JPH0137806B2 - - Google Patents
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- Publication number
- JPH0137806B2 JPH0137806B2 JP56042965A JP4296581A JPH0137806B2 JP H0137806 B2 JPH0137806 B2 JP H0137806B2 JP 56042965 A JP56042965 A JP 56042965A JP 4296581 A JP4296581 A JP 4296581A JP H0137806 B2 JPH0137806 B2 JP H0137806B2
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- Japan
- Prior art keywords
- dielectric constant
- composition
- value
- product
- 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.)
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- Compositions Of Oxide Ceramics (AREA)
- Ceramic Capacitors (AREA)
- Inorganic Insulating Materials (AREA)
Description
【発明の詳細な説明】
本発明は磁器組成物、特に950℃以下の低温で
焼結でき、誘電率と比抵抗の積が高い誘電体磁器
組成物に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a ceramic composition, particularly a dielectric ceramic composition that can be sintered at a low temperature of 950° C. or lower and has a high product of dielectric constant and specific resistance.
従来、誘電体磁器組成物として、チタン酸バリ
ウム(BaTiO3)などを主成分とする磁器が広く
実用化されていることは周知のとおりである。し
かしながら、BaTiO3などを主成分とするものは
焼結温度が通常1300〜1400℃の高温である。この
ため、これを積層形コンデンサに利用する場合に
は、内部電極としてこの焼結温度に耐え得る材
料、例えば白金、パラジウムなどの高価な貴金属
を使用しなければならず、製造コストが高くつく
という欠点がある。積層形コンデンサを安く作る
ためには、銀、ニツケルなどを主成分とする安価
な金属が使用できるような、できるだけ低温、特
に銀の融点である960℃より低い温度で焼結でき
る磁器が望まれている。 It is well known that porcelain containing barium titanate (BaTiO 3 ) as a main component has been widely put into practical use as a dielectric porcelain composition. However, the sintering temperature of materials whose main component is BaTiO 3 or the like is usually as high as 1300 to 1400°C. Therefore, when using this material in multilayer capacitors, materials that can withstand this sintering temperature must be used for the internal electrodes, such as expensive noble metals such as platinum and palladium, which increases manufacturing costs. There are drawbacks. In order to make multilayer capacitors cheaply, it is desirable to use porcelain that can be sintered at as low a temperature as possible, especially at a temperature lower than 960°C, which is the melting point of silver, and which allows the use of inexpensive metals mainly composed of silver and nickel. ing.
このため1000℃以下で焼結できるPb(Fe2/3
W1/3)O3−Pb(Fe1/2Nb1/2)O3系(特公昭55−
34962号公報参照。)や1050℃以下で焼結できる
(Sr・Pb)TiO3−Pb(Mg1/2W1/2)O3系(特開昭
52−21699号公報参照。)などが提案されている。
ところで磁器組成物を用い、実用的な積層形コン
デンサを作成する時に磁器組成物の特性として多
くの項目が評価されねばならない。誘電率はでき
るだけ大きく、誘電損失はできるだけ小さく、比
抵抗はできるだけ大きく、誘電率の温度変化率は
小さいことなどが基本的に要求される。ここで積
層コンデンサの容量は磁器の誘電率は比例する
が、磁器の厚みに反比例し、重なり合つた電極面
積および積層数に比例するため、誘電率の値は実
用上、絶対的要因ではない。さらに誘電率の温度
変化率は用途により種々許容された範囲があり、
これも絶対的要因ではない。誘電損失(tanδ)は
用途によりある値以下の限定があり、室温で最大
5.0%、望ましくは2.5%以下、が一般に望まれて
いる。 For this reason, Pb (Fe 2/3
W 1/3 ) O 3 −Pb (Fe 1/2 Nb 1/2 )
See Publication No. 34962. ) and (Sr/Pb) TiO 3 −Pb (Mg 1/2 W 1/2 ) O 3 system (JP-A-Sho
See Publication No. 52-21699. ) have been proposed.
By the way, when creating a practical multilayer capacitor using a ceramic composition, many items must be evaluated as the characteristics of the ceramic composition. Basically, it is required that the dielectric constant be as large as possible, the dielectric loss as small as possible, the resistivity as large as possible, and the rate of change of the dielectric constant with temperature as small as possible. Here, the capacitance of a multilayer capacitor is proportional to the dielectric constant of the porcelain, but inversely proportional to the thickness of the porcelain, and proportional to the area of overlapping electrodes and the number of laminated layers, so the value of the dielectric constant is not an absolute factor in practice. Furthermore, there are various allowable ranges for the temperature change rate of dielectric constant depending on the application.
This is also not an absolute factor. Dielectric loss (tanδ) is limited to a certain value depending on the application, and the maximum value is at room temperature.
5.0%, preferably 2.5% or less, is generally desired.
比抵抗に関しては、例えばEIAJ規格(日本電
子機械工業会の電子機器用積層磁器コンデンサ
(チツプ形)RC−3698Bに述べられているごと
く、積層コンデンサの絶縁抵抗として10000MΩ
以上または容量・抵抗積(CXR)で500μF・MΩ
以上のいずれか小さい方以上と規定されている。
すなわち磁器組成物の誘電率と比抵抗の積がある
絶対値以上なければ、任意の容量、特に大きな容
量のコンデンサを実用的規格に合せることができ
ず、その用途が非常に限定され、実用的な意味が
なくなる。この点を詳しく説明すると次の様にな
る。積層コンデンサでは、n+1個の内部電極を
構成して一般にn個の同じ厚さの層からなる単一
層コンデンサが積層された構造になつている。こ
の場合、単一層当りの容量をC0、絶縁抵抗をR0
とすれば積層コンデンサのCはC0のn倍になり、
絶縁抵抗RはR0の1/nになる。ここで磁器組
成物の誘電率をε、真空の誘電率をε0、磁器組成
物の比抵抗をρ、単一層コンデンサの磁器の厚さ
をd、重さなる電極面積をSとすれば、単一層コ
ンデンサのC0は(ε0εS)/dとなり、R0は
(ρd)/sとなる。従つてn層からなる積層コン
デンサの容量と絶縁抵抗の積C×Rは〔(ρd)/
(ns)〕×〔nε0εS)/d〕=ε0ερとなる。すなわ
ちど
のような容量の積層コンデンサもそのC×Rは磁
器組成物のεとρの積にε0を乗じた一定値に規格
化される。C×Rが500μF・MΩすなわち500F・
Ω以上ということは、ε0=8.855×10-14F/cmよ
り8.855×10-14×ε×ρ(F/cm)≧500F・Ω、よ
つてερ≧5.65×1015Ω・cmなる要求がある。例え
ばε=10000ではρ≧5.65×1011Ω・cm、ε=3000
ではρ≧1.88×1012Ω・cm、ε=500ではρ≧1.13
×1013Ω・cmが要求される。誘電率に応じてこれ
らの値以上のρを持つ磁器組成物であればどのよ
うな大きな容量の積層コンデンサも500μF・MΩ
を満足する。もしεが3000でρが要求値より1桁
低い1.88×1011Ω・cmとすればε0ερ=50μF・MΩ
で500μF・MΩは満足せず、絶縁抵抗として
10000MΩすなわち1010Ω以上を満足するには容量
Cとして0.005μF以下に限定されねばならない。
それはこの積層コンデンサのC×Rは常に
50μF・MΩを示しているのでRが10000MΩのと
きCは0.005μFとなり、Cがこれより大きければ
Rは10000MΩより小さくなる。0.005μFが規格を
満たす最高の容量となる。従つて磁器組成物の比
抵抗が低いとその材料の実用性、特に積層形コン
デンサの特長である小型、大容量の特長を生かす
ことはできないし、全く意味のないことにもな
る。よつて磁器組成物の比抵抗と誘電率の積があ
る値以上持つことが実用上極めて重要なことであ
る。 Regarding resistivity, for example, as stated in the EIAJ standard (Japan Electronics Industry Association's Multilayer Ceramic Capacitors (Chip Type) RC-3698B), the insulation resistance of a multilayer capacitor is 10000MΩ.
or more than 500μF・MΩ in capacitance/resistance product (CXR)
It is defined as the smaller of the above.
In other words, unless the product of the permittivity and resistivity of the ceramic composition exceeds a certain absolute value, a capacitor of any capacitance, especially a large capacitance, cannot be made to meet practical standards, and its uses are extremely limited and it is not practical. It loses its meaning. This point will be explained in detail as follows. A multilayer capacitor has a structure in which single-layer capacitors are stacked, generally consisting of n layers of the same thickness and forming n+1 internal electrodes. In this case, the capacitance per single layer is C 0 and the insulation resistance is R 0
Then, C of the multilayer capacitor becomes n times C0 ,
The insulation resistance R is 1/n of R 0 . Here, if the permittivity of the ceramic composition is ε, the permittivity of vacuum is ε 0 , the specific resistance of the ceramic composition is ρ, the thickness of the ceramic of the single-layer capacitor is d, and the area of the weighted electrode is S, then C 0 of a single layer capacitor becomes (ε 0 εS)/d, and R 0 becomes (ρ d )/s. Therefore, the product C×R of capacitance and insulation resistance of a multilayer capacitor consisting of n layers is [(ρ d )/
(ns)]×[nε 0 εS)/d]=ε 0 ερ. That is, C×R of a multilayer capacitor of any capacity is normalized to a constant value obtained by multiplying the product of ε and ρ of the ceramic composition by ε 0 . C×R is 500μF・MΩ, that is, 500F・
Ω or more means that ε 0 = 8.855×10 -14 F/cm, so 8.855×10 -14 ×ε×ρ (F/cm)≧500F・Ω, and therefore ερ≧5.65×10 15 Ω・cm. There is. For example, when ε=10000, ρ≧5.65×10 11 Ω・cm, ε=3000
Then, ρ≧1.88×10 12 Ω・cm, and when ε=500, ρ≧1.13
×10 13 Ω・cm is required. Any large capacitance multilayer capacitor of porcelain composition with ρ greater than these values depending on the dielectric constant is 500μF・MΩ.
satisfy. If ε is 3000 and ρ is 1.88×10 11 Ω・cm, which is one order of magnitude lower than the required value, then ε 0 ερ=50μF・MΩ
500μF・MΩ is not satisfied, and the insulation resistance is
In order to satisfy 10000 MΩ, that is, 10 10 Ω or more, the capacitance C must be limited to 0.005 μF or less.
That is, the C×R of this multilayer capacitor is always
Since it shows 50μF・MΩ, when R is 10000MΩ, C will be 0.005μF, and if C is larger than this, R will be smaller than 10000MΩ. 0.005μF is the highest capacitance that meets the standard. Therefore, if the specific resistance of the ceramic composition is low, the practicality of the material, especially the features of multilayer capacitors such as small size and large capacity, cannot be taken advantage of, and it is completely meaningless. Therefore, it is extremely important from a practical standpoint that the product of resistivity and dielectric constant of the ceramic composition is greater than a certain value.
ところでPb(Mg1/2W1/2)O3−PbTiO3系磁器組
成物については既にN.N.Krainik and A.I.
Aqranovskaya(Fiziko Tverdoqo Tela、Vo.2、
No.1、pp70〜72、Janoary 1960)より提案があ
り、(SrxPb1-xTiO3)a(PbMg0.5W0.5O3)b〔だた
しx=0〜0.10、aは0.35〜0.5、bは0.5〜0.65で
あり、そしてa+b=1〕についてモノリシツク
コンデンサおよびその製造方法として特開昭52−
21662号公報に開示され、また誘電体粉末組成物
として特開昭52−21699号公報に開示されている。
更にPb(Mg1/2W1/2)O3とPbTiO3を主とする組成
物であつて、Pb(Mg1/2W1/2)O3が20.0〜70.0モル
%、PbTiO3が30.0〜80.0モル%の範囲の組成物
に対しMgO量を計算値の30%以下添加含有した
ことを特徴とする高誘電率磁器組成物が特開昭55
−144609号公報として開示されている。しかしな
がらいずれも比抵抗に関する開示は全くされてお
らず、Pb(Mg1/2W1/2)O3−PbTiO3系磁器組成物
の実用性は明らかであつた。 By the way, Pb (Mg 1/2 W 1/2 ) O 3 −PbTiO 3 based porcelain compositions have already been reported by NNKrainik and AI.
Aqranovskaya (Fiziko Tverdoqo Tela, Vo.2,
No. 1, pp70-72, Janoary 1960), there is a proposal: (Sr x Pb 1-x TiO 3 ) a (PbMg 0.5 W 0.5 O 3 ) b 0.5;
It is disclosed in Japanese Patent Laid-Open No. 21662, and also disclosed as a dielectric powder composition in Japanese Patent Application Laid-open No. 21699/1983.
Furthermore, it is a composition mainly composed of Pb(Mg 1/2 W 1/2 ) O 3 and PbTiO 3 , in which Pb(Mg 1/2 W 1/2 ) O 3 is 20.0 to 70.0 mol%, and PbTiO 3 is A high dielectric constant porcelain composition characterized by containing an amount of MgO of 30% or less of the calculated value in a composition in the range of 30.0 to 80.0 mol% was disclosed in Japanese Patent Application Laid-Open No. 1983-1999.
-Disclosed as Publication No. 144609. However, none of them disclosed any specific resistance, and the practicality of the Pb(Mg 1/2 W 1/2 )O 3 --PbTiO 3 ceramic composition was clear.
本発明の目的は910℃〜950℃の温度で焼結で
き、静電率と比抵抗の積ερが5.65×1015Ω・cm、
すなわちε0ερが500F・Ω以上の値を持つ磁器組
成物を提供することにある。 The object of the present invention is that it can be sintered at a temperature of 910℃ to 950℃, the product ερ of electrostatic constant and specific resistance is 5.65×10 15 Ω・cm,
That is, the object is to provide a ceramic composition having a value of ε 0 ερ of 500 F·Ω or more.
本発明はPb(Mg1/2W1/2)O3−PbTiO3素二成分
からなりこれを〔Pb(Mg1/2W1/2)O3〕x
〔PbTiO3〕1-xと表わした時に0.7<x≦1.00の範囲
にあり、910℃〜950℃の温度で焼結でき、誘電率
と比抵抗の積が5.65×1015Ω・cm以上を持つこと
を特長とする磁器組成物である。 The present invention consists of a binary component of Pb(Mg 1/2 W 1/2 )O 3 -PbTiO 3 , which is combined into [Pb(Mg 1/2 W 1/2 )O 3 ] x
[PbTiO 3 ] When expressed as 1-x , it is in the range of 0.7<x≦1.00, can be sintered at a temperature of 910℃ to 950℃, and has a product of dielectric constant and specific resistance of 5.65×10 15 Ω・cm or more. It is a porcelain composition that is characterized by having
次に優れた特性を示す本発明を実施例にて詳細
に説明する。 Next, the present invention, which exhibits excellent characteristics, will be explained in detail with reference to Examples.
実施例
出発原料として純度99.9%以上の酸化鉛
(PbO)、酸化マグネシウム(MgO)、酸化タング
ステン(WO3)および酸化(TiO2)を使用し、
所定の配合比に秤量する。次にボールミル中で湿
式混合した後750〜800℃で予焼した。その後ボー
ルミルで粉砕し、別、乾燥後、有機バインダー
を入れ整粒後プレスし、直径16mm、厚さ約2mmの
円板を4枚作成した。次に空気中910〜950℃で1
時間焼結した。焼結した円板の上下面に銀電極を
焼付け、デジタルLCRメーターで周波数1KHz、
電圧1Vr.m.s.で容量と誘電損失(tanδ)を測定
し、誘電率を算出した。次に超絶縁抵抗計で50V
の電圧を1分間印加して絶縁抵抗を測定し、比抵
抗を算出した。4個の試料の平均値をとり、その
値をもつて配合比xの代表値とした。第1図に誘
電率(ε)の結果を、第2図に誘電損失(tanδ)
の結果を、第3図に誘電率(ε)と比抵抗(ρ)
の積に真空の誘電率(ε0)を乗じた結果をそれぞ
れ焼結温度をパラメーターにして示す。Example Using lead oxide (PbO), magnesium oxide (MgO), tungsten oxide (WO 3 ) and oxide (TiO 2 ) with a purity of 99.9% or more as starting materials,
Weigh to the predetermined mixing ratio. Next, after wet mixing in a ball mill, the mixture was pre-baked at 750-800°C. Thereafter, it was ground in a ball mill, separated and dried, and an organic binder was added thereto for sizing and pressing to produce four discs each having a diameter of 16 mm and a thickness of about 2 mm. Next, 1 at 910-950℃ in air.
Sintered for hours. Silver electrodes were baked on the top and bottom surfaces of the sintered disk, and a frequency of 1KHz was measured using a digital LCR meter.
The capacitance and dielectric loss (tan δ) were measured at a voltage of 1 Vr.ms, and the dielectric constant was calculated. Next, check 50V using a super insulation resistance tester.
The voltage was applied for 1 minute, the insulation resistance was measured, and the specific resistance was calculated. The average value of the four samples was taken, and that value was taken as the representative value of the blending ratio x. Figure 1 shows the results of dielectric constant (ε), and Figure 2 shows dielectric loss (tanδ).
Figure 3 shows the results of dielectric constant (ε) and specific resistance (ρ).
The results of multiplying the product by the vacuum dielectric constant (ε 0 ) are shown using the sintering temperature as a parameter.
第1図よりxが減るとεは増加している。xが
0.6では焼結温度によるεの値が大きく変動して
いることがわかる。第2図よりxが減るとtanδが
大きくなつている。第3図よりε0ερはxが0.9付
近で最大を示し、特にxが小さくなると急激に小
さくなる。xが0.65より大きければ910〜950℃で
焼結しても常に500MΩ・μF以上を実現している。
すなわち本発明の組成物は910〜950℃という低温
で焼結でき誘電率と比抵抗の積が高く、ε0ερとし
て500MΩ・μF以上を実現し、かつtanδも小さく、
積層コンデンサ用磁器組成物として優れた特長を
有している。なお本発明の磁器組成物はPb
(Mg1/2Ti1/2)xTi1-xO3からなり0.7<x≦1.00に限
定される。 From FIG. 1, as x decreases, ε increases. x is
At 0.6, it can be seen that the value of ε varies greatly depending on the sintering temperature. From Figure 2, tan δ increases as x decreases. From FIG. 3, ε 0 ερ reaches its maximum when x is around 0.9, and decreases rapidly especially as x becomes smaller. If x is larger than 0.65, even if sintered at 910 to 950°C, a value of 500MΩ・μF or more will always be achieved.
That is, the composition of the present invention can be sintered at a low temperature of 910 to 950°C, has a high product of dielectric constant and specific resistance, achieves ε 0 ερ of 500 MΩ・μF or more, and has a small tan δ.
It has excellent features as a ceramic composition for multilayer capacitors. Note that the porcelain composition of the present invention contains Pb
(Mg 1/2 Ti 1/2 ) x Ti 1-x O 3 and is limited to 0.7<x≦1.00.
その理由はx≦0.7ではε0ερが小さくなるため
である。 The reason is that ε 0 ερ becomes small when x≦0.7.
以上本発明の磁器組成物は910〜950℃という低
温で焼結でき、銀やニツケルなどの低価格金属を
使用できると共に、省エネルギーや炉材の節約と
いう経済的な観点および誘電率と比抵抗の積が高
いという特性的な観点をみても極めて実用的な材
料となつている。 As described above, the porcelain composition of the present invention can be sintered at a low temperature of 910 to 950°C, and low-cost metals such as silver and nickel can be used. It is an extremely practical material from the viewpoint of its characteristics, such as its high product density.
第1図〜第3図はそれぞれ本発明の磁器組成物
の配合比と諸特性の関係を示すものであり、第1
図に誘電率(ε)を、第2図に誘電損失(tanδ)
を、第3図に誘電率(ε)と比抵抗(ρ)の積に
真空の誘電率(ε0)を乗じた値をそれぞれ焼結温
度をパラメーターにして示す。
Figures 1 to 3 respectively show the relationship between the blending ratio and various properties of the porcelain composition of the present invention.
The figure shows the dielectric constant (ε), and the figure 2 shows the dielectric loss (tanδ).
FIG. 3 shows the product of the dielectric constant (ε) and specific resistance (ρ) multiplied by the vacuum permittivity (ε 0 ), each with the sintering temperature as a parameter.
Claims (1)
(Mg1/2W1/2)O3]とチタン酸鉛[PbTiO3]から
なる2成分組成物を[Pb(Mg1/2W1/2)O3]x
[PbTiO3]1-xと表わした時に、xが0.7<x≦1.00
の範囲にあり、誘電率と比抵抗の積が5.65×
1015Ω・cm以上であることを特徴とする磁器組成
物。1 Magnesium lead tungstate [Pb
(Mg 1/2 W 1/2 )O 3 ] and lead titanate [PbTiO 3 ], [Pb(Mg 1/2 W 1/2 )O 3 ] x
[PbTiO 3 ] When expressed as 1-x , x is 0.7<x≦1.00
is in the range of , and the product of permittivity and resistivity is 5.65×
A porcelain composition characterized by having a resistance of 10 to 15 Ω·cm or more.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56042965A JPS57157407A (en) | 1981-03-24 | 1981-03-24 | Porcelain composition |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56042965A JPS57157407A (en) | 1981-03-24 | 1981-03-24 | Porcelain composition |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57157407A JPS57157407A (en) | 1982-09-29 |
| JPH0137806B2 true JPH0137806B2 (en) | 1989-08-09 |
Family
ID=12650741
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56042965A Granted JPS57157407A (en) | 1981-03-24 | 1981-03-24 | Porcelain composition |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57157407A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55144609A (en) * | 1979-04-28 | 1980-11-11 | Tdk Electronics Co Ltd | High dielectric series porcelain composition |
-
1981
- 1981-03-24 JP JP56042965A patent/JPS57157407A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57157407A (en) | 1982-09-29 |
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