JPS593003B2 - Porcelain dielectric material for temperature compensation - Google Patents

Porcelain dielectric material for temperature compensation

Info

Publication number
JPS593003B2
JPS593003B2 JP56212399A JP21239981A JPS593003B2 JP S593003 B2 JPS593003 B2 JP S593003B2 JP 56212399 A JP56212399 A JP 56212399A JP 21239981 A JP21239981 A JP 21239981A JP S593003 B2 JPS593003 B2 JP S593003B2
Authority
JP
Japan
Prior art keywords
temperature
dielectric material
temperature coefficient
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
JP56212399A
Other languages
Japanese (ja)
Other versions
JPS57154708A (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 JP56212399A priority Critical patent/JPS593003B2/en
Publication of JPS57154708A publication Critical patent/JPS57154708A/en
Publication of JPS593003B2 publication Critical patent/JPS593003B2/en
Expired legal-status Critical Current

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  • Ceramic Capacitors (AREA)
  • Inorganic Insulating Materials (AREA)

Description

【発明の詳細な説明】 本発明はNd_2Ti_2O_7、Ca2Nb_2O_
7で表示される系、およびNd_2Ti_2O_7、C
a2Nb_2O_7、−Mg2XTi_26−2X04
−2X(ただし0<x<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 relates to Nd_2Ti_2O_7, Ca2Nb_2O_
7, and Nd_2Ti_2O_7,C
a2Nb_2O_7, -Mg2XTi_26-2X04
-2X (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10の値が変わらない
温度補償用磁器誘電材料を提供するものである。
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.
Moreover, the present invention provides a temperature-compensating ceramic dielectric material whose temperature coefficient 10 does not change 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、誘電率が
大きく、誘電損失が小さいことが15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
を保つことが望をれている。
Temperature-compensating porcelain capacitors are often used as circuit elements in communication equipment, color televisions, etc. In this case, it is always desirable to have a high dielectric constant and low dielectric loss, and the temperature coefficient can be set to any specified value. , and it is desired to maintain a constant value with respect to temperature.

これまで、この種類の材料としてSrTiO3、CaT
i03、MgTiO3、ca2ro3等を主成分とす■
0 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30〜1
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±60PFI/゜C以上と大
きい欠点があつた。
Until now, materials of this type include SrTiO3, CaT
Main ingredients include i03, MgTiO3, ca2ro3, etc.■
However, in these materials, those with a small temperature coefficient of dielectric constant have a dielectric constant value of 30 to 1.
6, and furthermore, the temperature dependence of the temperature coefficient, that is, the change in the temperature coefficient with respect to temperature, was as large as ±60 PFI/°C or more.

また、誘電率フ5 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
。そこでそれらの欠点を補う材料の一つとしてLa20
3−TiO2−MgO系の材料が開発された(特開昭4
9−12400)。この系では温度係10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、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。
Further, those having a large temperature coefficient of dielectric constant F5 have a drawback that the temperature coefficient varies greatly with temperature. Therefore, La20 is one of the materials that compensates for these drawbacks.
3-TiO2-MgO based materials were developed (Japanese Unexamined Patent Publication No.
9-12400). In this system, the temperature coefficient 10 has been successfully reduced to almost zero, and the temperature dependence of the temperature coefficient has also been improved to some extent. However, it has been impossible to adjust the temperature coefficient depending on the purpose. The present invention improves these drawbacks.

ノ5 すなわち、Nd_2Ti_2O_7、Ca2Nb
_2O_7で示される系およびNd_2Ti_2O_7
、Ca2Nb_2O_7、−Mg−xTi_22X04
−2X(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
度係数の値が一定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。更に焼成温度も
比較的低温であわ、1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。
No.5 That is, Nd_2Ti_2O_7, Ca2Nb
The system shown as _2O_7 and Nd_2Ti_2O_7
, Ca2Nb_2O_7, -Mg-xTi_22X04
By synthesizing a ceramic dielectric material of the system represented by -2 It has been discovered that this material can be an excellent temperature-compensating porcelain dielectric material that has a constant temperature coefficient of permittivity over a wide temperature range. Furthermore, it has been found that the composition can be fired at a relatively low temperature and is easy to manufacture. The effectiveness of the present invention will be explained below based on Examples.

実施例 2X(0〈X〈1.0)で構成されゐ磁器誘電材料につ
いてはNd2O3、TlO2、CacO3、Nb2O5
、MgOの粉末を、またNd2Ti2O7、Ca2Nb
2O7一Mg2XTl2−2X04−2X(XOO)で
構成される磁器誘電材料}よび、Nd2Ti2O7、C
a2Nb2O7で構成される磁器誘電材料についてはN
d2O3、TiO3、CacO3、Nb2O3の粉末を
各組成に応じて秤量し、ボールミルによつて混合の後沢
過、乾燥し、10000C〜1200℃、2時間の条件
で予焼した。
Example 2 For ceramic dielectric materials composed of X (0<X<1.0), Nd2O3, TlO2, CacO3, Nb2O5
, MgO powder, Nd2Ti2O7, Ca2Nb
2O7-Mg2XTl2-2X04-2X (XOO)} and Nd2Ti2O7, C
For the porcelain dielectric material composed of a2Nb2O7, N
Powders of d2O3, TiO3, CacO3, and Nb2O3 were weighed according to their respective compositions, mixed in a ball mill, filtered, dried, and prefired at 10000C to 1200C for 2 hours.

その後、直径1671tmの円板に加圧成形し1300
0C〜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1KHzの周波数でキャパシタンスブリツジを用いて
測定した。
After that, it was pressure-formed into a disc with a diameter of 1671 tm and
Firing was performed at 0C to 1450C 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. The dielectric constant and dielectric loss were measured using a capacitance bridge at a frequency of 1 KHz.

温度係数は誘電率の値を−3『C.O℃、20℃、55
℃、85゜C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。得られた結
果のうち、代表的な例を第1表に掲げて於いた。
The temperature coefficient is the dielectric constant value -3'C. O℃, 20℃, 55
It was measured at each temperature of 85°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. Among the results obtained, representative examples are listed in Table 1.

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℃までの各温度にふ・ける温度係数
が士の範囲内にあることを示してある。
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表の黒6訃よび應14−1〜14−3の第1表より
明らかなようにNd2Ti2O7、Ca2Nb2O7で
構成される磁器誘電材料、ち・よび〈xく1.0)で構
成される磁器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。
As is clear from Table 1, Black 6, and Table 1 of 14-1 to 14-3, it is composed of a porcelain dielectric material composed of Nd2Ti2O7, Ca2Nb2O7, and <x1.0). Porcelain dielectric materials exhibit excellent properties such as high dielectric constant and low dielectric loss.

更に組成比を調整することにより温度係数の値を、訃よ
そ+260PP[11/0Cから−500PF/℃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±30PIXI1
/℃以内または温度係数の±10%以内に卦さまつてい
る。一方、Nd2Ti2O7が5モル%より少ない組成
範囲およびCa2Nb2O7が95モル%以上の組成範
囲z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±30PP01/゜C以内、あるいは温
度係数の土]0%以内という条件と誘電率の値がtは本
発明の請求範囲外の組成である。
It is clear that by further adjusting the composition ratio, the value of the temperature coefficient can be adjusted in a very wide range from about +260 PP [11/0 C to about -500 PF/°C. Moreover, the change in temperature coefficient with respect to temperature is ±30 PIXI1
/°C or within ±10% of the temperature coefficient. On the other hand, in the composition range where Nd2Ti2O7 is less than 5 mol% and the composition range where Ca2Nb2O7 is 95 mol% or more and the composition range where z is more than 80 mol%, the temperature coefficient changes with temperature within ±30PP01/°C, or the temperature coefficient ]0% or less and the dielectric constant value t is a composition outside the scope of the claims of the present invention.

30以上という条件を同時には満足しない。The conditions of 30 or more are not satisfied at the same time.

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。(1) Nd2Ti2O7、Ca2Nb2O7
の二成分系に卦いて(ト)−α)Nd2Ti2O7、α
Ca2Nb2O7と表わしたとき、αの値がO〈α〈0
.95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。
Based on the above, the composition range of the present invention is limited to the following composition range. (1) Nd2Ti2O7, Ca2Nb2O7
In the binary system of (g) - α) Nd2Ti2O7, α
When expressed as Ca2Nb2O7, the value of α is O〈α〈0
.. A porcelain dielectric material for temperature compensation, characterized in that it has a composition that satisfies the conditions of 95.

(0〈xく1.0)の三成分系において α〔Nd2Tl2O7〕・β〔Ca2Nb2O7〕・γ
〔−Mg2XTi2−2X04−2X〕(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くα〈1.0、0くβく0.95、0〈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。
In the three-component system of (0<x×1.0), α[Nd2Tl2O7], β[Ca2Nb2O7], γ
[-Mg2XTi2-2X04-2X] (α+β
+γ=1.0), the values of α, β, and γ are 0.05 and α<1.0, 0 and β and 0.95 and 0<γ, respectively.
A porcelain dielectric material for temperature compensation, characterized in that it has a composition that satisfies the condition of <0.8.

Claims (1)

【特許請求の範囲】 1 Nd_2Ti_2O_7、Ca_2Nb_2O_7
の二成分系において(1−α)Nd_2Ti_2O_7
・αCa_2Nb_2O_7と表わしたとき、αの値が
0<α<0.95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。 2 Nd_2Ti_2O_7、Ca_2Nb_2O_7
、1/2Mg_2xTi_2−_2xO_4−_2x(
0≦x≦1.0)の三成分系においてα〔La_2Ti
_2O_7〕・β〔Ca_2Nb_2O_7〕・γ〔1
/2Mg_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の値のそれぞれ0.05≦α<1.0、0<β<0
.95、0<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 Nd_2Ti_2O_7, Ca_2Nb_2O_7
In the binary system of (1-α)Nd_2Ti_2O_7
- A porcelain dielectric material for temperature compensation characterized by having a composition in which the value of α, expressed as αCa_2Nb_2O_7, satisfies the condition of 0<α<0.95. 2 Nd_2Ti_2O_7, Ca_2Nb_2O_7
, 1/2Mg_2xTi_2−_2xO_4−_2x(
α[La_2Ti
_2O_7]・β[Ca_2Nb_2O_7]・γ[1
/2Mg_2_xTi_2-_2_xO_4-_2_x
] (however, α+β+γ=1.0), then α, β
, the value of γ is 0.05≦α<1.0, 0<β<0, respectively.
.. 95. A porcelain dielectric material for temperature compensation, characterized in that it has a composition that satisfies the condition of 0<γ<0.8.
JP56212399A 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation Expired JPS593003B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56212399A JPS593003B2 (en) 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56212399A JPS593003B2 (en) 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation

Publications (2)

Publication Number Publication Date
JPS57154708A JPS57154708A (en) 1982-09-24
JPS593003B2 true JPS593003B2 (en) 1984-01-21

Family

ID=16621936

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56212399A Expired JPS593003B2 (en) 1981-12-29 1981-12-29 Porcelain dielectric material for temperature compensation

Country Status (1)

Country Link
JP (1) JPS593003B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6164650A (en) * 1984-09-04 1986-04-03 Konishiroku Photo Ind Co Ltd Automatic document feeder

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6164650A (en) * 1984-09-04 1986-04-03 Konishiroku Photo Ind Co Ltd Automatic document feeder

Also Published As

Publication number Publication date
JPS57154708A (en) 1982-09-24

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