JPH04102202A - Magnetic field generator for magneto-optical recording - Google Patents
Magnetic field generator for magneto-optical recordingInfo
- Publication number
- JPH04102202A JPH04102202A JP21805690A JP21805690A JPH04102202A JP H04102202 A JPH04102202 A JP H04102202A JP 21805690 A JP21805690 A JP 21805690A JP 21805690 A JP21805690 A JP 21805690A JP H04102202 A JPH04102202 A JP H04102202A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- main pole
- magneto
- main
- optical recording
- 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
- 239000007769 metal material Substances 0.000 claims abstract description 20
- 230000005284 excitation Effects 0.000 claims description 24
- 238000004804 winding Methods 0.000 claims description 18
- 230000017525 heat dissipation Effects 0.000 claims description 2
- 239000000463 material Substances 0.000 description 12
- 230000005415 magnetization Effects 0.000 description 8
- 229910000859 α-Fe Inorganic materials 0.000 description 7
- 230000007423 decrease Effects 0.000 description 6
- 239000000696 magnetic material Substances 0.000 description 5
- 238000000034 method Methods 0.000 description 5
- 230000005855 radiation Effects 0.000 description 5
- 229910045601 alloy Inorganic materials 0.000 description 3
- 239000000956 alloy Substances 0.000 description 3
- 230000008859 change Effects 0.000 description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 229910000808 amorphous metal alloy Inorganic materials 0.000 description 2
- 229910052802 copper Inorganic materials 0.000 description 2
- 239000010949 copper Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000004907 flux Effects 0.000 description 2
- 239000011347 resin Substances 0.000 description 2
- 229920005989 resin Polymers 0.000 description 2
- 229910000702 sendust Inorganic materials 0.000 description 2
- 206010011224 Cough Diseases 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000007667 floating Methods 0.000 description 1
- 230000020169 heat generation Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 230000001050 lubricating effect Effects 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 230000001681 protective effect Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野]
本発明は、光磁気記録媒体に対して変調磁界を印加する
ための光磁気記録用磁界発生装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magnetic field generator for magneto-optical recording for applying a modulated magnetic field to a magneto-optical recording medium.
光磁気記録用磁界発注装置は、これまでにも種々のもの
が提案されている。この中には情報の書き換えが可能な
光磁気ディスクを光磁気記録媒体とする光磁気記録用磁
界発生装置がある。これは光磁気ディスクに情報を記録
する場合、第5図に示すようにして行う。この方法は、
いわゆる重ね書き(オーバーライド)が可能な磁界変調
方法であり、光磁気ディスク31の垂直磁化膜31aに
光学ピンクアップ32からのレーザ光を照射し、垂直磁
化膜31aの温度をキューリー点以上に上げておいて、
磁界発生装置33による磁場を磁界変調回路34による
記録信号で変調し、垂直磁化膜31aに磁場変化のパタ
ーンに対応した磁気パターンを残すことにより、情報の
記録を行うというものである。Various types of magnetic field ordering devices for magneto-optical recording have been proposed so far. Among them, there is a magnetic field generating device for magneto-optical recording which uses a rewritable magneto-optical disk as a magneto-optical recording medium. When recording information on a magneto-optical disk, this is done as shown in FIG. This method is
This is a magnetic field modulation method that allows so-called overwriting, in which the perpendicular magnetization film 31a of the magneto-optical disk 31 is irradiated with laser light from the optical pink-up 32 to raise the temperature of the perpendicular magnetization film 31a above the Curie point. Leave it behind.
Information is recorded by modulating the magnetic field from the magnetic field generator 33 with a recording signal from the magnetic field modulation circuit 34 and leaving a magnetic pattern corresponding to the pattern of magnetic field changes on the perpendicularly magnetized film 31a.
このような磁界変調方法において、磁界を光磁気ディス
クに印加させる構成には次のようなものがある。先ず、
磁界発生装置が、光磁気ディスク方向への移行や光磁気
ディスクの回転に対しても接触しないような離れた位置
(例えば0.1〜1.0mmの間隔を置いた位置)にあ
るように制御された状態で磁界を光磁気ディスクに印加
する構成がある。次に、板ハネ等で光磁気ディスク方向
に付勢された磁界発生装置が、潤滑保護膜を塗布した光
磁気ディスクに対向し、光磁気ディスクの回転により発
生する流動空気圧力により磁界発生装置全体が浮上した
際に、前記付勢力と浮上刃を調整して磁界発生装置と光
磁気ディスクとの間を5〜101JflI程度の距離と
した状態で磁界を光磁気ディスクに印加する構成がある
。In such a magnetic field modulation method, there are the following configurations for applying a magnetic field to a magneto-optical disk. First of all,
Control so that the magnetic field generator is located at a distant position (e.g., at a distance of 0.1 to 1.0 mm) so that it does not come into contact with movement in the direction of the magneto-optical disk or rotation of the magneto-optical disk. There is a configuration in which a magnetic field is applied to the magneto-optical disk in a state where the magnetic field is Next, the magnetic field generating device, which is urged in the direction of the magneto-optical disk by a plate blade or the like, is opposed to the magneto-optical disk coated with a lubricating protective film, and the entire magnetic field generating device is moved by the flowing air pressure generated by the rotation of the magneto-optical disk. There is a configuration in which when the magneto-optical disk is levitated, a magnetic field is applied to the magneto-optical disk with the distance between the magnetic field generating device and the magneto-optical disk being approximately 5 to 101 JflI by adjusting the biasing force and the floating blade.
前者の構成は、磁界発生装置が光磁気ディスク面と光分
離れた位置にあるので、両者が接触するという事態を防
止でき、両者の耐久性の向上を図れる。一方、この構成
は、磁界発生装置に大きな起磁力が要求される。例えば
、光磁気ディスクを磁化するに充分な磁界150e (
エルステッド)以上を発生させるためには、数10AT
(アンペア・タン)以上の起磁力が必要となるのである
。In the former configuration, since the magnetic field generating device is located at a position optically separated from the magneto-optical disk surface, it is possible to prevent the two from coming into contact with each other, thereby improving the durability of both. On the other hand, this configuration requires a large magnetomotive force from the magnetic field generator. For example, a magnetic field 150e (
Ørsted) In order to generate more than 10 AT
(Ampere Tan) or more is required.
後者の構成は、磁界発生装置が光磁気ディスクに充分近
づいているため、起磁力は小さくてすむが、両者が接触
してしまうおそれがあり、両者の耐久性に問題を生じて
しまう。In the latter configuration, since the magnetic field generating device is sufficiently close to the magneto-optical disk, the magnetomotive force can be small, but there is a risk that the two may come into contact with each other, which poses a problem in the durability of both.
ところで従来例のうち特開平1−152002号公報に
は、光磁気記録用電磁コイルのコア先端外周部に磁気遮
蔽体を被着した内容が開示しである。しかしこの磁気遮
蔽体は、コア露出部の大きさを小径化して記録密度の向
上、記録容量の増大を図るためのもので、コアに発生し
た熱を放出するようには構成されていない。By the way, among the conventional examples, Japanese Unexamined Patent Publication No. 1-152002 discloses that a magnetic shield is attached to the outer periphery of the core tip of an electromagnetic coil for magneto-optical recording. However, this magnetic shield is intended to reduce the size of the core exposed portion to increase recording density and recording capacity, and is not configured to release heat generated in the core.
また、特開昭63−53701号公報には、高周波変調
磁界発生装置の主磁極の一端を先細り形状とし、磁界発
生の特性を向上させるようにした内容が開示しである。Further, Japanese Patent Application Laid-Open No. 63-53701 discloses that one end of the main pole of a high-frequency modulated magnetic field generator is tapered to improve the characteristics of magnetic field generation.
主磁極の形状をこのように形成すると必要以上に電流を
供給しなくとも伸い磁界が得られるので、発熱等を抑え
ることができるが、磁界発生装置を光磁気記録媒体に対
し、充分に離れた位置に配設した構成のものに適用した
場合、ある程度の発熱は生してしまう。しかし、この従
来例では発生熱の放熱に関する構成は開示されていない
。If the shape of the main magnetic pole is formed in this way, an elongated magnetic field can be obtained without supplying more current than necessary, so heat generation etc. can be suppressed. When applied to a device configured to be disposed at a certain position, a certain amount of heat will be generated. However, this conventional example does not disclose a configuration for dissipating the generated heat.
前記従来技術のうち磁界発生装置を光磁気記録媒体に対
し、充分に離れた位置に配設する構成の場合をさらに説
明する。この構成により光磁気記録媒体に高密度記録を
するために、励磁周波数をI MHz以上に上げるには
、数10AT以上の起磁力を印加することとなる。する
と、磁束の集中する主磁極部のコア損失、コイル損失に
より主磁極部を中心に発熱し、30°以上の温度上昇を
引き起こすこととなってしまう。Among the conventional techniques described above, a case in which the magnetic field generating device is disposed at a position sufficiently distant from the magneto-optical recording medium will be further described. In order to perform high-density recording on a magneto-optical recording medium with this configuration, a magnetomotive force of several tens of AT or more must be applied to increase the excitation frequency to IMHz or more. Then, heat is generated mainly in the main magnetic pole due to core loss and coil loss in the main magnetic pole where magnetic flux is concentrated, causing a temperature rise of 30° or more.
こうした主磁極部を中心とした温度上昇が生じると、主
磁極部位性体の磁化低下による記録磁界が減少する、巻
線の絶縁皮膜が熱的劣化する、主磁極が光磁気記録媒体
に接近することにより光磁気記録媒体の温度が上昇し、
記録磁化パターンが変化して再生出力が変動する等の不
具合が生じる。When such a temperature rise occurs around the main pole, the recording magnetic field decreases due to the decrease in magnetization of the main pole part, the insulation film of the winding deteriorates thermally, and the main pole approaches the magneto-optical recording medium. This causes the temperature of the magneto-optical recording medium to rise,
Problems such as changes in the recorded magnetization pattern and variations in the reproduction output occur.
本発明は、上記不具合を解決すべく提案されるもので、
磁界発生装置を光磁気記録媒体に対し充分に離れた位置
に配設する構成において、主磁極の温度上昇を抑制し、
光磁気記録媒体に高密度記録をすることのできる光磁気
記録用磁界発生装置を提供することを目的としたもので
ある。The present invention is proposed to solve the above-mentioned problems.
In a configuration in which the magnetic field generator is located sufficiently far from the magneto-optical recording medium, the temperature rise of the main magnetic pole is suppressed,
The object of the present invention is to provide a magnetic field generation device for magneto-optical recording that can perform high-density recording on a magneto-optical recording medium.
〔課題を解決するための手段および作用〕本発明は、上
記目的を達成するために、一端が光磁気記録媒体に対向
する主磁極と、咳主磁極の外周に巻回し主磁極を励磁す
る励磁巻線とを有する磁気記録用発生装置において、主
磁極の少なくとも一部を熱伝導性の高い金属材料で形成
し、この金属材料部に放熱部材を連結した光磁気記録用
磁界発生装置としたものである。[Means and effects for solving the problem] In order to achieve the above object, the present invention has a main magnetic pole whose one end faces the magneto-optical recording medium, and an excitation device that is wound around the outer circumference of the cough main magnetic pole to excite the main magnetic pole. A magnetic field generating device for magneto-optical recording having a winding, in which at least a part of the main pole is formed of a metal material with high thermal conductivity, and a heat dissipation member is connected to this metal material part. It is.
このように、金属材料部に放熱フィンを連結したので、
主磁極を中心とした発生熱は金属材料部から放熱部材を
介して、空気中に放出することができ、主磁極近傍の温
度上昇を抑制できることとなる。In this way, since the radiation fins are connected to the metal material part,
The heat generated around the main magnetic pole can be released into the air from the metal material portion via the heat radiating member, making it possible to suppress the temperature rise in the vicinity of the main magnetic pole.
〔実施例〕 以下、図面を参照しながら本発明の詳細な説明する。〔Example〕 Hereinafter, the present invention will be described in detail with reference to the drawings.
第1図は、本発明の詳細な説明するための図である。主
磁極本体1aに熱伝導性の高い金属材から成る主磁極カ
バー4を設けるが、あるいは図示していないが主磁極1
全体を熱電導性の高い金属材で形成する。そして、この
金属材の延在部4aを放熱フィン3aと熱的に連結し、
主磁極1近傍での発主熱を放熱フィン3aを介して空気
中に放出させるようにしている。なお、放熱フィン3a
は、磁界発生装置内およびその周辺に設けている。FIG. 1 is a diagram for explaining the present invention in detail. A main pole cover 4 made of a metal material with high thermal conductivity is provided on the main pole body 1a, or, although not shown, the main pole 1
The entire structure is made of a metal material with high thermal conductivity. Then, the extending portion 4a of the metal material is thermally connected to the radiation fin 3a,
The main heat generated in the vicinity of the main magnetic pole 1 is released into the air via the radiation fins 3a. In addition, the radiation fin 3a
are provided in and around the magnetic field generator.
第2A図は本発明の第1実施例を示したもので全体斜視
図、第2B図は縦断面図である。FIG. 2A shows a first embodiment of the present invention, and is an overall perspective view, and FIG. 2B is a longitudinal sectional view.
上面中央部に小径円柱状の主磁極本体1aを突設した大
径円柱状のボディコア2は、方形台状の熱伝導性の高い
金属材料から成る放熱板3の上に載置固定されている。A large-diameter cylindrical body core 2 with a small-diameter cylindrical main pole body 1a protruding from the center of the upper surface is placed and fixed on a rectangular trapezoidal heat sink 3 made of a metal material with high thermal conductivity. .
主磁極本体1aの上端部は、光磁気記録媒体と対向する
部分であり、ボディコア2は、主磁極本体1aと光磁気
記録媒体とを磁気的に結合する部分である。主磁極本体
1aおよびボディコア2は、Mn−Zn系多結晶フェラ
イト材料から成る。The upper end portion of the main pole body 1a is a portion facing the magneto-optical recording medium, and the body core 2 is a portion that magnetically couples the main pole body 1a and the magneto-optical recording medium. The main pole body 1a and the body core 2 are made of Mn-Zn polycrystalline ferrite material.
主磁極本体1aの外周には、上端部近傍を残して円筒状
の主磁極カバー4を密接するように設けている。この主
磁極カバー4は、ボディコア2の表面を沿い、さらに前
記放熱板3の上面を沿うように延在する脚状の延在部4
aを有している。主磁極カバー4は熱伝導性の高い金属
材料から成り、主磁極本体1aとともに磁界発生装置の
主磁極1を形成している。A cylindrical main pole cover 4 is provided on the outer periphery of the main pole body 1a so as to be in close contact with the main pole body 1a except for the vicinity of the upper end. This main pole cover 4 has leg-shaped extension portions 4 extending along the surface of the body core 2 and further along the upper surface of the heat sink 3.
It has a. The main pole cover 4 is made of a metal material with high thermal conductivity, and forms the main pole 1 of the magnetic field generator together with the main pole body 1a.
主磁極カバー4の外周には、励磁用巻線5を巻回してい
る。そして、磁界変調された高周波の記録信号が励磁用
巻線5に流されると、主磁極1から光磁気記録媒体に対
し、垂直方向の記録信号に応じた磁界が発生し、光磁気
記録媒体に磁界変調記録が行われることとなる。An excitation winding 5 is wound around the outer periphery of the main pole cover 4. When a magnetic field-modulated high-frequency recording signal is sent to the excitation winding 5, a magnetic field corresponding to the recording signal in the perpendicular direction is generated from the main pole 1 to the magneto-optical recording medium. Magnetic field modulation recording will be performed.
上記主磁極カバー4および放熱板3は、熱伝導率の高い
材料により形成する必要がある。そこでアルミ−ニウム
(〜230W/m ・”C)や銅(〜400W /m
・”C)等を用いることが考えられるが、これらは非磁
性材であるため、主磁極カバー4に用いた場合は励磁用
巻線5と主磁極本体1aとの磁気的結合が悪くなり、記
録効率の低下を招くことがある。そこで少なくとも主磁
極本体1aには、熱伝導性、加工性がよ(かつ磁気特性
の優れた金属磁性材料であるアモルファス合金やセンダ
スト合金、パーマロイ合金等を用いた方がよい。The main pole cover 4 and the heat sink 3 need to be made of a material with high thermal conductivity. Therefore, aluminum (~230W/m・"C) and copper (~400W/m
・It is possible to use materials such as "C), but since these are non-magnetic materials, if they are used for the main pole cover 4, the magnetic coupling between the excitation winding 5 and the main pole body 1a will be poor, This may lead to a decrease in recording efficiency.Therefore, at least the main pole body 1a should be made of an amorphous alloy, sendust alloy, permalloy alloy, etc., which are metallic magnetic materials with good thermal conductivity and workability (and excellent magnetic properties). It's better to be there.
本実施例ではこのように構成しであるので、主磁極1を
中心として生じた発生熱は、主磁極カバ4、延在部4a
から放熱板3に効率的に伝熱し、放熱されることとなる
。例えば、光磁気記録媒体に高密度記録するために、I
MH2以上の高周波で30AT以上の起磁力が励磁用
巻線5に印加されると、主磁極本体1a、ボディコア2
は鉄損により、また励磁用巻線5は銅損により発熱する
。特に磁束の集中する主磁極1の近傍は、発熱量が多く
主磁極本体18表面では30°C以上の温度上昇となる
。この場合、主磁極カバー4の熱伝導率が主磁極本体1
aを形成する多結晶フェライト材の熱伝導率(4〜6W
/m・°C)と比較して充分に大きな値50〜300H
/m・°Cに設定されていると、主磁極本体1aで発生
した熱は主磁極カバー4、延在部4aを伝わり、さらに
熱伝導性の高い放熱板3から効率よく空気中に放熱され
てゆくのである。Since this embodiment is configured as described above, the heat generated centering on the main pole 1 is transferred to the main pole cover 4 and the extension portion 4a.
From there, heat is efficiently transferred to the heat sink 3 and the heat is radiated. For example, in order to perform high-density recording on a magneto-optical recording medium, I
When a magnetomotive force of 30 AT or more is applied to the excitation winding 5 at a high frequency of MH2 or more, the main pole body 1a and the body core 2
The excitation winding 5 generates heat due to iron loss, and the excitation winding 5 generates heat due to copper loss. In particular, near the main pole 1 where magnetic flux is concentrated, a large amount of heat is generated, resulting in a temperature rise of 30° C. or more on the surface of the main pole body 18. In this case, the thermal conductivity of the main pole cover 4 is equal to that of the main pole body 1.
Thermal conductivity of the polycrystalline ferrite material forming a (4 to 6 W
/m・°C) sufficiently large value 50 to 300H
/m・°C, the heat generated in the main pole body 1a is transmitted through the main pole cover 4 and the extension portion 4a, and is further efficiently radiated into the air from the heat sink 3, which has high thermal conductivity. I will continue to do so.
このように、この磁界発生装置は、高密度記録時におい
ても主磁極工の温度上昇を周囲温度に対して20″Cし
下とすることができる。そこで、光磁気記録装置の使用
環境温度が60″C程度になったとしでも、フェライト
材料のキューリー点(120〜200°C)近傍におけ
る磁化の低下によって、主磁極発生磁界の低下を招くこ
とがない。また、主磁極1に近接する光磁気記録媒体の
温度上昇によって、記録磁化パターンの変化に起因する
再生出力の低下や変動を招くことがない。さらに、励磁
用巻線5の被覆に用いられる絶縁樹脂が、耐熱温度(1
20〜200℃)近傍で熱変化することもない。In this way, this magnetic field generating device can keep the temperature rise of the main magnetic pole piece 20"C lower than the ambient temperature even during high-density recording. Therefore, the operating environment temperature of the magneto-optical recording device can be lowered by 20"C. Even if the temperature is about 60''C, the magnetic field generated by the main pole will not be reduced due to the reduction in magnetization near the Curie point (120 to 200°C) of the ferrite material. Furthermore, a temperature rise in the magneto-optical recording medium adjacent to the main pole 1 does not cause a decrease or fluctuation in the reproduction output due to a change in the recorded magnetization pattern. Furthermore, the insulating resin used to cover the excitation winding 5 has a heat resistant temperature (1
There is no thermal change in the vicinity of 20 to 200°C.
なお、放熱板3の周辺は、光磁気記録媒体の回転動に伴
い大きな空気流が生じているため、放熱板3の放熱面積
を広く形成すれば、さらに効率的な主磁極1近傍の冷却
を実施できることとなる。Note that a large air flow is generated around the heat sink 3 due to the rotation of the magneto-optical recording medium, so if the heat sink area of the heat sink 3 is made wide, cooling of the vicinity of the main magnetic pole 1 can be made more efficient. This means that it can be implemented.
第3図は、本発明の第2実施例に係る断面図である。第
1実施例に対応する個所には同一符号を付した。本実施
例では、放熱板3に載置固定しであるボディコア3の平
面中央部に、主磁極1と励磁用巻線5を配設するための
凹部を形成し、この凹部の中心部に主磁極lをその底部
が放熱板3に接するとともに下部外周がボディコア2と
密接するように固定する。さらに、主磁極1の上部外周
に励磁用巻線5を巻回する。FIG. 3 is a sectional view according to a second embodiment of the invention. The same reference numerals are given to parts corresponding to those in the first embodiment. In this embodiment, a recess for arranging the main magnetic pole 1 and the excitation winding 5 is formed in the center of the plane of the body core 3 which is placed and fixed on the heat sink 3, and the main magnetic pole is placed in the center of the recess. The magnetic pole l is fixed so that its bottom is in contact with the heat sink 3 and its lower outer periphery is in close contact with the body core 2. Further, an excitation winding 5 is wound around the upper outer periphery of the main pole 1 .
主磁極1は、全体が熱伝導性の高い金属磁性材から成り
、ボディコア2は、フェライト多結晶材から成っている
。そして、それらが放熱板3と接合する底部は、放熱板
3と密接するように平面研磨しである。本実施例は、主
磁極lが第1実施例に比較して単純な形状であるため、
加工性がよく磁性材料の選択範囲も広いという利点があ
る。The main pole 1 is entirely made of a metallic magnetic material with high thermal conductivity, and the body core 2 is made of a ferrite polycrystalline material. The bottom portions where these are joined to the heat sink 3 are surface-polished so that they come into close contact with the heat sink 3. In this embodiment, since the main magnetic pole l has a simpler shape than in the first embodiment,
It has the advantage of good workability and a wide selection range of magnetic materials.
このように構成しているので、主磁極1に発生した熱は
放熱板3に直接伝えられ、空気中に放熱されてゆ(。な
お、主磁極1のみならず、ボディコア2をも含めたコア
全体を熱伝導性の高いアモルファス合金、センダスト合
金等の金属磁性材料により形成してもよいが、これらは
フェライト材料よりも加工が困難であるとともに材料コ
スト面でも不利である。したがって、本実施例のように
主磁極1は、金属磁性材料のロット材(0,2〜0.5
1φ)で形成し、ボディコア2は、フェライト多結晶材
で形成するのが加工性、コスト面で有利である。With this structure, the heat generated in the main magnetic pole 1 is directly transmitted to the heat sink 3 and radiated into the air. The entire structure may be made of a magnetic metal material such as an amorphous alloy or sendust alloy with high thermal conductivity, but these materials are more difficult to process than ferrite materials and are disadvantageous in terms of material cost.Therefore, this embodiment The main magnetic pole 1 is made of a metal magnetic material lot material (0.2~0.5
It is advantageous in terms of workability and cost to form the body core 2 from a ferrite polycrystalline material.
第4図は、本発明の第3実施例に係る縦断面図である。FIG. 4 is a longitudinal sectional view according to a third embodiment of the present invention.
本実施例は、第I実施例と同様に主磁極本体1aとボデ
ィコア2とを一体に形成し、放熱板3に載置固定してい
る。そして、主磁極本体1aの周囲に第2実施例と同様
の励磁用巻線5を配設するための凹部を形成している。In this embodiment, the main pole main body 1a and the body core 2 are integrally formed and mounted and fixed on a heat sink 3, as in the first embodiment. A recessed portion for arranging the excitation winding 5 similar to that of the second embodiment is formed around the main pole body 1a.
また、フェライト材から成る主磁極本体1aの外周に、
上端部のみを残して熱伝導性の高い金属材料から成る円
筒状の主磁極カバー4を密接するように設けている。こ
の主磁極カバー4は、前記励磁用巻!5を配設するため
の凹部表面、さらにボディコア2の表面さらに放熱板3
の上面を沿うように延在する脚状の延在部4aを有して
いる。そして、主磁極カバー4は熱伝導性の高い金属材
料から成り、主磁極本体1aとともに磁界発生装置の主
磁極lを形成している。Further, on the outer periphery of the main pole body 1a made of ferrite material,
A cylindrical main pole cover 4 made of a highly thermally conductive metal material is provided in close contact with the main pole cover 4, leaving only the upper end. This main pole cover 4 is the excitation winding! 5, the surface of the body core 2, and the heat sink 3.
It has a leg-shaped extension part 4a extending along the upper surface of. The main pole cover 4 is made of a metal material with high thermal conductivity, and forms the main pole l of the magnetic field generator together with the main pole body 1a.
主磁極カバー4の外周には、励磁用巻線5を巻回してい
る。また、放熱板3を挾んで主磁極1等を設けている側
と反対側に、磁界発生装置の励磁駆動回路6を設けてお
り、放熱板3は励磁駆動回路60基板の台を兼ねるよう
にしている。そして、励磁駆動回路6の外側にはシール
ドケース7を設け、放熱板3に固定している。An excitation winding 5 is wound around the outer periphery of the main pole cover 4. Furthermore, the excitation drive circuit 6 of the magnetic field generator is provided on the opposite side of the heat sink 3 to the side where the main magnetic pole 1 etc. are provided, and the heat sink 3 is designed to also serve as a stand for the excitation drive circuit 60 board. ing. A shield case 7 is provided outside the excitation drive circuit 6 and fixed to the heat sink 3.
本実施例は、このように構成しているので、放熱板3お
よびシールドケース7がそれぞれ広い放熱面積を有して
おり、磁界発生装置および励磁駆動回路6から生じる熱
を効率よく空中に放出できることとなる。さらに、磁界
発生装置と励磁駆動回路6とが極めて近傍に設けである
ので、高密度記録をする場合に高周波励磁しても、励磁
電流の伝送線路での損失を小さくできるとともに電磁波
ノイズの低減化を図れる。Since the present embodiment is configured in this way, the heat sink 3 and the shield case 7 each have a large heat radiation area, and the heat generated from the magnetic field generator and the excitation drive circuit 6 can be efficiently released into the air. becomes. Furthermore, since the magnetic field generator and the excitation drive circuit 6 are installed very close to each other, even when high-frequency excitation is used for high-density recording, loss in the excitation current transmission line can be reduced, and electromagnetic noise can be reduced. can be achieved.
以上のごとく、本発明によれば主磁極の一部あるいは全
部を熱伝導性の高い金属材料で形成し、磁界発生装置内
等に設けた放熱板に対し伝熱可能に接続しているので、
主磁極を中心として生じるコア損失、巻線損失に伴う発
生熱を効率よく空中に放熱できる。As described above, according to the present invention, part or all of the main pole is made of a highly thermally conductive metal material, and is connected to a heat sink provided in a magnetic field generator or the like so that heat can be transferred.
Heat generated due to core loss and winding loss occurring around the main pole can be efficiently radiated into the air.
したがって、主磁極を中心とした温度上昇に起因する主
磁極磁性体の磁化の低下によって、主磁極発生磁界が低
下するということを防止できる。Therefore, it is possible to prevent the main pole generated magnetic field from decreasing due to a decrease in the magnetization of the main pole magnetic body due to a temperature rise around the main pole.
また、記録磁化パターンの変化に起因する再生出力の低
下や変動を防止できる。また、励磁用巻線の絶縁樹脂の
熱変化を防止できる。このようにして光磁気記録媒体に
高密度記録を適正に行うことが可能となった。Further, it is possible to prevent a decrease or fluctuation in the reproduction output due to a change in the recorded magnetization pattern. Further, thermal changes in the insulating resin of the excitation winding can be prevented. In this way, it has become possible to appropriately perform high-density recording on a magneto-optical recording medium.
第1図は、本発明の詳細な説明するための縦断面図、
第2図A、Bは、本発明の第1実施例を示した斜視図、
同縦断面図、
第3図は、本発明の第2実施例を示した縦断面図、
第4図は、本発明の第3実施例を示した縦断面図、
第5図は、従来の磁界変調方式の原理説明図である。
1・・・主磁極
3・・・放熱板
4・・・主磁極カバー
5・・・励磁用巻線FIG. 1 is a longitudinal sectional view for explaining the present invention in detail; FIGS. 2A and B are perspective views showing the first embodiment of the present invention;
3 is a vertical sectional view showing the second embodiment of the present invention, FIG. 4 is a longitudinal sectional view showing the third embodiment of the present invention, and FIG. 5 is a longitudinal sectional view showing the conventional FIG. 2 is a diagram explaining the principle of a magnetic field modulation method. 1... Main magnetic pole 3... Heat sink 4... Main magnetic pole cover 5... Excitation winding
Claims (1)
極の外周に巻回し主磁極を励磁する励磁巻線とを有する
磁気記録用磁界発生装置において、 主磁極の少なくも一部を熱伝導性の高い金 属材料で形成し、この金属材料部に放熱部材を連結した
ことを特徴とする光磁気記録用磁界発生装置。[Claims] 1. In a magnetic recording magnetic field generator having a main magnetic pole with one end facing the magneto-optical recording medium, and an excitation winding wound around the outer periphery of the main magnetic pole to excite the main magnetic pole, the main magnetic pole 1. A magnetic field generating device for magneto-optical recording, characterized in that at least a portion of the magnetic field generator is made of a metal material having high thermal conductivity, and a heat dissipation member is connected to the metal material portion.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21805690A JPH04102202A (en) | 1990-08-21 | 1990-08-21 | Magnetic field generator for magneto-optical recording |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21805690A JPH04102202A (en) | 1990-08-21 | 1990-08-21 | Magnetic field generator for magneto-optical recording |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04102202A true JPH04102202A (en) | 1992-04-03 |
Family
ID=16713960
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21805690A Pending JPH04102202A (en) | 1990-08-21 | 1990-08-21 | Magnetic field generator for magneto-optical recording |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04102202A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8869860B2 (en) | 2010-03-19 | 2014-10-28 | Fuji Seal International, Inc. | Fitting device |
-
1990
- 1990-08-21 JP JP21805690A patent/JPH04102202A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8869860B2 (en) | 2010-03-19 | 2014-10-28 | Fuji Seal International, Inc. | Fitting device |
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