JPS627154B2 - - Google Patents

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Publication number
JPS627154B2
JPS627154B2 JP11901679A JP11901679A JPS627154B2 JP S627154 B2 JPS627154 B2 JP S627154B2 JP 11901679 A JP11901679 A JP 11901679A JP 11901679 A JP11901679 A JP 11901679A JP S627154 B2 JPS627154 B2 JP S627154B2
Authority
JP
Japan
Prior art keywords
porcelain
ceramic
thermal expansion
characteristic element
insulators
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP11901679A
Other languages
Japanese (ja)
Other versions
JPS5645870A (en
Inventor
Yutaka Ogawa
Seiichi Asami
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.)
NGK Insulators Ltd
Original Assignee
NGK Insulators 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 NGK Insulators Ltd filed Critical NGK Insulators Ltd
Priority to JP11901679A priority Critical patent/JPS5645870A/en
Publication of JPS5645870A publication Critical patent/JPS5645870A/en
Publication of JPS627154B2 publication Critical patent/JPS627154B2/ja
Granted legal-status Critical Current

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  • Ceramic Products (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は碍子用磁器の貫通孔内に該碍子用磁器
とは熱膨張係数を異にする酸化亜鉛を主成分とす
るセラミツク特性要素を嵌め込んで低融点ガラス
により一体に固着したセラミツク構造体に関する
ものである。 碍子用磁器の貫通孔内はこれとは熱膨張係数を
異にする酸化亜鉛を主成分とするセラミツク特性
要素を嵌め込んだセラミツク構造体としては、加
熱、冷却時に碍子用磁器とセラミツク特性要素と
の熱膨張係数差によつていずれか一方または双方
が破損するおそれがあるため、例えば両端にベー
ス金具を取付けた碍子用磁器の筒体内にこれとは
熱膨張係数を異にするセラミツク特性要素を適当
数遊嵌し、このセラミツク特性要素を前記ベース
金具に固着された蓋にばねを介して押圧保持させ
るような設計が避雷器のように熱影響を受けるお
それのある機器類に採用されているが、このよう
な構造では気密性が不充分でOリングなどのシー
ル部材を使用した場合でもシール部材の劣化によ
つて長期耐用できず、シール部材を使用すること
なく充分な気密性が確保でき、しかも、熱影響を
受けても破損するおそれがない碍子用磁器の貫通
孔内にこれと熱膨張係数を異にするセラミツク特
性要素を嵌め込んだセラミツク構造体が強く要望
されている。 本発明は前記のような要望に応える目的の下に
完成されたもので、碍子用磁器の貫通孔内に酸化
亜鉛を主成分とするセラミツク特性要素を該碍子
用磁器の貫通孔の開口端面より少なくとも3mm以
上内部に嵌め込んで、碍子用磁器とセラミツク特
性要素の各熱膨張係数の中間もしくは等しい熱膨
張係数の低融点ガラスにより、前記セラミツク特
性要素の熱劣化温度以下の温度で一体に固着した
ことを特徴とするものである。 以下、本発明を図示の避雷器を実施例として詳
細に説明すれば、1は通常の碍子用磁器よりなる
筒体で、その内腔部には酸化亜鉛を主成分とした
セラミツク特性要素が前記碍子用磁器とは熱膨張
係数を異にした酸化亜鉛を主成分とするセラミツ
ク特性要素2が嵌め込まれている。なお、セラミ
ツク特性要素2は碍子用磁器の筒体1の開口端面
3よりも3mm以上の深さに内部に嵌め込まれて熱
膨張係数が該セラミツク特性要素2と前記碍子用
磁器の筒体1の各熱膨張係数の中間にある好まし
くはB2O3−PbO系の低融点ガラス4により碍子
用磁器の筒体1の内面に一体に固着されている。
また、碍子用磁器の筒体1の内腔部にはセラミツ
ク特性要素2を適確に嵌合させるため、開口端面
3より所要長さにわたる拡大孔部5が必要に応じ
形成されている。 このように構成されたものは、碍子用磁器の筒
体1とその内部に嵌め込まれているセラミツク特
性要素2が共にセラミツク製のものであるうえ両
者を一体に固着している低融点ガラス4も広義の
セラミツクに属するもので、全体が無機材質によ
り形成されているので性質が極めて近似している
から、適確に接着一体化されて気密性に優れたも
のとなるうえに三者共絶縁材よりなるために絶縁
性能もよく、しかも、碍子用磁器の筒体1内に嵌
め込まれて低融点ガラス4をもつて一体に固着さ
れているセラミツク特性要素2は碍子用磁器の筒
体1の開口端面3より3mm以上内部にあることに
よつて加熱、冷却が繰り返された場合、該碍子用
磁器の筒体1とは熱膨張係数を異にしているにも
かかわらず碍子用磁器の筒体1およびセラミツク
特性要素2のいずれにも亀裂が生じたり破損する
ことがない。この理由は完全に解明されてはいな
いが、下表に示す実験結果より明らかであつて、
埋め込みがない場合の亀裂が上端部から発生する
ことを考えると、埋め込み構造にすることで碍子
用磁器の筒体1の開口端に接着に関与してない部
分ができるために応力が集中せず、しかも、冷熱
試験において、接着に関与する部分が温度の急変
を受けにくくなるためであると考えられる。次に
本発明の効果を確認するため、それぞれ熱膨張係
数の異なる3種類の碍子用磁器からなる筒体1
と、B2O3〜PbO系の低融点ガラス4を3種類
と、酸化亜鉛を主成分とする直径30mmφ、長さ30
mmのセラミツク特性要素2の1種類を選び、ま
た、碍子用磁器の筒体1の内部に嵌合するセラミ
ツク特性要素2の端面が碍子用磁器の筒体1の開
口端面3よりそれぞれ0mm、3mm、7mm、15mm、
30mm、50mmだけ内部に嵌め込まれるように碍子用
磁器の筒体1の内部に拡大孔部5を形成し、これ
らの組み合わせによる接着実験を行なつた結果、
開口端面3より内部にセラミツク特性要素2が嵌
め込まれている場合にのみ亀裂の発生がないこと
を確認した。なお、碍子用磁器の筒体1とセラミ
ツク特性要素2との接着は低融点ガラスの粉末を
有機質バインダにて懸濁させ、真空脱泡ののちセ
ラミツク特性要素2と碍子用磁器の筒体1との間
隙に流し込んで有機質バインダを乾燥揮散させ、
電気炉中においてセラミツク特性要素2の熱劣化
以下の温度420〜460℃でそれぞれの低融点ガラス
の作業に適した温度で30分間加熱してガラス溶融
させた。このようにして得られたサンプルを全て
90℃の湯の中および20℃の水中に交互に3サイク
ル浸漬する冷熱試験を行い、肉眼ないし実体顕微
鏡でクラツクの有無を確認した。それらの結果を
示せば次の通りである。
The present invention relates to a ceramic structure in which a ceramic characteristic element mainly composed of zinc oxide, which has a different coefficient of thermal expansion from that of the insulator porcelain, is fitted into a through hole of the insulator porcelain and is fixed integrally with a low melting point glass. It is something. The inside of the through-hole of the insulator porcelain is a ceramic structure in which ceramic characteristic elements mainly composed of zinc oxide, which have different coefficients of thermal expansion, are inserted. Because there is a risk of damage to one or both of them due to the difference in their thermal expansion coefficients, for example, if a ceramic characteristic element with a different thermal expansion coefficient is placed inside a porcelain cylinder for insulators with base metal fittings attached to both ends, A design in which a suitable number of ceramic characteristic elements are fitted loosely and held by pressing against a lid fixed to the base metal fitting via a spring has been adopted for equipment such as lightning arresters that may be affected by heat. In such a structure, the airtightness is insufficient, and even if a sealing member such as an O-ring is used, the sealing member deteriorates and cannot be used for a long time, but sufficient airtightness can be secured without using a sealing member, Moreover, there is a strong demand for a ceramic structure in which a ceramic characteristic element having a different coefficient of thermal expansion is fitted into a through hole of porcelain for an insulator, which is not likely to be damaged even when subjected to heat effects. The present invention was completed with the purpose of meeting the above-mentioned demands, and it is possible to insert a ceramic characteristic element containing zinc oxide as a main component into the through hole of the insulator porcelain from the open end surface of the through hole of the insulator porcelain. At least 3 mm or more of the material is fitted inside and fixed together at a temperature below the thermal deterioration temperature of the ceramic characteristic element with a low melting point glass having a coefficient of thermal expansion that is between or equal to the coefficient of thermal expansion of the insulator porcelain and the ceramic characteristic element. It is characterized by this. Hereinafter, the present invention will be described in detail using the illustrated lightning arrester as an example. Reference numeral 1 denotes a cylinder made of ordinary porcelain for insulators, and a ceramic characteristic element mainly composed of zinc oxide is provided in the inner cavity of the insulator. A ceramic characteristic element 2 whose main component is zinc oxide and which has a different coefficient of thermal expansion from that of porcelain is fitted. The ceramic characteristic element 2 is fitted inside the porcelain cylindrical body 1 for insulators to a depth of 3 mm or more beyond the open end surface 3, so that the coefficient of thermal expansion is the same as that of the ceramic characteristic element 2 and the porcelain cylindrical body 1 for insulators. It is integrally fixed to the inner surface of the porcelain cylindrical body 1 for insulators by a low melting point glass 4, preferably of B 2 O 3 --PbO type, which has a coefficient of thermal expansion in between.
Further, in order to fit the ceramic characteristic element 2 properly into the inner cavity of the porcelain cylinder 1 for insulators, an enlarged hole 5 extending a required length from the open end surface 3 is formed as necessary. In this structure, both the insulator porcelain cylinder 1 and the ceramic characteristic element 2 fitted therein are made of ceramic, and the low melting point glass 4 that fixes them together is also used. It belongs to ceramics in a broad sense, and since it is entirely made of inorganic material, its properties are very similar, so it can be bonded together accurately and has excellent airtightness, and it can also be used as an insulating material for all three. The ceramic characteristic element 2, which is fitted into the porcelain cylinder 1 for insulators and fixed together with low melting point glass 4, has good insulation performance due to its structure. When heating and cooling are repeated due to being located 3 mm or more inside the end face 3, the porcelain cylindrical body 1 for insulators has a different coefficient of thermal expansion from the porcelain cylindrical body 1 for insulators. and the ceramic characteristic element 2 does not crack or break. The reason for this is not completely elucidated, but it is clear from the experimental results shown in the table below.
Considering that cracks will occur from the upper end when there is no embedding, by creating a embedding structure, there will be a part at the open end of the porcelain cylinder 1 for insulators that is not involved in adhesion, so stress will not concentrate. Moreover, it is thought that this is because the parts involved in adhesion are less susceptible to sudden changes in temperature during the thermal test. Next, in order to confirm the effects of the present invention, a cylindrical body 1 made of three types of insulator porcelain each having a different coefficient of thermal expansion.
, 3 types of B 2 O 3 -PbO-based low melting point glasses 4, and 30mmφ diameter, 30mm long glass whose main component is zinc oxide.
Select one type of ceramic characteristic element 2 of mm, and also make sure that the end face of the ceramic characteristic element 2 that fits inside the porcelain cylinder 1 for insulator is 0 mm and 3 mm, respectively, from the open end face 3 of the porcelain cylinder 1 for insulator. , 7mm, 15mm,
An enlarged hole 5 was formed inside the porcelain cylinder 1 for insulators so that it could be fitted into the inside by 30 mm and 50 mm, and as a result of adhesion experiments using these combinations, the results were as follows.
It was confirmed that cracks did not occur only when the ceramic characteristic element 2 was fitted inside the opening end face 3. The porcelain cylindrical body 1 for insulators and the ceramic characteristic element 2 are bonded together by suspending low melting point glass powder in an organic binder, and after vacuum degassing, the ceramic characteristic element 2 and the porcelain cylindrical body 1 for insulators are bonded together. Pour into the gap to dry and volatilize the organic binder,
The glass was melted by heating in an electric furnace for 30 minutes at a temperature of 420 to 460 DEG C., below the thermal deterioration of ceramic characteristic element 2, at a temperature suitable for the work of each low melting point glass. All samples obtained in this way
A cold-heat test was performed by immersing the specimen in 90°C hot water and 20°C water alternately for 3 cycles, and the presence or absence of cracks was confirmed with the naked eye or with a stereomicroscope. The results are as follows.

【表】【table】

【表】 すなわち、碍子用磁器の筒体の内部に嵌合した
セラミツク特性要素の埋め込み深さhが0mmのも
のにおいては、低融点ガラスと碍子用磁器の筒体
の各熱膨張係数に近似させても試料Dのように碍
子用磁器に亀裂を生じ、この種の接着は必ずしも
満足できる結果を得られない。この理由としては
筒体を構成する碍子用磁器の熱膨張係数を見掛上
常温から低融点ガラスの固化温度までの温度範囲
において該低融点ガラスの熱膨張係数と合わせて
も、磁器の熱膨張係数が部分的な温度範囲におい
ては磁器中の石英、ムライト、クリストバライト
などの熱膨張挙動のため必ずしも一様ではなく、
接着構造体の内部に応力を生じるためであろうと
考えられる。また、仮に磁器の熱膨張係数が上記
温度範囲において一様であつたとしても、磁器は
通常ガラスマトリツクスと多種の結晶の非平衡反
応系で構成されるので、最初の磁器の焼成条件に
よつて熱膨張係数が変化するため、低融点ガラス
の熱膨張係数に常に統一しておくことは実用上困
難である。これに対し図示するように、セラミツ
ク特性要素2の端部が碍子用磁器の筒体1の開口
端面3よりも内部に嵌め込まれている本発明品す
なわち、埋め込み深さhを3、7、15、30、50mm
としたものについて、それぞれ実験を行つた結果
は表中埋め込み深さ3、7、15、30、50mm欄に示
すような結果を得た。すなわち、碍子用磁器の筒
体1の開口端面3からセラミツク特性要素の端面
までの距離を3mmにすると試料A、Bにおいて亀
裂の発生が見られない。これは埋め込み深さhを
3mm以上確保することによつて碍子用磁器の筒体
1および低融点ガラス4とセラミツク特性要素2
との熱膨張係数の差が25×10-6(/℃)程度であ
れば、碍子用磁器の筒体1ないし低融点ガラス中
に発生する応力による亀裂の発生を防ぐことがで
きることを意味し、また、埋め込み深さhを7mm
以上とする試料C,Dから明らかなように、低融
点ガラス4の熱膨張係数を碍子用磁器の筒体1や
セラミツク特性要素2の熱膨張係数と等しくして
も亀裂の発生を防ぐことができることを意味して
いる。なお、低融点ガラス4の熱膨張係数はいず
れの場合も碍子用磁器とセラミツク特性要素の各
熱膨張係数の中間にあるものを使用して碍子用磁
器およびセラミツク特性要素に近似させておくこ
とが大切である。このように碍子用磁器とセラミ
ツク特性要素を嵌合する低融点ガラスの熱膨張係
数を両者の熱膨張係数の中間もしくは等しい値を
取らせることにより、セラミツク構造体が急激に
加熱あるいは冷却された際の熱応力による破壊が
防止できる。即ち、碍子用磁器とセラミツク特性
要素の熱膨張係数が異なる場合には、急熱、急冷
により熱膨張係数の差に応じた熱応力が両者の境
界に発生し、その値が材料の強度を越えれば破壊
に至こととなるのであるが、本発明においては低
融点ガラスの熱膨張係数を両者の熱膨張係数の中
間もしくは等しい値を取らせたので、低融点ガラ
スの層が緩衝層として作用して碍子用磁器とセラ
ミツク特性要素との間に生ずる熱応力を引き下げ
ることができることとなる。なお、碍子用磁器の
筒体1は有襞、無襞を問わないことは勿論であ
る。このようにして得られたセラミツク構造体に
ついてヘリウムガスの透過試験を実施したところ
いずれも4×10-10atm・c.c./sec以下の透過値で
機密性が充分確保されたものであつた。 本発明は前記説明によつて明らかなように、碍
子用磁器の貫通孔内に酸化亜鉛を主成分とするセ
ラミツク特性要素を該貫通孔の開口端面より内部
に嵌め込まれたものとして碍子用磁器とセラミツ
ク特性要素の各熱膨張係数の中間もしくは等しい
熱膨張係数の低融点ガラスにより一体化してあつ
て、温度の急変を受け易い開口側部分を接着に関
与させず応力的に自由な状態としてあるから、加
熱、冷却によつても亀裂の発生がなく、しかも、
碍子用磁器とセラミツク特性要素間の間隙に低融
点ガラスを注入する作業も容易となり、事後にお
いてセラミツク特性要素を導通処理する場合にも
セラミツク特性要素の上部の空間が有効なものと
なり、高い気密性と接着部分の長期的な電気絶縁
性が要求される碍子機器たとえば、ギヤツプレス
避雷器やコンデンサー碍子等に広く応用できる基
本のセラミツク構造体としてその用途は大きく、
産業の発達に寄与するところ大なものである。
[Table] In other words, when the embedding depth h of the ceramic characteristic element fitted inside the porcelain cylinder for insulators is 0 mm, the thermal expansion coefficients of the low melting point glass and the porcelain cylinder for insulators are approximated. However, as in Sample D, cracks occur in the insulator porcelain, and this type of adhesion does not necessarily yield satisfactory results. The reason for this is that the coefficient of thermal expansion of the porcelain for insulators constituting the cylinder apparently exceeds the coefficient of thermal expansion of the porcelain in the temperature range from room temperature to the solidification temperature of the low-melting point glass. The coefficient is not necessarily uniform in a partial temperature range due to the thermal expansion behavior of quartz, mullite, cristobalite, etc. in porcelain.
It is thought that this is because stress is generated inside the adhesive structure. Furthermore, even if the coefficient of thermal expansion of porcelain is uniform in the above temperature range, porcelain is usually composed of a non-equilibrium reaction system of a glass matrix and various types of crystals, so it depends on the initial firing conditions of porcelain. Since the coefficient of thermal expansion changes over time, it is practically difficult to always keep the coefficient of thermal expansion consistent with that of low-melting glass. On the other hand, as shown in the figure, in the case of the present invention in which the end of the ceramic characteristic element 2 is fitted inside the open end surface 3 of the porcelain cylinder 1 for insulators, the embedding depth h is 3, 7, 15. ,30,50mm
The results of experiments conducted for each of these were obtained as shown in the embedding depth 3, 7, 15, 30, and 50 mm columns in the table. That is, when the distance from the open end surface 3 of the porcelain insulator cylinder 1 to the end surface of the ceramic characteristic element is set to 3 mm, no cracks are observed in samples A and B. By ensuring an embedding depth h of 3 mm or more, the insulator porcelain cylinder 1, low melting point glass 4, and ceramic characteristic element 2 can be assembled.
If the difference in the coefficient of thermal expansion between the two and , and the embedding depth h is 7 mm.
As is clear from the above samples C and D, cracks cannot be prevented even if the coefficient of thermal expansion of the low-melting glass 4 is made equal to the coefficient of thermal expansion of the porcelain cylinder 1 for insulators or the ceramic characteristic element 2. It means that you can. In any case, the coefficient of thermal expansion of the low melting point glass 4 can be approximated to the characteristic elements of porcelain for insulators and ceramic by using a value that is between the coefficients of thermal expansion of each of the characteristic elements of porcelain for insulators and ceramic characteristic elements. It's important. In this way, by making the thermal expansion coefficient of the low melting point glass that fits the insulator porcelain and the ceramic characteristic element take a value that is between or equal to the thermal expansion coefficient of both, it is possible to prevent the ceramic structure from heating or cooling rapidly. Destruction due to thermal stress can be prevented. In other words, if the thermal expansion coefficients of insulator porcelain and ceramic characteristic elements are different, thermal stress corresponding to the difference in thermal expansion coefficient will be generated at the boundary between the two due to rapid heating and cooling, and the value will exceed the strength of the material. However, in the present invention, the coefficient of thermal expansion of the low melting point glass is set to a value that is between or equal to the coefficients of thermal expansion of both, so that the layer of low melting point glass acts as a buffer layer. As a result, the thermal stress generated between the insulator porcelain and the ceramic characteristic element can be reduced. It goes without saying that the porcelain cylinder 1 for insulators may be pleated or non-pleated. When a helium gas permeation test was carried out on the ceramic structures thus obtained, all of them had a permeation value of 4×10 -10 atm·cc/sec or less, and airtightness was sufficiently ensured. As is clear from the above description, the present invention is a porcelain for insulators in which a ceramic characteristic element containing zinc oxide as a main component is fitted into a through hole of the porcelain for insulators from the open end surface of the through hole. It is integrated with low-melting glass having a coefficient of thermal expansion that is between or equal to the coefficients of thermal expansion of the ceramic characteristic elements, and the opening side part, which is susceptible to sudden changes in temperature, is not involved in adhesion and is in a stress-free state. No cracks occur even when heated or cooled, and
It becomes easier to inject low-melting glass into the gap between the insulator porcelain and the ceramic characteristic element, and the space above the ceramic characteristic element becomes effective even when conducting conduction treatment on the ceramic characteristic element afterwards, resulting in high airtightness. It is widely used as a basic ceramic structure that can be widely applied to insulator devices that require long-term electrical insulation properties of the bonded parts, such as gear press lightning arresters and capacitor insulators.
It is a major contribution to the development of industry.

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

図面は本発明の実施例を示す一部切欠正面図で
ある。 1:碍子用磁器の筒体、2:セラミツク特性要
素、3:開口端面、4:低融点ガラス。
The drawing is a partially cutaway front view showing an embodiment of the present invention. 1: Porcelain cylinder for insulator, 2: Ceramic characteristic element, 3: Open end surface, 4: Low melting point glass.

Claims (1)

【特許請求の範囲】 1 碍子用磁器の貫通孔内に酸化亜鉛を主成分と
するセラミツク特性要素を該碍子用磁器の貫通孔
の開口端面より少なくとも3mm以上内部に嵌め込
んで、碍子用磁器とセラミツク特性要素の各熱膨
張係数の中間もしくは等しい熱膨張係数の低融点
ガラスにより、前記セラミツク特性要素の熱劣化
温度以下の温度で一体に固着したことを特徴とす
るセラミツク構造体。 2 低融点ガラスがB2O3−PbO系ガラスである
特許請求の範囲第1項記載のセラミツク構造体。
[Scope of Claims] 1. A ceramic characteristic element containing zinc oxide as a main component is inserted into a through-hole of the insulator porcelain at least 3 mm or more from the open end surface of the through-hole of the insulator porcelain, and the insulator porcelain is A ceramic structure characterized in that the ceramic characteristic elements are fixed together at a temperature below the thermal deterioration temperature of the ceramic characteristic elements by a low melting point glass having a thermal expansion coefficient intermediate or equal to each of the ceramic characteristic elements. 2. The ceramic structure according to claim 1, wherein the low melting point glass is a B2O3 - PbO glass.
JP11901679A 1979-09-17 1979-09-17 Ceramic structure mounted in ceramic cylindrical body with ceramic member having diffrent coefficient of thermal expansion Granted JPS5645870A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11901679A JPS5645870A (en) 1979-09-17 1979-09-17 Ceramic structure mounted in ceramic cylindrical body with ceramic member having diffrent coefficient of thermal expansion

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11901679A JPS5645870A (en) 1979-09-17 1979-09-17 Ceramic structure mounted in ceramic cylindrical body with ceramic member having diffrent coefficient of thermal expansion

Publications (2)

Publication Number Publication Date
JPS5645870A JPS5645870A (en) 1981-04-25
JPS627154B2 true JPS627154B2 (en) 1987-02-16

Family

ID=14750894

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11901679A Granted JPS5645870A (en) 1979-09-17 1979-09-17 Ceramic structure mounted in ceramic cylindrical body with ceramic member having diffrent coefficient of thermal expansion

Country Status (1)

Country Link
JP (1) JPS5645870A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5832038A (en) * 1981-08-14 1983-02-24 Hoya Corp Alkali-free glass for photoetching mask
JPS61141642A (en) * 1984-12-12 1986-06-28 Toshiba Glass Co Ltd Wear-resistant glass bead
JPS62243272A (en) * 1986-04-16 1987-10-23 中部電力株式会社 Arrestor
JPH0218366A (en) * 1988-07-02 1990-01-22 Ig Tech Res Inc Laminated ceramic panel

Also Published As

Publication number Publication date
JPS5645870A (en) 1981-04-25

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