JPS6214336A - Optical driving device - Google Patents

Optical driving device

Info

Publication number
JPS6214336A
JPS6214336A JP15242985A JP15242985A JPS6214336A JP S6214336 A JPS6214336 A JP S6214336A JP 15242985 A JP15242985 A JP 15242985A JP 15242985 A JP15242985 A JP 15242985A JP S6214336 A JPS6214336 A JP S6214336A
Authority
JP
Japan
Prior art keywords
objective lens
yoke
driving device
coil
magnetic flux
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
JP15242985A
Other languages
Japanese (ja)
Inventor
Yasuo Suzuki
康夫 鈴木
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 JP15242985A priority Critical patent/JPS6214336A/en
Publication of JPS6214336A publication Critical patent/JPS6214336A/en
Pending legal-status Critical Current

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  • Mechanical Optical Scanning Systems (AREA)
  • Optical Recording Or Reproduction (AREA)

Abstract

PURPOSE:To miniaturize a device by forming a supporting axis consisting of a ferromagnetic body and constituting a part of a magnetic circuit with it. CONSTITUTION:In a magnetic circuit consisting of a permanent magnet 6b, a supporting axis 1, a fixed yoke 11 and yokes 5a and 5b, by electromagnetic force generated by magnetic flux between permanent magnets 6a and 6b and the supporting axis 1 and current on a coil 10, and the electromagnetic force generated by magnetic flux H1 and magnetic flux H2 and the current on the coil 10, an objective lens supporting body 3 is slid in upper and lower directions, a focus control is performed. So that an objective lens driving device is constituted, the supporting axis 1 which is formed with the ferromagnetic body and the base plate of which is formed with the fixed yoke 11, magnetic flux density in the magnetic circuit is strengthened, and the supporting axis 1 functions as the inside yoke of the objective lens supporting body 3, eliminate the need for the inside yoke. Thereby, the structure of the device is simplified, with the number of parts reduced, and the device of inexpensive and miniaturized can be obtained.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は光学系駆動装置に係り、特に光学系保持体が支
持軸に対し少なくとも摺動又は回動可能に設けられ、電
磁力を用いてこの光学系保持体を駆動する光学系駆動装
置に関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to an optical system driving device, and in particular, an optical system holder is provided so as to be at least slidable or rotatable with respect to a support shaft, The present invention relates to an optical system drive device that drives this optical system holder.

〔従来の技術〕[Conventional technology]

一般に光デイスク装置、光磁気ディスク装置あるいはデ
ジタルオーディオ装置等においては、対物レンズを情報
記録媒体の半径方向に移動させてトラッキング制御を行
い、また情報記録媒体と垂直方向に移動させてフォーカ
ス制御を行う事によって、情報記録媒体から情報を読み
取る方式が用いられている。
Generally, in optical disk devices, magneto-optical disk devices, digital audio devices, etc., tracking control is performed by moving the objective lens in the radial direction of the information recording medium, and focus control is performed by moving the objective lens in the direction perpendicular to the information recording medium. Depending on the situation, a method of reading information from an information recording medium is used.

以下、図面を用いて従来の対物レンズ駆動装置について
説明する。
A conventional objective lens driving device will be described below with reference to the drawings.

第5図は従来の対物レンズ駆動装置の斜視図である。FIG. 5 is a perspective view of a conventional objective lens driving device.

第6図(−)は上記対物レンズ駆動装置の組立図であり
、(b)は(&)の組立図における合板部Mの平面図で
ある。
FIG. 6(-) is an assembled view of the objective lens driving device, and FIG. 6(b) is a plan view of the plywood portion M in the assembled view of (&).

第6図(1)に示すように合板16上に第1のヨーク1
2、及び支持軸1が固着される。支持軸1には軸受部材
2をかいして対物レンズ保持体3が取)付けられる。こ
の対物レンズ保持体3の頂部には対物レンズ4が取り付
けられ、側面部には第1のコイル10が巻かれ、この第
1のコイル】0上には4つの長方形の第2のコイル9m
+9b+9 e 、9 dが設けられる。又、台板16
上には永久磁石14が固着され、この永久磁石14上に
、2つの切り欠き部を有する第2のヨーク15が固着さ
れる。第5図に示すように、この第2のヨーク15は前
記4つの第2のコイル9m 、9b 。
As shown in FIG. 6(1), the first yoke 1 is placed on the plywood 16.
2, and the support shaft 1 are fixed. An objective lens holder 3 is attached to the support shaft 1 through a bearing member 2. An objective lens 4 is attached to the top of the objective lens holder 3, a first coil 10 is wound around the side surface, and four rectangular second coils 9m are mounted on the first coil.
+9b+9e and 9d are provided. Also, the base plate 16
A permanent magnet 14 is fixed on the top, and a second yoke 15 having two notches is fixed on the permanent magnet 14. As shown in FIG. 5, this second yoke 15 includes the four second coils 9m and 9b.

9o、9dの一部を覆うように配置される。第6図(b
)に示すように、台板16は対物レンズ4の可動範囲に
合わせて光窓13が開孔される。
It is arranged so as to cover part of 9o and 9d. Figure 6 (b
), the base plate 16 has an optical window 13 opened in accordance with the movable range of the objective lens 4.

対物レンズ保持体3の内側に設けられた第1のヨーク1
2と第2のヨーク15との間にできる磁界と、第1のコ
イル10に流す電流とによって生ずる電磁力(F+)に
よって前記対物レンズ保持体3は上下摺動し、フォーカ
ス制御がなされる。
A first yoke 1 provided inside the objective lens holder 3
The objective lens holder 3 is slid up and down by the electromagnetic force (F+) generated by the magnetic field created between the objective lens holder 2 and the second yoke 15 and the current flowing through the first coil 10, and focus control is performed.

又、前記磁界と第2のコイル9m+9b、9c。Also, the magnetic field and the second coils 9m+9b, 9c.

9dに流す電流とによって生ずる電磁力(F! )によ
って前記対物レンズ保持体3は左右回動し、トラッキン
グ制御がなされる。
The objective lens holder 3 is rotated left and right by the electromagnetic force (F!) generated by the current flowing through the lens 9d, and tracking control is performed.

対物レンズ保持体3の追従性能は前述した電磁力Fl 
、F、によって決められる。この電磁力F1*F1は次
式で示される。
The tracking performance of the objective lens holder 3 is determined by the electromagnetic force Fl described above.
,F,. This electromagnetic force F1*F1 is expressed by the following equation.

Fl 、F、=  BINl [N] B:磁束密度[T) I :電  流  〔A〕 N:コイルのターン数〔回〕 l;磁界中のコイルの良さ〔m〕 従って、従来の装置では、第1のヨーク12及び第2の
ヨーク15を用いて、高い磁束布1iBが得られる磁気
回路を構成していた。
Fl, F, = BINl [N] B: Magnetic flux density [T] I: Current [A] N: Number of turns of the coil [times] l: Strength of the coil in the magnetic field [m] Therefore, in the conventional device, The first yoke 12 and the second yoke 15 were used to configure a magnetic circuit capable of obtaining a high magnetic flux distribution of 1 iB.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかしながら、従来の光学系駆動装置は、対物レンズ保
持体3内に第1のヨーク12を配置する複雑な構造を有
し、部品数、製造工程の増加を招いていた。また大きな
中空の対物レンズ保持体が必要で、装置が大型化し易い
欠点があった。
However, the conventional optical system drive device has a complicated structure in which the first yoke 12 is disposed within the objective lens holder 3, resulting in an increase in the number of parts and the manufacturing process. Furthermore, a large hollow objective lens holder is required, which has the disadvantage that the apparatus tends to be large-sized.

〔問題点を解決するための手段〕[Means for solving problems]

上記の問題点は支持軸と、前記支持軸に対し少なくとも
摺動又は回動可能に設けられた光学系保持体と、前記光
学系保持体に固定されたコイルと、前記コイルに対し磁
界を形成する磁気回路とを備えた光学系駆動装置におい
て、前記支持軸が強磁性体から成り、前記磁気回路の一
部を構成することを特徴とする本発明の光学系駆動装置
によって解決される。
The above problem consists of a support shaft, an optical system holder that is provided to be at least slidable or rotatable with respect to the support shaft, a coil fixed to the optical system holder, and a magnetic field that forms a magnetic field for the coil. The problem is solved by the optical system driving device of the present invention, characterized in that the support shaft is made of a ferromagnetic material and constitutes a part of the magnetic circuit.

〔実施例〕〔Example〕

以下、本発明の実施例について図面を用いて説明する。 Embodiments of the present invention will be described below with reference to the drawings.

なお、以下の説明では、本発明の光学系駆動装置の実施
例として対物レンズ駆動装置の場合を取ね上げる。
In the following description, an objective lens driving device will be discussed as an example of the optical system driving device of the present invention.

第1図は本発明の1実施例である対物レンズ駆動装置の
斜視図である。
FIG. 1 is a perspective view of an objective lens driving device that is an embodiment of the present invention.

第2図は前記対物レンズ駆動装置の組立図である。FIG. 2 is an assembly diagram of the objective lens driving device.

第3図は前記対物レンズ駆動装置の平面図である。FIG. 3 is a plan view of the objective lens driving device.

第2図において、合板となる固定ヨーク11に、支持軸
1が固着される。該支持軸10両側にはヨーク5aと永
久磁石6a1ヨーク5bと永久磁石6bが固着される。
In FIG. 2, a support shaft 1 is fixed to a fixed yoke 11 made of plywood. A yoke 5a, a permanent magnet 6a1, a yoke 5b and a permanent magnet 6b are fixed to both sides of the support shaft 10.

対物レンズ保持体3は対物レンズ4及び軸受部材2とを
有し、その側面にはコイル9m、コイル9b、コイル1
0が設けられている。第1図に示すように、上記支持軸
1に軸受部材2を通して対物レンズ保持体3が設置され
る。
The objective lens holder 3 has an objective lens 4 and a bearing member 2, and has a coil 9m, a coil 9b, and a coil 1 on its side.
0 is set. As shown in FIG. 1, an objective lens holder 3 is installed on the support shaft 1 through a bearing member 2. As shown in FIG.

この設置された対物レンズ保持体3に設けられたコイル
9a*9bの一部を覆うように、永久磁石8aとヨーク
7畠、永久磁石8bとヨーク7bが固定ヨーク11に固
着される。第2図に示したように前記コイル9m、9b
は長方形状であり、今これらのコイル10の巻方向と垂
直な方向をA部。
A permanent magnet 8a and a yoke 7b, and a permanent magnet 8b and a yoke 7b are fixed to a fixed yoke 11 so as to partially cover the coils 9a*9b provided on the objective lens holder 3 thus installed. As shown in FIG. 2, the coils 9m and 9b
are rectangular in shape, and the direction perpendicular to the winding direction of these coils 10 is called A section.

B部と呼ぶ。It is called part B.

次に上記光学系の駆動装置の作用について説明する。Next, the operation of the drive device for the optical system will be explained.

第4図は前記対物レンズ駆動装置によって作られる磁気
回路の説明図である。
FIG. 4 is an explanatory diagram of a magnetic circuit created by the objective lens driving device.

永久磁石gm、支持軸1.固定ヨーク11.ヨーク7a
によりて構成される磁気回路中の永久磁石8畠と支持軸
1との間の磁界(Hl )と、この磁界(Hr)中のコ
イル910B部に流れる電流とで生ずる電磁力によって
支持軸1を中心とした回転力を得る。コイル9bは前記
コイル9&と逆向きにコイルが巻かれているために、同
様にして、永久磁石8bと支持軸1との間の磁界(Hm
)と、この磁界(H3)中のコイル9bのA部に流れる
電流とで生ずる電磁力も前記回転力と同一方向に働く。
Permanent magnet gm, support shaft 1. Fixed yoke 11. Yoke 7a
The support shaft 1 is moved by the electromagnetic force generated by the magnetic field (Hl) between the permanent magnets 8 in the magnetic circuit and the support shaft 1, and the current flowing through the coil 910B in this magnetic field (Hr). Obtain a centered rotational force. Since the coil 9b is wound in the opposite direction to the coil 9&, the magnetic field (Hm
) and the current flowing through the section A of the coil 9b in this magnetic field (H3).The electromagnetic force generated by this magnetic field (H3) also acts in the same direction as the rotational force.

従ってコイル9m、9bに流す電流の方向を切り換える
事により、対物レンズ保持体3は左右に回動し、対物レ
ンズ4はトラツキツク方向(光軸と垂直方向)に回動す
る事となり、トラッキング制御がなされる。
Therefore, by switching the direction of the current flowing through the coils 9m and 9b, the objective lens holder 3 is rotated left and right, and the objective lens 4 is rotated in the tracking direction (perpendicular to the optical axis), which allows tracking control. It will be done.

一方、第4図に示した永久磁石6b、支持軸1゜固定ヨ
ーク11.ヨーク5a I 5bとで構成される磁気回
路において、永久磁石6m、6bと支持軸lとの間の磁
界とコイル10に流れる電流とで生ずる電磁力及び前記
磁界(Ht)+磁界(馬)とコイル10に流れる電流と
で生ずる電磁力とによって、対物レンズ保持体3は上下
方向に摺動し、対物レンズ4がフォーカス方向(光軸方
向)に移動してフォーカス制御がなされる。対物レンズ
保持体3を上下方向に摺動するには、左右方向に回動す
る場合に比べて大きな電磁力が必要となる。
On the other hand, the permanent magnet 6b, the support shaft 1° fixed yoke 11. In a magnetic circuit composed of yokes 5a and 5b, the electromagnetic force generated by the magnetic field between the permanent magnets 6m and 6b and the support shaft l and the current flowing through the coil 10, and the magnetic field (Ht) + magnetic field (horse) Due to the electromagnetic force generated by the current flowing through the coil 10, the objective lens holder 3 slides in the vertical direction, and the objective lens 4 moves in the focus direction (optical axis direction) to perform focus control. In order to slide the objective lens holder 3 in the vertical direction, a larger electromagnetic force is required than in the case of rotating it in the horizontal direction.

電磁力(F)は前述したように F=BINl(N) なる式で示され、上式から磁束密度(B)を大きくすれ
ば電磁力(F)が大きくなる事がわかる。
As mentioned above, the electromagnetic force (F) is expressed by the formula F=BINl(N), and it can be seen from the above formula that the electromagnetic force (F) increases as the magnetic flux density (B) increases.

本発明による対物レンズ駆動装置は支持軸1を強磁性体
とし、合板を固定ヨーク11とした事により第4図に示
した磁気回路中の磁束密度を高め、又支持軸1が対物レ
ンズ保持体3の内側のヨークの役割りをはたし、内側の
ヨークは不用となるので、対物レンズ駆動装置を小型か
つ軽量にする事ができる。
In the objective lens driving device according to the present invention, the support shaft 1 is made of a ferromagnetic material and the fixed yoke 11 is made of plywood, thereby increasing the magnetic flux density in the magnetic circuit shown in FIG. 3, and the inner yoke is not needed, so the objective lens driving device can be made smaller and lighter.

前記実施例において対物レンズ保持体に取り付けるコイ
ルを3個として配賦したが、コイルの数は追従性能、対
物レンズ保持体の重置等によって決められ、3個に限定
されることはない。
In the above embodiment, three coils are attached to the objective lens holder, but the number of coils is determined by tracking performance, overlapping of the objective lens holder, etc., and is not limited to three.

〔発明の効果〕〔Effect of the invention〕

以上、詳細に説明したように、本発明の光学系駆動装置
によれば、支持軸を強磁性体としたために磁束密度を高
め電磁力を強くする事ができるので光学系の追従性能を
向上させる事ができ、又光学系保持体の内側のヨークを
除去できるので構造が簡単で、部品数が少なくなり、安
価で、小型な装置を提供する事ができ、加えて軽量化さ
れるために小さな電磁力で光学系保持体を駆動させる事
ができる。
As explained above in detail, according to the optical system driving device of the present invention, since the support shaft is made of ferromagnetic material, the magnetic flux density can be increased and the electromagnetic force can be strengthened, thereby improving the tracking performance of the optical system. In addition, since the inner yoke of the optical system holder can be removed, the structure is simple, the number of parts is reduced, and it is possible to provide an inexpensive and compact device. The optical system holder can be driven by electromagnetic force.

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

第1図は本発明の1実施例である対物レンズ駆動装置の
斜視図である。 第2図は前記対物レンズ駆動装置の組立図である。 第3図は前記対物レンズ駆動装置の平面図である。 第4図は前記対物レンズ駆動装置によって作られる磁気
回路の説明図である。 第5図は従来の対物レンズ駆動装置の斜視図である。 第6図(a)は上記対物レンズ駆動装置の組立図であり
、(b)は(a)の組立図における合板部の平面図であ
る。 1・・・支持軸、2・・・軸受部材、3・・・対物レン
ズ保持体、4・・・対物レンズ、5a r 5b r 
7m + 7b・・・ヨーり、” # 6 b * 8
 a r 8 b ・・・永久磁石、9m。 9b、10・・・コイル、11・・・固定ヨーク。
FIG. 1 is a perspective view of an objective lens driving device that is an embodiment of the present invention. FIG. 2 is an assembly diagram of the objective lens driving device. FIG. 3 is a plan view of the objective lens driving device. FIG. 4 is an explanatory diagram of a magnetic circuit created by the objective lens driving device. FIG. 5 is a perspective view of a conventional objective lens driving device. FIG. 6(a) is an assembled view of the objective lens driving device, and FIG. 6(b) is a plan view of the plywood portion in the assembled view of FIG. 6(a). DESCRIPTION OF SYMBOLS 1... Support shaft, 2... Bearing member, 3... Objective lens holder, 4... Objective lens, 5a r 5b r
7m + 7b...Yaw,"#6 b * 8
a r 8 b...Permanent magnet, 9m. 9b, 10... Coil, 11... Fixed yoke.

Claims (1)

【特許請求の範囲】[Claims] 支持軸と、前記支持軸に対し少なくとも摺動又は回動可
能に設けられた光学系保持体と、前記光学系保持体に固
定されたコイルと、前記コイルに対し磁界を形成する磁
気回路とを備えた光学系駆動装置において、前記支持軸
が強磁性体から成り、前記磁気回路の一部を構成するこ
とを特徴とする光学系駆動装置。
A support shaft, an optical system holder provided at least slidably or rotatably with respect to the support shaft, a coil fixed to the optical system holder, and a magnetic circuit that forms a magnetic field with respect to the coil. What is claimed is: 1. An optical system drive device comprising: an optical system drive device, wherein the support shaft is made of a ferromagnetic material and constitutes a part of the magnetic circuit.
JP15242985A 1985-07-12 1985-07-12 Optical driving device Pending JPS6214336A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15242985A JPS6214336A (en) 1985-07-12 1985-07-12 Optical driving device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15242985A JPS6214336A (en) 1985-07-12 1985-07-12 Optical driving device

Publications (1)

Publication Number Publication Date
JPS6214336A true JPS6214336A (en) 1987-01-22

Family

ID=15540328

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15242985A Pending JPS6214336A (en) 1985-07-12 1985-07-12 Optical driving device

Country Status (1)

Country Link
JP (1) JPS6214336A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6439641A (en) * 1987-08-05 1989-02-09 Seiko Epson Corp Objective lens actuator
US9463453B2 (en) 2012-07-04 2016-10-11 Mitsubishi Hitachi Power Systems, Ltd. Method for producing NOx removal catalyst for high-temperature exhaust gas

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6439641A (en) * 1987-08-05 1989-02-09 Seiko Epson Corp Objective lens actuator
JP2621200B2 (en) * 1987-08-05 1997-06-18 セイコーエプソン株式会社 Objective lens actuator
US9463453B2 (en) 2012-07-04 2016-10-11 Mitsubishi Hitachi Power Systems, Ltd. Method for producing NOx removal catalyst for high-temperature exhaust gas

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