JPH0614777B2 - Voice coil motor - Google Patents
Voice coil motorInfo
- Publication number
- JPH0614777B2 JPH0614777B2 JP17490484A JP17490484A JPH0614777B2 JP H0614777 B2 JPH0614777 B2 JP H0614777B2 JP 17490484 A JP17490484 A JP 17490484A JP 17490484 A JP17490484 A JP 17490484A JP H0614777 B2 JPH0614777 B2 JP H0614777B2
- Authority
- JP
- Japan
- Prior art keywords
- yoke
- magnetic
- gap
- voice coil
- coil motor
- 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
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K33/00—Motors with reciprocating, oscillating or vibrating magnet, armature or coil system
- H02K33/18—Motors with reciprocating, oscillating or vibrating magnet, armature or coil system with coil systems moving upon intermittent or reversed energisation thereof by interaction with a fixed field system, e.g. permanent magnets
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K41/00—Propulsion systems in which a rigid body is moved along a path due to dynamo-electric interaction between the body and a magnetic field travelling along the path
- H02K41/02—Linear motors; Sectional motors
- H02K41/035—DC motors; Unipolar motors
- H02K41/0352—Unipolar motors
- H02K41/0354—Lorentz force motors, e.g. voice coil motors
- H02K41/0356—Lorentz force motors, e.g. voice coil motors moving along a straight path
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Electromagnetism (AREA)
- Reciprocating, Oscillating Or Vibrating Motors (AREA)
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明はディスク駆動装置のボイスコイルモータ(以下
VCMと略称)に係り特に高出力の複数キャリッジ用ア
クチュエータに好適な磁気回路を提供することに関す
る。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a voice coil motor (hereinafter abbreviated as VCM) of a disk drive, and more particularly to providing a magnetic circuit suitable for a high-power actuator for a plurality of carriages.
第1図にデュアクチュエータの従来例を示す。デュアル
アクチュエータとは一式の円板群1に対し2つのキャリ
ッジ2をもっており、これによりディスクのスループッ
トの向上を計っている。FIG. 1 shows a conventional example of a du actuator. The dual actuator has two carriages 2 with respect to a set of disk groups 1 and thereby improves the throughput of the disk.
VCMモータはマグネット3、2ケのポールピース4、
フロントヨーク5、リヤヨーク6より構成され、フロン
トヨーク5のギャプ部に磁束を集中させ、キャリッジの
後部についているコイル7に電流を流すことにより力を
発生し、キャリッジを前後に動かすことが出来る。The VCM motor has a magnet 3, two pole pieces 4,
It is composed of a front yoke 5 and a rear yoke 6. A magnetic flux is concentrated on the gap portion of the front yoke 5 and an electric current is caused to flow through a coil 7 attached to the rear portion of the carriage to generate a force, so that the carriage can be moved back and forth.
第2図にVGMモータの説明図を示す。ポールピース4
の周囲にはコイル電流特性向上用にショートコイル8が
巻いてある。又磁束のフローを矢印で示してある。本モ
ータにおいてコイル7と交絡する磁束量を最大にしよう
とした時のクリティカルポイントは、ポールピース4の
磁気飽和又はフロントヨーク5のA部の磁気の飽和であ
る。FIG. 2 shows an explanatory view of the VGM motor. Pole piece 4
A short coil 8 is wound around to improve the coil current characteristics. Also, the flow of magnetic flux is shown by arrows. In this motor, the critical point when trying to maximize the amount of magnetic flux entangled with the coil 7 is the magnetic saturation of the pole piece 4 or the magnetic saturation of the portion A of the front yoke 5.
今キャリッジ間隙LSはディスクの配列及びアクチュエー
タ当りのヘッド数により決まるので、ギャップ寸法Lg、
ポールピース4の寸法L(他の一方の寸法をRLとす
る)、ポールピース4間ヨーク寸法LCの間にはLS=LC+
2Lg+Lの関係が存在し、LはLCは両方一度に大きく出
来ない。何故ならLCが小さいとヨークA部がすぐ飽和
し、Lが小さいとポールピースが飽和するためである。
ヨークが飽和を起こすとギャプB側とC側でアンバラン
スな磁束となりこの結果キャリッジにアンバランスな力
を発生させ振動や異状マモウ等の原因となる。Since the carriage gap L S is determined by the array of disks and the number of heads per actuator, the gap dimension L g ,
The dimension L of the pole piece 4 (the other dimension is RL) and the yoke dimension L C between the pole pieces 4 are L S = L C +
There is a relationship of 2L g + L, and L and L C cannot both be large at one time. This is because the yoke A portion is saturated immediately when L C is small, and the pole piece is saturated when L is small.
When the yoke is saturated, unbalanced magnetic flux is generated on the gaps B side and C side, and as a result, an unbalanced force is generated on the carriage, which causes vibration and abnormal mamou.
そこでフロントヨーク5のA部での磁束密度Baとポール
ピース4での時速密度Bpがともに等しく、最大Bmaxとな
る場合をkをパラメータに(kはポールピースの縦横
比)計算すると最大値が存在し、Ls=45mm、Tsr=1mm、
Bmax=19KG程度の場合、ポールピース4の最大磁束量Φ
pは、約160KMaxwell程度である。この程度のΦpではキ
ャリッジ重量にもよるが平均アクセスタイムの向上に対
して十分でなく更に大きなΦpが望まれる。(第4図の
α=0の曲線) この為の向上策としては、特開昭55−163813号
公報記載の例があるが、マグネットの配置が難かしく又
ポールピースにマグネットをつけるため大きなマグネッ
トは無理で、結果として大磁束密度を得るのは難かし
い。Therefore, when the magnetic flux density B a at the A portion of the front yoke 5 and the hourly speed density B p at the pole piece 4 are both equal and the maximum is B max , k is a parameter (k is the aspect ratio of the pole piece), and the maximum is calculated. Value exists, L s = 45 mm, T sr = 1 mm,
Maximum magnetic flux Φ of pole piece 4 when B max = 19KG
p is about 160 KM axwell . Although Φ p of this degree is not sufficient for improving the average access time, it depends on the weight of the carriage and a larger Φ p is desired. (Curve with α = 0 in FIG. 4) As an improvement measure for this, there is an example described in JP-A-55-163813, but it is difficult to dispose the magnet and a large magnet for attaching the magnet to the pole piece. Is impossible, and it is difficult to obtain a large magnetic flux density as a result.
本発明の目的は、複数個のポールピースのついたアクチ
ュエータにおいて、フロントヨークの磁気回路を変更す
ることによりギャップ部時速量の大きいVCMモータを
提供することにある。An object of the present invention is to provide a VCM motor having a large gap part speed per hour by changing the magnetic circuit of the front yoke in an actuator having a plurality of pole pieces.
すでに述べたように、本モータの磁気回路的クリティカ
ルパスはフロントヨーク及びポールピースである。本発
明においてはフロントヨークのポールピース間部に磁気
的なバイパスをもうけることによりΦpを大巾に向上が
出来、しかもコイル位置による出力バラツキ(リニアリ
ティと略す)の向上も期待出来るようになった。As described above, the magnetic circuit critical path of this motor is the front yoke and the pole piece. In the present invention, Φ p can be greatly improved by providing a magnetic bypass between the pole pieces of the front yoke, and it is also expected that the output variation (abbreviated as linearity) depending on the coil position can be improved. .
第3図に本発明の一実施例を示す。従来例との相違点は
フロントヨーク5部に補助磁気回路9をつけたことであ
る。本補助磁気回路9は周囲の磁気回路であるヨーク材
に比べて透磁率の高い磁性材のブロックで、通常の使い
方では通常のヨーク材として用いられる材料でも十分で
ある。本ブロック9をつけることにより磁束はこの部分
も通るため、ポールピース4のセンターヨーク部分の磁
束量を上げることが出来る。この結果ポールピース4も
大きく出来、ギャップ部の磁束量を大きくすることが出
来る。FIG. 3 shows an embodiment of the present invention. The difference from the conventional example is that the auxiliary magnetic circuit 9 is attached to the front yoke 5. The auxiliary magnetic circuit 9 is a block of a magnetic material having a higher magnetic permeability than the yoke material that is the surrounding magnetic circuit, and a material used as a normal yoke material is sufficient for normal use. Since the magnetic flux also passes through this portion by attaching the main block 9, the amount of magnetic flux in the center yoke portion of the pole piece 4 can be increased. As a result, the pole piece 4 can be made large, and the amount of magnetic flux in the gap can be increased.
第4図に本ブロックをもうけた時のポールピース4での
磁束量の値とkの関係を示す。パラメータαは補助ブロ
ックとフロントヨーク5のB部の断面積の比でα=0の
時はブロックがないことを示す。FIG. 4 shows the relationship between the value of the amount of magnetic flux in the pole piece 4 and k when this block is provided. The parameter α is the ratio of the cross-sectional areas of the auxiliary block and the portion B of the front yoke 5, and when α = 0 indicates that there is no block.
この図のようにα=1〜2程度となるとΦpはkが3程
度でも250〜300KMx程度と大きな量が確保出来ることが
分かる。As shown in this figure, when α = 1 to 2, Φ p can be secured as large as 250 to 300 KM x even when k is about 3.
次にリニアリティについて考察する。Next, let us consider linearity.
従来形のギャップ部周辺の磁束のフローは第2図に示す
通りでVCMモータ前部の磁気抵抗は、モータ内側に比
べて大きい。このためコイルの位置による出力のリニア
リティは図5の実線のようにコイルが円板内周側に位置
した場合は外周位置に比べリニアリティは悪くなる。こ
れに比べ本実施例においては、マグネット前部にブロッ
クがついているため前部の漏洩磁束が大きくなりこの結
果コイル内周位置での出力が大きくなりリニアリティが
向上する。(第5図の破線) 又ギャップD部とE部では本磁気回路の影響でコイルの
出力が違い、キャリッジにアンバランスな力が発生す
る。これをさける為にギャップの寸法を変えD/E部で
コイルに発生する力を均一にする。The flow of magnetic flux around the conventional gap is as shown in FIG. 2, and the magnetic resistance at the front of the VCM motor is larger than that at the inside of the motor. Therefore, the linearity of the output depending on the position of the coil becomes worse when the coil is located on the inner circumference side of the disk as shown by the solid line in FIG. In contrast to this, in the present embodiment, since the front portion of the magnet is provided with a block, the leakage magnetic flux at the front portion becomes large, and as a result, the output at the coil inner peripheral position becomes large and the linearity is improved. (Dashed line in FIG. 5) In the gaps D and E, the output of the coil is different due to the influence of this magnetic circuit, and an unbalanced force is generated in the carriage. In order to avoid this, the size of the gap is changed to make the force generated in the coil uniform in the D / E section.
以上ポールピースが2ケの場合について述べてきたが、
5ケ以上の複数個でも同様なことが言えることは明らか
である。So far, I have described the case of two pole pieces,
It is clear that the same thing can be said for a plurality of five or more.
以上本発明によれば、VCMモータのフロントヨークの
形状により左右ギャップ部での磁束量が変わるにもかか
わらず、ギャップ部の寸法を変化させることにより左右
均等な力を得ることが出来る。寸法変化量はブロックの
形状により異なるが一度決定されれば変化することはな
いので現物合わせでも簡単に決められる。As described above, according to the present invention, even if the amount of magnetic flux in the left and right gap portions changes depending on the shape of the front yoke of the VCM motor, it is possible to obtain a uniform left and right force by changing the dimensions of the gap portions. The amount of dimensional change varies depending on the shape of the block, but once determined, it does not change, so it can be easily determined by actual matching.
第1図はディスク,キャリッジ,マグネットの側面図、
第2図(a)及び(b)は従来型モータの正面図及び側面断面
図、第3図(a)〜(c)は本発明モータの正面図及び左右側
面断面図、第4図はk(ポールピースの縦横比)とポー
ルピース磁束量の関係を示す図、第5図はコイル位置と
出力のリニアリティの関係を示す図。 1……ディスク、2……キャリッジ、3……磁石、4…
…ポールピース、5……フロントヨーク、6……リアヨ
ーク、7……コイル、8……ショートコイル、9……補
助磁気回路。Figure 1 is a side view of the disk, carriage and magnet.
2 (a) and 2 (b) are a front view and a side sectional view of a conventional motor, FIGS. 3 (a) to 3 (c) are a front view and left and right side sectional views of the motor of the present invention, and FIG. FIG. 5 is a diagram showing a relation between (aspect ratio of pole pieces) and the amount of magnetic flux of pole pieces, and FIG. 5 is a diagram showing a relation between coil position and linearity of output. 1 ... Disc, 2 ... Carriage, 3 ... Magnet, 4 ...
... Pole piece, 5 ... Front yoke, 6 ... Rear yoke, 7 ... Coil, 8 ... Short coil, 9 ... Auxiliary magnetic circuit.
Claims (1)
されたフロントヨークと、該マグネットの後面に配置さ
れたリアヨークと、該リアヨークに配置された少なくと
も2つのボールピースにより磁気回路を形成し、該ポー
ルピースと該フロントヨークとの間隙に移動可能に配置
されたコイルにより、磁気ヘッドを磁気ディスク上に位
置決めする複数のキャリッジを駆動するボイスコイルモ
ータにおいて、 前記フロントヨーク上、前記磁気回路の外側であって、
前記少なくとも2つのボールピースの間に相当する位置
に、磁性材料片を配置し、 該磁性材料片に近い側の前記間隙と、該磁性材料片に遠
い側の前記間隙とを異ならしめたことを特徴とするボイ
スコイルモータ。1. A magnetic circuit is formed by a magnet, a front yoke arranged in front of the magnet, a rear yoke arranged in the rear surface of the magnet, and at least two ball pieces arranged in the rear yoke. A voice coil motor for driving a plurality of carriages for positioning a magnetic head on a magnetic disk by a coil movably arranged in a gap between a pole piece and the front yoke, wherein a voice coil motor is provided on the front yoke and outside the magnetic circuit. There
A magnetic material piece is arranged at a position corresponding between the at least two ball pieces, and the gap on the side close to the magnetic material piece and the gap on the side far from the magnetic material piece are made different from each other. Characteristic voice coil motor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17490484A JPH0614777B2 (en) | 1984-08-24 | 1984-08-24 | Voice coil motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17490484A JPH0614777B2 (en) | 1984-08-24 | 1984-08-24 | Voice coil motor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6154861A JPS6154861A (en) | 1986-03-19 |
JPH0614777B2 true JPH0614777B2 (en) | 1994-02-23 |
Family
ID=15986728
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP17490484A Expired - Lifetime JPH0614777B2 (en) | 1984-08-24 | 1984-08-24 | Voice coil motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0614777B2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5417380B2 (en) * | 2011-06-06 | 2014-02-12 | 株式会社日立ハイテクノロジーズ | Linear motor, movable stage and electron microscope |
-
1984
- 1984-08-24 JP JP17490484A patent/JPH0614777B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS6154861A (en) | 1986-03-19 |
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