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JPH0676894B2 - Magnetic scale - Google Patents
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JPH0676894B2 - Magnetic scale - Google Patents

Magnetic scale

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Publication number
JPH0676894B2
JPH0676894B2 JP60181366A JP18136685A JPH0676894B2 JP H0676894 B2 JPH0676894 B2 JP H0676894B2 JP 60181366 A JP60181366 A JP 60181366A JP 18136685 A JP18136685 A JP 18136685A JP H0676894 B2 JPH0676894 B2 JP H0676894B2
Authority
JP
Japan
Prior art keywords
base material
magnetic
thin film
plating
magnetic scale
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
JP60181366A
Other languages
Japanese (ja)
Other versions
JPS6242003A (en
Inventor
弘洋 中村
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.)
Shibaura Machine Co Ltd
Original Assignee
Toshiba Machine 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 Toshiba Machine Co Ltd filed Critical Toshiba Machine Co Ltd
Priority to JP60181366A priority Critical patent/JPH0676894B2/en
Publication of JPS6242003A publication Critical patent/JPS6242003A/en
Publication of JPH0676894B2 publication Critical patent/JPH0676894B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

Description

【発明の詳細な説明】 〔発明の属する技術分野〕 本発明は磁気スケールに関する。Description: TECHNICAL FIELD The present invention relates to a magnetic scale.

〔従来技術〕[Prior art]

磁気スケールは工業において広く使用されているが従来
の一例は、強磁性の母材に巾が1ないし2mmで深さが0.2
ないし0.3mmの溝を機械加工により等間隔に設け、この
溝を非磁性であるクローム等のメッキにより埋めてい
た。ここでメッキの厚さは通常0.02mm程度であり溝にメ
ッキをすると溝の側面と母材外面との接点である角部に
ヒゲが発生し、このヒゲは次にメッキをするとき邪魔に
なるためバフにより取除いていた。溝の深さを0.2mmと
するとこの煩雑なメッキ処理を10回くり返へすことにな
り多大な時間を必要としてコストを高くしていた。
Magnetic scales are widely used in industry, but one conventional example is a ferromagnetic base material with a width of 1-2 mm and a depth of 0.2 mm.
Or, grooves of 0.3 mm were provided at equal intervals by machining, and these grooves were filled with nonmagnetic chrome or the like. Here, the plating thickness is usually about 0.02 mm, and when plating the groove, a beard is generated at the corner that is the contact point between the side surface of the groove and the outer surface of the base material, and this beard interferes with the next plating. Therefore, it was removed by a buff. If the groove depth is 0.2 mm, this complicated plating process is repeated 10 times, which requires a lot of time and raises the cost.

他の従来例として非磁性の母材をリンを含むニッケルに
よりメッキし、表面のメッキ層を等間隔でレーザ光を照
射し約300℃に加熱することによりニッケルを強磁性に
変える方式がある。この方式は母材の表面を全部メッキ
するため第1の従来例のようなメッキの手間はないもの
の、メッキ層の厚さは層の密着性と生産性等から0.2mm
が限度である。一方、磁気スケールの検出器から発生す
る電気出力は上記メッキ層の厚さに比例するため電気出
力を大幅に増大させることは不可能である。さらに、こ
れらの方式はメッキ層の一部を加熱することにより強磁
性にしているため、磁気スケールが摩擦熱を受けたり機
械の故障等より磁気スケールが加熱されると特性、特に
電気出力が低下し、特に300℃付近になると使用不可能
になって、使用範囲が限定される欠点があった。
As another conventional example, there is a method in which a non-magnetic base material is plated with nickel containing phosphorus and the surface plated layer is irradiated with laser light at equal intervals and heated to about 300 ° C. to change nickel into ferromagnetic. With this method, the entire surface of the base material is plated, so there is no need for plating as in the first conventional example, but the thickness of the plated layer is 0.2 mm due to the adhesion of the layer and productivity.
Is the limit. On the other hand, since the electric output generated from the detector of the magnetic scale is proportional to the thickness of the plating layer, it is impossible to greatly increase the electric output. Furthermore, in these methods, part of the plating layer is heated to make it ferromagnetic, so if the magnetic scale is heated due to frictional heat or mechanical failure, the characteristics, especially the electrical output, will decrease. However, there is a drawback that it becomes unusable especially near 300 ° C. and the range of use is limited.

〔発明の目的〕[Object of the Invention]

本発明はこのような欠点を除去したものでその目的は、
コストが低くかつ検出器の電気出力が大きくさらに耐熱
性があって使用範囲の広い磁気スケールを提供すること
にある。
The present invention eliminates such drawbacks and its purpose is to
An object of the present invention is to provide a magnetic scale that is low in cost, has a large electric output of a detector, is more heat resistant, and has a wide range of use.

〔発明の要点〕[Main points of the invention]

本発明の磁気スケールは、鋼材で透磁率2000程度を有す
る母材の表面にニッケルメッキまたはクロームメッキあ
るいはニッケル、クローム、マンガン、炭素を含む合金
の溶射により薄膜を形成し、同薄膜の外周に所定の間隔
を保持してレーザ光線の照射あるいはアーク放電により
該薄膜および前記母材を加熱し短時間内に溶融して固化
させ、前記母材の表層部に規則的に配置され半月形ある
いはU字形の断面を有する非磁性の変質部を設けるよう
にしたことを特徴とする。
The magnetic scale of the present invention has a thin film formed on a surface of a base material having a magnetic permeability of about 2000 by nickel plating or chrome plating or thermal spraying of an alloy containing nickel, chrome, manganese, and carbon, and a predetermined outer periphery of the thin film. The thin film and the base material are heated and melted and solidified within a short time by irradiating a laser beam or arc discharge while maintaining the interval of the half-moon shape or U-shape which is regularly arranged on the surface layer part of the base material. It is characterized in that a non-magnetic alteration portion having a cross section of 1 is provided.

〔発明の実施例〕Example of Invention

以下本発明の一実施例を示した第1図および第2図につ
いて説明する。第1図において円柱形でかつ強磁性(透
磁率2000程度)を有する母材11の表面に、ニッケルがク
ロム或いはマンガンや炭素等の薄膜12をメッキ或いは溶
射等により形成する。この薄膜12を外方からレーザ光線
13を照射することにより母材11と薄膜12の一部を加熱し
て溶解させ、薄膜12を構成している金属と母材11とを構
成している金属とを融合させると半月形あるいはU字形
の断面を有する非磁性(透磁率2程度)の変質部14Aが
作られる。このとき母材11を回転させると変質部14Aは
リング状の変質部14になり、さらにレーザ光線13を軸方
向に所定間隔を置いて照射すれば、母材11には複数のリ
ング状変質部14が形成される。
1 and 2 showing one embodiment of the present invention will be described below. In FIG. 1, a thin film 12 made of nickel such as chromium or manganese or carbon is formed by plating or thermal spraying on the surface of a base material 11 having a cylindrical shape and having a ferromagnetic property (permeability of about 2000). This thin film 12 is laser beam from the outside.
When the base material 11 and a part of the thin film 12 are heated and melted by irradiating 13, the metal forming the thin film 12 and the metal forming the base material 11 are fused to form a half-moon shape or a U shape. A non-magnetic (permeability of about 2) altered portion 14A having a V-shaped cross section is formed. At this time, when the base material 11 is rotated, the altered portion 14A becomes a ring-shaped altered portion 14, and if the laser beam 13 is further irradiated at predetermined intervals in the axial direction, the base material 11 has a plurality of ring-like altered portions. 14 are formed.

このように非磁性の変質部14を構成させるためには変質
部14に含まれる金属を、ジエフラーの組織状態図に示さ
れるような安定なオーステナイト組織の領域成分にすれ
ばよい。従って母材11が特にニッケルやクロム或いはマ
ンガン等を多量に含有しているときは薄膜12の金属成分
を母材11の成分に対応して選択することが好ましい。
In order to form the non-magnetic altered portion 14 in this manner, the metal contained in the altered portion 14 may be made to be a region component of a stable austenite structure as shown in the diagram of the structure of the Jeefler. Therefore, when the base material 11 contains a large amount of nickel, chromium, manganese, or the like, it is preferable to select the metal component of the thin film 12 corresponding to the component of the base material 11.

次いで母材11の外周の薄膜12を研削等により除去した形
状が第2図であって、磁気スケール16は強磁性の母材11
のままの表層間部11Aと非磁性の変質部14とが交互にそ
の巾とピッチとを同一にして並んでいる。この磁気スケ
ール16に近接して検出器21を設置しこれを図において左
右方向に移動させると、検出器21は表層間部11Aの強磁
性と変質部14の非磁性とを検出し、表層間部11Aと変質
部14とに対応した電気信号、即ち左右方向の変位量に対
応した電気信号を発することにより変位量を測定する。
Next, the shape in which the thin film 12 on the outer periphery of the base material 11 is removed by grinding or the like is shown in FIG.
The surface layer portions 11A and the non-magnetic alteration portions 14 are arranged alternately with the same width and pitch. When the detector 21 is installed close to the magnetic scale 16 and moved in the horizontal direction in the figure, the detector 21 detects the ferromagnetism of the surface layer 11A and the non-magnetism of the altered layer 14, and The displacement amount is measured by emitting an electric signal corresponding to the portion 11A and the altered portion 14, that is, an electric signal corresponding to the displacement amount in the left-right direction.

上記した検出器21の細部一例を第3図ないし第5図によ
り説明する。検出器21の本体22内部には表層間部11Aと
変質部14とのピッチに対し同一間隔のU字形の永久磁石
23が挿入されており、永久磁石23の両端面と本体22の表
面との間には僅かな長さの磁気抵抗素子(以下単に素子
という)24が2個設けてある。この素子24は電気抵抗体
の一種でここを貫通する磁力線の数に比例して電気抵抗
の増大する性質を有している。
An example of the details of the detector 21 will be described with reference to FIGS. Inside the main body 22 of the detector 21, a U-shaped permanent magnet is arranged at the same intervals with respect to the pitch between the surface layer 11A and the altered portion 14.
23 is inserted, and two magnetoresistive elements (hereinafter simply referred to as elements) 24 having a slight length are provided between both end surfaces of the permanent magnet 23 and the surface of the main body 22. This element 24 is a kind of electric resistor and has a property that the electric resistance increases in proportion to the number of magnetic lines of force passing through the element.

従って第3図に示すように両素子24の直前に強磁性であ
って透磁率の高い表層間部11Aがあると、永久磁石23の
磁力線はコース26を通り両素子24に多くの磁力線が通る
ためその抵抗値は増大する。他方第4図に示すように両
素子24の直前に非磁性であって透磁率の低い変質部14が
あると永久磁石23の磁力線はコース27を通り両素子24に
はほとんど磁力線が通らないため抵抗値は小さい。
Therefore, as shown in FIG. 3, when there is a surface layer portion 11A that is ferromagnetic and has a high magnetic permeability immediately before both elements 24, many magnetic force lines of the permanent magnet 23 pass through the course 26 and both element 24 pass. Therefore, the resistance value increases. On the other hand, as shown in FIG. 4, if there is a non-magnetic and low-permeability altered portion 14 immediately in front of both elements 24, the magnetic lines of force of the permanent magnet 23 pass through the course 27 and almost no magnetic lines of force pass through both elements 24. The resistance value is small.

第5図に示すように2個の素子24を抵抗体28と共に直列
に電源29に接続すると、2個の素子24間の電圧Eは素子
24の抵抗が大きいときは高く抵抗の小さいときは低くな
る。従って磁気スケール16と検出器21との間の相対変位
量に対応して検出器21の出力電圧Eが変化し、これを不
図示の電気演算器により換算すれば相対変位量や相対速
度そして相対加速度は測定される。
As shown in FIG. 5, when the two elements 24 are connected in series with the resistor 28 to the power supply 29, the voltage E between the two elements 24 is
When 24 resistance is high, it is high, and when resistance is low, it is low. Therefore, the output voltage E of the detector 21 changes corresponding to the relative displacement amount between the magnetic scale 16 and the detector 21, and if this is converted by an electric calculator (not shown), the relative displacement amount, relative velocity and relative Acceleration is measured.

実施例1. 母材11として鋼材(SUS420J2)の表面に0.03mmのニッケ
ルメッキを行って薄膜12を形成した後、母材11を2m/分
の速度で回転させながら出力1.6kW、ビーム径1.3mmの炭
酸ガスレーザを照射し、次いで薄膜12を除去して第2図
に示す磁気スケール16にした図の変質部14の寸法Aおよ
びBはそれぞれ1mmと0.3mmであった。この場合鋼材(SU
S420J2)にはクロームが13ωt%と多量に含まれている
ため薄膜12は単なるニッケルメッキで充分目的は達成さ
れた。
Example 1. After forming a thin film 12 by plating 0.03 mm of nickel on the surface of a steel material (SUS420J2) as a base material 11, an output of 1.6 kW and a beam diameter of 1.3 while rotating the base material 11 at a speed of 2 m / min. The thin film 12 was irradiated with a carbon dioxide laser of mm, and the thin film 12 was removed to obtain the magnetic scale 16 shown in FIG. In this case steel (SU
Since S420J2) contains a large amount of chrome (13 ωt%), the thin film 12 was achieved by simple nickel plating.

実施例2 磁気スケール31は母材32として鋼材(S48C)の表面に厚
さ0.03mmのニッケルメッキと厚さ0.02mmのクロームメッ
キとの複層メッキにより薄膜33を形成し、母材32を2m/
分の速度で回転させながら出力2kW、ビーム径1.3mmの炭
酸ガスレーザを照射しさらに薄膜33を除去した。変質部
34の寸法は実施例1と同様1mmと0.3mmであった。
Example 2 In the magnetic scale 31, as a base material 32, a thin film 33 was formed on the surface of a steel material (S48C) by multi-layer plating of 0.03 mm thick nickel plating and 0.02 mm thick chrome plating. /
While rotating at a speed of a minute, a carbon dioxide gas laser with an output of 2 kW and a beam diameter of 1.3 mm was irradiated to further remove the thin film 33. Alteration part
The dimensions of 34 were 1 mm and 0.3 mm as in Example 1.

実施例3 この例は表面に高い耐摩耗性を要求される磁気スケール
で磁気スケールそのものが機械部品になる場合である。
第6図に示すように磁気スケール36は、母材32として鋼
材(S48C)の表面にニッケル65ωt%%・クローム20ω
t%・硅素10ωt%・ボロン5ωt%の自溶合金を溶射
により厚さを0.2mmとして焼付けて薄膜37とし、次いで
母材32を15m/分の速度で回転させながら出力2kWビーム
径1.3mmの炭酸ガスレーザで照射した後外周の薄膜37を
0.01mm残して研削する。この場合変質部38の寸法Xおよ
びYはそれぞれ1mmと0.5mmであった。
Example 3 In this example, the magnetic scale itself is a mechanical part, which requires high wear resistance on the surface.
As shown in FIG. 6, in the magnetic scale 36, as the base material 32, 65 ωt %% of nickel and 20 ω of chrome was formed on the surface of steel (S48C).
A self-fluxing alloy of t%, silicon 10ωt% and boron 5ωt% is baked by thermal spraying to a thickness of 0.2 mm to form a thin film 37, and then the base material 32 is rotated at a speed of 15 m / min and an output of 2 kW beam diameter of 1.3 mm After irradiating with carbon dioxide laser, thin film 37 on the outer periphery
Grind with leaving 0.01 mm. In this case, the dimensions X and Y of the altered portion 38 were 1 mm and 0.5 mm, respectively.

実施例4 この例は実施例2に示した磁気スケール31をダイカスト
機に使用したものでその一例を第7図および第8図に示
す。固定ダイプレート41に固着された固定金型42と不図
示の移動ダイプレートに固着された移動金型43との対向
面にはキャビティ44が形成されており、固定ダイプレー
ト41と固定金型42とにはバレル45が取付けられている。
バレル45内に注入された溶融金属46はプランジャ47の前
進(左進)によりキャビティ44へ圧入されて成形品にな
る。
Example 4 In this example, the magnetic scale 31 shown in Example 2 was used in a die casting machine, and one example thereof is shown in FIGS. 7 and 8. A cavity 44 is formed on the facing surface of the fixed die 42 fixed to the fixed die plate 41 and the movable die 43 fixed to the moving die plate (not shown), and the fixed die plate 41 and the fixed die 42 are formed. Barrel 45 is attached to and.
The molten metal 46 injected into the barrel 45 is pressed into the cavity 44 by the forward movement (leftward movement) of the plunger 47 to become a molded product.

ここで高品位の成形品を得るためには溶融金属46のキャ
ビティ44への圧入状態即ちプランジャ47の移動を制御す
る必要がある。このためプランジャ47を移動させる油圧
シリンダ48のピストンロッド49にこれと一体の磁気スケ
ール31を設ける。なお51は油圧シリンダ48を固定ダイプ
レート41を固着するための枠であり、52はプランジャ47
とピストンロッド49を連結するためのカップリングであ
り53は油圧シリンダ48の一側のフタである。
Here, in order to obtain a high-quality molded product, it is necessary to control the press-fitting state of the molten metal 46 into the cavity 44, that is, the movement of the plunger 47. Therefore, the piston rod 49 of the hydraulic cylinder 48 for moving the plunger 47 is provided with the magnetic scale 31 integral with the piston rod 49. Reference numeral 51 is a frame for fixing the hydraulic cylinder 48 to the fixed die plate 41, and 52 is a plunger 47.
Is a coupling for connecting the piston rod 49 with the piston rod 49, and 53 is a lid on one side of the hydraulic cylinder 48.

このような構成において、プランジャ47従ってピストン
ロッド49の移動は検出器21を介して検出され、その出力
信号は不図示の制御装置に送られることによりプランジ
ャ47の移動は制御される。この場合プランジャ47の移動
速度は2ないし3m/秒にもおよびかつ溶融金属46がキャ
ビティ44への圧入完了時にはプランジャ47は急速に停止
させられそのときの減加速度は50Gにも達する。
In such a configuration, the movement of the plunger 47, that is, the piston rod 49 is detected via the detector 21, and the output signal thereof is sent to a control device (not shown) to control the movement of the plunger 47. In this case, the moving speed of the plunger 47 is as high as 2 to 3 m / sec, and when the molten metal 46 is completely pressed into the cavity 44, the plunger 47 is rapidly stopped and the deceleration at that time reaches 50 G.

なお前述の説明では変質部はリング状であるが母材を板
のような平面状にしてその表面に線状の変質部にするこ
とは可能である。また前述の説明では変質部の巾はいづ
れも1mmであったが、レーザ光線のビーム径を変更する
ことにより使用目的で従って大きくしたり小さくするこ
とも可能である。さらに変質部と表層間部とは一定間隔
に並べたものを説明したがこれをバーコード状にするこ
とにより位置検出をすることも可能である。
In the above description, the altered portion has a ring shape, but it is possible to form the base material into a flat surface such as a plate to form a linear altered portion on the surface. Further, in the above description, the width of the altered portion was 1 mm in each case, but it can be increased or decreased according to the purpose of use by changing the beam diameter of the laser beam. Further, although the altered portion and the surface layer portion are described as being arranged at a constant interval, the position can be detected by forming the altered portion and the surface layer portion into a bar code shape.

実施例5 前述した第1ないし第3実施例において変質部のための
熱源はレーザ光線であったが、この例では溶接部の溶け
込み深さが特に大きい正極性のイナートガスタングステ
ンアーク溶接装置(以下TIGという)を使用する。第9
図に示すように強磁性の母材61とニッケルメッキ等の薄
膜62とを陽極としトーチ63の電極64を陰極として両極の
間でアーク放電を行わせると、薄膜62と母材61の一部は
溶解して前述の他の実施例と同様に非磁性の変質部65が
形成される。この場合TIGは大量の熱エネルギを集中的
に供給するため、変質部65の寸法WおよびGはそれぞれ
2ないし3mmと1.5ないし2mmの大きな数値になる。そし
てこの母材61と変質部65とは外周を研削して薄膜62を除
去すれば磁気スケール(図示せず)になる。
Embodiment 5 In the first to third embodiments described above, the heat source for the altered portion was a laser beam, but in this example, a positive inert gas tungsten arc welding device (hereinafter TIG) having a particularly large weld penetration depth. Is used). 9th
As shown in the figure, when the ferromagnetic base material 61 and the thin film 62 such as nickel plating are used as an anode and the electrode 64 of the torch 63 is used as a cathode to perform arc discharge between the two electrodes, the thin film 62 and a part of the base material 61 are formed. Is dissolved to form a non-magnetic altered portion 65 as in the other embodiments described above. In this case, since the TIG supplies a large amount of heat energy in a concentrated manner, the dimensions W and G of the altered portion 65 are large values of 2 to 3 mm and 1.5 to 2 mm, respectively. The base material 61 and the altered portion 65 become a magnetic scale (not shown) by grinding the outer periphery and removing the thin film 62.

上述した実施例5は大型の磁気スケールとか第10図に示
す位置決め装置に好適である。第9図において磁気スケ
ール71に近接して非磁性を検出する例えばリードスイッ
チのような検出器72を支持体73に取付け、磁気スケール
71或いは検出器72の何れかを矢印74方向に移動させると
両者に相対的変位が生じ、変質部65が検出器72に対向す
ると検出器72からは電気信号が発せられることにより位
置は測定される。このようにこの例では磁気スケール71
は機械装置部品の平面或いは円筒面等に容易に設けるこ
とが可能であり、従来のようにリミットスイッチとドッ
グとによる方式と比較して位置決め装置を小型にするこ
とが可能である。
The fifth embodiment described above is suitable for a large magnetic scale or the positioning device shown in FIG. In FIG. 9, a detector 72 such as a reed switch, which detects non-magnetism in the vicinity of the magnetic scale 71, is attached to the support body 73.
When either 71 or the detector 72 is moved in the direction of the arrow 74, relative displacement occurs between the two, and when the altered portion 65 faces the detector 72, an electric signal is emitted from the detector 72 to measure the position. It Thus, in this example, the magnetic scale 71
Can be easily provided on a flat surface or a cylindrical surface of a machine device component, and the positioning device can be downsized as compared with the conventional method using a limit switch and a dog.

〔発明の効果〕〔The invention's effect〕

本発明の磁気スケールは以上説明したように、従来は強
磁性の母材に機械加工により多数の溝等を設けこの溝等
に非磁性のメッキを施し、メッキの際発生するヒゲを取
り除くことならびにメッキ回数が多いためコストは高か
った。これに対し本発明では強磁性の母材に全面的なメ
ッキ加工を一度行い、これをレーザ光線等で熱処理して
非磁性の変質部を形成するようにしたためコストは大巾
に低下した。
As described above, the magnetic scale of the present invention is conventionally provided with a large number of grooves or the like by machining a ferromagnetic base material and non-magnetic plating is applied to the grooves or the like to remove a beard generated during plating. The cost was high due to the large number of platings. On the other hand, in the present invention, the entire surface of the ferromagnetic base material is subjected to plating and heat treatment is performed with a laser beam or the like to form the non-magnetic altered portion, so that the cost is drastically reduced.

また従来例では温度が上昇すると電気出力、耐熱性等の
特性が著しく低下したが、本発明の非磁性である変質部
は安定したオーステナイト組織であるため温度が上昇し
ても電気出力や耐熱性の特性が劣化することはない。さ
らに従来のスケールは移動体に腕等を出してこれに取付
けていたため、大きな加速度が加えられると容易に故障
するため強大な機構になりコストを高くすると共に操作
性を悪くしていたが、本発明では移動体そのものを磁気
スケールにすることが可能であるため、いかに大きな加
速度でも故障することがない等多くの利点を有する。こ
れらのほか本発明においては非磁性である変質部の厚さ
をアーク放電等の使用により大きくすることが可能であ
り検出器出力を高くしてSN比を良くする利点も有する。
Further, in the conventional example, when the temperature rises, the characteristics such as electric output and heat resistance are remarkably deteriorated, but since the non-magnetic alteration portion of the present invention has a stable austenite structure, the electric output and heat resistance are high even if the temperature rises. Does not deteriorate the characteristics. Furthermore, in the conventional scale, the arm is attached to the moving body by attaching it to the moving body, so it easily breaks down when a large acceleration is applied, resulting in a powerful mechanism that increases the cost and deteriorates the operability. According to the invention, since the moving body itself can be a magnetic scale, it has many advantages such as no failure even with a large acceleration. In addition to these, in the present invention, the thickness of the non-magnetic alteration portion can be increased by using arc discharge or the like, and there is an advantage that the detector output is increased and the SN ratio is improved.

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

第1図ないし第5図は本発明の一実施例を示し第1図は
加工中の断面図、第2図は加工終了時の断面図、第3図
および第4図は検出器の異なる時点における断面図、第
5図は検出器の電気系統図、第6図は本発明の他の実施
例における断面図、第7図および第8図は本発明の磁気
スケールをダイカスト機に使用した一例を示し第7図は
縦断面図、第8図は第7図の8−8線断面図、第9図は
本発明の他の実施例における加工中の断面図、第10図は
本発明の磁気スケールを位置決め装置に使用した一例の
断面図である。 11・32・61……母材、12・32・62……薄膜、13……レー
ザ光線、
1 to 5 show an embodiment of the present invention, FIG. 1 is a sectional view during processing, FIG. 2 is a sectional view at the end of processing, and FIGS. 3 and 4 are different time points of a detector. 5 is a sectional view of the detector, FIG. 5 is a sectional view of the detector, FIG. 6 is a sectional view of another embodiment of the present invention, and FIGS. 7 and 8 are examples of using the magnetic scale of the present invention in a die casting machine. 7 is a longitudinal sectional view, FIG. 8 is a sectional view taken along line 8-8 of FIG. 7, FIG. 9 is a sectional view during processing in another embodiment of the present invention, and FIG. 10 is a sectional view of the present invention. It is sectional drawing of an example which used the magnetic scale for the positioning device. 11 ・ 32 ・ 61 …… Base material, 12 ・ 32 ・ 62 …… Thin film, 13 …… Laser beam,

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭51−99557(JP,A) 「NIKKEI MECHANICAL (1985.5.20)」P.53 「鉄鋼材料便覧」(昭和42.6.30 丸 善発行)P.636〜P.638 Edited by C.R.Clay tom,C.M.Preece「Corr osion of Metals Pre cessed by Directed Energy Beams」(1982) 熱処理.17[3](昭和52−6)社団法 人 日本熱処理技術協会 P.131 図2 ─────────────────────────────────────────────────── ─── Continuation of the front page (56) Reference JP-A-51-99557 (JP, A) “NIKKEI MECHANICAL (1985.20.1985)” P. 53 “Steel Materials Handbook” (published by Maruzen, June 30, 1942) 636-P. 638 Edited by C.I. R. Clay tom, C.I. M. Prece "Corrion of Metals Precessed by Directed Energy Beams" (1982) Heat treatment. 17 [3] (Showa 52-6) Corporate Law Association Japan Heat Treatment Technology Association P. 131 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】鋼材で透磁率2000程度を有する母材の表面
にニッケルメッキまたはクロームメッキあるいはニッケ
ル、クローム、マンガン、炭素を含む合金の溶射により
薄膜を形成し、同薄膜の外周に所定の間隔を保持してレ
ーザ光線の照射あるいはアーク放電により該薄膜および
前記母材を加熱し短時間内に溶融して固化させ、前記母
材の表層部に規則的に配置され半月形あるいはU字形の
断面を有する非磁性の変質部を設けるようにしたことを
特徴とする磁気スケール。
1. A thin film is formed on the surface of a base material made of steel having a magnetic permeability of about 2000 by nickel plating or chrome plating or thermal spraying of an alloy containing nickel, chrome, manganese, and carbon, and a predetermined interval is provided on the outer periphery of the thin film. The thin film and the base material are heated by being irradiated with a laser beam or arc discharge to melt and solidify within a short time, and a half-moon or U-shaped cross section is regularly arranged on the surface layer of the base material. A magnetic scale characterized in that a non-magnetic alteration portion having a magnetic field is provided.
JP60181366A 1985-08-19 1985-08-19 Magnetic scale Expired - Lifetime JPH0676894B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60181366A JPH0676894B2 (en) 1985-08-19 1985-08-19 Magnetic scale

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60181366A JPH0676894B2 (en) 1985-08-19 1985-08-19 Magnetic scale

Publications (2)

Publication Number Publication Date
JPS6242003A JPS6242003A (en) 1987-02-24
JPH0676894B2 true JPH0676894B2 (en) 1994-09-28

Family

ID=16099468

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60181366A Expired - Lifetime JPH0676894B2 (en) 1985-08-19 1985-08-19 Magnetic scale

Country Status (1)

Country Link
JP (1) JPH0676894B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR101506028B1 (en) * 2006-03-08 2015-03-25 리브에르 프랑스 에스에이에스 Position measuring system for a hydraulic cylinder

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4839591A (en) * 1986-12-16 1989-06-13 Kayaba Kogyo Kabushiki-Kaisha Magnetic stroke sensor for detecting the stroke of a fluid-power cylinder
JPS63259413A (en) * 1987-04-15 1988-10-26 Kayaba Ind Co Ltd Manufacture of magnetic scale
JP2698586B2 (en) * 1987-08-31 1998-01-19 日本原子力研究所 Manufacturing method of heat resistant magnetic scale
US5180609A (en) * 1988-03-09 1993-01-19 Kabushiki Kaisha Toshiba Method of forming modified portion and magnetic recording member using this method
US5100692A (en) * 1988-03-09 1992-03-31 Kabushiki Kaisha Toshiba Method of forming a magnetically modified portion
JPH059562A (en) * 1991-06-28 1993-01-19 Toyota Motor Corp Formation of signal pattern utilizing change of magnetic property
US6253460B1 (en) * 1999-06-10 2001-07-03 Geoffrey W. Schmitz Apparatus for position measurement and a system and a method for using the same
JP5324348B2 (en) * 2009-07-21 2013-10-23 株式会社リベックス Displacement detection member

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5199557A (en) * 1975-02-28 1976-09-02 Tokyo Shibaura Electric Co SUKEERUNOSEIZOHOHO

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
「NIKKEIMECHANICAL(1985.5.20)」P.53
「鉄鋼材料便覧」(昭和42.6.30丸善発行)P.636〜P.638
EditedbyC.R.Claytom,C.M.Preece「CorrosionofMetalsPrecessedbyDirectedEnergyBeams」(1982)
熱処理.17[3(昭和52−6)社団法人日本熱処理技術協会P.131図2

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR101506028B1 (en) * 2006-03-08 2015-03-25 리브에르 프랑스 에스에이에스 Position measuring system for a hydraulic cylinder

Also Published As

Publication number Publication date
JPS6242003A (en) 1987-02-24

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