JPS60189845A - Deflection york - Google Patents

Deflection york

Info

Publication number
JPS60189845A
JPS60189845A JP4512084A JP4512084A JPS60189845A JP S60189845 A JPS60189845 A JP S60189845A JP 4512084 A JP4512084 A JP 4512084A JP 4512084 A JP4512084 A JP 4512084A JP S60189845 A JPS60189845 A JP S60189845A
Authority
JP
Japan
Prior art keywords
magnetic field
correction
eddy current
deflection
magnetic
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
JP4512084A
Other languages
Japanese (ja)
Inventor
Masaaki Ito
正明 伊藤
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.)
Victor Company of Japan Ltd
Nippon Victor KK
Original Assignee
Victor Company of Japan Ltd
Nippon Victor KK
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 Victor Company of Japan Ltd, Nippon Victor KK filed Critical Victor Company of Japan Ltd
Priority to JP4512084A priority Critical patent/JPS60189845A/en
Publication of JPS60189845A publication Critical patent/JPS60189845A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/46Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
    • H01J29/70Arrangements for deflecting ray or beam
    • H01J29/701Systems for correcting deviation or convergence of a plurality of beams by means of magnetic fields at least
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/46Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
    • H01J29/70Arrangements for deflecting ray or beam
    • H01J29/72Arrangements for deflecting ray or beam along one straight line or along two perpendicular straight lines
    • H01J29/76Deflecting by magnetic fields only

Landscapes

  • Video Image Reproduction Devices For Color Tv Systems (AREA)

Abstract

PURPOSE:To enable correction to be performed without causing any convergence shift by installing magnetic-field-producing means facing metallic parts installed in a color picture tube to produce magnetic fields contradicting magnetic fields produced by eddy currents induced by the metallic parts. CONSTITUTION:A deflection york 20 is attached to a color receiver 2 in such a manner that an upper permanent magnet 22 faces a metallic member 8 and a lower permanent magnet 23 faces metallic members 9 and 10, so that a correction magnetic field 26 overlaps eddy current magnetic fields 13 and 13' and a correction magnetic field 28 overlaps eddy current magnetic fields 14 and 14'. Therefore the eddy currents 13 and 13' are contradicted by the correction magnetic field 26 and the eddy current magnetic fields 14 and 14' are contradicted by the correction magnetic field 28. As a result, misconvergences 15 and 16 are both corrected and an image with good quality is regenerated on a screen 2b. Accordingly correction can be performed without causing any convergence shift as a side effect.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は偏向ヨークに係り、特にインライン配置の3木
の電子銃を有するカラー受像管に用いられる偏向ヨーク
に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a deflection yoke, and more particularly to a deflection yoke used in a color picture tube having three in-line electron guns.

従来技術 一般に、インライン型のカラー受像装置1は、第1図に
示すように、カラー受像管2に偏向ヨーク3を組付けて
なる4i4成である。偏向ヨーク3は、セパレータ4の
外側の上下側に垂直偏向コイル5a、5b、セパレータ
4の内側の左右側に第2図に示す水平偏向コイル6a 
、6bを設けた構成である。
BACKGROUND OF THE INVENTION In general, an in-line type color image receiving apparatus 1 is of a 4i4 configuration in which a deflection yoke 3 is assembled to a color picture tube 2, as shown in FIG. The deflection yoke 3 has vertical deflection coils 5a, 5b on the upper and lower sides outside the separator 4, and horizontal deflection coils 6a shown in FIG. 2 on the left and right sides inside the separator 4.
, 6b are provided.

水平偏向コイル6a 、6bには、第3図に示す鋸歯状
波形aの水平偏向電流が加えられ、偏向ヨーク3内に垂
直方向の磁束群よりなる水平偏向磁界7が発生し、ネッ
ク2a内の電子銃より出射された電子ビームR,G、B
が水平方向に変更されてスクリーン2b上を左から右方
向へ走査しつ)スクリーン2bの左上部から順次右下部
へ走M丈る。なお第2図は第1図中■−■線に沿う拡大
断m1矢視図であり、以j(第2図に似た図は全てスク
リーン211側よりみた図である。また、第2図は、下
方に向く磁束が減少しつ)あり、蛍光面2C上のビーム
スボッ(・がスクリーン211の左側端より中火に向か
って移動しつ)ある途中の状態を示1゜ところで、カラ
ー受像管2は、第1図に示t J:うに、この内部C−
n ’)水平変更磁界7内に、全C全屈製である電子銃
の篩部8.ゲッタ9.及びゲッタ支持板10(以下金属
部品ともいう)を有する。これらは、偏向ヨーク3をJ
J準にしてみると、水平偏向コイル6a 、6bが相対
向する面(水平軸Xで示J)に対して、偏向」−り1の
中心0点−(直交Jる垂直軸Y上に配されている。
A horizontal deflection current having a sawtooth waveform a as shown in FIG. Electron beams R, G, B emitted from the electron gun
is changed in the horizontal direction and scans the screen 2b from left to right, and then sequentially moves from the upper left to the lower right of the screen 2b. Note that FIG. 2 is an enlarged cross-sectional view taken along the line ■-■ in FIG. 1° shows a state in which the downward magnetic flux is decreasing) and the beam spot on the phosphor screen 2C is moving from the left end of the screen 211 toward the medium flame. 2 is shown in Figure 1.
n') In the horizontally changing magnetic field 7, the sieve part 8 of the electron gun, which is made of all-C, is placed in the horizontally changing magnetic field 7. Getta 9. and a getter support plate 10 (hereinafter also referred to as metal component). These are the deflection yoke 3
In terms of J, the horizontal deflection coils 6a and 6b face each other (indicated by the horizontal axis has been done.

金属部品8.9.10に交流の水平偏向磁界7が印加さ
れると、これらに渦電流が発生し、この渦電流により渦
電流磁界が水平偏向磁界を形成している垂直方向磁束の
変化を妨げるにうに発生り−る。
When an alternating current horizontal deflection magnetic field 7 is applied to metal parts 8.9.10, eddy currents are generated in these parts, and the eddy current magnetic field causes changes in the vertical magnetic flux forming the horizontal deflection magnetic field. There are things that will hinder you.

ビームスボッ]・がスクリーン2bの左端より中央−〇
移動しつ・あり、1・方に向く水平偏向磁束が減少づる
方向に変化しているときには、金属部品8.9.10の
渦電流は第2図に示1ように水平偏向磁束を増す方向の
磁束11a、1 lb、12a。
When the beam block] is moving from the left end of the screen 2b to the center and the horizontal deflection magnetic flux toward 1 is changing in a decreasing direction, the eddy current in the metal part 8.9.10 is As shown in the figure, magnetic fluxes 11a, 1 lb, and 12a are directed to increase the horizontal deflection magnetic flux.

1211を発生し、金属部品8及び金属部品9゜10の
周囲には夫々渦電流磁界13.14が形成される。また
ビームスボッ1−がスクリーン2bの中央を通過し史に
これを右方に移動さけるときには、水平偏向磁束は方向
が反転して上方に向き、徐々に増加゛する。この場合に
は、金属部品8,9゜10の渦電流は、この水平偏向磁
束を減する方向の磁束、即ち上記磁束t1a、11b、
12a。
1211, and eddy current magnetic fields 13 and 14 are formed around the metal parts 8 and 9 and 10, respectively. Further, when the beam spot 1- passes through the center of the screen 2b and moves to the right, the horizontal deflection magnetic flux reverses its direction and points upward, gradually increasing. In this case, the eddy currents in the metal parts 8, 9 and 10 cause the magnetic flux in the direction that reduces this horizontal deflection magnetic flux, that is, the magnetic flux t1a, 11b,
12a.

12bど同じ方向の磁束11a’ 、1111’ 。Magnetic flux 11a', 1111' in the same direction as 12b.

12a’、12b’ を発生し、金属部品8及び金属部
品9.10の周囲には夫々上記の渦電流磁卯13.17
Iど同質の渦電流磁界13’ 、14’ が形成される
。即ち、偏向ヨーク3内には、本来の水平偏向磁界7に
加えて、渦電流磁界13.13’。
12a', 12b', and the above-mentioned eddy current magnetic circles 13.17 are generated around the metal parts 8 and 9.10, respectively.
Similar eddy current magnetic fields 13' and 14' are formed. That is, in the deflection yoke 3, in addition to the original horizontal deflection magnetic field 7, there is an eddy current magnetic field 13,13'.

14、II’が形成されることになる。14, II' will be formed.

このため、電子ビームR,G、Bのうら特に両側の電子
ビームR,13は、第4図中上d;に示づように、スク
リーン21)の上下方向中心より上方に偏向されて:I
r−、右方向中心部を走査する際に、渦電流磁界13.
13’ により矢印F+、F2で示す偏向力を受り、ま
た同図中下部に示Iにうに、スクリーン21)の+hに
偏向されて左右方向中心部を走査づる際に、;スト^電
流磁界14.14’ により矢印F3..F<で示づ偏
向力を受ける。これにより、スクリーン2bにtよ、第
5図に示づ゛にうに1上下側のIEイコ1j向申央イ]
近に、破線丸印で間Iυで示すミスコンバーゼンス15
.16が発生ずる。
Therefore, the back of the electron beams R, G, and B, particularly the electron beams R and 13 on both sides, are deflected upward from the vertical center of the screen 21), as shown in FIG.
r-, eddy current magnetic field 13. when scanning the center right direction.
13' receives deflection forces shown by arrows F+ and F2, and as shown in I at the bottom of the same figure, when the screen 21) is deflected by +h and scans the center in the left and right direction, ;sto^ current magnetic field 14.14' indicates arrow F3. .. It receives a deflection force indicated by F<. As a result, the screen 2b is displayed as shown in FIG.
Nearby, Miss Convergence 15 is indicated by the dashed circle and the interval Iυ.
.. 16 will occur.

上記の渦電流磁界はゲッタ9の近傍で特に大となり、上
記の渦電2It H1t界に起因するミスコンバーゼン
スはゲッタ9側で人となる。またこのミスコンバーゼン
ス15.16は、高級ディスプレイ装置等のように水平
偏向周波数が高くなる程顕著となって、画像品位を低下
させるものであり、補正する必要がある。
The above-mentioned eddy current magnetic field becomes particularly large near the getter 9, and the misconvergence caused by the above-mentioned eddy electric 2It H1t field becomes noticeable on the getter 9 side. Further, this misconvergence 15.16 becomes more pronounced as the horizontal deflection frequency becomes higher, such as in a high-end display device, and degrades the image quality, so it is necessary to correct it.

なJ3、上記のミスコンバーゼンス15.16は、垂直
偏向磁界分布を変えてなお9つ垂直偏向磁界の中心軸と
電子ビームの中心軸をノf右方向にずらすことで修正す
ることがG能ではある。しかし、この修正の結果、スク
リーンの四隅に、第6図に示すような横線のコンバーゼ
ンスずれ、即ち、左側で所謂正クロス、右側で逆クロス
というパターンが副作用的に生じてしまい、このコンバ
ーゼンスずれを更に補正づ−る必要がありこの修正方法
は生産性上採用づることは困難である。
J3, the above misconvergence 15.16 can be corrected by changing the vertical deflection magnetic field distribution and shifting the center axis of the vertical deflection magnetic field and the center axis of the electron beam to the right. be. However, as a result of this correction, a convergence shift of the horizontal lines as shown in Figure 6 occurs as a side effect at the four corners of the screen, that is, a pattern of a so-called normal cross on the left side and a reverse cross on the right side, and this convergence shift is caused. Further correction is required, and this correction method is difficult to employ in terms of productivity.

問題点を解決づるための手段 そこで、本発明は上記問題点を解決した偏向ヨークを提
供することを目的どするものであり、その構成は、イン
ライン配F?の3本の電子銃を右づるカラー受像管に組
付けられて使用される偏向ヨークにおいて、該カラー受
像管に絹(=Jけられた状態で該カラー受像管内の金属
部に対向Jる位首に、偏向磁Wにより該金属部に誘起さ
れる渦電流により生ずる渦電流磁界を打ち消すようζ’
cWA界を発生さ′Uる磁界発生手段を備えてなる構成
としたものである。
Means for Solving the Problems Therefore, it is an object of the present invention to provide a deflection yoke that solves the above-mentioned problems, and the structure thereof is an in-line arrangement F? In a deflection yoke that is used with the three electron guns attached to a right-handed color picture tube, the color picture tube is fitted with silk (=J) that faces the metal part inside the color picture tube when it is cut out. ζ' on the neck to cancel the eddy current magnetic field generated by the eddy current induced in the metal part by the deflection magnet W.
The structure includes magnetic field generating means for generating a cWA field.

実施例 第7図は本発明になる偏向ヨーク20の−実茄例を示し
、第8図はこの偏向ヨーク20をI]刊け〔なるカラー
受象装置21を丞づ。第9図は偏向二1−り20にJ、
るミスコンバーぜンス補正動作を説明づる図で69る1
、各図中、第1図及び第2図に小り(14成部分と同一
部分には同一符号をイ」シその説明は省略り゛る。
Embodiment FIG. 7 shows an actual example of the deflection yoke 20 according to the present invention, and FIG. 8 shows the deflection yoke 20 with a color receiving device 21. FIG. 9 shows J on the deflection 21-20;
A diagram explaining the misconvergence correction operation
, in each figure, the same parts as those shown in FIG. 1 and FIG.

q!7図中、22.23は人々永久磁石であり、偏向ヨ
ーク20の大(¥口側を囲繞゛するリング部材271の
保持部2/la、24b内に収納されて、偏向]−り2
0の中心Oを通る垂直軸Y上に設りられている。この垂
直軸Yは水平偏向磁界7を形成りる磁束の方向と同じ方
向に延在する線である。
q! In Fig. 7, reference numerals 22 and 23 are permanent magnets, which are housed in the holding parts 2/la and 24b of the ring member 271 that surrounds the large side of the deflection yoke 20, and are used for deflection.
It is placed on the vertical axis Y passing through the center O of 0. This vertical axis Y is a line extending in the same direction as the direction of the magnetic flux forming the horizontal deflection magnetic field 7.

また永久I!i石22.23は磁極の方向をYlllh
と一致した向ぎで配しである。
Eien I again! i stone 22.23 has the magnetic pole direction Yllllh
It is arranged in the same direction.

特に上側の永久磁石22は、下側がS極であり、磁束2
5a 、 2 !”)11で表わされる補正磁界2Gを
光牛J−る。−F側の永久磁石23は−L側がN極であ
り、磁束27a、271)で表わされる補正磁界28を
光牛Jる。
In particular, the upper permanent magnet 22 has an S pole on the lower side, and the magnetic flux 2
5a, 2! The permanent magnet 23 on the -F side has an N pole on the -L side, and the correction magnetic field 28 expressed as magnetic fluxes 27a and 271) is applied.

」−記の偏向ヨー920は、第8図及び第9図に示すよ
うに、上側の永久磁石22が金属部品8に対向し、下側
の永久磁?Ei23が金属部品9,10に対向して、カ
ラー受像管2に紺イ・]()られており、補正磁界2G
は渦電流磁界13.13’ と重畳し、補正磁界2ε3
は渦電流磁界14,1/l’ と重畳J−る。
As shown in FIGS. 8 and 9, the deflection yaw 920 shown in FIG. Ei 23 is placed in navy blue on the color picture tube 2 facing the metal parts 9 and 10, and a correction magnetic field 2G is applied.
is superimposed with the eddy current magnetic field 13.13', and the correction magnetic field 2ε3
is superimposed with the eddy current magnetic field 14,1/l'.

こ)で、補正van26の磁束25a、25bLL、前
記の渦電流磁界13.13’の磁束11a。
In this case, the magnetic fluxes 25a and 25bLL of the correction van 26 and the magnetic flux 11a of the eddy current magnetic field 13 and 13'.

11a’ 、11b、11b’ と逆方向であり、電子
ビームR,Bは補正磁界2G内を通過づるどさに、前記
偏向力[箱、[−2とは逆向きで且つこれら、と等しい
大ぎさの偏向力Fl’、F2’を受りる。このため、電
子ビームR,Bは、渦電流磁界13.13’ ど補正磁
界26どが徂昏している磁界内を通過覆るときには、」
−記偏向力[:1ど]:1′及び]:2とF2’ とが
バランスし、Y軸方向へは偏向されずにX軸(水平方向
)に偏向され、第5図中上側のミスコンバーゼンス15
は修正されて解消される。
11a', 11b, and 11b', and as the electron beams R and B pass through the correction magnetic field 2G, the deflection force [box, [-2] is in the opposite direction and is equal to these. It receives the deflection forces Fl' and F2' of the grip. Therefore, when the electron beams R and B pass through the magnetic fields in which the eddy current magnetic fields 13, 13' and the correction magnetic field 26 are wandering,
- The deflection forces [:1, etc.]:1' and ]:2 and F2' are balanced, and the deflection is not deflected in the Y-axis direction but in the X-axis (horizontal direction). Convergence 15
will be corrected and eliminated.

また、補正vAvI28 (7)磁束27a、27bl
l、前記の渦電流磁界14.14’ の磁束12a。
Also, correction vAvI28 (7) Magnetic flux 27a, 27bl
l, magnetic flux 12a of said eddy current magnetic field 14.14'.

12a’ 、12b、12b’ と逆方向であり、電子
ビーム1<、Bは補正磁界28内を通過覆るときに、前
記偏向力F3.F4とは逆向きで1つこれらと等しい人
ささの偏向力F3’ *、、Fa ’ を受りる。この
ため、電子ビームR,Bは、渦電流磁界1/1.14’
 ど補正磁界28とが重畳し−(いる磁界内を通過する
どきには、上記偏向力F3と1−3′及び「4どF4’
 とがバランスし、Y軸方向へは偏向されずにX軸(水
平方向)に偏向され、915図中下側のミス」ンバーゼ
ンス1Gが修正されて解消される。
12a', 12b, 12b', and when the electron beam 1<, B passes through the correction magnetic field 28, the deflection force F3. It receives a man-sized deflection force F3'*, , Fa' which is opposite to F4 and equal to these. Therefore, the electron beams R and B have an eddy current magnetic field of 1/1.14'
When passing through a magnetic field in which the correction magnetic field 28 is superimposed, the deflection forces F3 and 1-3' and "F4'
are balanced, and the beam is deflected in the X-axis (horizontal direction) without being deflected in the Y-axis direction, and the misconvergence 1G on the lower side of Figure 915 is corrected and eliminated.

換言すれば、渦電流磁界13.13’ は補正磁界2G
により、’dr^電梳磁界14.14は補正磁界28に
より人々(」消された状態となり、上記のミスコンバー
ゼンス15,16は其に補正され、スクリーン2bには
良質の画像が再生される。
In other words, the eddy current magnetic field 13.13' is the correction magnetic field 2G
As a result, the electric field 14, 14 is erased by the correction magnetic field 28, the above-mentioned misconvergence 15, 16 is corrected, and a high-quality image is reproduced on the screen 2b.

なお、こ)で永久磁石22.23の磁力は、渦電流磁界
13.13’ 、1/1.14’ を打消しうる強さの
補正磁界26.28を発生しうるように定めであるのは
勿論である。
In this case, the magnetic force of the permanent magnets 22.23 is determined to generate a correction magnetic field 26.28 strong enough to cancel the eddy current magnetic field 13.13', 1/1.14'. Of course.

なお、スクリーン2bの上部又は下部のいずれか一方で
コンバーげンスずれが大きく、他方で小さい場合には、
永久磁石をずれが人さい側だけに配すれば、実用上十分
な効果が得られることもある。
Note that if the convergence shift is large at either the top or bottom of the screen 2b and small at the other,
If the permanent magnets are placed only on the side with the slightest deviation, a sufficient practical effect may be obtained.

また、上記の永久磁?Ei22.23の代わりに、直流
電流を供給され、巻軸線をY軸と一致ざUて配されたコ
イルを使用してもよく、」−記と同様の補正磁界26.
28が形成されて同様の効果を右づる。
Also, the permanent magnetism mentioned above? Instead of Ei 22.23, a coil may be used which is supplied with a direct current and whose winding axis is aligned with the Y axis, and which has a correction magnetic field 26.
28 is formed to create a similar effect.

上記の実施例では、渦電流磁界13.13’ 。In the above example, the eddy current magnetic field 13.13'.

11!1.14’ を常時打消づ構成としであるが、渦
電流磁界は電子ビーム1(、Bがこの磁界内にあるとき
に打?l’jされ1ばよいことになる。従って上記直流
電流の代わりに垂直偏向電流の一部を上記田イルに流り
ようにしてもよい。この場合には、電子ビーム1(、B
が上下に偏向されたとき補正磁界2G、28が形成され
て、渦電流磁界が打消され、ミスコンバーゼンス15,
16が共に補正された画像が1!lられる。
11!1.14' is always canceled, but the eddy current magnetic field only needs to be struck when the electron beam 1 (, B) is within this magnetic field. Therefore, the above DC Instead of the current, a part of the vertical deflection current may be made to flow through the column. In this case, the electron beam 1 (, B
is deflected vertically, correction magnetic fields 2G, 28 are formed, canceling the eddy current magnetic field, and causing misconvergence 15, 28.
The image with 16 corrected together is 1! I will be beaten.

また、上記の永久磁石22.23又はコイルは偏向ヨー
ク本体の代わりにカラー受像管2に取付りられCbよく
、上記ど同様に作用するのは勿論−Cある。
Further, the above-mentioned permanent magnets 22, 23 or coils may be attached to the color picture tube 2 instead of the deflection yoke body, and of course -C may function in the same manner as above.

効果 上述の如く、本発明になる偏向ヨークにJ:れば、スラ
ー受像管内の金属部が原因で発生ずる渦電流磁シνをi
ri接的に打消Jことが出来るため、渦電流磁界に起因
りるミスコンバーゼンスを、補正の所謂副作用としての
コンバーゼンスずれを発生さUることなく、補11Jる
ことが出来、しかも、高価である動的な」ンバーゼンス
補正装置を使用1−ることイjく、例えば永久磁石を利
用した簡単にに構成ど′す゛ることも出来、然して、上
記のミスコンバーゼンスを良好にしかも容易に且つ安価
に補正りることが出来るという特長をイ4する。
Effects As mentioned above, the deflection yoke according to the present invention reduces the eddy current magnetic field ν caused by the metal parts in the slurry picture tube.
Since it is possible to tangentially cancel the misconvergence caused by the eddy current magnetic field, it is possible to compensate for the misconvergence caused by the eddy current magnetic field without causing a convergence shift as a so-called side effect of the correction, and it is also expensive. The use of a dynamic "convergence correction device", which can be easily constructed using, for example, a permanent magnet, allows the above-mentioned misconvergence to be corrected well, easily and at low cost. 4.

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

第1図は一般的なインライン型カラー受像装置を概略的
に示す図、第2図はカラー受像管内の磁界の状況を示す
第1図中■−■線に沿う拡大矢視図、第3図は水平偏向
電流の波形図、第4図は電子ビームR,Bが渦電流磁界
ににり偏向される状況を示J図、第5図は第4図のla
f向ににり生じたミスコンバーゼンスパターンを示づ図
、第6図は第5図のミスコンバーゼンスを補正したどき
にその副作用どして生じたミスコンバーゼンスパターン
を示す図、第7図は本発明になる偏向」−りの一実施例
の斜視図、第8図はこの偏向ヨークを紺+J tノでな
るカラー受像装置を概略的に示1図、第9図は第7図の
偏向ヨークによるミスコンバーゼンスの補正動作を説明
づる図である。。 2・・・カラー受像管、5a、5b・・・垂直偏向コイ
ル、6a、6b・・・水平偏向コイル、7・・・水平偏
向磁界、8・・・電子銃の一部、9・・・ゲッタ、1o
・・・ゲッタ支持機、11a、llb、12a、12b
。 11a’ 、11b’ 、12a’ 、12b’ ・6
11束、 ′13.13’ 、14.14’・・・渦電
流磁界、15゜16・・・ミスコンバーゼンス、2o・
・・偏向ヨーク、21・・・カラー受像装置、22.2
3・・・永久磁石、24・・・リング部祠、24a 、
2411・・・保持部、25a 、25b 、27a 
、27b−・・磁束、2628 ・・・ ン山 正 磁
 シν 。 特晶′1出願人 口木ビクター株式会社代 理 人 弁
理士 伊 東 忠 彦 第1図 815≧61ンJ 第7図 つ 手続補正書 昭和60年4月211 (特許庁審査官 殿) 1、事件の表示 118和59 年 特 許 願第 4512[] 9号
2発明の名称 偏 向 ヨ − り 3、補正をする者 特 許 出願人 住 所 ・221 、M+奈川用、1.横浜市神奈用区
守屋町3丁g12i地名称 (432) 日本ビクター
株式会社代表名 取?a役社長 宍 道 −部 4、代理人 自発補正 6、7山 正 の 対 奮! 明flll六の発明の訂:#11な説明の欄。 7、 補正の内容 (1)明細711中、第2頁第17行及び第3頁第7行
記載の1−変更」を「偏向」ど補正覆る。 (2)同、第6頁第7行記載の「生産性上採用ザること
番よ困テ11である。」を[生産性を阻害づる要因とな
る。」ど補止りる。 (311同、第11頁第8行記載の「スラー」を1′カ
ラー」と補11−りる。
Figure 1 is a diagram schematically showing a general in-line color picture receiver, Figure 2 is an enlarged view along the line ■-■ in Figure 1, showing the state of the magnetic field inside the color picture tube, and Figure 3. is a waveform diagram of the horizontal deflection current, Figure 4 shows the situation where electron beams R and B are deflected by the eddy current magnetic field, and Figure 5 is the la of Figure 4.
A diagram showing a misconvergence pattern that occurred in the f direction, FIG. 6 is a diagram showing a misconvergence pattern that occurred as a side effect when the misconvergence in FIG. 5 was corrected, and FIG. FIG. 8 is a perspective view of an embodiment of the deflection yoke shown in FIG. FIG. 3 is a diagram illustrating a misconvergence correction operation. . 2... Color picture tube, 5a, 5b... Vertical deflection coil, 6a, 6b... Horizontal deflection coil, 7... Horizontal deflection magnetic field, 8... Part of electron gun, 9... Getta, 1o
...Getter support machine, 11a, llb, 12a, 12b
. 11a', 11b', 12a', 12b' ・6
11 flux, '13.13', 14.14'... Eddy current magnetic field, 15°16... Misconvergence, 2o.
...Deflection yoke, 21...Color image receiving device, 22.2
3... Permanent magnet, 24... Ring part shrine, 24a,
2411... Holding section, 25a, 25b, 27a
, 27b-...magnetic flux, 2628...Nyama positive magnetic siν. Special Crystal '1 Applicant Kuchiki Victor Co., Ltd. Agent Patent Attorney Tadahiko Ito Figure 1 815≧61nJ Figure 7 Procedural Amendment April 1985 211 (To the Patent Office Examiner) 1. Indication of case 118 Wa 59 Patent Application No. 4512 [] No. 9 2 Name deviation of invention 3, Amendment person patent Applicant address ・221, M+For Nagawa, 1. 3-g12i Moriyamachi, Kanayō-ku, Yokohama City Place name (432) Victor Company of Japan Co., Ltd. Representative name Tori? A role president Shimichi - Department 4, agent voluntary compensation 6, 7 Yama Tadashi's efforts! Revised invention of Akira Roku: #11 Explanation column. 7. Contents of the amendment (1) In Specification 711, 1-Change described in page 2, line 17 and page 3, line 7 is overturned as ``deflection.'' (2) In the same article, page 6, line 7 states, ``It is difficult to hire employees in terms of productivity.'' [This is a factor that impedes productivity.] ” Do make up for it. (311 Ibid., page 11, line 8, ``slur'' is supplemented with ``1'color.'')

Claims (1)

【特許請求の範囲】 1、 インク・イン配貨の3木の電子銃を有するカラー
受像管にII伺りられて使用される偏向ヨークにおいて
、該カラー受像管に組付けられた状態′caカラー受像
管内の金属部に対向Jる位置に、−向磁稈により該金属
部に誘起される渦電流により生ずる渦電流磁界を打ちt
l!lずような磁界を発生させる磁界発生手段を備えて
なることを特徴とりる編向ヨーク。 2、 該磁界発生手段は、磁極を該金属部に向1ノて配
された永久磁石片であることを特徴とするtk Fil
’ 請求の範囲第1項記載の偏向ヨーク。 3、 該磁界発生手段は、その巻軸線を該金属部に向1
ノで配され、直流電流或いは垂直偏向電流を供給される
コイルであることを特徴とする特11晶求の範囲第1項
記載の偏向ヨーク。
[Scope of Claims] 1. In a deflection yoke used in a color picture tube having three electron guns with ink-in delivery, the 'ca color when assembled to the color picture tube An eddy current magnetic field generated by an eddy current induced in the metal part by a magnetic culm is applied to a position opposite to the metal part in the picture tube.
l! 1. A knitting yoke characterized by comprising magnetic field generating means for generating a magnetic field of a certain magnitude. 2. The magnetic field generating means is a permanent magnet piece with magnetic poles facing the metal part.
' The deflection yoke according to claim 1. 3. The magnetic field generating means directs its winding axis toward the metal part.
The deflection yoke according to item 1 of item 11, characterized in that the deflection yoke is a coil arranged in the form of a coil and supplied with a direct current or a vertical deflection current.
JP4512084A 1984-03-09 1984-03-09 Deflection york Pending JPS60189845A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4512084A JPS60189845A (en) 1984-03-09 1984-03-09 Deflection york

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4512084A JPS60189845A (en) 1984-03-09 1984-03-09 Deflection york

Publications (1)

Publication Number Publication Date
JPS60189845A true JPS60189845A (en) 1985-09-27

Family

ID=12710408

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4512084A Pending JPS60189845A (en) 1984-03-09 1984-03-09 Deflection york

Country Status (1)

Country Link
JP (1) JPS60189845A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63271851A (en) * 1987-04-30 1988-11-09 Hitachi Ltd Deflection yoke
EP0322845A2 (en) * 1987-12-26 1989-07-05 Kabushiki Kaisha Toshiba Improved deflection device for a color picture tube apparatus
US4943753A (en) * 1987-08-13 1990-07-24 International Business Machines Corporation Magnetic shunt for deflection yokes
CN105373097A (en) * 2015-11-24 2016-03-02 中冶南方工程技术有限公司 Non-contact type traveling wave magnetic field eddy current deviation-correcting device and method of metal strip continuous production line

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5530658A (en) * 1978-08-28 1980-03-04 Fujirebio Inc Sensitized latex for inspecting adeno virus desease and production thereof

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5530658A (en) * 1978-08-28 1980-03-04 Fujirebio Inc Sensitized latex for inspecting adeno virus desease and production thereof

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63271851A (en) * 1987-04-30 1988-11-09 Hitachi Ltd Deflection yoke
US4943753A (en) * 1987-08-13 1990-07-24 International Business Machines Corporation Magnetic shunt for deflection yokes
EP0322845A2 (en) * 1987-12-26 1989-07-05 Kabushiki Kaisha Toshiba Improved deflection device for a color picture tube apparatus
US4975618A (en) * 1987-12-26 1990-12-04 Kabushiki Kaisha Toshiba Deflection device for a color picture tube apparatus
CN105373097A (en) * 2015-11-24 2016-03-02 中冶南方工程技术有限公司 Non-contact type traveling wave magnetic field eddy current deviation-correcting device and method of metal strip continuous production line
CN105373097B (en) * 2015-11-24 2018-03-27 中冶南方工程技术有限公司 The contactless travelling-magnetic-field vortex correcting device and method of a kind of sheet metal strip tinuous production

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