JPH081789B2 - Deflection yoke - Google Patents
Deflection yokeInfo
- Publication number
- JPH081789B2 JPH081789B2 JP61061449A JP6144986A JPH081789B2 JP H081789 B2 JPH081789 B2 JP H081789B2 JP 61061449 A JP61061449 A JP 61061449A JP 6144986 A JP6144986 A JP 6144986A JP H081789 B2 JPH081789 B2 JP H081789B2
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- wire
- deflection
- deflection coil
- coil
- 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
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は陰極線管に用いられる偏向ヨークに関する
ものである。TECHNICAL FIELD The present invention relates to a deflection yoke used in a cathode ray tube.
コンピユータの端末装置として近年急速に発展するキ
ヤラクターデイスプレイやグラフイツクデイスプレイ用
モニター等に使用される高解像度陰極線管用偏向ヨーク
は、表示性能を向上させるため水平の偏向走査周波数が
高くなる傾向にある。従来、この水平偏向周波数は、テ
レビジヨン用の偏向周波数15.75KHzと同じ位であつたが
高解像度化に伴ない64KHzあるいはそれ以上、最高130KH
zもの高い周波数で使用されるようになつてきた。The deflection yoke for a high resolution cathode ray tube used for a monitor for a character display or a graphic display, which has been rapidly developed in recent years as a computer terminal device, tends to have a high horizontal deflection scanning frequency in order to improve display performance. Conventionally, this horizontal deflection frequency was about the same as the deflection frequency of 15.75 KHz for televisions, but with the increase in resolution, it was 64 KHz or higher, with a maximum of 130 KH.
It has come to be used at high frequencies as high as z.
偏向ヨークに流れる偏向のこぎり波電流の周波数が高
くなると、偏向コイルについてはうず電流損や表皮損失
が増大する。また一方偏向ヨーク用コアにおいては同じ
くうず電流損やヒステリシス損が増大する傾向にある。
偏向ヨークの動作時にこれらの損失は偏向ヨーク自体の
全体の発熱として現われ、結果的に偏向ヨークの温度上
昇を招き、信頼性を損うばかりでなく、ミスコンバーゼ
ンス、ミスランデイングやラスター歪といつた表示デバ
イスとしては致命的な性能欠陥を起こすおそれもある。When the frequency of the sawtooth wave current of the deflection flowing through the deflection yoke increases, the eddy current loss and the skin loss of the deflection coil increase. On the other hand, in the core for the deflection yoke, eddy current loss and hysteresis loss also tend to increase.
When the deflection yoke operates, these losses appear as the entire heat generation of the deflection yoke itself, resulting in an increase in the temperature of the deflection yoke, impairing the reliability, and causing misconvergence, mislanding, and raster distortion. As a display device, there is a possibility of causing a fatal performance defect.
上記うず電流の発生を第4図および第5図に示すサド
ル型水平偏向コイル(1)について説明する。この水平
偏向コイル(1)は導線(5)を巻回することによつて
形成され、巻回導線の磁束発生状況は第6図に示すよう
になる。ここで、それぞれの導線(5a)〜(5c)には、
同一の方向に電流が流れるため各導線(5a)〜(5c)が
その周囲に作る磁束φa〜φcは隣合う導線(5a)〜
(5c)を横切り、結果的に互にその導線(5a)〜(5c)
に流れる電流の実効導体断面積を制限する。これは一種
のうず電流損を発生させることになり、水平偏向コイル
(1)に流れる電流の周波数が高くなるにつれて大とな
る。The generation of the eddy current will be described with reference to the saddle type horizontal deflection coil (1) shown in FIGS. 4 and 5. This horizontal deflection coil (1) is formed by winding a conducting wire (5), and the magnetic flux generation state of the winding conducting wire is as shown in FIG. Here, in each conductor (5a) ~ (5c),
Since the electric currents flow in the same direction, the magnetic fluxes φa to φc created by the respective conducting wires (5a) to (5c) around the conducting wires (5a) to (5c) are adjacent to each other.
(5a) to (5c) as a result of crossing (5c)
Limits the effective conductor cross section of the current flowing in This causes a kind of eddy current loss, which increases as the frequency of the current flowing through the horizontal deflection coil (1) increases.
このため、水平偏向コイルの発熱対策としては、従来
特開昭59−186239号公報に示されるように細線の撚線、
いわゆるリツツ線をコイル成形用導線に使用することが
多い。その構造を第7図に示す。同図において、リツツ
線(2)は、絶縁層(4)で被われた各素線(3)の径
が従来テレビジヨン用偏向ヨークとして用いられていた
導線の1/3〜1/4程度、すなわち線径0.1〜0.15mmのもの
を複数本撚り合わせたもので、コイルの実効的な導体幅
を小さくすることにより、コイル導線内部に生じるうず
電流損を軽減するものである。Therefore, as a measure against heat generation of the horizontal deflection coil, as shown in Japanese Patent Laid-Open No. 59-186239, a twisted wire of thin wire,
A so-called litz wire is often used for a coil forming conductor. Its structure is shown in FIG. In the same figure, the diameter of each strand (3) covered with the insulating layer (4) is about 1/3 to 1/4 of the conductor wire which is conventionally used as a deflection yoke for televisions. That is, a plurality of wires having a wire diameter of 0.1 to 0.15 mm are twisted together, and the effective conductor width of the coil is reduced to reduce the eddy current loss generated inside the coil conductor.
しかしながら、偏向ヨークは、この偏向周波数の高い
水平偏向コイルとして第4図のようなサドル型のコイル
(1)を使用する場合、数本の導線を束ねて金型に巻線
し、通電加熱によりコイル融着成形して作るのが一般的
である。このような製造工程を経るサドル型コイルで
は、前述の第7図のリツツ線(2)はその構造上取扱い
が難しく、製品のばらつきを招いたり、製造歩留りの悪
化をもたらす等の問題がある。また64KHz走査位まで
は、リツツ線(2)の使用や低損失コア材の使用により
実用上問題のないレベルまで発熱を抑えることができる
が、130KHz走査では、たとえリツツ構造を採用しても発
熱に関しては、まだ、不充分である。すなわちたとえリ
ツツ構造を採用しても偏向コイルの発熱を実用上問題の
ないレベルまで抑えることはむつかしい。以上から従来
の課題を整理すると3つの課題があった。However, when the saddle type coil (1) as shown in FIG. 4 is used as the horizontal deflection coil having a high deflection frequency, the deflection yoke is formed by bundling several conductor wires and winding them in a die and heating them by energization heating. It is generally made by coil fusion molding. In the saddle type coil that undergoes such a manufacturing process, the ridge wire (2) shown in FIG. 7 is difficult to handle because of its structure, which causes problems such as variations in products and deterioration in manufacturing yield. Up to 64KHz scanning, it is possible to suppress heat generation to a level where there is no practical problem by using the rits wire (2) and the use of low-loss core material, but at 130KHz scanning, even if the rits structure is adopted, heat is generated. As for, it is still insufficient. That is, even if the lit structure is adopted, it is difficult to suppress the heat generation of the deflection coil to a level at which there is no practical problem. From the above, there are three problems when the conventional problems are sorted out.
つまり従来の偏向ヨークに於ては第1の課題として単
線形状の導線による偏向ヨーク用の偏向コイルは、偏向
周波数が64KHz程度でも巻回導線の相互の鎖交磁束に起
因する伝導路の実効断面積の減少と渦電流の損失によ
り、発熱があり実用上問題があった。In other words, the first problem with the conventional deflection yoke is that the deflection coil for the deflection yoke using a single wire-shaped conducting wire has an effective disconnection of the conduction path due to mutual flux linkage of the wound conducting wires even when the deflection frequency is about 64 KHz. Due to the reduction of the area and the loss of the eddy current, there was heat generation and there was a practical problem.
そして第2の課題として前記第1の課題を解決する手
段として偏向周波数が64KHz程度でもあえてリツツ構造
の導線(第7図に示す)を用いらざるおえないため、リ
ツツ構造の導線では負数本撚り合わせであるがゆえにサ
ドル型コイル(第4図に示す)に成形するのが難しく結
果として製品のばらつきと製造歩留りが悪いという問題
があった。As the second problem, as a means for solving the first problem, since a deflection wire having a deflection frequency of about 64 KHz is unavoidably used, it is inevitable to use a ricks-structured conductor wire (shown in FIG. 7). Since they are matched, it is difficult to form a saddle type coil (shown in FIG. 4), and as a result, there is a problem in that product variations and manufacturing yields are poor.
更に第3の課題として更に偏向周波数が130KHz程度に
高くなると、たとえ従来の単なるリツツ構造の導線を用
いても電流損失増大にともなう発熱の点でこのリツツ構
造の導線を用いることに問題があった。Further, as a third problem, when the deflection frequency is further increased to about 130 KHz, there is a problem in using the conductor wire of this rit structure even in the case of using the conventional conductor wire of the rit structure, because of the heat generation due to the increase of the current loss. .
この発明は、上記のような問題点を解消するためにな
されたもので、特に高周波走査時に水平偏向コイル全体
に発生する発熱を充分に低減することができる偏向ヨー
クを提供することを目的としている。The present invention has been made to solve the above problems, and an object of the present invention is to provide a deflection yoke capable of sufficiently reducing heat generated in the entire horizontal deflection coil during high frequency scanning. .
この発明に係る偏向ヨークは、水平偏向コイルおよび
垂直偏向コイルの少なくともいずれか一方を成形するた
めの導線の導体外表面上に、従来の絶縁層に代えて予め
高透磁率の磁性層とこの磁性層の上に絶縁層とを各々連
続的に設け、磁性層が導線の導体内部を通過する磁束を
抑制するとともに、絶縁層が導線の最外周を絶縁するこ
の導線を巻回或形して上記偏向コイルを構成としたこと
を特徴とするものである。In the deflection yoke according to the present invention, a magnetic layer having a high magnetic permeability and a magnetic layer having a high magnetic permeability are provided on an outer surface of a conductor of a conductor for forming at least one of a horizontal deflection coil and a vertical deflection coil, instead of a conventional insulating layer. An insulating layer is continuously provided on each of the layers, the magnetic layer suppresses a magnetic flux passing through the inside of the conductor, and the insulating layer insulates the outermost circumference of the conductor. It is characterized in that a deflection coil is configured.
この発明によれば、偏向ヨークを成形するための導線
の導体の外周が、予め連続した高透磁率の磁性層ととも
にその上に絶縁層を備えているため、従来の導線と同じ
ように各隣接する導線の導体が絶縁された上でなおかつ
隣接導体内部への磁束の通過が軽減され、高周波走査時
においても実効導体面積が減らず、たとえば、64KHz程
度では、水平偏向コイル用の導線の構造に関してあえて
リツツ構造を採らずとも、つまり従来の単線形状の導線
の構造のままでも、水平偏向コイル全体の発熱が抑制さ
れる。According to the present invention, the outer circumference of the conductor of the conductor for forming the deflection yoke is provided with a continuous magnetic layer having a high magnetic permeability in advance and an insulating layer on the magnetic layer. The conductor of the conducting wire is insulated, and the passage of the magnetic flux into the adjacent conductor is reduced, and the effective conductor area does not decrease even during high frequency scanning.For example, regarding the structure of the conducting wire for the horizontal deflection coil at about 64 KHz. Even if the rit structure is not taken, that is, even if the structure of the conventional single wire-shaped conductor is used, the heat generation of the entire horizontal deflection coil is suppressed.
以下、この発明の実施例を図面にしたがつて説明す
る。Embodiments of the present invention will be described below with reference to the drawings.
第1図はこの発明に係る偏向ヨークの水平偏向コイル
形成用導線を示すものである。同図において、(6)は
細い単線の導体で、この導体(6)の外周面には、予め
鉄メツキからなる高透磁率の磁性層(7)が連続的に形
成されており、その上から絶縁層(4)が被覆されてい
る。これら導体(6)や磁性層(7)及び絶縁層(4)
等からなる単線形状の導線(8)を第4図のようなサド
ル型に巻回して或形することにより水平偏向コイル
(1)が形成される。FIG. 1 shows a horizontal deflection coil forming conductor of a deflection yoke according to the present invention. In the figure, (6) is a thin single wire conductor, and a high magnetic permeability magnetic layer (7) made of iron plating is continuously formed on the outer peripheral surface of the conductor (6). To an insulating layer (4). These conductor (6), magnetic layer (7) and insulating layer (4)
A horizontal deflection coil (1) is formed by winding or forming a single wire conductor (8) made of, for example, a saddle shape as shown in FIG.
つぎに、上記構成の動作を第2図を参照して説明す
る。Next, the operation of the above configuration will be described with reference to FIG.
各導線(8a)〜(8c)の表面にはそれぞれ鉄メツキか
らなる透磁率の高い磁性層(7)があるため、隣合う導
線(8a)〜(8c)から生じる磁束φa〜φcは磁性層
(7)にバイパスされる。したがつて各導体(6a)〜
(6c)内部への磁束φa〜φcの通過が抑制される。こ
の結果、水平偏向コイル(1)に流れる電流の周波数が
64KHz程度の高い場合でも、実効導体断面積が減される
ことなく、有効に導体に高周波電流を流すことが可能と
なる。すなわち、偏向周波数が65KHz程度までであれ
ば、第1図に示す断面を有する上記構成の単線形状の導
線(8)をそのまま従来と同じようにサドル型に巻回す
るだけで、うず電流損の抑制をともなった上で、水平偏
向コイルを構成することができることになり、偏向ヨー
クの製造の容易化に寄与できる。つまり先に述べた従来
の問題点が解決できる。Since there are magnetic layers (7) made of iron plated and having high magnetic permeability on the surfaces of the conductors (8a) to (8c), the magnetic fluxes φa to φc generated from the adjacent conductors (8a) to (8c) are Bypassed to (7). Therefore, each conductor (6a)
(6c) Passage of the magnetic fluxes φa to φc to the inside is suppressed. As a result, the frequency of the current flowing in the horizontal deflection coil (1)
Even if the frequency is as high as 64 KHz, it is possible to effectively pass a high-frequency current through the conductor without reducing the effective conductor cross-sectional area. That is, if the deflection frequency is up to about 65 KHz, the eddy current loss can be obtained by simply winding the single-wire-shaped conductor wire (8) having the above-mentioned configuration shown in FIG. With suppression, the horizontal deflection coil can be configured, which can contribute to the ease of manufacturing the deflection yoke. That is, the conventional problems described above can be solved.
第3図はこの発明の他の例を示し、前記構成の導線
(8)、たとえば素線径が0.1〜0.2mmのものに磁性層
(7)とその上に絶縁層(4)を形成した単線形状もの
を数本撚り合わせてリツツ線(9)としたものであり、
このリツツ線(9)をサドル型に巻回して水平偏向コイ
ル(1)が形成される。この場合、リツツ構造化による
製造上の複雑さの犠牲があっても、リツツ構造による従
来からの実効的な導体幅の減少効果と、先の実施例によ
る新たな効果、つまり絶縁層に包まれ磁性層(7)によ
る隣接導体(6)への鎖交磁束密度の減少効果との相乗
効果により、うず電流損を大幅に軽減でき、偏向周波数
が64KHz以上、とくに130KHz程度までのものにも対応可
能となる。FIG. 3 shows another example of the present invention, in which a magnetic layer (7) and an insulating layer (4) are formed on a conductor wire (8) having the above-mentioned structure, for example, a wire having a diameter of 0.1 to 0.2 mm. It is a rope wire (9) made by twisting several single wires into one.
The rope wire (9) is wound in a saddle shape to form a horizontal deflection coil (1). In this case, even if there is a sacrifice in manufacturing complexity due to the rit structure, the effect of reducing the effective conductor width from the conventional structure due to the rit structure and the new effect of the previous embodiment, that is, the insulating layer is included. The eddy current loss can be greatly reduced by the synergistic effect of the magnetic layer (7) and the effect of reducing the interlinkage magnetic flux density to the adjacent conductor (6), and the deflection frequency of 64 KHz or more, especially up to about 130 KHz is also supported. It will be possible.
上記各例においては、磁性層(7)として鉄メツキで
構成したもので説明したが、他の磁性メツキでもよく、
またメツキ以外の方法で形成されるものであつてもよ
い。In each of the above examples, the magnetic layer (7) is made of iron plating, but other magnetic plating may be used.
Further, it may be formed by a method other than plating.
また、上記の例では、水平偏向コイル(1)について
説明したが、この発明の構成は垂直偏向コイルにも適用
可能である。Further, in the above example, the horizontal deflection coil (1) has been described, but the configuration of the present invention is also applicable to the vertical deflection coil.
以上のようにこの発明は、水平偏向コイルおよび垂直
偏向コイルの少なくともいずれか一方を成形するための
導線の導体外表面上に、従来の絶縁層に代えて順に高透
磁率の磁性層と前記磁性層の上に絶縁層とを各々導体の
流さ方向に連続的に設け、磁性層が導線の導体内部を通
過する磁束を抑制して又絶縁層が導線の最外周を絶縁す
るこの単線形状の導線を巻回成形して上記偏向コイルを
構成したから、偏向周波数が64KHz程度までなら水平偏
向コイルにその巻線成形が難しいリツツ線を採用するこ
となく、たとえば従来の導線と同じ形状の単線形状の本
願発明の導線(8)を従来の単線形状の導線より低い発
熱状態で用いることができる。つまり偏向周波数が64KH
z程度までなら、たとえば従来のリツツ線に代えて単線
形状の本願発明の導線を用いても、高い偏向周波数での
偏向コイルの隣接導線間に於て発生する鎖交磁束が導線
の導体内部を通過することを磁性層が抑制する。その結
果導線の導体部を流れる電流路の実効導体断面積の減少
がおさえられ、かつ渦電流損失も低減でき、換言すれば
結果的に偏向コイル全体にわたり従来に比較して発熱の
低い偏向ヨークを容易に製造でき、また、性能上の関点
だけからすれば、リツツ構造を採用することにより一層
高い偏向周波数、たとえば130KHz偏向走査においても発
熱を有効に抑制し得る利点がある。As described above, according to the present invention, a magnetic layer having a high magnetic permeability and the magnetic layer are formed on the outer surface of the conductor of the conductor for forming at least one of the horizontal deflection coil and the vertical deflection coil in place of the conventional insulating layer. An insulating layer is continuously provided on the layer in the flow direction of the conductor, the magnetic layer suppresses the magnetic flux passing inside the conductor of the conductor, and the insulating layer insulates the outermost circumference of the conductor. Since the above deflection coil is formed by winding molding, if the deflection frequency is up to about 64 KHz, the horizontal deflection coil does not have to use a ridge wire, which is difficult to form its winding wire. The conductor wire (8) of the present invention can be used in a heat generation state lower than that of the conventional single wire-shaped conductor wire. In other words, the deflection frequency is 64KH
Up to about z, for example, even if a single wire-shaped conductor of the present invention is used in place of the conventional ridge wire, the interlinkage magnetic flux generated between the adjacent conductors of the deflection coil at a high deflection frequency is generated inside the conductor of the conductor. The magnetic layer suppresses passage. As a result, the effective conductor cross-sectional area of the current path flowing through the conductor portion of the conductor can be suppressed, and the eddy current loss can be reduced. In other words, as a result, a deflection yoke that generates less heat than the conventional deflection coil over the entire deflection coil can be obtained. It is easy to manufacture, and from the point of view of performance only, there is an advantage that the rits structure can effectively suppress heat generation even at a higher deflection frequency, for example, 130 KHz deflection scanning.
第1図はこの発明に係る偏向ヨークの一実施例である水
平偏向コイル成形用導線を示す断面図、第2図は第1の
導線で水平偏向コイルを成形した場合の作用説明図、第
3図はこの発明の他の例を示す断面図、第4図はサドル
型水平偏向コイルを示す斜視図、第5図はサドル型水平
偏向コイルの概略断面図、第6図は従来構造の導線に水
平偏向コイルを成形した場合の作用説明図、第7図は従
来のリツツ線の断面図である。 (1)……サドル型水平偏向コイル、(6)……導体、
(7)……磁性層、(8)……導線、(9)……リツツ
線。 なお、図中、同一符号は同一もしくは相当部分を示す。FIG. 1 is a cross-sectional view showing a horizontal deflection coil forming conductor which is an embodiment of the deflection yoke according to the present invention, and FIG. 2 is an operation explanatory view when the horizontal deflection coil is formed by the first conductor, and FIG. FIG. 4 is a sectional view showing another example of the present invention, FIG. 4 is a perspective view showing a saddle type horizontal deflection coil, FIG. 5 is a schematic sectional view of a saddle type horizontal deflection coil, and FIG. 6 is a conductor wire of a conventional structure. FIG. 7 is an explanatory view of the operation when a horizontal deflection coil is molded, and FIG. 7 is a sectional view of a conventional ridge line. (1) ... saddle type horizontal deflection coil, (6) ... conductor,
(7) ... Magnetic layer, (8) ... Conductive wire, (9) ... Ritsu wire. In the drawings, the same reference numerals indicate the same or corresponding parts.
Claims (3)
なくともいずれか一方を成形するための導線の導体外表
面上に、順に高透磁率の磁性層と前記磁性層の上に絶縁
層とを各々導体の長さ方向に連続的に設け、前記磁性層
が前記導線の導体内部を通過する磁束を抑制するととも
に前記絶縁層が前記導線の最外周を絶縁するこの単線形
状の導線を巻回或形して上記偏向コイルを構成したこと
を特徴とする偏向ヨーク。1. A conductor for forming at least one of a horizontal deflection coil and a vertical deflection coil, a conductor having a magnetic layer of high permeability and an insulating layer formed on the magnetic layer in that order on the outer surface of the conductor. Is continuously provided in the length direction of the wire, and the magnetic layer suppresses a magnetic flux passing inside the conductor of the wire, and the insulating layer insulates the outermost circumference of the wire. A deflection yoke comprising the above deflection coil.
許請求の範囲第1項記載の偏向ヨーク。2. A deflection yoke according to claim 1, wherein the conducting wire is formed as a stranded wire.
許請求の範囲第1項または第2項記載の偏向ヨーク。3. The deflection yoke according to claim 1 or 2, wherein the magnetic layer is formed by plating.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61061449A JPH081789B2 (en) | 1986-03-17 | 1986-03-17 | Deflection yoke |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61061449A JPH081789B2 (en) | 1986-03-17 | 1986-03-17 | Deflection yoke |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62216140A JPS62216140A (en) | 1987-09-22 |
| JPH081789B2 true JPH081789B2 (en) | 1996-01-10 |
Family
ID=13171375
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61061449A Expired - Lifetime JPH081789B2 (en) | 1986-03-17 | 1986-03-17 | Deflection yoke |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH081789B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01163944A (en) * | 1987-12-21 | 1989-06-28 | Toshiba Corp | Deflection yoke device |
| JP5668097B2 (en) * | 2013-05-15 | 2015-02-12 | 東京特殊電線株式会社 | Electric wire and coil |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5225284B2 (en) * | 1973-07-20 | 1977-07-06 | ||
| JPS52116015A (en) * | 1976-03-25 | 1977-09-29 | Toshiba Corp | Deflecting coil unit of cathode ray tube |
-
1986
- 1986-03-17 JP JP61061449A patent/JPH081789B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62216140A (en) | 1987-09-22 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4692731A (en) | Composite wire, coil and deflection unit for HF applications | |
| US4336420A (en) | Superconducting cable | |
| KR101837264B1 (en) | Coil device and manufacturing method thereof | |
| JPH081789B2 (en) | Deflection yoke | |
| KR101052656B1 (en) | Superconducting cable with wide superconducting wire | |
| JP2002358840A (en) | Flat knit litz wire for high frequency coil | |
| JPS62274535A (en) | deflection yoke | |
| JPH10321358A (en) | Induction heating cooker | |
| JP2001143945A (en) | Transformer for arc welding machine | |
| CN110033918A (en) | A kind of high temperature superconductor coil electric field controls structure | |
| US4982497A (en) | Process for manufacture of a superconductor | |
| JPS63198309A (en) | High frequency transformer | |
| JPS6132335A (en) | Deflection yoke | |
| JPH03248506A (en) | Insulated conductor bundle | |
| JPH0534090Y2 (en) | ||
| US4829417A (en) | High-power transformer | |
| JP3642109B2 (en) | Deflection yoke | |
| JPH0341446Y2 (en) | ||
| JPS62274536A (en) | deflection yoke | |
| JP2602414Y2 (en) | Air core reactor | |
| JPH0315112A (en) | Ritz wire for deflection coil | |
| JPS61109248A (en) | deflection yoke | |
| JPS63264851A (en) | high definition cathode ray tube | |
| JPH0713912B2 (en) | Work coil | |
| JPH11307011A (en) | Deflection yoke |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |