JPS5829897Y2 - electromagnetic deflection yoke - Google Patents

electromagnetic deflection yoke

Info

Publication number
JPS5829897Y2
JPS5829897Y2 JP16356877U JP16356877U JPS5829897Y2 JP S5829897 Y2 JPS5829897 Y2 JP S5829897Y2 JP 16356877 U JP16356877 U JP 16356877U JP 16356877 U JP16356877 U JP 16356877U JP S5829897 Y2 JPS5829897 Y2 JP S5829897Y2
Authority
JP
Japan
Prior art keywords
coil
deflection yoke
core
winding
distribution
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
Application number
JP16356877U
Other languages
Japanese (ja)
Other versions
JPS5488222U (en
Inventor
真和 綾
正和 寺岡
章 青木
Original Assignee
松下電器産業株式会社
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 松下電器産業株式会社 filed Critical 松下電器産業株式会社
Priority to JP16356877U priority Critical patent/JPS5829897Y2/en
Publication of JPS5488222U publication Critical patent/JPS5488222U/ja
Application granted granted Critical
Publication of JPS5829897Y2 publication Critical patent/JPS5829897Y2/en
Expired legal-status Critical Current

Links

Description

【考案の詳細な説明】 陰極線管用の電磁偏向ヨークにおいて、水平コイル又は
垂直コイルの磁界分布を画像特性が最適になる様に偏向
ヨークを設計する為に、コイルの捲線分布を変えること
は、よく行なわれている。
[Detailed description of the invention] In an electromagnetic deflection yoke for a cathode ray tube, in order to design the deflection yoke so that the magnetic field distribution of the horizontal coil or vertical coil optimizes the image characteristics, it is often necessary to change the winding distribution of the coil. It is being done.

特に、コサイン分布と称し、C08xθなる電線分で捲
線するものは、その代表的なものである。
In particular, a typical one is called a cosine distribution and is wound with wire segments of C08xθ.

ところが、コアとして断面形状が円形のものを用いると
コサイン巻きしたのではコアとコイルとの間に空間が生
じて偏向ヨーク効率が悪くなり、また絶縁セパレータも
面倒なものとなる欠点があった。
However, when a core with a circular cross-sectional shape is used and cosine winding is used, a space is created between the core and the coil, resulting in poor deflection yoke efficiency, and the insulating separator is also troublesome.

一方、電磁偏向ヨークの偏向エネルギーはフインクに依
ると(テレビジョン・工学ハンドブック)次式であられ
される。
On the other hand, according to Fink (Television Engineering Handbook), the deflection energy of the electromagnetic deflection yoke is expressed by the following equation.

WM=0.35310 ’E X D a X Fβj
ouleE:高圧(KV)Da:コア内径(cm)Fβ
:定数つまりコア内径に偏向エネルギーが比例すること
を意味している。
WM=0.35310 'E X D a X Fβj
ouleE: High pressure (KV) Da: Core inner diameter (cm) Fβ
: Constant, meaning that the deflection energy is proportional to the core inner diameter.

そこで本考案は、断面円形のコアを用いてしかもコサイ
ン分布と同様の磁界分布をコアとコイルとの空間を少な
くして実現できる電磁偏向ヨークを提供するものである
Therefore, the present invention provides an electromagnetic deflection yoke that uses a core with a circular cross section and can realize a magnetic field distribution similar to a cosine distribution while reducing the space between the core and the coil.

以下、本考案の一実施について図面を参照して説明する
Hereinafter, one implementation of the present invention will be described with reference to the drawings.

第1図において、1 a、1 b、2a、2bは、水平
コイル、3はセパレーター、4は垂直コイル、5はフェ
ライトコアである。
In FIG. 1, 1a, 1b, 2a, and 2b are horizontal coils, 3 is a separator, 4 is a vertical coil, and 5 is a ferrite core.

第1図から明らかな様に、コアの内径は点P1〜P4の
ところで決定される。
As is clear from FIG. 1, the inner diameter of the core is determined at points P1 to P4.

つまり電線の捲線角度を変えてもコサイン分布とほぼ同
一の磁界分布を得ることができれば、上記の問題点を解
決できる。
In other words, if it is possible to obtain a magnetic field distribution that is almost the same as a cosine distribution even if the winding angle of the electric wire is changed, the above problem can be solved.

実験例を以下に示す。An experimental example is shown below.

ここでは断面形状が第2図のように大径a=110mm
、小径b=60mm、長さc=50mmのコア5を用い
、ピッチ1.098°(360゜に328本捲ける)で
捲溝を設は各溝に第3図に示すように番号を付与する。
Here, the cross-sectional shape is large diameter a = 110 mm as shown in Figure 2.
Using a core 5 with a small diameter b = 60 mm and a length c = 50 mm, winding grooves were created at a pitch of 1.098° (328 windings at 360°), and each groove was numbered as shown in Figure 3. do.

そして、まず従来のコサイン分布巻きとして、第2〜1
8,20,21,22,24,25゜26.28,30
,32,36,40,42.50の各溝に同一方向に捲
線をし、それらに同一方向に電流を流す。
First, as a conventional cosine distribution winding, the second to first
8,20,21,22,24,25°26.28,30
, 32, 36, 40, 42, and 50 grooves in the same direction, and current is passed through them in the same direction.

この場合には巻線分布が第4図aのように片寄るので空
間が生じる。
In this case, since the winding distribution is biased as shown in FIG. 4a, a space is created.

これに対し、本考案の実施例においては、第2.4,6
,8,10,12,14,16,18,20,22,2
4,26,28゜30.32,36.40;42.50
の各溝に同一方向に捲線し、第58.62,64,66
.68,70,72,74,76.78の各溝には逆方
向に電流を流すように捲線して両捲線を接続した。
On the other hand, in the embodiment of the present invention, Nos. 2.4 and 6
,8,10,12,14,16,18,20,22,2
4,26,28°30.32,36.40;42.50
Winding in the same direction in each groove of No. 58, 62, 64, 66
.. Each of the grooves 68, 70, 72, 74, 76, and 78 was wound with a wire so that the current flowed in the opposite direction, and the two windings were connected.

このコイルの磁界分布は従来のコサイン分布巻のものと
ほぼ同一の磁界分布となった。
The magnetic field distribution of this coil was almost the same as that of the conventional cosine distribution winding.

この場合には捲線分布は第4図すのように一様につなが
るが、このように巻線角度を変えても理想的な磁界分布
を得ることができたものである。
In this case, the winding distribution is uniformly connected as shown in Figure 4, but even if the winding angle is changed in this way, an ideal magnetic field distribution can be obtained.

具体的な実施方法としては、第1図の水平コイルの1a
、1b、2a、2bの部分を第4図すの様に構成して実
現できる。
As a specific implementation method, 1a of the horizontal coil in Fig.
, 1b, 2a, and 2b can be constructed as shown in FIG.

また、垂直コイルに対して同様に実施することもできる
ものである。
Moreover, it can also be implemented in the same way for vertical coils.

このように本考案によれば、一様な捲線分布で実現でき
るのでコアの内径を小さくすることができて効率を向上
することができ、かつ、セパレーターの製作を容易にす
ることができるものである。
As described above, according to the present invention, since a uniform winding distribution can be realized, the inner diameter of the core can be reduced, efficiency can be improved, and the separator can be manufactured easily. be.

また、プリントコイル等を用いる場合に特に効果がある
ものである。
Moreover, it is particularly effective when using a printed coil or the like.

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

第1図は本考案の一実施例における電磁偏向ヨークの断
面図、第2図は同ヨークに用いるコアの断側面図、第3
図は捲線を説明するための図、第4図は捲線分布を説明
するための図である。 1 a、1 b、2 a、2 b・・・・・・水平コイ
ル、3・・・・・・セパレータ、4・・・・・・垂直コ
イル、5・・・・・・コア。
Fig. 1 is a sectional view of an electromagnetic deflection yoke according to an embodiment of the present invention, Fig. 2 is a sectional side view of a core used in the yoke, and Fig. 3 is a sectional view of a core used in the yoke.
The figure is a diagram for explaining the winding, and FIG. 4 is a diagram for explaining the winding distribution. 1 a, 1 b, 2 a, 2 b...horizontal coil, 3...separator, 4...vertical coil, 5...core.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 水平コイルと垂直コイルを有し、水平偏向軸と垂直偏向
軸とで分割される4つの領域のどの一つの領域において
もその領域内の水平コイルもしくは垂直コイルの一部の
電線に流れる電流の向きを残りの部分の電線に流れる電
流の向きと異ならせてなる電磁偏向ヨーク。
In any one of the four regions that have a horizontal coil and a vertical coil and are divided by a horizontal deflection axis and a vertical deflection axis, the direction of the current flowing in a part of the electric wire of the horizontal coil or vertical coil in that region. An electromagnetic deflection yoke that makes the current flow in a different direction from the rest of the wire.
JP16356877U 1977-12-05 1977-12-05 electromagnetic deflection yoke Expired JPS5829897Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16356877U JPS5829897Y2 (en) 1977-12-05 1977-12-05 electromagnetic deflection yoke

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16356877U JPS5829897Y2 (en) 1977-12-05 1977-12-05 electromagnetic deflection yoke

Publications (2)

Publication Number Publication Date
JPS5488222U JPS5488222U (en) 1979-06-22
JPS5829897Y2 true JPS5829897Y2 (en) 1983-06-30

Family

ID=29160322

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16356877U Expired JPS5829897Y2 (en) 1977-12-05 1977-12-05 electromagnetic deflection yoke

Country Status (1)

Country Link
JP (1) JPS5829897Y2 (en)

Also Published As

Publication number Publication date
JPS5488222U (en) 1979-06-22

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