JPS61188709A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPS61188709A JPS61188709A JP2909785A JP2909785A JPS61188709A JP S61188709 A JPS61188709 A JP S61188709A JP 2909785 A JP2909785 A JP 2909785A JP 2909785 A JP2909785 A JP 2909785A JP S61188709 A JPS61188709 A JP S61188709A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic head
- magnetic
- head body
- flux density
- saturation
- 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.)
- Pending
Links
- 229910000859 α-Fe Inorganic materials 0.000 claims abstract description 23
- 238000001816 cooling Methods 0.000 claims abstract description 8
- 239000003507 refrigerant Substances 0.000 claims description 4
- 230000004907 flux Effects 0.000 abstract description 10
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 abstract description 8
- 239000007788 liquid Substances 0.000 abstract description 6
- 229910052757 nitrogen Inorganic materials 0.000 abstract description 4
- 230000002159 abnormal effect Effects 0.000 abstract description 3
- 239000002826 coolant Substances 0.000 abstract description 3
- 230000005347 demagnetization Effects 0.000 abstract description 3
- 229910045601 alloy Inorganic materials 0.000 description 9
- 239000000956 alloy Substances 0.000 description 9
- 229910000702 sendust Inorganic materials 0.000 description 8
- 239000013078 crystal Substances 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 230000005415 magnetization Effects 0.000 description 4
- 238000004804 winding Methods 0.000 description 4
- LYCAIKOWRPUZTN-UHFFFAOYSA-N Ethylene glycol Chemical compound OCCO LYCAIKOWRPUZTN-UHFFFAOYSA-N 0.000 description 3
- 239000002184 metal Substances 0.000 description 3
- 229910000808 amorphous metal alloy Inorganic materials 0.000 description 2
- 239000000696 magnetic material Substances 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 230000035699 permeability Effects 0.000 description 2
- 238000007789 sealing Methods 0.000 description 2
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229910052598 goethite Inorganic materials 0.000 description 1
- AEIXRCIKZIZYPM-UHFFFAOYSA-M hydroxy(oxo)iron Chemical compound [O][Fe]O AEIXRCIKZIZYPM-UHFFFAOYSA-M 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 239000006247 magnetic powder Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 229910006297 γ-Fe2O3 Inorganic materials 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/40—Protective measures on heads, e.g. against excessive temperature
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/10—Structure or manufacture of housings or shields for heads
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/133—Structure or manufacture of heads, e.g. inductive with cores composed of particles, e.g. with dust cores, with ferrite cores with cores composed of isolated magnetic particles
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/187—Structure or manufacture of the surface of the head in physical contact with, or immediately adjacent to the recording medium; Pole pieces; Gap features
- G11B5/193—Structure or manufacture of the surface of the head in physical contact with, or immediately adjacent to the recording medium; Pole pieces; Gap features the pole pieces being ferrite or other magnetic particles
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Abstract
Description
【発明の詳細な説明】
庄1」Jl生肚分盟−
この発明は、磁気記録を行う磁気ヘッド、特に高記録密
度が要求されるVTR等に使用できる磁気ヘッドに関す
るものである。DETAILED DESCRIPTION OF THE INVENTION This invention relates to a magnetic head that performs magnetic recording, and particularly to a magnetic head that can be used in VTRs and the like that require high recording density.
従速]支術−
従来よりVTRやコンピュータ等の磁気記録を行わせる
磁気ヘッドは、高透磁率、高飽和磁束密度、低抗磁力、
そして高周波特性や媒体に対する耐摩耗性等の特性が要
求される。したがって、その磁気へッドファは、周知の
通り磁性材料であり、その代表例としては、Mn−Zn
単結晶フェライトやセンダスト合金及・びアモルファス
合金がある。まずMn−Zn単結晶フェライトコア(以
下単にフェライトコアと記す)は、記録媒体の材質が、
以前から採用されて来た、針状ゲータイト粒子から得ら
れるγ−Fe2O3に適合するので賞月されているが、
飽和を磁束密度特性では、より一層の向上は困難とされ
ている。つぎに、センダスト合金及びアモルファス合金
コアは、媒体がFe−GoやFe−Go−Nt等を主組
成とする、メタル磁性粉使用の場合、フェライトコアが
適合しないのに対して、確実に適応するので、今後の実
用化が期待されている。その中で、センダスト合金は、
公知化されている通り、Fe−51−Ml等を主組成と
する合金であって、例えば、第7回日本応用磁気学会学
術講演概要集(1983・11.8PA−11,P12
3)や特開昭58−18916号公報等に紹介されてい
る。Traditionally, magnetic heads used for magnetic recording in VTRs, computers, etc. have high magnetic permeability, high saturation magnetic flux density, low coercive force,
Further, characteristics such as high frequency characteristics and wear resistance against media are required. Therefore, the magnetic head is made of a magnetic material as is well known, and a typical example thereof is Mn-Zn.
There are single crystal ferrite, sendust alloy, and amorphous alloy. First, the Mn-Zn single crystal ferrite core (hereinafter simply referred to as ferrite core) has a recording medium made of
It has been praised because it is compatible with γ-Fe2O3 obtained from acicular goethite particles, which has been used for a long time.
It is considered difficult to further improve saturation in magnetic flux density characteristics. Next, Sendust alloy and amorphous alloy cores are definitely compatible with metal magnetic powder, where the medium has a main composition such as Fe-Go or Fe-Go-Nt, whereas ferrite cores are not compatible. Therefore, it is expected that it will be put into practical use in the future. Among them, Sendust alloy is
As is publicly known, it is an alloy whose main composition is Fe-51-Ml etc.
3) and Japanese Unexamined Patent Publication No. 18916/1983.
フェライトコアとセンダスト合金コアの具体的な諸性性
を比較すると、次の表1の通りである。A comparison of the specific properties of the ferrite core and the sendust alloy core is shown in Table 1 below.
表1 ビデオヘッド用磁性材料
ロ (よ′ 。占
ところで、上述した第1表から判るように、センダスト
合金コアは、フェライトコアに比べてビッカース硬度が
小さり、シたがって4′F11!耗性が劣る。また高周
波帯域における透磁率も低い欠点がある。しかも、セン
ダスト合金は、コアの巻線溝やトラック溝などの加工を
施す場合、フェライトよりも脆く、実用性の面でやや難
色がある。このような欠点があるにもかかわらず、セン
ダスト合金が高記録密度となるメタルテープ等に対する
磁気ヘッドに採用され始めた根拠は、フェライトに比べ
飽和磁束密度が圧倒的に高いからに尽きる。Table 1 Magnetic materials for video heads By the way, as can be seen from Table 1 above, the Sendust alloy core has a lower Vickers hardness than the ferrite core, and therefore has a wear resistance of 4'F11! It also has the disadvantage of low magnetic permeability in the high frequency band.In addition, Sendust alloy is more brittle than ferrite when processing core winding grooves and track grooves, making it somewhat difficult to use in terms of practicality. Despite these drawbacks, the reason why Sendust alloy has begun to be used in magnetic heads for metal tapes with high recording densities is that it has an overwhelmingly higher saturation magnetic flux density than ferrite.
したがって、フェライトコアを用いても高飽和磁束密度
が得られればよい訳であるが、フェライトの材質改善は
困難であった。この発明は、以上の経緯があって、フェ
ライトコアの欠点是正を図った磁気ヘッドを提案するも
のである。Therefore, even if a ferrite core is used, it is sufficient to obtain a high saturation magnetic flux density, but it has been difficult to improve the material quality of the ferrite. Based on the above background, the present invention proposes a magnetic head in which the drawbacks of the ferrite core are corrected.
口 ′ こ
のこの発明は、フェライトコアを従来と同様に用いて
形成した磁気ヘッド本体を、冷媒を充填した冷却装置に
取付けすることを提唱する。すなわち、この発明は、磁
気ヘッド本体自身は、従来より実績があるフェライトコ
アを採用し、冷却装置に取付けることによって、高飽和
磁束密度特性を得よ・うとする点に特徴がある。Mouth
This invention proposes that a magnetic head body formed using a ferrite core in a conventional manner be attached to a cooling device filled with a coolant. That is, the present invention is characterized in that the magnetic head body itself uses a ferrite core, which has been used in the past, and is attached to a cooling device to obtain high saturation magnetic flux density characteristics.
作1−
この発明では、冷却装置によって、磁気ヘンド本体が極
めて低い温度に設定されるので、飽和磁束密度が大幅に
上昇する。またこの発明では、磁気ヘッド本体が常時冷
却されているので、記録媒体と摺動させる場合でも、摺
動摩擦による焼き付きや、異常昇温か生じて減磁してし
まう危険性が排除できる。Production 1 - In this invention, the temperature of the magnetic hend body is set to an extremely low temperature by the cooling device, so that the saturation magnetic flux density increases significantly. Further, in this invention, since the magnetic head main body is constantly cooled, even when sliding with a recording medium, it is possible to eliminate the risk of burning due to sliding friction or demagnetization due to abnormal temperature rise.
炎監外
第1図は、この発明の一実施例を説明する上で参照する
磁気ヘッドの概念図である。まず、1は、極めて低い温
度にする冷却装置の真空デユアである。2は、真空デユ
ア1の内壁と、密封壁3との間の密閉空間に完全に充填
された冷媒としての液体窒素で、液温を約77°Kに設
定したものである。FIG. 1 is a conceptual diagram of a magnetic head to be referred to in explaining an embodiment of the present invention. First, 1 is a vacuum dure of a cooling device that brings the temperature to an extremely low temperature. 2 is liquid nitrogen as a refrigerant that is completely filled in the sealed space between the inner wall of the vacuum dure 1 and the sealing wall 3, and the liquid temperature is set to about 77°K.
4は、密封壁3に囲繞されたヘッド本体収納テープで、
中央部に設けられた窓部5に、磁気へノド本体6が磁気
ギャップを有する頂面を露出するように固定されている
。さて、磁気ヘッド本体6は、従来と同様なMn −Z
n単結晶フェライトコアを用いたもので、第2図に示す
通りの構造である。すなわち第2図で、7,8はコア半
休であり、巻線挿通窓9、巻線係止溝10.11を設け
、低融点ガラス12を接着材として接合したものである
。そして、磁気ヘッド本体6の曲面研磨された頂面13
上のほぼ中央部に、磁気ギャップ14が形成されている
。4 is a head body storage tape surrounded by a sealing wall 3;
A magnetic nod main body 6 is fixed to a window 5 provided in the center so as to expose the top surface having a magnetic gap. Now, the magnetic head main body 6 is made of Mn-Z similar to the conventional one.
It uses an n single-crystal ferrite core and has a structure as shown in FIG. That is, in FIG. 2, cores 7 and 8 are half-open, provided with a winding insertion window 9, a winding locking groove 10, 11, and bonded with low melting point glass 12 as an adhesive. Then, the curved polished top surface 13 of the magnetic head main body 6
A magnetic gap 14 is formed approximately in the upper center.
また15は、コイル巻線である。Further, 15 is a coil winding.
以上構造概略を説明した磁気ヘッドは、冷却装置にて、
磁気ヘッド本体6が約776にという低温に設定されて
いるので、フェライトコアの飽和磁束密度Bsが、数十
%上昇する。この点は、第3図に示すように、Mn−Z
n単結晶フェライトコアの温度−飽和磁化特性曲線16
上の常温でのA点と、1000にでのB点との飽和磁化
Msを比べると、B点ではA点に対して約50%増加す
ることから判明する。The magnetic head whose structure has been explained above is installed in a cooling device.
Since the magnetic head body 6 is set at a low temperature of about 776°C, the saturation magnetic flux density Bs of the ferrite core increases by several tens of percent. This point is important for Mn-Z, as shown in Figure 3.
Temperature-saturation magnetization characteristic curve 16 of n single crystal ferrite core
Comparing the saturation magnetization Ms at point A at normal temperature and point B at 1000 ℃ above, it is found that the saturation magnetization Ms increases by about 50% at point B compared to point A.
尚、上記実施例では、フェライトコアとしてMn−zn
単結晶フェライト、冷媒として液体窒素を掲げたが、こ
の発明ではその他に、ホットプレスフェライトとしたり
、エチレングリコール等を用いたりしてもよい。In the above embodiment, Mn-zn is used as the ferrite core.
Although single crystal ferrite and liquid nitrogen are used as the refrigerant, in this invention, hot pressed ferrite, ethylene glycol, etc. may also be used.
光朋」峠l良
この発明によれば、従来よりのフエライトコアの欠点で
ある飽和磁束密度が低い点が是正されるので、メタルテ
ープ等の記録媒体にも十分対応でき、センダスト合金コ
アを用いなくても高密度記録が可能な磁気ヘッドが得ら
れる。またこの発明によれば、異常昇温によるコアの減
磁等の事故が回避でき、安定した動作をする磁気ヘッド
が期待できる。According to this invention, the low saturation magnetic flux density, which is a drawback of conventional ferrite cores, can be corrected, so it is fully compatible with recording media such as metal tapes, and it can be used with sendust alloy cores. A magnetic head capable of high-density recording can be obtained even without this. Further, according to the present invention, accidents such as demagnetization of the core due to abnormal temperature rise can be avoided, and a magnetic head that operates stably can be expected.
第1図は、この発明の一実施例を説明するための磁気ヘ
ッドの概念図、第2図は、その磁気ヘッド本体の斜視図
、第3図は、Mn−Zn単結晶フェライトの温度−飽和
磁化特性曲線図である。
1・・・・・・冷却装置(真空デユア)、2・・・・・
・冷媒(液体窒素)、
6・・・・・・磁気ヘッド本体。FIG. 1 is a conceptual diagram of a magnetic head for explaining an embodiment of the present invention, FIG. 2 is a perspective view of the main body of the magnetic head, and FIG. 3 is a temperature-saturation diagram of Mn-Zn single crystal ferrite. It is a magnetization characteristic curve diagram. 1... Cooling device (vacuum dua), 2...
- Refrigerant (liquid nitrogen), 6...Magnetic head body.
Claims (1)
した冷却装置に取付けしたことを特徴とする磁気ヘッド
。A magnetic head characterized in that a magnetic head body using a ferrite core is attached to a cooling device filled with a refrigerant.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2909785A JPS61188709A (en) | 1985-02-16 | 1985-02-16 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2909785A JPS61188709A (en) | 1985-02-16 | 1985-02-16 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61188709A true JPS61188709A (en) | 1986-08-22 |
Family
ID=12266847
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2909785A Pending JPS61188709A (en) | 1985-02-16 | 1985-02-16 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61188709A (en) |
-
1985
- 1985-02-16 JP JP2909785A patent/JPS61188709A/en active Pending
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