JP2878302B2 - Piezoelectric vibrator and manufacturing method thereof - Google Patents
Piezoelectric vibrator and manufacturing method thereofInfo
- Publication number
- JP2878302B2 JP2878302B2 JP9151789A JP9151789A JP2878302B2 JP 2878302 B2 JP2878302 B2 JP 2878302B2 JP 9151789 A JP9151789 A JP 9151789A JP 9151789 A JP9151789 A JP 9151789A JP 2878302 B2 JP2878302 B2 JP 2878302B2
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- Japan
- Prior art keywords
- ferroelectric
- piezoelectric vibrator
- powder
- porous
- porosity
- 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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- Piezo-Electric Transducers For Audible Bands (AREA)
- Transducers For Ultrasonic Waves (AREA)
Description
本発明は、超音波を送受信する圧電振動子、特に複数
の共振周波数の超音波を発生する圧電振動子とその製造
方法に関するものである。The present invention relates to a piezoelectric vibrator that transmits and receives ultrasonic waves, and more particularly to a piezoelectric vibrator that generates ultrasonic waves having a plurality of resonance frequencies and a method of manufacturing the same.
超音波は人体に無害であり、また非破壊により異物を
検知することができるため、医療、漁業等の広い範囲に
使用されている。超音波を生体または海中に伝搬させた
とき、伝搬体が均質であれば反射波は生じないが、伝搬
体に音響インピーダンスの異なる部分が存在すると、そ
の部分で反射波を生じる。この反射波の大きさ、受波ま
での時間を測定することにより、その異物の位置、性質
を観察できる。例えば医療分野では腫瘍の検査、胎児あ
るいは心臓の観察等に応用されており、漁業分野では魚
群、海底地形あるいは障害物等の探査のために応用され
ている。 超音波の周波数は観察する対象により異なる。周波数
が高い超音波は、解像度が高いため微細な異物を観察で
きる。反面、伝搬損失が大きいため伝搬距離は短くな
る。一方、周波数が低い超音波は、前者と比較すると微
細な異物の観察は困難になる反面、超音波の伝搬距離は
長くなる。 これらの超音波は、例えばチタン酸バリウムBaTiO3、
チタン酸鉛PbTiO3、ジルコン酸チタン酸鉛Pb(Zr,Ti)O
3(PZT)等の強誘電体セラミックスからなる圧電振動子
に電圧を印加することにより発生させる。そして超音波
の用途に応じて圧電振動子の形状や寸法を決めることに
より共振周波数を制御している。しかし寸法が定まった
1個の圧電振動子から任意の複数の周波数を持つ超音波
を発生させるのは困難である。従来、複数の周波数の超
音波を発生させるためには、圧電振動子の振動モードと
して例えば径振動及び厚み振動を応用するか、異なった
共振周波数を持つ複数の圧電振動子を複数個配列してい
る。 医療、漁業分野では圧電振動子材料としてジルコン酸
チタン酸鉛が多用されている。これはジルコン酸鉛PbZr
O3とチタン酸鉛PbTiO3の二成分系であり、その組成比を
変化させることにより特性の多様化が図られている。し
かし形状、寸法の定まった1個の圧電振動子1に任意の
複数の周波数を持たせることは、この材質であっても困
難である。通常、探触子には圧電振動子の異なった振動
モードによる異なった共振周波数、またはそれら共振周
波数の和または差による異なった共振周波数を用いなけ
ればならない。また共振周波数と圧電振動子の厚さの積
である周波数定数の異なるものを、行列状または環状に
複数配列することにより得られる複数の素子からの異な
った共振周波数を用いなければなかった。Ultrasonic waves are harmless to the human body and can detect foreign substances by non-destruction, and are therefore used in a wide range of fields such as medical treatment and fishing. When an ultrasonic wave is propagated in a living body or in the sea, a reflected wave is not generated if the propagator is homogeneous, but if a portion having a different acoustic impedance is present in the propagator, a reflected wave is generated in that portion. By measuring the magnitude of the reflected wave and the time until reception, the position and properties of the foreign matter can be observed. For example, in the medical field, it is applied to inspection of tumors, observation of fetuses or hearts, and in the field of fishery, it is applied to exploration of fish schools, marine topography, obstacles, and the like. The frequency of the ultrasonic wave differs depending on the object to be observed. Ultrasonic waves having a high frequency can observe fine foreign matters because of their high resolution. On the other hand, the propagation distance is short because the propagation loss is large. On the other hand, in the case of an ultrasonic wave having a low frequency, it is more difficult to observe a fine foreign substance than in the former case, but the propagation distance of the ultrasonic wave becomes longer. These ultrasonic waves are, for example, barium titanate BaTiO 3 ,
Lead titanate PbTiO 3 , lead zirconate titanate Pb (Zr, Ti) O
3 Generated by applying voltage to a piezoelectric vibrator made of ferroelectric ceramics such as (PZT). The resonance frequency is controlled by determining the shape and size of the piezoelectric vibrator according to the application of the ultrasonic wave. However, it is difficult to generate ultrasonic waves having arbitrary plural frequencies from one piezoelectric vibrator whose dimensions are determined. Conventionally, in order to generate ultrasonic waves of a plurality of frequencies, for example, radial vibration and thickness vibration are applied as vibration modes of the piezoelectric vibrator, or a plurality of piezoelectric vibrators having different resonance frequencies are arranged. I have. In the medical and fishery fields, lead zirconate titanate is frequently used as a piezoelectric vibrator material. This is lead zirconate PbZr
It is a binary system of O 3 and lead titanate PbTiO 3 , and the characteristics are diversified by changing the composition ratio. However, it is difficult to provide a plurality of arbitrary frequencies to one piezoelectric vibrator 1 having a fixed shape and dimensions. In general, the probe must use different resonance frequencies due to different vibration modes of the piezoelectric vibrator, or different resonance frequencies depending on the sum or difference of the resonance frequencies. Further, it is necessary to use different resonance frequencies from a plurality of elements obtained by arranging a plurality of elements having different frequency constants, which are products of the resonance frequency and the thickness of the piezoelectric vibrator, in a matrix or ring.
【発明が解決しようとする課題】 しかしながら、1個の圧電振動子の異なった共振周波
数を用いる場合、圧電振動子の直径、厚さ、つまり圧電
振動子の形状、寸法により目的とする周波数で干渉する
場合があり、周波数の設定が困難になるという問題があ
った。 また圧電振動子材料自身の周波数定数が異なるものを
複数配列する場合、探触子の形状が複雑且つ大型になる
という問題があった。個別の振動子に各々電気的な結合
も必要になり、必然的に製造工程及び構造が複雑になる
という問題もあった。 本発明は、上記の問題を除去するためになされたもの
であり、1個の圧電振動子に複数の共振周波数を持たせ
ることにより振動子の構成部品の削減、コスト低減及び
小型化、高性能化した圧電振動子を得ることを目的とす
るものである。However, when different resonance frequencies of one piezoelectric vibrator are used, interference occurs at a target frequency depending on the diameter and thickness of the piezoelectric vibrator, that is, the shape and size of the piezoelectric vibrator. In some cases, it is difficult to set the frequency. Further, when a plurality of piezoelectric vibrator materials having different frequency constants are arranged, there is a problem that the shape of the probe becomes complicated and large. Each of the individual vibrators also needs to be electrically coupled, which inevitably complicates the manufacturing process and structure. SUMMARY OF THE INVENTION The present invention has been made to eliminate the above-described problem. By providing a plurality of resonance frequencies to one piezoelectric vibrator, the number of components of the vibrator can be reduced, the cost can be reduced, and the size can be reduced. It is an object of the present invention to obtain a piezoelectric vibrator.
上記課題を解決するため、本発明者らは多孔質圧電振
動子について研究を重ねた。その結果、単位体積当たり
に占める空孔の比率、すなわち空孔率の異なる多孔質圧
電振動子の電圧特性は、第4図の空孔率と周波数定数の
特性図に示すように、空孔率の変化により共振周波数と
圧電振動子の厚さの積である周波数定数が異なることを
見出した。そのため一個の圧電振動子に空孔率が異なる
領域を設けると、異なる共振周波数が得られる。 複数の領域を持つ多孔質圧電振動子は、圧電振動子の
大部分を通常の強誘電体とし、一部の領域を多孔質構造
に形成すればよく、強誘電体原料粉末と強誘電体粉末の
中に強誘電体の焼成温度により低温で気化する粉体(気
化性粉末)を混合したものを一体に形成し焼成し、さら
に分極処理することにより得られる。 しかし焼成のとき、異なる材料の境界部分で熱膨張率
の差が大きいと、熱応力により焼結体が破壊する場合が
ある。そこで空孔率が異なる圧電振動子について熱膨張
率を測定した結果、緻密なジルコン酸チタン酸鉛と、空
孔率35%を持つジルコン酸チタン酸鉛の温度と膨張係数
とには第5図に示す特性があることを見出した。同図に
おいて、Aは緻密なジルコン酸チタン酸鉛、Bは空孔率
35%を持つジルコン酸チタン酸鉛の特性を示す。この特
性によれば固相反応領域である500℃以上の温度におい
ては、両者の熱膨張率の差が小さいことがわかった。空
孔率35%未満の領域でもこの関係は成り立っている。し
かし空孔率が35%を越えると500℃以上での熱膨張率の
差が大きくなる。このため緻密なジルコン酸チタン酸鉛
と、空孔率35%以上のジルコン酸チタン酸鉛を一体に焼
成したとき、破壊が生じやすいことがわかった。 この結果、一部の領域に多孔質構造を持つか、多孔質
化した圧電振動子の一部の領域に空孔率の異なる多孔質
構造を持たせることにより、各領域で各々異なった共振
周波数をもたせることができる。空孔率が35%未満であ
ると機械的強度の大きい安定した焼結体が得られること
が確認できた。 上記のような知見の下になされた本発明を、実施例に
対応する図面を参照して説明すると以下のとおりであ
る。 本発明の第1発明の圧電振動子1(第1図参照)は、
緻密な強誘電体3からなる内柱部と多孔質化した強誘電
体2からなる外筒部とを一体化して焼成し、緻密な強誘
電体と該多孔質化した強誘電体が並列する方向に、分極
処理を施してあることを特徴としている。 本発明の第2発明の圧電振動子8(第2図参照)は、
空孔率が互いに異なって多孔質化した複数の強誘電体2
および9の一方を内柱部、別な方を筒部とし一体化して
焼成し、複数の強誘電体が並列する方向に、分極処理を
施してあることを特徴としている。 本発明の第3発明の圧電振動子は、前記第1発明また
は第2発明の多孔質化した強誘電体の空孔率が35%まで
の範囲にあることを特徴としている。 本発明の第4発明の圧電振動子は、前記第1発明、第
2発明または第3発明の強誘電体がジルコン酸チタン酸
鉛、チタン酸バリウム、チタン酸鉛から選ばれる物質で
あることを特徴としている。 本発明の第5発明の圧電振動子の製造方法は、多孔質
化した強誘電体2と緻密な強誘電体3が隣接する圧電振
動子1(第1図参照)を製造する方法であり、仕切り6
を有する型4(第3図参照)内の一方側2aに強誘電体の
原料粉末と、その強誘電体を焼成する温度より低い温度
で気化する粉体とを混合して型入れし、その型4内のも
う一方側3aに強誘電体だけを型入れし、仕切り6を型4
から取り去り成形する。それを加熱して粉体を気化さ
せ、強誘電体を焼成する。そして分極処理をする。 本発明の第6発明の圧電振動子の製造方法は、隣接し
て異なった空孔率で多孔質化した強誘電体2および9の
圧電振動子8(第2図参照)を製造する方法であり、仕
切り6を有する型4(第3図参照)内の一方側2aに強誘
電体の原料粉末と該強誘電体を焼成する温度より低い温
度で気化する粉体とを混合して型入れし、その型4内の
もう一方側3aに強誘電体の原料粉末と気化性粉体とを前
記とは異なった比率で混合して型入れし、仕切り6を型
から取り去り成形する。それを加熱して粉体を気化さ
せ、強誘電体を焼成する。そして分極処理をする。In order to solve the above problems, the present inventors have repeated research on a porous piezoelectric vibrator. As a result, the ratio of the porosity per unit volume, that is, the voltage characteristics of the porous piezoelectric vibrators having different porosity, are as shown in the porosity and frequency constant characteristic diagram of FIG. It has been found that the frequency constant, which is the product of the resonance frequency and the thickness of the piezoelectric vibrator, is different due to the change in. Therefore, if regions having different porosity are provided in one piezoelectric vibrator, different resonance frequencies can be obtained. For a porous piezoelectric vibrator having multiple regions, most of the piezoelectric vibrator may be made of a normal ferroelectric, and some regions may be formed in a porous structure. A mixture of powder (vaporizable powder) that evaporates at a low temperature depending on the firing temperature of the ferroelectric substance is integrally formed, fired, and further subjected to a polarization treatment. However, if the difference in the coefficient of thermal expansion is large at the boundary between different materials during firing, the sintered body may be broken by thermal stress. The thermal expansion coefficient of piezoelectric vibrators having different porosity was measured. As a result, the temperature and expansion coefficient of dense lead zirconate titanate and lead zirconate titanate having porosity of 35% are shown in FIG. Have the following characteristics. In the same figure, A is a dense lead zirconate titanate, and B is a porosity.
Shows the properties of lead zirconate titanate with 35%. According to this characteristic, the difference in the coefficient of thermal expansion between the two was small at a temperature of 500 ° C. or higher, which is the solid-phase reaction region. This relationship holds even in a region having a porosity of less than 35%. However, if the porosity exceeds 35%, the difference in the coefficient of thermal expansion at 500 ° C. or more increases. For this reason, it was found that when the dense lead zirconate titanate and the lead zirconate titanate having a porosity of 35% or more were integrally fired, breakage easily occurred. As a result, by providing a porous structure in some regions or a porous structure having a different porosity in some regions of a piezoelectric vibrator that has been made porous, the resonance frequency differs in each region. Can be provided. It was confirmed that when the porosity was less than 35%, a stable sintered body having high mechanical strength was obtained. The present invention based on the above knowledge will be described below with reference to the drawings corresponding to the embodiments. The piezoelectric vibrator 1 of the first invention of the present invention (see FIG. 1)
The inner pillar portion made of the dense ferroelectric material 3 and the outer cylindrical portion made of the porous ferroelectric material 2 are integrated and fired, and the dense ferroelectric material and the porous ferroelectric material are arranged in parallel. It is characterized in that a polarization process is performed in the direction. The piezoelectric vibrator 8 of the second invention of the present invention (see FIG. 2)
Plurality of ferroelectrics 2 having different porosity and made porous
And 9 are made into an inner pillar portion and the other is made into a cylindrical portion, and are integrally fired, and are subjected to a polarization treatment in a direction in which a plurality of ferroelectrics are arranged in parallel. A piezoelectric vibrator according to a third invention of the present invention is characterized in that the porosity of the porous ferroelectric material according to the first invention or the second invention is in a range up to 35%. A piezoelectric vibrator according to a fourth invention of the present invention is characterized in that the ferroelectric substance of the first invention, the second invention or the third invention is a substance selected from lead zirconate titanate, barium titanate and lead titanate. Features. The method for manufacturing a piezoelectric vibrator according to the fifth invention of the present invention is a method for manufacturing a piezoelectric vibrator 1 (see FIG. 1) in which a ferroelectric substance 2 and a dense ferroelectric substance 3 are adjacent to each other. Partition 6
The raw material powder of the ferroelectric and the powder that evaporates at a temperature lower than the temperature at which the ferroelectric is fired are mixed and placed in one side 2a of the mold 4 (see FIG. 3) having The ferroelectric material alone is put into the other side 3a of the mold 4 and the partition 6 is put into the mold 4
And molded. It is heated to vaporize the powder and bake the ferroelectric. Then, a polarization process is performed. The method for manufacturing a piezoelectric vibrator according to the sixth invention of the present invention is a method for manufacturing the piezoelectric vibrator 8 (see FIG. 2) of the ferroelectrics 2 and 9 adjacent to each other and made porous with different porosity. A ferroelectric raw material powder and a powder that is vaporized at a temperature lower than the temperature at which the ferroelectric is fired are mixed and molded into one side 2a of a mold 4 having a partition 6 (see FIG. 3). Then, a ferroelectric raw material powder and a vaporizable powder are mixed in a ratio different from that described above in the other side 3a in the mold 4 and the mold is formed. The partition 6 is removed from the mold and molded. It is heated to vaporize the powder and bake the ferroelectric. Then, a polarization process is performed.
以下、本発明の実施例を詳細に説明する。 第1図は本発明の圧電振動子の一実施例を示し、
(a)は平面図、(b)は縦断面図である。同図に示す
焼成体1は緻密なジルコン酸チタン酸鉛の焼結体からな
る内柱部2と、空孔率35%の多孔質構造を持つジルコン
酸チタン酸鉛の焼結体からなる外筒部3とから円柱状に
構成されている。 焼成体1を成形する場合は、第3図に示す外筒5と仕
切りである境界筒6からなる成形型4を用いる。境界筒
6の内部2aにジルコン酸チタン酸鉛だけを入れる。外筒
2と境界筒6の中間部3aにはジルコン酸チタン酸鉛にメ
タクリル粉体を10重量%混合したものを入れる。そして
境界筒6を取り除き加圧することにより成形体を得る。
この成形体は電気炉により500℃で2時間加熱しながら
保持する。すると成形体からメタクリル粉体が気化し去
る。それをさらに1200℃で2時間焼成することにより、
内柱部2に緻密なジルコン酸チタン酸鉛の焼結体、外筒
部3に空孔率35%の多孔質構造を持つジルコン酸チタン
酸鉛の焼結体1を得ることができた。 この焼結体1の内柱部2と外筒部3との境界を調べた
結果、両部分は良好な接合となっていた。 さらにこの円柱状の焼結体1を厚さ1mmに研磨した
後、公知の方法で厚さ方向に分極処理して圧電振動子を
得た。その圧電振動子の共振周波数を調べた結果、緻密
なジルコン酸チタン酸鉛の部分2の共振周波数は1840KH
zであった。空孔率35%の多孔質化したジルコン酸チタ
ン酸鉛の部分3の共振周波数は940KHzであった。 上記実施例では強誘電体としてジルコン酸チタン酸鉛
を用いたが、チタン酸バリウムBaTiO3、チタン酸鉛PbTi
O3等でも同様に異なった共振周波数が得られる。また空
孔を形成する材料としてメタクリル粉体を用いている
が、強誘電体の焼成温度より低い温度で気化する架橋ポ
リスチレン粉体、炭素粉体等の合成樹脂や無機粉体でも
同様に空孔を形成できる。 また上記実施例では、緻密なジルコン酸チタン酸鉛と
多孔質化したジルコン酸チタン酸鉛での構成を示した
が、空孔率の異なる複数の多孔質化したものを組合わせ
た焼成体からも、1個で任意の複数の共振周波数を発振
する圧電振動子を得ることができる。 さらに上記実施例の構成では、1個の圧電振動子で得
られる共振周波数は2つの周波数であるが、空孔率の異
なる領域の数を増やすことにより共振周波数の数をさら
に増やすことができる。Hereinafter, embodiments of the present invention will be described in detail. FIG. 1 shows an embodiment of the piezoelectric vibrator of the present invention,
(A) is a plan view and (b) is a longitudinal sectional view. The sintered body 1 shown in FIG. 1 has an inner pillar portion 2 made of a dense sintered body of lead zirconate titanate and an outer pillar made of a sintered body of lead zirconate titanate having a porous structure with a porosity of 35%. It is formed in a cylindrical shape from the cylindrical portion 3. When the fired body 1 is formed, a forming die 4 including an outer cylinder 5 and a boundary cylinder 6 serving as a partition shown in FIG. 3 is used. Only lead zirconate titanate is put into the inside 2a of the boundary cylinder 6. A mixture of lead zirconate titanate and 10% by weight of methacrylic powder is placed in the intermediate portion 3a between the outer cylinder 2 and the boundary cylinder 6. Then, the boundary cylinder 6 is removed and pressurized to obtain a molded body.
The molded body is held while being heated at 500 ° C. for 2 hours in an electric furnace. Then, the methacrylic powder evaporates from the molded body. By firing it at 1200 ° C for 2 hours,
A dense sintered body of lead zirconate titanate was obtained in the inner column portion 2 and a sintered body 1 of lead zirconate titanate having a porous structure with a porosity of 35% was obtained in the outer cylindrical portion 3. As a result of examining the boundary between the inner column portion 2 and the outer cylindrical portion 3 of the sintered body 1, both portions were found to have a good joint. Further, the cylindrical sintered body 1 was polished to a thickness of 1 mm, and then subjected to polarization treatment in the thickness direction by a known method to obtain a piezoelectric vibrator. As a result of examining the resonance frequency of the piezoelectric vibrator, the resonance frequency of the dense lead zirconate titanate portion 2 was 1840 KH.
z. The resonance frequency of the portion 3 of porous zirconate titanate having a porosity of 35% was 940 KHz. In the above embodiment, lead zirconate titanate was used as the ferroelectric, but barium titanate BaTiO 3 , lead titanate PbTi
Similarly, different resonance frequencies can be obtained with O 3 and the like. Also, methacrylic powder is used as a material for forming pores, but synthetic resin such as crosslinked polystyrene powder, carbon powder, and inorganic powder which evaporate at a temperature lower than the firing temperature of ferroelectrics, and pores are similarly used. Can be formed. Further, in the above-described embodiment, the configuration of dense lead zirconate titanate and porous zirconate titanate was shown, but a fired body obtained by combining a plurality of porous materials having different porosity was used. In addition, a single piezoelectric vibrator that oscillates a plurality of arbitrary resonance frequencies can be obtained. Further, in the configuration of the above embodiment, the resonance frequency obtained by one piezoelectric vibrator is two frequencies, but the number of resonance frequencies can be further increased by increasing the number of regions having different porosity.
以上説明したように、本発明の圧電振動子は、1個の
中の複数の各領域に異なった共振周波数を持たせるよう
にしたから、振動子の構成部品数の削減、コスト低減及
び小型化、高性能化を図ることができる。この圧電振動
子を用いる超音波送受波器の構造を簡単にすることがで
き、医療用、漁業用等の広い範囲に応用することができ
る。 また本発明の製造方法によれば、上記の特性を有する
圧電振動子を効率よく造ることができる。As described above, in the piezoelectric vibrator of the present invention, a plurality of regions in one have different resonance frequencies, so that the number of components of the vibrator is reduced, the cost is reduced, and the size is reduced. And high performance can be achieved. The structure of the ultrasonic transducer using the piezoelectric vibrator can be simplified, and it can be applied to a wide range such as medical use, fishery use and the like. Further, according to the manufacturing method of the present invention, a piezoelectric vibrator having the above characteristics can be efficiently manufactured.
第1図は本発明を適用する圧電振動子の実施例の平面図
と縦断面図、第2図は同じく別な実施例の同上図、第3
図は成形型の実施例の平面図と縦断面図、第4図は周波
数定数と空孔率の特性図、第5図は温度と線膨張係数の
特性図である。 1、8……圧電振動子、2、9……多孔質化強誘電体、
3……緻密な強誘電体、4……成形型、5……型外筒、
6……仕切りFIG. 1 is a plan view and a longitudinal sectional view of an embodiment of a piezoelectric vibrator to which the present invention is applied. FIG.
FIG. 4 is a plan view and a longitudinal sectional view of an embodiment of a molding die, FIG. 4 is a characteristic diagram of frequency constant and porosity, and FIG. 5 is a characteristic diagram of temperature and linear expansion coefficient. 1, 8 ... piezoelectric vibrator, 2, 9 ... porous ferroelectric,
3 ... dense ferroelectric, 4 ... molding die, 5 ... mold outer cylinder,
6 ... partition
フロントページの続き (58)調査した分野(Int.Cl.6,DB名) H01L 41/08 H01L 41/24 H04R 17/00 Continuation of the front page (58) Field surveyed (Int.Cl. 6 , DB name) H01L 41/08 H01L 41/24 H04R 17/00
Claims (6)
した強誘電体からなる外筒部とを一体化して焼成し、分
極処理を施してあることを特徴とする圧電振動子。1. A piezoelectric vibrator characterized in that an inner column portion made of a dense ferroelectric and an outer cylindrical portion made of a porous ferroelectric are integrally fired and polarized. .
の強誘電体の一方を内柱部、別な方を筒部とし一体化し
て焼成し、分極処理を施してあることを特徴とする圧電
振動子。2. The method according to claim 1, wherein one of a plurality of porous ferroelectric materials having different porosity is formed into an inner pillar portion, and the other is formed into a cylindrical portion, which is integrally fired and subjected to a polarization treatment. Piezoelectric vibrator.
までの範囲にあることを特徴とする請求項第1項または
第2項に記載の圧電振動子。3. The porosity of the porous ferroelectric material is 35%.
The piezoelectric vibrator according to claim 1, wherein the piezoelectric vibrator is in the range described above.
タン酸バリウム、チタン酸鉛から選ばれる物質であるこ
とを特徴とする請求項第1項、第2項または第3項に記
載の圧電振動子。4. The method according to claim 1, wherein said ferroelectric substance is a substance selected from the group consisting of lead zirconate titanate, barium titanate, and lead titanate. Piezoelectric vibrator.
料粉末と該強誘電体を焼成する温度より低い温度で気化
する粉体とを混合して型入れし、該型内のもう一方に強
誘電体だけを型入れし、前記仕切りを型から取り去って
成形した後、加熱して該粉体を気化させ、強誘電体を焼
成し、分極処理をすることを特徴とする多孔質化した強
誘電体と緻密な強誘電体が隣接する圧電振動子を製造す
る方法。5. A ferroelectric raw material powder and a powder that is vaporized at a temperature lower than the temperature at which the ferroelectric is fired are mixed and placed in one of the molds having a partition. On the other hand, only the ferroelectric material is put into the mold, the partition is removed from the mold, and after molding, the powder is heated to evaporate, the ferroelectric material is baked, and a polarization process is performed. A method of manufacturing a piezoelectric vibrator in which a ferroelectric that has been converted and a dense ferroelectric are adjacent to each other.
料粉末と該強誘電体を焼成する温度より低い温度で気化
する粉体とを混合して型入れし、該型内のもう一方に該
原料粉末と該粉体とを前記とは異なった比率で混合して
型入れし、前記仕切りを型から取り去って成形した後、
加熱して該粉体を気化させ、強誘電体を焼成し、分極処
理をすることを特徴とする隣接して異なった空孔率で多
孔質化した強誘電体の圧電振動子を製造する方法。6. A ferroelectric raw material powder and a powder which is vaporized at a temperature lower than the temperature at which the ferroelectric is fired are mixed and placed in one of the molds having a partition. On the other hand, after mixing the raw material powder and the powder at a ratio different from the above and molding, removing the partition from the mold and molding,
A method for producing a ferroelectric piezoelectric vibrator having adjacently different porosity and being porous, comprising heating to vaporize the powder, firing the ferroelectric, and performing polarization treatment. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9151789A JP2878302B2 (en) | 1989-04-11 | 1989-04-11 | Piezoelectric vibrator and manufacturing method thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9151789A JP2878302B2 (en) | 1989-04-11 | 1989-04-11 | Piezoelectric vibrator and manufacturing method thereof |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02270383A JPH02270383A (en) | 1990-11-05 |
| JP2878302B2 true JP2878302B2 (en) | 1999-04-05 |
Family
ID=14028604
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9151789A Expired - Fee Related JP2878302B2 (en) | 1989-04-11 | 1989-04-11 | Piezoelectric vibrator and manufacturing method thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2878302B2 (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP4443907A4 (en) * | 2021-11-29 | 2025-10-22 | Murata Manufacturing Co | ULTRASOUND TRANSDUCER AND METHOD FOR MANUFACTURING SAME |
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1989
- 1989-04-11 JP JP9151789A patent/JP2878302B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02270383A (en) | 1990-11-05 |
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