JPH04184740A - Magneto-optical disc device - Google Patents

Magneto-optical disc device

Info

Publication number
JPH04184740A
JPH04184740A JP31703190A JP31703190A JPH04184740A JP H04184740 A JPH04184740 A JP H04184740A JP 31703190 A JP31703190 A JP 31703190A JP 31703190 A JP31703190 A JP 31703190A JP H04184740 A JPH04184740 A JP H04184740A
Authority
JP
Japan
Prior art keywords
coil
yoke
height
center yoke
sectional area
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
Application number
JP31703190A
Other languages
Japanese (ja)
Inventor
Takao Matsui
伯夫 松井
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP31703190A priority Critical patent/JPH04184740A/en
Publication of JPH04184740A publication Critical patent/JPH04184740A/en
Pending legal-status Critical Current

Links

Landscapes

  • Moving Of Heads (AREA)
  • Reciprocating, Oscillating Or Vibrating Motors (AREA)

Abstract

PURPOSE:To increase an output per a unit space of a voice coil motor by making the height of a coil surrounding a center yoke approximately the same as that of a side yoke, on the inside of which a permanent magnet is installed, while the sectional area of the side yoke is made the same as or larger than that of the center yoke. CONSTITUTION:A magnetic circuit is composed of a center yoke 12 surrounded by a coil 11, a permanent magnet 13 oppositely faced to the coil 11 from the outside of the coil 11 and a side yoke 14 on the outside of the magnet 13. The height Hc of the coil 11 is made approximately the same as that Hy of the side yoke 14 while the sectional area Am of the center yoke 12 is made the same as or smaller than that As of the side yoke 14 at that time. When currents are conducted through the coil 11, electromagnetic force is generated by the line of magnetic force generated by the center yoke 12, the permanent magnet 13 and the side yoke 14 constituting the magnetic circuit, a carriage 2 can be driven in the direction orthogonal to a paper surface. Accordingly, an output from a voice coil motor per a unit space is increased.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、光ピツクアップを搭載するキャリッジを、電
磁力を利用して移動させるためのボイスコイルモータを
有する光磁気ディスク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 magneto-optical disk device having a voice coil motor for moving a carriage carrying an optical pickup using electromagnetic force.

[従来の技術] 第6図は従来の磁気光学効果を利用して情報を記録再生
する装置の駆動系の一例を示している。
[Prior Art] FIG. 6 shows an example of a drive system of a conventional apparatus for recording and reproducing information using the magneto-optic effect.

固定光学系lから出射されたレーザー光はキャリッジ2
に設けられた図示しない光軸折り曲げミラーを経て対物
レンズ3に入射する。アクチュエータ4が対物レンズ3
を駆動することにより、回転するディスクDに対してオ
ートフォーカシング、オートトラッキングがなされ、デ
ィスクロ上における情報の記録再生がレーザー光によっ
て行われる。
The laser beam emitted from the fixed optical system l is sent to the carriage 2.
The light enters the objective lens 3 through an optical axis bending mirror (not shown) provided in the. Actuator 4 is objective lens 3
By driving the disc D, auto-focusing and auto-tracking are performed on the rotating disc D, and information is recorded and reproduced on the disc D using a laser beam.

アクチュエータ4だけの駆動では、ディスクロ上の情報
の記録再生できる範囲が狭いため、対物レンズ3を駆動
するアクチュエータ4をキャリッジ2に搭載し、ディス
クDの半径方向に移動させることにより、情報の配録再
生可能な範囲をディスクDの略全周域に確保している。
If only the actuator 4 is driven, the range in which information can be recorded and reproduced on the disc is narrow. Therefore, the actuator 4 that drives the objective lens 3 is mounted on the carriage 2 and moved in the radial direction of the disc D, thereby changing the arrangement of information. A recordable and reproducible range is secured over substantially the entire circumference of the disc D.

キャリッジ2はベアリングによって転がり支持され、ヨ
ーク5と永久磁石6の組合わせによる磁気回路と、キャ
リッジ2に取り付けられたコイル7とにより構成される
ボイスコイルモータによって発生する電磁力によってキ
ャリッジ2は駆動される。
The carriage 2 is rolled and supported by bearings, and is driven by electromagnetic force generated by a voice coil motor composed of a magnetic circuit formed by a combination of a yoke 5 and a permanent magnet 6, and a coil 7 attached to the carriage 2. Ru.

ここで、第7図は一般的なボイスコイルモータの構成を
示し、磁気回路は′鉄系の材質から成るヨーク部材によ
って構成された直方体を組合わせた環体であるヨーク5
の一長辺内側に永久磁石6を設け、これに対向するヨー
ク5の長辺の周囲にコイル7を設ける。コイル7に通電
し、磁気回路によって発生する磁力との間の相互作用で
電磁力を発生させ、対象物の移動のための駆動力Fを得
る。
Here, FIG. 7 shows the configuration of a general voice coil motor, in which the magnetic circuit consists of a yoke 5 which is a ring body made up of a combination of rectangular parallelepipeds made of yoke members made of iron-based materials.
A permanent magnet 6 is provided inside one long side of the yoke 5, and a coil 7 is provided around the long side of the yoke 5 facing the permanent magnet 6. The coil 7 is energized to generate an electromagnetic force through interaction with the magnetic force generated by the magnetic circuit, thereby obtaining a driving force F for moving the object.

第8図は光磁気ディスク装置に一般的に用いられるボイ
スコイルモータの断面図の一例を示し、装置の略中夫に
キャリッジ2が配置され、キャリッジ2の両側に対称的
にボイスコイルモータが配置されている。キャリッジ2
の両側面にはコイル7が取り付けられており、コイル7
の内側にセンタヨーク5aが挿通され、更にコイル7の
外側に永久磁石6とサイドヨーク5bが配置され、これ
らによって2組の磁気回路が構成されている。
FIG. 8 shows an example of a cross-sectional view of a voice coil motor commonly used in a magneto-optical disk device, in which a carriage 2 is arranged approximately in the middle of the device, and the voice coil motors are arranged symmetrically on both sides of the carriage 2. has been done. Carriage 2
Coils 7 are attached to both sides of the coil 7.
A center yoke 5a is inserted inside the coil 7, and a permanent magnet 6 and a side yoke 5b are arranged outside the coil 7, and these constitute two sets of magnetic circuits.

また、サイドヨーク5bの高さをHy、コイル7の高さ
をHc、センタヨーク5aの高さをH■で示している。
Further, the height of the side yoke 5b is indicated by Hy, the height of the coil 7 is indicated by Hc, and the height of the center yoke 5a is indicated by H■.

[発明が解決しようとする課題1 しかしながら上述の従来例では、ボイスコイルモータの
最大高さはコイル7の高さHcにより決定される。これ
は、コイル7の内寸にセンタヨーク5aの高さH園を合
わせ、それに合わせてサイドヨーク5bの高さHyを決
めているからである。このため、サイドヨーク5bとコ
イル7の高さの差の分(Hc−Hy)だけ空きスペース
が生じてしまい、そこに無駄な空間が生ずる。これでは
空間の効率的な利用とはならず、任意の空間内で可能な
限りの効率を高めたボイスコイルモータ得ることができ
ない。
[Problem to be Solved by the Invention 1] However, in the conventional example described above, the maximum height of the voice coil motor is determined by the height Hc of the coil 7. This is because the height H of the center yoke 5a is matched to the inner dimension of the coil 7, and the height Hy of the side yoke 5b is determined accordingly. Therefore, an empty space is created by the difference in height between the side yoke 5b and the coil 7 (Hc-Hy), resulting in wasted space. This does not result in efficient use of space, and it is not possible to obtain a voice coil motor with the highest possible efficiency within a given space.

また、ボイスコイルモータの出力は、磁気回路の発生す
る磁力、コイル7の巻数、通電する電流値、及び磁力線
をコイル7が横切る有効長の積で決まるが、従来例では
有効長がほぼサイドヨーク5bの高さHyと等しくなり
、略コイル高さHcに対して有効長が短い。このため、
コイル7の有効長よりも長い分は無駄となり、ボイスコ
イルモータの単位体積当たりの出力の減少につながる。
In addition, the output of the voice coil motor is determined by the product of the magnetic force generated by the magnetic circuit, the number of turns of the coil 7, the value of the current flowing, and the effective length that the coil 7 crosses the lines of magnetic force.In the conventional example, the effective length is approximately equal to the side yoke. It is equal to the height Hy of 5b, and the effective length is shorter than approximately the coil height Hc. For this reason,
A length longer than the effective length of the coil 7 is wasted, leading to a decrease in the output per unit volume of the voice coil motor.

本発明の目的は、上述の欠点を解消し、ボイスコイルモ
ータの単位空間当たりの出力が大きい光磁気ディスク装
置を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks and provide a magneto-optical disk device in which the voice coil motor has a large output per unit space.

[課題を解決するための手!] 上述の目的を達成するために、本発明に係る光磁気ディ
スク装置においては、キャリッジを駆動するボイスコイ
ルモータの磁気回路のうち、センタヨークを囲むコイル
の高さを、永久磁石を内側に設けたサイドヨークの高さ
と略同等とすると共に、磁路内を通過する磁束を確保す
るために前記サイドヨークの断面積を前記センタヨーク
の断面積と同等又はそれよりも大きくしたことを特徴と
するものである。
[Hands to solve problems! ] In order to achieve the above object, in the magneto-optical disk device according to the present invention, in the magnetic circuit of the voice coil motor that drives the carriage, the height of the coil surrounding the center yoke is adjusted such that a permanent magnet is provided inside. The height of the side yokes is approximately equal to that of the center yoke, and the cross-sectional area of the side yoke is equal to or larger than the cross-sectional area of the center yoke in order to ensure magnetic flux passing through the magnetic path. It is something.

[作用] 上述の構成を有する光磁気ディスク装置は、与えられた
空間を効率良く使用することができ、またコイルの有効
長部が長くなるためコイル長の無駄な部分の割合が低く
なり、単位空間当たりのボイスコイルモータの出力効率
が高い。
[Function] The magneto-optical disk device having the above-mentioned configuration can efficiently use the given space, and since the effective length of the coil becomes long, the ratio of wasted portions of the coil length is reduced, and the unit The output efficiency of the voice coil motor per space is high.

[実施例] 本発明を第1図〜第5図に図示の実施例に基づいて詳細
に説明する。なお、従来例と同一の符号は同一の部材を
表している。
[Example] The present invention will be described in detail based on the example illustrated in FIGS. 1 to 5. Note that the same reference numerals as in the conventional example represent the same members.

第1図は第1の実施例の断面図、第2図は磁力線の分布
図を示し、第1図において、アクチュエータ4を搭載し
紙面に垂直な方向に可動に支持されたキャリッジ2に関
して左右対称に磁気回路が配置され、キャリッジ2の左
右側面にコイル11が取り付けられている。磁気回路は
コイル11に囲まれたセンタヨーク12とコイル11の
外側からコイル11に対向する永久磁石13と更にその
外側のサイドヨーク14とによって構成されている。こ
こで、コイル11の高さをHc、サイドヨーク14の高
さをHy、センタヨーク12の高さをHsa、センタヨ
ーク12の断面積をA園、サイドヨーク14の断面積を
Asで示され、次の関係式を満足している。
Fig. 1 shows a cross-sectional view of the first embodiment, and Fig. 2 shows a distribution diagram of magnetic lines of force. A magnetic circuit is arranged on the carriage 2, and coils 11 are attached to the left and right sides of the carriage 2. The magnetic circuit is composed of a center yoke 12 surrounded by a coil 11, a permanent magnet 13 facing the coil 11 from the outside of the coil 11, and a side yoke 14 further outside. Here, the height of the coil 11 is Hc, the height of the side yoke 14 is Hy, the height of the center yoke 12 is Hsa, the cross-sectional area of the center yoke 12 is A, and the cross-sectional area of the side yoke 14 is As. , satisfies the following relational expression.

HC>Hll          ・・・filHc#
Hy                ・・・ (2)
Age4 As  又は All<AS   −f31
fi1式はセンタヨーク12がコイル11に囲まれてい
るため当然必要な条件であり、(2)式はサイドヨーク
14の高さの条件、(3)式はサイドヨーク14の断面
積の条件である。
HC>Hll...filHc#
Hy... (2)
Age4 As or All<AS-f31
The formula fi1 is a necessary condition because the center yoke 12 is surrounded by the coil 11, the formula (2) is a condition for the height of the side yoke 14, and the formula (3) is a condition for the cross-sectional area of the side yoke 14. be.

コイル11に電流を通電することにより、磁気回路を構
成するセンタヨーク12と永久磁石13とサイドヨーク
14により発生する磁力線によって電磁力が発生し、キ
ャリッジ2を紙面と直交方向に駆動することができる。
By applying current to the coil 11, electromagnetic force is generated by magnetic lines of force generated by the center yoke 12, permanent magnets 13, and side yokes 14 that constitute a magnetic circuit, and the carriage 2 can be driven in a direction perpendicular to the plane of the paper. .

ここで、センタヨーク12の断面積Amを通過する磁束
と、サイドヨークの断面積Asを通過する磁束の大きさ
はほぼ等しいので、センタヨーク12の断面積Amとサ
イドヨーク14の断面積Asをほぼ等しいか、又はサイ
ドヨーク14の断面積Asをセンタヨーク12の断面積
Amよりも太き(しておけば、磁界の漏洩が殆どない閉
磁路を構成できるので、磁気回路中の磁束の利用効率が
高まる。
Here, since the magnitude of the magnetic flux passing through the cross-sectional area Am of the center yoke 12 and the magnetic flux passing through the cross-sectional area As of the side yokes are almost equal, the cross-sectional area Am of the center yoke 12 and the cross-sectional area As of the side yokes 14 are If the cross-sectional area As of the side yoke 14 is approximately equal to or larger than the cross-sectional area Am of the center yoke 12, a closed magnetic path with almost no magnetic field leakage can be constructed, so that the magnetic flux in the magnetic circuit can be utilized. Increased efficiency.

コイル11の有効長はほぼコイル高さHcと等しくなっ
ており、第2図に示す磁力線の分布より、永久磁石13
及びサイドヨーク14を通る磁束をほぼ全面的に活用で
きるので、コイル長の無駄な部分の割合が少なくなり、
単位空間当たりの出力が高い。
The effective length of the coil 11 is approximately equal to the coil height Hc, and from the distribution of magnetic lines of force shown in FIG.
Since the magnetic flux passing through the side yoke 14 can be utilized almost entirely, the proportion of wasted portions of the coil length is reduced.
High output per unit space.

第3図は第2の実施例を示し、磁気回路がキャリッジ2
の移動方向である紙面と直交する方向及び鉛直方向に平
行な平面内に構成され、コイル21の上方に永久磁石2
2が配置され、その上にサイドヨーク23が配置されて
いる。この場合も、第1の実施例と同様な効果が得られ
る。
FIG. 3 shows a second embodiment in which the magnetic circuit is connected to the carriage 2.
The permanent magnet 2 is arranged above the coil 21 in a direction perpendicular to the plane of the paper, which is the moving direction of the coil 21, and in a plane parallel to the vertical direction.
2 is arranged, and a side yoke 23 is arranged thereon. In this case as well, the same effects as in the first embodiment can be obtained.

第4図は第3の実施例を示し、センタヨーク31、コイ
ル32、永久磁石33に曲率を持たせているので、永久
磁石33とセンタヨーク31間のギャップ長が略等しく
均一の分布が得られる。
FIG. 4 shows a third embodiment, in which the center yoke 31, the coil 32, and the permanent magnet 33 have curvature, so that the gap length between the permanent magnet 33 and the center yoke 31 is approximately equal, and a uniform distribution is obtained. It will be done.

第5図は第4の実施例を示し、第2の実施例で示した磁
気回路を上側だけでなく下側にも設け、上下対称に配置
している。この場合は有効長が単純に2倍になるので、
上下磁気回路中の磁束が第2の実施例と同程度であれば
出力が2倍になる。
FIG. 5 shows a fourth embodiment, in which the magnetic circuit shown in the second embodiment is provided not only on the upper side but also on the lower side, and arranged symmetrically above and below. In this case, the effective length simply doubles, so
If the magnetic flux in the upper and lower magnetic circuits is about the same as in the second embodiment, the output will be doubled.

なお、上述の実施例において、磁気回路の配置はキャリ
ッジ2の両側に対して対称としたが、同様な構成をキャ
リッジ2の片側だけのものとしてもよい。
In the above-described embodiment, the magnetic circuits were arranged symmetrically on both sides of the carriage 2, but a similar configuration may be provided only on one side of the carriage 2.

[発明の効果] 以上説明したように本発明に係る光磁気ディスク装置は
、単位空間当たりのボイスコイルモータ出力が太き(、
磁気回路のスペースファクタが良好なため、装置が小型
化できる。
[Effects of the Invention] As explained above, the magneto-optical disk device according to the present invention has a large voice coil motor output per unit space (
Since the magnetic circuit has a good space factor, the device can be made smaller.

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

図面第1図〜第5図は本発明に係る光磁気ディスク装置
の実施例を示し、第1図は第1の実施例のボイスコイル
モータの断面図、第2図はその磁力線分布図、第3図、
第4図、第5図はそれぞれ第2、第3、第4の実施例の
ボイスコイルモータの断面図であり、第6図は従来の光
磁気ディスク装置のボイスコイルモータの斜視図、第7
図は一般的なボイスコイルモータの構成図、第8図は従
来例のボイスコイルモータの断面図である。 符号2はキャリッジ、4はアクチュエータ、11.21
.32はコイル、12.31はセンタヨーク、13.2
2.33は永久磁石、14.23はサイドヨークである
。 特許出願人  キャノン株式会社 第2図 第3図
1 to 5 show an embodiment of the magneto-optical disk device according to the present invention, FIG. 1 is a sectional view of the voice coil motor of the first embodiment, FIG. 2 is a distribution diagram of lines of magnetic force, and FIG. Figure 3,
4 and 5 are sectional views of voice coil motors of second, third, and fourth embodiments, respectively, and FIG. 6 is a perspective view of a voice coil motor of a conventional magneto-optical disk device.
The figure is a configuration diagram of a general voice coil motor, and FIG. 8 is a sectional view of a conventional voice coil motor. 2 is the carriage, 4 is the actuator, 11.21
.. 32 is the coil, 12.31 is the center yoke, 13.2
2.33 is a permanent magnet, and 14.23 is a side yoke. Patent applicant Canon Co., Ltd. Figure 2 Figure 3

Claims (1)

【特許請求の範囲】[Claims] 1、キャリッジを駆動するボイスコイルモータの磁気回
路のうち、センタヨークを囲むコイルの高さを、永久磁
石を内側に設けたサイドヨークの高さと略同等とすると
共に、磁路内を通過する磁束を確保するために前記サイ
ドヨークの断面積を前記センタヨークの断面積と同等又
はそれよりも大きくしたことを特徴とする光磁気ディス
ク装置。
1. In the magnetic circuit of the voice coil motor that drives the carriage, the height of the coil surrounding the center yoke is approximately equal to the height of the side yokes with permanent magnets installed inside, and the magnetic flux passing through the magnetic path is A magneto-optical disk device characterized in that the cross-sectional area of the side yokes is equal to or larger than the cross-sectional area of the center yoke in order to ensure the following.
JP31703190A 1990-11-20 1990-11-20 Magneto-optical disc device Pending JPH04184740A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31703190A JPH04184740A (en) 1990-11-20 1990-11-20 Magneto-optical disc device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP31703190A JPH04184740A (en) 1990-11-20 1990-11-20 Magneto-optical disc device

Publications (1)

Publication Number Publication Date
JPH04184740A true JPH04184740A (en) 1992-07-01

Family

ID=18083656

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31703190A Pending JPH04184740A (en) 1990-11-20 1990-11-20 Magneto-optical disc device

Country Status (1)

Country Link
JP (1) JPH04184740A (en)

Similar Documents

Publication Publication Date Title
US4553227A (en) Optical pickup
JP2002352452A (en) Optical pickup actuator
JPH04184740A (en) Magneto-optical disc device
US5561646A (en) Focus/tracking actuator with moving-magnet motors
KR100486279B1 (en) An optical pickup actuator and an optical disk drive using the same
KR100300379B1 (en) Actuating device for optical pick-up
JPS59121636A (en) Electromagnetic type driving device
JP2005038496A (en) Objective lens driving device for optical head
JP4046665B2 (en) Optical head device
JPH06119725A (en) Voice coil linear motor
JP2000090456A (en) Objective lens drive assembly and optical disk device
JPH053056B2 (en)
JPS6319946Y2 (en)
JPH08194962A (en) Biaxial actuator
JPS60202551A (en) Optical head for optical information recording and reproducing
JP2560977Y2 (en) Head device for magneto-optical disk
JPH0660406A (en) Driving device for objective lens
JPH05325218A (en) Objective lens driving device
JPH06301992A (en) Lens moving device
JPH0319103A (en) Bias magnetic field supply device
JPH0863908A (en) Linear motor
JPS6337830A (en) Movable magnet type two-dimensional actuator
JPH08180433A (en) Optical pickup
JPH035934A (en) Objective lens driving device
JPH01277376A (en) Recording and reproducing device