JPH01154441A - Deflection yoke device - Google Patents
Deflection yoke deviceInfo
- Publication number
- JPH01154441A JPH01154441A JP31211987A JP31211987A JPH01154441A JP H01154441 A JPH01154441 A JP H01154441A JP 31211987 A JP31211987 A JP 31211987A JP 31211987 A JP31211987 A JP 31211987A JP H01154441 A JPH01154441 A JP H01154441A
- Authority
- JP
- Japan
- Prior art keywords
- deflection yoke
- coils
- horizontal
- magnetic flux
- increase
- 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
- 230000002093 peripheral effect Effects 0.000 claims description 3
- 238000004804 winding Methods 0.000 abstract description 2
- 230000004907 flux Effects 0.000 description 33
- 230000005855 radiation Effects 0.000 description 6
- 230000000694 effects Effects 0.000 description 3
- 241000252233 Cyprinus carpio Species 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 238000010894 electron beam technology Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 238000000691 measurement method Methods 0.000 description 2
- 230000007246 mechanism Effects 0.000 description 2
- 230000035699 permeability Effects 0.000 description 2
- 230000001105 regulatory effect Effects 0.000 description 2
- 239000007787 solid Substances 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は陰極線管(以下CRTという)において高エ
ネルギーの電子ビームを用いる場合に、この電子ビーム
を電磁的に偏向させる偏向ヨーク装置の改良に関するも
のである。[Detailed Description of the Invention] [Industrial Application Field] This invention relates to an improvement in a deflection yoke device for electromagnetically deflecting a high-energy electron beam in a cathode ray tube (hereinafter referred to as CRT). It is something.
第4図は例えばrNHKカラーテレビ受信技術」P19
4 (日本放送協会昭和62年4月10日発行)に示さ
れた従来の偏向ヨーク装置を示す側面図であり、図にお
いて、1はCRT、2はCRTlの細径部1a(電子銃
近傍)部分に取り付けられる略円筒形の環状コア(トロ
イダルコア)、3゜4は上記環状コア2の内周面に沿っ
て略水平方向に対向して配置された水平コイル、5.6
は上記環状コア2の周囲に巻回されて上記水平コイル3
゜4の磁束と直交する方向の磁束を生じさせる垂直コイ
ルで、これら水平コイル3,4と垂直コイル5.6とに
より偏向ヨーク7を構成する。なお、第5図においては
60Hz付近の周波数で駆動される垂直コイル5.6は
西独の電磁波不要輻射規制規格VDEO871の磁束領
域(Magnetic fi−eld No1se)で
規制する範囲が10KHzからであり、その高調波もレ
ベルが限度に及ばないので、説明を簡単にするために省
略する。Figure 4 shows, for example, "rNHK color television reception technology" P19
4 (published by Japan Broadcasting Corporation on April 10, 1986). In the figure, 1 is a CRT, and 2 is a narrow diameter portion 1a of the CRTl (near the electron gun). A substantially cylindrical annular core (toroidal core) attached to the section, 3.4 horizontal coils disposed facing each other in a substantially horizontal direction along the inner peripheral surface of the annular core 2, 5.6
is wound around the annular core 2 to form the horizontal coil 3.
The horizontal coils 3 and 4 and the vertical coils 5 and 6 constitute a deflection yoke 7, which is a vertical coil that generates a magnetic flux in a direction perpendicular to the magnetic flux of 4°. In addition, in Fig. 5, the vertical coil 5.6 driven at a frequency around 60 Hz is regulated in the magnetic flux range (Magnetic field No. 1se) of the West German electromagnetic wave unnecessary radiation control standard VDEO871 from 10 kHz, and the range is regulated from 10 kHz. Since the level of harmonics does not reach the limit, they will be omitted to simplify the explanation.
次に動作について説明する。Next, the operation will be explained.
原理的には水平コイル3,4は水平磁束を発生し、垂直
コイル5,6は垂直磁束を発生する。このため、この2
方向の磁束を有する磁界が環状コア2を中心に形成され
る。また、上記水平磁束と垂直(1束とは水平コイル3
.4および垂直コイル5.6に流れる電流量により磁界
の強さが変化する。そして、この磁界により上記環状コ
ア2の中央部分を挿通したCRTIの細径部la内を通
過する電子ビームが偏向されてCRTlに画像を形成す
ることになる。すなわち、第5図において、偏向ヨーク
7の水平コイル3,4に符号8,9で示すような電流が
流れると、実線矢印で示すような水平磁束■]が発生し
、符号10で示すように偏向する。In principle, the horizontal coils 3 and 4 generate horizontal magnetic flux, and the vertical coils 5 and 6 generate vertical magnetic flux. For this reason, these two
A magnetic field having directional magnetic flux is formed around the annular core 2. In addition, the above horizontal magnetic flux and perpendicular (one flux is the horizontal coil 3
.. The strength of the magnetic field changes depending on the amount of current flowing through the vertical coils 4 and 5.6. Then, due to this magnetic field, the electron beam passing through the narrow diameter portion la of the CRTI inserted through the central portion of the annular core 2 is deflected to form an image on the CRTl. That is, in FIG. 5, when currents as shown by symbols 8 and 9 flow through the horizontal coils 3 and 4 of the deflection yoke 7, a horizontal magnetic flux shown by the solid arrow is generated, and as shown by the symbol 10. deflect.
ところで、水平コイル3.4の前端3a、4aおよび後
端3b、4bの符号8.9で示す電流方向が変化する場
所ではそれぞれ磁束11.12゜13.14が発生する
と共に、これらの磁界発生メカニズムにより偏向には特
に寄与しない不要輻射磁束15.16が発生する。この
不要輻射磁束15.16のレベルは偏向ヨーク7の前部
側が大きく開口しているためと、磁束11.12の線路
HM(1X束13.14に較べ長いためとで不要輻射磁
束15が大きくなっている。この従来の偏向ヨ一り装置
を内蔵したデイスプレィモニタDMまたはテレビを西独
の不要輻射規制規格VDEO877の測定方法で測定し
たときの磁束を第6図に示すと、偏向ヨーク7の前側磁
束17,18.19は地面の透磁率が大気中より大きい
ため地面でループしている。By the way, magnetic fluxes of 11.12° and 13.14 are generated at the front ends 3a, 4a and the rear ends 3b, 4b of the horizontal coil 3.4 at the locations indicated by reference numeral 8.9 where the current direction changes, and these magnetic fields are The mechanism generates unnecessary radiated magnetic flux 15,16 that does not particularly contribute to deflection. The level of this unnecessary radiated magnetic flux 15.16 is due to the large opening on the front side of the deflection yoke 7 and the fact that the line HM of magnetic flux 11.12 is longer than the 1X flux 13.14. Figure 6 shows the magnetic flux when measuring a display monitor DM or television equipped with this conventional deflection/yielding device using the measurement method of the West German unnecessary radiation control standard VDEO877. The front magnetic fluxes 17, 18, and 19 are looped on the ground because the magnetic permeability of the ground is greater than that of the atmosphere.
従来の偏向ヨーク装置は以上のように構成されているの
で、偏向ヨーク7から発生する不要輻射磁束15の影響
を与えないようにするために鉄板やパーマロイなどの透
磁率の高い材料で磁路をショートループさせなければな
らず、電子回路を含めCRTIや偏向ヨーク7を鉄板で
囲んだりするため、内部電子回路の温度上昇による寿命
低下や重量増を招いたりしてサービスの悪化を招くする
という問題点があった。Since the conventional deflection yoke device is configured as described above, the magnetic path is made of a material with high magnetic permeability such as an iron plate or permalloy in order to prevent the influence of the unnecessary radiated magnetic flux 15 generated from the deflection yoke 7. Since the CRTI and deflection yoke 7, including the electronic circuits, must be short-circuited and surrounded by a steel plate, the temperature of the internal electronic circuits increases, resulting in reduced service life and increased weight, resulting in deterioration of service. There was a point.
この発明は上記のような問題点を解消するためになされ
たもので、内部電子回路の温度上昇による寿命の低下や
重量増を招かないようにした偏向ヨーク装置を得るこき
を目的とする。The present invention was made to solve the above-mentioned problems, and aims to provide a deflection yoke device that does not cause a decrease in life or an increase in weight due to temperature rise of internal electronic circuits.
この発明に係る偏向ヨーク装置は陰極線管の細径部分に
取り付けられる略円筒形の環状コアと、この環状コアの
内周面に沿って設けられる水平コイルと、上記環状コア
に巻回される垂直コイルと、上記環状コアの周囲方向に
巻回されたキャンセルコイルとを備えたものである。The deflection yoke device according to the present invention includes a substantially cylindrical annular core attached to a narrow diameter portion of a cathode ray tube, a horizontal coil provided along the inner peripheral surface of this annular core, and a vertical coil wound around the annular core. It includes a coil and a canceling coil wound around the annular core.
この発明における傾向ヨーク装置は環状コアの周囲方向
に巻回されたキャンセルコイルに水平偏向電流を流すこ
とで偏向ヨークの前側から発生する磁界をキャンセルま
たは減少させるようにしたものである。The tendency yoke device according to the present invention cancels or reduces the magnetic field generated from the front side of the deflection yoke by passing a horizontal deflection current through a cancellation coil wound in the circumferential direction of an annular core.
以下、この発明の一実施例を図について説明する。第1
図はこの発明の一実施例を示す断面図であって、第1図
において第4図と同一または均等部分には同一符号を付
して重複説明を省略する。An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure is a sectional view showing one embodiment of the present invention, and the same or equivalent parts in FIG. 1 as in FIG. 4 are given the same reference numerals, and redundant explanation will be omitted.
第1図において、21.22は環状コア2の周囲方向に
沿って巻回されるキャンセルコイルで、このキャンセル
コイル21.22は偏向ヨーク7の上側水平コイル3の
前側から発生する不要輻射磁束16の大きさを小さくす
るためのものである。In FIG. 1, reference numerals 21 and 22 denote canceling coils wound along the circumferential direction of the annular core 2, and the canceling coils 21 and 22 are the unnecessary radiated magnetic flux 16 generated from the front side of the upper horizontal coil 3 of the deflection yoke 7. This is to reduce the size of.
また、キャンセルコイル21.22には水平コイル3.
4に流す水平偏向電流と同じか相似波形で、周波数がn
倍(nは1〜5程度)の電流を流す。Further, the canceling coils 21 and 22 include horizontal coils 3.
The waveform is the same or similar to the horizontal deflection current flowing through 4, and the frequency is n.
A current twice as large (n is about 1 to 5) is applied.
次に動作について説明する。Next, the operation will be explained.
第2図において、偏向ヨーク7の水平コイル3゜4に符
号8.9で示すような電流を流すと、実線矢印で示すよ
うな水平磁束I]が発生する。また、キャンセルコイル
21.22に水平偏向電流を流した場合、磁束23.2
4が発生する。よって、水平コイル3,4の前端3a、
4aおよび後端3b、4bの符号8.9で示す電流方向
が変化する場所に発生するそれぞれの磁束25,26.
27゜28はキャンセルコイル21.22の磁束23゜
24の影響を受けて、磁束25より磁束26の方が、ま
た磁束28より磁束27の方が強く発生し、これらの磁
界発生メカニズムにより偏向には特に寄与しない不要輻
射磁束15.16は第2図に示すように弯曲する。In FIG. 2, when a current as indicated by reference numeral 8.9 is passed through the horizontal coil 3.4 of the deflection yoke 7, a horizontal magnetic flux I as indicated by the solid arrow is generated. In addition, when a horizontal deflection current is passed through the canceling coil 21.22, the magnetic flux 23.2
4 occurs. Therefore, the front ends 3a of the horizontal coils 3, 4,
4a and rear ends 3b, 4b, respectively, magnetic fluxes 25, 26, ., generated at locations where the current direction changes, indicated by reference numeral 8.9.
27 and 28 are influenced by the magnetic fluxes 23 and 24 of the canceling coils 21 and 22, and the magnetic flux 26 is generated stronger than the magnetic flux 25, and the magnetic flux 27 is stronger than the magnetic flux 28, and these magnetic field generation mechanisms affect the deflection. The unnecessary radiated magnetic flux 15,16 which does not particularly contribute is curved as shown in FIG.
この偏向ヨーク装置を内蔵したデイスプレィモニタDM
またはテレビジョンを西独の不要輻射規制規格VDEO
877の測定方法で測定したときの磁界を第3図に示す
と、偏向ヨーク7の前側磁束17,18.19は強く地
面側に弯曲し、不要輻射測定用ループアンテナEMIで
は検出されなくなる。また、偏向ヨーク7の後側磁束は
空中側に弯曲するもののもともと小さな磁束であるため
に妨害源とはならない。Display monitor DM with built-in deflection yoke device
Or use the West German unnecessary radiation control standard VDEO for televisions.
FIG. 3 shows the magnetic field measured by the No. 877 measurement method. The front magnetic fluxes 17, 18, and 19 of the deflection yoke 7 are strongly curved toward the ground, and are no longer detected by the loop antenna EMI for measuring unnecessary radiation. Further, although the rear magnetic flux of the deflection yoke 7 curves toward the air, it is originally a small magnetic flux and does not become a source of interference.
なお、上記実施例ではキャンセルコイル21゜22に水
平偏向電流を流すように説明したが、水平偏向電流のn
倍の周波数の相似波形電流を流した場合はn倍の不要輻
射成分を強く打ち消すことができる。In the above embodiment, the horizontal deflection current is passed through the canceling coils 21 and 22, but the horizontal deflection current n
When a similar waveform current with twice the frequency is passed, it is possible to strongly cancel n times the unnecessary radiation component.
以上のようにこの発明によれば偏向ヨーク装置を環状コ
アの周囲方向にキャンセルコイルを巻回させて構成した
ので、水平コイルの前側不要輻射磁束を対地側に弯曲さ
せることができ、特に磁気シールドさせる材料を用いる
ことなく。不要輻射対策が行え、内部電子回路の温度上
昇に伴う寿命の低下や重量増を招かないようにした安価
な装置が得られる効果がある。As described above, according to the present invention, since the deflection yoke device is constructed by winding the canceling coil around the annular core, the unnecessary radiated magnetic flux on the front side of the horizontal coil can be curved toward the ground side, and in particular, the magnetic shield without using materials that cause This has the effect of providing an inexpensive device that can take measures against unnecessary radiation and that does not cause a decrease in life or an increase in weight due to temperature rises in internal electronic circuits.
第1図はこの発明の一実施例による偏向ヨーク装置を示
す断面図、第2図は第1図の動作を説明するための偏向
ヨーク装置の概念図、第3図はこの発明の偏向ヨーク装
置を用いて不要輻射磁束を測定した場合の磁束分布を示
す側面図、第4図は従来の偏向ヨーク装置の一例を示す
一部切欠側面図、第5図は第4図の動作を説明するため
の傾向ヨーク装置の概念図、第6図は従来の偏向ヨーク
装置を用いて不要輻射磁束を測定した場合の磁束分布を
示す側面図である。
■は陰極線管(CRT) 、2は環状コア、3゜4は水
平コイル、5,6は垂直コイル、21.22はキャンセ
ルコイル。
なお、図中同一符号は同一または相当部分を示す。
弛 1 は
2:環状コア
3.4 : 7に平コイ)し
21.22:キャンt)レコ/1)し
第 22
第3図
5,6:垂直コイ1し
第5図
第6図FIG. 1 is a sectional view showing a deflection yoke device according to an embodiment of the present invention, FIG. 2 is a conceptual diagram of the deflection yoke device for explaining the operation of FIG. 1, and FIG. 3 is a deflection yoke device of the present invention. Fig. 4 is a partially cutaway side view showing an example of a conventional deflection yoke device, and Fig. 5 is for explaining the operation of Fig. 4. FIG. 6 is a side view showing the magnetic flux distribution when unnecessary radiated magnetic flux is measured using a conventional deflection yoke device. ■ is a cathode ray tube (CRT), 2 is an annular core, 3°4 is a horizontal coil, 5 and 6 are vertical coils, and 21.22 is a canceling coil. Note that the same reference numerals in the figures indicate the same or corresponding parts. Relaxation 1 is 2: Annular core 3.4: Flat carp to 7) and 21.22: Can t) Rec/1) and 22 3 Figures 5 and 6: Vertical carp 1 and 5 Figure 6
Claims (1)
コアと、この環状コアの内周面に沿って設けられる水平
コイルと、上記環状コアに巻回される垂直コイルとを備
えた偏向ヨーク装置において、上記環状コアの周囲方向
にキャンセルコイルを巻回したことを特徴とする偏向ヨ
ーク装置。A deflection yoke device comprising a substantially cylindrical annular core attached to a narrow diameter portion of a cathode ray tube, a horizontal coil provided along the inner peripheral surface of the annular core, and a vertical coil wound around the annular core. A deflection yoke device characterized in that a canceling coil is wound around the annular core.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31211987A JPH01154441A (en) | 1987-12-11 | 1987-12-11 | Deflection yoke device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31211987A JPH01154441A (en) | 1987-12-11 | 1987-12-11 | Deflection yoke device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01154441A true JPH01154441A (en) | 1989-06-16 |
Family
ID=18025473
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP31211987A Pending JPH01154441A (en) | 1987-12-11 | 1987-12-11 | Deflection yoke device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01154441A (en) |
-
1987
- 1987-12-11 JP JP31211987A patent/JPH01154441A/en active Pending
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