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JPS5941287B2 - Manufacturing method of voltage nonlinear resistance element - Google Patents
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JPS5941287B2 - Manufacturing method of voltage nonlinear resistance element - Google Patents

Manufacturing method of voltage nonlinear resistance element

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Publication number
JPS5941287B2
JPS5941287B2 JP54154721A JP15472179A JPS5941287B2 JP S5941287 B2 JPS5941287 B2 JP S5941287B2 JP 54154721 A JP54154721 A JP 54154721A JP 15472179 A JP15472179 A JP 15472179A JP S5941287 B2 JPS5941287 B2 JP S5941287B2
Authority
JP
Japan
Prior art keywords
pressure
manufacturing
binder
molding
voltage
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
JP54154721A
Other languages
Japanese (ja)
Other versions
JPS5676507A (en
Inventor
和生 江田
泰治 菊池
道雄 松岡
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP54154721A priority Critical patent/JPS5941287B2/en
Publication of JPS5676507A publication Critical patent/JPS5676507A/en
Publication of JPS5941287B2 publication Critical patent/JPS5941287B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は酸化亜鉛(ZnO)を主成分とする電圧非直線
抵抗素子の製造方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a voltage nonlinear resistance element containing zinc oxide (ZnO) as a main component.

避雷器や過電圧保護素子として電圧非直線抵抗素子(以
下バリスタと称す)が用いられている。
BACKGROUND ART Voltage nonlinear resistance elements (hereinafter referred to as varistors) are used as lightning arresters and overvoltage protection elements.

このような用途に用いる場合、バリスタさしては、(1
)電圧非直線指数αが大きいこと、(但し、αはI=(
V/C)αで定義され、■は電流、■は電圧、Cは定数
である。
When used for such purposes, the varistor should be (1
) The voltage nonlinearity index α is large (however, α is I=(
V/C)α, where ■ is current, ■ is voltage, and C is a constant.

)(2)制限電圧特性が良いこと、(制限電圧は、大電
流における電圧と微小電流における電圧の比で表わし、
通常避雷器などの場合には100A〜10KAにおける
電圧■1oooA〜Vt0KAと1mAにおける電圧V
1 m Aの比で表わす。
) (2) Good limiting voltage characteristics (Limiting voltage is expressed as the ratio of voltage at large current to voltage at minute current,
In the case of normal lightning arresters, the voltage at 100A to 10KA ■1oooA to Vt0KA and the voltage V at 1mA
Expressed as a ratio of 1 mA.

)(3) サージエネルギー耐量が大きいこと(サー
ジエネルギー耐量に、一回に耐えられる最大のサージエ
ネルギーを表わす。
) (3) Large surge energy withstand capacity (surge energy withstand capacity refers to the maximum surge energy that can be withstood at one time).

)が望ましい。従来知られているバリスタの中で、炭化
珪素を高温で焼き固めたSiCバリスタは、αが3〜7
であり、制限電圧比もきわめて悪い。
) is desirable. Among conventionally known varistors, SiC varistors made of silicon carbide baked and hardened at high temperatures have an α of 3 to 7.
The limiting voltage ratio is also extremely poor.

そこで近年ではZnOを主成分とするZnOバリスタが
多く用いられるようになっている。
Therefore, in recent years, ZnO varistors containing ZnO as a main component have been increasingly used.

ZnOバリスタは、ZnOを主成分とし、これに0.5
〜1.0モル%程度の5i203.Co2032MnO
2,5b203゜Cr2O3などを加えて混合した後金
型で成形し、1000℃以上の空気中で焼成することに
より得られる。
ZnO varistor has ZnO as the main component and 0.5
~1.0 mol% of 5i203. Co2032MnO
It is obtained by adding and mixing 2,5b203°Cr2O3, etc., molding it in a mold, and firing it in air at a temperature of 1000°C or higher.

このZnOバリスタは、αが大きく、また制限電圧特性
や、サージエネルギー耐量にも優れ、広く過電圧保護素
子や避雷器に用いられている。
This ZnO varistor has a large α, excellent limiting voltage characteristics and surge energy resistance, and is widely used in overvoltage protection elements and lightning arresters.

そこで最近では、さらに高圧電力用の避雷器への応用が
試みられている。
Therefore, recently, attempts have been made to apply it to lightning arresters for high-voltage power.

高圧電力用に応用するためには必然的に素子の大型化が
必要となる。
In order to apply it to high-voltage power, it is necessary to increase the size of the device.

しかしながら、素子を大型化するとせっかくの素子の優
れた性質が低下し、大型化したにもかかわらずそれほど
特性が向上しないといった現象が見られる。
However, as the size of the device increases, the excellent properties of the device deteriorate, and there is a phenomenon in which the characteristics do not improve much despite the increase in size.

本発明は、かかる状況に鑑み、大型化しても素子の特性
が劣化しない、電圧非直線指数、制限電圧特性、サージ
エネルギー耐量の優れた電圧非直線抵抗素子の製造方法
の提供を目的とし、以下に実施例と共に詳細を示す。
In view of this situation, the present invention aims to provide a method for manufacturing a voltage nonlinear resistance element that does not deteriorate in characteristics even when increased in size and has excellent voltage nonlinearity index, limiting voltage characteristics, and surge energy withstand capacity. Details are shown together with examples.

過電圧保護や避雷器用としてよく用いられる最も標準的
な材料組成として、Zn0(97,0モル%)、B I
203(0,5モル%)、、 Co203 (0,5
モル%)、M n 02 (0,5モル%)、5b20
3(1,0モル%)、Cr2 o3(0,5モル%)を
選んで従来方法と本発明方法を適用し、得られた素子の
特性を比較検討した。
The most standard material compositions often used for overvoltage protection and lightning arresters are Zn0 (97.0 mol%), B I
203 (0,5 mol%), Co203 (0,5
mol%), M n 02 (0.5 mol%), 5b20
3 (1.0 mol%) and Cr2O3 (0.5 mol%) were selected and the conventional method and the method of the present invention were applied, and the characteristics of the obtained devices were compared and studied.

通常のZnOバリスクは次の様な手順で製造される。A normal ZnO barisk is manufactured by the following procedure.

まず上記材料をボールミルなどで充分粉砕、混合すると
共に成形体の強度を保つためポリビニールアルコールな
どの有機バインダーを加えて平均の粒径が50〜150
μm程度になる様に造粒し、これを円筒状の金型に入れ
て円板状に圧縮成形を行う。
First, the above materials are thoroughly ground and mixed using a ball mill, etc., and an organic binder such as polyvinyl alcohol is added to maintain the strength of the molded product, so that the average particle size is 50 to 150.
The granules are granulated to a size of approximately μm, and then placed in a cylindrical mold and compressed into a disk shape.

成形圧力は通常250〜400 kg/=である。The molding pressure is usually 250 to 400 kg/=.

次いで電気炉に入れ、昇温速度100〜200°C/時
間で1150°C〜13000Cまで昇温し、2〜5時
間焼結を行わせる。
Next, it is placed in an electric furnace, and the temperature is raised to 1150°C to 13000C at a heating rate of 100 to 200°C/hour, and sintering is performed for 2 to 5 hours.

このようにして得られた円板状焼結体の両面を研磨後、
焼結体の端を2玉程度残して全体にアルミニウムの溶射
電極を設ける。
After polishing both sides of the disk-shaped sintered body thus obtained,
A sprayed aluminum electrode is provided over the entire sintered body, leaving about two beads at the edges.

このような方法により、直径20朋、厚さ5mm程度の
円板状のものまでは、比較的特性の良いものが得られる
By such a method, disk-shaped pieces up to about 20 mm in diameter and 5 mm in thickness can be obtained with relatively good characteristics.

しかしこれ以上直径を大きくしたり、厚みを厚くすると
、単位面積あたり、あるいは単位体積あたりの特性が低
下し、素子を大きくしたにもかかわらず全体としての特
性はそれほど向上しないといった結果になる。
However, if the diameter is made larger or the thickness is made thicker, the characteristics per unit area or per unit volume deteriorate, and the overall characteristics do not improve much even though the element is made larger.

第1図は従来の製造方法において、素子の厚みを10關
とし、素子の直径を5闘から112闘まで変えたときの
α、制限電圧比およびサージエネルギー耐量の変化を示
したものである。
FIG. 1 shows changes in α, limiting voltage ratio, and surge energy withstand capacity when the thickness of the element is 10 mm and the diameter of the element is changed from 5 mm to 112 mm in the conventional manufacturing method.

いずれも面積補正を行い、単位面積あたりに流れる電流
を一定にしたときのα、制限電圧比、および単位本体積
あたりのサージエネルギー耐量で示している。
In both cases, the area is corrected and the current flowing per unit area is kept constant, and α, the limiting voltage ratio, and the surge energy withstand capacity per unit volume are shown.

詳しくは、αは1c11t、に0.1mAおよび1mA
の電流が流れたときの電圧比から求めた値であり、制限
電圧比は1dに100OAおよび1mAの電流が流れた
ときの電圧比で表わしている。
Specifically, α is 1c11t, 0.1mA and 1mA
The limiting voltage ratio is expressed as the voltage ratio when currents of 100 OA and 1 mA flow in 1d.

なお、1000Aにおける電圧の測定については8×2
0、、、sの衝撃電流を用い、他の測定については直流
を用いて測定を行った。
In addition, for voltage measurement at 1000A, 8×2
Measurements were performed using an impact current of 0, s, and direct current for other measurements.

またサージエネルギー耐量は2mS以上の長波尾の衝撃
電流を用い、素子が破壊する値を求めたものである。
In addition, the surge energy withstand capacity is determined by using an impact current with a long wave tail of 2 mS or more and determining the value at which the element is destroyed.

第1図において素子の直径が20m以上になると、α、
制限電圧比、サージエネルギー耐量のいずれの特性も低
下していることが認められる。
In Fig. 1, when the diameter of the element becomes 20 m or more, α,
It is recognized that both the limiting voltage ratio and surge energy withstand characteristics have decreased.

第2図は素子の直径を56mmとし、素子の厚みを5朋
から50mmまで変えたときの、α、制限電圧比、サー
ジエネルギー耐量について求めたものである。
FIG. 2 shows α, limiting voltage ratio, and surge energy withstand capacity when the element diameter is 56 mm and the element thickness is varied from 5 mm to 50 mm.

素子の厚みが5mm以上になると、やはりα、制限電圧
比、サージエネルギー耐量が低下する。
When the thickness of the element becomes 5 mm or more, α, limiting voltage ratio, and surge energy withstand capacity also decrease.

また、従来の方法で製造された素子の均一性について分
析した。
We also analyzed the uniformity of devices manufactured using conventional methods.

第3図は従来の製造方法で作られた大型素子における特
性分布を示す。
FIG. 3 shows the characteristic distribution of a large-sized element manufactured by the conventional manufacturing method.

これは直径56mm、厚み40朋の素子の中央部を、厚
み方向に5個、直径方向に6個の角型に切り出し、各部
のαと制限電圧比を測定して求めたものである。
This was determined by cutting out five squares in the thickness direction and six squares in the diameter direction from the center of an element having a diameter of 56 mm and a thickness of 40 mm, and measuring the α and limiting voltage ratio of each part.

内部はどα、制限電圧比が低下していることがわかる。It can be seen that internally, the limiting voltage ratio is decreasing.

また第4図は、直径112mm、厚みl□mmの素子に
ついて、各部分の1mAにおける電圧V1mAの分布を
測定した結果を示したものである。
Moreover, FIG. 4 shows the results of measuring the distribution of voltage V1 mA at 1 mA in each part for an element having a diameter of 112 mm and a thickness of 1 mm.

直径を大きくすると、このように横断面内の抵抗分布の
均一性が器くなり、電流の集中を招いて単位体積あたり
のサージエネルギー耐量が低下するものと思われる。
It is thought that when the diameter is increased, the uniformity of the resistance distribution within the cross section becomes poor, resulting in concentration of current and a decrease in the surge energy withstand capacity per unit volume.

次に本発明に係る製造方法について述べる。Next, the manufacturing method according to the present invention will be described.

前記と同一の組成の材料を、従来方法と同じ様に粉砕、
混合、造粒の後、円筒型の金型により100に9/er
aの圧力で円板状に圧縮成形を行い、予備成形する。
The material with the same composition as above is crushed in the same way as the conventional method.
After mixing and granulation, 9/er to 100 using a cylindrical mold
Compression molding is performed into a disk shape at a pressure of a to preform.

次いでこの予備成形体をゴム袋に入れ、真空ポンプで中
の空気を除去した後ゴム袋を密閉する。
Next, this preform is placed in a rubber bag, and after removing the air inside with a vacuum pump, the rubber bag is sealed.

次に、これを水を充満した圧力容器内に収容した後、圧
力容器内の水に外部から500kg/cr?t。
Next, after storing this in a pressure vessel filled with water, 500 kg/cr? t.

の圧力を加えて本成形を行う。Main molding is performed by applying pressure.

次にゴム袋より成形体を取り出し、500℃の空気中で
2時間程度加熱してバインダーを除去した後電気炉に入
れ、50℃/時間の昇温速度で1200℃まで昇温し、
その温度に5時間保持して焼結を行わせる。
Next, the molded body was taken out from the rubber bag, heated in air at 500°C for about 2 hours to remove the binder, and then placed in an electric furnace and heated to 1200°C at a heating rate of 50°C/hour.
The temperature is maintained for 5 hours to allow sintering.

以後の手順は従来方法と同じである。The subsequent steps are the same as the conventional method.

このようにして得られた素子の特性を第5図および第6
図に示す。
The characteristics of the device thus obtained are shown in Figures 5 and 6.
As shown in the figure.

第5図は素子の厚みを10rrtmとし、直径を変えた
場合の各素子の特性を、第6図は素子の直径を55mm
とし、厚みを変えた場合の各素子の特性を示している。
Figure 5 shows the characteristics of each element when the thickness of the element is 10rrtm and the diameter is changed, and Figure 6 shows the characteristics of each element when the diameter of the element is 55mm.
The characteristics of each element are shown when the thickness is changed.

いずれも、このような方法で製造することにより素子を
大きくした場合の特性低下が著しく改善されている。
In either case, by manufacturing with this method, the deterioration in characteristics when the device is increased in size is significantly improved.

次に金型による予備成形圧力と、加圧液体による本成形
圧力の関係について調べた。
Next, we investigated the relationship between the preforming pressure by the mold and the main molding pressure by the pressurized liquid.

第1表に直径56mm、厚み107nrnの素子につい
て予備成形圧力及び本成形圧力を変化させた場合の各特
性の測定結果を示す。
Table 1 shows the measurement results of each characteristic when the preforming pressure and the main molding pressure were varied for an element having a diameter of 56 mm and a thickness of 107 nm.

第1表から、後で加えられる本成形圧力が予備成形圧力
よりも高くないと特性改善の効果がないこと、また予備
成形圧力が500kL;!/dより大きくなるとやはり
改善の効果が薄れることがわかる。
From Table 1, it can be seen that there is no effect of improving the properties unless the main molding pressure applied later is higher than the preforming pressure, and the preforming pressure is 500kL! It can be seen that when the value becomes larger than /d, the improvement effect becomes weaker.

また予備成形圧力が50kg/iより小さくなると成形
体強度が弱く、取扱いが極めて困難であった1、従って
予備成形圧力は50〜500 kg/C7?L内の値に
選び、本成形圧力は予備成形圧力よりも大きくする必要
がある。
In addition, when the preforming pressure is less than 50 kg/i, the strength of the molded product is weak and handling is extremely difficult1.Therefore, the preforming pressure is 50 to 500 kg/C7? The main molding pressure must be greater than the preforming pressure.

また本成形圧力は200 kg/cn以上でないと効果
が薄く、2000 kg/i以上は特性が飽和してあま
り改善の効果がなかった。
Moreover, the effect is weak unless the main molding pressure is 200 kg/cn or more, and the properties are saturated when it is 2000 kg/i or more, and there is not much improvement effect.

従って本成形圧力は200〜2000 kg/iが望ま
しい。
Therefore, the main molding pressure is preferably 200 to 2000 kg/i.

以上述べた特性の改善は、成形時の圧力分布が大型素子
の特性に強く関係している点を利用したものである。
The above-mentioned improvements in properties take advantage of the fact that the pressure distribution during molding is strongly related to the properties of large elements.

すなわち、金型成形の場合には、−軸性の圧力であり、
かつ金型部分と成形体との間に摩擦力が作用することに
よって成形体の表面と内部で圧力の加わり力が非常に異
なってくること、直径を大きくした場合には粉体の充填
むらなどによる圧力分布を生じることなどにより、素子
の均一性が損われ、特性が低下するものと考えられる。
In other words, in the case of mold forming, it is -axial pressure,
Additionally, due to the frictional force acting between the mold part and the molded object, the pressure applied on the surface and inside of the molded object will be very different, and if the diameter is increased, uneven filling of powder may occur. It is thought that the uniformity of the element is impaired and the characteristics are deteriorated due to the pressure distribution caused by this.

これに対し、本発明に係る方法においては金型による予
備成形で形を決定し、ついで加圧液体中で等方的に圧力
を加えて金型成形による圧力の分布を除去するので、均
一性が向上し、大型の素子にしても特性低下が少ないも
のと考えられる。
In contrast, in the method according to the present invention, the shape is determined by preforming with a mold, and then pressure is applied isotropically in a pressurized liquid to remove the pressure distribution caused by molding, so that uniformity is achieved. It is considered that the characteristics are improved and the characteristics deteriorate less even if the device is made large.

ところで、この様にして得られた圧力分布の均一な成形
体を用いても、焼成条件によってはその効果が弱められ
る。
By the way, even if a molded body with a uniform pressure distribution obtained in this manner is used, the effect may be weakened depending on the firing conditions.

すなわち、昇温速度があまり速すぎると、内部と外部で
温度差を生じ、その温度差があまり大きくなりすぎると
焼結反応が内部と外部で異なり、均一な成形体を用いた
にもかかわらず不均一な焼結体になってしまうためと考
えられる。
In other words, if the heating rate is too fast, a temperature difference will occur between the inside and the outside, and if that temperature difference becomes too large, the sintering reaction will be different between the inside and outside, and even if a uniform compact is used, This is thought to be because the sintered body becomes non-uniform.

そこで、直径56mm、厚み50+u+の素子について
焼成時の昇温速度を変えて特性の変化を調べた。
Therefore, changes in characteristics were investigated by changing the heating rate during firing for an element with a diameter of 56 mm and a thickness of 50+u+.

その結果を第2表に示す。第2表から1時間あたりの昇
温速度が80℃以下であれば、焼結時に特性が悪化する
現象が避けられることがわかる。
The results are shown in Table 2. It can be seen from Table 2 that if the temperature increase rate per hour is 80° C. or less, the phenomenon of deterioration of properties during sintering can be avoided.

また、素子が大型になると焼成昇温時にバインダーが完
全に除去されない場合があるため、焼成前にバインダー
の除去を行なわないと特性が低下する。
Furthermore, if the device becomes large in size, the binder may not be completely removed when the temperature is increased during firing, so if the binder is not removed before firing, the characteristics will deteriorate.

特に本発明方法では本成形圧力を予備成形圧力よりも高
くしているので、高圧力を加えることになり、例えば5
00 kg/cyyt以上の圧力を加えるようになると
、バインダーが焼成昇温時に逸散しにくくなるため、焼
成前のバインダー除去が必要である。
In particular, in the method of the present invention, the main molding pressure is higher than the preforming pressure, so high pressure is applied, for example,
If a pressure of 0.00 kg/cyyt or more is applied, it becomes difficult for the binder to escape when the temperature is increased during firing, so it is necessary to remove the binder before firing.

バインダー除去の温度は200〜700°Cで1〜5時
間程度が良い。
The temperature for removing the binder is preferably 200 to 700°C for about 1 to 5 hours.

これは、200℃以下ではバインダーがなかなか逸散せ
ず、700℃以上では焼結が始まるためである。
This is because the binder does not easily dissipate at temperatures below 200°C, and sintering begins at temperatures above 700°C.

なお、上記実施例では加圧液体による本成形時に加圧媒
体として水を用いたが、その原理から考えて水と同様の
働きをするもの、すなわち液体であればどれでも良く、
たとえば油などを用いても同じ効果を期待できることは
明らかである。
In addition, in the above embodiment, water was used as the pressurizing medium during main molding using pressurized liquid, but considering the principle, any medium that functions similarly to water, that is, any liquid may be used.
It is clear that the same effect can be expected by using oil, for example.

また、加圧時に成形体を水から完全に隔離しておくこと
が必要であり、しかもその隔離手段は水圧が成形体に充
分伝わると共に成形体の形状の変化に追従して変形し得
る様に収縮性を有する必要がある。
In addition, it is necessary to completely isolate the molded body from water during pressurization, and the isolation means must be such that the water pressure is sufficiently transmitted to the molded body and that it can deform to follow changes in the shape of the molded body. Must have contractility.

その様なものとしてはゴム製の袋が最も適しており、成
形体収容後袋内を真空にして水圧が成形体に十分に伝わ
る様にする。
A rubber bag is most suitable for such a bag, and after housing the molded product, the inside of the bag is evacuated so that water pressure can be sufficiently transmitted to the molded product.

しかし、ゴム袋に限らず上記の条件を満たすものであれ
ば、その他の手段を採用することもできる。
However, the bag is not limited to a rubber bag, and other means may be used as long as they meet the above conditions.

本発明の電圧非直線抵抗素子の製造方法によれば、上記
の説明から明らかな様に大型の素子においても特性の劣
化のない素子が得られ、従って高圧電力用避雷器など大
型の素子を必要とする分野での効果が犬である。
According to the method for manufacturing a voltage nonlinear resistance element of the present invention, as is clear from the above explanation, an element with no deterioration in characteristics can be obtained even in a large-sized element, and therefore a large-sized element such as a surge arrester for high-voltage power is not required. The effect in the field is dogs.

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

第1図乃至第4図は従来方法により製造された素子の時
性を示し、第1図は素子の直径と特性との関係を示すグ
ラフ、第2図は素子の厚さと特性との関係を示すグラフ
、第3図は素子の縦断面内の特性分布を示す図、第4図
は横断面内の特性の分布を示す図、第5図及び第6図は
本発明の一実施例により製造された素子の特性を示し、
第5図は素子の直径と特性との関係を示すグラフ、第6
図は素子の厚さと特性との関係を示すグラフである。
Figures 1 to 4 show the time characteristics of elements manufactured by conventional methods, Figure 1 is a graph showing the relationship between element diameter and characteristics, and Figure 2 is a graph showing the relationship between element thickness and characteristics. 3 is a diagram showing the characteristic distribution in the vertical cross section of the device, FIG. 4 is a diagram showing the characteristic distribution in the cross section, and FIGS. 5 and 6 are graphs showing the characteristic distribution in the longitudinal section of the device. The characteristics of the device are shown.
Figure 5 is a graph showing the relationship between element diameter and characteristics;
The figure is a graph showing the relationship between element thickness and characteristics.

Claims (1)

【特許請求の範囲】 1 バインダーにて粒状化された酸化亜鉛と添加物の混
合物を金型によって予備成形し、この予備成形体を予備
成形圧より大きな圧力の加圧液体によって本成形し、本
成形完了後バインダー除去を行い、その後徐々に昇温し
で焼結することを特徴とする電圧非直線抵抗素子の製造
方法。 2 前記予備成形圧力を50〜500kg/Cr?Lと
し、本成形圧力を200〜2000kg/Cr4とする
ことを特徴とする特許請求の範囲第1項記載の製造方法
。 3 焼結時の昇温速度を1時間あたり80℃以下とする
ことを特徴とする特許請求の範囲第1項記載の方法。 4 予備成形体を可撓性と収縮性を有する密閉容器内に
収容しかつ容器内を真空にして密閉し、該容器を液体を
充填した加圧容器内に収容した後前記液体に圧力を加え
て本成形することを特徴とする特許請求の範囲第1項記
載の製造方法。 5 バインダー除去の温度を200〜700℃とするこ
とを特徴とする特許請求の範囲第1項記載の製造方法。
[Claims] 1. A mixture of zinc oxide and additives granulated with a binder is preformed in a mold, and this preform is subjected to main molding using a pressurized liquid at a pressure higher than the preforming pressure. A method for manufacturing a voltage nonlinear resistance element, which comprises removing the binder after completion of molding, and then sintering by gradually raising the temperature. 2. Is the preforming pressure 50 to 500 kg/Cr? The manufacturing method according to claim 1, characterized in that the main molding pressure is 200 to 2000 kg/Cr4. 3. The method according to claim 1, characterized in that the temperature increase rate during sintering is 80° C. or less per hour. 4. The preform is placed in a flexible and contractible airtight container, the container is evacuated and sealed, and the container is placed in a pressurized container filled with liquid, and then pressure is applied to the liquid. 2. The manufacturing method according to claim 1, wherein the final molding is carried out using a wafer. 5. The manufacturing method according to claim 1, wherein the binder removal temperature is 200 to 700°C.
JP54154721A 1979-11-28 1979-11-28 Manufacturing method of voltage nonlinear resistance element Expired JPS5941287B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP54154721A JPS5941287B2 (en) 1979-11-28 1979-11-28 Manufacturing method of voltage nonlinear resistance element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP54154721A JPS5941287B2 (en) 1979-11-28 1979-11-28 Manufacturing method of voltage nonlinear resistance element

Publications (2)

Publication Number Publication Date
JPS5676507A JPS5676507A (en) 1981-06-24
JPS5941287B2 true JPS5941287B2 (en) 1984-10-05

Family

ID=15590504

Family Applications (1)

Application Number Title Priority Date Filing Date
JP54154721A Expired JPS5941287B2 (en) 1979-11-28 1979-11-28 Manufacturing method of voltage nonlinear resistance element

Country Status (1)

Country Link
JP (1) JPS5941287B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5850702A (en) * 1981-09-21 1983-03-25 株式会社東芝 Method of producing voltage nonlinear resistor
JPS62141701A (en) * 1985-12-16 1987-06-25 富士電機株式会社 Manufacture of voltage nonlinear resistor

Also Published As

Publication number Publication date
JPS5676507A (en) 1981-06-24

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