JPS593009B2 - Porcelain dielectric material for temperature compensation - Google Patents

Porcelain dielectric material for temperature compensation

Info

Publication number
JPS593009B2
JPS593009B2 JP56212406A JP21240681A JPS593009B2 JP S593009 B2 JPS593009 B2 JP S593009B2 JP 56212406 A JP56212406 A JP 56212406A JP 21240681 A JP21240681 A JP 21240681A JP S593009 B2 JPS593009 B2 JP S593009B2
Authority
JP
Japan
Prior art keywords
temperature
temperature coefficient
dielectric material
temperature compensation
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.)
Expired
Application number
JP56212406A
Other languages
Japanese (ja)
Other versions
JPS57154713A (en
Inventor
知利 中井
和明 内海
留治 大野
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 JP56212406A priority Critical patent/JPS593009B2/en
Publication of JPS57154713A publication Critical patent/JPS57154713A/en
Publication of JPS593009B2 publication Critical patent/JPS593009B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Compositions Of Oxide Ceramics (AREA)
  • Ceramic Capacitors (AREA)
  • Inorganic Insulating Materials (AREA)

Description

【発明の詳細な説明】 本発明はsr2Nb_2O_7、sr2Ta_2O_7
、一M献Ti_2_−_2_x04−!X(ただし0く
xく1.0)で表示される系の磁器誘電材料に関するも
のである。
Detailed Description of the Invention The present invention provides sr2Nb_2O_7, sr2Ta_2O_7
, 1M contribution Ti_2_-_2_x04-! This relates to a ceramic dielectric material of the system represented by X (0 x 1.0).

本発明は誘電率が大きく、誘電損失が小さく、しかも誘
電率の温度係数を広い範囲で自由に変えることができ、
かつ、広範な温度領域で温度係数の値が変らない温度補
償用磁器誘電材料を提供するものである。5 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、誘電率が大きく、
誘電損失が小さいことが常に望まれ、温度係数は指定さ
れた任意の値で、かつ、温度に対して一定値を保つこと
が望まれて・o いる。
The present invention has a large dielectric constant, low dielectric loss, and can freely change the temperature coefficient of the dielectric constant over a wide range.
Furthermore, the present invention provides a temperature-compensating ceramic dielectric material whose temperature coefficient does not change over a wide temperature range. 5 Temperature-compensating porcelain capacitors are often used as circuit elements in communication equipment, color televisions, etc. In this case, they have a large dielectric constant,
It is always desired that the dielectric loss be small, and it is desired that the temperature coefficient be any specified value, and that it should remain constant with respect to temperature.

これまで、この種類の材料としてSrTiO3、CaT
i03、MgTiO3、CaZrO3等を主成分とする
組成物が用いられていたが、これらの材料では誘電率の
温度係数が小さいものでは誘電率の値が、3015〜1
6と小さく、さらに温度係数の温度依存性、すなわち温
度に対する温度係数の変化も±60pμm/C以上と大
きい欠点があつた。
Until now, materials of this type include SrTiO3, CaT
Compositions containing i03, MgTiO3, CaZrO3, etc. as main components have been used, but these materials have a small temperature coefficient of dielectric constant, with a dielectric constant value of 3015 to 1.
6, and furthermore, the temperature dependence of the temperature coefficient, that is, the change in temperature coefficient with respect to temperature, was as large as ±60 pμm/C or more.

また、誘電率の温度係数の大きいものでは温度係数が温
度に対して大きく変化してしまう欠点があつた。フ0
そこで、これらの欠点を補う材料の一つとしてLa_2
03−TiO2−MgO系の材料が開発された(特開昭
49−12400)。この系では温度係数をほぼ零にせ
しめることに成功し、かつ温度係数の温度依存性もある
程度改善されている。しかし、ク5 目的に応じて温度
係数を調整することは不可能であつた。本発明は、これ
らの欠点を改善したものである。
In addition, materials with a large temperature coefficient of dielectric constant have the disadvantage that the temperature coefficient varies greatly with temperature. F0
Therefore, La_2 is one of the materials that can compensate for these drawbacks.
03-TiO2-MgO based materials have been developed (Japanese Patent Application Laid-Open No. 12400/1983). In this system, we have succeeded in reducing the temperature coefficient to almost zero, and the temperature dependence of the temperature coefficient has also been improved to some extent. However, it was impossible to adjust the temperature coefficient depending on the purpose. The present invention improves these drawbacks.

すなわち、sr2Nb_2O_7、sr2Ta_2O_
7、一Mg_2XTi_2_−_2_x04−練ただし
0くXく1.0)で示される系の磁器誘電材料を合成す
ることにより誘電率が大きく、誘電損失が小さく、しか
も誘電率の温度係数を広い範囲で自由に変えることがで
き、かつ広範な温度領域で誘電率の温度係数の値が一あ
定な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。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。以下、
実施例にもとづいて本発明の有効性を説明する。
That is, sr2Nb_2O_7, sr2Ta_2O_
7. By synthesizing porcelain dielectric materials of the system represented by 1. We have discovered that this material is an excellent temperature-compensating porcelain dielectric material that can be freely changed and has a constant temperature coefficient of permittivity over a wide temperature range. Furthermore, it has been found that the firing temperature is relatively low and the composition is easy to manufacture. below,
The effectiveness of the present invention will be explained based on Examples.

実施例 (0〈xく1.0)で構成される磁器誘電材料について
はSrCO3,Nb2O,,Ta2O5,TiO2,M
gOの粉末を、また、Sr2Nb2O7,sr2Ta2
O7,−Mg2XTi2−!XO4l(X=0)で構成
される磁器誘電材料については、SrCO3,Nb2O
5,Ta2O,,TlO2の粉末を、またSr2N鴎0
7,sr2Ta2〜,t!式12,0490(X=1.
0)で構成される磁器誘電材料についてはSrCO3,
Nb2O5,Ta2O5,MgOの粉末を各組成に応じ
て秤量し、ボールミルによつ混合の後、ろ過、乾燥し、
1000℃〜1200℃、2時間の条件で予焼した。
For the porcelain dielectric material composed of the example (0<x 1.0), SrCO3, Nb2O, Ta2O5, TiO2, M
gO powder, Sr2Nb2O7, sr2Ta2
O7, -Mg2XTi2-! For porcelain dielectric materials composed of XO4l (X=0), SrCO3, Nb2O
5. Ta2O,, TlO2 powder and Sr2N 0
7,sr2Ta2~,t! Equation 12,0490 (X=1.
0) for the porcelain dielectric material composed of SrCO3,
Nb2O5, Ta2O5, MgO powders were weighed according to each composition, mixed in a ball mill, filtered, dried,
Prebaking was performed at 1000°C to 1200°C for 2 hours.

その後、直径16uの円板に加圧成形し、1300℃/
1450℃1〜2時間の条件で焼成を行なつた。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。誘電率と誘電損失は1KH
zの周波数でキヤバシタンスブリツジを用いて測定した
。温度係数は誘電率の値を−30℃、O℃、20℃、5
5℃、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。ここで温度係数の計算は次式
に従つて行なつた。
After that, it was pressure-formed into a disc with a diameter of 16u and heated to 1300℃/
Firing was performed at 1450° C. for 1 to 2 hours. After baking silver electrodes on both sides of the obtained porcelain at 600°C, dielectric properties were measured under the following conditions. Dielectric constant and dielectric loss are 1KH
Measurements were made using a capacitance bridge at a frequency of z. The temperature coefficient is the dielectric constant value -30℃, O℃, 20℃, 5
It was measured at each temperature of 5°C and 85°C, and the dielectric constant value at 20°C was used as a reference. Here, the temperature coefficient was calculated according to the following formula.

得られた結果のうち、代表的な例を第1表に掲げておい
た。なお、第1表の温度係数の欄に士の表示をしてある
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てある。
Among the results obtained, representative examples are listed in Table 1. In addition, the display of 2 in the column of temperature coefficient in Table 1 indicates that the temperature coefficient at each temperature from -30°C to 85°C is within the range of 2.

第1表より明らかなようにSr2Nb2O,,Sr2T
a2O7,−2V1g2XTi2ィXO4S!X(0≦
xく1.0)で構成される磁気誘電材料は誘電率が大き
く、誘電損失が小さいすぐれた特性を示している。更に
組成比を調整することにより温度係数の値を、およそ+
60Ppm/Cから−1100ppm/C程度と非常に
広い範囲に調整できることが明らかである。しかも温度
係数の温度に対する変化も±30ppm/C以内または
温度係数の±10%以内におさまつている。一方、Sr
2Ta2O7が60モル%より多い組成範囲では焼成を
1450℃で行なつてもち密に焼結しない。
As is clear from Table 1, Sr2Nb2O,, Sr2T
a2O7, -2V1g2XTi2-XO4S! X(0≦
The magneto-dielectric material composed of x x 1.0) has a high dielectric constant and exhibits excellent characteristics such as low dielectric loss. By further adjusting the composition ratio, the temperature coefficient value can be adjusted to approximately +
It is clear that it can be adjusted in a very wide range from about 60 Ppm/C to -1100 ppm/C. Furthermore, the change in temperature coefficient with respect to temperature is within ±30 ppm/C or within ±10% of the temperature coefficient. On the other hand, Sr.
In a composition range in which 2Ta2O7 is more than 60 mol %, dense sintering is not achieved even when firing is performed at 1450°C.

このため、この組成範囲は実用材料としては不適当であ
る。またSr2Nb2O7が65モル%より多い組成範
囲、および芦,。Ti24A,(0くxく1.0)が2
0モル%より少ない組成範囲では温度係数の温度に対す
る変化が±30ppm//C以内、あるいは温度係数の
±10%以内という条件を満足しない。またSr2Nb
2O7が5モル(!)1より少ない組成範囲およびか!
2XTi21X罎x(0<.x≦1.0)が80モル%
より多い組成範囲では温度係数の温度に対する変化が±
30ppm/℃あるいは温度係数の±10%以内という
条件と誘電率の値が30以上という条件を同時には満足
しない。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。
Therefore, this composition range is inappropriate as a practical material. Also, a composition range in which Sr2Nb2O7 is more than 65 mol%, and Ashi. Ti24A, (0 x x 1.0) is 2
In a composition range less than 0 mol %, the condition that the change in temperature coefficient with respect to temperature is within ±30 ppm//C or within ±10% of the temperature coefficient is not satisfied. Also Sr2Nb
A composition range in which 2O7 is less than 5 moles (!) 1 and!
2XTi21X(0<.x≦1.0) is 80 mol%
Over a larger composition range, the change in temperature coefficient with temperature is ±
The conditions of 30 ppm/° C. or within ±10% of the temperature coefficient and the condition that the dielectric constant value is 30 or more are not satisfied at the same time. Based on the above, the composition range of the present invention is limited to the following composition range.

Claims (1)

【特許請求の範囲】 1 Sr_2Nb_2O_7、Sr_2Ta_2O_7
、1/2Mg_2_xTi_2_−_2_xO_4_−
_2_x(0<x≦1.0)の三成分系において、α〔
Sr_2Nb_2O_7〕・β〔Sr_2Ta_2O_
7〕・γ〔−Mg_2_xTi_2_−_2_xO_4
_−_2_x〕(ただし、α+β+γ=1.0)と表わ
したとき、α、β、γの値が、それぞれ0.05≦α≦
0.65、0<β≦0.6、0.2≦γ≦0.8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。
[Claims] 1 Sr_2Nb_2O_7, Sr_2Ta_2O_7
, 1/2Mg_2_xTi_2_-_2_xO_4_-
In the three-component system of _2_x (0<x≦1.0), α[
Sr_2Nb_2O_7]・β[Sr_2Ta_2O_
7]・γ[-Mg_2_xTi_2_-_2_xO_4
____2_x] (however, α+β+γ=1.0), the values of α, β, and γ are each 0.05≦α≦
A porcelain dielectric material for temperature compensation, characterized in that it has a composition that satisfies the following conditions: 0.65, 0<β≦0.6, 0.2≦γ≦0.8.
JP56212406A 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation Expired JPS593009B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56212406A JPS593009B2 (en) 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56212406A JPS593009B2 (en) 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation

Publications (2)

Publication Number Publication Date
JPS57154713A JPS57154713A (en) 1982-09-24
JPS593009B2 true JPS593009B2 (en) 1984-01-21

Family

ID=16622053

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56212406A Expired JPS593009B2 (en) 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation

Country Status (1)

Country Link
JP (1) JPS593009B2 (en)

Also Published As

Publication number Publication date
JPS57154713A (en) 1982-09-24

Similar Documents

Publication Publication Date Title
JPS593009B2 (en) Porcelain dielectric material for temperature compensation
JPS6229008A (en) Dielectric ceramic composition
JPS5851363B2 (en) Porcelain dielectric material for temperature compensation
US5254278A (en) Lead titanate based piezoelectric ceramic material
JPS593006B2 (en) Porcelain dielectric material for temperature compensation
JPS593010B2 (en) Porcelain dielectric material for temperature compensation
JPS597167B2 (en) Porcelain dielectric material for temperature compensation
JPS593005B2 (en) Porcelain dielectric material for temperature compensation
JPS593008B2 (en) Porcelain dielectric material for temperature compensation
JPH06333426A (en) Dielectric ceramic composition for high frequency
JPS593004B2 (en) Porcelain dielectric material for temperature compensation
JPS593003B2 (en) Porcelain dielectric material for temperature compensation
JPS596001B2 (en) Jikiyu Dentai Zairiyou
JPS593007B2 (en) Porcelain dielectric material for temperature compensation
JPS5835321B2 (en) Ondohoshiyoyoujikiyudenzairiyou
JPS5858761B2 (en) dielectric composition
JPS5858762B2 (en) dielectric composition
JPH0369560A (en) Microwave dielectric ceramics
JPS5857844B2 (en) Porcelain dielectric material for temperature compensation
JP3071529B2 (en) Dielectric porcelain composition
JPS6344710B2 (en)
KR0157635B1 (en) Electrolytic components
JPS5858763B2 (en) dielectric composition
JPS6020852B2 (en) Porcelain dielectric material for temperature compensation
JPS61110904A (en) Dielectric porcelain composition