JPS6242472A - Electrostriction element - Google Patents
Electrostriction elementInfo
- Publication number
- JPS6242472A JPS6242472A JP60180942A JP18094285A JPS6242472A JP S6242472 A JPS6242472 A JP S6242472A JP 60180942 A JP60180942 A JP 60180942A JP 18094285 A JP18094285 A JP 18094285A JP S6242472 A JPS6242472 A JP S6242472A
- Authority
- JP
- Japan
- Prior art keywords
- induced strain
- hysteresis
- small
- electrostriction element
- field
- 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.)
- Pending
Links
Abstract
Description
【発明の詳細な説明】 〔発明の技術分野〕 本発明は電歪素子に関する。[Detailed description of the invention] [Technical field of invention] The present invention relates to an electrostrictive element.
従来から、超精密位置決め用アクチェエータとしてPb
(Mgl/3Nb2/3)Oat主成分とする磁器材料
の電界誘起歪を利用した電歪素子が知られている。Conventionally, Pb has been used as an actuator for ultra-precision positioning.
(Mgl/3Nb2/3)An electrostrictive element is known that utilizes electric field-induced strain in a ceramic material having Oat as its main component.
特にPb (Mg 1/3Nb 2/3 ) 050T
l o、1o )03の電界誘起歪は。Especially Pb (Mg 1/3Nb 2/3) 050T
The electric field induced strain of lo, 1o)03 is.
Pb(Zrt−1Tiz)03系圧電材料に匹適する大
きさを有することが知られている。It is known to have a size comparable to that of Pb(Zrt-1Tiz)03-based piezoelectric materials.
しかしながらPb〔(Mg1/3Nb2/3)Osjo
Tlo10〕03の電界誘起歪は電界歪の関係に大きな
ヒステリシスを有し、電圧で変位量を精密に制御するこ
とは困難であった。However, Pb [(Mg1/3Nb2/3) Osjo
The electric field-induced strain of Tlo10]03 had a large hysteresis in the relationship with the electric field strain, and it was difficult to precisely control the amount of displacement using voltage.
本発明は、を圧−変位量の関係においてヒステリシスの
小さな電歪素子を提供することを目的とする。An object of the present invention is to provide an electrostrictive element with small hysteresis in the pressure-displacement relationship.
本発明は、大きな電界誘起歪を発生する磁器として*
Pb〔(Mg1/3Nb2/3)1−x’rtx)o
3co、os≦X≦0.15)に着目し、この磁器の電
界誘起歪において有するヒステリシスを小さくする目的
で、上記磁器組成において鉛原子の一部をBaで置換し
た磁器材料の電歪効果を採用することにより、上記の目
的を達成した電歪素子である。The present invention is a porcelain that generates large electric field-induced strain*
Pb [(Mg1/3Nb2/3)1-x'rtx)o
3 co, os ≦ This is an electrostrictive element that achieves the above objectives by employing the above-mentioned method.
Pb〔(Mg1/3Nb2/3) 1−xTlK)03
IlcおいてXが0.05未満では電界誘起歪が小ざ
いため電歪素子には不適でろる。またXが0.15を超
えるとヒステリシスが大きくなるため本発明によるBa
の置換をもってしても、このヒステリシスの除去が困難
である。Pb [(Mg1/3Nb2/3) 1-xTlK)03
If X in Ilc is less than 0.05, the electric field induced strain will be small, making it unsuitable for use as an electrostrictive element. Moreover, when X exceeds 0.15, the hysteresis increases, so the Ba according to the present invention
Even with the substitution of , it is difficult to remove this hysteresis.
またPbを置換するBaO量であるが、Pb原子のza
tmチ程度が望ましい。4atmチを超えると電界誘起
歪が小さくなってしまう。Baは少量の置換で効果を発
揮するが実用上は11Ltmチ以上とすることが好まし
い。Also, regarding the amount of BaO to replace Pb, the za of the Pb atom
It is desirable that the thickness be around tm. If it exceeds 4 atm, the electric field induced strain will become small. Although a small amount of Ba is effective when substituted, it is practically preferable to use 11 Ltm or more.
電歪素子としては、上述の磁器組成物の電歪縦効果を利
用した積層型電歪素子や電歪横効果を利用したバイモル
フ型電歪素子が代表例として挙げられる。Typical examples of the electrostrictive element include a laminated electrostrictive element that utilizes the longitudinal electrostrictive effect of the above-mentioned ceramic composition and a bimorph electrostrictive element that utilizes the transverse electrostrictive effect of the ceramic composition.
本発明によれば、大きな電界誘起歪と小さなヒステリシ
スを有する磁器材料を採用することにより、素子の形状
としては小型化が可能で、しかもフィードバック機構が
不要な超精密位置決め用電歪素子を提供できる。According to the present invention, by employing a ceramic material having large electric field-induced strain and small hysteresis, it is possible to provide an electrostrictive element for ultra-precision positioning that can be made smaller in element shape and does not require a feedback mechanism. .
以下に本発明の詳細な説明する。 The present invention will be explained in detail below.
本発明で採用した磁器材料は一般的な粉末冶金的方法に
よって製造した。すなわちPbO,TiO2゜MgO,
Nb2O5、BaCO3などの原料を所定の網金に正確
に秤取し、それらをボールミルによってよく混合した。The porcelain material employed in the present invention was manufactured by a common powder metallurgy method. That is, PbO, TiO2゜MgO,
Raw materials such as Nb2O5 and BaCO3 were accurately weighed onto a predetermined mesh, and mixed well using a ball mill.
次いで前記混合物を800〜850℃の視度で予備焼成
し、さらにボールミルによって粉砕して調製粉とした。Next, the mixture was preliminarily calcined at a diopter of 800 to 850°C, and further pulverized using a ball mill to obtain a prepared powder.
しかる後この製粉末に水あるいはポリビニルアルコール
などの粘結剤を添加配合して、直径251m、厚さ2r
t+ra程度の円板状に加圧成形し、1150〜125
0’O程度の温変で焼成した。焼結された試料を直径2
0龍、厚さ0.5朋に研磨し、両面に1極を焼き付けた
。この円板を20枚、導電性接着剤により積層し一層お
きの電極から交互に正負のリード線を取り出した。以上
のように作製した積層型電歪索子を第2図に示す。After that, water or a binder such as polyvinyl alcohol was added to this powder to form a powder with a diameter of 251 m and a thickness of 2 r.
Pressure molded into a disc shape of about t + ra, 1150 ~ 125
It was fired at a temperature change of about 0'O. The sintered sample has a diameter of 2
It was polished to a thickness of 0.0 mm and a thickness of 0.5 mm, and 1 pole was baked on both sides. Twenty of these disks were laminated with a conductive adhesive, and positive and negative lead wires were taken out alternately from the electrodes of every other layer. The laminated electrostrictive cable produced as described above is shown in FIG. 2.
この素子に、 0.1Hzの±500v三角波電圧を
印加した時の、変位特性を第1図に示す。変位の検出に
は無接触型直線変位ポテンショメータを用いた。図中X
の数値は採用した磁器材料の(Pb 1−xBaz)〔
(Mg1/3Nb2/3)ogoTlo、to〕o3に
おけるBa1iffi換世を表わしている。Figure 1 shows the displacement characteristics when a 0.1 Hz ±500 V triangular wave voltage was applied to this element. A non-contact linear displacement potentiometer was used to detect displacement. X in the diagram
The value of (Pb 1-xBaz) of the adopted porcelain material [
(Mg1/3Nb2/3) ogoTlo, to] represents the Ba1iffi transition in o3.
第1図から、Bafi換量を増加するにつれヒステリシ
スが小さくなりx−0.02でほとんど無視し得る債に
減少することは明らかである。ざらにBatft換量を
増加すると、変位置が小さくなる傾向にるり、電歪索子
として次第に不適当になる。From FIG. 1, it is clear that as the Bafi conversion amount increases, the hysteresis decreases and decreases to an almost negligible bond at x-0.02. If the Batft exchange amount is increased too much, the displacement position tends to become smaller, and it gradually becomes unsuitable as an electrostrictive rope.
f$1図は(Pb 1−zBaz ) ((Mg 1/
3Nb 2/3 )o、9oTio、to )03で表
わされる組成においてXを変化させた磁器材料を用いた
積/1ffl電歪素子の電圧−変位特性を示す図。
第2図は、第1図の特性の測定に用いた。積層型電歪素
子の構造を示す図。
代理人 弁理士 則 近 憲 佑
同 竹 花 喜久男The f$1 diagram is (Pb 1-zBaz ) ((Mg 1/
3Nb 2/3 )o, 9oTio, to )03 A diagram showing voltage-displacement characteristics of a product/1ffl electrostrictive element using a ceramic material in which X is varied in the composition. FIG. 2 was used to measure the characteristics shown in FIG. FIG. 3 is a diagram showing the structure of a stacked electrostrictive element. Agent Patent Attorney Nori Chika Yudo Kikuo Takehana
Claims (2)
1_−_xTi_x)O_3(0.05≦0.15)で
表わされる組成範囲を有する磁器においてPb原子の4
atm%以下をBaで置換した磁器材料を用いたことを
特徴とする電歪素子。(1) Pb [(Mg_1_/_3Nb_2_/_3)_
1_-_xTi_x)O_3 (0.05≦0.15)
An electrostrictive element characterized in that it uses a porcelain material in which atm% or less is replaced with Ba.
とした特許請求の範囲第1項記載の電歪素子。(2) The electrostrictive element according to claim 1, wherein the amount of Ba is 1 atm% or more.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60180942A JPS6242472A (en) | 1985-08-20 | 1985-08-20 | Electrostriction element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60180942A JPS6242472A (en) | 1985-08-20 | 1985-08-20 | Electrostriction element |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6242472A true JPS6242472A (en) | 1987-02-24 |
Family
ID=16091969
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60180942A Pending JPS6242472A (en) | 1985-08-20 | 1985-08-20 | Electrostriction element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6242472A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4918590A (en) * | 1987-11-16 | 1990-04-17 | Sanyo Electric Co., Ltd. | Hybrid circuit module having bridge circuit and rectifying circuit disposed on a same substrate |
-
1985
- 1985-08-20 JP JP60180942A patent/JPS6242472A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4918590A (en) * | 1987-11-16 | 1990-04-17 | Sanyo Electric Co., Ltd. | Hybrid circuit module having bridge circuit and rectifying circuit disposed on a same substrate |
US5005113A (en) * | 1987-11-16 | 1991-04-02 | Sanyo Electric Co., Ltd. | Hybrid circuit module having bridge circuit and rectifying circuit disposed on a same substrate |
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