JPS6237842A - Indirectly-heated cathode heater - Google Patents

Indirectly-heated cathode heater

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Publication number
JPS6237842A
JPS6237842A JP60177411A JP17741185A JPS6237842A JP S6237842 A JPS6237842 A JP S6237842A JP 60177411 A JP60177411 A JP 60177411A JP 17741185 A JP17741185 A JP 17741185A JP S6237842 A JPS6237842 A JP S6237842A
Authority
JP
Japan
Prior art keywords
alumina
particles
purity
particle size
sintered
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.)
Granted
Application number
JP60177411A
Other languages
Japanese (ja)
Other versions
JPH0654633B2 (en
Inventor
Toshiaki Arato
利昭 荒戸
Kosuke Nakamura
浩介 中村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP60177411A priority Critical patent/JPH0654633B2/en
Publication of JPS6237842A publication Critical patent/JPS6237842A/en
Publication of JPH0654633B2 publication Critical patent/JPH0654633B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To enhance the withstanding properties against voltage and thermal stress, by coating the surface of a tungsten coil with a sintered alumina material in which high-purity spherical alumina grains having two prescribed different diameters are contained at a prescribed ratio. CONSTITUTION:100 weight parts of high-purity alumina grains, which are made spherical by a hydrothermal crystallization method or the like and have a mean diameter of 1-5mum, and weight parts of high-purity alumina grains, which are made spherical by the method or the like and have a mean diameter equal to 1/10-1/20 of that of the former, are mixed together. A sintered alumina material in which the alumina grains are contained at a filling ratio of 50-70% is manufactured to coat a tungsten coil. Even if the sintered alumina material is repeatedly heated to a temperature of 1,600 deg.C or more, the thermal stress thereof is reduced and the high-purity alumina grains are unlikely to excessively diffuse. Therefore, the generation of a crack in the sintered alumina material at the time of heating thereof is suppressed. The withstanding properties against voltage and thermal stress are thus enhanced.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は傍熱型陰極ヒータ(例えばブラウン管の)に係
)、特にヒータt−構成するタングステンコイル表面の
アルミナ焼結被覆体を改良した傍熱型陰極ヒータに関す
る。
Detailed Description of the Invention [Field of Application of the Invention] The present invention relates to an indirectly heated cathode heater (for example, for a cathode ray tube), and particularly to an indirectly heated cathode heater (for example, for a cathode ray tube), in which an improved alumina sintered coating on the surface of a tungsten coil constituting the heater T is used. The present invention relates to type cathode heaters.

〔発明の背景〕[Background of the invention]

従来の例えばブラウン管の傍熱型陰極用のヒータは、通
常タングステン素線全ヒータとし、その表面にアルミナ
を主成分とする電気絶縁用の焼結被覆材を施して形成さ
れているが、ブラウン管の性能向上のために陰極を最高
約1000℃以上に加熱する必要がアリ、このためタン
グステンヒータ自体は1600℃乃至1800℃に加熱
される必要がある。しかしこのことによって、ヒータ表
層部に熱応力負荷が発生し、焼結被覆材であるアルミナ
にクラックが発生、伝播する結果、アルミナ層が剥離し
、ヒータとヒータカバーとの接触がおこシ、絶縁不良を
起すという現象がめった。公知例(%開開57−433
37 、同55−41694 ’)では、ヒータのコイ
ル各部位に粒径および粒径分布の異なるアルミナ粒子を
被覆し、熱応力を緩和する方法を採るとしており、50
0メツシ瓢と900メツシエの混合されたアル建すを使
用することが開示されているが、アルミナの粒径が大き
すぎ且つ破砕粒を用いているために適正な充填率の範囲
に制御することができず、耐電圧のより更なる向上がで
きないという問題があった。
Conventional heaters for the indirectly heated cathodes of cathode ray tubes, for example, are usually made entirely of tungsten wire, and the surface is coated with a sintered coating material mainly composed of alumina for electrical insulation. In order to improve performance, it is necessary to heat the cathode to a maximum of about 1000°C or higher, and therefore the tungsten heater itself needs to be heated to 1600°C to 1800°C. However, this causes a thermal stress load on the surface layer of the heater, which causes cracks to occur and propagate in the alumina sintered covering material, causing the alumina layer to peel off, causing contact between the heater and the heater cover, and causing insulation. The phenomenon of causing defects is rare. Known example (% opening 57-433
37, 55-41694'), a method is adopted in which each part of the heater coil is coated with alumina particles having different particle sizes and particle size distributions to alleviate thermal stress.
It has been disclosed to use a mixture of 0 and 900 mesh alumina, but since the particle size of alumina is too large and crushed grains are used, it is difficult to control the filling rate within an appropriate range. There was a problem in that the withstand voltage could not be further improved.

〔発明の目的〕[Purpose of the invention]

従って本発明の目的は、傍熱型陰極ヒータ表面を被覆す
る絶縁材としてのアルZす焼結体の耐電圧特性および耐
熱応力負荷特性を同上させた傍熱型陰極ヒータを提供す
ることにある。
Therefore, an object of the present invention is to provide an indirectly heated cathode heater in which the dielectric strength characteristics and thermal stress load characteristics of the AlZ sintered body as an insulating material covering the surface of the indirectly heated cathode heater are improved. .

〔発明の概要〕[Summary of the invention]

本発明の特徴は、上記目的を達成するために、傍熱型陰
極ヒータのタングステンコイル表面に高純度の球状アル
tす粒子を用い、アルミナ粒子の充填率を50〜70チ
の範囲に制御するとともに粒子間隙が均一になる′よう
にし友アルミナ焼結被覆体で被覆したことにある。
In order to achieve the above object, the present invention is characterized by using high-purity spherical aluminum particles on the surface of the tungsten coil of an indirect cathode heater, and controlling the filling rate of the alumina particles in the range of 50 to 70 particles. At the same time, the particles were coated with a sintered alumina coating to ensure uniform particle gaps.

〔発明の実施例〕[Embodiments of the invention]

第1図は本発明の一実施例による傍熱型陰極用ヒータ表
面のアルミナ被覆層(焼結前)の横断面の走査電子顕微
鏡による観察像を模式図的に示したものである。
FIG. 1 schematically shows an image observed by a scanning electron microscope of a cross section of an alumina coating layer (before sintering) on the surface of an indirectly heated cathode heater according to an embodiment of the present invention.

本実施例においては上記アルミナ被覆層を構成するアル
ミナには(1)平均粒径2,0μm s (2)平均粒
径0.2μmの2種類の平均粒径の高純度アルきす粒子
を使用した。(1)及び(2)の各粒子はいずれもほぼ
球状を呈しているものを用いた。粒子配合の割合は重量
比で上記(1)の粒子が100に対して(2)の粒子が
10の割合にした0上記配合比は、平均粒径の大きい(
1)のアルミナ粒子を稠密六方状に充填すると仮定した
時、その空隙中に平均粒径の小さい(2)のアルミナ粒
子が充填される時の、充填率に等しい。このような配合
にした理由は、アルミナをタングステン表面に被覆する
際の充填率を後記の如く50〜70チの範囲にすること
におる。そうして、そのような結果を得るために、上記
(1)及び(2)のアルミナ粒子を十分に混合、分散さ
せ友アルコール溶液を使用し、電気泳動法でタングステ
ン素線の表面にアルミナ粒子を被覆させた。その結果、
第1図に示した如く平均粒径2.0μmのアルミナ粒子
1の相互間隙に平均粒径0,2μmのアル2す粒子2が
侵入し友様な配列を得た。
In this example, the alumina constituting the alumina coating layer was made of high-purity alkylene particles with two types of average particle sizes: (1) average particle size of 2.0 μm s, and (2) average particle size of 0.2 μm. . The particles (1) and (2) were each approximately spherical. The ratio of the particles is 100 by weight of the particles of (1) and 10 of the particles of (2).
Assuming that the alumina particles of 1) are packed in a dense hexagonal shape, it is equal to the filling rate when the alumina particles of (2) with a small average particle size are filled into the voids. The reason for this combination is that the filling rate when coating the tungsten surface with alumina is in the range of 50 to 70 inches as described later. In order to obtain such a result, the alumina particles in (1) and (2) above are thoroughly mixed and dispersed, and alumina particles are applied to the surface of a tungsten wire using an electrophoretic method using an alcoholic solution. was coated. the result,
As shown in FIG. 1, Al2 particles 2 with an average particle size of 0.2 μm entered the gaps between the alumina particles 1 with an average particle size of 2.0 μm, resulting in a friendly arrangement.

以上のようにして形成したアルミナ被覆全焼結し友。こ
のアルミナ焼結体表面に出現するクラック数およびクラ
ック長さは、本実施例の場合と、(1)平均粒赫2.θ
μ・もしくけ(2)平均粒径0.2β・のアルミナ粒子
を単独で使用した場合とを比べてみると、第2図に示す
如くであった口 すなわち、第2図はアル之す被覆を1600℃で1時間
、水素気流中で焼結して得た傍熱型陰極ヒータ表面のア
ルミナ焼結被覆層表面の顕微鏡観察より調べた結果を示
す、縦軸は100μm平方の視野の中で観察されたクラ
ック長の平均値、横軸は同じく平均クラック数を示す。
The alumina-coated fully sintered friend formed as described above. The number of cracks and the crack length appearing on the surface of this alumina sintered body are as follows: (1) average grain size, 2. θ
μ・Moshikke (2) When comparing the case where alumina particles with an average particle size of 0.2β・ were used alone, the results were as shown in Figure 2. The vertical axis shows the results of microscopic observation of the alumina sintered coating layer surface on the surface of an indirectly heated cathode heater obtained by sintering at 1600°C for 1 hour in a hydrogen stream. The average value of the observed crack lengths, and the horizontal axis also shows the average number of cracks.

図中のカーブAは、平均粒径2.0μmのアルミナ粒子
だけを被覆焼結してなる焼結体、カーブBは同0.2μ
mのアルミナ粒子だけを被覆焼結してなる焼結体、カー
ブCは本実施例により粒径2,0μmと0.2μmの粒
子の混合比’Ito:tとした混合粒子を被覆焼結して
なる焼結体に関する結果である。 ゛ 本実施例によれば、単位面積当りのクラック数は平均粒
径0.2μmのアルミナ粒子を焼結被覆してなる焼結体
より条目であるが、全体的にクラ□ツク長が短く、有利
性が認められる。
Curve A in the figure is a sintered body made by coating and sintering only alumina particles with an average particle size of 2.0 μm, and curve B is the same 0.2 μm.
Curve C, which is a sintered body formed by coating and sintering only alumina particles of m, is obtained by coating and sintering mixed particles with a mixture ratio of particles of 2.0 μm and 0.2 μm at a mixing ratio of 'Ito:t' according to this example. These results relate to a sintered body made of゛According to this example, the number of cracks per unit area is more streaky than the sintered body formed by sintering and coating alumina particles with an average particle size of 0.2 μm, but overall the crack length is shorter, Advantages are recognized.

本発明の他の実施例として、■平均粒径4.5一合して
前記と同様の仕方でアル建す焼結体を作成し、また■平
均粒径1.5岸 粒子を混合比10/1で混合してアルiす焼結体を同じ
く作成した。用いた粒子はいずれも球形高純度アルミナ
粒子である。これらのアルミナ焼結被覆体について前記
と同様に試験を行い、第2図と同様の整理をした結果、
第3図を得た。なお第3図には第2図の内容も併せ示し
て套る。この図によっても本発明の有効性が認められる
As another example of the present invention, (1) a sintered body was prepared by combining particles with an average particle size of 4.5 in the same manner as described above, and (2) mixing particles with an average particle size of 1.5 at a mixing ratio of 10. An aluminum sintered body was also prepared by mixing the mixture at a ratio of 1/1. The particles used were all spherical high-purity alumina particles. These alumina sintered coatings were tested in the same manner as above, and the results were arranged in the same way as shown in Figure 2.
Figure 3 was obtained. Note that FIG. 3 also shows the contents of FIG. 2. This figure also confirms the effectiveness of the present invention.

なお、用いた高純度アルミナの純度は、原料粉において
Na o<o. 0 1 % 、8102<0.0 1
 ’1 。
In addition, the purity of the high-purity alumina used is Na<o. 0 1%, 8102<0.0 1
'1.

F・20,<0.001%、その他の不純物成分濃度は
痕跡以下であった。tた同アルミナを使用して作成した
アル電す被覆の分析結果は、焼成後の値がNazOは痕
跡程度、8102= 0. 0 2 % 、 Fe12
, −0、005% 、 Mg0=0、008チという
値であった。ここでMgOは、泳動液に電解質成分とし
て添加したMg(NOIS)、にもとづくものである。
F.20, <0.001%, and the concentration of other impurity components was less than a trace. The analysis results of the aluminum coating made using the same alumina showed that the value after firing was only a trace of NazO, 8102 = 0. 02%, Fe12
, -0,005%, Mg0=0,008chi. Here, MgO is based on Mg (NOIS) added to the electrophoresis solution as an electrolyte component.

本発明において高純度アルミナが望まれるのは第4図に
示す通シでおる。第4図は不純物のS tO2に注目し
、At20.100部に対して混合した5102の割合
とヒートサイクル試験5000時間経過後のヒータ破断
率との関係を示したものである。
In the present invention, high purity alumina is desired as shown in FIG. FIG. 4 focuses on the impurity S tO2 and shows the relationship between the ratio of 5102 mixed to 20.100 parts of At and the heater breakage rate after 5000 hours of heat cycle test.

なお、球形アルミナ粒子は「水熱結晶化法」で製造する
ことができる。「水熱結晶化法」とは、高温高圧下のH
2Oの存在のもとでゾル−ダル等の非晶質物質を結晶化
させ、結晶質物質を得る方法である。同法によシ製造さ
れ九粒子の特徴は■微粒である、■よく発達した結晶質
である、■粒度分布の幅が狭い、■歪が少ない、■比較
的低温で作成できる、等である。
Note that spherical alumina particles can be produced by a "hydrothermal crystallization method." “Hydrothermal crystallization method” refers to H
This is a method of crystallizing an amorphous material such as Zoldal in the presence of 2O to obtain a crystalline material. The characteristics of the nine particles produced by the same method are: ■ Fine grains, ■ Well-developed crystallinity, ■ Narrow particle size distribution, ■ Little distortion, ■ Can be produced at relatively low temperatures, etc. .

第5図は絶縁用アルさす焼結体のアルミナ膜厚に対する
アルミナ充填率の関係、および第6図は同じくアルミナ
膜厚に対する耐電圧の関係である。
FIG. 5 shows the relationship between the alumina filling rate and the alumina film thickness of a sintered body made of insulating aluminum, and FIG. 6 similarly shows the relationship between the withstand voltage and the alumina film thickness.

これら図における各記号で示す各点のデータは次の表の
通りである。
The data at each point indicated by each symbol in these figures is as shown in the following table.

これら図からアルミナ充填率が50−以下ならば耐電圧
は充分に高くならず、また逆にアルミナ粒子の充填率が
70−以上に達すると、ヒータ加熱時にクラックが発生
して、やはシ耐電圧が低下することがわかる。従って高
耐電圧を維持し、かつクラック発生を抑えるためKはア
ルミナ粒子の充填率を50乃至70チの範囲にする必要
のおることがわかる。ちなみに先述の公知例にみられる
900メツシエ(平均粒径3.5μm)と500メツシ
&C平均粒径6μm)の破砕アルミナ粒子混合被覆の場
合、アル建す充填率は図示の如く50チに到達せず、従
って耐電圧が満足すべき値に達しなか−) fl−@ 〔発明の効果〕 本発明によれば、従来のアルミナ焼結体(例えば500
メツシ孤および90.0メツシ凰粒径の破砕アル電す粒
子からなる焼結体)に比べ、アル建す充填率が適正な範
囲にあシ、このことは1600℃以上に繰り返し加熱さ
れる際の熱膨張に対して熱応力負荷を緩和する方向に作
用し、また、高純度アル建す粒子を用いたことによシ、
粒子間での過度の相互拡散が進行しに<<、繰り返し加
熱嘔れた際に発生するクラック長および数を抑制するこ
とができ、これらの総合効果として傍熱型陰極ヒータの
耐電圧を従来より一層向上させることができる。
From these figures, if the alumina filling rate is less than 50-, the withstand voltage will not be high enough, and conversely, if the alumina particle filling rate reaches 70- or more, cracks will occur during heating with the heater, and the withstand voltage will not be high enough. It can be seen that the voltage decreases. Therefore, it can be seen that in order to maintain a high withstand voltage and suppress the occurrence of cracks, it is necessary to set the filling rate of alumina particles in the range of 50 to 70 inches. By the way, in the case of a mixed coating of crushed alumina particles of 900 mesh (average particle size 3.5 μm) and 500 mesh & C (average particle size 6 μm) seen in the previously mentioned known example, the filling rate of the aluminum can reach 50 mesh as shown in the figure. [Effects of the Invention] According to the present invention, the conventional alumina sintered body (for example, 500
Compared to the sintered body made of crushed aluminized particles with a grain size of 90.0 and 90.0, the filling rate of alumina is within an appropriate range, which means that when repeatedly heated to 1600°C or higher, It acts in the direction of relieving the thermal stress load against the thermal expansion of
It is possible to suppress the length and number of cracks that occur due to repeated heating due to excessive interdiffusion between particles, and the overall effect of these is to lower the withstand voltage of indirect cathode heaters to a level higher than that of conventional cathode heaters. This can be further improved.

【図面の簡単な説明】 第1図は本発明の実施例によるタングステンコイル表面
に被覆した高純度アルミナ粒子の被覆状況を表わした縦
断面模式図、第2図、第3図はアル電す焼結体のクラッ
ク長とクラック数の関係を示す実験結果の図、第4図は
不純物たる810□の含有量とヒータ破断率の関係を示
す実験図、第5図はアルミナ焼結体のアルミナ膜厚とア
ルiす充填率の関係を示す実験結果の図、第6図は同じ
くアルミナ膜厚と耐電圧との関係を示す実験結果の図で
ある。 1・・・平均粒径2.0μmのアルミナ粒子2・・・平
均粒径0.2μmのアルミナ粒子3・・・タングステン
表面 ′aC’=θb (%)事項1「に−1
[Brief explanation of the drawings] Fig. 1 is a schematic vertical cross-sectional view showing the state of coating of high-purity alumina particles on the surface of a tungsten coil according to an embodiment of the present invention, and Figs. Figure 4 is an experimental diagram showing the relationship between the crack length and number of cracks in the compact. Figure 4 is an experimental diagram showing the relationship between the content of 810□ as an impurity and the heater rupture rate. Figure 5 is the alumina film of the alumina sintered body. FIG. 6 is a diagram of experimental results showing the relationship between thickness and aluminum filling rate, and FIG. 6 is a diagram of experimental results showing the relationship between alumina film thickness and withstand voltage. 1... Alumina particles with an average particle size of 2.0 μm 2... Alumina particles with an average particle size of 0.2 μm 3... Tungsten surface 'aC' = θb (%) Item 1 "-1

Claims (2)

【特許請求の範囲】[Claims] (1)球状を呈する高純度アルミナ粒子よりなる充填率
50%以上70%以下のアルミナ焼結体でタングステン
コイル表面が被覆されていることを特徴とする傍熱型陰
極ヒータ。
(1) An indirectly heated cathode heater characterized in that the surface of a tungsten coil is covered with an alumina sintered body made of spherical high-purity alumina particles with a filling rate of 50% to 70%.
(2)前記アルミナ粒子は、1μm以上5μm以下の平
均粒径を持つ粒子と、上記平均粒径の1/10ないし1
/20の平均粒径を持つ粒子との二種類の粒子の混合か
らなる特許請求の範囲第1項記載の傍熱型陰極ヒータ。
(2) The alumina particles have an average particle size of 1 μm or more and 5 μm or less, and 1/10 to 1/10 of the above average particle size.
2. The indirectly heated cathode heater according to claim 1, comprising a mixture of two types of particles: particles having an average particle size of /20.
JP60177411A 1985-08-12 1985-08-12 Indirect heating type cathode heater Expired - Lifetime JPH0654633B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60177411A JPH0654633B2 (en) 1985-08-12 1985-08-12 Indirect heating type cathode heater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60177411A JPH0654633B2 (en) 1985-08-12 1985-08-12 Indirect heating type cathode heater

Publications (2)

Publication Number Publication Date
JPS6237842A true JPS6237842A (en) 1987-02-18
JPH0654633B2 JPH0654633B2 (en) 1994-07-20

Family

ID=16030454

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60177411A Expired - Lifetime JPH0654633B2 (en) 1985-08-12 1985-08-12 Indirect heating type cathode heater

Country Status (1)

Country Link
JP (1) JPH0654633B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02181337A (en) * 1988-12-29 1990-07-16 Hitachi Ltd cathode ray tube heater
US6294065B1 (en) 1997-12-19 2001-09-25 Matsushita Electric Industrial Co., Ltd. Methods of manufacturing heater and cathode-ray tube comprising the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02181337A (en) * 1988-12-29 1990-07-16 Hitachi Ltd cathode ray tube heater
US6294065B1 (en) 1997-12-19 2001-09-25 Matsushita Electric Industrial Co., Ltd. Methods of manufacturing heater and cathode-ray tube comprising the same

Also Published As

Publication number Publication date
JPH0654633B2 (en) 1994-07-20

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