JPH02126514A - Bound insulation cable and deflection yoke using same - Google Patents
Bound insulation cable and deflection yoke using sameInfo
- Publication number
- JPH02126514A JPH02126514A JP16315989A JP16315989A JPH02126514A JP H02126514 A JPH02126514 A JP H02126514A JP 16315989 A JP16315989 A JP 16315989A JP 16315989 A JP16315989 A JP 16315989A JP H02126514 A JPH02126514 A JP H02126514A
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- wire
- insulated wire
- coil
- bundled
- 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
- 238000009413 insulation Methods 0.000 title abstract description 13
- 239000004020 conductor Substances 0.000 claims abstract description 59
- 239000011248 coating agent Substances 0.000 claims abstract description 7
- 238000000576 coating method Methods 0.000 claims abstract description 7
- 239000003973 paint Substances 0.000 claims abstract description 6
- 238000004804 winding Methods 0.000 claims description 7
- 230000000694 effects Effects 0.000 description 8
- 230000020169 heat generation Effects 0.000 description 5
- 238000004519 manufacturing process Methods 0.000 description 5
- 230000000052 comparative effect Effects 0.000 description 4
- 230000004927 fusion Effects 0.000 description 3
- 239000004952 Polyamide Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000002500 effect on skin Effects 0.000 description 2
- 229920002647 polyamide Polymers 0.000 description 2
- 229920002635 polyurethane Polymers 0.000 description 2
- 239000004814 polyurethane Substances 0.000 description 2
- 239000000853 adhesive Substances 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229920006122 polyamide resin Polymers 0.000 description 1
- 229920005749 polyurethane resin Polymers 0.000 description 1
Abstract
Description
【発明の詳細な説明】
c′M業上の利用分野〕
本発明は、高周波用コイルに用いるに好適な絶縁電線に
関し、更にほこの絶g電線を用いて偏向コイルの発熱を
抑制せしめた高精細度用途に好適な偏向ヨークに関する
ものである。[Detailed Description of the Invention] Field of Application in the C'M Industry] The present invention relates to an insulated wire suitable for use in a high-frequency coil, and furthermore, the present invention relates to an insulated wire suitable for use in a high-frequency coil, and furthermore, the present invention relates to an insulated wire suitable for use in a high-frequency coil, and furthermore, the present invention relates to a high-temperature insulated wire suitable for use in a high-frequency coil, and furthermore, a high-temperature insulated wire that suppresses heat generation in a deflection coil by using a low-g wire. This invention relates to a deflection yoke suitable for high-definition applications.
周知のように、高周波コイルの発熱はコイルの直流抵抗
損失分によ′る発熱と1°b周波抵抗損失分による発熱
とに要因を区分することができる。偏向ヨークにあって
は、その主たる発熱源として偏向コイルが挙げられ、最
近のように、IfE精細精細度−段と進んだ陰極線管表
示装置においては、偏向ヨークに適用される偏向走査周
波数は33klb、 84敗更には130に&といった
高周波数となってきている。このような高周波域になる
と、偏向コイル導体中に発生する渦電流による損失が無
視し得なくなり、直流抵抗分による損失に比し高周波域
程度による損失の影響が暑く増大する。上記の高周波域
程度ではコイル導体の表皮効果による損失の影響はあま
り顕著ではなく、堝i!流損失が支配的である。かかる
偏向コイルの高周波抵抗損失の増大は当然のことながら
偏向コイルの発熱量の増大をもたらし、偏向ヨークの性
能、信頼性を低下せしめることになる。As is well known, the causes of heat generation in a high frequency coil can be divided into heat generation due to direct current resistance loss of the coil and heat generation due to 1°b frequency resistance loss. In the deflection yoke, the main heat source is the deflection coil, and in recent years, in cathode ray tube display devices that have advanced to IfE definition, the deflection scanning frequency applied to the deflection yoke is 33 klb. , 84 losses and even 130 losses, which is becoming a high frequency. In such a high frequency range, the loss due to eddy current generated in the deflection coil conductor cannot be ignored, and the influence of the loss due to the high frequency range increases significantly compared to the loss due to DC resistance. In the above-mentioned high frequency range, the effect of loss due to the skin effect of the coil conductor is not very noticeable, and the effect of loss due to the skin effect of the coil conductor is not so significant. flow loss is dominant. Such an increase in the high frequency resistance loss of the deflection coil naturally results in an increase in the amount of heat generated by the deflection coil, resulting in a decrease in the performance and reliability of the deflection yoke.
そこで、偏向コイルの高周波抵抗損失の低減を図る目的
で、従来より偏向コイルのコイル用ffl線として、複
数本の細径絶縁I1互いに撚り合わせ、各絶縁素線が撚
り線の断面のすべての位置を順次重めるよう形成したり
ソツ線或は絶g:素線の複数本を単に同芯撚りまたは集
合撚りした集合撚り電線が公知であり、これら電線を用
いた偏向ヨークがまたよく知られている。Therefore, in order to reduce the high-frequency resistance loss of the deflection coil, conventionally, as an FFL wire for the coil of the deflection coil, a plurality of small diameter insulated I1 wires are twisted together, and each insulated wire is located at every position in the cross section of the stranded wire. A group-stranded electric wire in which a plurality of wires are simply concentrically twisted or collectively twisted is known, and a deflection yoke using these electric wires is also well-known. ing.
以下、高周波用電線として一般的なリッツ線を例に説明
を進める。The following explanation will be given using a litz wire, which is a common high-frequency electric wire, as an example.
第4図にリッツ線の構造を図示する。同図(a)はりソ
ツ線の横断面図、同図(b)は自己融着型リッツ線の横
断面図、同図(C)は自己融着型リッツ線の外観斜視図
である。FIG. 4 illustrates the structure of a litz wire. Figure (a) is a cross-sectional view of the beam wire, Figure (b) is a cross-sectional view of the self-fusion type litz wire, and Figure (C) is an external perspective view of the self-fusion type litz wire.
10はリッツ線511はリッツ線を構成する細径絶縁素
線で細径導体12の外周に絶縁度V、層13が被覆され
ている。そして、この複数本の細径絶a索線11の各々
が、上述の如く、撚り合わせ断面のすべての位置を順次
に占めるよう互いに撚り合わせられてリッツ線lOが形
成されている。クラ型偏向コイルに巻回する場合には、
同図(b)に図示する如く、上記リッツ線10の外周上
に融着層6を施した自己融着型リッツ線10’が用いら
れる。10, a litz wire 511 is a thin insulated wire constituting a litz wire, and the outer periphery of a thin conductor 12 is coated with a layer 13 having an insulation degree of V. As described above, each of the plurality of small-diameter wires 11 is twisted together to form a litz wire 10 so as to sequentially occupy all the positions of the twisted cross section. When winding around a Kura-type deflection coil,
As shown in FIG. 2B, a self-fusion type litz wire 10' is used, in which a fusion layer 6 is provided on the outer periphery of the litz wire 10.
リッツ線或は集合撚り電線は高周波コイル用電線として
用いられたとき高周波抵抗損失が低減され、これを巻回
した偏向コイルは高周波抵抗ttt失に伴う発熱量を低
減せしめる上でそれなりの効果を発揮している。しかし
、リッツ線や集合撚り電線を使用した偏向コイルはコイ
ルの信頼性や製品コス1−の面でなお改善すべき課題を
有している。When a litz wire or a mass stranded electric wire is used as a wire for a high-frequency coil, high-frequency resistance loss is reduced, and a deflection coil wound with this wire has a certain effect in reducing the amount of heat generated due to the loss of high-frequency resistance ttt. are doing. However, deflection coils using Litz wires or collectively stranded electric wires still have problems that need to be improved in terms of coil reliability and product cost.
即ち、
illリッツM成は集合撚り電線を巻回した偏向コイル
にあっては、偏向コイルのコイル形成部所面精に占める
コイル導体の有効断面積がリッツ線或は集合撚り電線を
構成する各絶縁素線の絶縁皮膜の総計皮膜断面積の分だ
け減少せしめられている。In other words, in the case of a deflection coil made by winding a stranded wire, the effective cross-sectional area of the coil conductor in the coil forming area of the deflection coil is equal to that of each of the litz wires or the stranded wire. It is reduced by the total cross-sectional area of the insulation coating of the insulating wire.
コイルの導体実効断面積が減ぜられるということは後述
するように、コイルの発熱量低減に対しマイナスの作用
を及ぼすものである。The reduction in the effective cross-sectional area of the conductor of the coil has a negative effect on reducing the amount of heat generated by the coil, as will be described later.
(2)リッツ線或は集合撚りffi線は、それぞれに絶
縁皮膜を施した各素線を比較的細かなピッチで撚り合わ
せて形成するものであるため、撚り工程で各絶縁素線の
絶縁皮膜に加工劣化を及ぼす恐れも多く、偏向コイルの
信頼性を損う恐れがある。(2) Litz wires or mass-twisted FFI wires are formed by twisting individual wires each coated with an insulating film at a relatively fine pitch. There is also a high risk that processing deterioration may occur, which may impair the reliability of the deflection coil.
(3)更に、リッツ線或は集合黙り電線は電線の製造工
数を多く要するため電線コストの面から、又偏向コイル
の製造工程の面では偏向コイルのリード線の端末処理工
程における各細径絶B電線の絶縁皮膜除去処理など煩雑
な作業を多く生じ、偏向ヨーク生産の効率を悪くしてい
た。(3) Furthermore, since Litz wires or collective silent wires require a large number of man-hours to manufacture wires, in terms of wire costs, and in terms of the manufacturing process of deflection coils, it is important to This resulted in a lot of complicated work such as removing the insulation film from the B wires, which made the production of deflection yokes less efficient.
本発明は、かかる従来のりソツ線或は集合撚り電線及び
これを使用した偏向ヨークの課題を解決し、高周波抵抗
損失に伴う発熱量をより低減せしめた。より信頼性の高
い、生産性の良い高周波用コイル電線及びこれを用いた
偏向ヨークを堤供しようとするものである。The present invention solves the problems of the conventional twisted wire or multi-stranded electric wire and the deflection yoke using the same, and further reduces the amount of heat generated due to high frequency resistance loss. The present invention aims to provide a high-frequency coil electric wire with higher reliability and better productivity, and a deflection yoke using the same.
本発明は、複数本の裸導体を断面略円形状に束ねた集束
導体を芯導体とし、この集束導体の外周に絶縁塗料を塗
布焼付して絶縁皮膜を施した集束絶縁電線、或はコイル
形成の必要性に応じ前記絶縁皮膜層上に自己融着皮膜層
を施した自己融着型の集束絶縁電線を特徴とし、更にか
かる集束絶縁電線を水平偏向コイルまたは垂直偏向コイ
ルのいずれか一方の偏向コイル若しくは両偏向コイルに
巻回した偏向ヨークを特徴とするものである。The present invention provides a focused insulated wire or a coil formed by using a focusing conductor made by bundling a plurality of bare conductors with a substantially circular cross section as a core conductor, and applying and baking an insulating paint to the outer periphery of the focusing conductor to form an insulating film. The invention is characterized by a self-fusing insulated wire in which a self-fusing film layer is applied on the insulating film layer according to the necessity of the invention, and the insulated wire is further deflected into either a horizontal deflection coil or a vertical deflection coil. It is characterized by a deflection yoke wound around a coil or both deflection coils.
本発明の集束絶縁電線或は自己融着型集束絶縁′11!
線にあっては、これら絶縁電線を初成する複数本の導体
素線はそれぞれ絶縁層の施されていない裸導体であり、
集束された各裸導体素線は互いに導通状態にある。従っ
て、当然集束導体内には高周波渦電流が生ずることにな
る。しかし、隣接する各導体素線相互には、各導体素線
が円形であるところから、横断面において点接触導通を
形成することになる。このため、集束導体内での渦電流
経路の電気抵抗が高く、発生する渦電流は低く押えられ
、渦電流損に伴う高周波抵抗の増加は比較的小さなもの
となり、更に次に述べる効果の影響が大きく作用し、従
来のりソツ線或は集合撚り電線に比しコイルの発熱量を
全体として低減せしめる結果となる。即ち、本発明の集
束絶縁電線或は自己融着型集束絶R電線の場合、同一仕
上外径。The bundled insulated wire or self-bonding type bundled insulation '11 of the present invention!
In the case of wires, the multiple conductor strands that initially form these insulated wires are bare conductors without an insulating layer,
The bundled bare conductor strands are electrically connected to each other. Therefore, high frequency eddy currents naturally occur within the focusing conductor. However, since each conductor strand is circular, point contact continuity is formed between adjacent conductor strands in the cross section. Therefore, the electrical resistance of the eddy current path within the focusing conductor is high, the generated eddy current is kept low, the increase in high frequency resistance due to eddy current loss is relatively small, and the effects described below are This has a large effect, resulting in a reduction in the amount of heat generated by the coil as a whole compared to conventional twisted wires or collective stranded wires. That is, in the case of the bundled insulated wire or the self-bonding type bundled insulated wire of the present invention, the finished outer diameter is the same.
同一素線本数で構成されるリンツ線或は集合撚り1!線
と比較したとき、集束絶縁電線又は自己融着型集束絶縁
i[線を構成する各導体1r4線は絶縁皮膜の施されて
いない分、各導体lF4線の導体径を太くすることが可
能である。このことは、コイル電線としてコイルに巻回
したとき、コイル形成断面積に占めるコイル導体部の実
効断面積、即ち導体占積率を高めることになる。a向コ
イルにおいて、コイル導体占積率を高めるということは
、偏向コイルのインダクタンスLと直流抵抗Rの比、L
/Rを高めることにつながる。何となれば、インダクタ
ンスLは偏向コイルの巻数により、また直流抵抗Rは偏
向コイル導体の断面積により一義的に定まるものである
からである。Linz wire or collective twist consisting of the same number of strands 1! When compared to wires, each conductor 1r4 wire constituting the focused insulated wire or self-bonding focused insulated wire is not coated with an insulating film, so it is possible to increase the conductor diameter of each conductor IF4 wire. be. This increases the effective cross-sectional area of the coil conductor portion in the coil forming cross-sectional area, that is, the conductor space factor when the wire is wound around a coil as a coil wire. In the a-direction coil, increasing the coil conductor space factor means increasing the ratio of the deflection coil inductance L to DC resistance R, L
/R. This is because the inductance L is uniquely determined by the number of turns of the deflection coil, and the DC resistance R is uniquely determined by the cross-sectional area of the deflection coil conductor.
一方、L/Rと偏向コイルの発熱に伴う温度上昇度との
間には明らかな相関関係があることが発明各等によって
実験的に確認されている。第2図は偏向走査周波数を3
3臘に設定したときのクラ型偏向コイルの温度上昇度△
TとL/Rの関係を示す実間結果である。即ち、L/R
は偏向コイルの発熱量と密接な関連を持ち、L/Rを大
きく取ることが偏向コイルの発熱量を低減せしめる上で
大きな効果をもたらすことが明白にL’lめられる。On the other hand, it has been experimentally confirmed by various inventors that there is a clear correlation between L/R and the degree of temperature rise due to heat generation of the deflection coil. Figure 2 shows the deflection scanning frequency of 3
Temperature rise degree of Cla-shaped deflection coil when set to 3 △
These are actual results showing the relationship between T and L/R. That is, L/R
is closely related to the amount of heat generated by the deflection coil, and it is clear that increasing L/R has a large effect on reducing the amount of heat generated by the deflection coil.
〔実施例〕
以下、本発明の実施例を第1図に沿い説明する。第1図
(a)は本発明の集束絶縁電線の横断面図、同図(b)
は各導体素線を平行に束ねた集束絶縁電線の外観斜視図
、同図(e)は各導体J4mを撚り合わせて東ねた儂束
絶81!線の外観斜視図、同図(d)は自己融着型集束
絶M電線の横断面図である。[Example] Hereinafter, an example of the present invention will be described with reference to FIG. FIG. 1(a) is a cross-sectional view of the bundled insulated wire of the present invention, and FIG. 1(b) is a cross-sectional view of the bundled insulated wire of the present invention.
is a perspective view of a bundled insulated wire in which each conductor wire is bundled in parallel, and the same figure (e) is a diagram of a bundled insulated wire made by twisting each conductor J4m together. The external perspective view of the wire is shown in FIG.
1は集束絶縁ffi線である。集束1体4は複数本の裸
導体素tiA3を平行に断面略円形状に束ねるか若しく
は複数本の裸導体素線3を集束導体4の層芯径の約10
0倍以上の極めて粗い撚りを付与し断面略円形状に束ね
て形成される。なお、集束導体4は複数本の裸導体素線
3を通常の撚りピッチで同芯撚り或は集合撚りしたもの
であっても何等差し支えない、そして、かかる集束導体
4の外周にポリウレタン樹脂等の絶縁塗料を所要膜厚と
なるよう塗布焼付して絶縁皮膜6を施すことにより、集
束絶縁電線1が形成される。また、クラ型偏向コイルの
如き自己保持型コイルに巻回するときは、上記の集束絶
縁電線lの絶縁皮膜層5の外周に更にポリアミド系樹脂
などの自己FsA着塗料を塗布焼付してPJA着層6を
設けた自己l!IlR型集束絶縁”11M2が用いられ
る。1 is a focused insulated ffi wire. The bundle 4 is made by bundling a plurality of bare conductor elements tiA3 in parallel to have a substantially circular cross section, or by bundling a plurality of bare conductor wires 3 into a bundle approximately 10 times the layer core diameter of the bundle conductor 4.
It is formed by giving an extremely coarse twist of 0 times or more and bundling it into a substantially circular cross section. Note that the focusing conductor 4 may be made by concentrically or collectively twisting a plurality of bare conductor strands 3 at a normal twisting pitch, and the outer periphery of the focusing conductor 4 may be made of polyurethane resin or the like. The bundled insulated wire 1 is formed by applying an insulating coating 6 by applying and baking an insulating paint to a required thickness. When winding around a self-holding coil such as a club type deflection coil, a self-adhesive FsA paint such as polyamide resin is further coated on the outer periphery of the insulating film layer 5 of the above-mentioned bundled insulated wire l and baked to adhere to the PJA. Self with layer 6! IIR type focused insulation "11M2" is used.
一実施例として、係る自己融着型集束絶B電線2を巻回
した本発明にJ&づくクラ型偏向コイルと、比較例とし
て従来の自己mm型リッツ線10’を巻回したクラ型偏
向コイルについて、性能比較を行なった結果を次に記す
。As an example, there will be shown a Kura-type deflection coil made by J& of the present invention, which is wound with such a self-fusion type focused wire 2, and as a comparative example, a Kula-type deflection coil, which is formed by winding a conventional self-fusing mm-type Litz wire 10'. The results of the performance comparison are described below.
比較例のクラ型偏向コイルは、素線導体径0.12關φ
のポリウレタン絶縁素線7本をピッチ6Illlで撚り
合わせ、外周にポリアミド融着層を施し仕上り外径0.
46−φとした自己融着型リンツ線を巻回して形成され
た。実施例のクラ型偏向コイルは、導体径0.14−φ
の裸導体素線を7水平行に断面略円形状に東ね、この外
周にポリウレタン絶縁層及びポリアミド融で層を順次施
し、前記比較例の自己融着型リンツ線と同一仕上り外径
0.46+amφとした自己融着型集束絶縁電線を巻回
して形成された。The comparative example of the Cla-type deflection coil has a wire conductor diameter of 0.12 mm.
Seven polyurethane insulated wires are twisted together at a pitch of 6 Ill, and a polyamide fusion layer is applied to the outer periphery to give a finished outer diameter of 0.
It was formed by winding a self-fusing Lindt wire with a diameter of 46-φ. The Cla-shaped deflection coil of the example has a conductor diameter of 0.14-φ
Bare conductor wires were laid out in 7 horizontal parallels to have an approximately circular cross section, and a polyurethane insulating layer and a polyamide melting layer were successively applied to the outer periphery of the bare conductor wire to give the same finish and outer diameter as the self-bonding Lindt wire of the comparative example. It was formed by winding a self-fusion type focused insulated wire having a diameter of 46+amφ.
この実施例及び比較例のクラ型偏向コイルについてそれ
ぞれの特性を比較測定した結果9本発明の自己融着型集
束絶縁電線を巻回したクラ型偏向コイルは従来の自己融
着型リッツ線を巻回したクラ型偏向コイルに比へ、偏向
コイルの導体占積宰即ちL/Hにおいて36%向−ヒし
、偏向走査周波数331&における偏向コイルの温度上
昇度は7〜8deg(摂氏)低下することが確認された
。なお1本発明の集束絶giitt線或は自己融着型集
束絶縁電線は上記の偏向コイルの実施例に限定されるも
のではなく、その他の高周波用コイルにも適用できるこ
とは勿論であり、同様の効果が得られることはいうまで
もない。The results of comparing and measuring the characteristics of the Cla-type deflection coils of this example and comparative example. Compared to the rotated horn type deflection coil, the conductor density of the deflection coil is 36% higher at L/H, and the temperature rise of the deflection coil at the deflection scanning frequency of 331& is reduced by 7 to 8 degrees (Celsius). was confirmed. Note that the insulated insulated wire or self-bonding insulated wire of the present invention is not limited to the deflection coil described above, and can of course be applied to other high-frequency coils, as well as similar Needless to say, it is effective.
上述の如く、本発明の集束絶縁電線或は自己融着型集束
絶縁Iu線は、これをコイル巻線したとき、コイルの導
体占8!率が大幅に向上する結果、コイルの高周波抵抗
損失に伴う発熱量低減に大きく寄与する。更に電線の端
末処理における絶縁皮膜除去が容易となる。As mentioned above, when the bundled insulated wire or self-bonding type bundled insulated Iu wire of the present invention is wound into a coil, the conductor of the coil is 8! As a result of the greatly improved efficiency, this greatly contributes to reducing the amount of heat generated due to high-frequency resistance loss in the coil. Furthermore, the insulation film can be easily removed during wire terminal treatment.
また、上記の集束絶縁tTl線或は自己融、n型集束性
の向上が図られるとともに、偏向コイルのリド端末処理
工程における絶縁皮膜除去が容易となるなど偏向ヨーク
の組立作業の効率が向上し、偏向ヨーク製造コストの低
減を可能とした。In addition, the above-mentioned focusing insulated tTl wire or self-fusing, n-type focusing ability is improved, and the efficiency of the assembly work of the deflection yoke is improved, such as by making it easier to remove the insulation film in the lead terminal processing process of the deflection coil. This made it possible to reduce the manufacturing cost of the deflection yoke.
第1図は本発明の集束絶縁電線を丞し、同図(a)は集
束線M′電線の横断面図、同図(b)は各導体素線を平
行に束ねた集束絶縁電線の外a1斜視図、同図(c)は
各導体、製線を撚り合わせて束ねた集束絶縁電線の外観
斜視図、同図(d)は自己融着型集束絶縁電線の横断面
図である。第2図はクラ型偏向コイルのインダクタンス
Lと直流抵抗Rとの比。
■、/Rとクラ型偏向コイルの温度上只度Δ′Fとの関
係を示すグラフ(偏向走査周波数33−ヒにおける)、
第3図はクラ型偏向コイルの外形図、第4図(a)はり
ソツ線の横断面図、同図(b)は自己融着型リッツ線の
横断面図、同図(c)は自己融着型リッツ線の斜視外g
i図である。
1−一集束絶縁電線、2 自己融着型集束絶縁R線、
3− 裸導体素線
4 懐束導体、5
絶B層、6 融刀層。
クラ型偏向コイルFigure 1 shows a bundled insulated wire of the present invention, (a) is a cross-sectional view of the bundled wire M' wire, and (b) is a cross-sectional view of the bundled insulated wire in which each conductor wire is bundled in parallel. A1 is a perspective view, FIG. 1C is an external perspective view of a bundled insulated wire made by twisting and bundling each conductor and wire, and FIG. 1D is a cross-sectional view of a self-fusion type bundled insulated wire. Figure 2 shows the ratio between the inductance L and the DC resistance R of the Cla-shaped deflection coil. (2) A graph showing the relationship between /R and the temperature difference Δ'F of the curved deflection coil (at a deflection scanning frequency of 33-hi);
Figure 3 is an outline drawing of a Cla-shaped deflection coil, Figure 4 (a) is a cross-sectional view of a beam-shaped deflection coil, Figure 4 (b) is a cross-sectional view of a self-fusion type Litz wire, and Figure 4 (c) is a cross-sectional view of a self-fusing type Litz wire. Oblique view of fused litz wire g
This is a diagram. 1-1 bundled insulated wire, 2 self-fusion type bundled insulated R wire,
3- Bare conductor strand 4 Bundled conductor, 5 Absolute B layer, 6 Fusion layer. Cla type deflection coil
Claims (6)
導体を形成し、該集束導体の外周上に絶縁塗料を塗布焼
付けして、絶縁皮膜を施したことを特徴とする集束絶縁
電線。(1) A focusing device characterized in that a plurality of bare conductor strands are bundled to have a substantially circular cross section to form a focusing conductor, and an insulating coating is applied on the outer periphery of the focusing conductor by coating and baking an insulating coating. Insulated wire.
向に平行に断面略円形状に束ねられていることを特徴と
する請求項1記載の集束絶縁電線。(2) The bundled insulated wire according to claim 1, wherein the bundled conductor is a bundle of a plurality of bare conductor strands parallel to the longitudinal direction of the strands so as to have a substantially circular cross section.
以上の極めて粗い撚りを付与し、断面略円形状に束ねら
れていることを特徴とする請求項1記載の集束絶縁電線
。(3) The focused insulated wire according to claim 1, wherein the focusing conductor is twisted extremely coarsely at least about 100 times the layer core diameter of the focusing conductor, and is bundled to have a substantially circular cross section.
縁皮膜外周上に自己融着性塗料を塗布焼付けして自己融
着皮膜を施したことを特徴とする自己融着型の集束絶縁
電線。(4) A self-fusing type bundle characterized in that a self-fusing coating is applied by applying and baking a self-fusing paint on the outer periphery of the insulating film of the bundled insulated wire according to claim 1, 2 or 3. Insulated wire.
向ヨークの少なくとも一方の偏向コイルに、請求項1、
2又は3記載の集束絶縁電線を巻回してなることを特徴
とする偏向ヨーク。(5) Claim 1,
A deflection yoke characterized by being formed by winding the focused insulated wire according to 2 or 3.
方をクラ型偏向コイルで形成した偏向ヨークの該少なく
とも一方のクラ型偏向コイルに、請求項4記載の自己融
着型集束絶縁電線を巻回してなることを特徴とする偏向
ヨーク。(6) The self-fusion type focusing insulated wire according to claim 4 is wound around at least one of the horizontal deflection coil and the vertical deflection coil in the deflection yoke, in which at least one of the horizontal deflection coil and the vertical deflection coil is formed of a cross-shaped deflection coil. A deflection yoke characterized by:
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63-167374 | 1988-07-05 | ||
JP16737488 | 1988-07-05 |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02126514A true JPH02126514A (en) | 1990-05-15 |
Family
ID=15848530
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16315989A Pending JPH02126514A (en) | 1988-07-05 | 1989-06-26 | Bound insulation cable and deflection yoke using same |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02126514A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008053143A (en) * | 2006-08-28 | 2008-03-06 | Matsushita Electric Works Ltd | High frequency power supply line |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61109207A (en) * | 1984-11-01 | 1986-05-27 | 住友電気工業株式会社 | Insulated stranded wire |
JPS6261206A (en) * | 1985-09-10 | 1987-03-17 | 住友電気工業株式会社 | Melting twist-insulated wire for internal machine wiring |
-
1989
- 1989-06-26 JP JP16315989A patent/JPH02126514A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61109207A (en) * | 1984-11-01 | 1986-05-27 | 住友電気工業株式会社 | Insulated stranded wire |
JPS6261206A (en) * | 1985-09-10 | 1987-03-17 | 住友電気工業株式会社 | Melting twist-insulated wire for internal machine wiring |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008053143A (en) * | 2006-08-28 | 2008-03-06 | Matsushita Electric Works Ltd | High frequency power supply line |
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