JPS648476B2 - - Google Patents
Info
- Publication number
- JPS648476B2 JPS648476B2 JP54141755A JP14175579A JPS648476B2 JP S648476 B2 JPS648476 B2 JP S648476B2 JP 54141755 A JP54141755 A JP 54141755A JP 14175579 A JP14175579 A JP 14175579A JP S648476 B2 JPS648476 B2 JP S648476B2
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric
- pyroelectric
- tubular body
- polymeric material
- internal electrode
- 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
Links
- 239000000463 material Substances 0.000 claims description 59
- 239000002861 polymer material Substances 0.000 claims description 20
- 239000004020 conductor Substances 0.000 claims description 19
- 238000002844 melting Methods 0.000 claims description 16
- 230000010287 polarization Effects 0.000 claims description 16
- 230000008018 melting Effects 0.000 claims description 15
- 239000002033 PVDF binder Substances 0.000 claims description 11
- 229920002981 polyvinylidene fluoride Polymers 0.000 claims description 11
- 229920005989 resin Polymers 0.000 claims description 10
- 239000011347 resin Substances 0.000 claims description 10
- 239000012510 hollow fiber Substances 0.000 claims description 9
- 238000000034 method Methods 0.000 claims description 8
- 239000012530 fluid Substances 0.000 claims description 7
- 238000004519 manufacturing process Methods 0.000 claims description 7
- 229910052751 metal Inorganic materials 0.000 claims description 3
- 239000002184 metal Substances 0.000 claims description 3
- 229910001092 metal group alloy Inorganic materials 0.000 claims description 3
- 239000000126 substance Substances 0.000 claims description 3
- 239000013078 crystal Substances 0.000 claims description 2
- 239000008151 electrolyte solution Substances 0.000 claims description 2
- 230000005616 pyroelectricity Effects 0.000 description 10
- FAPWRFPIFSIZLT-UHFFFAOYSA-M Sodium chloride Chemical compound [Na+].[Cl-] FAPWRFPIFSIZLT-UHFFFAOYSA-M 0.000 description 8
- 229910000679 solder Inorganic materials 0.000 description 8
- 230000000694 effects Effects 0.000 description 5
- 229910052782 aluminium Inorganic materials 0.000 description 4
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 4
- 239000007864 aqueous solution Substances 0.000 description 4
- 239000000919 ceramic Substances 0.000 description 4
- 238000006073 displacement reaction Methods 0.000 description 4
- 229920000642 polymer Polymers 0.000 description 4
- 229920002620 polyvinyl fluoride Polymers 0.000 description 4
- 229920001971 elastomer Polymers 0.000 description 3
- 230000005684 electric field Effects 0.000 description 3
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical group [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 3
- 230000004044 response Effects 0.000 description 3
- 229920006395 saturated elastomer Polymers 0.000 description 3
- 239000011780 sodium chloride Substances 0.000 description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 2
- VSCWAEJMTAWNJL-UHFFFAOYSA-K aluminium trichloride Chemical compound Cl[Al](Cl)Cl VSCWAEJMTAWNJL-UHFFFAOYSA-K 0.000 description 2
- 230000008859 change Effects 0.000 description 2
- 239000002131 composite material Substances 0.000 description 2
- 229920001577 copolymer Polymers 0.000 description 2
- 239000011796 hollow space material Substances 0.000 description 2
- 229920001519 homopolymer Polymers 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 239000000243 solution Substances 0.000 description 2
- BQCIDUSAKPWEOX-UHFFFAOYSA-N 1,1-Difluoroethene Chemical compound FC(F)=C BQCIDUSAKPWEOX-UHFFFAOYSA-N 0.000 description 1
- 238000002441 X-ray diffraction Methods 0.000 description 1
- 230000009471 action Effects 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 229910000365 copper sulfate Inorganic materials 0.000 description 1
- ARUVKPQLZAKDPS-UHFFFAOYSA-L copper(II) sulfate Chemical compound [Cu+2].[O-][S+2]([O-])([O-])[O-] ARUVKPQLZAKDPS-UHFFFAOYSA-L 0.000 description 1
- 238000004132 cross linking Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 229940021013 electrolyte solution Drugs 0.000 description 1
- 238000010894 electron beam technology Methods 0.000 description 1
- 238000001125 extrusion Methods 0.000 description 1
- 230000009969 flowable effect Effects 0.000 description 1
- XUCNUKMRBVNAPB-UHFFFAOYSA-N fluoroethene Chemical compound FC=C XUCNUKMRBVNAPB-UHFFFAOYSA-N 0.000 description 1
- 230000009477 glass transition Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000002427 irreversible effect Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000000615 nonconductor Substances 0.000 description 1
- 239000003973 paint Substances 0.000 description 1
- 229920001184 polypeptide Polymers 0.000 description 1
- 102000004196 processed proteins & peptides Human genes 0.000 description 1
- 108090000765 processed proteins & peptides Proteins 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N30/00—Piezoelectric or electrostrictive devices
- H10N30/80—Constructional details
- H10N30/85—Piezoelectric or electrostrictive active materials
- H10N30/857—Macromolecular compositions
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N30/00—Piezoelectric or electrostrictive devices
- H10N30/01—Manufacture or treatment
- H10N30/09—Forming piezoelectric or electrostrictive materials
- H10N30/098—Forming organic materials
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N30/00—Piezoelectric or electrostrictive devices
- H10N30/60—Piezoelectric or electrostrictive devices having a coaxial cable structure
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Measuring Fluid Pressure (AREA)
- Radiation Pyrometers (AREA)
- Inorganic Insulating Materials (AREA)
- Non-Insulated Conductors (AREA)
Description
【発明の詳細な説明】
本発明は、延伸され且つ配向分極された高分子
材料からなる管状の圧電又は焦電材料の中空管内
部に内部電極を設けた線状の圧電又は焦電体およ
びその製造方法に係る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a linear piezoelectric or pyroelectric material in which an internal electrode is provided inside a hollow tube of a tubular piezoelectric or pyroelectric material made of a stretched and orientation-polarized polymeric material; It concerns the manufacturing method.
管状圧電材料又は焦電材料は、その内部を流れ
る流体の圧力変化を直接検出してその流量を制御
する事ができ、また流体の温度変化をも検知する
事ができる。また、管状特に毛管状(内径が数mm
以下)の圧電材料又は焦電材料は、微量な応力、
微小局部の温度変化等を求める上で有用な形態で
ある。この様な形状を得ようとすると、まず加工
性の良いことが要求される。この点で難がある無
機結晶材料および強誘電体セラミツクス等は実用
的でない。又、この形状に於ては、狭い空間であ
る管内で内側電極と圧電材料又は焦電材料との密
着性の良い状態で、内側電極が形成されなければ
ならない。この点で、ポリ弗化ビニリデン又はポ
リ弗化ビニル等は延伸操作を施こさないと圧電性
又は焦電性を示さないが、特開昭54−37299号で
指摘している様に、延伸操作したものは線状電極
を被覆して利用することが密着性の点で困難であ
り、これらも実現されていなかつた。そのため、
強誘電体セラミツクスを主成分とするポリ弗化ビ
ニリデンと強誘電体セラミツクスとの複合体や合
成ポリペプチド等の延伸操作を施こさなくとも圧
電性を発現し且つ加工性の良好な材料が用いられ
てきたに過ぎない。 A tubular piezoelectric material or pyroelectric material can directly detect changes in the pressure of a fluid flowing therein to control its flow rate, and can also detect changes in temperature of the fluid. In addition, tubular, especially capillary (with an inner diameter of several mm)
The following piezoelectric materials or pyroelectric materials
This is a useful form for determining temperature changes in minute local areas. In order to obtain such a shape, first of all, good workability is required. Inorganic crystal materials and ferroelectric ceramics, which have problems in this respect, are not practical. In addition, in this shape, the inner electrode must be formed in a state in which the inner electrode and the piezoelectric material or pyroelectric material have good adhesion within the tube, which is a narrow space. In this respect, polyvinylidene fluoride or polyvinyl fluoride does not exhibit piezoelectricity or pyroelectricity unless it is stretched, but as pointed out in JP-A-54-37299, stretching However, it is difficult to cover and utilize a linear electrode in terms of adhesion, and these methods have not been realized yet. Therefore,
Materials that exhibit piezoelectricity without stretching and have good processability are used, such as composites of polyvinylidene fluoride and ferroelectric ceramics, whose main component is ferroelectric ceramics, and synthetic polypeptides. It just came.
しかし、これらの従来実用的であるとされてき
た材料の圧電性はせいぜいd31=7〜10×
10-12C/N程度であり、大きな圧電性とは云えな
かつた。 However, the piezoelectricity of these materials that have been considered to be practical is at most d 31 = 7 to 10×
It was about 10 -12 C/N, so it could not be said that it had great piezoelectricity.
本発明は、上記従来技術の欠点を克服し、従来
製造が困難とされていた延伸され且つ配向分極さ
れて圧電性又は焦電性を附与された高分子材料か
らなる管状の圧電又は焦電材料を具備する圧電又
は焦電体を提供するものであり、圧電性高分子材
料の管状体の中空管内部に、前記高分子材料の融
点以下の温度で流動性を有する導電体からなる内
部電極を設けることを特徴とする。かかる内部電
極は、管状圧電材料又は焦電材料の中空管内部に
注入する際、流動状態であるため、管状体の内側
表面との密着性が非常に良いものが得られること
に着眼したものである。 The present invention overcomes the drawbacks of the prior art described above, and provides a tubular piezoelectric or pyroelectric material made of a polymeric material that is stretched and orientation-polarized to impart piezoelectricity or pyroelectricity, which has been difficult to manufacture in the past. The present invention provides a piezoelectric or pyroelectric material comprising a piezoelectric material, and an interior made of a conductor having fluidity at a temperature below the melting point of the polymer material, inside a hollow tube of a tubular body of a piezoelectric polymer material. It is characterized by providing an electrode. This invention focused on the fact that when this internal electrode is injected into the hollow tube of a tubular piezoelectric material or pyroelectric material, it is in a fluid state, so that it can have very good adhesion to the inner surface of the tubular body. It is.
以下、本発明を詳細に説明する。 The present invention will be explained in detail below.
本発明に係る圧電性高分子材料とは、配向分極
処理により圧電性又は焦電性を有する高分子物質
又は該高分子物質を含有する圧電材料を意味し、
代表的にはポリ弗化ビニリデン系樹脂又はポリ弗
化ビニル系樹脂が挙げられる。ここでポリ弗化ビ
ニリデン系樹脂とは、ポリ弗化ビニリデンホモポ
リマー、弗化ビニリデンを50モル%以上とするコ
ポリマー、これらのいずれかを主とする組成物等
を指す。又同様にポリ弗化ビニル系樹脂とは、ポ
リ弗化ビニルホモポリマー、弗化ビニルを50モル
%以上とするコポリマー、これらのいずれかを主
とする組成物等を指す。上記例からも知られる様
に、本発明における圧電体又は焦電体とは、圧電
体と焦電体の両方を有する場合も含むことは云う
迄もない。 The piezoelectric polymer material according to the present invention means a polymer substance that has piezoelectricity or pyroelectricity due to orientation polarization treatment, or a piezoelectric material containing the polymer substance,
Typical examples include polyvinylidene fluoride resins and polyvinyl fluoride resins. Here, the polyvinylidene fluoride resin refers to a polyvinylidene fluoride homopolymer, a copolymer containing 50 mol % or more of vinylidene fluoride, a composition mainly containing any of these, and the like. Similarly, the polyvinyl fluoride resin refers to a polyvinyl fluoride homopolymer, a copolymer containing 50 mol % or more of vinyl fluoride, a composition mainly containing any of these, and the like. As is known from the above examples, it goes without saying that the piezoelectric material or pyroelectric material in the present invention includes cases in which the piezoelectric material or the pyroelectric material includes both a piezoelectric material and a pyroelectric material.
上述の配向分極処理により圧電性又は焦電性が
附与される高分子材料は、単独で又は重ねられた
若しくは重ねられていないが共軸の樹脂と共に複
数で、例えば公知の中空糸の製造法等を用いて管
状に形成される。次いで、かかる圧電性又は焦電
性が附与される高分子材料の管状体の中空管内部
に、該高分子材料の融点以下の温度で流導性を有
する導電体からなる内部電極が形成される。尚、
中空管内部とは中空管の中空部分全体であつても
良いが、全体でなくても例えば圧電性又は焦電性
が附与される高分子材料管状体の内壁であつても
良い。該導電体は焦電体又は圧電体の一方の電極
として用いられ、場合によつては配向分極の際の
電極としても用いられ得る。従つて、その使用さ
れる電極の目的に応じ、その使用前に本発明の導
電体を流動し得る状態にして管状体の中空管内部
に注入し、該導電体からなる内部電極が形成され
る。このため、導電体は上述高分子材料の融点以
下の温度で流導性を有することが必要である。
尚、高分子材料の延伸後に延伸温度以上で本発明
の導電体からなる内部電極を形成するときは、管
状体を緊張状態で行わなければならないことは云
う迄もない。 The polymer material to which piezoelectricity or pyroelectricity is imparted by the above-mentioned orientation polarization treatment may be used alone or in combination with a coaxial resin, which may be superimposed or not superimposed, for example, by a known hollow fiber manufacturing method. It is formed into a tubular shape using, etc. Next, an internal electrode made of a conductor having flow conductivity at a temperature below the melting point of the polymer material is formed inside the hollow tube of the polymer material tube to which piezoelectricity or pyroelectricity is imparted. be done. still,
The interior of the hollow tube may be the entire hollow portion of the hollow tube, but it may also be the inner wall of a polymeric tubular body imparted with piezoelectricity or pyroelectricity, for example. The conductor is used as one electrode of a pyroelectric material or a piezoelectric material, and may also be used as an electrode during orientation polarization in some cases. Therefore, depending on the purpose of the electrode to be used, before use, the conductor of the present invention may be made in a flowable state and injected into the hollow tube of the tubular body to form an internal electrode made of the conductor. Ru. Therefore, the conductor needs to have flow conductivity at a temperature below the melting point of the above-mentioned polymer material.
It goes without saying that when forming the internal electrode made of the conductor of the present invention at a temperature higher than the stretching temperature after stretching the polymeric material, the tubular body must be kept under tension.
かかる導電体としては、例えば千住金属工業の
製造に係る融点が62℃のはんだである登録商標
「低温はんだ−62」および融点が78℃の「低温は
んだ−78」等の如き、高分子の融点よりも低い融
点の金属合金;例えば塩化ナトリウム水溶液およ
び硫酸銅水溶液の如き、電解質溶液;例えば融点
又は融点を有しない場合には軟化点が上記高分子
材料の融点よりも低い樹脂に金属粉末、カーボン
等を含めた如き、導電性樹脂、樹脂ハンダ、導電
性ゴム等が用いられ得る。これらを中空管内部に
形成するには、例えば管状体の一端から吸引しな
がら他端から注入する方法;導電性樹脂を共押出
する方法;導電性ゴムを未架橋の状態で注入して
その後架橋させる方法等の公知の方法が用いられ
得る。これら導電体は常温でも流動状態である方
が、管状高分子材料を圧電材料又は焦電材料とし
て使用する上で望ましいが、必ずしもその必要は
なく、中空管内へ充填する際に流動し得る状態で
あれば良い。 Examples of such conductors include polymer melting point solders, such as the registered trademark "Kyosei Solder-62", which is a solder with a melting point of 62°C manufactured by Senju Metal Industries, and "Kyosei Solder-78", which has a melting point of 78°C. metal alloys with a melting point lower than that of the polymer material; electrolyte solutions such as aqueous sodium chloride and copper sulfate solutions; Conductive resin, resin solder, conductive rubber, etc. may be used. These can be formed inside a hollow tube by, for example, suctioning from one end of the tubular body and injecting it from the other end; coextruding conductive resin; or injecting conductive rubber in an uncrosslinked state and then Known methods such as crosslinking may be used. It is desirable for these conductors to be in a fluid state even at room temperature in order to use the tubular polymer material as a piezoelectric material or pyroelectric material, but it is not necessary that they be in a fluid state when filling the hollow tube. It's good to have.
ところで、圧電定数d31は素子のヤング率が小
さい程大きくなる。即ち、一定応力に対する歪は
ヤング率が小さい程大きく、その結果発生する電
荷量が大きくなる。従つて、たとえ常温で流動し
得ないものであつても中空内へ注入する際に流動
し得る状態の導電体であり、常温でのヤング率が
比較的低いものであれば、圧電体又は焦電体とし
て用いる際にそのまま内側電極として使用する事
ができる。またヤング率が大きい場合には他の比
較的ヤング率の小さな導電体にとりかえて使用す
れば良い。例えば銅のヤング率は12×1010N/m2
であるのに対し、本発明に用いられうる低融点金
属合金の千住金属工業の製造に係る融点が62℃の
はんだである「低温はんだ−62」のヤング率は約
3×1010N/m2である。 By the way, the piezoelectric constant d 31 increases as the Young's modulus of the element decreases. That is, the smaller the Young's modulus, the greater the strain with respect to a constant stress, and as a result, the amount of charge generated increases. Therefore, even if it cannot flow at room temperature, if it is a conductor that can flow when injected into a hollow space and has a relatively low Young's modulus at room temperature, it can be used as a piezoelectric material or a pyroelectric material. When used as an electric body, it can be used as is as an inner electrode. If the Young's modulus is large, another conductor with a relatively small Young's modulus may be used instead. For example, Young's modulus of copper is 12×10 10 N/m 2
On the other hand, the Young's modulus of "low-temperature solder-62", which is a solder with a melting point of 62°C manufactured by Senju Metal Industry, a low-melting metal alloy that can be used in the present invention, is approximately 3 × 10 10 N/m. It is 2 .
かかる上記導電体を配向分極時に用いず、管状
高分子材料を圧電材料又は焦電材料として使用す
る時にのみ用いても良いが、その場合には例えば
配向分極時の内部電極としては中空糸又はそれを
延伸した管の内径よりも細い金属線を内部電極と
し、コロナ放電させる方法等が採用され得る。他
方、外側の電極は、配向分極の際及び圧電又は焦
電作用をさせる時に電子線を用いる場合には必要
ないが、通常は必要であり、フイルム状の圧電又
は焦電素子の電極形成と同様な方法で形成され
得、蒸着金属膜、導電性塗料、導電性ゴム等が用
いられ得る。 The above conductor may not be used during orientation polarization and may be used only when the tubular polymer material is used as a piezoelectric material or pyroelectric material, but in that case, for example, a hollow fiber or the like may be used as the internal electrode during orientation polarization. A method may be adopted in which a metal wire thinner than the inner diameter of a stretched tube is used as an internal electrode to cause corona discharge. On the other hand, the outer electrode is not necessary when using an electron beam for orientational polarization and for piezoelectric or pyroelectric action, but it is usually necessary, and is similar to the electrode formation of film-like piezoelectric or pyroelectric elements. A vapor-deposited metal film, a conductive paint, a conductive rubber, etc. can be used.
上記導電体からなる内部電極を配向分極時の内
部電極としても用いる場合、該導電体を中空内へ
注入する時としては高分子材料の延伸前であつて
も延伸後であつても良いが、延伸前であれば口径
が延伸後よりも大きい故中空内へ注入しやすいと
いう製造上の有利性がある。更に、中空内へ何も
充填しないで延伸するよりも、10〜15%程度延伸
倍率を大きくすることができるという予想だにし
得なかつた効果もあり、その結果圧電性、焦電性
を向上させることができる。 When using the internal electrode made of the above-mentioned conductor as an internal electrode during orientation polarization, the conductor may be injected into the hollow before or after stretching the polymer material. Since the diameter is larger before stretching than after stretching, there is an advantage in manufacturing that it is easier to inject into the hollow. Furthermore, there is an unexpected effect that the stretching ratio can be increased by about 10 to 15% compared to stretching without filling the hollow space with anything, and as a result, piezoelectricity and pyroelectricity are improved. be able to.
この場合、注入後両端を封じることが望まし
い。その場合、空気等の導電体でないものが中空
内に含まれない様にすることが望ましいが、ある
程度含まれていても実用上問題ない。 In this case, it is desirable to seal both ends after injection. In that case, it is desirable to prevent non-conductors such as air from being included in the hollow, but there is no practical problem even if a certain amount is included.
延伸操作は、配向分極と同時になされても良い
し、配向分極前になされても良く、フイルムと同
様に公知の方法でなされる。周知の如く、ポリ弗
化ビニリデン系樹脂の場合には、延伸操作により
β構造を主体とする構造にすることが圧電性又は
焦電性を附与させる上で必要である。そのために
は周知の如く、延伸温度が低い程又延伸倍率が大
きい程β構造が得られやすいので、延伸倍率、延
伸温度を適宜選択して延伸することによりβ構造
を主体とすることができる。尚、β構造がどの程
度含まれているかはX線解析で調べるのが管状体
に対しては確実である。 The stretching operation may be performed simultaneously with the orientation and polarization, or may be performed before the orientation and polarization, and can be performed by a known method similar to that for films. As is well known, in the case of polyvinylidene fluoride resin, it is necessary to form a structure mainly consisting of a β structure by a stretching operation in order to impart piezoelectricity or pyroelectricity. For this purpose, as is well known, the lower the stretching temperature or the higher the stretching ratio, the easier it is to obtain a β structure, so by appropriately selecting the stretching ratio and stretching temperature and stretching, the β structure can be obtained as the main component. Note that for tubular bodies, it is certain to examine the extent to which the β structure is contained by X-ray analysis.
又、配向分極もフイルムに用いられた公知の方
法が採用され、絶縁耐力にできるだけ近い電界を
印加することが望ましく、配向分極の温度も高分
子のガラス転移温度以上、融点以下の温度で行な
われる。 Also, for orientation polarization, a known method used for films is adopted, and it is desirable to apply an electric field as close to the dielectric strength as possible, and orientation polarization is performed at a temperature above the glass transition temperature of the polymer and below the melting point. .
以下、実施例を示す。 Examples are shown below.
実施例 1
ポリ弗化ビニリデンを中空糸状に溶融押出し、
内径500μ、外径800μの中空糸を得、その後70℃
で3.3倍に延伸し、内径300μ、外径500μの毛管を
得、管表面にアルミニウムを蒸着した。次いで中
空管内に塩化アルミニウム飽和水溶液を注入し、
両端を封じ、アルミニウム蒸着膜に触れない様に
塩化ナトリウム飽和水溶液と導通するリード線を
取り出した。又、アルミニウム蒸着面からもリー
ド線を取り出して60℃で600KV/cmの直流電界
を15分間印加し、その後室温迄電界を印加したま
ま冷却した。圧電定数d31は20×10-21C/Nであ
つた。これは通常のポリ弗化ビニリデン一軸延伸
フイルムの圧電定数d31とほぼ同等な値である。
尚、ここで圧電定数の測定の際の電極面積は管状
体の内径に接している電極面積と外径に接してい
る電極面積の調和平均をとつたものである。以下
の実施例も同様である。Example 1 Melt extrusion of polyvinylidene fluoride into hollow fibers,
Obtain hollow fibers with an inner diameter of 500μ and an outer diameter of 800μ, then at 70°C.
A capillary tube with an inner diameter of 300μ and an outer diameter of 500μ was obtained by stretching 3.3 times, and aluminum was vapor-deposited on the tube surface. Next, inject a saturated aqueous solution of aluminum chloride into the hollow tube,
Both ends were sealed, and a lead wire connected to the saturated sodium chloride aqueous solution was taken out without touching the aluminum vapor-deposited film. Further, the lead wire was taken out from the aluminum vapor-deposited surface, and a DC electric field of 600 KV/cm was applied at 60° C. for 15 minutes, and then cooled to room temperature while the electric field was applied. The piezoelectric constant d 31 was 20×10 −21 C/N. This value is approximately equivalent to the piezoelectric constant d 31 of a normal polyvinylidene fluoride uniaxially stretched film.
Here, the electrode area in the measurement of the piezoelectric constant is the harmonic average of the electrode area in contact with the inner diameter of the tubular body and the electrode area in contact with the outer diameter. The same applies to the following examples.
比較例 1
実施例1の塩化ナトリウム飽和水溶液の代わり
に径300μの銅線を中空内に無理矢理に挿入した
以外は実施例1と同様に実施したところ、圧電定
数d31は0であつた。Comparative Example 1 The same procedure as in Example 1 was conducted except that a copper wire with a diameter of 300 μm was forcibly inserted into the hollow instead of the saturated sodium chloride aqueous solution in Example 1, and the piezoelectric constant d 31 was 0.
実施例 2
千住金属工業の製造に係り、融点が62℃のはん
だである「低温はんだ−62」を実施例1の延伸前
中空糸の管内に67℃で注入し、両端をチヤツクに
より封じた後、80℃で3.5倍に延伸し、内径250μ、
外径450μの毛管体を得た。この毛管体の外側に
アルミニウムを蒸着し実施例1と同様にリード線
を取り出し、90℃で600KV/cmの直流電圧を15
分間印加して、更に電圧を印加したまま室温迄冷
却した。圧電定数d31ははんだをそのまま内部電
極として測定すると7×10-12C/Nであつた。Example 2 "Low-temperature solder-62", a solder with a melting point of 62°C, manufactured by Senju Metal Industries, was injected at 67°C into the tube of the unstretched hollow fiber of Example 1, and both ends were sealed with chucks. , stretched 3.5 times at 80℃, inner diameter 250μ,
A capillary body with an outer diameter of 450μ was obtained. Aluminum was vapor-deposited on the outside of this capillary body, the lead wire was taken out as in Example 1, and a DC voltage of 600 KV/cm was applied at 90°C for 15 minutes.
The voltage was applied for a minute, and the voltage was further cooled to room temperature while the voltage was being applied. The piezoelectric constant d 31 was 7×10 −12 C/N when measured using the solder as an internal electrode.
実施例 3
実施例2の配向分極後、70℃に加熱してはんだ
を抜き取り、その代わりに塩化ナトリウム飽和水
溶液を注入し、これを内部電極として用いると、
圧電定数d31は2.3×10-11C/Nであつた。Example 3 After the orientational polarization in Example 2, the solder is removed by heating to 70°C, and a saturated aqueous solution of sodium chloride is injected instead, and this is used as the internal electrode.
The piezoelectric constant d 31 was 2.3×10 −11 C/N.
実施例 4
ポリ弗化ビニリデンを内径700μ、外径1200μの
中空糸状に溶融押出し、実施例2と同じ「低温は
んだ−62」を67℃で管内に注入し、80℃で5.0倍
に延伸し、内径350μ、外径600μの毛管体を得た。
実施例2と同様に成極し、圧電定数d31を求めた
ところ、1×10-11C/Nであつた。これを実施例
3と同様にしたところ、3×10-11C/Nであつ
た。Example 4 Polyvinylidene fluoride was melt-extruded into a hollow fiber shape with an inner diameter of 700 μm and an outer diameter of 1200 μm, the same “low temperature solder-62” as in Example 2 was injected into the tube at 67°C, and it was stretched 5.0 times at 80°C. A capillary body with an inner diameter of 350μ and an outer diameter of 600μ was obtained.
Polarization was carried out in the same manner as in Example 2, and the piezoelectric constant d 31 was determined to be 1×10 −11 C/N. When this was done in the same manner as in Example 3, it was 3×10 -11 C/N.
実施例 5
実施例4に於いて、「低温はんだ−62」の注入
操作と延伸操作の順序を逆にした以外は実施例4
と同様に実施したところ、延伸倍率は4.5倍が限
度であり、圧電定数d31はそのため9×10-12C/
Nであつた。これを実施例3と同様にしたとこ
ろ、2.7×10-11C/Nであつた。Example 5 Same as Example 4 except that the order of injection operation and stretching operation of "low temperature solder-62" was reversed.
When carried out similarly to
It was N. When this was done in the same manner as in Example 3, it was 2.7×10 -11 C/N.
実施例 6
実施例4により得た毛管状電圧焦電体の温度変
化により分極量の変化、即ち焦電効果を不可逆な
成分を取除いてから測定したところ、焦電係数は
3.5×10-9C/cm2・degであつた。Example 6 When the change in the amount of polarization, that is, the pyroelectric effect, due to the temperature change of the capillary voltage pyroelectric body obtained in Example 4 was measured after removing irreversible components, the pyroelectric coefficient was
It was 3.5×10 -9 C/cm 2・deg.
この試料の圧電定数d31ははんだを内側電極と
して用いた場合8×12-12C/Nであり、塩化ナト
リウム飽和水溶液を用いた場合は2.6×10-11C/
Nであつた。この圧電定数d31と焦電係数の対応
関係はフイルム状ポリ弗化ビニリデン圧電焦電体
のそれと良く一致しており、常温で1年間経過し
ても、なお安定な圧電性、焦電性が得られた。 The piezoelectric constant d 31 of this sample is 8×12 -12 C/N when solder is used as the inner electrode, and 2.6×10 -11 C/N when a saturated aqueous sodium chloride solution is used.
It was N. This correspondence relationship between the piezoelectric constant d 31 and the pyroelectric coefficient is in good agreement with that of the film-like polyvinylidene fluoride piezoelectric pyroelectric material, and even after one year at room temperature, the piezoelectricity and pyroelectricity remain stable. Obtained.
以上の実施例からも知られる様に、従来の管状
圧電体である高分子物質と強誘電体セラミツクス
との複合体が示した圧電定数d31はせいぜい10×
10-12C/Nであつたが、本発明においてはd31が
30×10-12C/Nである圧電体が得られ、また焦電
定数が3.5×10-9C/cm2・degである焦電体が得ら
れ、いずれも経時的変化に対して安定であり、実
用性のある圧電性及び焦電性である。更にフイル
ムあるいはシート状圧電体の圧電効果は、例えば
2次元的な変位に対しては圧電効果の異方性やあ
るいは変位のせん断成分のために、その応答は変
位量と明解な対応関係を持ち得ないためある特定
の方向に対する刺激にのみ、定量化のできる応答
しか得られない。しかるに、線状圧電体を例えば
Z軸に沿つて設置し、片端を自由な状態にする
と、xy平面内の変位に対してその方向は任意で
あつても、変位に比例した応答を得る事ができる
という特徴も有し、フイルム状圧電では得られな
い効果を有するものである。 As is known from the above examples, the piezoelectric constant d 31 exhibited by the conventional tubular piezoelectric material, a composite of a polymer material and ferroelectric ceramics, is at most 10×
10 -12 C/N, but in the present invention d 31 is
A piezoelectric material with a value of 30×10 -12 C/N and a pyroelectric material with a pyroelectric constant of 3.5×10 -9 C/cm 2・deg were obtained, both of which are stable against changes over time. It has practical piezoelectricity and pyroelectricity. Furthermore, the piezoelectric effect of a film or sheet-like piezoelectric material has a clear correspondence with the amount of displacement, for example, due to the anisotropy of the piezoelectric effect or the shear component of the displacement in response to two-dimensional displacement. Therefore, only quantifiable responses can be obtained to stimuli in a specific direction. However, if a linear piezoelectric material is installed along the Z-axis and one end is left free, it is possible to obtain a response proportional to the displacement in the xy plane, even if the direction is arbitrary. It also has the feature that it can be used as a piezoelectric material, and has effects that cannot be obtained with film-like piezoelectric materials.
Claims (1)
分子材料の中空管内部に、該高分子材料の融点以
下の温度で流動性を有する導電体からなる内部電
極が設けられていることを特徴とする線状の圧電
又は焦電体。 2 圧電性高分子材料の管状体の中空管内部全体
に内部電極が設けられていることを特徴とする特
許請求の範囲第1項に記載の圧電又は焦電体。 3 圧電性高分子材料の管状体の内壁に内部電極
が設けられていることを特徴とする特許請求の範
囲第1項に記載の圧電又は焦電体。 4 内部電圧が圧電性高分子材料の融点よりも低
い融点を有する金属合金からなることを特徴とす
る特許請求の範囲第1項乃至第3項のいずれかに
記載の圧電又は焦電体。 5 内部電極が電解質溶液からなることを特徴と
する特許請求の範囲第1項乃至第3項のいずれか
に記載の圧電又は焦電体。 6 圧電性高分子材料がポリ弗化ビニリデン系樹
脂からなり、主としてβ型結晶構造を有するもの
であることを特徴とする特許請求の範囲第1項乃
至第5項のいずれかに記載の圧電又は焦電体。 7 圧電性高分子材料を中空糸状に押出して管状
体に成形し、次いで該高分子材料の融点以下の温
度で流動性を有する導電体を該高分子材料の管状
体の中空管内部に流動状態で注入し、次いで管状
の該高分子材料を延伸し、該延伸と同時に又は該
延伸後に注入した導電体を内部電極として該高分
子材料の配向分極処理をすることからなる線状の
圧電又は焦電体の製造方法。 8 圧電性高分子材料を中空糸状に押出して管状
体に成形し、次いで管状の該高分子材料を延伸
し、次いで該高分子材料の融点以下の温度で流動
性を有する導電体を延伸された該高分子材料の管
状体の中空管内部に流動状態で注入し、注入した
導電体を内部電極として該高分子材料の配向分極
処理をすることからなる線状の圧電又は焦電体の
製造方法。 9 圧電性高分子材料を中空糸状に押出して管状
体に成形し、管状の該高分子材料を延伸し、該延
伸と共に又は該延伸後に金属線を内部電極として
コロナ成極し、該金属線をはずし、次いで該高分
子材料の融点以下の温度で流動性を有する導電体
を延伸され且つ配向分極された該高分子材料の管
状体の中空管内部に流動状態で注入することから
なる線状の圧電又は焦電体の製造方法。[Claims] 1. An internal electrode made of a conductor that has fluidity at a temperature below the melting point of the polymer material is provided inside a hollow tube of a stretched and orientation-polarized piezoelectric polymer material. A linear piezoelectric or pyroelectric material characterized by: 2. The piezoelectric or pyroelectric body according to claim 1, wherein an internal electrode is provided throughout the hollow tube of the tubular body made of a piezoelectric polymer material. 3. The piezoelectric or pyroelectric material according to claim 1, wherein an internal electrode is provided on the inner wall of the tubular body made of a piezoelectric polymer material. 4. The piezoelectric or pyroelectric material according to any one of claims 1 to 3, characterized in that it is made of a metal alloy whose internal voltage has a melting point lower than that of the piezoelectric polymer material. 5. The piezoelectric or pyroelectric material according to any one of claims 1 to 3, wherein the internal electrode is made of an electrolyte solution. 6. The piezoelectric or piezoelectric material according to any one of claims 1 to 5, characterized in that the piezoelectric polymer material is made of polyvinylidene fluoride resin and mainly has a β-type crystal structure. Pyroelectric body. 7 A piezoelectric polymeric material is extruded into a hollow fiber shape to form a tubular body, and then a conductor having fluidity at a temperature below the melting point of the polymeric material is flowed into the hollow tube of the tubular body of the polymeric material. linear piezoelectric or Method of manufacturing pyroelectric material. 8 A piezoelectric polymeric material is extruded into a hollow fiber shape to form a tubular body, and then the tubular polymeric material is stretched, and then a conductor having fluidity at a temperature below the melting point of the polymeric material is stretched. Production of a linear piezoelectric or pyroelectric material by injecting the polymeric material in a fluid state into the hollow tube of a tubular body, and performing orientation polarization treatment on the polymeric material using the injected conductor as an internal electrode. Method. 9 Extrude a piezoelectric polymer material into a hollow fiber shape to form a tubular body, stretch the tubular polymer material, perform corona polarization using a metal wire as an internal electrode during or after the stretching, and Then, a conductor having fluidity at a temperature below the melting point of the polymeric material is injected in a fluid state into the hollow tube of the stretched, oriented and polarized tubular body of the polymeric material. A method for manufacturing a piezoelectric or pyroelectric substance.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14175579A JPS5666081A (en) | 1979-10-31 | 1979-10-31 | Linear piezoelectric or pyroelectric material and thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14175579A JPS5666081A (en) | 1979-10-31 | 1979-10-31 | Linear piezoelectric or pyroelectric material and thereof |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5666081A JPS5666081A (en) | 1981-06-04 |
| JPS648476B2 true JPS648476B2 (en) | 1989-02-14 |
Family
ID=15299431
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14175579A Granted JPS5666081A (en) | 1979-10-31 | 1979-10-31 | Linear piezoelectric or pyroelectric material and thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5666081A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0620703A1 (en) * | 1993-04-12 | 1994-10-19 | Ibiden Co, Ltd. | Resin compositions and printed circuit boards using the same |
| CN105047813A (en) * | 2015-06-17 | 2015-11-11 | 扬州大学 | Liquid core piezoelectric polymer device and preparation method and application thereof |
| CN107195770A (en) * | 2017-05-10 | 2017-09-22 | 扬州大学 | Polyvinylidene fluoride piezoelectric transducer |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4629925A (en) * | 1983-11-22 | 1986-12-16 | Raychem Corporation | Piezoelectric coaxial cable |
| JPS60104748U (en) * | 1983-12-21 | 1985-07-17 | 日本特殊陶業株式会社 | Piezoelectric sensor for internal combustion engines |
| CA1267216A (en) * | 1984-07-06 | 1990-03-27 | Pravin L. Soni | Piezoelectric device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5499086U (en) * | 1977-12-26 | 1979-07-12 |
-
1979
- 1979-10-31 JP JP14175579A patent/JPS5666081A/en active Granted
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0620703A1 (en) * | 1993-04-12 | 1994-10-19 | Ibiden Co, Ltd. | Resin compositions and printed circuit boards using the same |
| CN105047813A (en) * | 2015-06-17 | 2015-11-11 | 扬州大学 | Liquid core piezoelectric polymer device and preparation method and application thereof |
| CN107195770A (en) * | 2017-05-10 | 2017-09-22 | 扬州大学 | Polyvinylidene fluoride piezoelectric transducer |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5666081A (en) | 1981-06-04 |
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