JPH0210543B2 - - Google Patents
Info
- Publication number
- JPH0210543B2 JPH0210543B2 JP15195383A JP15195383A JPH0210543B2 JP H0210543 B2 JPH0210543 B2 JP H0210543B2 JP 15195383 A JP15195383 A JP 15195383A JP 15195383 A JP15195383 A JP 15195383A JP H0210543 B2 JPH0210543 B2 JP H0210543B2
- Authority
- JP
- Japan
- Prior art keywords
- coil
- deflection
- coils
- core
- turns
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
- H01J29/46—Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
- H01J29/70—Arrangements for deflecting ray or beam
- H01J29/72—Arrangements for deflecting ray or beam along one straight line or along two perpendicular straight lines
- H01J29/76—Deflecting by magnetic fields only
- H01J29/764—Deflecting by magnetic fields only using toroidal windings
Description
【発明の詳細な説明】
この発明はテレビジヨン受信機等の陰極線管に
装着される偏向ヨークの改良に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a deflection yoke mounted on a cathode ray tube of a television receiver or the like.
従来のテレビジヨン受像機に用いられる偏向ヨ
ークとしては、第1図に示すように略円筒状もし
くはラツパ状のコア1に線材をトロイダル状に巻
き付けてコイル2としたものが知られており、こ
のコイル2は巻数、線材径等巻線仕様をほぼ同一
とした略点対称の一対あるいは複数対のものとし
て形成されている。また、それぞれのコイル2は
第2図に示すように直列(あるいは並列)に接続
して略同一電流が流れるように構成し、第3図に
示すような略対称形の磁界分布を形成している。 A known deflection yoke used in conventional television receivers is one in which a coil 2 is formed by winding a wire in a toroidal shape around a substantially cylindrical or wrapper-shaped core 1, as shown in FIG. The coil 2 is formed as a pair or a plurality of substantially symmetrical pairs with substantially the same winding specifications such as the number of turns and wire diameter. In addition, the respective coils 2 are connected in series (or in parallel) as shown in Fig. 2 so that substantially the same current flows, and a substantially symmetrical magnetic field distribution as shown in Fig. 3 is formed. There is.
このような従来のトロイダル形偏向ヨークは次
のような欠点を有している。 Such a conventional toroidal deflection yoke has the following drawbacks.
(1) 同一性のかなり高い一対もしくは複数対のコ
イルを製造しなければならないため、巻線装置
に特別の配慮が必要。(1) Because one or more pairs of coils with a high degree of identity must be manufactured, special consideration is required for the winding device.
(2) 高インピーダンス、すなわち多数巻数を要求
されるコイルにおいては、リンギング等の対策
から多層分割巻としなければならず、製造時間
が長くなる。(2) For coils that require high impedance, that is, a large number of turns, multi-layer split winding is required to prevent ringing, etc., which increases manufacturing time.
等である。etc.
この発明は以上のような欠点に鑑みてなされた
もので、一方のコイルを閉回路として誘導電流に
よつて偏向磁界を形成し、偏向コイルの製造を容
易としたものである。 The present invention has been made in view of the above-mentioned drawbacks, and it is intended to facilitate the manufacture of a deflection coil by forming a deflection magnetic field using an induced current by forming one of the coils into a closed circuit.
以下、この発明を一実施例である第4図、第5
図について説明する。 Hereinafter, this invention will be described as an example in FIGS. 4 and 5.
The diagram will be explained.
第5図において、2は本来の巻線仕様でコア1
に巻き付けられた第1のコイル、3は第1のコイ
ル2と断面が点対称となるように形成された第2
のコイルで、インダクタンスと直流抵抗の比が第
1のコイル2と同一となる巻線仕様に形成されて
いる。また、一対のコイル2,3は第4図に示す
ように第1のコイル2を偏向回路出力端に接続
し、第2のコイル3を閉回路としている。 In Figure 5, 2 is the original winding specification and core 1
The first coil 3 is wound around the first coil 2, and the second coil 3 is formed so that its cross section is point symmetrical to that of the first coil 2.
The coil is formed with winding specifications such that the ratio of inductance to DC resistance is the same as that of the first coil 2. Further, as shown in FIG. 4, the pair of coils 2 and 3 connects the first coil 2 to the output end of the deflection circuit, and makes the second coil 3 a closed circuit.
このような構成のもとで、一対のコイル2,3
間の関係は内鉄形の変圧器と同じであり、第1の
コイル2側からみた交流インピーダンスはコイル
2,3の巻数比で変換され、直列接続時のインピ
ーダンスと同等になる。また、第2のコイル3に
は第1のコイル2による誘導電圧により、
i2=N1/N2i1
i1:第1のコイル2に流える電流
N2:第1のコイル2の巻数
i2:第2のコイル3に流れる電流
N2:第2のコイル3の巻数
となり、巻数比の逆比の電流が流れることにな
る。したがつて、第2のコイル3による発生磁界
φ2は、
φ2=K・N2・12=K・N2・N1/N2・i1
=K・N1・11≒φ1
となり、一対のコイル2,3の巻数比には無関係
で第1のコイル2による発生磁界φ1にかなり近
い磁界を得ることが可能となる。例えば14″カラ
ーテレビ用偏向ヨークにおいて、本来の巻線仕様
のコイルを製作し、第2図に示すように直列接続
した場合と、第4図に示すように一方のコイルを
短絡した場合を比較した結果、後者の偏向ヨーク
による垂直振幅は前者の約98%であつた。すなわ
ち、第2のコイル3を第1のコイル2の巻線仕様
と異ならせても、インダクタンスと直流抵抗の比
を同一にすればほぼ同等の偏向磁界を発生させる
ことができ、この結果、第2のコイル3を第1の
コイル2より太い線材によつて形成すれば、第2
のコイル3の巻線を減少させることが可能とな
り、製造時間を短縮することができる。例えば、
第1のコイル2として直径Dの線材を用いて巻数
Nの本来の巻線仕様に製作し、第2のコイル3と
して直径が√2Dの線材を用いて巻数がN/2のコ
イルを製作すれば、両コイル2,3を同一仕様の
ものにした従来のものとほぼ同様の偏向特性を持
つ偏向ヨークを得ることができる。 Under such a configuration, a pair of coils 2 and 3
The relationship between them is the same as that of a core type transformer, and the AC impedance seen from the first coil 2 side is converted by the turns ratio of the coils 2 and 3, and becomes equivalent to the impedance when connected in series. In addition, due to the induced voltage caused by the first coil 2 in the second coil 3, i 2 =N 1 /N 2 i 1 i 1 : Current flowing in the first coil 2 N 2 : Current flowing in the first coil 2 Number of turns i 2 : Current flowing through the second coil 3 N 2 : Number of turns of the second coil 3, and a current having the inverse ratio of the turns ratio flows. Therefore, the magnetic field φ 2 generated by the second coil 3 is: φ 2 =K・N 2・1 2 =K・N 2・N 1 /N 2・i 1 =K・N 1・1 1 ≒φ 1 , and it is possible to obtain a magnetic field quite close to the magnetic field φ 1 generated by the first coil 2, regardless of the turns ratio of the pair of coils 2 and 3. For example, for a deflection yoke for a 14" color TV, compare the case where coils with the original winding specifications are manufactured and connected in series as shown in Figure 2, and the case where one coil is short-circuited as shown in Figure 4. As a result, the vertical amplitude due to the deflection yoke of the latter was about 98% of the former.In other words, even if the winding specifications of the second coil 3 were different from those of the first coil 2, the ratio of inductance to DC resistance could be maintained. If they are made the same, almost the same deflection magnetic field can be generated.As a result, if the second coil 3 is made of a thicker wire than the first coil 2, the second coil 3
It becomes possible to reduce the number of windings of the coil 3, and the manufacturing time can be shortened. for example,
The first coil 2 is manufactured to the original winding specification with the number of turns N using a wire with a diameter of D, and the second coil 3 is manufactured with a wire with a diameter of √2D and the number of turns is N/2. For example, it is possible to obtain a deflection yoke having almost the same deflection characteristics as the conventional one in which both the coils 2 and 3 have the same specifications.
このことは、第2のコイル3を製作する際に巻
数を半分にすることが可能であり、巻線時間の短
縮に有利であるばかりではなく、使用する線材の
直径が大きくなることにより材料費単価が安くな
る利点がある。巻数を1/3、1/4…と少なくするこ
とにより、この利点は拡大する。また、第2のコ
イル3の閉回路中に可変抵抗、可変インダクタン
ス等の電流調整素子を挿入することによつて非対
象性等の補正を行なわせることができ、さらにコ
ア1の結合係数を調整することによつて直線性の
補正も行なわせることができる。さらにまた、第
1のコイル2に直流分を重畳すれば、第2のコイ
ル3には流れないため歪や非対象性の補正に対し
て有効である。 This allows the number of turns to be halved when manufacturing the second coil 3, which is not only advantageous in shortening the winding time, but also reduces material costs by increasing the diameter of the wire used. It has the advantage of being cheaper. This advantage is expanded by reducing the number of turns to 1/3, 1/4, etc. In addition, by inserting a current adjustment element such as a variable resistor or variable inductance into the closed circuit of the second coil 3, it is possible to correct asymmetry, etc., and further adjust the coupling coefficient of the core 1. By doing so, linearity can also be corrected. Furthermore, if a DC component is superimposed on the first coil 2, it will not flow through the second coil 3, which is effective for correcting distortion and asymmetry.
なお、上述の実施例においては、一対の略点対
称のコイルを例として説明したが、複数対偶数個
のトロイダルコイルで構成される偏向ヨークにお
いても同様に適用することができる。 In the above-mentioned embodiment, a pair of substantially point-symmetrical coils was explained as an example, but the present invention can be similarly applied to a deflection yoke composed of a plurality of pairs of even number of toroidal coils.
以上、説明したように、この発明によれば、偏
向ヨークの設計、製造に新たな自由度を与えるこ
とができ、この発明の実用価値は大である。 As described above, according to the present invention, a new degree of freedom can be given to the design and manufacture of the deflection yoke, and the practical value of the present invention is great.
第1図〜第3図は従来のトロイダル形偏向ヨー
クの構成を示す概要図、第4図、第5図はこの発
明の一実施例である偏向ヨークを示す概要図であ
る。
図中、1はコア、2は第1のコイル、3は第2
のコイルである。なお、図中、同一符号は同一あ
るいは相当する部分を示すものとする。
1 to 3 are schematic diagrams showing the structure of a conventional toroidal deflection yoke, and FIGS. 4 and 5 are schematic diagrams showing a deflection yoke according to an embodiment of the present invention. In the figure, 1 is the core, 2 is the first coil, and 3 is the second coil.
It is a coil of In addition, in the figures, the same reference numerals indicate the same or corresponding parts.
Claims (1)
にトロイダル状に巻き付けられた第1のコイル
と、この第1のコイルと断面が点対称となるよう
に上記コアにトロイダル状に巻き付けられ、イン
ダクタンスと直流抵抗の比が上記第1のコイルと
同一の第2のコイルとを備え、上記第1のコイル
を偏向回路出力端に接続すると共に、上記第2の
コイルを閉回路として上記第1のコイルに流れる
電流を誘導させ、偏向磁界を形成するようにした
ことを特徴とする偏向ヨーク。1 A cylindrical or wrapper-shaped core, a first coil wound toroidally around this core, and a first coil wound toroidally around the core so that its cross section is point symmetrical to that of the first coil, and an inductance. a second coil having the same direct current resistance ratio as the first coil; the first coil is connected to the output end of the deflection circuit, and the second coil is connected to the first coil as a closed circuit; A deflection yoke characterized by inducing a current flowing through the yoke to form a deflection magnetic field.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15195383A JPS6044946A (en) | 1983-08-20 | 1983-08-20 | deflection yoke |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15195383A JPS6044946A (en) | 1983-08-20 | 1983-08-20 | deflection yoke |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6044946A JPS6044946A (en) | 1985-03-11 |
| JPH0210543B2 true JPH0210543B2 (en) | 1990-03-08 |
Family
ID=15529813
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15195383A Granted JPS6044946A (en) | 1983-08-20 | 1983-08-20 | deflection yoke |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6044946A (en) |
-
1983
- 1983-08-20 JP JP15195383A patent/JPS6044946A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6044946A (en) | 1985-03-11 |
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