JPH0662315U - Automatic vertical magnetic braking system - Google Patents
Automatic vertical magnetic braking systemInfo
- Publication number
- JPH0662315U JPH0662315U JP5424692U JP5424692U JPH0662315U JP H0662315 U JPH0662315 U JP H0662315U JP 5424692 U JP5424692 U JP 5424692U JP 5424692 U JP5424692 U JP 5424692U JP H0662315 U JPH0662315 U JP H0662315U
- Authority
- JP
- Japan
- Prior art keywords
- braking
- pendulum
- radius
- plate
- automatic vertical
- 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
Landscapes
- Dynamo-Electric Clutches, Dynamo-Electric Brakes (AREA)
Abstract
(57)【要約】
【目的】 振子の揺動を制動する制動力を、振子の下端
の制動板がどの位置に運動しても常に一定になるように
して制動性能を向上させる
【構成】 振子3の下端の制動板13を、振子の揺動支
点を中心とした半径R1の円弧状に湾曲させるととも
に、制動用磁石14・15を、同揺動支点を中心とした
半径R1より大きい半径R2の円弧線上に配置する。
(57) [Abstract] [Purpose] Improving the braking performance by making the braking force for braking the swing of the pendulum always constant regardless of the position of the brake plate at the lower end of the pendulum [Configuration] Pendulum The braking plate 13 at the lower end of 3 is curved in an arc shape with a radius R1 centered on the swing fulcrum of the pendulum, and the braking magnets 14 and 15 have a radius R2 larger than the radius R1 centered on the swing fulcrum. Place on the arc line of.
Description
【0001】[0001]
本考案は、レーザ光線等の光線を振子から投射する自動鉛直器において、振子 の揺動を磁力により制動する磁気制動装置に関する。 The present invention relates to a magnetic braking device for braking swing of a pendulum by magnetic force in an automatic vertical device that projects a light beam such as a laser beam from a pendulum.
【0002】[0002]
自動鉛直器には、投射するレーザ光線等の光線を自動的に鉛直に補正して常に 一つの光学的鉛直線を作るために、振子を常に鉛直状態にする自動補正機構が備 えられている。また、その補正を効果的に行うために振子の揺動を制動装置で制 動するようになっている。 The automatic vertical device is equipped with an automatic correction mechanism that keeps the pendulum in the vertical state in order to automatically correct the projected light beam such as laser beam to make one optical vertical line. . Further, in order to effectively perform the correction, the swing of the pendulum is controlled by a braking device.
【0003】 図1及び図2に従来のこの種の自動鉛直装置を示す。この自動鉛直装置は、架 台1の上板2に円筒形の振子3をジンバル機構4によって揺動自在に懸垂してい る。振子3内にはレーザ光線を投射する投光系5が設けられている。ジンバル機 構4は、上板2上の一対の軸受6に、リング7を第1の軸8でX方向に揺動自在 に支承するとともに、振子3の上端部を、該リング7に第1の軸8と軸線が直角 な軸9によってY方向に揺動自在に支承したもので、架台1が振動しても振子3 は重力で常に鉛直に保たれるようになっている。1 and 2 show a conventional automatic vertical device of this type. In this automatic vertical device, a cylindrical pendulum 3 is suspended by a gimbal mechanism 4 on an upper plate 2 of a pedestal 1 so as to be swingable. A light projecting system 5 for projecting a laser beam is provided in the pendulum 3. The gimbal mechanism 4 supports the ring 7 on the pair of bearings 6 on the upper plate 2 so as to be swingable in the X direction by the first shaft 8, and the upper end portion of the pendulum 3 is attached to the ring 7 at the first position. The shaft 8 is rotatably supported in the Y direction by a shaft 9 whose axis is perpendicular to the shaft 8. Even if the pedestal 1 vibrates, the pendulum 3 is always kept vertically by gravity.
【0004】 振子3の下端には、銅や銀等の金属製の制動板10が固着され、また架台1の ベース11上にはX方向の2組の制動用磁石12とY方向の2組の制動用磁石1 3とが配設されている。制動板10は上下面が平行な単に平らな円板であり、ま た制動用磁石12・13は同一水平面上に位置している。A braking plate 10 made of metal such as copper or silver is fixed to the lower end of the pendulum 3, and two sets of braking magnets 12 in the X direction and two sets in the Y direction are mounted on the base 11 of the pedestal 1. And the braking magnet 13 of FIG. The braking plate 10 is a simple flat disc whose upper and lower surfaces are parallel to each other, and the braking magnets 12 and 13 are located on the same horizontal plane.
【0005】 制動板10が動くと制動用磁石12・13の磁力線を切ることになるため、制 動板10に局部的に渦電流が生じ、制動板10にその運動方向と反対方向の制動 力が働く。この制動力Fは一般的には、F=K(dφ)/R(dt)で表される 。ここで、Kは比例定数、Rは電気抵抗であり、制動力Fは単位時間(dt)に おける磁束の変化の割合(dφ)に比例する。When the braking plate 10 moves, the lines of magnetic force of the braking magnets 12 and 13 are cut, so that an eddy current is locally generated in the braking plate 10, and the braking force in the direction opposite to the movement direction of the braking plate 10 is generated. Works. This braking force F is generally represented by F = K (dφ) / R (dt). Here, K is a proportional constant, R is an electric resistance, and the braking force F is proportional to the rate of change (dφ) of the magnetic flux per unit time (dt).
【0006】[0006]
しかし、これは、制動板10が磁石12・13に対して平行に運動した場合の 条件であり、上記従来の構造では、図3に示すように磁石12・13から見て制 動板10に平行運動のみならず上下方向の運動も加わるため、同方向の磁石にお いて制動板10との距離が異なることになり、a点とb点とでは制動力に差(ア ンバランス)が生じ、制動性能が良くないという問題があった。 However, this is a condition when the braking plate 10 moves in parallel with the magnets 12 and 13, and in the above-described conventional structure, as shown in FIG. Since not only parallel motion but also vertical motion is applied, the distance between the magnets in the same direction and the braking plate 10 is different, and a difference (unbalance) in braking force occurs at points a and b. However, there was a problem that the braking performance was not good.
【0007】 本考案の目的は、制動板と磁石との間の制動力を、制動板がどの位置に運動し ても常に一定になるようにして制動性能を向上させることにある。An object of the present invention is to improve the braking performance by keeping the braking force between the braking plate and the magnet constant at any position of the braking plate.
【0008】[0008]
本考案による磁気制動装置では、振子の下端の制動板を、振子の揺動支点を中 心とした半径R1の円弧状に湾曲させるとともに、制動用磁石を、同揺動支点を 中心とした半径R1より大きい半径R2の円弧線上に配置したものである。 In the magnetic braking device according to the present invention, the braking plate at the lower end of the pendulum is curved in an arc shape having a radius R1 with the swing fulcrum of the pendulum as the center, and the braking magnet has a radius with the swing fulcrum as the center. It is arranged on an arc line having a radius R2 larger than R1.
【0009】[0009]
従って、制動板がどの位置に揺動してもそれと磁石との距離は常に一定で、制 動力がアンバランスになることはない。 Therefore, no matter where the braking plate swings, the distance between it and the magnet is always constant, and the braking force does not become unbalanced.
【0010】[0010]
以下、本考案の実施例を図面に基づき詳細に説明する。 図4に本考案を適用した自動鉛直器を示す。この自動鉛直器は、架台1の上板 2に、円筒形の振子3をジンバル機構4によって図1に示したものと同様に揺動 自在に懸垂しているが、振子3の下端に設けられた制動板13と架台1のベース 11上に配設されたX方向及びY方向の制動磁石14・15とによる磁気制動装 置に、次のような構成を採っている。 Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. FIG. 4 shows an automatic vertical device to which the present invention is applied. In this automatic vertical device, a cylindrical pendulum 3 is suspended by a gimbal mechanism 4 on an upper plate 2 of a pedestal 1 in the same manner as that shown in FIG. The magnetic braking device including the braking plate 13 and the braking magnets 14 and 15 in the X and Y directions arranged on the base 11 of the gantry 1 has the following configuration.
【0011】 制動板13は、振子3の揺動支点Oを中心とした半径R1の球面形(碗形)を なし、また制動磁石14及び15は、いずれも揺動支点Oを中心とした半径R2 (R1>R2)の円弧線上に配置され、しかもそれらの着磁面は、揺動支点Oに 向かって直角になるようにベース11上に固定されている。The braking plate 13 has a spherical shape (a bowl shape) with a radius R1 around the swing fulcrum O of the pendulum 3, and the braking magnets 14 and 15 both have a radius around the swing fulcrum O. They are arranged on the arc line of R2 (R1> R2), and their magnetized surfaces are fixed on the base 11 so as to be perpendicular to the swing fulcrum O.
【0012】 従って、振子3のX方向及びY方向のいずれの方向の揺動についても、制動板 13の下面と制動磁石14及び15との距離は常に一定であり、制動板13の揺 動位置の如何にかかわらず制動力は常に一定になる。Therefore, in both swinging of the pendulum 3 in the X and Y directions, the distance between the lower surface of the brake plate 13 and the brake magnets 14 and 15 is always constant, and the swing position of the brake plate 13 is constant. Regardless of, the braking force is always constant.
【0013】 なお、制動板13は球面形に限らず、図7に示すような2枚もの、つまり揺動 支点Oを中心とした円弧に沿って湾曲するX方向とY方向の2枚の長板13a ・ 13b で構成しても良く、また図8に示すように一方向のみ湾曲する1枚の長板 13a で構成しても良い。It should be noted that the braking plate 13 is not limited to the spherical shape, but two such members as shown in FIG. 7, that is, two lengths in the X direction and the Y direction which are curved along an arc centered on the swing fulcrum O are provided. It may be constituted by the plates 13a and 13b, or may be constituted by one long plate 13a which is curved only in one direction as shown in FIG.
【0014】[0014]
以上述べたとおり本考案の磁気制動装置によれば、振子の下端の制動板を、振 子の揺動支点を中心とした半径R1の円弧状に湾曲させ、また制動用磁石を半径 R1より大きい半径R2の円弧線上に配置したので、制動板がどの位置に揺動し てもそれと磁石との距離は常に一定で、制動力が制動板の揺動によりアンバラン スになることはなく、制動性能を従来よりも向上させることができる。 As described above, according to the magnetic braking device of the present invention, the braking plate at the lower end of the pendulum is curved in an arc shape with a radius R1 centered on the swing fulcrum of the pendulum, and the braking magnet is larger than the radius R1. Since it is placed on the arc line of radius R2, no matter which position the braking plate swings, the distance between it and the magnet is always constant, and the braking force does not become an imbalance due to the swinging of the braking plate. Can be improved over the conventional one.
【図1】従来の自動鉛直器の斜視図である。FIG. 1 is a perspective view of a conventional automatic vertical device.
【図2】同上の断面図である。FIG. 2 is a sectional view of the same.
【図3】同自動鉛直器の磁気制動装置では制動力がアン
バランスなることを示す動作説明図である。FIG. 3 is an operation explanatory view showing that the braking force is unbalanced in the magnetic braking device of the automatic vertical device.
【図4】本考案による磁気制動装置を備えた自動鉛直器
の斜視図である。FIG. 4 is a perspective view of an automatic vertical device including a magnetic braking device according to the present invention.
【図5】同磁気制動装置の動作説明図である。FIG. 5 is an operation explanatory view of the magnetic braking device.
【図6】同磁気制動装置における制動板の斜視図であ
る。FIG. 6 is a perspective view of a braking plate in the magnetic braking device.
【図7】制動板の他の例の斜視図である。FIG. 7 is a perspective view of another example of the braking plate.
【図8】制動板の更に別例の斜視図である。FIG. 8 is a perspective view of still another example of the braking plate.
1 架台 3 振子 4 ジンバル機構 13 制動板 14・15 磁石 1 mount 3 pendulum 4 gimbal mechanism 13 braking plate 14 ・ 15 magnet
Claims (1)
蔵した振子を、ジンバル機構により架台に揺動自在に懸
垂し、該振子の下端に金属製の制動板を設け、また架台
のベース上に制動用磁石を配置した自動鉛直器の磁気制
動装置において、前記制動板を、前記振子の揺動支点を
中心とした半径R1の円弧状に湾曲させるとともに、前
記制動用磁石を、同揺動支点を中心とした半径R1より
大きい半径R2の円弧線上に配置したことを特徴とする
自動鉛直器の磁気制動装置。1. A pendulum having a built-in light projecting system for projecting a light beam such as a laser beam is suspended by a gimbal mechanism so as to be swingable, and a metal braking plate is provided at the lower end of the pendulum. In a magnetic braking device for an automatic vertical device in which a braking magnet is arranged on a base, the braking plate is curved in an arc shape having a radius R1 around a swing fulcrum of the pendulum, and the braking magnet is the same. A magnetic braking device for an automatic vertical device, wherein the magnetic braking device is arranged on an arc line having a radius R2 larger than a radius R1 centered on a swing fulcrum.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5424692U JPH0662315U (en) | 1992-07-10 | 1992-07-10 | Automatic vertical magnetic braking system |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5424692U JPH0662315U (en) | 1992-07-10 | 1992-07-10 | Automatic vertical magnetic braking system |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0662315U true JPH0662315U (en) | 1994-09-02 |
Family
ID=12965190
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5424692U Pending JPH0662315U (en) | 1992-07-10 | 1992-07-10 | Automatic vertical magnetic braking system |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0662315U (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH10141957A (en) * | 1996-11-12 | 1998-05-29 | Touhan Seiki Kk | Laser marking device |
JPH10260040A (en) * | 1997-03-17 | 1998-09-29 | Toyo Techno Kk | Marking device for laser liner |
JPH1130520A (en) * | 1997-07-10 | 1999-02-02 | Daishowa Seiki Co Ltd | Marking device |
JP2004354051A (en) * | 2003-05-26 | 2004-12-16 | Matsushita Electric Works Ltd | Level |
WO2005019771A1 (en) * | 2003-08-26 | 2005-03-03 | Matsushita Electric Works, Ltd. | Level |
KR20160106488A (en) * | 2015-03-02 | 2016-09-12 | 최해용 | A Support Bar for a Virtual Reality Camera |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58145088A (en) * | 1982-02-08 | 1983-08-29 | シ−メンス・アクチエンゲゼルシヤフト | Electric resistor and method of producing same |
JPH0325132U (en) * | 1990-05-10 | 1991-03-14 |
-
1992
- 1992-07-10 JP JP5424692U patent/JPH0662315U/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58145088A (en) * | 1982-02-08 | 1983-08-29 | シ−メンス・アクチエンゲゼルシヤフト | Electric resistor and method of producing same |
JPH0325132U (en) * | 1990-05-10 | 1991-03-14 |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH10141957A (en) * | 1996-11-12 | 1998-05-29 | Touhan Seiki Kk | Laser marking device |
JPH10260040A (en) * | 1997-03-17 | 1998-09-29 | Toyo Techno Kk | Marking device for laser liner |
JPH1130520A (en) * | 1997-07-10 | 1999-02-02 | Daishowa Seiki Co Ltd | Marking device |
JP2004354051A (en) * | 2003-05-26 | 2004-12-16 | Matsushita Electric Works Ltd | Level |
WO2005019771A1 (en) * | 2003-08-26 | 2005-03-03 | Matsushita Electric Works, Ltd. | Level |
KR20160106488A (en) * | 2015-03-02 | 2016-09-12 | 최해용 | A Support Bar for a Virtual Reality Camera |
JP2016218430A (en) * | 2015-03-02 | 2016-12-22 | ヘ−ヨン・チョイ | Support rod device for virtual reality camera |
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