JPS63108651A - Deflection device for cathode-ray tube - Google Patents

Deflection device for cathode-ray tube

Info

Publication number
JPS63108651A
JPS63108651A JP25237386A JP25237386A JPS63108651A JP S63108651 A JPS63108651 A JP S63108651A JP 25237386 A JP25237386 A JP 25237386A JP 25237386 A JP25237386 A JP 25237386A JP S63108651 A JPS63108651 A JP S63108651A
Authority
JP
Japan
Prior art keywords
magnetic field
core
deflection coil
electron gun
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.)
Pending
Application number
JP25237386A
Other languages
Japanese (ja)
Inventor
Norio Oomura
大村 則生
Yukio Nakamura
幸雄 中村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Sony Corp
Original Assignee
Sony Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Sony Corp filed Critical Sony Corp
Priority to JP25237386A priority Critical patent/JPS63108651A/en
Publication of JPS63108651A publication Critical patent/JPS63108651A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To compensate efficiently the mis-convergence in the vertical direction by providing a roop-state core to the electron gun side of a vertical deflection coil. CONSTITUTION:A ring core 5 is provided to the electron gun side from a bend part 2a of the electron gun side of a horizontal deflection coil 2. The core 5 is composed by divided by two and the gap 5g of 5-10 mm is formed between divided parts. The horizontal deflection coil 2 is wrapped and mounted saddlelikely on a bobbin 1. The magnetic field generated at the back side of the coil 4 is absorbed into the core 5 by providing the core 5 to the electron gun side of the vertical deflection coil 4, and a barrel magnetic field is produced at the core 5 part. On the other hand, a pincushion magnetic field is relatively generated at the back side of the coil 4 as a vertical deflection magnetic field is absorbed. The mis-convergence in the vertical direction is compensated at the faceplate peripheral part as an electron beam from the electron gun deflects as the beam proceeds from the core 5 to the coil 4, then the barrel magnetic field is produced at the central part and the pincushion magnetic field at the outside part, and the barrel magnetic field at the peripheral part is made weaker than the intermediate part.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、陰極線管の偏向装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a deflection device for a cathode ray tube.

〔発明のm要〕[Essentials of invention]

本発明は水平偏向コイルが鞍型に巻装されると共に圭直
偏向コイルがトロイダル型に巻装された陰極線管の偏向
装置において、垂直偏向コイルの電子銃側にループ状の
コアを設けることにより、ミスコンバーゼンスが補正さ
れるようにしたものである。
The present invention provides a deflection device for a cathode ray tube in which a horizontal deflection coil is wound in a saddle shape and a straight deflection coil is wound in a toroidal shape, by providing a loop-shaped core on the electron gun side of the vertical deflection coil. , misconvergence is corrected.

〔従来の技術〕[Conventional technology]

例えば、インライン型カラー陰極線管に用いる偏向装置
として第4図に示すものが提案されている。
For example, a deflection device shown in FIG. 4 has been proposed for use in an in-line color cathode ray tube.

同図において、(11はボビンであり、このボビン(1
)の内側に水平偏向コイル(2)が鞍型に巻装される。
In the same figure, (11 is a bobbin, and this bobbin (1
) is wound with a horizontal deflection coil (2) in a saddle shape.

また、ボビン(11の外側において環状のコア(3)に
垂直偏向コイル(4)がトロイダル型に巻装される。
Further, a vertical deflection coil (4) is wound in a toroidal shape around an annular core (3) on the outside of the bobbin (11).

ここで、例えば第5図Aに示すような垂直方向のミスコ
ンバーゼンスを補正するため、垂直偏向コイル(4)に
よる乗置偏向磁界をバレル磁界とすることが知られてい
る。第5図において、Rは赤の電子ビーム、Bは青の電
子ビームを示している。
Here, in order to correct misconvergence in the vertical direction as shown in FIG. 5A, for example, it is known to use a barrel magnetic field as the mounting deflection magnetic field by the vertical deflection coil (4). In FIG. 5, R indicates a red electron beam and B indicates a blue electron beam.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

この場合、画面周辺部でミスコンバーゼンスが補正され
るようにバレル磁界の強さを定めると、中間部ではバレ
ル磁界が弱すぎ、第5図Bに示すようにミスコンバーゼ
ンスは完全には補正されない。
In this case, if the strength of the barrel magnetic field is determined so that the misconvergence is corrected at the periphery of the screen, the barrel magnetic field is too weak at the center, and the misconvergence is not completely corrected as shown in FIG. 5B.

逆に、画面中間部でミスコンバーゼンスが補正されるよ
うにバレル磁界の強さを定めると、周辺部ではバレル磁
界が強すぎ、第5図Cに示すようにミスコンバーゼンス
は過補正されてしまう。
On the other hand, if the strength of the barrel magnetic field is determined so that the misconvergence is corrected in the middle part of the screen, the barrel magnetic field is too strong in the peripheral part, and the misconvergence is overcorrected as shown in FIG. 5C.

本発明は斯る点に鑑み、垂直方向のミスコンバーゼンス
が一層効果的に補正できるようにするものである。
In view of this point, the present invention enables vertical misconvergence to be corrected more effectively.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、上述問題点を解決するため、垂直偏向コイル
(4)の電子銃側にループ状、例えばリング状のコア(
5)を設けるものである。
In order to solve the above-mentioned problems, the present invention provides a loop-shaped, for example, a ring-shaped core (
5).

〔作用〕[Effect]

垂直偏向コイル(4)の電子銃側にリング状コア(5)
を設けることにより、生立偏向コイル(4)の後側に発
生する磁界がコア(5)に吸収され、このコア(5)の
部分でバレル磁界が発生する。一方、垂直偏向コイル(
4)の後(μ;では磁界が吸収されることにより相対的
にビンクッション磁界となる。
A ring-shaped core (5) is placed on the electron gun side of the vertical deflection coil (4).
By providing this, the magnetic field generated on the rear side of the vertical deflection coil (4) is absorbed by the core (5), and a barrel magnetic field is generated in this core (5). On the other hand, the vertical deflection coil (
After 4) (μ;), the magnetic field is absorbed and becomes a relative bin cushion magnetic field.

電子ビームはコア(5)から垂直偏向コイル(4)に進
むにつれて振れていくので、相対的にみて中心部はバレ
ル磁界、外側はビンクッション磁界となり、画面中間部
と周辺部とで逆の歪の磁場が形成される。。
The electron beam deflects as it advances from the core (5) to the vertical deflection coil (4), so relatively speaking, the center becomes a barrel magnetic field and the outside becomes a bottle cushion magnetic field, resulting in opposite distortion between the middle and periphery of the screen. A magnetic field is formed. .

〔実施例〕〔Example〕

以下、図面を参照しながら本発明の一実施例について説
明する。図面において、第4図と対応する部分には同一
符号を付し、その詳IIl説明は省略する。
An embodiment of the present invention will be described below with reference to the drawings. In the drawings, parts corresponding to those in FIG. 4 are designated by the same reference numerals, and detailed explanation thereof will be omitted.

本例においては、築1図に示すように、水平偏向コイル
(2)の電子銃(図示せず)側のベンド部(2a)より
電子銃側にリング状コア(5)が設けられる。このコア
(5)は、例えば焼結コア、モールドコア、プラスチッ
クフェライト、ゴムフェラ・イト、パーマロイ、鉄板等
の軟性強磁性体で形成される。
In this example, as shown in Figure 1, a ring-shaped core (5) is provided closer to the electron gun than the bend portion (2a) of the horizontal deflection coil (2) on the electron gun (not shown) side. This core (5) is formed of a soft ferromagnetic material such as a sintered core, molded core, plastic ferrite, rubber ferrite, permalloy, or iron plate.

また、コア(5)は第2図に示すように2分割されて構
成され、夫々の間に5〜10ymのギャップ(5g)が
形成される。
The core (5) is divided into two parts as shown in FIG. 2, and a gap (5 g) of 5 to 10 mm is formed between each part.

その他は、第4図例と同様に構成される。The rest of the structure is the same as the example shown in FIG.

本例においては、垂直偏向コイル(4)の電子銃側にコ
ア(5)を設けることにより、垂直偏向コイル(4)の
後側に発生する磁界はコア(5)に吸収され、このコア
(5)の部分でバレル磁界が発生する。一方、垂直偏向
コイル(4)の後側では!直偏向磁界が吸収されること
により相対的にビンクッション磁界となる。第3図実線
aはコアク5)を設けたときのvm直偏向磁界の分布を
、コア(5)及び垂直偏向コイル(4)の位置と対応さ
せて示したものである。VX直偏向コイル(4)の後側
の部分lが相対的にビンクッション磁界となっている。
In this example, by providing the core (5) on the electron gun side of the vertical deflection coil (4), the magnetic field generated on the rear side of the vertical deflection coil (4) is absorbed by the core (5). A barrel magnetic field is generated in the part 5). On the other hand, behind the vertical deflection coil (4)! By absorbing the direct deflection magnetic field, it becomes a relative bin cushion magnetic field. The solid line a in FIG. 3 shows the distribution of the vm direct deflection magnetic field when the core (5) is provided, in correspondence with the positions of the core (5) and the vertical deflection coil (4). The rear portion l of the VX direct deflection coil (4) is relatively a bottle cushion magnetic field.

尚、同図破線すはコア(5)を設けないときの分布を示
したものである。
Incidentally, the broken line in the figure shows the distribution when the core (5) is not provided.

電子!Jc (図示せず)からの電子ビームはコア(5
)から垂直偏向コイル(4)に進むにつれて振れていく
ので、相対的にみて中心部はバレル磁界、外側はビンク
ッション磁界となり、画面中間部と周辺部とで逆の歪の
磁場が形成される。結局、周辺部でのバレル磁界は中間
部に比べて弱・められることとなる。したがって、本例
によれば画面周辺部で垂直方向のミスコンバーゼンスが
補正されるようにバレル磁界の強さを定めるとき、中間
部でのバレル磁界は充分強く、第5図りに示すようにミ
スコンバーゼンスが完全に補正される。
Electronic! The electron beam from Jc (not shown) is directed to the core (5
) to the vertical deflection coil (4), so relatively speaking, the center becomes a barrel magnetic field, the outside becomes a bottle cushion magnetic field, and magnetic fields with opposite distortions are formed in the middle and periphery of the screen. . As a result, the barrel magnetic field at the periphery becomes weaker than at the middle. Therefore, according to this example, when determining the strength of the barrel magnetic field so that the vertical misconvergence is corrected at the periphery of the screen, the barrel magnetic field at the middle part is strong enough to correct the misconvergence as shown in Figure 5. is completely corrected.

また、本例においては、コア(5)にギャップ(5g)
が設けられており、このギャップ(5g)のためにコア
(5)に吸収される垂直偏向磁界が減少されるので、ラ
スター歪に対する影響が軽減される。
In addition, in this example, there is a gap (5g) in the core (5).
is provided, and the vertical deflection magnetic field absorbed by the core (5) is reduced due to this gap (5 g), so that the influence on raster distortion is reduced.

このように本例によれば、垂直方向のミスコンバーゼン
スを略完全に補正することができる。
As described above, according to this example, misconvergence in the vertical direction can be almost completely corrected.

尚、上述実施例において、コア(5)は水平偏向コイル
(2)のベンド部(2a)より電子銃側に設けられてい
るが、第1図破線で示すように、水平偏向コイル(2)
のベンド部(2a)と工直偏向コイル(4)との間に設
けてもよい。また、上述実施例において、コア(5)は
リング状とされているが、必ずしもリング状である必要
はなくループ状であればよい。また、上述実施例におい
て、コア(5)にはギャップ(5g)が設けられている
が、ラスター歪に対する影響を考えないならば、ギャッ
プ(5g)を設ける必要はない。
In the above embodiment, the core (5) is provided closer to the electron gun than the bend portion (2a) of the horizontal deflection coil (2), but as shown by the broken line in FIG.
It may be provided between the bend portion (2a) and the engineering deflection coil (4). Further, in the above-mentioned embodiments, the core (5) is ring-shaped, but it does not necessarily have to be ring-shaped and may be loop-shaped. Further, in the above embodiment, the core (5) is provided with a gap (5g), but if the influence on raster distortion is not considered, there is no need to provide the gap (5g).

ところで、同様にリング状磁性体を設ける偏向装置は例
えば実開昭58−64058号公報に記載されているが
、その考案においては、垂直偏向磁界を螢光面(スクリ
ーン)側においてビンクッション磁界とするものにおい
て、垂直偏向磁界の中心を螢光面側にずらすために設け
られるものであり、本発明とは全く異なるものである。
By the way, a deflection device similarly provided with a ring-shaped magnetic body is described in, for example, Japanese Utility Model Application No. 58-64058, but in that device, the vertical deflection magnetic field is converted into a bottle cushion magnetic field on the fluorescent surface (screen) side. This is provided to shift the center of the vertical deflection magnetic field toward the fluorescent surface, and is completely different from the present invention.

〔発明の効果〕〔Effect of the invention〕

以上述べた実施例からも明らかなように本発明によれば
、生立偏向コイルの電子銃側にループ状のコアを設け、
相対的にみて中心部はバレル磁界、外側はビンクッショ
ン磁界となり、両面中間部と周辺部とで逆の歪の磁場が
形成されるようにしたので、垂直方向のミスコンバーゼ
ンスを略完全に補正することができる。
As is clear from the embodiments described above, according to the present invention, a loop-shaped core is provided on the electron gun side of the vertical deflection coil,
Relatively speaking, the center part becomes a barrel magnetic field and the outer part becomes a bottle cushion magnetic field, so that magnetic fields with opposite distortions are formed in the middle part and the peripheral part of both sides, so vertical misconvergence can be almost completely corrected. be able to.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図及び第2図は本発明の一実施例を示す構成図、第
3図はその説明のための図、第4図は従来例の構成図、
第5図はミスコンバーゼンスの説明図である。 (1)はボビン、(2)は水平偏向コイル、(3)はコ
ア、(4)は世直偏向コイル、(5)はリング状コア、
(5g)はギャップである。
1 and 2 are configuration diagrams showing one embodiment of the present invention, FIG. 3 is a diagram for explaining the same, and FIG. 4 is a configuration diagram of a conventional example,
FIG. 5 is an explanatory diagram of misconvergence. (1) is a bobbin, (2) is a horizontal deflection coil, (3) is a core, (4) is a world deflection coil, (5) is a ring-shaped core,
(5g) is a gap.

Claims (1)

【特許請求の範囲】 水平偏向コイルが鞍型に巻装されると共に垂直偏向コイ
ルがトロイダル型に巻装された陰極線管の偏向装置にお
いて、 上記垂直偏向コイルの電子銃側にループ状のコアを設け
ることを特徴とする陰極線管の偏向装置。
[Claims] In a cathode ray tube deflection device in which a horizontal deflection coil is wound in a saddle shape and a vertical deflection coil is wound in a toroidal shape, a loop-shaped core is provided on the electron gun side of the vertical deflection coil. A deflection device for a cathode ray tube.
JP25237386A 1986-10-23 1986-10-23 Deflection device for cathode-ray tube Pending JPS63108651A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25237386A JPS63108651A (en) 1986-10-23 1986-10-23 Deflection device for cathode-ray tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25237386A JPS63108651A (en) 1986-10-23 1986-10-23 Deflection device for cathode-ray tube

Publications (1)

Publication Number Publication Date
JPS63108651A true JPS63108651A (en) 1988-05-13

Family

ID=17236402

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25237386A Pending JPS63108651A (en) 1986-10-23 1986-10-23 Deflection device for cathode-ray tube

Country Status (1)

Country Link
JP (1) JPS63108651A (en)

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