JPH0531091B2 - - Google Patents
Info
- Publication number
- JPH0531091B2 JPH0531091B2 JP58033298A JP3329883A JPH0531091B2 JP H0531091 B2 JPH0531091 B2 JP H0531091B2 JP 58033298 A JP58033298 A JP 58033298A JP 3329883 A JP3329883 A JP 3329883A JP H0531091 B2 JPH0531091 B2 JP H0531091B2
- Authority
- JP
- Japan
- Prior art keywords
- yoke
- permanent magnet
- electromagnetic force
- coils
- opposite
- 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
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L1/00—Measuring force or stress, in general
- G01L1/08—Measuring force or stress, in general by the use of counterbalancing forces
- G01L1/086—Measuring force or stress, in general by the use of counterbalancing forces using electrostatic or electromagnetic counterbalancing forces
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- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
- Electromagnets (AREA)
Description
【発明の詳細な説明】 (イ) 産業上の利用分野 本発明は電磁力発生装置に関する。[Detailed description of the invention] (b) Industrial application fields The present invention relates to an electromagnetic force generating device.
(ロ) 従来技術
電磁力平衡型の天びん等に用いられる、磁気回
路と電磁コイルから成る従来の電磁力発生装置
は、例えば第1図に示すような構造を有し、永久
磁石11、磁極片12、および内周上部に磁極部
14を有する底付円筒型のヨーク15から成る静
磁気回路の、磁極片12と磁極部14の間に生ず
る磁場と、この磁場に直交して流れる電磁コイル
13の面に直角な方向、即ち、永久磁石の軸方向
に発生するよう構成されている。しかしこのよう
な構造の装置では永久磁石が磁路の縦方向部分に
挿入されているので装置の高さを低くする上で制
限があり、特に天びんの平衡力発生手段に用いる
場合、他の付属機構と合いまつて秤量皿の位置を
低くすることが非常に困難である。また、このよ
うな装置では電磁コイル13に流れる電流のつく
る磁場が静磁気回路の磁場にも影響をおよぼし、
発生する電磁力と電流の間に厳密には線形関係が
成りたたなくなるので、高精度が要求される場合
には、補償コイル16により磁場の補正を行う必
要がある。なお、実開昭55−164519の考案のよう
に、円筒型電磁石の1つの直径に関して対称な両
半円部のそれぞれに、コイル面に垂直で、かつ、
互いに逆向きの静磁場を加え、電磁コイル面内の
上記に直径に垂直な方向に電磁力が発生するよう
構成された電磁力発生装置では、電磁コイルのつ
くる磁場が静磁場におよぼす影響は静磁場の全回
路のわたつて打ち消され、補償コイルによる磁場
補正の必要はない。しかし、この装置では、電磁
力の発生に係わる電磁コイル導体部の有効長さが
幾何学的長さの2/πに減少するという欠点があ
る。これらの欠点を克服し、装置全体の高さが低
く、静磁場の補償手段を要せず、電磁力の発生に
関して電磁コイル導線部の全長が100%有効に作
用する装置として第2図に示すような構成を有す
るものがある。図において、同じ強磁性体より成
る円筒型外側ヨーク3と円筒型内側ヨーク7は同
軸2重円筒型ヨークを構成し、外側ヨーク3の内
面に、磁化の向きが円筒軸の半径方向に向いた環
状の永久磁石2と磁化の向きが反対の永久磁石1
が固着されている。永久磁石2および1と内側ヨ
ーク7の間の間隙にはそれぞれ同軸に形成された
コイル4および5が位置し、共通の巻枠6に保持
されている。巻枠6はヨークの軸方向に可動に保
持されている(保持機構は省略されている)。な
お、外側ヨーク3と内側ヨーク7は、非磁性体よ
り成る支持板8により支持されている。第3図は
第2図におけるコイル部分近傍の部分拡大図であ
り、図において点線と矢印は静磁場の方向を示
し、コイル4および5の断面にはそれぞれコイル
に電流の向きが示されている。図示した磁場およ
び電流の向きでは、コイル全体に下向きの電磁力
が発生するが、図から明らかなように、両コイル
の電流の向きが互いに反対であるため、それらが
つくる磁場の、静磁場への影響は相殺され、従つ
て、静磁場の補償手段は不必要になつている。(b) Prior Art A conventional electromagnetic force generating device consisting of a magnetic circuit and an electromagnetic coil used in an electromagnetic balance type balance has a structure as shown in FIG. 1, for example, and includes a permanent magnet 11, a magnetic pole piece 12, and a magnetic field generated between the magnetic pole piece 12 and the magnetic pole part 14 of a static magnetic circuit consisting of a bottomed cylindrical yoke 15 having a magnetic pole part 14 on the upper inner circumference, and an electromagnetic coil 13 flowing orthogonally to this magnetic field. The magnetic field is generated in a direction perpendicular to the plane of the permanent magnet, that is, in the axial direction of the permanent magnet. However, in devices with this type of structure, the permanent magnets are inserted into the vertical part of the magnetic path, which limits the ability to reduce the height of the device, especially when used as a balance force generating means for a balance. It is very difficult to lower the position of the weighing pan in conjunction with the mechanism. Furthermore, in such a device, the magnetic field created by the current flowing through the electromagnetic coil 13 also affects the magnetic field of the static magnetic circuit.
Strictly speaking, there is no linear relationship between the generated electromagnetic force and the current, so if high accuracy is required, it is necessary to correct the magnetic field using the compensation coil 16. In addition, as in the invention of Utility Model Application No. 55-164519, each of the two semicircular parts symmetrical with respect to one diameter of the cylindrical electromagnet is perpendicular to the coil surface and
In an electromagnetic force generator configured to apply static magnetic fields in opposite directions to generate electromagnetic force in a direction perpendicular to the diameter of the electromagnetic coil, the influence of the magnetic field generated by the electromagnetic coil on the static magnetic field is static. The magnetic field is canceled across the entire circuit, and there is no need for field correction by compensation coils. However, this device has the disadvantage that the effective length of the electromagnetic coil conductor part involved in the generation of electromagnetic force is reduced to 2/π of the geometric length. Figure 2 shows a device that overcomes these drawbacks, has a low overall height, does not require a means for compensating the static magnetic field, and allows the entire length of the electromagnetic coil conductor to work 100% effectively in generating electromagnetic force. Some devices have such a configuration. In the figure, a cylindrical outer yoke 3 and a cylindrical inner yoke 7 made of the same ferromagnetic material constitute a coaxial double cylindrical yoke. Annular permanent magnet 2 and permanent magnet 1 with opposite magnetization direction
is fixed. Coaxially formed coils 4 and 5 are located in the gaps between the permanent magnets 2 and 1 and the inner yoke 7, respectively, and are held by a common winding frame 6. The winding frame 6 is held movably in the axial direction of the yoke (a holding mechanism is omitted). Note that the outer yoke 3 and the inner yoke 7 are supported by a support plate 8 made of a non-magnetic material. FIG. 3 is a partially enlarged view of the vicinity of the coil in FIG. 2. In the figure, dotted lines and arrows indicate the direction of the static magnetic field, and the cross sections of coils 4 and 5 indicate the direction of current in the coils. . In the direction of the magnetic field and current shown in the figure, a downward electromagnetic force is generated throughout the coil, but as is clear from the figure, the direction of the current in both coils is opposite to each other, so the magnetic field created by them is influenced by the static magnetic field. The effects of are canceled out, so that compensating means for the static magnetic field become unnecessary.
しかしながら、これら従来の電磁力発生装置に
おいては、いずれも磁石の強度の可逆温度変化に
よる発生電磁力の温度依存性については何も考慮
されておらず、温度変動があるときは高精度な線
形関係を維持することができず、温度変化の影響
による誤差が問題となつていた。すなわち、一般
に永久磁石の磁場の強さは温度が高くなるほど弱
くなる傾向を有するため、たとえば第2図におい
て磁石2および1付近の温度が高くなるとこれら
磁石による磁場が弱くなりこの磁場に直交して流
れる電磁コイル13の電流との相互作用により発
生する電磁力もまた弱くなるように変動するとい
う問題があつた。 However, in these conventional electromagnetic force generators, no consideration is given to the temperature dependence of the generated electromagnetic force due to reversible temperature changes in the strength of the magnet, and when there are temperature fluctuations, a highly accurate linear relationship is required. It was not possible to maintain this temperature, and errors caused by temperature changes were a problem. In other words, in general, the strength of the magnetic field of a permanent magnet tends to become weaker as the temperature rises, so for example in Fig. 2, as the temperature near magnets 2 and 1 rises, the magnetic field from these magnets becomes weaker and the magnetic field is perpendicular to this magnetic field. There was a problem in that the electromagnetic force generated by the interaction with the flowing current of the electromagnetic coil 13 also varied to become weaker.
(ハ) 目的
本発明の目的は従来技術に伴う上記問題を克服
し、磁石の強度の可逆温度変化すなわち温度変動
の影響も抑制されるよう構成された電磁力発生装
置を提供することにある。(c) Purpose An object of the present invention is to overcome the above-mentioned problems associated with the prior art and to provide an electromagnetic force generating device configured to suppress reversible temperature changes in the strength of a magnet, that is, the influence of temperature fluctuations.
(ニ) 構成
上記の目的を達成するために、本発明による電
磁力発生装置では、
強磁性体の同軸2重円筒型に形成された外側ヨ
ーク内周面と内側ヨーク外周面のうち少なくとも
一方の面に、同軸2重円筒の軸方向に所定の間隔
を隔てて、磁化の向きが同軸2重円筒半径方向外
向きで全体として環状形状を有する第1の永久磁
石と、磁化の向きが第1の永久磁石と反対で全体
として環状形状を有する第2の永久磁石とが固着
されて成る磁気回路と、ヨーク軸方向で内外両ヨ
ークの環状間隙に可動に保持された枠体を巻枠と
して第1および第2の環状コイルが前記第1、第
2の永久磁石に対向して巻回されて成る電磁コイ
ルユニツトとを構成要素とし、第1および第2の
コイルの間にこれら両コイルに流れる電流の向き
が互いに逆向きになるよう回路接続がなされた電
磁力発生機構において、
内外両ヨークの少なくとも一方のヨークは円筒
軸線方向のスリツトで分割形成し、このヨークを
ヨーク自身とは熱膨張係数が異なる支持体により
保持することによつて前記内外両ヨークの間隙を
温度変化に応じて微調整するようにしたことを特
徴とする。(D) Structure In order to achieve the above object, the electromagnetic force generating device according to the present invention has the following features: at least one of the inner circumferential surface of the outer yoke and the outer circumferential surface of the inner yoke formed in a coaxial double cylindrical shape of a ferromagnetic material. A first permanent magnet whose magnetization direction is directed outward in the radial direction of the coaxial double cylinder and has an annular shape as a whole is placed on the surface at a predetermined interval in the axial direction of the coaxial double cylinder; A magnetic circuit is formed by fixing a permanent magnet and a second permanent magnet having an annular shape as a whole opposite to the permanent magnet, and a frame body movably held in the annular gap between the inner and outer yokes in the yoke axis direction as a winding frame. and an electromagnetic coil unit in which first and second annular coils are wound opposite to the first and second permanent magnets, and a current flows between the first and second coils. In an electromagnetic force generation mechanism in which the circuit is connected so that the current direction is opposite to each other, at least one of the inner and outer yokes is divided by a slit in the direction of the cylinder axis, and this yoke has a coefficient of thermal expansion that is different from the yoke itself. The present invention is characterized in that the gap between the inner and outer yokes can be finely adjusted in accordance with temperature changes by holding the inner and outer yokes with different supports.
(ホ) 実施例
以下に、本発明の実施例を図面に基づいて説明
する。第6図は本発明の一実施例の構成を示す図
であり、第5図は本実施例の内側ヨークの構成を
示す斜視図である。図において同じ強磁性体より
成る円筒型外側ヨーク3と円筒型内側ヨーク7は
同軸2重円筒型ヨークを構成し、外側ヨーク3の
内面に、磁化の向きが円筒軸の半径方向に向いた
環状の永久磁石2と、この永久磁石2と磁化の向
きが反対の永久磁石1が固着されている。永久磁
石2および1と内側ヨーク7の間の間隙にはそれ
ぞれ同軸2重円筒型ヨークと同軸に形成されたコ
イル4および5が位置し、共通の巻枠6に保持さ
れている。巻枠6はヨークの軸方向に可動に保持
されている(保持機構は省略されている)。なお、
外側ヨーク3と内側ヨーク7は、非磁性体より成
る支持板8により支持されている。内側ヨーク7
はこのヨーク7自身がもつ熱膨張係数より大きい
熱膨張係数を有する物質から成る円筒9に固着さ
れるとともに、ヨーク自身は同軸2重円筒の軸線
方向に設けられたスリツトにより分割形成され
る。本実施例による構成によれば、円筒9の熱膨
張係数をこのヨーク7自身がもつ熱膨張係数より
大きい熱膨張係数の範囲で適当に選ぶことによ
り、温度変化による内外両ヨーク間の間隙を小さ
くするような変化を与えることができるので、磁
場の強度の可逆変化による発生電磁力の温度依存
性が抑制される。(e) Examples Examples of the present invention will be described below based on the drawings. FIG. 6 is a diagram showing the structure of an embodiment of the present invention, and FIG. 5 is a perspective view showing the structure of the inner yoke of this embodiment. In the figure, a cylindrical outer yoke 3 and a cylindrical inner yoke 7 made of the same ferromagnetic material constitute a coaxial double cylindrical yoke. A permanent magnet 2 and a permanent magnet 1 whose magnetization direction is opposite to this permanent magnet 2 are fixed. In the gaps between the permanent magnets 2 and 1 and the inner yoke 7, coils 4 and 5 formed coaxially with the coaxial double cylindrical yoke are located, respectively, and are held by a common winding frame 6. The winding frame 6 is held movably in the axial direction of the yoke (a holding mechanism is omitted). In addition,
The outer yoke 3 and the inner yoke 7 are supported by a support plate 8 made of a non-magnetic material. inner yoke 7
is fixed to a cylinder 9 made of a material having a coefficient of thermal expansion larger than that of the yoke 7 itself, and the yoke itself is divided by slits provided in the axial direction of the coaxial double cylinder. According to the configuration of this embodiment, by appropriately selecting the thermal expansion coefficient of the cylinder 9 within a range that is larger than the thermal expansion coefficient of the yoke 7 itself, the gap between the inner and outer yokes due to temperature changes can be reduced. Therefore, the temperature dependence of the generated electromagnetic force due to a reversible change in the strength of the magnetic field can be suppressed.
なお、本発明は環状の永久磁石2および1を、
第4図部分切欠斜視図に示すように、円弧上分割
構成して実施することもできる。 In addition, in the present invention, the annular permanent magnets 2 and 1 are
As shown in the partially cutaway perspective view of FIG. 4, it can also be implemented by having a divided structure on an arc.
また、本実施例では内側ヨーク7をこの内外ヨ
ーク自身がもつ熱膨張係数より大きい熱膨張係数
を有する物質から成る円筒9の外周面に固着され
たが、これとは逆に外側ヨーク3をこの内外ヨー
ク自身がもつ熱膨張係数より小さい熱膨張係数を
有する物質から成る環状支持体の内周面に固着し
てもよい。 Further, in this embodiment, the inner yoke 7 is fixed to the outer peripheral surface of the cylinder 9 made of a material having a coefficient of thermal expansion larger than that of the inner and outer yokes themselves. The inner and outer yokes may be fixed to the inner circumferential surface of an annular support made of a material having a coefficient of thermal expansion smaller than that of the inner and outer yokes themselves.
(ヘ) 効果
以上の説明から明らかなように、本発明によれ
ば、電磁力発生装置に温度変化が発生して永久磁
石の磁場の強さが変動したときでも、熱膨張係数
の違いを利用して内外両ヨークの間隙をその温度
変化に応じて微調整できるようにし、これにより
磁石の磁場の強さの変動分を打ち消すようにした
ことで、発生する電磁力の変動を抑制することが
でき、温度変動があつても高精度な線形関係を有
する電磁力発生装置を提供できる。(F) Effect As is clear from the above explanation, according to the present invention, even when a temperature change occurs in the electromagnetic force generating device and the strength of the magnetic field of the permanent magnet fluctuates, the difference in thermal expansion coefficients can be utilized. This allows the gap between the inner and outer yokes to be finely adjusted according to temperature changes, thereby canceling out fluctuations in the strength of the magnet's magnetic field, thereby suppressing fluctuations in the electromagnetic force generated. Therefore, it is possible to provide an electromagnetic force generating device that has a highly accurate linear relationship even when there are temperature fluctuations.
第1図は従来技術による電磁力発生装置の構成
図である。第2図は従来技術による電磁力発生装
置の他の例の構成図である。第3図は第2図に示
す従来例の作用を説明するための部分拡大図であ
る。第4図は本発明の他の実施例における外側ヨ
ークと永久磁石の構成を示す部分切欠斜視図であ
る。第5図は第6図に示す本発明実施例における
内側ヨークの構成を示す斜視図であり、第6図は
本発明による電磁力発生装置の実施例の構成図で
ある。
1,2,11……永久磁石、3……外側ヨー
ク、4,5,13……電磁コイル、6……巻枠、
7……内側ヨーク、8……支持板、9……内側ヨ
ーク支持円筒、16……補償コイル。
FIG. 1 is a block diagram of an electromagnetic force generating device according to the prior art. FIG. 2 is a configuration diagram of another example of an electromagnetic force generating device according to the prior art. FIG. 3 is a partially enlarged view for explaining the operation of the conventional example shown in FIG. FIG. 4 is a partially cutaway perspective view showing the structure of an outer yoke and a permanent magnet in another embodiment of the present invention. FIG. 5 is a perspective view showing the configuration of the inner yoke in the embodiment of the present invention shown in FIG. 6, and FIG. 6 is a configuration diagram of the embodiment of the electromagnetic force generating device according to the present invention. 1, 2, 11... Permanent magnet, 3... Outer yoke, 4, 5, 13... Electromagnetic coil, 6... Winding frame,
7... Inner yoke, 8... Support plate, 9... Inner yoke support cylinder, 16... Compensation coil.
Claims (1)
ヨーク内周面と内側ヨーク外周面のうち少なくと
も一方の面に、同軸2重円筒の軸方向に所定の間
隔を隔てて、磁化の向きが同軸2重円筒半径方向
外向きで全体として環状形状を有する第1の永久
磁石と、磁化の向きが第1の永久磁石と反対で全
体として環状形状を有する第2の永久磁石とが固
着されて成る磁気回路と、ヨーク軸方向で内外両
ヨークの環状間隙に可動に保持された枠体を巻枠
として第1および第2の環状コイルが前記第1、
第2の永久磁石に対向して巻回されて成る電磁コ
イルユニツトとを構成要素とし、第1および第2
のコイルの間にこれら両コイルに流れる電流の向
きが互いに逆向きになるよう回路接続がなされた
電磁力発生機構において、 内外両ヨークの少なくとも一方のヨークは円筒
軸線方向のスリツトで分割形成し、このヨークを
ヨーク自身とは熱膨張係数が異なる支持体により
保持することによつて前記内外両ヨークの間隙を
温度変化に応じて微調整するようにしたことを特
徴とする電磁力発生装置。[Claims] 1. At least one of the inner circumferential surface of the outer yoke and the outer circumferential surface of the inner yoke formed in the shape of a coaxial double cylinder made of ferromagnetic material is provided with a predetermined interval in the axial direction of the coaxial double cylinder. Separated from each other, a first permanent magnet whose magnetization direction is directed outward in the radial direction of a coaxial double cylinder and has an annular shape as a whole, and a second permanent magnet whose magnetization direction is opposite to that of the first permanent magnet and which has an annular shape as a whole. The first and second annular coils include a magnetic circuit having a permanent magnet fixed thereto, and a frame movably held in the annular gap between the inner and outer yokes in the yoke axis direction.
an electromagnetic coil unit wound opposite to a second permanent magnet;
In an electromagnetic force generating mechanism in which a circuit is connected between two coils so that the directions of current flowing through the two coils are opposite to each other, at least one of the inner and outer yokes is divided by a slit in the direction of the cylinder axis, An electromagnetic force generating device characterized in that the gap between the inner and outer yokes can be finely adjusted according to temperature changes by holding the yoke by a support member having a coefficient of thermal expansion different from that of the yoke itself.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3329883A JPS59159034A (en) | 1983-02-28 | 1983-02-28 | Electromagnetic-force generating device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3329883A JPS59159034A (en) | 1983-02-28 | 1983-02-28 | Electromagnetic-force generating device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59159034A JPS59159034A (en) | 1984-09-08 |
| JPH0531091B2 true JPH0531091B2 (en) | 1993-05-11 |
Family
ID=12382636
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3329883A Granted JPS59159034A (en) | 1983-02-28 | 1983-02-28 | Electromagnetic-force generating device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59159034A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5485748A (en) * | 1994-01-26 | 1996-01-23 | Zeamer; Geoffrey H. | Magnetically levitated force/weight measurement system |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3955638A (en) * | 1975-03-05 | 1976-05-11 | Voland Corporation | Precision balance |
| CH586897A5 (en) * | 1975-07-22 | 1977-04-15 | Mettler Instrumente Ag | |
| CH654411A5 (en) * | 1981-06-02 | 1986-02-14 | Mettler Instrumente Ag | ELECTRIC SCALE. |
-
1983
- 1983-02-28 JP JP3329883A patent/JPS59159034A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59159034A (en) | 1984-09-08 |
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