JPH041455Y2 - - Google Patents
Info
- Publication number
- JPH041455Y2 JPH041455Y2 JP15538284U JP15538284U JPH041455Y2 JP H041455 Y2 JPH041455 Y2 JP H041455Y2 JP 15538284 U JP15538284 U JP 15538284U JP 15538284 U JP15538284 U JP 15538284U JP H041455 Y2 JPH041455 Y2 JP H041455Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- head
- thin plates
- permeability material
- magnetic permeability
- 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 31
- 230000035699 permeability Effects 0.000 claims description 26
- 230000004907 flux Effects 0.000 claims description 12
- 239000000696 magnetic material Substances 0.000 description 15
- 229910000889 permalloy Inorganic materials 0.000 description 12
- DMFGNRRURHSENX-UHFFFAOYSA-N beryllium copper Chemical compound [Be].[Cu] DMFGNRRURHSENX-UHFFFAOYSA-N 0.000 description 7
- 238000010030 laminating Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 3
- 238000003475 lamination Methods 0.000 description 3
- 230000005389 magnetism Effects 0.000 description 3
- 230000005415 magnetization Effects 0.000 description 2
- 230000002238 attenuated effect Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 125000006850 spacer group Chemical group 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Landscapes
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Transmission And Conversion Of Sensor Element Output (AREA)
Description
【考案の詳細な説明】
〔考案の技術的範囲〕
この考案は磁気スケールの磁化パターンを検出
して電気信号に変換するための磁束応答型マルチ
ギヤツプヘツドに関する。[Detailed Description of the Invention] [Technical Scope of the Invention] This invention relates to a magnetic flux responsive multi-gap head for detecting the magnetization pattern of a magnetic scale and converting it into an electrical signal.
磁気スケール上の磁化パターンを検出して長さ
や角度を電気的に読みとるに際し、高精度、高分
解能、安定高出力を得るために開発、実用化され
ている磁束応答型マルチギヤツプヘツドは、n個
のヘツドをλm/2(λmはマルチギヤツプヘツド
の固有波長)の間隙で配置し、隣り合うヘツドを
互いに逆向きで全部を直列に接続している。そし
て各ヘツドの出力はそれぞれ加え合わされるよう
になつており、マルチギヤツプヘツドの固有波長
λmが磁気スケールの波長λと一致したときに出
力が最大となり、1個のヘツドのn倍の出力が得
られるようになつている。そして逆に磁気スケー
ルの波長λとマルチギヤツプヘツドの固有波長が
一致しない場合は各ヘツドの出力に位相差を生じ
出力が減衰することになる。
The magnetic flux responsive multi-gear head has been developed and put into practical use in order to obtain high accuracy, high resolution, and stable high output when detecting the magnetization pattern on the magnetic scale and electrically reading the length and angle. n heads are arranged with a gap of λm/2 (λm is the characteristic wavelength of the multi-gap head), and all are connected in series with adjacent heads facing in opposite directions. The outputs of each head are then added together, and when the characteristic wavelength λm of the multi-gap head matches the wavelength λ of the magnetic scale, the output reaches its maximum, and the output is n times that of a single head. It is becoming possible to obtain Conversely, if the wavelength λ of the magnetic scale and the characteristic wavelength of the multi-gap head do not match, a phase difference will occur in the output of each head and the output will be attenuated.
このような、磁束応答型マルチギヤツプヘツド
は、従来第2図に示すように高透磁率材料(例え
ばパーマロイ)の薄板a,c,eをコアとし、非
磁性材料(例えばベリリルム銅)の薄板b,dを
セパレータとして交互の積み重ね、各コアが1つ
のギヤツプを持つように構成されていた。そして
ギヤツプ間隔は例えば0.1mmと微小であり、この
ギヤツプの変動はマルチギヤツプヘツドの固有波
長に大きな影響を及ぼすことになるので、従来は
積層する高透磁率材料の薄板a,c,eと非磁性
材料の薄板b,dの厚みを一定の範囲内に規定し
て、これを積層することによつてギヤツプ間隔を
保持するようにしている。 As shown in Fig. 2, such a magnetic flux responsive multi-geap head conventionally has a core made of thin plates a, c, and e made of a high magnetic permeability material (e.g. permalloy), and a core made of a non-magnetic material (e.g. beryllium copper). The thin plates b and d were stacked alternately as separators, and each core had one gap. The gap spacing is as small as 0.1 mm, for example, and variations in this gap have a large effect on the characteristic wavelength of the multi-gap head. The thickness of the thin plates b and d of non-magnetic material are defined within a certain range, and the gap distance is maintained by laminating them.
例えば前述したギヤツプ間隔を0.1mmにする場
合には、高透磁率材料(パーマロイ)の薄板a,
c,eおよび非磁性材(ベリリウム銅)の薄板
b,dの板厚は0.05mmに正確に規定しなければ磁
気のギヤツプが形成されない。そして、その積層
に際しても厚みの変動に注意しながら行う必要が
あり、板厚の管理も高透磁率材料と非磁性材料の
二種類について正確に行う必要があり、多くの労
力と細心の注意を必要とするなど磁束応答型マル
チギヤツプヘツドを製作する際の隘路となつてい
た。 For example, if the gap spacing mentioned above is set to 0.1 mm, thin plate a of high magnetic permeability material (permalloy),
The thicknesses of thin plates b, d made of non-magnetic material (beryllium copper) and c and e must be precisely defined to 0.05 mm to form a magnetic gap. Furthermore, when laminating the layers, it is necessary to pay attention to variations in thickness, and the thickness must be precisely controlled for two types of materials: high magnetic permeability material and non-magnetic material, which requires a lot of effort and careful attention. This has become a bottleneck in producing a magnetic flux responsive multi-gear head.
〔考案の目的〕
この考案は、磁気の実情にもとづいてなされた
もので、その目的とするところは、マルチギヤツ
プヘツドのコア用として厳重な厚さ規制を要求さ
れる高透磁率材料ならびに非磁性材料の薄板のう
ち、高透率材料の薄板だけでマルチギヤツプヘツ
ドを構成し板厚の管理を1種類の材料のものだけ
で済むようにすることを目的としている。[Purpose of the invention] This invention was made based on the actual situation of magnetism, and its purpose is to use high magnetic permeability materials and materials that require strict thickness regulations for the core of multi-gap heads. Among the thin plates of non-magnetic materials, the purpose is to construct a multi-gap head using only thin plates of high permeability material and to manage the thickness of the plates by using only one type of material.
この考案は、従来高透磁率材料の薄板と非磁性
材料の薄板を交互に積層してマルチギヤツプヘツ
ドのコアとしていたものを磁気スケールの記録波
長λの1/4λの厚さの高透磁率材料の薄板だけを
積層して構成するようにしたもので、すなわち、
積層する高透磁率材料の薄板のうちの1部の薄板
を磁気抵抗が大きくなるような形状に成形し、こ
れを従来の非磁性材料の代りにセパレータとして
使用して磁束応答型マルチギヤツプヘツドを構成
するものである。
This idea replaces the core of a multi-gap head, which was conventionally made by laminating thin plates of high magnetic permeability material and thin plates of non-magnetic material alternately, into a high-permeability core with a thickness of 1/4λ of the recording wavelength λ of the magnetic scale. It is constructed by laminating only thin plates of magnetic material, that is,
A part of the laminated thin plates of high magnetic permeability material is formed into a shape that increases magnetic resistance, and this is used as a separator instead of the conventional non-magnetic material to create a magnetic flux responsive multi-gap. This constitutes the head.
以下、この考案を図面に示す実施例にもとづい
て説明する。
This invention will be explained below based on embodiments shown in the drawings.
第1図において磁束応答型マルチギヤツプヘツ
ドを構成する薄板はすべて磁気スケールの記録波
長λの1/4λの厚さを有する高透磁率材料(パー
マロイ)とし、そしてこの高透磁率材料(パーマ
ロイ)の薄板f,g,h,i,jのうち薄板gと
iの形状を図に示したようにできるだけ磁気抵抗
が大きくなるように中心部で二分割するととも
に、磁気スケールを挿通するスケール穴1は薄板
f,h,jのスケール穴2より充分大きくとつ
て、磁気スケールとの間の磁気抵抗を増加させる
ため中心部で切離された薄板の各々に半円形の切
り欠きを設けてある。このような形状に形成され
た高透磁率材料(パーマロイ)の薄板gとiは、
高透磁率材料であるが従来の非磁性材料の薄板と
同じようにスペサーとしての役割を充分に果し、
ギヤツプ間隔の保持がなされる。 In Fig. 1, all the thin plates constituting the magnetic flux responsive multi-gap head are made of a high magnetic permeability material (permalloy) having a thickness of 1/4λ of the recording wavelength λ of the magnetic scale. ) out of the thin plates f, g, h, i, and j, the shapes of thin plates g and i are divided into two at the center so that the magnetic resistance is as large as possible as shown in the figure, and a scale hole is inserted into which the magnetic scale is inserted. 1 is made sufficiently larger than the scale hole 2 of the thin plates f, h, and j, and a semicircular notch is provided in each of the thin plates cut at the center in order to increase the magnetic resistance between the thin plates and the magnetic scale. . The thin plates g and i of high magnetic permeability material (permalloy) formed in such a shape are:
Although it is a high magnetic permeability material, it fully fulfills the role of a spacer in the same way as a conventional thin plate of non-magnetic material.
Gap spacing is maintained.
したがつて、従来の磁束応答型マルチギヤツプ
ヘツドのように高透磁率材料(パーマロイ)と非
磁性材料(ベリリウム銅)の二つの材料の板厚を
正確に管理して使用する必要がなく高透磁率材料
(パーマロイ)の板厚だけの管理ですみ、そして
高透磁率材料(パーマロイ)の磁気抵抗を大きく
するための形状の形成については、エツチング技
術によつて簡単に形成させることが可能である。 Therefore, there is no need to accurately control the thickness of two materials, high magnetic permeability material (permalloy) and non-magnetic material (beryllium copper), as in conventional magnetic flux responsive multi-gap heads. It is only necessary to control the plate thickness of the high magnetic permeability material (permalloy), and the shape to increase the magnetic resistance of the high magnetic permeability material (permalloy) can be easily formed using etching technology. It is.
また、従来の磁束応答型マルチギヤツプヘツド
では、高透磁率材料(パーマロイ)と非磁性材料
(ベリリウム銅)を積層するものであるから、両
材料間に硬度の差があるため積層段階で圧力を加
えると硬度の低い非磁性材料(ベリリウム銅)に
機械的な歪が生じることになるが、この考案は高
透磁率材料(パーマロイ)のみであるから積層時
に圧力を加えることができる。 In addition, in conventional magnetic flux responsive multi-geap heads, a high magnetic permeability material (permalloy) and a non-magnetic material (beryllium copper) are laminated, so there is a difference in hardness between the two materials, so there is a difference in hardness during the lamination stage. When pressure is applied, mechanical distortion occurs in a non-magnetic material with low hardness (beryllium copper), but since this idea uses only a high magnetic permeability material (permalloy), pressure can be applied during lamination.
なお、高透磁率材料(パーマロイ)と非磁性材
料(ベリリウム銅)を積層するものは、第3図イ
に示すようにヘツドの端面Aに高透磁率材料(パ
ーマロイ)と非磁性材料(ベリリウム銅)が交互
に表われるので、信号の取り出しには第3図ロに
示す集磁用部分3を有する特殊の形をしたピツク
アツプ部材4を用いなければならず、このためピ
ツクアツプコイルの捲回に手数を要したが、この
考案のものではヘツド端面Aはすべて高透磁率材
料(パーマロイ)であるから、第3図ハに示すよ
うに集磁用部分3のない単純な形状のピツクアツ
プ部材5を用いることで目的が達せられる。 In addition, when a high magnetic permeability material (permalloy) and a non-magnetic material (beryllium copper) are laminated, the high magnetic permeability material (permalloy) and the non-magnetic material (beryllium copper) are layered on the end face A of the head, as shown in Figure 3A. ) appear alternately, so a specially shaped pick-up member 4 having a magnetism collecting portion 3 shown in Fig. 3(b) must be used to extract the signal. However, in this device, the end face A of the head is entirely made of a high magnetic permeability material (permalloy), so a pick-up member 5 of a simple shape without a magnetic collecting part 3 is used as shown in FIG. 3C. This will help you achieve your goal.
以上説明したように、この考案の磁束応答型マ
ルチギヤツプヘツドは、ヘツドを構成するための
薄板は高透磁率材料だけであるから、従来のよう
に2種類の板厚を管理する必要がなく、また、薄
板の積層時に圧力を加えることができるのでヘツ
ドとして積層後における寸法の調整が可能とな
る。さらにこの考案では高透磁率材料の薄板だけ
を積層しているから、ヘツドの端面は高透磁率材
料だけで露出するので特殊形状をしたピツクアツ
プ部材を用いる必要がなく、コイルの捲回が極め
て容易になるなどの効果を有するものである。
As explained above, in the magnetic flux-responsive multi-gear head of this invention, the thin plates used to construct the head are only high magnetic permeability materials, so there is no need to manage two types of plate thickness as in the past. Moreover, since pressure can be applied when laminating the thin plates, it becomes possible to adjust the dimensions after lamination as a head. Furthermore, since this device only laminates thin plates of high magnetic permeability material, the end face of the head is exposed only with high magnetic permeability material, so there is no need to use a specially shaped pick-up member, and winding of the coil is extremely easy. It has the effect of becoming.
第1図はこの考案の一実施例の概略的斜視図、
第2図は従来の磁束応答型マルチギヤツプヘツド
のヘツド構成を示す概略的斜視図、第3図は従来
のヘツドとこの考案のヘツドに対するピツクアツ
プ部材の装着状態を示す概略的斜視図である。
a,c,e,f,g,h,i,j……高透磁率
材料、b,d……非磁性材料、1,2……スケー
ル穴、3……集磁用部分、5……ピツクアツプ部
材。
FIG. 1 is a schematic perspective view of an embodiment of this invention;
FIG. 2 is a schematic perspective view showing the head configuration of a conventional magnetic flux responsive multi-geap head, and FIG. 3 is a schematic perspective view showing the state in which a pick-up member is attached to the conventional head and the head of this invention. . a, c, e, f, g, h, i, j... High magnetic permeability material, b, d... Non-magnetic material, 1, 2... Scale hole, 3... Magnetism collecting part, 5... Pick-up parts.
Claims (1)
る磁気パターンを検出する磁束応答型マルチギヤ
ツプヘツドにおいて、磁気スケールの記録波長λ
の1/4λの厚さの高透磁率材料の薄板と、この高
透磁率材料の薄板と同じ厚みであるが磁気抵抗が
大きくなるような形状とした高透磁率材料の薄板
とを交互に複数枚積み重ね高透磁率材料の薄板だ
けでヘツドを構成したことを特徴とする磁束応答
型マルチギヤツプヘツド。 In a magnetic flux responsive multi-gap head that detects a magnetic pattern formed by magnetically recording a signal of a fixed wavelength on a magnetic medium, the recording wavelength λ of the magnetic scale is
A plurality of thin plates of high magnetic permeability material with a thickness of 1/4λ of λ and thin plates of high magnetic permeability material with the same thickness as this thin plate of high magnetic permeability material but shaped to increase magnetic resistance are alternately used. A magnetic flux-responsive multi-gap head characterized in that the head is composed only of stacked thin plates of high magnetic permeability material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15538284U JPH041455Y2 (en) | 1984-10-15 | 1984-10-15 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15538284U JPH041455Y2 (en) | 1984-10-15 | 1984-10-15 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6170716U JPS6170716U (en) | 1986-05-14 |
| JPH041455Y2 true JPH041455Y2 (en) | 1992-01-20 |
Family
ID=30713391
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15538284U Expired JPH041455Y2 (en) | 1984-10-15 | 1984-10-15 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH041455Y2 (en) |
-
1984
- 1984-10-15 JP JP15538284U patent/JPH041455Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6170716U (en) | 1986-05-14 |
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