TW200409167A - Deflection yoke for cathode ray tube - Google Patents

Deflection yoke for cathode ray tube Download PDF

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Publication number
TW200409167A
TW200409167A TW092116028A TW92116028A TW200409167A TW 200409167 A TW200409167 A TW 200409167A TW 092116028 A TW092116028 A TW 092116028A TW 92116028 A TW92116028 A TW 92116028A TW 200409167 A TW200409167 A TW 200409167A
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TW
Taiwan
Prior art keywords
deflection
core
thickness
yoke
iron core
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Application number
TW092116028A
Other languages
Chinese (zh)
Inventor
Hyung-Dal Joo
Woo-Young Yang
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Lg Philips Displays Korea
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Application filed by Lg Philips Displays Korea filed Critical Lg Philips Displays Korea
Publication of TW200409167A publication Critical patent/TW200409167A/en

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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21LLIGHTING DEVICES OR SYSTEMS THEREOF, BEING PORTABLE OR SPECIALLY ADAPTED FOR TRANSPORTATION
    • F21L4/00Electric lighting devices with self-contained electric batteries or cells
    • F21L4/005Electric lighting devices with self-contained electric batteries or cells the device being a pocket lamp
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21LLIGHTING DEVICES OR SYSTEMS THEREOF, BEING PORTABLE OR SPECIALLY ADAPTED FOR TRANSPORTATION
    • F21L4/00Electric lighting devices with self-contained electric batteries or cells
    • F21L4/08Electric lighting devices with self-contained electric batteries or cells characterised by means for in situ recharging of the batteries or cells
    • F21L4/085Pocket lamps
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21SNON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
    • F21S9/00Lighting devices with a built-in power supply; Systems employing lighting devices with a built-in power supply
    • F21S9/02Lighting devices with a built-in power supply; Systems employing lighting devices with a built-in power supply the power supply being a battery or accumulator
    • F21S9/022Emergency lighting devices
    • F21S9/024Emergency lighting devices using a supplementary light source for emergency lighting
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V17/00Fastening of component parts of lighting devices, e.g. shades, globes, refractors, reflectors, filters, screens, grids or protective cages
    • F21V17/10Fastening of component parts of lighting devices, e.g. shades, globes, refractors, reflectors, filters, screens, grids or protective cages characterised by specific fastening means or way of fastening
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V33/00Structural combinations of lighting devices with other articles, not otherwise provided for
    • F21V33/0064Health, life-saving or fire-fighting equipment
    • F21V33/0076Safety or security signalisation, e.g. smoke or burglar alarms, earthquake detectors; Self-defence devices
    • GPHYSICS
    • G08SIGNALLING
    • G08BSIGNALLING OR CALLING SYSTEMS; ORDER TELEGRAPHS; ALARM SYSTEMS
    • G08B13/00Burglar, theft or intruder alarms
    • G08B13/02Mechanical actuation
    • G08B13/14Mechanical actuation by lifting or attempted removal of hand-portable articles

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  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Computer Security & Cryptography (AREA)
  • Environmental & Geological Engineering (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Video Image Reproduction Devices For Color Tv Systems (AREA)

Abstract

A deflection yoke for a cathode ray tube, with reduced weight and volume plus a low cost of manufacture is obtained by making a ferrite core housed in the deflection yoke very light and thin, based on an optimized design obtained through a number of experimental trials.

Description

200409167 五、發明說明(1) 【發明所屬之技術領域】 有關 [001]本發明有關一種陰極射線 一種以多次實驗試驗獲得的最佳t轉磁輕,尤其 射線管偏轉磁軛,由於1中六 ° °十為基礎的陰極 轉磁軛的重量與體積較;且:極輕而,,因此偏 【先前技術】 且^成本較低。 my圖1解說—先前技術彩色陰極射線管之姓M [003]此彩色陰極射線之、,“冓。 真空管之正面上,並右一干工A 赏先屏’位於一錐形 屏另側之頸部上,藉此::=一偏轉磁軛,位於螢光 撞擊在螢光屏上以‘示一。#發射的電子束被偏轉與 [0 0 4 ]如圖1所示,彩辛 彼此緊密封合為一 -,:ί :面板1與漏斗2係 空狀態。 —所以陰極射線官11之内部通常為真 斗内[Γ,5]Λ有榮光物質(或碟光劑)之螢光屏12係置於漏 之相反側^杨1 3係容置在漏斗之頸部内,位於螢光屏i 2 * 0 6 ]赏光屏12與電子搶13之間一預定空間内,更明 ;i 4較靠近螢光屏1 2之位置,設一選擇色彩用的陰 2n 0同日才’漏斗頸部内設一偏轉磁軛1 5,用以偏轉從電< 子杨1 3發射之電子束。 秩作 ]以下解說具有上述結構之彩色陰極射線管如何 ^ i電子搶13發射的電子束16被偏轉磁軛15朝水平與垂 方向偏轉’被水平/垂直偏轉後的電子束16通過蔭罩14 200409167 五、發明說明(2) 上的電子束通孔而終於打擊在前 示所要的圖像。 ㈣的螢先屏12上’藉此顯 丨〇〇8]圖2較詳盡地說明偏轉磁軛之結構。 偏轉線圖2 ’先前技術之偏轉磁扼15包括一水平 束朝2偏轉線圈22 ’可將電子搶發射的電子 轉線圈產= 芯24,可使水平及垂直偏 低;-支座23,可回路徑中的損失減至最 確侔 支撐水平及垂直偏轉線圈21、22之,並 ^ 25b 121 ^22 Γθ1 ^ ^ ^ ; ^ ^ ®25a 以、、肖广僬鐘刀 ;支座23近f光屏側之頂端與底端,用 -ί ΐ螢光屏及頸部内產生的磁場漏沒;* 4 ΐϊ子束ΐ:ΐί水平偏轉線圈21與連接線之端子及 用遠i Lt L 預定位置之補償電路協助下,利 21連接、.泉26a、26b連接消除線圈25a、⑽與水平偏轉線圈 [〇〇1〇]通常,偏轉磁軛15允許頻率為1 5 75khz或 電流流至水平偏轉線圈21,並利用該線圈周圍產= 勺“,冑陰極射線管内部的電子束16朝水平方向偏轉。 0011 ]同時,偏轉磁軛15允許頻率為6〇Hz之電 =偏轉線圈22 ’並利用該線圈周圍 射線管内部的電子束朝垂直方向偏轉。 將陰桎 [0012]因此,當偏轉磁軛15將電子束16朝水平及 :向偏#’並將它們會聚在螢光屏上的 即可顯示一圖像。 策尤杵上 第7頁 200409167 五、發明說明(3) [0 0 1 3 ]近來發展的偏轉磁概之一,為一種自會聚型偏 轉磁軛,它利用水平與垂直偏轉線圈2丨、2 2周圍的非均 磁場,以使紅(R)、綠(G)、藍(B)三色電子束16會聚在 光屏上,而不使用另外的個別電路或裝置。 [0 0 1 4 ]換έ之,藉由調整水平與垂直偏轉線圈2丨、 的轉向分佈,自會聚型偏轉磁軛在每一區段(亦即, 部、中間部及頸部)產生一鼓形或枕形磁場;同時,儘管 二,電子束16的母-電子束其起始與結束位置各 但自會聚型㈣磁輛仍允許每一色電子束&其位置而 不同的偏轉力(但是從不同距離會聚在一點上)。 、馭 [0015]此4 ’偏轉磁軛之螢光屏部係指 =相對較大直徑截面之部份,頸部則指示榮光屏ί; 側具有相對較小直徑截面之部份。 赏尤幵丨另 [0 0 1 6 ]中間部,如其名摇夕 立 乂 頸部的中間部位。 3思,係指示螢光屏部與 [0017]以上定義亦分別適 支座、及锶#夕、狄氺尸划 用於偏轉磁概、偏轉線圈、 ϋ端鐵…先屏#、頸部、榮光屏側-端、及頭部 [〇 0 1 8 ]同時,陰極射線管制1 是,如果只利用水平及垂直偏二=的典型問題之-及垂直偏轉線圈21、22周圍產4勺電μ >;IL入線圈而在水平 子束16偏轉到整個螢光屏上。的磁場時,其實很難將電 係數的鐵芯2 4來最小化水平及此,通常使用具有南導礤 磁場於其返回路徑上的損失,直偏轉線圈21、22產生的 、 亚進而改善磁效率與磁力。200409167 V. Description of the invention (1) [Technical field to which the invention belongs] Related [001] The present invention relates to a cathode ray and an optimal t-rotation light weight obtained by multiple experimental tests, especially a ray tube deflection yoke, since 1 in The weight and volume of the cathode-to-magnet yoke based on six degrees and ten degrees are relatively light; therefore, it is extremely light, so it is [prior art] and has lower cost. my Figure 1 Explanation—The surname M of the prior art color cathode ray tube [003] This color cathode ray tube, "冓. On the front side of the vacuum tube, and a right hand A A screen is located on the neck of the other side of a tapered screen In this way: == a deflection yoke, which is located on the fluorescent screen and hits the fluorescent screen as' showing one. # The electron beam emitted is deflected and [0 0 4] as shown in Figure 1, Cai Xin is close to each other Sealed as one- ,: ί: Panel 1 and funnel 2 are in an empty state. —So the inside of cathode ray officer 11 is usually a fluorescent screen in the real bucket [Γ, 5] Λ with a glorious substance (or dishing agent). The 12 series is placed on the opposite side of the drain ^ Yang 1 The 3 series is housed in the neck of the funnel, located on the fluorescent screen i 2 * 0 6] in a predetermined space between the light screen 12 and the electronic grab 13, i. 4 Closer to the fluorescent screen 12, a yin 2n 0 for color selection is set on the same day. A deflection yoke 15 is set in the neck of the funnel to deflect the electron beam emitted from electricity < Ziyang 1 3 Rank work] The following explains how a color cathode ray tube having the above structure ^ i The electron beam 16 emitted by the electron grab 13 is deflected by the yoke 15 in the horizontal and vertical directions. / The vertically deflected electron beam 16 passes through the shadow mask 14 200409167 V. The electron beam through hole in the description of the invention (2) finally strikes the desired image shown in the front. 〇8] Figure 2 illustrates the structure of the deflection yoke in more detail. Deflection diagram Figure 2 'The deflection yoke 15 of the prior art includes a horizontal beam towards 2 deflection coils 22' An electronic coil coil capable of robbing electrons for emission = core 24 , Can make the horizontal and vertical low;-support 23, the loss in the return path can be reduced to the most accurate support horizontal and vertical deflection coils 21, 22, and ^ 25b 121 ^ 22 Γθ1 ^ ^ ^ ^ ^ ® 25a Yi, Xiao Guangqi Bell Knife; the top and bottom of the support 23 near the f-light screen side, the magnetic field generated in the fluorescent screen and the neck is leaked; * 4 ΐϊ 子 束 ΐ: ΐίHorizontal deflection coil 21 With the help of the terminal of the connection line and the compensation circuit at a predetermined position with far i Lt L, the 21 connection, the spring 26a, 26b connection eliminates the coil 25a, ⑽ and the horizontal deflection coil [〇〇1〇] Usually, the deflection yoke 15 allows a frequency of 1 5 75khz or current to flow to the horizontal deflection coil 21, and uses the output around this coil = "Electron beam cathode ray tube 16 inside of the helmet in the horizontal direction deflection. [0011] Meanwhile, the deflection yoke 15 allows electricity having a frequency of 60 Hz = the deflection coil 22 'and uses the electron beam inside the ray tube around the coil to deflect in a vertical direction. [0012] Therefore, when the deflection yoke 15 directs the electron beam 16 horizontally and toward the ## and converges them on a fluorescent screen, an image can be displayed. On the policy you page 7200409167 V. Description of the invention (3) [0 0 1 3] One of the recently developed deflection magnets is a self-converging type deflection yoke, which uses horizontal and vertical deflection coils 2 丨, 2 The surrounding non-uniform magnetic field causes the red (R), green (G), and blue (B) three-color electron beams 16 to converge on the light screen without using another individual circuit or device. [0 0 1 4] In other words, by adjusting the steering distribution of the horizontal and vertical deflection coils 2 and 1, the self-converging type deflection yoke generates one in each section (ie, the middle, the middle, and the neck). Drum or pincushion magnetic field; At the same time, although the mother and electron beams of the electron beam 16 have different starting and ending positions, the self-convergence type magnetic field vehicle allows each color electron beam & But converges at one point from different distances). [0015] The screen portion of this 4 'deflection yoke refers to the portion with a relatively large diameter cross section, and the neck portion indicates the glory screen; the side has a portion with a relatively small diameter cross section.幵 尤 幵 丨 Another [0 0 1 6] The middle part, as the name suggests, is the middle part of the neck. Think about it, it indicates that the fluorescent screen and [0017] the above definitions are also suitable for the support, and the strontium #Xi, Di Di corpse is used to deflect the magnetic concept, deflection coil, ϋ 端 铁 ... 先 屏 #, neck, The side of the glorious screen and the head [〇0 1 8] At the same time, the cathode ray control 1 is, if only the typical problem of horizontal and vertical deviation = =-and the vertical deflection coils 21, 22 produce 4 scoops of electricity μ > The IL is coiled and the horizontal sub-beam 16 is deflected over the entire screen. It is actually difficult to minimize the level of the iron core 2 4 with the electric coefficient. Generally, the loss of the magnetic field with a south conduction chirp on its return path is usually used. Efficiency and magnetics.

200409167 五、發明說明(4) [00 1 9 ]然而,我們可以看到,偏轉磁軛之螢光屏 頸部經常不僅產生可朝水平及垂直方向偏轉電子束的磁場 ,也產生不必要的、對人體極有害的磁場漏洩。 [00 2 0 ]因此,需要一種可降低陰極射線管偏轉磁 生磁場漏洩的手段。 知 具體地說,務必使陰極射線管周圍產生的磁 漏保持低於一預定量。鑑於範圍在5Ηζ至2kHz :(明帶與範圍在2kHz至4GGkHz之間的甚低頻(Μ)帶低非 n ’所以’降低磁場漏茂的手段是絕對必要的。 之丰Γ然有ί製造商曾嘗試增加偏轉磁軛螢光屏部 Α之::二、f i 1』獲得高偏轉角並於最後降低陰極射線 吕之紇長,但徒然引起磁場漏洩之增加。 [0023]如前所述,曾右今夕 陰極射線管之總長。為;點集…何降低 獲得高偏轉角的技術 '然而,在此項:展展::: 平===屏部之半徑與傾角;同時“。 …果水千偏轉線圈處產生更多磁場漏洩。 [0024 ]降低磁場漏洩的 光屏部頂端與底端’安裝消二時疋’可在支座23之螢 24螢光屏側一端至水平偏轉圈狄a、25b,或增加鐵芯( 圈25a、2旰係附接在支座轉/輛之、‘構’其中消除線 [。㈣]就技術上而Ϊ ==端與底端。 底端的一對消除線圈25a、25b Μ $ 4坐螢光屏部頂端與 產生的磁場’可消除磁場200409167 V. Description of the invention (4) [00 1 9] However, we can see that the neck of the fluorescent screen of the deflection yoke often not only generates a magnetic field that can deflect the electron beam in horizontal and vertical directions, but also generates unnecessary, Leaks of extremely harmful magnetic fields. [0020] Therefore, there is a need for a means capable of reducing leakage of a deflected magnetic field of a cathode ray tube. Specifically, it is necessary to keep the magnetic leakage generated around the cathode ray tube below a predetermined amount. Given that the range is from 5 至 ζ to 2kHz: (the bright band and the very low frequency (M) band between 2kHz and 4GGkHz, the low non-n 'so' means to reduce the magnetic field leakage is absolutely necessary. Zhifeng there are manufacturers Attempts have been made to increase the deflection yoke fluorescent screen section A :: 2, fi 1 ″ to obtain a high deflection angle and finally reduce the length of the cathode ray Lu Zhi, but it caused an increase in magnetic field leakage in vain. [0023] As mentioned before, Zeng Right Tonight, the total length of the cathode ray tube. The point set ... how to reduce the technology to obtain a high deflection angle '. However, in this item: exhibition :: flat === the radius and inclination of the screen; at the same time ... [0024] The top and bottom ends of the light-shielding portion that reduces the magnetic field leakage can be 'installed to eliminate two times', which can be from the end of the fluorescent screen 24 on the support 23 to the horizontal deflection circle. a, 25b, or increase the iron core (circles 25a, 2 旰) are attached to the support turn / car, the 'structure' of which the elimination line [.㈣] is technically Ϊ == end and bottom end. Suppressing the coils 25a, 25b Μ $ 4 sitting on the top of the fluorescent screen portion and the generated magnetic field 'can eliminate the magnetic field

I 第9頁 200409167 五、發明說明(5) 漏洩。 [0 0 2 7 ]消除線圈2 5 a、2 5 b與水平偏轉線圈的連接方式 ,可使水平偏轉線圈2 1的螢光屏部所產生的磁場漏洩,與 消除線圈25a、25b内行進的水平偏轉電流所產生的主偏轉 磁場相反,因此消除在偏轉磁軛丨5螢光屏部與頸部產生的 磁場漏茂。 [0 0 2 8 ]如上所述,若對水平及垂直偏轉線圈2丨、2 2提 供電流以產生磁場,以便將電子束丨6偏轉到整個螢光屏時 ,以此方式產生的磁場並不足以達成此一目的。因此,要 使用具有高導磁係數的鐵芯24,將水平及垂直偏轉線圈2 i 、2 2所產生的磁場在其返回路徑上的損失減至最少,並 而改善磁效率與磁力。 w [ 0 0 2 9 ]通常,具有高導磁係數的鐵芯24基本上 化鐵(F 〇3)及其他添加物(例如猛、鎂等)。 年 [ 0 0 3 0 ]用於陰極射線管製品之鐵芯24,其形狀大 為圓形’但亦可使用矩形鐵芯以便增強效率。 刀 [〇〇31]圖3(a)顯示圓形鐵芯31 ,圖3(b)顯示矩形鐵芯 [ 0 0 32 ]實際上,鐵芯厚度與其放置位置 轉磁輛敏感度與磁場漏、;贫時的重要事項,戶斤以應 设什適當的鐵芯,以製造高品質的偏轉磁軛。〜、/思 [ 0 033 ]如前所述,鐵芯24對消除磁場極 ^ 可改善偏轉磁軛的偏轉效率並減少磁場漏洩:因此错, 24經常看來像個封閉的環圈,圍住偏轉磁軛。 鐵心I Page 9 200409167 V. Description of the invention (5) Leakage. [0 0 2 7] The elimination of the connection between the coils 2 5 a and 2 5 b and the horizontal deflection coil can make the magnetic field generated by the fluorescent screen portion of the horizontal deflection coil 21 leak, and the magnetic field generated in the elimination coils 25 a and 25 b The main deflection magnetic field generated by the horizontal deflection current is opposite, so the magnetic field leakage between the deflection yoke and the fluorescent screen and the neck is eliminated. [0 0 2 8] As mentioned above, if current is applied to the horizontal and vertical deflection coils 2 and 2 to generate a magnetic field so as to deflect the electron beam 6 to the entire screen, the magnetic field generated in this way is insufficient. To achieve this. Therefore, it is necessary to use an iron core 24 with a high magnetic permeability to minimize the loss of the magnetic field generated by the horizontal and vertical deflection coils 2 i, 2 2 on its return path, and improve the magnetic efficiency and magnetic force. w [0 0 2 9] In general, the iron core 24 having a high magnetic permeability is basically made of iron (F 0 3) and other additives (for example, ferrite, magnesium, etc.). [0 0 3 0] The iron core 24 used in cathode ray tube products has a large circular shape, but a rectangular iron core can also be used in order to enhance efficiency. Knife [〇〇31] Fig. 3 (a) shows a circular core 31, and Fig. 3 (b) shows a rectangular core [0 0 32] In fact, the thickness of the core and its placement position change the sensitivity and magnetic field leakage of the magnetic vehicle, Important matters when poor, households should set appropriate iron cores to make high-quality deflection yoke. ~ 、 / 思 [0 033] As mentioned before, the iron core 24 can eliminate the magnetic field poles ^ can improve the deflection efficiency of the deflection yoke and reduce the leakage of the magnetic field: so wrong, 24 often looks like a closed loop, enclosing Deflect the yoke. core

200409167 五、發明說明· (6) ’鐵芯24應具有高導磁係 以使由於渦電流而產生 根據先前技術之陰極射 及 [ 0034 ]若要實現所述的目押 數(/〇(例如高於300 )與高電^ 的任何損失最小化。 [0035]儘管有上述各種努 線瞢中,/含絲1 + 力’根據先前技 、、、良吕中偏轉磁軛用的鐵芯仍有盥# 品質關聯的各種問題。 有〃成本、重置、體積 [0036 ]例如,大部份偏轉 芯,其厚度高達6_或更厚,而错輛/使用的圓形/錐形鐵 達8關或更厚。 而鐵心之對角轉角厚度更高 [〇〇37]然而,若鐵芯厚度超過一 份(亦即大於預定之厚度)只產生邊卜”私度蚪’超過部 必要[°°:以]簡;;不: 受尸坏以,儘官不應如此,但JL制、主Λ、丄+ ^ 轉磁軛非常重而龐大。此外,偏轉磁:二:j使偏 費用方面的花費也比必要的程度偏高。、下卩牛,在運送 【發明内容】 η [ 0039 ]本發明目的之一是至少解決上述 點’並至少提供以下所述優點。 、/或缺 [0 0 4 0 ]因此’本發明目的之一是提 — 之偏轉磁輛…藉由實質減少習知鐵芯線管 有較低重量與體積’但不劣化其特性,以期 [ 004 1 ]本發明另一目的在於提供—種陰極 轉磁軛,其中藉由進行多數實驗而產出具射、、泉e之偏 /、为攻佳厚度之鐵 第11頁 200409167 五、發明說明(7) — 芯,因而降低製造成本、體積、重盎 化其偏轉能力。 /、衣運費用,但不劣 [ 0 042 ]本發明另一目的在於提供一種陰 轉磁軛:其中包括一水平偏轉線圈、一垂】偏轉線:、一 支撐並隔絕水平與垂直偏轉線圈 作書詈及辦拜士 Am —可降低漏磁通 仁重里及體積大幅減少而特性與大鐵芯 二 鐵芯可能引起的任何結構性問題的 :之鐵心、及湾 [0 0 4 3 ]為了實現前述及其他 的陰極射線管設有一面板、二 、、二,本發明提供 搶、及-可使電子搶發射之電偏轉:;子束之電子 轉磁軛包括一水平偏轉線圈,可 7轉磁軛。該偏 ,·一垂直偏轉線圈,可將電子束朝月水平方向偏轉 ’可支撐並同時隔絕該水平盥^:::偏轉;-支座 可降低該水平與垂直偏轉線圈;及-鐵芯, 磁通。其中,該鐵芯之厚度 格仏上的漏 -最大厚度點與一最小二:6_,且若該鐵芯内存在 小於3_。 …度點日…鐵芯之最大厚度點不 [ 0044 ]本發明另一層面提供的陰極射 、一漏斗、一發射電子束之電子 、吕叹有一面板 之電子束偏轉的偏轉磁軛。咳偏 可使電子搶發射 圈,可將電子束朝水平方向;=括—水平偏轉線 電子束朝垂直方向偏轉;一^:;2偏轉線圈,可將 平與垂直偏轉線圈;及一鐵芯,^ ^並同時隔絕該水 線圈所生磁場於返回路徑上的二& Μ水平與垂直偏轉 扪4磁通。其中,該鐵芯之厚 第12頁 20040916/ 五、發明說明(8) 度小於6mm,且該鐵芯内存在一 點’而該鐵芯之最大厚度點 二度:與-最小厚度 之間,其中,U是鐵芯長度。载〜,員4側一端與1/21^ 、一[漏°°斗45弋:=;】:=:陰=靖”—面板 之電子束偏轉的偏轉磁輛。該偏“輛包:!=::: 平與垂直偏轉線圈鐵Ϊ座可: = = =該水 -安裝磁輥之磁輛放置部上放=内;== =磁=置部内、外二表面之截面 == 漸?形改變為非圓形;且該鐵心之最大= 厚度在3mm至6mm間。 又…、占 [ 0046 ]本發明其他優點、目的及特徵,有一部 以下說明陳述’有些部份則為對此類技術有一般技能之人 查或實施本發明時即可理解的。 範圍中特別之指出’可實現及獲得本發明各項目的 【實施方式】 [0 0 5 6 ]以:芩照附圖詳細說明根據本發明一較佳每 例之陰極射線管偏轉磁幸厄。 貝心 [ 0057 ]通常,垂直偏轉之垂直電感值隨鐵芯漸薄而 少’而若施加電流時,冑光屏尺寸會稍微縮小。然而,藉200409167 V. Description of the invention · (6) 'The iron core 24 should have a high magnetic permeability system so that the cathodic emission according to the prior art is generated due to eddy currents and [0034] To achieve the stated number of charges (/〇(e.g. Higher than 300) and any loss of high power ^. [0035] Despite the above-mentioned various wires, the / core 1 + force 'according to the prior art, deflection yoke core is still有 洗 # Various problems related to quality. There are cost, replacement, and volume. [0036] For example, most deflection cores have a thickness of 6 mm or more, and the wrong car / round / tapered iron is used. 8 or thicker. The diagonal corner thickness of the core is higher [〇〇37] However, if the core thickness is more than one part (that is, greater than the predetermined thickness), only the marginal “privacy” is necessary [ °°: Yi] Jian; No: You should n’t be damaged by corpses, but the JL system, the main Λ, 丄 + ^ turn yoke is very heavy and huge. In addition, deflection magnetism: two: j bias cost The cost is also higher than necessary. Lower yak, transporting [Content of the invention] η [0039] One of the objects of the present invention is at least Resolve the above points and provide at least the advantages described below, and / or lack [0 0 4 0] Therefore, 'one of the objects of the present invention is to improve the deflection of magnetic vehicles ... by substantially reducing the conventional iron core tube has a lower 'Weight and volume' without deteriorating its characteristics, with a view to [004 1] Another object of the present invention is to provide a cathode-to-magnetic yoke, in which, by performing most experiments, a radiant, quasi-e bias /, is better Thickness of iron Page 11 200409167 V. Description of the invention (7)-core, thus reducing manufacturing cost, volume, and reversing its deflection ability. /, Clothing costs, but not inferior [0 042] Another object of the present invention is to Provide a female rotating yoke: including a horizontal deflection coil, a vertical] deflection line :, a support and isolation of the horizontal and vertical deflection coils for books and Ambassador Am-can reduce the magnetic flux leakage and the volume is greatly reduced The characteristics and any structural problems that the large iron core and two iron cores may cause: the iron core, and the bay. [0 0 4 3] In order to achieve the foregoing and other cathode ray tubes, a panel, two, and two are provided. The present invention provides Grab, and-make electricity Grab the electric deflection of the launch: the electron beam yoke of the sub-beam includes a horizontal deflection coil, which can turn 7 yokes. The deflection, a vertical deflection coil, can deflect the electron beam in the horizontal direction of the moon. Can be supported and isolated The horizontal toilet ^ ::: deflection;-the support can reduce the horizontal and vertical deflection coils; and-the iron core, the magnetic flux. Among them, the leakage of the thickness of the iron core grid-the maximum thickness point and a minimum two: 6_, and if there is less than 3_ in the iron core......... ....... degrees of the day ... the maximum thickness point of the iron core is not [0044] the cathode emission provided by another aspect of the present invention, a funnel, an electron that emits an electron beam, Lu Tan has a The deflection yoke of the panel's electron beam deflection. Cough deviation can make the electron grab the emission circle, which can direct the electron beam toward the horizontal direction; = bracket-horizontal deflection line, the electron beam is deflected toward the vertical direction; a ^ :; 2 deflection coil, which can flat and vertical deflection coil; ^^ At the same time, the magnetic field generated by the water coil is isolated from the two & M horizontal and vertical deflection magnetic fluxes on the return path. Among them, the thickness of the iron core Page 12 20040916 / V. Description of the invention (8) The degree is less than 6mm, and there is a point in the iron core, and the maximum thickness of the iron core is two degrees: between-and the minimum thickness, where , U is the core length. Load ~, one end of the 4 side and 1/21 ^, one [leak °° bucket 45 弋: =;]: =: yin = jing "—the deflection magnetic vehicle of the panel's electron beam deflection. The partial" car package :! " = ::: The flat and vertical deflection coil iron pedestal can be: = = = this water-the magnetic vehicle placement part on which the magnetic roller is installed is placed on the inside; = = = magnetic = the cross section of the inner and outer surfaces of the placement part = = gradually? The shape is changed to non-circular; and the maximum of the core = thickness is between 3mm and 6mm. [...] [0046] Other advantages, objects, and features of the present invention include one of the following descriptions stating that some parts are understood by those with ordinary skills in this type of technology when examining or implementing the present invention. It is particularly pointed out in the scope that the various objects of the present invention can be achieved and obtained. [Embodiment] [0 0 5 6] The detailed description of a cathode ray tube deflection magnetic circuit according to a preferred embodiment of the present invention will be described in detail with reference to the drawings. Beixin [0057] In general, the vertical inductance value of vertical deflection decreases with the thinning of the iron core ', and when the current is applied, the size of the chirped light screen will be slightly reduced. However, borrow

200409167 五、發明說明(9) ---- 由縮小習式偏轉線圈内的銅絲粗細及增加線圈圈數,可輕 易解決這個問題,而未必增加偏轉線圈之敏感度與增加制 造費用。 9衣 [0 0 5 8 ]這強調了發展技術降低鐵芯厚度的需要。 [0 0 5 9 ]陰極射線管製造商不介意使用此種厚鐵芯的主 要原因是’與通常龐大的偏轉磁軛製造成本比較時,鐵芯 的製造成本是微不足道的。 ~ [0 0 6 0 ]然而’現在許多人理解低成本是陰極射線管市 場競爭者的驅動力。從此一層面來看,能夠免除不必要的 生產成本並發展鐵芯薄、重量與體積都降低的陰極射線管 ,同時簡化產品運輸或處理等問題,乃當急之務。 [0 0 6 1 ]通常,一般咸信每塊鐵芯重量可使製造成本降 低1 0 %,並且如此可導致每一鐵芯價格下降5 %。然而,若 使用本發明之鐵芯,鐵芯重量可減少3 〇 %或更多。 曰[0 0 6 2 ]若鐵芯變薄,即有可能減少在偏轉磁軛(尤其 是在水平偏轉線圈)產生的磁場漏洩。 [0 0 6 3 ]換言之,若使用比習式鐵芯更薄的鐵芯時,也 可減少降低磁場漏洩(VLMF)所需的消除線圈圈數,並因此 相對地降低製造成本。 、[〇 〇 6 4 ]圖4中’(a)為一概要圖,顯示水平偏轉線圈與❿ 鐵芯的相對位置。 山[0 0 6 5 ]圖中之Lh指示水平偏轉線圈從〇至螢光屏側〆 之長度,〇指示水平偏轉線圈頸部側一端之位置。Lf 指不從鐵芯24頸部側一端之位置(Lfs)至鐵芯24螢光屏側200409167 V. Description of the invention (9) ---- By reducing the thickness of the copper wire in the conventional deflection coil and increasing the number of coils, this problem can be easily solved without necessarily increasing the sensitivity of the deflection coil and increasing the manufacturing cost. [0 0 5 8] This emphasizes the need to develop technology to reduce the thickness of the core. [0 0 5 9] The main reason why cathode ray tube manufacturers do not mind using such a thick iron core is that the manufacturing cost of the iron core is insignificant when compared with the manufacturing cost of the usually large deflection yoke. ~ [0 0 6 0] However, many people now understand that low cost is a driving force for competitors in the cathode ray tube market. From this perspective, it is an urgent task to eliminate unnecessary production costs and develop cathode ray tubes with thin cores, reduced weight and volume, and simplify product transportation or handling. [0 0 6 1] Generally, it is generally believed that the weight of each core can reduce the manufacturing cost by 10%, and in this way, the price of each core can be reduced by 5%. However, if the core of the present invention is used, the core weight can be reduced by 30% or more. [0 0 6 2] If the iron core becomes thin, it is possible to reduce the magnetic field leakage generated in the deflection yoke (especially in the horizontal deflection coil). [0 0 6] In other words, if a thinner core than a conventional core is used, the number of coil elimination coils required to reduce the magnetic field leakage (VLMF) can also be reduced, and thus the manufacturing cost can be relatively reduced. , [〇 〇 6 4] In FIG. 4, '(a) is a schematic diagram showing the relative position of the horizontal deflection coil and the ❿ iron core. In the mountain [0 0 6 5], Lh indicates the length of the horizontal deflection coil from 0 to the side of the fluorescent screen, and 0 indicates the position of the end of the horizontal deflection coil on the neck side. Lf refers to the position from the end of the neck side of the iron core 24 (Lfs) to the side of the iron core 24 fluorescent screen

200409167 五、發明說明(10) —端之位置(Lff)的長度。 [ 0 06 6 ]為了使鐵芯24較薄,Lh與Lf之比也應最佳化。 首先根據進行的實驗(稍後會說明)作一結論,Lf之範圍是 從O.ILh至〇.9Lh,且Lf較佳不少於35mm且不大於55mm。 [0 0 6 7 ]圖4 (b)顯示計算本發明薄鐵芯厚度之理論背景 [〇 〇 6 8 ]如先前之解說,本發明主要目的是設計一種具 有最小厚度之鐵芯。為此,其所使用的方法是根據鐵芯内 部磁通量的份量決定厚度。200409167 V. Description of the invention (10)-Length of the end position (Lff). [0 06 6] In order to make the iron core 24 thin, the ratio of Lh to Lf should also be optimized. First, make a conclusion based on the experiments performed (which will be described later). The range of Lf is from 0.1 ILh to 0.9Lh, and Lf is preferably not less than 35 mm and not more than 55 mm. [0 0 6 7] FIG. 4 (b) shows the theoretical background for calculating the thickness of the thin iron core of the present invention. [0060] As explained earlier, the main purpose of the present invention is to design an iron core with a minimum thickness. For this purpose, the method used is to determine the thickness based on the amount of magnetic flux inside the core.

[ 0 0 6 9 ]假設鐵芯内徑為2a,鐵芯外徑為2b,鐵芯頸部 旬至其末端之(直線)長度為c。那麼,從鐵芯内部線圈帶 入鐵芯區域之磁通量(0 i n ),以及鐵芯之飽和磁通量密度 (Bm),有0 ln $知之關係。其中,0m=:c(b_a)Bm,係表 示鐵芯之最高磁通量密度。 ’、 [ 0 0 70 ]由於等式中的(b — a)對應鐵芯之厚度七, 上等式可改寫為t^[(0in)/(Bm 。 旦[007 1 ]因此,鐵芯的最佳厚度可根據鐵芯厚度、磁 里、及鐵芯頸部側長度間的關係而獲得。[0 0 6 9] Assume that the inner diameter of the core is 2a, the outer diameter of the core is 2b, and the (straight) length from the neck of the core to its end is c. Then, the magnetic flux (0 i n) brought from the inner coil of the core into the core region and the saturation magnetic flux density (Bm) of the core have a relationship of 0 ln $. Among them, 0m =: c (b_a) Bm, which represents the highest magnetic flux density of the iron core. ', [0 0 70] Since (b — a) in the equation corresponds to the thickness of the core of seven, the above equation can be rewritten as t ^ [(0in) / (Bm. Once [007 1], therefore, the The optimal thickness can be obtained based on the relationship between the core thickness, the magnetic back, and the length of the neck side of the core.

[0 072 ]例如,在本發明中係選用最廣泛使用 現=中狀8_厚鐵芯作實,驗,以獲得鐵 7 果為了貫驗,鐵芯曾以多種方法修改並檢查有無更化心 [0073]通常,電視的偏轉磁軛與監 ,若其各自之陰極射線管呈有彳 、扁轉磁軛中 ”有相同的偏轉角時,則偏轉磁[0 072] For example, in the present invention, the most widely used current = medium-thick 8-thick iron core is used as a test to obtain iron. In order to perform the test, the iron core has been modified in various ways and checked for more changes. [0073] Generally, the deflection yoke and the monitor of a television have the same deflection angle if their respective cathode ray tubes have the same deflection angle in the yoke and the oblate yoke.

200409167 五、發明說明(11) 軛内部具有幾乎完全相同的磁場。 [0 0 7 4 ]當然,調整(或更改)磁場強度的方法各不相同 。然而,僅從磁場層面來看時,兩種裝置之一内的線圈所 產生的磁場大小,彼此差異並非那麼大,而且,若磁場相 同的鐵芯彼此結構及位置相同時,它們會執行同樣的工作 。其基本論題是,鐵芯是否具有相同的磁場強度。 [0 0 7 5 ]簡言之,雖然本發明實驗僅使用監視器偏轉磁 軛之鐵芯,但也可使用電視偏轉磁軛之鐵芯。 [0 0 7 6 ]此外,安裝磁軛之磁軛放置部其内表面之截面 ,或其内、外二表面之截面,係從頸部側往螢光屏側,逐φ 漸從圓形變成非圓形,或者也可以保持圓形。 [0 0 7 7 ]圖5為截面圖,顯示根據本發明之鐵芯的厚度 :圖6為立體圖,顯示鐵芯頸.部側一端之厚度及内徑。 [ 0 0 78 ]圖5(a)中顯示鐵芯24位於頸部側一端之厚度Τη ,鐵芯往螢光屏側之不同厚度11、12、13、…、t η,鐵芯 長度Lf,及鐵芯頸部側一端之直徑Dn。 [0079]圖5(b)顯示圓形鐵芯52之截面及其厚度tl、t2 、t3、…、tn ;圖5(c)顯示矩形鐵芯53之截面及其厚度11 、12、13、…、t η 〇 [0 0 8 0 ]圖6為一圓形鐵芯6 1之立體外觀圖。圖5 ( a )中 · 有關Τη與Dn的定義也適用於此處。 [0 0 8 1 ]如前所述,本發明之實驗使用6. 8mm厚的鐵芯 ,且於每次觀察中,逐漸減少其厚度0 . 5 m m。繼續此過程 ,直到鐵芯厚度比原樣品薄3. 5 m m為止。200409167 V. Description of the invention (11) The yoke has almost the same magnetic field inside. [0 0 7 4] Of course, the methods of adjusting (or changing) the magnetic field strength are different. However, from the perspective of the magnetic field only, the magnitudes of the magnetic fields generated by the coils in one of the two devices are not so different from each other, and if the cores with the same magnetic field have the same structure and position, they will perform the same jobs. The basic issue is whether the cores have the same magnetic field strength. [0 0 7] In short, although the experiment of the present invention uses only the iron core of the monitor deflection yoke, the iron core of the television deflection yoke can also be used. [0 0 7 6] In addition, the cross section of the inner surface of the yoke placement part on which the yoke is installed, or the cross section of the inner and outer surfaces thereof, is gradually changed from circular to φ from the neck side to the fluorescent screen side. Non-circular, or it can remain circular. [0 0 7 7] FIG. 5 is a sectional view showing the thickness of the iron core according to the present invention: FIG. 6 is a perspective view showing the thickness and inner diameter of one end of the core neck. [0 0 78] FIG. 5 (a) shows the thickness Tn of the iron core 24 at one end of the neck side, the different thicknesses 11, 12, 13, ... t η of the iron core toward the fluorescent screen side, and the core length Lf, And the diameter Dn of the end of the neck side of the core. [0079] FIG. 5 (b) shows the cross section of the circular iron core 52 and its thickness t1, t2, t3, ..., tn; FIG. 5 (c) shows the cross section of the rectangular iron core 53 and its thickness 11, 12, 13, ..., t η 〇 [0 0 8 0] FIG. 6 is a three-dimensional appearance view of a circular iron core 61. The definitions of Tn and Dn in Figure 5 (a) also apply here. [0 0 8 1] As mentioned previously, the experiment of the present invention uses a 6.8 mm thick iron core, and in each observation, its thickness is gradually reduced by 0.5 m m. This process continues until the core thickness is 3.5 mm thinner than the original sample.

第16頁 200409167Page 16 200409167

[0082]更具體地說,實 & ^ 铽厘声筘圊你fi sm攸 、把甲、、心半備了 8個樣品,鐵 〜尽度粑圍攸6. 8_降至3. 3_。然後 线 涉及磁特性、對螢光屏盥 樣°卩接叉各種 ,、了罪性(生熱特性)之影響的試驗 [ 0 0 8 3 ][表1 厚度(mm) 6. 8 電感(mH) 0. 13 6 « 可以得到的結 習用6. 8mm厚 鐵芯厚度減 [0 0 9 0 ]如果鐵芯溫度上升而其特性劣化時,將會是個3__3. 3_ . Then the line involves magnetic characteristics, various types of fluorescent screens, and various tests of the influence of heat (heat generation characteristics) [0 0 8 3] [Table 1 Thickness (mm) 6. 8 Inductance (mH ) 0. 13 6 «Available for conventional 6.8mm thick iron core minus [0 0 9 0] If the core temperature rises and its characteristics deteriorate, it will be a

200409167 五、發明說明(13) 嚴重的問題。然而’很幸運地,習用鐵芯之居禮溫度高於 13 0 C ’而鐵芯之導磁係數在抵達居禮溫度前,有更好的 傾向。因此,這個問題也可視為可忽略來處理。 [0 0 9 1 ]在垂直偏轉線圈的情況時,由於其位置較靠近 鐵芯,所以其電感隨鐵芯厚度稱微下降。 [ 0092 ][表2] 厚度(mm) 6. 8 6. 3 5. 8 4. 8 4. 3 3. 8 3.3 電感(mH) 6. 33 5 6. 30 0 6· 31 3 6.30 6 ----—一·· _ 6. 25 4 6. 23 7 6. 21 0 6. 06 [0 0 9 3 ]表2顯示垂直偏轉線圈之電感值隨鐵芯厚度改 變的情況。 [ 00 94 ]如表2所示,當正常鐵芯厚度從68mm降至33 mm時,垂直偏轉線圈之電感降低〇. 27mH(約下降4%)。 [0095]此外,電子束之垂直偏轉尺寸也下降。 、[ 0 0 9 6 ]由於鐵芯厚度減少所造成的垂直偏轉線圈4%的 電感下降,可以藉由增加垂直偏轉線圈的圈數(通常為丨〇 〇 圈)4-6圈而輕易補償。以此方式,偏轉線圈可以執行其正 常工作,亦即偏轉電子束,而不會造成功率損失或需要修 改線圈之實質結構。 / [ 0 0 9 7 ]若鐵芯厚度減少3mm,諸如從68關減至3 8_❿ ’垂直偏轉線圈之電感只降低一小量,諸如從6335_降 至6.21〇11111,顯示下降不超過2%左右。 [ 0098 ]同樣地,儘管鐵芯厚度減少,但是根據垂直偏 轉的會聚度並未觀察到重大改變。200409167 V. Description of the invention (13) Serious problems. However, ‘fortunately, the habit temperature of conventional iron cores is higher than 13 0 C’ and the magnetic permeability of the iron core has a better tendency before reaching the rite temperature. Therefore, this problem can also be treated as negligible. [0 0 9 1] In the case of a vertical deflection coil, since its position is closer to the iron core, its inductance decreases slightly with the thickness of the iron core. [0092] [Table 2] Thickness (mm) 6. 8 6. 3 5. 8 4. 8 4. 3 3. 8 3.3 Inductance (mH) 6. 33 5 6. 30 0 6 · 31 3 6.30 6- ----- _ 6. 25 4 6. 23 7 6. 21 0 6. 06 [0 0 9 3] Table 2 shows how the inductance of the vertical deflection coil changes with the thickness of the core. [00 94] As shown in Table 2, when the normal iron core thickness was reduced from 68 mm to 33 mm, the inductance of the vertical deflection coil was reduced by 0.27 mH (about 4%). [0095] In addition, the vertical deflection size of the electron beam is also reduced. [0 0 9 6] Due to the decrease of the core thickness, the inductance of the vertical deflection coil decreases by 4%, which can be easily compensated by increasing the number of turns of the vertical deflection coil (usually 丨 〇 〇) 4-6. In this way, the deflection coil can perform its normal work, that is, deflecting the electron beam without causing power loss or needing to modify the physical structure of the coil. / [0 0 9 7] If the thickness of the iron core is reduced by 3mm, such as from 68 to 3 8_❿ 'The inductance of the vertical deflection coil is only reduced by a small amount, such as from 6335_ to 6.21〇11111, which shows that the decrease is not more than 2% about. [0098] Similarly, no significant change was observed in the degree of convergence according to the vertical deflection despite the decrease in the core thickness.

200409167 五、發明說明(14) [0 0 9 9 ]總而έ之’以水平偏轉 ^ 減少原始厚度(亦即7mm)的50°/。或更夕·而。’鐵心厚度可 而言,鐵芯之適當厚度可根據垂直二’而以垂直偏轉線圈 [謝。〇]假設現行垂直偏轉沒直有偏門轉g之補_ 度是垂直電感之5%,那麼鐵芯的較喊,而鐵』適當厚 3.〇_。 "^土最低厚度可以下降到 [〇〇101 ]使用此種薄鐵芯,加h — a u _ 圈數及線圈厚度相關),即有可能制、心:術:助(與線圈 芯但仍維持鐵芯的重要特性。衣k成本大為低廉之鐵 [ 0 0 1 02 ]根據表1及表2顯示的實驗結果及肖其所作的 分析’本發明之鐵芯所需的最大厚度點是在3襲至6 圍内。 [00103]此外,根據本發明之薄鐵芯,其長度“應在 O.ILh至0.9Lh的範圍内,才不致於造成鐵怒特性劣化,並 可產生與以前相同的效果。 [ 0 0 1 04 ]更佳是,鐵芯之最大厚度點是在4mm至6mm的 範圍内。 [0 0 1 0 5 ]隶佳是’如果希望最小化製造成本而不改變 鐵怒本身的特性時,鐵芯之最大厚度點是在4m[n至5. 5的 範圍内。 [ 0 0 1 0 6 ]同時,薄鐵芯頸部側一端之厚度Tn不大於5mm ,且不小於4mm。 [0 0 1 0 7 ]此種類型之鐵芯,不論從其頸部侧一端至螢 光屏側一端之形狀是否完全為圓形、或其頸部側一端之截200409167 V. Description of the invention (14) [0 0 9 9] In short, ‘to deflection horizontally ^ Reduce the original thickness (ie 7mm) by 50 ° /. Or even more. "The thickness of the core can be said, the appropriate thickness of the core can be vertical deflection coil according to the vertical two" [thanks. 〇] Assuming that the current vertical deflection is not straight, the complement of the gate rotation g is 5% of the vertical inductance, then the iron core is shouted, and the iron is appropriately thick 3.〇_. " ^ The minimum thickness of the soil can be reduced to [〇〇101] Using this thin iron core, adding h — au _ number of turns and the thickness of the coil is related, it is possible to control, heart: surgery: help (with the coil core but still maintain iron The important characteristics of the core. The cost of iron is very low [0 0 1 02] According to the experimental results shown in Tables 1 and 2 and the analysis made by Xiao Qi ', the maximum thickness point required for the core of the present invention is 3 [00103] In addition, according to the thin iron core of the present invention, the length "should be in the range of 0.1 ILh to 0.9 Lh, so as not to cause the deterioration of iron rage characteristics, and can produce the same effect as before. [0 0 1 04] More preferably, the maximum thickness point of the iron core is in the range of 4mm to 6mm. [0 0 1 0 5] Lijia is' if you want to minimize the manufacturing cost without changing the characteristics of the iron rage itself At this time, the maximum thickness point of the iron core is in the range of 4m [n to 5.5]. [0 0 1 0 6] At the same time, the thickness Tn of the neck-side end of the thin iron core is not more than 5mm and not less than 4mm. [0 0 1 0 7] This type of iron core, regardless of whether the shape from its neck side end to the screen side end is completely round, Sectional side end of the neck

19 200409167 五、發明說明(15) 面九竟為圓形或矩形、或其螢光屏側一端之截面是否為矩 形’都可廣泛使用之。 [ 0 0 1 08 ]在後一情況時,最大厚度點較佳在3mn]至6mm 的範圍内。 [0 0 1 0 9 ]此外,本發明之原理也適用於分段型鐵芯。 [0 0 1 1 0 ]至於螢光屏側一端截面為矩形之鐵芯,其長 度Lf之範圍在〇.1Lh至〇.9Lh之間,其中,Lh是水平偏轉線 圈之長度。更具體地說,Lf不大於5 5 mm且不小於35 mm。 [0 0 111 ]尤其是螢光屏側一端截面為矩形之鐵芯,其 农大厚度點更佳是在4mm至6mm的範圍内。 、[0 0 11 2 ]最佳是,如果希望最小化製造成本而不改變 鐵芯本身的特性時,鐵芯之最大厚度點是在4mm至5·5ιηπ]的 範圍内。 [0 0 11 3 ]螢光屏側一端截面為矩形之鐵芯,其頸部側 立而之隶大厚度Τη較佳不大於5mn]且不小於^!^。 [0 0 11 4 ]本發明之鐵芯可應用於電視與電腦監視器。 用1電視日^ ’其敢大水平掃描頻率低於4 8 k η z ;用於監視 為時’其最大水平掃描頻率低於8〇kHz。 [00115] 通常’監視器使用鞍/鞍型偏轉線圈(前者對 應水平偏轉線圈而後者對應垂直偏轉線圈,其中,"鞍型”· 才曰不線圈形狀);電視則使用鞍/鞍型或鞍/環型線圈(前者 對應水-平偏轉線圈而後者對應垂直偏轉線圈,其中,”環 型表示鐵芯為直接用線圈環繞)。 [00116] 不論型式如何,都可使用本發明之薄鐵芯。 200409167 五、發明說明(16) 此乃因為,只要其内部磁場強度不過度改變,鐵芯厚度並 不需要顯著改變。 [0 0 1 1 7 ]因此,當本發明之薄鐵芯應用在監視器與電 視時,每種都可證明鐵芯的不同特性。這些特性有些已在 先前討論過,現在則說明其他特性。 [0 0 1 1 8 ]在多數情況中,鐵芯頸部側一端與鐵芯總厚 度比較時,是非常厚的。此乃因為鐵芯頸部側一端的溫度 高於其他部位,表示它應相對具有較佳的放熱特性。 [0 0 1 1 9 ]因此,當使用本發明之薄鐵芯時,頸部側一 端之厚度應為4mm-5mm左右,且應至少為最大厚度的80%。 [0 0 1 2 0 ]根據觀察,當頸部側一端為最厚,或比最大 厚度的8 0 %薄時,鐵芯之放熱特性會退化。因此,務必要 使頸部側一端之厚度至少保持在鐵芯最大厚度點的8〇%。 [00121]圖7(a)中顯示非完全圓形的鐵芯71,圖7(b) 顯示完全圓形的鐵芯7 2。 [0 0 1 2 2 ]請參照圖7,n Max. Dnπ指示鐵芯頸部側一端之 最大内徑Dn,n Max· Τη”則指示鐵芯頸部側一踹夕旧L, 、,叫 鳊之取大厚麿 Τη。此二變數為設計本發明之薄鐵芯時,不減損 性與優點的重要因數。 、’、、戥心特19 200409167 V. Description of the invention (15) Face 9 is actually round or rectangular, or whether the cross section of the side of the fluorescent screen is rectangular, can be widely used. [0 0 1 08] In the latter case, the maximum thickness point is preferably in the range of 3 mm] to 6 mm. [0 0 1 0 9] In addition, the principles of the present invention are also applicable to segmented cores. [0 0 1 1 0] As for the iron core with a rectangular cross section at one end of the phosphor screen, the length Lf thereof ranges from 0.1 Lh to 0.9 Lh, where Lh is the length of the horizontal deflection coil. More specifically, Lf is not more than 55 mm and not less than 35 mm. [0 0 111] Especially, the iron core with a rectangular cross section at one end on the side of the fluorescent screen has a thickness of more than 4 mm to 6 mm. [0 0 11 2] The best is that if you want to minimize the manufacturing cost without changing the characteristics of the core itself, the maximum thickness point of the core is in the range of 4mm to 5.5mm. [0 0 11 3] A rectangular iron core having a rectangular cross section at one end on the side of the fluorescent screen, and a large thickness Tn on the side of the neck side is preferably not more than 5mn] and not less than ^! ^. [0 0 11 4] The iron core of the present invention can be applied to televisions and computer monitors. With 1 TV day ^ ', it dares to have a large horizontal scanning frequency below 4 8 k η z; for monitoring, its maximum horizontal scanning frequency is below 80 kHz. [00115] In general, a monitor uses a saddle / saddle type deflection coil (the former corresponds to a horizontal deflection coil and the latter corresponds to a vertical deflection coil, of which " saddle type " is not a coil shape); a television uses a saddle / saddle type or Saddle / ring coil (the former corresponds to the horizontal-horizontal deflection coil and the latter corresponds to the vertical deflection coil, where "ring type" means that the iron core is directly surrounded by the coil). [00116] Regardless of the type, the thin iron core of the present invention can be used. 200409167 V. Description of the invention (16) This is because, as long as the internal magnetic field strength does not change excessively, the core thickness does not need to change significantly. [0 0 1 1 7] Therefore, when the thin iron core of the present invention is applied to a monitor and a television, each can prove different characteristics of the iron core. Some of these features have been discussed previously, but others are now explained. [0 0 1 1 8] In most cases, the end of the core neck side is very thick when compared with the total thickness of the core. This is because the temperature at the end of the neck of the iron core is higher than other parts, which indicates that it should have relatively good heat dissipation characteristics. [0 0 1 1 9] Therefore, when the thin iron core of the present invention is used, the thickness at the end of the neck side should be about 4mm-5mm, and it should be at least 80% of the maximum thickness. [0 0 1 2 0] According to observation, when the end of the neck side is the thickest or is thinner than 80% of the maximum thickness, the heat release characteristics of the iron core are degraded. Therefore, it is important to keep the thickness of the neck-side end at least 80% of the maximum thickness of the core. [00121] A non-fully circular iron core 71 is shown in FIG. 7 (a), and a completely circular iron core 72 is shown in FIG. 7 (b). [0 0 1 2 2] Please refer to FIG. 7, n Max. Dnπ indicates the maximum inner diameter Dn of the end on the neck side of the iron core, n Max · Tη ”indicates the old L,,,, called Take a large thickness. This two variables are important factors in designing the thin iron core of the present invention without detracting from the advantages and advantages.

[0 0 1 2 3 ]較佳是,對圖7所示 而言,鐵芯最大厚度與頸部側一 2且不小於1. 〇。〇。 [0 0 1 2 3] Preferably, as shown in FIG. 7, the maximum thickness of the core and the neck side is 2 and not less than 1.0.

200409167 五 、發明說明(17) '200409167 V. Description of Invention (17) ''

Max. Dn與鐵芯最大厚度之比不大於1〇· 5且不小於7. 〇。另 一方面,至於用於電視的偏轉磁軛,其比值不大於丨2. 5且 不小於9 . 0。 [0 0 1 2 5 ]圖8為一概要圖,顯示鐵芯從螢光屏側一端起 位於長度1/3點之厚度,與鐵芯頸部側一端之厚度。如前 所述,此圖表示最佳薄度鐵芯24從f光屏側—端往頸部側 =點之厚度(T—1/3s)與頸部側一端最大厚度Max. Τη 間的關係。 ^々[2 〇i t不淪螢光屏側一端之截面為圓形或橢圓形, 二,夫二=側一端往頸部側位於1 /3點之厚度與頸部側 一H厚度Max.Tn之比,不大於1〇且不小於〇 8。 f作一薄& _總广,本發明主要焦點在於根據最佳化設計 要:。本發明鐵芯之優點在於去除厚鐵芯 性。 ^而可降低製造成本,但不損失鐵芯本身的特 偏轉[:=]重?:體言積使用本發一明之鐵芯,可大幅降低 量化。因&,可降:運衿;:卜’它有助於陰極射線管之輕 容易得多。 輪費用’陰極射線管之處理也變得 [〇 0 1 2 9 ]以上雖然是失日” 示與說明本發明,但孰/此:,明若干較•實施例以顯 形式與細節可作多種變;;$ =技術之人士應可理解,其中 圍中定義的精神與範圍。不脫離本發明所附申請專利範 [〇〇130]前述實施例與優點僅為解說之用,並非用以 200409167 五、發明說明(18) 限制本發明。本發明可隨時應用於其他類型之裝置。本發 明說明目的在舉例說明而非限制申請專利範圍之範圍。熟 悉此類技術之人士顯然可作許多選擇、修改與變更。各項 請求項中的手段加功能語句,其目的是涵括本文說明用以 執行所述功能的結構,其不僅包括結構同等品,亦包括各 種同等結構。〇。 The ratio of Max. Dn to the maximum thickness of the core is not more than 10.5 and not less than 7.0. On the other hand, as for the deflection yoke for television, its ratio is not more than 2.5 and not less than 9.0. [0 0 1 2 5] FIG. 8 is a schematic diagram showing the thickness of the iron core at a length of 1/3 from the end of the phosphor screen side and the thickness of the iron core neck side end. As mentioned before, this figure shows the relationship between the optimal thinness iron core 24 from the f-screen side to the neck side = the thickness of the point (T-1 / 3s) and the maximum thickness at the neck side Max. Τη . ^ 々 [2 〇it The cross section of the end of the fluorescent screen is circular or oval. Second, the second side = the thickness of the side to the neck side at 1/3 points and the thickness of the neck side H. Max.Tn The ratio is not more than 10 and not less than 0. f make a thin & _ total, the main focus of the present invention is to optimize the design according to:. The core of the present invention has the advantage of removing the thick core. ^ It can reduce the manufacturing cost without losing the special deflection of the core itself [: =] : The body language product uses the iron core of this invention, which can greatly reduce the quantization. Because of &, it can be lowered: 运 衿;: 卜 ’It helps the cathode ray tube to be much easier. The cost of the round cathode cathode ray tube processing has also become [〇0 1 2 9] Although the above is an "out of date", the present invention is shown and explained, but this is not clear: some examples can be used in various forms and details. Change ;; $ = technical people should understand that the spirit and scope defined in it. Without departing from the patent application attached to the present invention [00130] The foregoing embodiments and advantages are for illustration purposes only, not for 200409167 V. Description of the invention (18) Limits the invention. The invention can be applied to other types of devices at any time. The purpose of the description of the invention is to illustrate rather than limit the scope of patent applications. Those skilled in this technology can obviously make many choices, Modifications and changes. The means and functional statements in each request are intended to include the structure described in this article to perform the described function, which includes not only structural equivalents, but also various equivalent structures.

第23頁 200409167Page 23 200409167

【圖式簡單說明】 [0 0 4 7 ]本發明係參昭以 的參考標號係指稱相同^件了,圖作詳細說明,圖中相同 [0 0 4 8 ]圖1為一概要圖,_圖匕括. 管; ^不一先前技術之陰極射線 [0049] 圖2為一陰極粉妙其/么 射線e偏轉磁軛之立體外觀圖; [0050] 圖3說明圓形鐵芯與矩形鐵芯之結構; [0 0 5 1 ]圖4解說水平偏轉線圈與鐵芯之相對位置,並 表示根據本發明之鐵芯其厚度的計算背景; [〇 〇 5 2 ]圖5為根據本發明之鐵芯其厚度之截面圖; [0 0 5 3 ]圖6為一立體圖,顯示鐵芯頸部側一端之厚度 與鐵芯之内徑; [0 0 5 4 ]圖7為概要圖,分別顯示近圓形與圓形鐵芯其 頸部側一端之厚度與内徑;以及 [〇 〇 5 5 ]圖8為一概要圖,顯示本發明中鐵芯從螢光屏 側一端開始至鐵芯長度1 / 3點之位置的厚度,與鐵芯頸部 側一端之厚度。 【元件符號對應表】 I 面板[Brief description of the drawings] [0 0 4 7] The reference numerals used in the present invention refer to the same ^ pieces, the drawings are described in detail, the same in the drawings [0 0 4 8] Figure 1 is a schematic diagram, _ Figure 2 shows a tube; ^ a cathode ray of a prior art. [0049] FIG. 2 is a perspective view of a cathode powder mag / ray ray deflection yoke; [0050] FIG. 3 illustrates a circular iron core and a rectangular iron. Structure of the core; [0 0 5 1] FIG. 4 illustrates the relative position of the horizontal deflection coil and the iron core, and shows the calculation background of the thickness of the iron core according to the present invention; [〇〇5 2] FIG. Sectional view of the thickness of the iron core; [0 0 5 3] FIG. 6 is a perspective view showing the thickness at the end of the neck side of the iron core and the inner diameter of the iron core; [0 0 5 4] FIG. 7 is a schematic diagram showing each The thickness and inner diameter of the neck-side end of the near-circular and circular cores; and [〇〇5 5] FIG. 8 is a schematic diagram showing the length of the core from the end of the fluorescent screen side to the core length in the present invention The thickness at the point of 1/3, and the thickness at the end of the neck side of the core. [Component symbol correspondence table] I panel

II 陰極射線管 12 螢光屏 13 電子搶 14 蔭罩 15 偏轉磁軛II cathode ray tube 12 fluorescent screen 13 electron grab 14 shadow mask 15 deflection yoke

第24頁 200409167 圖式簡單說明 16 電子束 2 漏斗 21 水平偏轉線圈 22 垂直偏轉線圈 23 支座 24 鐵芯 2 5 a 消除線圈 2 5 b 消除線圈 2 6 a 連接線 26b 連接線 27 連接板 31 圓形鐵芯 32 矩形鐵芯 5 2 圓形鐵芯 53 矩形鐵芯 61 圓形鐵芯 71 鐵芯 72 鐵芯Page 24 200409167 Brief description of the diagram 16 Electron beam 2 Funnel 21 Horizontal deflection coil 22 Vertical deflection coil 23 Stand 24 Iron core 2 5 a Elimination coil 2 5 b Elimination coil 2 6 a Connection line 26b Connection line 27 Connection plate 31 Round Shaped iron core 32 rectangular iron core 5 2 round iron core 53 rectangular iron core 61 round iron core 71 iron core 72 iron core

第25頁Page 25

Claims (1)

200409167 六、申請專利範圍 1 · 一種陰極射線管之偏轉磁軛,μ 電子搶用以發射電子束、及一 ς二面板、一漏斗、一 搶發射之電子束;該偏轉磁軛包括軛用以偏轉該電子 一水平偏轉線圈,可將 -垂直偏轉線圈,可:水平方向偏轉; -支座,可支樓並同垂直方向偏轉; ,•及 亥水平與垂直偏轉線圈 鐵心,可降低該水平盘 返回路徑上的漏磁通;i中; 專線圈所生磁場於 若該鐵芯中存在最大與最厚y,且 點不小於3_。 与度2日可,該鐵芯最大厚度 ΐ偏轉磁輕’設有-面板、-漏斗、- 搶發射之電子束;該偏轉磁辆=輕用以偏轉該電子 -::偏轉線圈’可將電子束朝水平 一=偏轉線圈,可將電子束朝垂直方向偏轉: ;及1座’可支撐並同時隔絕該水平與垂直偏轉線圈 :鐵芯,可降低該水平與垂直偏轉線圈所生磁 該属磁通;其中該鐵芯之厚度小於6_,且, j鐵心中存在最大與最小厚度點;該鐵芯最大厚户且 ,芯頸部側一端與1/2Lf之間,其中,Lf是“係 漏 種陰極射線管之偏轉磁概,設有一面板、 200409167 六、申請專利範圍 電子搶用以發射電子束、及_偏轉磁 搶發射之電子束;該偏轉磁軛包括: 偏轉该電子 一水平偏轉線圈,可將電子束朝 一垂直偏轉線圈,可將電子束 偏轉; 一 #庙叮士产、,门士 采朝垂直方向偏轉; :及可支撑亚同日爾該水平與垂直偏轉線圈 返回的;:Π:與垂直偏轉線圈所生磁場於 、w峪仏上的漏磁通,其中該漏斗具穷孓 軛放置部,且該磁軛放置部内表 ,石軛之磁 丨 外一表面之截面,係從頸部 、夏 從圓形改變為非圓形;且該鐵幵貝1 ,逐漸 至6mm的範圍間。 之取大厚度點厚度在 4. 如申請專利範圍第!至第3項之偏轉磁軛 芯最小厚度點之厚度不小於2mm。 ,、 4於该鐵 5. 如:請專利範圍第i至第3項之偏轉磁輛,其中 芯取大厚度點之厚度在4mm至6襲的範圍間了 。" ’ 6. 如申請專利範圍第i至第3項之偏轉磁輛,立 轉線圈從頸部俱1 一端至螢光屏彻! 一端之長度^ 頸:側一端至勞光屏側-端之長度為Lf :而該;载J 頸則一端至該鐵芯螢光屏側一端係位 , 圈之0· ILh至0· 9Lh的範圍内。 > 卞獅得、、泉 7. 如申請專利範圍第i至第3項之偏轉磁 頸部側-端至榮光屏側—端之長度不大於55襲且不小二 35mm 〇 ' 第27頁 200409167 六、申請專利範圍 8 ·如申請專利範圍第 截面為圓形或橢圓 9.如申請專利範圍第 部側一端之厚度不 10·如申請專利範圍 最大厚度與該鐵芯 於1 · 2且不小於1. 〇 11 ·如申請專利範圍 從螢光屏側一端開 芯頸部側一端之最 〇· 8 〇 12· 如申請專 為一分段式 13· 如申請專 偏轉磁|厄之 1 4 ·如申請專 側一端之最 且不小於7. 15, 如申請專 偏轉磁輕之 1 6 ·如申請專 側一端之最 I不小於9. 1?, 如申請專 利範圍 鐵芯。 利範圍 陰極射 利範圍 大内經 利範圍 陰極射 利範圍 大内徑 3 ° 利範圍200409167 VI. Application Patent Scope 1. A deflection yoke of a cathode ray tube, in which μ electrons are used to emit an electron beam, and a two-plate, a funnel, and an electron beam are emitted; the deflection yoke includes a yoke for To deflect the electron, a horizontal deflection coil can deflect the vertical deflection coil: horizontal deflection;-a stand that can support the building and deflect in the vertical direction; and the horizontal and vertical deflection coil cores can lower the horizontal disc The leakage magnetic flux on the return path; i; The magnetic field generated by the special coil is if the largest and thickest y exists in the core, and the point is not less than 3_. With the degree of 2 days, the maximum thickness of the iron core ΐ deflection magnetic light 'is provided with-panel,-funnel,-grab the emitted electron beam; the deflection magnetic vehicle = light to deflect the electron-:: deflection coil' can The electron beam is oriented horizontally = deflection coil, which can deflect the electron beam vertically:; and 1 'can support and isolate the horizontal and vertical deflection coils at the same time: iron core, which can reduce the magnetic generated by the horizontal and vertical deflection coils. It is a magnetic flux; where the thickness of the iron core is less than 6_, and there are maximum and minimum thickness points in the iron core; the maximum thickness of the iron core is between the end of the core neck side and 1 / 2Lf, where Lf is " The deflection magnetism of the leaky cathode ray tube is provided with a panel. 200409167 VI. Patent application scope Electronic grabbers are used to emit electron beams and _deflected magnetic grabbers are used to emit electron beams; The deflection yoke includes: deflects the electrons to a level The deflection coil can direct the electron beam toward a vertical deflection coil, which can deflect the electron beam; ## iaodingshi production, Menshicai deflection in the vertical direction; and the horizontal and vertical deflection coils that can support the return of the horizontal and vertical deflection coils in Asia : Π: leakage magnetic flux on w, with the magnetic field generated by the vertical deflection coil, wherein the funnel has a poor yoke placement part, and the inner surface of the yoke placement part, the cross section of the outer surface of the magnet of the stone yoke, It changes from the neck and Xia from circular to non-circular; and the iron scallop 1 gradually ranges from 6mm. The thickness is taken as the point thickness. 4. As the scope of the patent application No.! To No. 3 deflection The thickness of the minimum thickness point of the yoke core is not less than 2mm. , 4 and the iron 5. For example, please apply for the deflection magnetic vehicle of item i to item 3, where the thickness of the core is 4mm to 6 The range is between. &Quot; '6. For the deflecting magnetic vehicles of the scope of application for items i to 3, the vertical turning coil runs from the neck to the end of the fluorescent screen! The length of one end ^ Neck: one end to the side The length of the screen side-end is Lf: and this; the end of the J-carrying neck is tied to the end of the iron core fluorescent screen side, in the range of 0 · ILh to 0.9Lh. ≫ 卞 狮 得 、、 泉7. The length of the deflection magnetic neck side-end to the glorious screen side-end of the scope of application for the items i to 3 is not more than 55 and not less than 35m m 〇 ', page 27, 200409167 6. Application scope of patent 8 · If the scope of the scope of patent application is circular or oval 9. If the thickness of the end of the side of the part of the scope of patent application is not 10 At 1 · 2 and not less than 1. 〇11 · If the scope of patent application is from the end of the fluorescent screen side to the end of the neck side to the end of the maximum 0 · 8 〇12 · If the application is for a segmented type 13 · If the application is for deflection Magnetic | Ergent 1 4 · If applying for the side of the exclusive side and not less than 7.15, if applying for the special deflection magnetic light 1 6 · If applying for the side of the exclusive side not less than 9.1? Iron core. Profit range Cathode radiation profit range Large internal profit range Cathode radiation profit range Large inner diameter 3 ° Profit range 1至第3項之偏轉磁軛,其中該鐵芯之 1至第3項之偏轉磁軛,其中該鐵芯頸 大於5mm且不小於4mm。 第1至第3項之偏轉磁軛,豆中該鐵芯 頸部側-端之最大厚度,其比值不大 0 第1至第3項之偏轉磁軛,其中該鐵芯 始到鐵心長度1 / 3點之厚度,與該鐵 大厚度其比值不大於1 · 〇且不小於 第1至第3項之偏轉磁車厄,其中該鐵芯 第1至第3項之偏轉磁軛,1中應用該 線管為一監視器。 ’、 第1 3項之偏轉磁軛,其中該鐵芯頸部 與該鐵芯最大厚度之比,^大於1〇·5 f 1至第3項之偏轉磁軛,立中應用該 線管為一彩色電視。 / 5項,偏轉磁軛,其中該鐵芯頸部 “鐵'。最大厚度之比,不大於I2·5 第1或第3項之偏轉磁扼,其中該鐵心 200409167 六、申凊專利範圍 _ 以於鐵芯頸部側-端與摩之間,其 厚度點‘ m:二17項之偏轉磁軛’其中該鐵芯最大 19.如申請專^二5·至 偏轉線圈為一鞍型偏轉線圈員之偏轉磁輕,其中該水平 2 0 ·如申請專利範圍 偏轉線圈為一鞍型偏轉線圈J;之偏轉磁軛,其中該蜜直 2 1 ·如申請專利範圍第1至第3 ^ 偏轉線圈為一環型偏轉線圈員之偏轉磁幸厄,其中該蜜直The deflection yoke of 1 to 3, wherein the deflection yoke of 1 to 3 of the iron core, wherein the core neck is larger than 5 mm and not less than 4 mm. The deflection yoke of items 1 to 3, the maximum thickness of the side-end of the core of the iron core in the bean, the ratio is not large. 0 The deflection yoke of items 1 to 3, where the core starts to the core length 1 / 3 point thickness, the ratio of the thickness to the large iron thickness is not greater than 1 · 〇 and not less than the deflection magnets of items 1 to 3, where the deflection yoke of the iron core items 1 to 3, 1 in Use this conduit as a monitor. '. The deflection yoke of item 13 in which the ratio of the core neck to the maximum thickness of the core is ^ greater than 10.5 f 1 to the deflection yoke of item 3, and the bobbin is used as A color TV. / 5, deflection yoke, in which the core neck is "iron '. The ratio of the maximum thickness is not greater than the deflection yoke in item 1 or 3 of I2 · 5, in which the core is 200409167. Between the side-end of the neck of the iron core and the friction, the thickness point 'm: deflection yoke of item 2 of 17', of which the core is the largest 19. If you apply for a special ^ 2: 5 · until the deflection coil is a saddle deflection The deflection magnetism of the coiler is light, in which the level is 20. If the deflection yoke in the scope of the patent application is a saddle-type deflection yoke J; the deflection yoke in which the honey is straight 2 1; The coil is a deflection magnet of a ring-shaped deflection coiler, where the honey straight 第29頁Page 29
TW092116028A 2002-11-19 2003-06-13 Deflection yoke for cathode ray tube TW200409167A (en)

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