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JP2676385B2 - Piezoelectric composite material for hydrophone - Google Patents
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JP2676385B2 - Piezoelectric composite material for hydrophone - Google Patents

Piezoelectric composite material for hydrophone

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Publication number
JP2676385B2
JP2676385B2 JP63223342A JP22334288A JP2676385B2 JP 2676385 B2 JP2676385 B2 JP 2676385B2 JP 63223342 A JP63223342 A JP 63223342A JP 22334288 A JP22334288 A JP 22334288A JP 2676385 B2 JP2676385 B2 JP 2676385B2
Authority
JP
Japan
Prior art keywords
piezoelectric
powder
piezoelectric ceramic
synthetic rubber
hydrostatic pressure
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 - Fee Related
Application number
JP63223342A
Other languages
Japanese (ja)
Other versions
JPH0270193A (en
Inventor
幸治 小倉
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.)
Niterra Co Ltd
Original Assignee
NGK Spark Plug 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 NGK Spark Plug Co Ltd filed Critical NGK Spark Plug Co Ltd
Priority to JP63223342A priority Critical patent/JP2676385B2/en
Publication of JPH0270193A publication Critical patent/JPH0270193A/en
Application granted granted Critical
Publication of JP2676385B2 publication Critical patent/JP2676385B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 <産業上の利用分野> 本発明は、合成ゴム等に圧電磁器粉末を配合してなる
ものであり、水中に音波または超音波を送出したり、逆
に水中を伝播する音波または超音波を受波する水中マイ
クロフォン等として応用され得るハイドロフォン用圧電
複合材料に関する。
DETAILED DESCRIPTION OF THE INVENTION <Industrial field of application> The present invention is one in which piezoelectric ceramic powder is blended with synthetic rubber or the like, and sends sound waves or ultrasonic waves into water, or conversely propagates in water. The present invention relates to a piezoelectric composite material for a hydrophone that can be applied as a hydrophone that receives sound waves or ultrasonic waves.

<従来技術> 合成ゴム中にチタン酸鉛などの圧電磁器粉末を混合し
てなる圧電複合材料は、一般の焼結質圧電磁器よりも低
密度で媒質中を伝搬する音波の音速が小さいため、水と
の間に良好な音響的整合が得られ、またその可撓性から
水中深く浸漬しても水圧による影響が小さいので、水中
マイクロフォン等のハイドロフォン用圧電複合材料とし
て好適である。
<Prior Art> A piezoelectric composite material obtained by mixing piezoelectric ceramic powder such as lead titanate in a synthetic rubber has a lower sound velocity of a sound wave propagating in a medium at a lower density than that of a general sinter piezoelectric ceramic. It is suitable as a piezoelectric composite material for a hydrophone such as a hydrophone because it has good acoustic matching with water and its flexibility makes it less susceptible to water pressure even when immersed deep in water.

<発明が解決しようとする課題> ところで、ハイドロフォン用圧電複合材料は、できる
限り水中での受波感度が高いことが要求されるが、受波
感度の高い材料は、受波感度の静水圧力依存性が伴い易
いことが判明した。
<Problems to be Solved by the Invention> Piezoelectric composite materials for hydrophones are required to have as high a wave receiving sensitivity in water as possible. However, a material having a high wave receiving sensitivity is a hydrostatic pressure of the wave receiving sensitivity. It turned out that it is likely to be dependent.

本発明は、この種のハイドロフォン用圧電複合材料に
あって、受波感度が高く、しかも静水圧力依存性の低い
材料を抵抗することを目的とするものである。
An object of the present invention is to resist a piezoelectric composite material for a hydrophone of this type, which has high wave receiving sensitivity and low hydrostatic pressure dependency.

<問題点を解決するための手段> 本発明は、合成ゴム中に圧電磁器粉末を加硫剤と共に
混合し、成形し、さらに分極して得られるハイドロフォ
ン用圧電複合材料において、 前記圧電磁器粉末が、平均粒径を異にする二種以上の
粉末材料からなり、圧電磁器粉末/合成ゴム配合比が、
65〜75(体積%)であることを特徴とするものである。
<Means for Solving Problems> The present invention relates to a piezoelectric composite material for a hydrophone, which is obtained by mixing piezoelectric ceramic powder with a vulcanizing agent in a synthetic rubber, molding the mixture, and further polarizing the piezoelectric ceramic powder. Is composed of two or more kinds of powder materials having different average particle diameters, and the compounding ratio of piezoelectric ceramic powder / synthetic rubber is
It is characterized by being 65 to 75 (volume%).

<作用> 静水圧力依存性は、圧電複合材料内での磁器粉末間の
空気層の介在によるものと考えられる。ところが、平均
粒径を異にする二種以上の粉末材料を、圧電磁器粉末/
合成ゴム配合比が、65〜75(体積%)となる範囲で混合
すると、平均粒径が等しい単一の粉末材料に比して、粒
径の異なる粒子相互が複雑に混合しあって充填効率が向
上し、これにより粒子間の空気層が減少する。このた
め、静水圧力依存性が低下する。
<Operation> It is considered that the hydrostatic pressure dependency is due to the presence of an air layer between the porcelain powders in the piezoelectric composite material. However, two or more kinds of powder materials having different average particle diameters are used as piezoelectric ceramic powder /
When the synthetic rubber compounding ratio is mixed in the range of 65 to 75 (volume%), compared to a single powder material with the same average particle size, particles with different particle sizes are mixed intricately and filling efficiency is improved. Is improved, which reduces the air layer between the particles. Therefore, the hydrostatic pressure dependency is reduced.

ここで圧電ゴムシートの実測密度と、理論密度とのず
れは、圧電磁器粉末/合成ゴム配合比が75%を越えると
急激に低下する。この領域では、圧電ゴムシート内に空
気層が含有されていることが推定され、従ってこの配合
比が上限となる。また、圧電磁器粉末/合成ゴム配合比
が65%未満であると、充分な受波感度を得ることができ
ない。従ってこの配合比が下限となる。
The deviation between the measured density and the theoretical density of the piezoelectric rubber sheet drastically decreases when the piezoelectric ceramic powder / synthetic rubber compounding ratio exceeds 75%. In this region, it is estimated that an air layer is contained in the piezoelectric rubber sheet, and therefore, this compounding ratio becomes the upper limit. Further, if the piezoelectric ceramic powder / synthetic rubber compounding ratio is less than 65%, sufficient wave receiving sensitivity cannot be obtained. Therefore, this mixing ratio becomes the lower limit.

<実施例> 市販の純度99%以上のPbO(平均粒径3μm以下)及
び純度99.5%以上のTiO2をPbTiO3の組成式のもとで配合
し、2.5Kg秤量して振動ミルでアルミナ玉石(3.5Kg)に
て3時間の乾式混合を行なった。この際、振動ミルのポ
ットの内面壁はウレタン樹脂で内張りし、これにより不
純物の混入を防ぐようにした。
<Example> Commercially available PbO with a purity of 99% or more (average particle size of 3 μm or less) and TiO 2 with a purity of 99.5% or more were compounded under the composition formula of PbTiO 3 , 2.5 Kg was weighed, and alumina boulder was added with a vibration mill. Dry mixing was carried out at (3.5 Kg) for 3 hours. At this time, the inner wall of the pot of the vibrating mill was lined with urethane resin to prevent impurities from being mixed.

次に金型を用いて350Kg/cm2の加圧により外形47mm,厚
み5mm,プレス密度4.5g/cm3のタブレットを作り、高アル
ミナ質るつぼで1050℃にて2時間、固相反応を行なっ
た。その後、この高温塊を冷却水槽に投入することによ
って水中急冷を生ぜしめ微粒子を得た。さらに崩壊促進
のためにプロペラ式撹拌機を用いて5時間以上の撹拌を
行なった。こうして形成されたチタン酸鉛粉末を水を切
って100℃,24時間下で乾燥させた後に、篩に通して、二
種類(32μm,7μm)の平均粒径群の磁器粉末を分別し
た。
Next, a tablet with an outer diameter of 47 mm, a thickness of 5 mm, and a press density of 4.5 g / cm 3 is made by pressurizing at 350 Kg / cm 2 using a mold, and a solid phase reaction is performed in a high alumina crucible at 1050 ° C. for 2 hours. It was Thereafter, the high-temperature mass was put into a cooling water tank to cause rapid cooling in water to obtain fine particles. Furthermore, in order to promote disintegration, stirring was carried out for 5 hours or more using a propeller stirrer. The lead titanate powder thus formed was drained of water, dried at 100 ° C. for 24 hours, and then passed through a sieve to separate two types (32 μm, 7 μm) of porcelain powder having an average particle size group.

次に、この二種類の粉末を、32μm/7μmの割合が0
〜100(重量%)の範囲で、25%おきとなるように調合
して、夫々混合し、複数の混合粉末試料を製作した。
Next, the ratio of 32 μm / 7 μm is 0
In the range of up to 100 (wt%), every 25% was prepared and mixed, and a plurality of mixed powder samples were manufactured.

そしてこの各混合粉末に、合成ゴムとしてネオプレン
ゴムからなる合成ゴムを、種々の配合割合で混合した。
このチタン酸鉛混合粉末(圧電磁器粉末)/合成ゴムの
配合比は、50〜80体積%の範囲で、5%おきとなる様に
夫々調合した。さらに加硫剤として、Pb3O4,ZnO及びジ
ベンゾチアジルジスルフィド(商品名;ノクセラーDM)
を混入した。前記加硫剤の配合割合は、合成ゴム100重
量部に対して、Pb3O4:ZnO:ノクセラーDM=20重量部:5重
量部:0.5重量部とした。
Then, each of the mixed powders was mixed with a synthetic rubber made of neoprene rubber as a synthetic rubber in various compounding ratios.
The lead titanate mixed powder (piezoelectric ceramic powder) / synthetic rubber was compounded at a compounding ratio of 50 to 80% by volume, and every 5%. Furthermore, as a vulcanizing agent, Pb 3 O 4 , ZnO and dibenzothiazyl disulfide (trade name; Nocceller DM)
Was mixed. The compounding ratio of the vulcanizing agent was Pb 3 O 4 : ZnO: Noccer DM = 20 parts by weight: 5 parts by weight: 0.5 parts by weight with respect to 100 parts by weight of the synthetic rubber.

さらにこれを小型ロール機でロール成型し、温度170
℃,圧力140Kg/cm2,時間15分の条件のもとで、加硫プレ
ス機により架橋して、厚み1mmtのシート状に成形し、そ
の表裏面に銀ペーストの塗布により、方形状電極を形成
した。
Furthermore, this is roll-molded with a small roll machine, and the temperature is 170
Under the conditions of ℃, pressure 140Kg / cm 2 and time 15 minutes, it is cross-linked by vulcanizing press and molded into a sheet with a thickness of 1mmt. Formed.

そしてこのシートを、20℃の絶縁液中に浸漬し、該液
中で70KV/cmの直流電圧の印加を1時間に渡り継続し、
分極処理し、ハイドロフォン用圧電ゴムシート(圧電複
合材料)を得た。
Then, this sheet was immersed in an insulating solution at 20 ° C., and a DC voltage of 70 KV / cm was continuously applied in the solution for 1 hour,
Polarization treatment was performed to obtain a piezoelectric rubber sheet for a hydrophone (piezoelectric composite material).

そして、各圧電ゴムシートの、所定静水圧力下におけ
る受波感度の変化を測定した。この測定は、フロリーナ
ート液を使用した受波感度測定水槽を使用した。また静
水圧力依存性は5Kg/cm2から150Kg/cm2に変化させた場合
の受波感度の減少値を測定した。
Then, the change in the wave receiving sensitivity of each piezoelectric rubber sheet under a predetermined hydrostatic pressure was measured. For this measurement, a wave receiving sensitivity measurement water tank using a Florinate solution was used. The hydrostatic pressure dependence was measured as the decrease value of the receiving sensitivity when changing from 5 Kg / cm 2 to 150 Kg / cm 2 .

一方、各材料につき理論密度と、実測密度とのずれを
測定した。この密度は、圧電ゴムシートに空中重力及
び、フローリナート液中での重量を測定してもとめ、各
々の原料の密度と、配合比により求めた理論密度と比較
した。
On the other hand, the deviation between the theoretical density and the measured density was measured for each material. The density was determined by measuring the gravity in the air and the weight in the flow linen liquid on the piezoelectric rubber sheet, and compared with the density of each raw material and the theoretical density obtained by the compounding ratio.

また圧電ゴムの加硫成形時の成形のしやすさの目処と
なるML値についてはキュラストメータを使用して測定し
た。
Further, the M L value, which is a target for ease of molding during vulcanization molding of the piezoelectric rubber, was measured using a curast meter.

<実験結果> 第1図は、各配合比での圧電ゴムシートの受波感度を
示す。第2図は各配合比での圧電ゴムシートの受波感度
の静水圧力依存性を示す。
<Experimental Results> FIG. 1 shows the wave receiving sensitivity of the piezoelectric rubber sheet at each compounding ratio. FIG. 2 shows the hydrostatic pressure dependence of the wave receiving sensitivity of the piezoelectric rubber sheet at each compounding ratio.

これらにより圧電磁器粉末/合成ゴムの配合比が60%
までは受波感度が−205〜−206dBと低いが、静水圧力依
存性も1dB以下と小さく、さらに配合比を大きくするこ
とにより受波感度は上昇するが、ほぼこれに比例する様
に静水圧力依存性は大きくなることが解る。
With these, the compounding ratio of piezoelectric ceramic powder / synthetic rubber is 60%.
Up to -205 to -206 dB, the sensitivity to hydrostatic pressure is as low as 1 dB or less. Increasing the blending ratio also increases the sensitivity to waves, but the hydrostatic pressure is almost proportional to this. It can be seen that the dependence increases.

例えば、受波感度が最高となる圧電磁器粉末/合成ゴ
ム配合比=65%、粉末粒径配合比=100%のときには、
−198.4dBと最高感度を示すが、静水圧力依存性も5.3dB
と最高である。一方、2番目に高い受波感度を示す圧電
磁器粉末/合成ゴム配合比=70%、粉末粒径配合比=0
%のときには、−201.1dBであるが、静水圧力依存性は
2.7dBと比較的小さくなる。
For example, when the piezoelectric ceramic powder / synthetic rubber compounding ratio = 65% and the powder particle size compounding ratio = 100%, which gives the highest wave sensitivity,
It shows the highest sensitivity of -198.4 dB, but also has a hydrostatic pressure dependency of 5.3 dB.
And is the best. On the other hand, the piezoelectric ceramic powder / synthetic rubber compounding ratio showing the second highest wave sensitivity = 70%, powder particle size compounding ratio = 0
% Is -201.1 dB, but the hydrostatic pressure dependence is
It is relatively small at 2.7 dB.

尚、第1図から、圧電磁器粉末/合成ゴム配合比が65
%未満であると、充分な受波感度を得ることができない
ことが解る。
From Fig. 1, it can be seen that the compounding ratio of piezoelectric ceramic powder / synthetic rubber is 65
It is understood that if it is less than%, sufficient wave receiving sensitivity cannot be obtained.

次に第3図は、圧電磁器粉末/合成ゴム配合比に対す
るε33 Tの変化、圧電ゴムシートの実測密度と理論
密度とのずれ、及び受波感度の静水圧力依存性を夫々示
す。
Next, FIG. 3 shows the change in ε 33 T / ε 0 with respect to the piezoelectric ceramic powder / synthetic rubber compounding ratio, the deviation between the measured density and the theoretical density of the piezoelectric rubber sheet, and the hydrostatic pressure dependence of the wave sensitivity. .

圧電ゴムシートの実測密度と、理論密度とのずれは、
圧電磁器粉末/合成ゴム配合比=60%間では+3%程度
で、ほぼ一定であるが、これを越えると徐々に低下し、
特に粉末粒径配合比=0%にあっては圧電磁器粉末/合
成ゴム配合比=75%を越える領域で急激に低下する。こ
の領域では、圧電ゴムシート内に空気層が含有されてい
ることが推定される。
The difference between the measured density of the piezoelectric rubber sheet and the theoretical density is
When the compounding ratio of piezoelectric ceramic powder / synthetic rubber is 60%, it is about + 3%, which is almost constant, but when it exceeds this value, it gradually decreases,
In particular, when the powder particle size compounding ratio = 0%, it sharply decreases in the region where the piezoelectric ceramic powder / synthetic rubber compounding ratio = 75%. In this region, it is estimated that the piezoelectric rubber sheet contains an air layer.

ここでε33 Tは、圧電磁器粉末/合成ゴム配合比
を大きくするに従って、ほぼ直線的に大きくなるが、75
%を越える領域では、この直線は下がっており、実測密
度と、理論密度とのずれと良い一致を見せている。
Here, ε 33 T / ε 0 increases almost linearly as the compounding ratio of piezoelectric ceramic powder / synthetic rubber increases, but
In the area exceeding%, this straight line is lowered, showing a good agreement with the deviation between the measured density and the theoretical density.

余論であるが、ポーラスなPZT及び空気層を含んだPVD
Fにおいては、静水圧力依存性が表われ、空気層と静水
圧力依存性は密度に関係していることが報告されてい
る。
As an aside, PVD containing porous PZT and air layer
In F, hydrostatic pressure dependence appears, and it is reported that the air layer and hydrostatic pressure dependence is related to density.

尚、受波感度と静水圧力依存性については、実測密度
と理論密度のずれ及びε33 Tの変化との因果関係
が、図中で表われていない。このことから、空気層と静
水圧力依存性は関係しているが、定量的には他の因子も
導入して検討すべきであることが示唆される。
Regarding the wave sensitivity and the hydrostatic pressure dependency, the causal relationship between the deviation between the measured density and the theoretical density and the change in ε 33 T / ε 0 is not shown in the figure. This suggests that the air layer and hydrostatic pressure dependence are related, but quantitatively, other factors should also be introduced for consideration.

而して、第3図により、圧電磁器粉末/合成ゴム配合
比が、65〜75(体積%)で、二種類の粉末粒径を配合し
たものは、単一平均粒径のものよりも、受波感度を損な
うことなく静圧力依存性が低くなることが解った。
Thus, as shown in FIG. 3, when the piezoelectric ceramic powder / synthetic rubber compounding ratio is 65 to 75 (volume%) and two types of powder particle sizes are compounded, a compound having a single average particle size is It was found that the dependence on static pressure is reduced without impairing the receiving sensitivity.

第4図は、粉末粒径配合比に対する圧電ゴムシートの
実測密度と、理論密度とのずれ、キュラストメータM
L値、受波感度の静水圧力依存性を示す。これにより粉
末粒径配合比=50%近傍で各々の値が極大、極小を示
す。つまり粉末粒径が32μm単独のもの及び7μm単独
のものより、32μmと7μmを50%づつ配合したものの
方が密度大きくなり、キュラストメータML値は小さくな
って成形性が良くなり、静水圧力依存性も小さくできる
ことが解る。これは、異なった圧電磁器粉末の粒径を混
ぜた方が充填効果が高まることにより空気層の量も少な
くすることができるためと考えられる。
Fig. 4 shows the deviation between the measured density and the theoretical density of the piezoelectric rubber sheet with respect to the powder particle size mixture ratio, and the curast meter M
Shows hydrostatic pressure dependence of L value and receiving sensitivity. As a result, each value shows a maximum and a minimum in the vicinity of the powder particle size mixture ratio = 50%. In other words, the powders with 32% and 7 μm mixed in 50% each have a higher density than those with a powder particle size of 32 μm alone and 7 μm alone, and the curability meter M L value becomes smaller, resulting in better moldability and hydrostatic pressure. It can be seen that the dependency can also be reduced. It is considered that this is because mixing the particle diameters of different piezoelectric ceramic powders enhances the filling effect, so that the amount of the air layer can be reduced.

上述の実験では、32μmと7μmの二種類の平均粒径
の粉末材料を混合したものであるが、二種類以上の混合
によっても、充填効率が高まり、静水圧力依存性を低下
することができるものと考えられる。
In the above-mentioned experiment, powder materials having two average particle sizes of 32 μm and 7 μm were mixed, but the mixing efficiency can be increased and the hydrostatic pressure dependency can be reduced by mixing two or more kinds of powder particles. it is conceivable that.

<発明の効果> 本発明の圧電複合材料は、圧電磁器粉末を平均粒径を
異にする二種以上の粉末材料で構成すると共に、圧電磁
器粉末/合成ゴム配合比が、65〜75(体積%)となる範
囲で混合してなるものであり、所要の受波感度を得るこ
とができ、かつ静水圧力依存性が低く、このため、静水
圧力に変化があっても、安定した高出力を得ることがで
きる等の優れた効果がある。
<Effects of the Invention> The piezoelectric composite material of the present invention comprises piezoelectric ceramic powder with two or more kinds of powder materials having different average particle sizes, and the piezoelectric ceramic powder / synthetic rubber compounding ratio is 65 to 75 (volume). %), The required wave receiving sensitivity can be obtained, and the hydrostatic pressure dependency is low. Therefore, even if the hydrostatic pressure changes, a stable high output can be obtained. There is an excellent effect that it can be obtained.

【図面の簡単な説明】[Brief description of the drawings]

第1図は各配合比での圧電ゴムシートの受波感度を示す
グラフ、第2図は各配合比での圧電ゴムシートの受波感
度の静水圧力依存性を示すグラフ、第3図は圧電磁器粉
末/合成ゴム配合比に対するε33 Tの変化、圧電ゴ
ムシートの実測密度と理論密度とのずれ、及び受波感度
の静水圧力依存性を夫々示すグラフ、第4図は粉末粒径
配合比に対する圧電ゴムシートの実測密度と、理論密度
とのずれ、キュラストメータML値、受波感度の静水圧力
依存性を示すグラフである。
1 is a graph showing the wave receiving sensitivity of the piezoelectric rubber sheet at each mixing ratio, FIG. 2 is a graph showing the hydrostatic pressure dependency of the wave receiving sensitivity of the piezoelectric rubber sheet at each mixing ratio, and FIG. 3 is the piezoelectric Graphs showing changes in ε 33 T / ε 0 with respect to porcelain powder / synthetic rubber compounding ratio, deviation between measured density and theoretical density of piezoelectric rubber sheet, and hydrostatic pressure dependence of wave sensitivity, respectively. 6 is a graph showing the difference between the actually measured density and the theoretical density of the piezoelectric rubber sheet with respect to the diameter mixture ratio, the curastometer ML value, and the hydrostatic pressure dependence of the wave receiving sensitivity.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】合成ゴム中に圧電磁器粉末を加硫剤と共に
混合し、成形し、さらに分極して得られるハイドロフォ
ン用圧電複合材料において、 前記圧電磁器粉末が、平均粒径を異にする二種以上の粉
末材料からなり、圧電磁器粉末/合成ゴム配合比が、65
〜75(体積%)であることを特徴とするハイドロフォン
用圧電複合材料。
1. A piezoelectric composite material for a hydrophone obtained by mixing piezoelectric ceramic powder with a vulcanizing agent in a synthetic rubber, molding the mixture, and polarizing the composite, wherein the piezoelectric ceramic powder has different average particle diameters. Composed of two or more types of powder materials, with a piezoelectric ceramic powder / synthetic rubber mixing ratio of 65
Piezoelectric composite material for hydrophone, characterized by being ~ 75 (volume%).
JP63223342A 1988-09-05 1988-09-05 Piezoelectric composite material for hydrophone Expired - Fee Related JP2676385B2 (en)

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JP63223342A JP2676385B2 (en) 1988-09-05 1988-09-05 Piezoelectric composite material for hydrophone

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JPH0270193A JPH0270193A (en) 1990-03-09
JP2676385B2 true JP2676385B2 (en) 1997-11-12

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Publication number Priority date Publication date Assignee Title
US5320910A (en) * 1991-12-09 1994-06-14 Ngk Spark Plug Co., Ltd. Piezoelectric composite material

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* Cited by examiner, † Cited by third party
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JPS5136598A (en) * 1974-09-20 1976-03-27 Matsushita Electric Industrial Co Ltd

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