JPS5835321B2 - Ondohoshiyoyoujikiyudenzairiyou - Google Patents

Ondohoshiyoyoujikiyudenzairiyou

Info

Publication number
JPS5835321B2
JPS5835321B2 JP49057660A JP5766074A JPS5835321B2 JP S5835321 B2 JPS5835321 B2 JP S5835321B2 JP 49057660 A JP49057660 A JP 49057660A JP 5766074 A JP5766074 A JP 5766074A JP S5835321 B2 JPS5835321 B2 JP S5835321B2
Authority
JP
Japan
Prior art keywords
temperature
temperature coefficient
dielectric
dielectric constant
composition
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
JP49057660A
Other languages
Japanese (ja)
Other versions
JPS50149999A (en
Inventor
留治 大野
知利 中井
和明 内海
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.)
NEC Corp
Original Assignee
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP49057660A priority Critical patent/JPS5835321B2/en
Publication of JPS50149999A publication Critical patent/JPS50149999A/ja
Publication of JPS5835321B2 publication Critical patent/JPS5835321B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明はL a2T 1207 ・S r2N b20
7で構成される二成分系磁器誘電材料に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to L a2T 1207 ・S r2N b20
The present invention relates to a two-component ceramic dielectric material composed of 7.

本発明は誘電率が大きく、誘電損失が小さく、しかも誘
電率の温度系数が小さく、かつ広範な温度領域で直線性
の良好な温度補償用磁器誘電材料を提供するものである
The present invention provides a ceramic dielectric material for temperature compensation which has a large dielectric constant, a small dielectric loss, a small temperature coefficient of the dielectric constant, and good linearity over a wide temperature range.

温度補償用磁器コンデンサは通信機器や、カラーテレビ
等の回路素子として多用されており、この場合温度係数
は小さく(例えば−350〜+20 opp、”c )
、しかも温度係数は温度に対して一定値を保つことが望
まれている。
Temperature-compensating porcelain capacitors are often used as circuit elements in communication equipment and color televisions, and in this case the temperature coefficient is small (for example -350 to +20 opp, "c").
Moreover, it is desired that the temperature coefficient maintains a constant value with respect to temperature.

これまでこの種の材料として、S rT i03 、
CaT i03 。
Until now, materials of this type include S rT i03,
CaT i03.

MgTiO3,CaZrO3等を主成分とする組成物が
用いられている。
Compositions containing MgTiO3, CaZrO3, etc. as main components are used.

しかし、これらの材料では誘電率の温度係数が−350
〜+200 pHll/’Cのものでは誘電率の値が3
0〜16と小さく、さらに温度係数の温度依存性すなわ
ち温度係数の直線性も±601)1111/’C以上と
大きい欠点があった。
However, these materials have a temperature coefficient of dielectric constant of -350
~+200 pHll/'C has a dielectric constant of 3
0 to 16, and the temperature dependence of the temperature coefficient, that is, the linearity of the temperature coefficient, was also large, being more than ±601)1111/'C.

これらの欠点を補う材料としてL a 203−T i
o2MgO系の材料が開発された(特開昭491240
0)。
As a material that compensates for these drawbacks, L a 203-T i
o2MgO-based materials were developed (Japanese Patent Application Laid-Open No. 491240
0).

この材料は、温度係数をほぼ零にせしめることに成功し
、η)つ温度係数の温度依存性もある程度改善されてい
る。
This material has succeeded in reducing the temperature coefficient to almost zero, and the temperature dependence of the temperature coefficient has been improved to some extent.

しかし、目的に応じて、温度係数の調整をすることは不
可能であった。
However, it has been impossible to adjust the temperature coefficient depending on the purpose.

本発明はこれらの欠点を改善したものである。The present invention improves these drawbacks.

すなわちLa2T 1207 ・S r2Nb207で
構成される磁器誘電材料を台底することにより誘電率の
温度係数が小さく、誘電率が高く、誘電損失が小さくか
つ誘電率の温度変化がほぼ直線的である、すぐれた温度
補償用磁器誘電材料になることを見い出したものである
In other words, by using a porcelain dielectric material composed of La2T1207 and Sr2Nb207, the temperature coefficient of dielectric constant is small, the dielectric constant is high, the dielectric loss is small, and the change in dielectric constant with temperature is almost linear. It was discovered that this material can be used as a porcelain dielectric material for temperature compensation.

更に焼成温度も比較的低温であり、製造容易な組成物で
あることも見い出された。
Furthermore, it has been found that the firing temperature is relatively low and the composition is easy to manufacture.

以下実施例にもとずいて、本発明の詳細な説明する。The present invention will be described in detail below based on Examples.

実施例 La2T 1207 、 S r2Nb207で構成°
される磁器誘電材料についてはL a203 、 T
i 02 、5rCO3)Nb205の粉末を各組成に
応じて秤量し、ボールミルによって混合の後、沢過、乾
燥し、1000℃〜1200℃、2時間の条件で予焼し
た。
Example: Consisting of La2T 1207, S r2Nb207°
For the porcelain dielectric material used, L a203, T
i 02 , 5rCO3) Nb205 powder was weighed according to each composition, mixed in a ball mill, filtered through a sieve, dried, and pre-fired at 1000° C. to 1200° C. for 2 hours.

その後、直径16mmの円板に加圧成形し1300°C
〜1450°01〜2時間の条件で焼成を行なった。
After that, it was pressure-formed into a disc with a diameter of 16 mm and heated to 1300°C.
Firing was performed at ~1450° for 1 to 2 hours.

得られた磁器の両面に銀電極を600℃で焼き付けた後
、次の条件で誘電特性を測定した。
After baking silver electrodes on both sides of the obtained porcelain at 600°C, dielectric properties were measured under the following conditions.

誘電率と誘電損失は11d(zの周波数で、キャパシタ
ンスブリッジを用いて測定した。
The dielectric constant and dielectric loss were measured using a capacitance bridge at a frequency of 11d(z).

温度係数は誘電率の値を一80℃、0℃、20℃、55
℃、85℃の各温度で測定し、20℃における誘電率の
値を基準として求めた。
The temperature coefficient is the dielectric constant value - 80℃, 0℃, 20℃, 55
It was measured at each temperature of .degree. C. and 85.degree. C., and the dielectric constant value at 20.degree. C. was used as a reference.

ここで温度係数の計算は次式に従って行なった。Here, the temperature coefficient was calculated according to the following formula.

得られた結果のうち代表的な例を表に掲げておいた。Representative examples of the results obtained are listed in the table.

なお、表の温度係数の欄に士の表示をしであるのは、−
30℃から+85℃までの各温度における温度係数が士
の範囲内にあることを示しである。
In addition, the symbol indicated in the temperature coefficient column of the table indicates -
This shows that the temperature coefficient at each temperature from 30° C. to +85° C. is within the range of +85° C.

表より明らかなように、本発明の組成物は誘電率が大き
く、誘電損失が小さな優れた誘電特性を示している。
As is clear from the table, the composition of the present invention exhibits excellent dielectric properties with a high dielectric constant and low dielectric loss.

更に実用上、最も重要な特性の一つである温度係数は組
成比の調整により+11011%/’C程度から−15
0111111/’C程度まで自由に変えられることが
分かる。
Furthermore, the temperature coefficient, which is one of the most important properties in practice, can be changed from about +11011%/'C to -15% by adjusting the composition ratio.
It can be seen that it can be freely changed up to about 0111111/'C.

しかもその温度係数の温度に対する変化も±30ppl
/℃以下と非常に小さく、すなわち誘電率の温度変化が
直線的である。
Moreover, the change in temperature coefficient with respect to temperature is ±30ppl.
/°C or less, that is, the change in dielectric constant with temperature is linear.

以上の特徴は通信機器の回路素子として最も望ましいも
のである。
The above characteristics are most desirable as a circuit element for communication equipment.

なおLa2Ti2O7の組成が15モルφ以上100モ
ル係未満の組成範囲では表からもわかるようにすぐれた
特性が得られることが明らかである。
As can be seen from the table, it is clear that excellent properties can be obtained when the composition of La2Ti2O7 is in the range of 15 moles or more and less than 100 moles.

しかしL a2 T 120□の組成化が15モル俤よ
り少なくなると誘電損失がl0XIO−’を越え、温度
係数の温度に対する変化も±30111F/’Cを越え
てしまう。
However, when the composition of L a2 T 120□ is less than 15 molar, the dielectric loss exceeds 10XIO-' and the change in temperature coefficient with respect to temperature also exceeds ±30111 F/'C.

以上のことから本発明の組成範囲を次の組成範囲に限定
する。
Based on the above, the composition range of the present invention is limited to the following composition range.

すなわちL a2 T I 2072 S r2Nb2
07の二成分系において、(l−α)La2T s 2
07 ?αS r2 N b207 と表わされる誘電
体磁器組成物でαの値が0くα≦0.85の条件をみた
す範囲である。
That is, L a2 T I 2072 S r2Nb2
In the binary system of 07, (l-α)La2T s 2
07? In the dielectric ceramic composition expressed as αS r2 N b207 , the value of α is in a range that satisfies the condition of 0 and α≦0.85.

Claims (1)

【特許請求の範囲】[Claims] I La2Tt207,5r2Nb207の二成分系
において(1−α) L a2T +207 ・α5r
2Nb207と表わしたときαの値がOくα≦0.85
の条件をみたす範囲で作られる組成を持つことを特徴と
する温度補償用磁器誘電材料。
In the binary system of I La2Tt207,5r2Nb207 (1-α) L a2T +207 ・α5r
When expressed as 2Nb207, the value of α is O and α≦0.85
A porcelain dielectric material for temperature compensation, characterized by having a composition made within a range that satisfies the following conditions.
JP49057660A 1974-05-22 1974-05-22 Ondohoshiyoyoujikiyudenzairiyou Expired JPS5835321B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP49057660A JPS5835321B2 (en) 1974-05-22 1974-05-22 Ondohoshiyoyoujikiyudenzairiyou

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP49057660A JPS5835321B2 (en) 1974-05-22 1974-05-22 Ondohoshiyoyoujikiyudenzairiyou

Publications (2)

Publication Number Publication Date
JPS50149999A JPS50149999A (en) 1975-12-01
JPS5835321B2 true JPS5835321B2 (en) 1983-08-02

Family

ID=13062040

Family Applications (1)

Application Number Title Priority Date Filing Date
JP49057660A Expired JPS5835321B2 (en) 1974-05-22 1974-05-22 Ondohoshiyoyoujikiyudenzairiyou

Country Status (1)

Country Link
JP (1) JPS5835321B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5837139Y2 (en) * 1976-02-04 1983-08-22 日本電気株式会社 High frequency high power transistor amplifier
JP4541692B2 (en) * 2003-12-24 2010-09-08 日本特殊陶業株式会社 Dielectric porcelain composition

Also Published As

Publication number Publication date
JPS50149999A (en) 1975-12-01

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