JP3009560U - Electromagnetic drive type magneto-optical device - Google Patents
Electromagnetic drive type magneto-optical deviceInfo
- Publication number
- JP3009560U JP3009560U JP1994013076U JP1307694U JP3009560U JP 3009560 U JP3009560 U JP 3009560U JP 1994013076 U JP1994013076 U JP 1994013076U JP 1307694 U JP1307694 U JP 1307694U JP 3009560 U JP3009560 U JP 3009560U
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- Prior art keywords
- magneto
- gap
- magnetic yoke
- magnetic
- bobbin
- 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.)
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Abstract
(57)【要約】
【目的】 装置の小型化を図り、小電力で駆動でき、し
かも応答時間を短縮できるようにする。
【構成】 磁性ヨーク20によって形成する磁気回路中
にギャップ22を設け、該ギャップ内に磁気光学素子2
4を配置し、ギャップを取り囲むようにコイル26を設
ける。2個の同一形状の磁性ヨークを相対向させて配置
する。磁性ヨークは、例えば、中央脚が両側脚よりも短
いE型で、その中央脚を光ビーム通過孔が貫通する構造
とする。ボビンは、磁性ヨークに嵌合する円筒部と、そ
の一端に位置するフランジ部とを一体成形した半ボビン
を、2個、間に素子ホルダを介在させて組み合わせ、素
子ホルダは、円環部の両面にボビン円筒部が嵌合する段
部を形成し、その少なくとも一方の面に磁気光学素子を
取り付けるのがよい。
(57) [Abstract] [Purpose] To reduce the size of the device, drive it with a small amount of power, and shorten the response time. A gap 22 is provided in a magnetic circuit formed by the magnetic yoke 20, and the magneto-optical element 2 is placed in the gap.
4 is arranged, and the coil 26 is provided so as to surround the gap. Two magnetic yokes having the same shape are arranged to face each other. The magnetic yoke is, for example, an E type having a central leg shorter than both side legs, and has a structure in which a light beam passage hole penetrates the central leg. The bobbin is a combination of two half bobbins integrally formed with a cylindrical portion fitted to the magnetic yoke and a flange portion located at one end of the bobbin with an element holder interposed therebetween. It is preferable to form stepped portions on both sides of which the bobbin cylindrical portion fits, and attach the magneto-optical element to at least one surface thereof.
Description
【0001】[0001]
本考案は、電磁石方式で駆動する磁気光学装置に関し、更に詳しく述べると、 磁気回路に形成されているギャップに磁気光学素子を配置し、そのギャップの周 囲にコイルを設けて磁界を印加する電磁駆動式の磁気光学装置に関するものであ る。この装置は、例えは光スイッチあるいは磁界センサなどに有用である。 The present invention relates to a magneto-optical device driven by an electromagnet method. More specifically, the magneto-optical element is arranged in a gap formed in a magnetic circuit, and a coil is provided around the gap to apply a magnetic field. The present invention relates to a drive type magneto-optical device. This device is useful, for example, as an optical switch or a magnetic field sensor.
【0002】[0002]
光通信、光計測、光記録などの分野においては、電磁石によって磁気光学素子 を磁化させる装置が用いられている。その代表的な例は、光スイッチや磁界セン サなどである。このような装置においては、磁性ヨークの一部にギャップを設け て、そのギャップに磁気光学素子を挿入し、磁性ヨークの他の部分にコイルを設 け、その巻線の電流を制御するように構成している。 In fields such as optical communication, optical measurement, and optical recording, a device that magnetizes a magneto-optical element with an electromagnet is used. Typical examples are optical switches and magnetic field sensors. In such a device, a gap is provided in a part of the magnetic yoke, a magneto-optical element is inserted in the gap, a coil is provided in the other part of the magnetic yoke, and the current of the winding is controlled. I am configuring.
【0003】 具体的には、例えば図9のAに示すように、ほぼC型で平板形状の磁性ヨーク 10を用い、ギャップ12内に磁気光学素子14を配置し、ギャップ12とは反 対側のヨーク中央の部分にコイル16を設けている。これは、磁気光学素子14 を通る光ビームを妨げないようにするためである。あるいは図9のBに示すよう な形状の磁性ヨーク形18を使用し、その磁性ヨークの中央脚部の先端と外周部 との間に形成されるギャップ12に磁気光学素子14を配置し、中央脚部の基端 側にコイル16を設ける構造もある。Specifically, as shown in FIG. 9A, for example, a substantially C-shaped magnetic yoke 10 having a flat plate shape is used, and a magneto-optical element 14 is disposed in a gap 12, and the opposite side of the gap 12 is provided. The coil 16 is provided at the center of the yoke. This is so as not to obstruct the light beam passing through the magneto-optical element 14. Alternatively, a magnetic yoke shape 18 having a shape as shown in FIG. 9B is used, and the magneto-optical element 14 is arranged in the gap 12 formed between the tip of the central leg of the magnetic yoke and the outer peripheral portion, and There is also a structure in which the coil 16 is provided on the proximal end side of the leg portion.
【0004】[0004]
ところが、このような従来の構成では、コイルの位置がギャップの位置から離 れているため、コイルによって磁性ヨークに生じる磁束が大きくても、磁気回路 での漏れ磁束が大きくなり、ギャップ近傍では磁束が小さくなる。そのため、磁 気光学素子に大きな磁界を印加することが必要な時に、大きな起磁力が必要とな り、コイルの巻数を多くするか、あるいは励磁電流を大きくしなければならず、 結局、装置が大型化し、大電力消費となる。更に、コイル巻数が多いと、インダ クタンスが増加し、スイッチングに要する応答時間が長くなる欠点もある。 However, in such a conventional configuration, since the coil position is separated from the gap position, even if the magnetic flux generated in the magnetic yoke by the coil is large, the leakage magnetic flux in the magnetic circuit is large, and the magnetic flux near the gap is large. Becomes smaller. Therefore, when it is necessary to apply a large magnetic field to the magneto-optical element, a large magnetomotive force is required, and the number of turns of the coil must be increased or the exciting current must be increased. Larger size and higher power consumption. Further, when the number of coil turns is large, there is a drawback that the inductance increases and the response time required for switching becomes long.
【0005】 本考案の目的は、上記のような従来技術の欠点を解消し、装置を小型化でき、 小電力で駆動でき、しかも応答時間の短縮を図ることのできる電磁駆動式の磁気 光学装置を提供することである。An object of the present invention is to solve the above-mentioned drawbacks of the prior art, to downsize the device, to drive with a small electric power, and to shorten the response time, and an electromagnetic drive type magneto-optical device. Is to provide.
【0006】[0006]
上記の目的を達成できる本考案は、磁性ヨークによって形成する磁気回路中に ギャップを設け、該ギャップ内に磁気光学素子を配置し、ギャップを取り囲むよ うにコイルを設けた電磁駆動式磁気光学装置である。より好ましくは、2個の同 一形状の磁性ヨークを相対向させて配置することでギャップを有する磁気回路を 形成し、該ギャップ内に磁気光学素子を配置し、ギャップを取り囲むようにボビ ンに巻線を施したコイルを設ける。 The present invention that can achieve the above object is an electromagnetic drive type magneto-optical device in which a gap is provided in a magnetic circuit formed by a magnetic yoke, a magneto-optical element is disposed in the gap, and a coil is provided so as to surround the gap. is there. More preferably, a magnetic circuit having a gap is formed by arranging two magnetic yokes having the same shape so as to face each other, a magneto-optical element is arranged in the gap, and a bobbin surrounds the gap. Provide a coil with windings.
【0007】 ここで磁性ヨークは、例えば、中央脚が両側脚よりも短いE型で、その中央脚 を光ビーム通過孔が貫通する構造とする。あるいは、一方の脚が他方の脚よりも 短いU型で、その短い方の脚を光ビーム通過孔が貫通した構造でもよいし、中央 筒部が周壁部よりも短く、それらの一端で端板部により連結した構造でもよい。 ボビンは、磁性ヨークに嵌合する円筒部と、その一端に位置するフランジ部とを 一体成形した半ボビンを、2個、間に素子ホルダを介在させて組み合わせる構造 であり、該素子ホルダは、円環部の両面にボビン円筒部が嵌合する段部を形成し た構成とする。そして該素子ホルダの少なくとも一方の面に磁気光学素子を取り 付ける。あるいは、ボビンは、磁性ヨークの短い方の脚部又は中央筒部に嵌合す る円筒部と、その両端に一体成形したフランジ部とを具備し、円筒部の内周面中 央部に内径の異なる段差を設ける構成とする。その場合、素子ホルダは、円環状 であって、一方の面で前記段差に当接状態で取り付け、他方の面に磁気光学素子 を取り付ける。Here, the magnetic yoke has, for example, an E shape in which a central leg is shorter than both side legs, and a light beam passage hole penetrates the central leg. Alternatively, one leg may have a U-shape that is shorter than the other leg, and the light beam passage hole may penetrate through the shorter leg, or the central tube part may be shorter than the peripheral wall part and the end plate may be formed at one end thereof. The structure may be connected by parts. The bobbin has a structure in which two half bobbins integrally formed with a cylindrical portion fitted to the magnetic yoke and a flange portion located at one end of the bobbin are combined by interposing an element holder between them. The structure is such that steps are formed on both sides of the annular part to fit the bobbin cylindrical part. Then, the magneto-optical element is attached to at least one surface of the element holder. Alternatively, the bobbin is provided with a cylindrical portion that fits into the shorter leg of the magnetic yoke or the central cylindrical portion, and flange portions that are integrally molded at both ends of the bobbin, and an inner diameter is formed in the center of the inner peripheral surface of the cylindrical portion. Different steps are provided. In this case, the element holder has a ring shape, and is attached to the step while being in contact with the step on one surface and the magneto-optical element on the other surface.
【0008】 更に、磁性ヨークは、中央脚が両側脚よりも短い平板E型構造であり、その磁 性ヨークを相対向させてギャップを有するように組み合わせ、それを2段、間に スペーサを介して重ね合わせ、ギャップの部分に磁気光学素子を配置し、両ギャ ップを取り囲むようにコイルを設けた構成でもよい。Further, the magnetic yoke has a flat plate E-shaped structure in which the central leg is shorter than both side legs, and the magnetic yokes are combined so as to face each other so as to have a gap, and they are arranged in two steps with a spacer interposed therebetween. Alternatively, the magneto-optical element may be arranged in the gap, and the coil may be provided so as to surround both gaps.
【0009】[0009]
磁性ヨークに設けられているギャップを取り囲むように巻線を施すと、ソレノ イドコイルの磁界が大きくなり、該ギャップ内に配置した磁気光学素子は効率よ く磁化される。また磁性ヨークを通る磁束密度も増大し、ギャップに作用する磁 界が強くなるため、磁気光学素子は更に強力に磁化される。このため、起磁力が 小さくても十分飽和できることになる。従ってコイルの巻数が少なくても、また 励磁電流が小さくてもよく、結局、小型で小駆動電力の装置が得られる。更に上 記の理由で、コイルの巻数を少なくできるし、それによって磁気回路の磁路長も 短縮でき、それらの効果が相俟てインダクタンスを低減でき、高速スイッチング を実現できる。 When the winding is provided so as to surround the gap provided in the magnetic yoke, the magnetic field of the solenoid coil is increased and the magneto-optical element arranged in the gap is efficiently magnetized. Further, the magnetic flux density passing through the magnetic yoke also increases, and the magnetic field acting on the gap becomes stronger, so that the magneto-optical element is magnetized more strongly. Therefore, even if the magnetomotive force is small, it can be sufficiently saturated. Therefore, the number of windings of the coil may be small, and the exciting current may be small, and as a result, a device having a small size and a small driving power can be obtained. Further, for the above reason, the number of turns of the coil can be reduced, the magnetic path length of the magnetic circuit can be shortened, and these effects can be combined to reduce the inductance and realize high-speed switching.
【0010】[0010]
図1〜図3は本考案に係る電磁駆動式磁気光学装置の一実施例を示しており、 図1はその断面図、図2は巻線を除いた状態での組立斜視図、図3は分解斜視図 である。2個の同一形状の磁性ヨーク20を相対向させてギャップ22を有する 磁気回路を形成するように組み合わせ、該ギャップ22内に磁気光学素子24を 配置し、ギャップ22を取り囲むようにボビンに巻線を施したコイル26を設け る。 1 to 3 show an embodiment of an electromagnetically driven magneto-optical device according to the present invention. FIG. 1 is a sectional view thereof, FIG. 2 is a perspective view of an assembly without windings, and FIG. It is an exploded perspective view. Two magnetic yokes 20 having the same shape are combined so as to face each other to form a magnetic circuit having a gap 22, a magneto-optical element 24 is arranged in the gap 22, and a bobbin is wound so as to surround the gap 22. The coil 26 is provided.
【0011】 磁性ヨーク20は、中央脚20aが両側脚20bよりも短いE型で、その中央 脚20aを光ビーム通過孔28が貫通している。この実施例では、中央脚20a 及び両側脚20bは断面ほぼ円形である。この磁性ヨーク20は、例えばフェラ イトなどで製作する。The magnetic yoke 20 has an E shape in which a central leg 20 a is shorter than both side legs 20 b, and a light beam passage hole 28 penetrates through the central leg 20 a. In this embodiment, the central leg 20a and the side legs 20b have a substantially circular cross section. The magnetic yoke 20 is made of, for example, ferrite.
【0012】 次にボビン30は、前記磁性ヨーク20の中央脚20aに丁度嵌合する円筒部 32aと、その一端に位置するフランジ部32bとを樹脂成形により一体的に形 成した半ボビン32を、2個、フランジ部32bが外側にくるように向かい合わ せて配置する構成である。そして、両円筒部32aの間に素子ホルダ34を介在 させる。素子ホルダ34は、円環部の両面の外周縁にボビン円筒部32aが嵌合 する段部34aを形成し、該素子ホルダ34の少なくとも一方の面に磁気光学素 子24を取り付ける。磁気光学素子24は、例えば液相エピタキシャル成長によ るビスマス置換希土類鉄ガーネット単結晶膜(LPE膜)である。Next, the bobbin 30 is a half bobbin 32 in which a cylindrical portion 32a just fitted to the central leg 20a of the magnetic yoke 20 and a flange portion 32b located at one end thereof are integrally formed by resin molding. Two flanges 32b are arranged facing each other so that they are on the outside. Then, the element holder 34 is interposed between the cylindrical portions 32a. The element holder 34 has stepped portions 34a formed on the outer peripheral edges of both surfaces of the annular portion, into which the bobbin cylindrical portion 32a is fitted, and the magneto-optical element 24 is attached to at least one surface of the element holder 34. The magneto-optical element 24 is, for example, a bismuth-substituted rare earth iron garnet single crystal film (LPE film) formed by liquid phase epitaxial growth.
【0013】 磁気光学素子24と素子ホルダ34、及び素子ホルダ34と半ボビン32は、 接着剤により固定する。そして、それらの周囲に巻線を施し、コイルとする。ボ ビン30は、磁性ヨーク20の位置決めの機能も果たしている。磁性ヨーク20 の中央脚20aを半ボビン32の穴に嵌入して、両方の磁性ヨーク20の両側脚 20bの端面同士を衝合する。この時、中央脚20aは短いため、両方の中央脚 の端面間にギャップ22が生じ、このギャップ22中に磁気光学素子24が位置 することになる。The magneto-optical element 24 and the element holder 34, and the element holder 34 and the half bobbin 32 are fixed by an adhesive. Then, winding is applied around them to form a coil. The bobbin 30 also functions to position the magnetic yoke 20. The center leg 20a of the magnetic yoke 20 is fitted into the hole of the half bobbin 32, and the end faces of both side legs 20b of both magnetic yokes 20 are abutted. At this time, since the central leg 20a is short, a gap 22 is formed between the end faces of both central legs, and the magneto-optical element 24 is located in this gap 22.
【0014】 コイル巻線に通電することで、磁性ヨーク20に磁束が発生し、ギャップ22 に磁界が生じる。ギャップ部分はコイルで取り囲まれているため、漏れ磁束は少 なく、発生した磁束はほぼ完全に磁気光学素子24を通過することになり、それ を磁化する。この磁界によって、磁気光学素子24の偏光面を所定の角度まで回 転させるなどの動作が行われる。By energizing the coil winding, a magnetic flux is generated in the magnetic yoke 20 and a magnetic field is generated in the gap 22. Since the gap portion is surrounded by the coil, the leakage magnetic flux is small, and the generated magnetic flux almost completely passes through the magneto-optical element 24 and magnetizes it. The magnetic field causes an operation such as rotating the polarization plane of the magneto-optical element 24 to a predetermined angle.
【0015】 図4及び図5は、本考案で用いることのできる磁性ヨークの他の例を示してい る。図4においては、磁性ヨーク40は、一方の脚40aが他方の脚40bより も短いU型で、その短い方の脚40aを光ビーム通過孔42が貫通した構造であ る。両方の磁性ヨーク40を向かい合わせて衝合した時、短い方の脚40aの端 面の間にギャップができる。従って、このギャップに磁気光学素子を配置するこ とになる。この磁性ヨーク40も、例えばフェライトなどで製作する。両方の磁 性ヨークの間に組み込むボビンや素子ホルダ、磁気光学素子などは、図3に示し たものと同じ構造のものを使用できる。FIG. 4 and FIG. 5 show another example of the magnetic yoke that can be used in the present invention. In FIG. 4, the magnetic yoke 40 has a U-shape in which one leg 40a is shorter than the other leg 40b, and the light beam passage hole 42 penetrates the shorter leg 40a. When both magnetic yokes 40 face each other, a gap is formed between the end faces of the shorter leg 40a. Therefore, the magneto-optical element is arranged in this gap. The magnetic yoke 40 is also made of, for example, ferrite. The bobbin, the element holder, the magneto-optical element, etc. incorporated between the two magnetic yokes can have the same structure as that shown in FIG.
【0016】 次に図5に示した磁性ヨーク50は、中央筒部50aが周壁部50bよりも短 く、それらの一端で端板部50cにより連結した一体構造をなしている。このよ うな形状の磁性ヨークは、フェライトで構成してもよいし、金属材料で構成して もよい。2個の磁性ヨーク50を向き合わせて衝合すると、短い中央筒部50a の端面同士の間にギャップが生じるから、そのギャップに磁気光学素子を配置す ることになる。この場合も、図3に示すコイル構造をそのまま組み込むことが可 能である。但し、図5の場合には、磁性ヨークが全体として円筒状であるため、 薄型化の点ではやや問題が残り、実装上は前記の各実施例の場合に比べてやや不 利となる。なお、この磁性ヨーク50では、中央筒部50aに設けられるている 穴が光ビーム通過孔となる。Next, the magnetic yoke 50 shown in FIG. 5 has an integral structure in which the central cylindrical portion 50a is shorter than the peripheral wall portion 50b and one end thereof is connected by the end plate portion 50c. The magnetic yoke having such a shape may be made of ferrite or a metal material. When the two magnetic yokes 50 face each other and abut against each other, a gap is formed between the end faces of the short central tubular portion 50a, so that the magneto-optical element is arranged in the gap. Also in this case, the coil structure shown in FIG. 3 can be incorporated as it is. However, in the case of FIG. 5, since the magnetic yoke is cylindrical as a whole, a problem remains in terms of thinning, and it is slightly disadvantageous in mounting in comparison with the case of each of the above embodiments. In this magnetic yoke 50, the hole provided in the central tubular portion 50a becomes the light beam passage hole.
【0017】 図6は本考案で用いることのできるボビンの他の例を示し、図7にそれを用い た磁気光学装置の断面を示す。ボビン60は、例えば図1に示すような磁性ヨー クを用いる場合、磁性ヨーク20の中央脚に嵌合する円筒部60aと、その両端 に一体成形したフランジ部60bとを具備する。そして円筒部60aの内周面ほ ぼ中央に内径の異なる段差60cを設ける。他方、素子ホルダ62は単純な円環 状でよく、前記円筒部60aの大きな内径部を通過するが小さな内径部は通過し えないような外形に設定する。そして一方の面で前記段差60cに当接した状態 で取り付け、該素子ホルダ62の他方の面に磁気光学素子64を取り付ける。な お、磁気光学素子がLPE膜のような薄肉構造ではなく、ブロック状の素子の場 合には、素子ホルダを用いることなく直接前記段差60cに取り付けることも可 能である。FIG. 6 shows another example of the bobbin that can be used in the present invention, and FIG. 7 shows a cross section of a magneto-optical device using the bobbin. When using the magnetic yoke as shown in FIG. 1, for example, the bobbin 60 includes a cylindrical portion 60a fitted to the central leg of the magnetic yoke 20 and flange portions 60b integrally formed at both ends thereof. Then, a step 60c having a different inner diameter is provided near the center of the inner peripheral surface of the cylindrical portion 60a. On the other hand, the element holder 62 may have a simple annular shape, and is set to have an outer shape that can pass through the large inner diameter portion of the cylindrical portion 60a but cannot pass through the small inner diameter portion. Then, one surface is attached in contact with the step 60c, and the magneto-optical element 64 is attached to the other surface of the element holder 62. When the magneto-optical element is not a thin structure such as the LPE film but a block-shaped element, it is possible to directly attach it to the step 60c without using an element holder.
【0018】 このようなボビン60を用いる場合も、図7に示すように、磁性ヨーク20に よるギャップ22中に磁気光学素子64を配置し、それを取り囲むようにコイル を設けることができる。ボビン60の外周に所定の巻線を施すことは言うまでも ない。円筒部60aの大きな内径部分と磁性ヨークの中央脚と間に隙間が生じる が、その隙間に円筒状のスペーサ66を嵌合しておけば、正確な位置決め・保持 が可能である。このボビンは図4あるいは図5に示す構造の磁性ヨークにも適用 できる。但し、磁気光学素子を取り付けた素子ホルダをボビンの内部に挿入し固 定する作業が必要となるため、ボビンの長さが長くなった場合には、若干作業が 難しくなる。その点では、前記2分割構造のボビンの方が、組立作業性は良好で ある。Even when such a bobbin 60 is used, as shown in FIG. 7, the magneto-optical element 64 can be arranged in the gap 22 formed by the magnetic yoke 20, and a coil can be provided so as to surround it. It goes without saying that a predetermined winding is provided on the outer circumference of the bobbin 60. A gap is formed between the large inner diameter portion of the cylindrical portion 60a and the central leg of the magnetic yoke, but if a cylindrical spacer 66 is fitted in the gap, accurate positioning / holding is possible. This bobbin can also be applied to the magnetic yoke having the structure shown in FIG. 4 or 5. However, since it is necessary to insert and fix the element holder with the magneto-optical element inside the bobbin, the work becomes slightly difficult when the bobbin becomes long. In this respect, the bobbin having the two-part structure has better assembling workability.
【0019】 図8は本考案の更に他の実施例を示している。磁性ヨーク70は、中央脚が両 側脚よりも短い平板E型構造であり、その磁性ヨーク70を相対向させてギャッ プ72を有するように組み合わせ、それを2段、間にスペーサ74を介して重ね 合わせる。磁性ヨーク70としては金属材料が好ましい。スペーサ74は、磁性 体でも非磁性体でもよく、磁性体の場合には磁性ヨークと同じ金属材料を複数枚 積層することで、所定の間隔に調整することができる。そしてギャップの部分に 磁気光学素子76を配置し、両ギャップを取り囲むようにコイル78を設ける。 なお、スペーサ74の位置にもよるが、それが光ビームの通過部に位置している 場合には、光ビーム通過孔75を設ける必要がある。FIG. 8 shows still another embodiment of the present invention. The magnetic yoke 70 has a flat plate E-type structure in which the center leg is shorter than both side legs, and the magnetic yokes 70 are assembled so as to face each other and have a gap 72. And stack them. A metal material is preferable for the magnetic yoke 70. The spacer 74 may be a magnetic material or a non-magnetic material, and in the case of a magnetic material, it can be adjusted to a predetermined interval by laminating a plurality of metal materials same as the magnetic yoke. Then, the magneto-optical element 76 is arranged in the gap portion, and the coil 78 is provided so as to surround both gaps. It should be noted that although depending on the position of the spacer 74, if it is located at the light beam passage portion, it is necessary to provide the light beam passage hole 75.
【0020】 図8に示す磁気光学装置は、図9のBに示す従来の磁気光学装置とほぼ同様の 寸法形状である。そこで両者による特性を測定し、性能について比較検討した。 図9のBに示す構造の場合は、LPE膜に163Gの磁束密度を与えるために、 コイル巻数(線径0.12mmφ)を30回とし、1.1Aの電流を流す必要があ った。この時、コイルのインダクタンスは37.1μH、コイルの抵抗値は0. 44Ωであり、応答時間は123μS、消費電力は0.53Wであった。それに 対して図8に示す構造では、LPE膜の磁束密度が178Gの場合、必要な電流 値は1.1A、コイル巻数は8回でよく、コイルのインダクタンスは0.302 μH、コイル抵抗値は0.106Ωに減少し、応答時間は3.5μS、消費電力 は0.13Wと著しく低減した。The magneto-optical device shown in FIG. 8 has substantially the same size and shape as the conventional magneto-optical device shown in FIG. 9B. Therefore, the characteristics of both were measured, and the performance was compared and examined. In the case of the structure shown in FIG. 9B, in order to give a magnetic flux density of 163 G to the LPE film, the number of coil turns (wire diameter 0.12 mmφ) was set to 30 and a current of 1.1 A was required to flow. At this time, the inductance of the coil is 37.1 μH and the resistance value of the coil is 0. It was 44Ω, the response time was 123 μS, and the power consumption was 0.53 W. On the other hand, in the structure shown in FIG. 8, when the magnetic flux density of the LPE film is 178 G, the required current value is 1.1 A, the number of coil turns is eight, the coil inductance is 0.302 μH, and the coil resistance value is It was decreased to 0.106Ω, the response time was 3.5 μS, and the power consumption was 0.13 W, which was a remarkable decrease.
【0021】 以上、本考案の実施例について説明したが、本考案は図面に示す構造のみに限 られるものではなく、種々の変更が可能である。例えば、磁性ヨークの形状は、 脚部、特に中央脚の断面として円形断面であったが、その部分を方形断面にして もよいし、楕円形断面にしてもよい。それに伴って、ボビンの筒状部の形状を、 円筒状から角筒状や楕円筒状などに変更することになる。Although the embodiments of the present invention have been described above, the present invention is not limited to the structure shown in the drawings, and various modifications can be made. For example, the shape of the magnetic yoke is a circular cross section as a cross section of the leg portion, especially the central leg, but that portion may be a square cross section or an elliptical cross section. Along with that, the shape of the cylindrical portion of the bobbin is changed from a cylindrical shape to a rectangular cylindrical shape or an elliptic cylindrical shape.
【0022】[0022]
本考案は、磁気回路中に形成されているギャップ内に磁気光学素子を配置し、 ギャップを取り囲むようにコイルを設けたから、コイルで発生する磁界が効果的 に磁気光学素子に印加されて、該磁気光学素子は効率良く磁化され、そのため起 磁力が小さくても十分に飽和させることができる。この結果、コイル巻数が少な くてもよいし、励磁電流を小さくすることもでき、結局、小型で小駆動電力の装 置が得られる。またコイル巻数を低減することができるため、それによって磁気 回路の磁路長も短縮でき、それらの効果が相俟てインダクタンスを低減でき、電 流の過渡現象による応答時間が短くなり、高速スイッチングが可能となる。 In the present invention, the magneto-optical element is arranged in the gap formed in the magnetic circuit, and the coil is provided so as to surround the gap. Therefore, the magnetic field generated by the coil is effectively applied to the magneto-optical element, The magneto-optical element is efficiently magnetized, so that it can be sufficiently saturated even if the magnetomotive force is small. As a result, the number of coil turns may be small, and the exciting current may be small, resulting in a compact device with low driving power. In addition, since the number of coil turns can be reduced, the magnetic path length of the magnetic circuit can be shortened, and the effects of these can be combined to reduce the inductance, the response time due to the transient phenomenon of the current can be shortened, and high-speed switching can be achieved. It will be possible.
【図1】本考案に係る磁気光学装置の一実施例を示す断
面図。FIG. 1 is a sectional view showing an embodiment of a magneto-optical device according to the present invention.
【図2】その巻線を除く組立斜視図。FIG. 2 is an assembled perspective view excluding the winding.
【図3】巻線を除く分解斜視図。FIG. 3 is an exploded perspective view excluding windings.
【図4】磁性ヨークの他の実施例を示す斜視図。FIG. 4 is a perspective view showing another embodiment of the magnetic yoke.
【図5】磁性ヨークの更に他の実施例を示す斜視図。FIG. 5 is a perspective view showing still another embodiment of the magnetic yoke.
【図6】ボビンの他の実施例を示す一部破断斜視図。FIG. 6 is a partially cutaway perspective view showing another embodiment of the bobbin.
【図7】そのボビンを用いた磁気光学装置の一例を示す
断面図。FIG. 7 is a sectional view showing an example of a magneto-optical device using the bobbin.
【図8】本考案に係る磁気光学装置の更に他の実施例を
示す説明図。FIG. 8 is an explanatory view showing still another embodiment of the magneto-optical device according to the present invention.
【図9】従来技術の例を示す説明図。FIG. 9 is an explanatory diagram showing an example of a conventional technique.
20 磁性ヨーク 22 ギャップ 24 磁気光学素子 26 コイル 28 光ビーム通過孔 30 ボビン 32 半ボビン 34 素子ホルダ 20 magnetic yoke 22 gap 24 magneto-optical element 26 coil 28 light beam passage hole 30 bobbin 32 half bobbin 34 element holder
Claims (8)
にギャップを設け、該ギャップ内に磁気光学素子を配置
し、ギャップを取り囲むようにコイルを設けた電磁駆動
式磁気光学装置。1. An electromagnetic drive type magneto-optical device in which a gap is provided in a magnetic circuit formed by a magnetic yoke, a magneto-optical element is arranged in the gap, and a coil is provided so as to surround the gap.
せて配置することでギャップを有する磁気回路を形成
し、該ギャップ内に磁気光学素子を配置し、ギャップを
取り囲むようにボビンに巻線を施したコイルを設けた電
磁駆動式磁気光学装置。2. A magnetic circuit having a gap is formed by arranging two magnetic yokes having the same shape so as to face each other, a magneto-optical element is disposed in the gap, and the bobbin is wound so as to surround the gap. An electromagnetically driven magneto-optical device provided with a coil having a wire.
いE型で、その中央脚を光ビーム通過孔が貫通している
請求項2記載の磁気光学装置。3. The magneto-optical device according to claim 2, wherein the magnetic yoke is E-shaped with a central leg shorter than both side legs, and a light beam passage hole penetrates through the central leg.
も短いU型で、その短い方の脚を光ビーム通過孔が貫通
している請求項2記載の磁気光学装置。4. The magneto-optical device according to claim 2, wherein the magnetic yoke has a U-shape in which one leg is shorter than the other leg, and the light beam passage hole penetrates the shorter leg.
短く、それらの一端で端板部により連結している請求項
2記載の磁気光学装置。5. The magneto-optical device according to claim 2, wherein the magnetic yoke has a central tubular portion shorter than the peripheral wall portion and is connected at one end thereof by an end plate portion.
る円筒部と、その一端に位置するフランジ部とを一体成
形した半ボビンを、2個、間に素子ホルダを介在させて
組み合わせ、該素子ホルダは、円環部の両面にボビン円
筒部が嵌合する段部を形成した構造をなし、該素子ホル
ダの少なくとも一方の面に磁気光学素子を取り付けた請
求項3記載の磁気光学装置。6. The bobbin is a combination of two half bobbins integrally formed with a cylindrical portion fitted to a central leg of a magnetic yoke and a flange portion located at one end thereof, with an element holder interposed therebetween. 4. The magneto-optical device according to claim 3, wherein the element holder has a structure in which a step portion into which a bobbin cylindrical portion is fitted is formed on both surfaces of an annular portion, and a magneto-optical element is attached to at least one surface of the element holder. .
中央筒部に嵌合する円筒部と、その両端に一体成形した
フランジ部とを具備し、円筒部の内周面ほぼ中央に内径
の異なる段差を設け、素子ホルダは、円環状であって一
方の面で前記段差に当接した状態で取り付けられ、該素
子ホルダの他方の面に磁気光学素子を取り付けた請求項
3、4又は5記載の磁気光学装置。7. The bobbin includes a cylindrical portion fitted to the shorter leg of the magnetic yoke or the central cylindrical portion, and flange portions integrally formed at both ends thereof, and an inner diameter is formed substantially at the center of the inner peripheral surface of the cylindrical portion. Different step is provided, and the element holder is attached in a state in which the element holder has an annular shape and is in contact with the step on one surface, and the magneto-optical element is attached to the other surface of the element holder. 5. The magneto-optical device according to item 5.
い平板E型構造であり、その磁性ヨークを相対向させて
ギャップを有するように組み合わせ、それを2段、間に
スペーサを介して重ねて、ギャップの部分に磁気光学素
子を配置し、両ギャップを取り囲むようにコイルを設け
た電磁駆動式磁気光学装置。8. The magnetic yoke has a flat plate E-shaped structure in which a central leg is shorter than both side legs, and the magnetic yokes are combined so as to face each other so as to have a gap. An electromagnetic drive type magneto-optical device in which a magneto-optical element is arranged in the gap portion and a coil is provided so as to surround both gaps.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1994013076U JP3009560U (en) | 1994-09-28 | 1994-09-28 | Electromagnetic drive type magneto-optical device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1994013076U JP3009560U (en) | 1994-09-28 | 1994-09-28 | Electromagnetic drive type magneto-optical device |
Publications (1)
Publication Number | Publication Date |
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JP3009560U true JP3009560U (en) | 1995-04-04 |
Family
ID=43145352
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Application Number | Title | Priority Date | Filing Date |
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JP1994013076U Expired - Lifetime JP3009560U (en) | 1994-09-28 | 1994-09-28 | Electromagnetic drive type magneto-optical device |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP3510205B2 (en) | 2000-12-14 | 2004-03-22 | Tdk株式会社 | Optical attenuator |
WO2005071470A1 (en) * | 2004-01-22 | 2005-08-04 | Fdk Corporation | Variable faraday rotor and variable optical attenuator |
-
1994
- 1994-09-28 JP JP1994013076U patent/JP3009560U/en not_active Expired - Lifetime
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP3510205B2 (en) | 2000-12-14 | 2004-03-22 | Tdk株式会社 | Optical attenuator |
WO2005071470A1 (en) * | 2004-01-22 | 2005-08-04 | Fdk Corporation | Variable faraday rotor and variable optical attenuator |
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