JPS6095901A - Positive temperature coefficient semiconductor porcelain - Google Patents
Positive temperature coefficient semiconductor porcelainInfo
- Publication number
- JPS6095901A JPS6095901A JP58204082A JP20408283A JPS6095901A JP S6095901 A JPS6095901 A JP S6095901A JP 58204082 A JP58204082 A JP 58204082A JP 20408283 A JP20408283 A JP 20408283A JP S6095901 A JPS6095901 A JP S6095901A
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- resistance
- semiconductor porcelain
- positive
- porcelain
- 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
Links
Landscapes
- Compositions Of Oxide Ceramics (AREA)
- Thermistors And Varistors (AREA)
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】
産業上の利用分野
本発明は各種電子機器及び自動車等に電流制御素子及び
定温発熱体として用いられる正の抵抗温度係数を有する
正特性チタン酸バリウム系の正特性半導体磁器に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a barium titanate-based positive temperature semiconductor porcelain having a positive resistance temperature coefficient, which is used as a current control element and a constant temperature heating element in various electronic devices, automobiles, etc. It is related to.
従来例の構成とその問題点
従来より大きな正の抵抗温度係数をもつ正特性半導体磁
器材料が開発され、各種の電流制御素子及び定温発熱体
として用いられてきた0この正特性半導体磁器は最初低
い温度、すなわち低抵抗状態にある時に大きな電流を流
し得るも4のであり、一定時間経過後に正特性半導体磁
器自体のシュ°−ル熱による自己発熱により加熱されて
高温となり、正特性半導体磁器を高抵抗として電流値を
74%さく制御するとともに高温状態を保つものである
。Structure of the conventional example and its problems A positive temperature coefficient semiconductor porcelain material with a positive temperature coefficient of resistance larger than that of the conventional example has been developed and has been used as various current control elements and constant temperature heating elements. It is a material that can flow a large current when it is in a low resistance state, and after a certain period of time, it is heated by self-heating due to the surreal heat of the positive temperature semiconductor porcelain itself, and becomes high temperature, causing the positive temperature semiconductor porcelain to become high temperature. As a resistor, it controls the current value by 74% and maintains a high temperature state.
最近、正特性半導体磁器を用いて、上記のような電流制
御をさらに大きな電流に対しても11おうとする傾向に
ある。したがって、正特性半導体磁器に印加される電源
電圧が大きくなり、正特性半導体磁器が大きな電圧印加
に対して耐えられなくなり破壊するという問題があった
。また、正特性半導体磁器を定温発熱体として用い、さ
らに高出力・高効率化をしようとする傾向にある。この
ために正特性半導体磁器に印加される電源電圧力;ツ(
きくなったり、磁器表面に放熱用の金属板を取イ二1け
、放熱効率の向上環の工夫がなされている。しかしなが
ら、こうした正特性半導体磁器への大きな電圧の印加や
、放熱効率の向上による磁器表面温度と内部温度との温
度差により電圧破壊力;生じたり、断続負荷試験におい
て常温抵抗が増加するという問題があった。Recently, there has been a trend to use positive characteristic semiconductor ceramics to perform the above-described current control even for larger currents. Therefore, there is a problem in that the power supply voltage applied to the positive characteristic semiconductor ceramic becomes large, and the positive characteristic semiconductor ceramic becomes unable to withstand the large voltage application and breaks down. Additionally, there is a trend toward using positive characteristic semiconductor porcelain as a constant temperature heating element to further increase output and efficiency. For this purpose, the power supply voltage force applied to the positive characteristic semiconductor porcelain;
Efforts have been made to improve heat dissipation efficiency, such as by adding metal plates for heat dissipation to the surface of the porcelain. However, the application of a large voltage to such positive characteristic semiconductor porcelain and the temperature difference between the surface temperature of the porcelain and its internal temperature due to improved heat dissipation efficiency can cause problems such as voltage breakdown and an increase in room temperature resistance during intermittent load tests. there were.
上記のように、正特性半導体磁器は、自己のジュール熱
により自己発熱し電流を制御するものである。この正特
性半導体磁器の自己発熱は磁器の内部でおこシ、表面近
傍に比較し内部は熱放散が良好でなく、中心部はど温度
が高くなることは避けられない。従って、素子の各部分
において第1図に示すような同一の抵抗温度係数をもっ
ているので、中心温度T2は表面近傍温度T1 より高
くなり、中心部の抵抗R2は表面近傍の抵抗R1に比べ
て非常に大きい値となる。このため正特性半導体磁器へ
の印加電圧の大部分は中心部に加えられ、局部的に破壊
が生じたシ、断続負荷試験において常温抵抗の増加を生
じさせているものと考えられる。第1図中、TCはキュ
リ一温度を示[7、常温抵抗の2倍の抵抗値を示す温度
である。As mentioned above, the positive characteristic semiconductor ceramic generates heat by itself using its own Joule heat and controls the current. This self-heating of positive characteristic semiconductor porcelain occurs inside the porcelain, and heat dissipation is not as good inside the porcelain as compared to the vicinity of the surface, so it is inevitable that the temperature at the center will be high. Therefore, each part of the element has the same temperature coefficient of resistance as shown in Figure 1, so the center temperature T2 is higher than the temperature near the surface T1, and the resistance R2 at the center is much higher than the resistance R1 near the surface. becomes a large value. For this reason, most of the voltage applied to the positive characteristic semiconductor porcelain was applied to the center, causing local breakdown and an increase in room temperature resistance during the intermittent load test. In FIG. 1, TC indicates the Curie temperature [7, which is the temperature at which the resistance value is twice the room temperature resistance.
発明の目的
本発明は上記欠点に鑑み、電流制御素子及び定温発熱体
として用いられる正特性半導体磁器の温度分布差により
生じる抵抗値分布を制御し、大電流・大電圧に十分耐え
得る耐電圧特性にすぐれ、断続負荷試験における常温抵
抗の増加が少ない高信頼性の正特性半導体磁器を提供し
ようとするものである。Purpose of the Invention In view of the above-mentioned drawbacks, the present invention aims to control the resistance value distribution caused by the temperature distribution difference of positive characteristic semiconductor porcelain used as a current control element and a constant temperature heating element, and to develop a withstand voltage characteristic that can sufficiently withstand large currents and large voltages. The purpose of this invention is to provide a highly reliable positive characteristic semiconductor porcelain with excellent performance and little increase in room temperature resistance during intermittent load tests.
発明の構成
この目的を達成するために本発明にかかる正特性半導体
磁器は、その素子内において、鉛、ストロンチウム、カ
ルシウムまたは錫に濃度差をもたせ、キュリ一温度が素
子中心部で最も高く表面近傍が低くなるように形成した
構成とされており、動作時の正特性半導体磁器内の抵抗
値分布を抑制し、耐電圧特性にすぐれ、信頼性の高い正
特性半導体磁器が得ることができるという特有の効果を
有する。Structure of the Invention In order to achieve this object, the positive characteristic semiconductor porcelain according to the present invention has lead, strontium, calcium, or tin with different concentrations within the element, and the Curie temperature is highest in the center of the element and near the surface. It is unique in that it is formed to have a low resistance value, suppresses the resistance value distribution in the positive temperature semiconductor porcelain during operation, and can obtain a positive temperature semiconductor porcelain with excellent withstand voltage characteristics and high reliability. It has the effect of
すなわち、本発明にかかる正特性半導体磁器は第2図に
示すように、素子の表面近傍部の抵抗温度係数八くキュ
リ一温度Tc1)と中心部の抵抗温度曲線B(キュリ一
温度TC2)とが異なる。そして、この正特性半導体磁
器は中心部温度T2の方が表面近傍温度T1 よシも温
度が高くなることは避けられないが、素子内温度差(T
2−71)と抵抗温度特性の差がキュリ一温度差(Tc
2−Tc1)であり、常温抵抗及び抵抗温度係数がほぼ
等しいなら、動作時における表面近傍抵抗R1と中心部
における抵抗R2はほぼ等しくなり、従って正特性半導
体磁器全体にわたって抵抗値分布差が小さくなるので、
正特性半導体磁器に加えられる電界強度は全体に均一と
なり、耐電圧特性及び信頼性が著しく改善されることと
なる。That is, as shown in FIG. 2, the positive characteristic semiconductor porcelain according to the present invention has a resistance temperature coefficient of 8 × Curie temperature Tc1) near the surface of the element and a resistance temperature curve B (Curie temperature TC2) of the center part. is different. In this positive characteristic semiconductor porcelain, it is inevitable that the temperature at the center T2 is higher than the temperature near the surface T1, but the temperature difference within the element (T
2-71) and the resistance temperature characteristic is the Curie temperature difference (Tc
2-Tc1), and if the resistance at room temperature and the temperature coefficient of resistance are approximately equal, the resistance R1 near the surface and the resistance R2 at the center during operation will be approximately equal, and therefore the difference in resistance value distribution will be small over the entire positive characteristic semiconductor porcelain. So,
The electric field strength applied to the positive characteristic semiconductor ceramic becomes uniform throughout, and the withstand voltage characteristics and reliability are significantly improved.
以下、本発明の実施例を詳細に説明する。Examples of the present invention will be described in detail below.
実施例の説明
BaCo3. PbO、TtO2,Nb2O,、S i
2.MnO2を出十0.024Si02+0.Ooo4
Mn02及び
(Ba0.ワPb0.2o)Tio3+o、oo1oN
b2o5+0.024SiO2+OΩ004MnO2の
組成となるように配合し、20時間ボールミルにて混合
1−to5σCfイ而桔1番の乞 9n賎間ボールミル
にて粉砕し乾燥したものを、それぞれ5 wt%のポリ
ビニルアルコールを10wt%、加えて造粒し、それら
は原料1及び原料2とした0次に、原料1の1.31を
1001ψ/−にて加圧したのち、原料2の1.31を
加え100.lje/crltにて加圧し、さらに原料
1の1.3fを加え100 Kg/ctlにて加圧した
のち、全体を1000 Kl/ct/lにて加圧成形し
第3図に示す層状成形体を作製した0第3図中。Description of Examples BaCo3. PbO, TtO2, Nb2O,, Si
2. Exit MnO2 0.024Si02+0. Ooo4
Mn02 and (Ba0.waPb0.2o)Tio3+o, oo1oN
B2O5 + 0.024SiO2 + OΩ004MnO2, mixed in a ball mill for 20 hours, crushed and dried in a 9N Shama ball mill, and mixed with 10wt of 5wt% polyvinyl alcohol. %, and granulated, and they were made into raw material 1 and raw material 2. Next, 1.31 of raw material 1 was pressurized at 1001ψ/-, and then 1.31 of raw material 2 was added to 100. After applying pressure at lje/crlt, further adding 1.3f of raw material 1 and pressurizing at 100 Kg/ctl, the whole was press-molded at 1000 Kl/ct/l to obtain the layered molded product shown in Fig. 3. Figure 3.
1及び3は原料1の層、2は原料20層を示す0また、
比較のために原料1及び原料2をそれぞれ単独にて10
00Kf/cdの圧力にて、直径18mm+厚さ311
1mの円板形状に加圧成形した。このようにして得られ
たこれらの成形体を1300℃にて1時間焼成し、オー
ミック性銀電極を付与して試料1,2゜3を作製した。1 and 3 indicate the layer of raw material 1, and 2 indicates the layer of raw material 20.
For comparison, raw material 1 and raw material 2 were each used separately for 10
At a pressure of 00Kf/cd, diameter 18mm + thickness 311
It was press-molded into a 1 m disc shape. These molded bodies thus obtained were fired at 1300°C for 1 hour, and ohmic silver electrodes were provided thereon to prepare samples 1, 2°3.
ここで、試料1は本発明による第3図の成形体を用いた
ものであり、試料2,3はそれぞれ原料2,3を単独に
用いて作製したものである。こうして得られた試料の抵
抗温度特性を傘4図に示すとともに、表1に耐電圧、断
続負荷試験における抵抗変化率、常温比抵抗及びキュリ
一温度を示した。第4図中、Aは試料1.Bは試料2.
Cは試料3の抵抗温度特性をそれぞれ示す01だ、表中
の耐電圧は一定電圧にて3分間耐えることのできる電圧
で、soVづつ昇圧して試験した。450Vとあるのは
400■では3分間保持されたが、450Vでは3分以
内に破壊したことを意味する。同様に抵抗変化率は断続
負荷試験における抵抗変化率警示し、試料に175vの
電圧を10秒間印加し、350秒間停止するといった電
圧の間欠印加を3600回繰り返した際の常温抵抗の変
化率を示している。壕だ、常温比抵抗は26°Cにおけ
る比抵抗であり、キュリ一温度は常温抵抗の2倍の抵抗
を示す温度としだ。Here, Sample 1 was prepared using the molded article shown in FIG. 3 according to the present invention, and Samples 2 and 3 were prepared using Raw Materials 2 and 3 alone, respectively. The resistance-temperature characteristics of the sample thus obtained are shown in Figure 4, and Table 1 shows the withstand voltage, rate of change in resistance in the intermittent load test, specific resistance at room temperature, and Curie temperature. In FIG. 4, A indicates sample 1. B is sample 2.
C is 01, which indicates the resistance-temperature characteristics of sample 3. The withstand voltage in the table is a voltage that can be withstood for 3 minutes at a constant voltage, and the test was performed by increasing the voltage by soV. 450V means that at 400V it was held for 3 minutes, but at 450V it was destroyed within 3 minutes. Similarly, the rate of change in resistance indicates the rate of change in resistance in an intermittent load test, and indicates the rate of change in room temperature resistance when intermittent voltage application of 175 V is applied to the sample for 10 seconds and then stopped for 350 seconds is repeated 3600 times. ing. The resistivity at room temperature is the resistivity at 26°C, and the Curie temperature is the temperature at which the resistance is twice the resistance at room temperature.
上表より明らかなように、pb K濃度差をもたせキュ
リ一温度が中心部で高くなるようにした本発明による試
料1は、耐電圧が著しく向上するとともに常温断続負荷
試験における抵抗変化率を小さくすることができ、信頼
性が向上するという特有の効果を発揮する。As is clear from the above table, Sample 1 according to the present invention, which has a difference in PBK concentration and has a higher Curie temperature in the center, has a markedly improved withstand voltage and a smaller rate of resistance change in the room temperature intermittent load test. It has the unique effect of improving reliability.
なお、上記以外のキュリ一温度移動元素として鉛、 ス
トo ンチウム、カルシウム、錫を単独または2種類以
上同時に添加し、キュリ一温度が異なる原料を作成し、
上記実施例のように3層以上の層状構造をもだせても同
様の効果が得られた。In addition, lead, strontium, calcium, and tin may be added singly or at the same time as two or more of the above-mentioned Curie temperature transfer elements to create raw materials with different Curie temperatures,
Similar effects were obtained even when a layered structure of three or more layers was created as in the above embodiment.
また、キュリ一温度差は正特性半導体磁器の実使用条件
での素子内温度分布を測定し、設定するのが好ましい。Further, it is preferable that the Curie temperature difference is set by measuring the temperature distribution within the element under the actual usage conditions of the positive characteristic semiconductor porcelain.
また、ストロンチウム・カル/ラム・錫を酸化物、チタ
ン酸塩まだは種々の塩の形にて800℃〜1000℃の
予備焼結体表面に塗布し、125o〜1400℃にて焼
成し、キュリ一温度分布をもたせても同様の効果が得ら
れた0分間の効果
以上のように本発明は、正特性チタン酸バリウム系半導
体磁器素子内において、鉛、ストロンチウム、カルシウ
ムまたは錫に濃度差をもたせ、キュリ一温度が素子中心
部で最も高く表面近傍が鉢くなるように形成することに
より、正特性半導体磁器に印加される電界強度を全体に
均一とすることができるとともに、耐電圧特性及び信頼
性が著しく改善することができるという特有の効果を有
し、産業上の価値は大なるものがある。In addition, strontium cal/rum tin is applied in the form of oxides, titanates, and various salts to the surface of the pre-sintered body at 800°C to 1000°C, fired at 125°C to 1400°C, and cured. The same effect was obtained even with one temperature distribution.As described above, the present invention provides a difference in concentration of lead, strontium, calcium, or tin in a positive characteristic barium titanate semiconductor ceramic element. By forming the device so that the Curie temperature is highest at the center and concave near the surface, it is possible to make the electric field strength applied to the positive characteristic semiconductor porcelain uniform throughout the device, and improve withstand voltage characteristics and reliability. It has the unique effect of significantly improving physical properties and is of great industrial value.
第1図は従来の正特性磁器素子内における温度分布によ
り生じる抵抗分布を示す抵抗一温度曲線・を示す図、第
2図に本発明による正特性半導体磁器の動作原理を説明
するだめの抵抗一温度曲線を示す図、第3図は本発明に
よる正特性半導体磁器の実施例における成形体の構成を
示す図、第4図は実施例における試料の抵抗一温度曲線
を示す図である。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
→−J益戊(°C)
第 2 図
→う番ノ演;(°C)Fig. 1 is a diagram showing a resistance-temperature curve showing the resistance distribution caused by temperature distribution in a conventional PTC porcelain element, and Fig. 2 is a resistance-temperature curve illustrating the operating principle of the PTC semiconductor porcelain according to the present invention. FIG. 3 is a diagram showing the structure of a molded body in an example of the positive characteristic semiconductor porcelain according to the present invention, and FIG. 4 is a diagram showing a resistance-temperature curve of a sample in the example. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure → −J benefit (°C) 2nd figure → Uban no performance; (°C)
Claims (1)
鉛、ストロンチウム、カルシウムまだは錫に濃度差をも
たせ、キュリ一温度が素子中心部で最も高く表面近傍が
低くなるように形成してなることを特徴とする特性半導
体磁器。In a positive characteristic barium titanate semiconductor ceramic element,
A characteristic semiconductor porcelain characterized by having lead, strontium, calcium, and tin having different concentrations so that the Curie temperature is highest at the center of the element and lower near the surface.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58204082A JPS6095901A (en) | 1983-10-31 | 1983-10-31 | Positive temperature coefficient semiconductor porcelain |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58204082A JPS6095901A (en) | 1983-10-31 | 1983-10-31 | Positive temperature coefficient semiconductor porcelain |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6095901A true JPS6095901A (en) | 1985-05-29 |
Family
ID=16484478
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58204082A Pending JPS6095901A (en) | 1983-10-31 | 1983-10-31 | Positive temperature coefficient semiconductor porcelain |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6095901A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0346201A (en) * | 1989-07-13 | 1991-02-27 | Murata Mfg Co Ltd | Semiconductor porcelain possessing positive resistance-temperature characteristic |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5273363A (en) * | 1975-12-17 | 1977-06-20 | Hitachi Ltd | Thermistor with positive characteristics and method of making same |
-
1983
- 1983-10-31 JP JP58204082A patent/JPS6095901A/en active Pending
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5273363A (en) * | 1975-12-17 | 1977-06-20 | Hitachi Ltd | Thermistor with positive characteristics and method of making same |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0346201A (en) * | 1989-07-13 | 1991-02-27 | Murata Mfg Co Ltd | Semiconductor porcelain possessing positive resistance-temperature characteristic |
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