar with sufficiently high ferromagnetism and strength. It is characterized by the fact that it can be manufactured using The above “metastable austenitic steel” is
For example, when stainless steels such as SUS301 and SUS304 undergo solution treatment, they become completely austenitic and exhibit non-magnetic properties, but subsequent cold working causes strain-induced transformation, resulting in a martensitic structure that becomes ferromagnetic. However, when applied to the present invention, the type is not critical. This invention will be explained in more detail below. First, it is extremely important to use a plurality of drawing passes in the method of the present invention, but this is because it takes not "one pass" but "two passes" to achieve a predetermined area reduction rate to obtain a drawn product. Pass or better”
This means that the passes are divided into two, and as this reduces the heat generated during processing per pass, it is possible to sufficiently promote processing-induced transformation. By the way, when a large area reduction rate is required in general drawing processing, and it is impossible to draw the material in one pass due to breakage of the material or limitations on the capacity of the drawing machine, it is necessary to divide the material into multiple passes. This is a method that has been used in the past. However, multi-pass drawing in this case is carried out only from the perspective of "performing the drawing work without operational trouble", and is only adopted when it is impossible to perform the drawing work in one pass. It is a means of On the other hand, in the method of the present invention, we target metastable austenitic steel as the material to be drawn, and the area reduction rate that can be drawn in one pass is This is done from the perspective of "reducing the area reduction rate per pass in order to prevent the temperature from rising to the point where the process-induced transformation of the drawn material is inhibited," and the purpose of dividing the drawing pass into multiple passes is completely They are different. In other words, the purpose of dividing the passes in the method of the present invention is to lower the material temperature during drawing, and the drawing temperature can be significantly lowered by lowering the area reduction rate during drawing, thereby significantly promoting deformation-induced transformation. It will be done. Therefore, when carrying out the method of the present invention, 1
It is possible to increase the number of drawing dies on the drawing line, which is impossible with the above-mentioned ``multi-pass drawing'' from the conventional perspective, which requires drawing with a drawing device for each pass (one die). A method of arranging the dies in a straight line and pulling out the total area reduction in one drawing operation using one drawing device (referred to here as the ``multiple die method'').''
is also possible and sufficient.
Fig. 1 is a conceptual diagram of the above-mentioned "multiple die method", in which a plurality of drawing dies 2, 2,... are arranged in a straight line, and even in one drawing operation, the required area reduction rate is achieved all at once. This figure shows how the drawing material 1 is pulled out. Since this "multiple die method" can complete processing in one step, it is an extremely preferable method as it ensures superior productivity compared to conventional multi-pass drawing. However, if productivity is not emphasized, the conventional It goes without saying that the effect of promoting deformation-induced transformation can also be obtained by the multi-pass drawing method. In addition, previously published Japanese Patent Application Laid-open No. 58-221611 discloses a method that uses two dies and one drawing device and uses this to pull out the drawn material at once. This is done to ensure dimensional accuracy and pass center when inspecting the surface flaws of the material between dies, and it goes without saying that this is essentially different from the method of the present invention. Now, as mentioned above, in the method of the present invention, control of the inlet drawing temperature is extremely important, and plays a dominant role in determining the performance as a material for, for example, a magnetic scale. If the inlet drawing temperature exceeds 140°C, sufficient ferromagnetization of the drawn product cannot be achieved, and when applied to magnetic scales, the ferromagnetic properties are insufficient and a satisfactory product cannot be obtained. Therefore, it is necessary to set the number of drawing passes until the specified area reduction rate is reached so that the inlet drawing temperature does not exceed 140°C, or divide the number of passes to reduce the rise in drawing temperature, and then perform drawing at the die entrance. It is necessary to supplementally cool the material. However, especially when the multiple die method is applied, the temperature of the material increases with each pass due to insufficient cooling between the dies, and it is actually conceivable that the upper limit of 140°C may be exceeded in the final pass. As mentioned above, even in such a case, if measures such as the method of the present invention are basically taken, the deformation-induced transformation will be sufficiently promoted in the previous pass, and the magnetic properties will be sufficiently improved. For this reason, in practice, the desired purpose can be fully achieved by multiple passes in the air at room temperature, but if more powerful suppression of temperature rise is desired, a refrigerant below room temperature such as liquefied gas may be used. The material may be cooled at the die entrance before passing through the die. Forced cooling improves the ferromagnetic effect accordingly. When performing forced cooling using the multiple die method,
Specifically, as shown in FIG. 2, there are methods such as spraying a gas or liquid coolant 3 onto the drawn material 1 between the dies 2 and 2, or immersing the entire drawn material in a cooling liquid. Can be adopted. In this case, it is even more advantageous to apply a cooling liquid that exhibits a lubricating effect during drawing. By the way, a method known as the "direct cooling wire drawing method" in which the material immediately after exiting the die is directly cooled with a refrigerant is known, but this method involves drawing with high carbon steel wire, etc. This is applied to suppress static strain aging due to line temperature. On the other hand, since the deformation-induced transformation ends while the material remains in the die, it is meaningless to cool the metastable austenitic steel material after it leaves the die, as in the case of the direct cooling wire drawing method. Reducing the temperature at the inlet is an important issue. Therefore, in the method of the present invention, there is no need to perform forced cooling at the exit of the final die. Next, the present invention will be specifically explained using examples. <Example> Example 1 First, C: 0.05%, Si: 0.50%, Mn: 1.40%,
A metastable austenitic steel containing 6.81% Ni, 0.02% N, and the remainder substantially Fe was hot rolled into a 27mmφ bar, and heated to 1100℃ for 2 hours.
After soaking and solution treatment for a period of time, the surface was peeled to obtain a drawn material rod of 25 mmφ. Next, this was subjected to a fluorine-based resin film treatment to form a lubricating base film, and this was drawn out to a diameter of 21.6 mm under various conditions. Then, the drawn bar was passed through a two-roll rotary bend straightening machine to obtain a straight bar with a straightness of 0.3 to 0.5 mm/m. As shown in Table 1, the drawing conditions are one-pass drawing or multi-die drawing using 1 to 4 drawing dies, intermediate cooling is natural cooling or forced air cooling, and the drawing speed is 0.5 m at the final die exit. / minute.
In addition, the material temperature at the exit of each die was measured with a thermocouple type contact thermometer. A test piece of 10 mmφ was cut out from the straight bar obtained in this way, and its DC magnetization characteristics were measured to determine the saturation magnetic flux density [Bs] as a measure of ferromagnetization.
The results are also shown in Table 1. In addition, when evaluating ferromagnetization, the position detection accuracy on the magnetic scale mentioned above is determined by the saturation magnetic flux density [Bs]
Another study by the present inventors has revealed that practical accuracy can be achieved with "Bs≧5KG", and this was used as the standard for evaluation. As is clear from the results shown in Table 1,
It can be seen that sufficient ferromagnetism cannot be achieved with one-pass drawing, and that the more passes the number of passes yields better results. Also, from Table 1, when forced air cooling was applied, a cooling effect of 3 to 8 degrees Celsius was observed and the temperature decreased overall, but in the final pass it was rather

【表】【table】

【表】 パスの場合よりも温度が高くなることが明らかと
なつたが、それ以前のパスでの低温が効果を発揮
し、飽和磁束密度[Bs]の向上効果が自然放冷
の場合よりも目立つことが分かる。 実施例 2 まず、実施例1と同じ成分の材料を用い、実施
例1と同じ工程により20.5mmφの引抜素材棒材を
得た。 次いで、これを第2表の条件にて引抜いて直径
が18mmφの棒材とし、更に回転曲げ矯正機にて真
直度が0.3〜0.5mm/mの直棒としたが、この時の
ダイス間における素材の冷却は水スプレー法で実
施し、その他の引抜条件並びに矯正条件は実施例
1の場合と同じにした。 このようにして得られた直棒から10mmφの試験
片を切り出し、直流磁化特性を測定して強磁性化
の尺度としての飽和磁束密度[Bs]を求めて、
その結果を第2表に併せて示した。 この例では、冷却が十分であるので引抜の温度
はかなり低下し、全パスとも140℃以下となつた
が、このため、第2表に示される結果から明らか
な如く十分な磁気特性の向上効果が得られた。 <効果の総括> 以上に説明した如く、この発明によれば、格別
な高能力設備等を必要とすることなく十分に強磁
性化された準安定オーステナイト鋼引抜棒材を安
定して提供することができ、磁気目盛等の素材に
適用して優れた性能の製品をコスト易く得ること
が可能となるなど、産業上有用な効果がもたらさ
れるのである。
[Table] It is clear that the temperature is higher than in the case of a pass, but the low temperature in the previous pass is effective, and the effect of improving the saturation magnetic flux density [Bs] is greater than in the case of natural cooling. I know it's noticeable. Example 2 First, a drawn material bar with a diameter of 20.5 mm was obtained using the same materials as in Example 1 and the same steps as in Example 1. Next, this was drawn out under the conditions shown in Table 2 to make a bar with a diameter of 18 mmφ, and then a straight bar with a straightness of 0.3 to 0.5 mm/m was made using a rotary bend straightening machine. The material was cooled by a water spray method, and other drawing conditions and straightening conditions were the same as in Example 1. A test piece of 10 mmφ was cut out from the straight bar obtained in this way, and its DC magnetization characteristics were measured to determine the saturation magnetic flux density [Bs] as a measure of ferromagnetization.
The results are also shown in Table 2. In this example, since the cooling was sufficient, the drawing temperature was considerably lower and was below 140°C for all passes, which resulted in a sufficient improvement in magnetic properties as is clear from the results shown in Table 2. was gotten. <Summary of Effects> As explained above, according to the present invention, it is possible to stably provide a metastable austenitic steel drawn bar material that is sufficiently ferromagnetic without requiring special high-capacity equipment. This brings about industrially useful effects, such as making it possible to obtain products with excellent performance at low cost by applying it to materials such as magnetic scales.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本発明に係る多重ダイス法を示す概
念図である。第2図は、本発明に係る冷却手段を
併用した多重ダイス法を示す概念図である。第3
図は、従来の棒材引抜手段である1パス引抜法を
示す概念図である。 図面において、1…引抜素材、2…引抜ダイ
ス、3…冷媒。
FIG. 1 is a conceptual diagram showing the multiple dice method according to the present invention. FIG. 2 is a conceptual diagram showing a multiple die method using a cooling means according to the present invention. Third
The figure is a conceptual diagram showing a one-pass drawing method, which is a conventional bar drawing method. In the drawings, 1... Drawing material, 2... Drawing die, 3... Refrigerant.

Claims (1)

【特許請求の範囲】 1 準安定オーステナイト鋼棒を引抜加工するに
際し、引抜パス数を複数として1パス当りの減面
率を小さくすることで各パスにおける入口引抜温
度を140℃以下に維持しつつ冷間引抜を行い、こ
れによつて加工誘起変態を積極的に生ぜしめると
共に強度の向上を図ることを特徴とする、準安定
オーステナイト鋼棒の強磁性化引抜方法。 2 複数の引抜ダイスを直線上に配置して全パス
の引抜を1回の引抜動作により終了する、特許請
求の範囲第1項に記載の準安定オーステナイト鋼
棒の強磁性化引抜方法。 3 準安定オーステナイト鋼棒を引抜加工するに
際し、引抜パス数を複数として1パス当りの減面
率を小さくすると共に、各パス通過前の中間素材
を強制冷却してその直前の引抜ダイス通過による
温度上昇を抑えることで各パスにおける入口引抜
温度を140℃以下に維持しつつ冷間引抜を行い、
これによつて加工誘起変態を積極的に生ぜしめる
と共に強度の向上を図ることを特徴とする、準安
定オーステナイト鋼棒の強磁性化引抜方法。 4 複数の引抜ダイスを直線上に配置して全パス
の引抜を1回の引抜動作により終了する、特許請
求の範囲第3項に記載の準安定オーステナイト鋼
棒の強磁性化引抜方法。
[Claims] 1. When drawing a metastable austenitic steel bar, a plurality of drawing passes are performed to reduce the area reduction rate per pass, thereby maintaining the inlet drawing temperature at 140°C or less in each pass. A method of drawing a metastable austenitic steel bar to make it ferromagnetic, which is characterized by performing cold drawing to actively cause deformation-induced transformation and to improve its strength. 2. The method for ferromagnetizing a metastable austenitic steel bar according to claim 1, wherein a plurality of drawing dies are arranged in a straight line and all passes of drawing are completed in one drawing operation. 3. When drawing a metastable austenitic steel bar, the number of drawing passes is made to reduce the area reduction rate per pass, and the intermediate material before passing through each pass is forcibly cooled to reduce the temperature caused by passing through the drawing die immediately before that. By suppressing the rise, cold drawing is performed while maintaining the inlet drawing temperature in each pass below 140℃,
A method for drawing a metastable austenitic steel bar to make it ferromagnetic, which is characterized by actively causing deformation-induced transformation and improving its strength. 4. The method for ferromagnetizing a metastable austenitic steel bar according to claim 3, wherein a plurality of drawing dies are arranged in a straight line and all passes of drawing are completed in one drawing operation.
JP17905487A 1987-07-20 1987-07-20 Method for ferromagnetic drawing metastable austenitic steel bar Granted JPS6422412A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17905487A JPS6422412A (en) 1987-07-20 1987-07-20 Method for ferromagnetic drawing metastable austenitic steel bar

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17905487A JPS6422412A (en) 1987-07-20 1987-07-20 Method for ferromagnetic drawing metastable austenitic steel bar

Publications (2)

Publication Number Publication Date
JPS6422412A JPS6422412A (en) 1989-01-25
JPH0527490B2 true JPH0527490B2 (en) 1993-04-21

Family

ID=16059310

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JPS6422412A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03104821A (en) * 1989-09-14 1991-05-01 Nippon Steel Corp Production of extra fine steel wire having high strength and high ductility
JP3311427B2 (en) * 1993-06-18 2002-08-05 株式会社デンソー Composite magnetic member, method for producing the same, and solenoid valve using the composite magnetic member
GB201103675D0 (en) 2011-03-03 2011-04-20 Rls Merlina Tehnika D O O Method of scale substrate manufacture

Also Published As

Publication number Publication date
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