JPS5967606A - Method of producing nonlinear resistor - Google Patents

Method of producing nonlinear resistor

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Publication number
JPS5967606A
JPS5967606A JP57177631A JP17763182A JPS5967606A JP S5967606 A JPS5967606 A JP S5967606A JP 57177631 A JP57177631 A JP 57177631A JP 17763182 A JP17763182 A JP 17763182A JP S5967606 A JPS5967606 A JP S5967606A
Authority
JP
Japan
Prior art keywords
nonlinear resistor
time
resistor
present
linear
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP57177631A
Other languages
Japanese (ja)
Inventor
東畑 孝二
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP57177631A priority Critical patent/JPS5967606A/en
Publication of JPS5967606A publication Critical patent/JPS5967606A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、特に電気系統における過電圧保護装置に使用
される非直線抵抗体の製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a method of manufacturing a nonlinear resistor used particularly in an overvoltage protection device in an electrical system.

〔発明の技術的背景と問題点〕[Technical background and problems of the invention]

電気系統において、正常な電圧(二重畳される過電圧を
除去し、電気系統や電気機器を保砕するため、サージア
プソ」パ及び避雷器などの過電圧保護装置が用いられる
In electrical systems, overvoltage protection devices such as surge absorbers and lightning arresters are used to remove normal voltage (double overvoltage) and protect electrical systems and electrical equipment.

この過電圧保護装置には、正常な電圧ではほぼ絶縁特性
を示し、過電圧が印加されたときには比較的低抵抗値に
なる非直線抵抗体が用いられる。
This overvoltage protection device uses a non-linear resistor that exhibits almost insulating properties at normal voltage and has a relatively low resistance value when overvoltage is applied.

非直線抵抗体は炭化けい素(8iC)若しくは酸化亜鉛
(ZnO)に金属酸化物を混合した素材をプレスして成
形し、焼成して造られる。
The non-linear resistor is made by pressing and molding a material made of silicon carbide (8iC) or zinc oxide (ZnO) mixed with a metal oxide, and firing the material.

ZnO系の非直線抵抗体は、小電流域における非直線特
性が急I唆で、かつ、大電流域に到るまで鋭い立ち上り
をもつため、SiC系の非直線抵抗体を用いた過電圧保
護装置よりもすぐれた過電圧保護装置を作ることができ
る。
ZnO-based non-linear resistors have sharp non-linear characteristics in small current ranges and have a sharp rise up to large current ranges, so overvoltage protection devices using SiC-based non-linear resistors are recommended. You can make a better overvoltage protection device than this.

しかし、従来のZnO系の非直線抵抗体は、常時課電電
圧に対する漏洩゛磁流の増加が大きく、かつ衝撃電流に
よる′幅圧降下が大きい。従って長期間にわたって雷パ
ルスや電圧サージパルスを受ける過電圧保護装置には不
適当であり、長期間にわたって安定した電気特性、即ち
寿命特性を有する非直線抵抗体が要望されていた。
However, in the conventional ZnO-based nonlinear resistor, the leakage magnetic current increases greatly with respect to the constantly applied voltage, and the width pressure drop due to the impact current increases. Therefore, it is unsuitable for an overvoltage protection device that is subjected to lightning pulses or voltage surge pulses over a long period of time, and there has been a demand for a nonlinear resistor that has stable electrical characteristics over a long period of time, that is, has long life characteristics.

〔発明の目的〕[Purpose of the invention]

本発明は上記要望に鑑みなされたもので、長期間にわた
って安定した電気特性、即ち寿命特性を有する非直線抵
抗体の製造方法を提供することを目的とする。
The present invention was made in view of the above-mentioned needs, and an object of the present invention is to provide a method for manufacturing a nonlinear resistor having stable electrical characteristics over a long period of time, that is, long life characteristics.

〔発明の概要〕[Summary of the invention]

かかる目的を達成するために、本発明では酸化亜鉛を主
成分とする金属酸化物を混合成形した後焼成する非直線
抵抗体の製造方法において、前記焼成した非直線抵抗素
体に一定時間の課電エージングを行い、且つ、一定時間
の課電エージングは非直線抵抗体の初期漏洩電流が減少
した後一定値をその特徴とする。
In order to achieve such an object, the present invention provides a method for manufacturing a non-linear resistor in which a metal oxide containing zinc oxide as a main component is mixed and molded, and then fired. Electrical aging is performed, and the aging for a certain period of time is characterized by a constant value after the initial leakage current of the nonlinear resistor decreases.

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

以下、本発明を実施例に基づいて説明する。 Hereinafter, the present invention will be explained based on examples.

主成分である酸化亜鉛(ZnO)の粉末(二酸化ビスマ
ス(”yes) +酸化アンチモン(sb、Os) 、
酸化クロム(Crtos) 、酸化コバルト(C00)
及ヒ酸化マンガン(MnO)等の粉末をそれぞれ0.0
1〜60モル係の範囲で添加し、ボールミルで混合する
。このとき酸化物と有機結合剤例えばポリビニルアルコ
ールとを同時に混合する。このようにしてイHられた混
合物を乾燥造粒装置、例えばスプレードライヤーに入れ
、球状団粒にする。この粉末状混合物をプレスにかけ、
例えば直径IQQ7M、厚さ25iaの円板に成形する
。その後、l000〜1400℃で暁成し、得られた焼
結体の表面を研磨した後、アルミニウム電極を溶射して
非直線抵抗体を形成する。このようにして形成された非
直線抵抗体に例えば、周囲温度90’G、課71率(印
加電圧波高値とバリスタ市川V、mAの比)85%で、
一定時間課小、し、温度及び′lh圧ストストレスえ、
課電エージングを行なう。温度及び゛電圧ストレスを加
える時間(課電時間)は、非直線抵抗体の漏洩電流の変
化を測定して決定する。第1図は、上記実施例に於ける
非直線抵抗体の漏洩電流の変化を示したもので、温度及
び′電圧ストレスを加える時間(課電時間)は、一旦減
少した漏洩電流がほぼ一定値Aに落ちつく時点までの時
間B(約24時間)が望ましい。
The main component is zinc oxide (ZnO) powder (bismuth dioxide ("yes) + antimony oxide (sb, Os),
Chromium oxide (Crtos), cobalt oxide (C00)
and powder of manganese oxide (MnO), etc., each at 0.0
It is added in a range of 1 to 60 moles and mixed in a ball mill. At this time, the oxide and an organic binder such as polyvinyl alcohol are mixed simultaneously. The mixture thus prepared is placed in a dry granulation device, such as a spray dryer, to form spherical aggregates. This powdered mixture is pressed,
For example, it is formed into a disk having a diameter of IQQ7M and a thickness of 25ia. Thereafter, the sintered body is sintered at 1000 to 1400°C, and the surface of the obtained sintered body is polished, and then an aluminum electrode is sprayed to form a nonlinear resistor. For example, the non-linear resistor formed in this way has an ambient temperature of 90'G and a duty ratio of 71% (ratio of applied voltage peak value to varistor Ichikawa V, mA) of 85%.
Temperature and pressure stress for a certain period of time,
Perform charging aging. The temperature and voltage stress application time (electrification time) are determined by measuring the change in leakage current of the nonlinear resistor. Figure 1 shows the change in the leakage current of the non-linear resistor in the above example.The temperature and the time for which voltage stress is applied (electrification time) are such that the leakage current, once reduced, remains approximately constant. Time B (approximately 24 hours) until reaching point A is desirable.

この温度及び電圧ストレスを加える条件、すなわち、周
囲温度及び課電率は、非直線抵抗体の組成及び形成方法
によって異なり、第1図(−示すような漏洩電流の変化
のパターン(即ち、初期の漏洩電流が減少した後一定値
に落ちつく〕<ターン)を与えるような条件が望ましく
、シたがって周囲温度及び課電率の条件は上記実施例に
限定されるものではない。
The conditions for applying this temperature and voltage stress, that is, the ambient temperature and charge rate, vary depending on the composition and formation method of the nonlinear resistor. It is desirable to use conditions that give a constant value after the leakage current decreases. Therefore, the conditions of ambient temperature and charging rate are not limited to those in the above embodiments.

また、温度及び電圧ストレスを加える時間(課電時間)
も、上記実施例に限定されるものでな1)ことは勿論で
ある。′ 第2図は、本発明と従来の非直線抵抗体の寿命特性を示
すもので、周囲温度110℃、課電率95%を印加した
時の非直線抵抗体の漏洩電流の変化を示したものである
。実線Cは従来の非直線抵抗体の特性を鉛線りは本発明
による非直線抵抗体の特性を示す。
Also, the time to apply temperature and voltage stress (power application time)
Of course, the present invention is not limited to the above-mentioned embodiments1). ' Figure 2 shows the life characteristics of the non-linear resistor of the present invention and the conventional one, and shows the change in leakage current of the non-linear resistor when an ambient temperature of 110°C and a charge rate of 95% are applied. It is something. The solid line C shows the characteristics of the conventional non-linear resistor, and the vertical line C shows the characteristics of the non-linear resistor according to the present invention.

また、−第1表は本発明と従来の非直線抵抗体の非直線
性を示すもので、 VxmA は、交流抵抗分1mAを
流シタ時の電r−E テアル。V、。KA/v11nA
、v、■lA/V(、、、mA + vo、、 mA/
V0.。、mAは同相(にそれぞれの電ぴtを流した時
の′電圧の比であり、値の小さし)もの程良い非直線性
を示す。
Table 1 shows the nonlinearity of the nonlinear resistors of the present invention and the conventional nonlinear resistor. V. KA/v11nA
, v, ■lA/V(,,, mA + vo,, mA/
V0. . , mA is the ratio of the voltages when the respective electric currents t are applied to the in-phase (the smaller the value), the better the nonlinearity is.

第2図及び第1表から明らかなように本発明、すなわち
、課電エージングを行なった非直線抵抗体は、従来の非
直線抵抗体に比べて寿命特性及び非直線性が著しく改良
されている。このように、本発明に係る非直線抵抗体は
ギヤツブレス避雷g4用の非直線抵抗体に要望される特
性を満足させるものである。
As is clear from FIG. 2 and Table 1, the nonlinear resistor of the present invention, that is, subjected to energized aging, has significantly improved life characteristics and nonlinearity compared to conventional nonlinear resistors. . As described above, the nonlinear resistor according to the present invention satisfies the characteristics required of a nonlinear resistor for gearless lightning arrester G4.

本発明のように優れた特性か得られる理由は、常規対地
′電圧程度の低電界領域におけるZnO系非直線抵抗体
の導電機構によって説明できる。導電機構はZnO粒子
の粒界層域に二つのショトキーノ(リヤが形成され、逆
バイアス側バリヤのショトキー効果により支配される。
The reason why such excellent characteristics as in the present invention can be obtained can be explained by the conduction mechanism of the ZnO-based nonlinear resistor in a low electric field region of about the normal ground voltage. The conduction mechanism is dominated by the Schottky effect of the barrier on the reverse bias side, in which two Schottky's are formed in the grain boundary layer region of the ZnO particles.

その電流密度(J)は次式%式% )) ) に=ボルツマン定敷 T−絶、対温度 e=電荷 ε0=真空の誘電率 ε−バリヤを作っている物質の比誘電率上式は漏洩電流
がバリヤの高さφ、電界強度E(課電率に比例)と周囲
温度Tに依存することを示し、一定の′磁界と周囲温度
下での漏洩電流の増加、すなわち課電劣化はショトキ−
バリヤの変形によって起ることを示している。したがっ
て、上記バリヤの高さを高めて常規運転電圧におけるリ
ーク電流を減少させ、常規運転時に非直線抵抗体内に発
生するジュール熱を低下させることにより、寿命特性は
向上する。
The current density (J) is calculated by the following formula: It is shown that the leakage current depends on the barrier height φ, the electric field strength E (proportional to the charging rate), and the ambient temperature T, and the increase in leakage current under a constant magnetic field and ambient temperature, that is, the charging degradation shorty
This shows that this occurs due to deformation of the barrier. Therefore, by increasing the height of the barrier to reduce leakage current at normal operating voltage and reducing Joule heat generated within the nonlinear resistor during normal operation, the life characteristics are improved.

第3図は」二記実施例(周囲温度90′G、課電率85
%で、一定時間課電し、温度及び電圧ストレスを加えた
時)の非直線抵抗体のバリヤの高さφの変化を示すもの
である。
Figure 3 shows the second embodiment (ambient temperature 90'G, charge rate 85
%, which shows the change in the barrier height φ of the nonlinear resistor when electricity is applied for a certain period of time and temperature and voltage stress are applied.

第3図から明らかなように、本発明、すなわち、課電エ
ージングを行なった非直線抵抗体は、バリヤの高さφが
高くなる為、寿命特性及び非直線性が著しく向上するの
である。
As is clear from FIG. 3, in the present invention, that is, in the non-linear resistor subjected to energized aging, the barrier height φ is increased, so that the life characteristics and non-linearity are significantly improved.

本発明の製造方法に使用する装置は上記実施例に限定さ
れるものではなく、本発明の製造方法に使用しうるもの
であれば各種の装置を適用できることは勿論である。
The apparatus used in the manufacturing method of the present invention is not limited to the above-mentioned embodiments, and it goes without saying that various types of apparatus can be applied as long as they can be used in the manufacturing method of the present invention.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、長時間にわたっ
て安定した電気特性、即ち寿命特性の優れた非直線抵抗
体を提供できる。
As described above, according to the present invention, it is possible to provide a nonlinear resistor with stable electrical characteristics over a long period of time, that is, with excellent life characteristics.

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

第1図、@2図は本発明の一実施例に係る非直線抵抗体
の課電時間−漏洩電流の変化の度合を示す特性線図、第
3図は本発明の一実施例に係る非直線抵抗体の課電時間
−バリヤの高さの変化の度合を示す特性線図である。 (7317)  代伊j人 弁理士 則 近 憲 佑 
(ほか1名)25− 課電■%PJ’j CH) 謀室峙聞CH)
Figures 1 and 2 are characteristic diagrams showing the degree of change in leakage current versus energization time of a nonlinear resistor according to an embodiment of the present invention, and Figure 3 is a characteristic diagram showing the degree of change in leakage current versus energization time of a nonlinear resistor according to an embodiment of the present invention. FIG. 3 is a characteristic diagram showing the degree of change in the height of a barrier versus the energization time of a linear resistor. (7317) Kensuke Chika, Patent Attorney Nori
(1 other person) 25- Charge ■%PJ'j CH) Secret room investigation CH)

Claims (1)

【特許請求の範囲】 1、 酸化亜鉛を主成分とする金属酸化物を混合成形し
た後焼成する非直線抵抗体の製造方法において、前記焼
成した非直線抵抗I体に一定時間のν→ 千−1一定時間の課電エージングは非直線抵抗記幇定値
に維持される時点まで行うことを特徴とする非直線抵抗
体の製造方法。
[Claims] 1. In a method for manufacturing a non-linear resistor in which a metal oxide containing zinc oxide as a main component is mixed and molded and then fired, the fired non-linear resistor I is subjected to ν→1,000- for a certain period of time. 1. A method for manufacturing a non-linear resistor, characterized in that aging by applying electricity for a certain period of time is carried out until the non-linear resistance is maintained at a constant value.
JP57177631A 1982-10-12 1982-10-12 Method of producing nonlinear resistor Pending JPS5967606A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57177631A JPS5967606A (en) 1982-10-12 1982-10-12 Method of producing nonlinear resistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57177631A JPS5967606A (en) 1982-10-12 1982-10-12 Method of producing nonlinear resistor

Publications (1)

Publication Number Publication Date
JPS5967606A true JPS5967606A (en) 1984-04-17

Family

ID=16034374

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57177631A Pending JPS5967606A (en) 1982-10-12 1982-10-12 Method of producing nonlinear resistor

Country Status (1)

Country Link
JP (1) JPS5967606A (en)

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