JPH05333045A - Piezoelectric acceleration sensor - Google Patents

Piezoelectric acceleration sensor

Info

Publication number
JPH05333045A
JPH05333045A JP16334292A JP16334292A JPH05333045A JP H05333045 A JPH05333045 A JP H05333045A JP 16334292 A JP16334292 A JP 16334292A JP 16334292 A JP16334292 A JP 16334292A JP H05333045 A JPH05333045 A JP H05333045A
Authority
JP
Japan
Prior art keywords
piezoelectric
piezoelectric body
acceleration
amount
acceleration sensor
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
Application number
JP16334292A
Other languages
Japanese (ja)
Inventor
Koichi Mizumura
光一 水村
Yoshiaki Kurihara
義昭 栗原
Hiroshi Ohashi
寛 大橋
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.)
Japan Radio Co Ltd
Original Assignee
Japan Radio 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 Japan Radio Co Ltd filed Critical Japan Radio Co Ltd
Priority to JP16334292A priority Critical patent/JPH05333045A/en
Publication of JPH05333045A publication Critical patent/JPH05333045A/en
Pending legal-status Critical Current

Links

Landscapes

  • Pressure Sensors (AREA)

Abstract

PURPOSE:To easily miniaturize the apparatus and to measure even a small acceleration with high sensitivity by using a piezoelectric body showing a large amount of piezoelectric distortion which is formed of a porous piezoelectric material with many voids. CONSTITUTION:Powders of lead zirconate titanate(PZT) of about 1.2mum average particle size and metacrylic resin of about 30mum average particle size are blended in a suitable ratio, molded and baked. An electric field of approximately 1kV is applied to the baked body, which is then polarized. As a result, a piezoelectric body 1 is obtained. The mixing ratio of the PZT powders and resin powders determines the ratio of voids to the total volume of the obtained porous piezoelectric material (void volume), and also the amount of the piezoelectric distortion. Accordingly, since the piezoelectric body 1 is constructed as above, the amount of the piezoelectric distortion is made large, enabling detection of a small acceleration. Moreover, a minute difference of the acceleration can be detected with high sensitivity.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、圧電体を用いた圧電加
速度センサに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a piezoelectric acceleration sensor using a piezoelectric body.

【0002】[0002]

【従来の技術】図1は、圧電体を用いた圧電加速度セン
サの構成の概略を示す断面図であり、図において、1は
圧電体、2は電極、3は重り(慣性物体)、4はケー
ス、5はベース、6はリード線であり、図面の矢印は圧
電体1の分極方向である。
2. Description of the Related Art FIG. 1 is a sectional view showing the outline of the configuration of a piezoelectric acceleration sensor using a piezoelectric body. In the figure, 1 is a piezoelectric body, 2 is an electrode, 3 is a weight (inertial object), and 4 is Case 5, 5 is a base, 6 is a lead wire, and the arrow in the drawing indicates the polarization direction of the piezoelectric body 1.

【0003】この加速度センサは、加速度を測定する測
定対象物に設置して、重り3の慣性力で加速度を測定す
る。すなわち、ベース5の受ける加速度は、重り3の慣
性力として圧電体1に働き、これに応じて圧電体1の圧
電効果(piezoelectric effect)
により電荷がチャージされる。圧電体1にチャージされ
る電荷量は、圧電体1に電圧を印加したときの圧電体の
歪(electrostriction)と、重り3の
質量と、加速度とに比例する。また、このときに電極2
の両端で発生する電圧は、圧電体1で発生した電荷に比
例し、圧電体1の静電容量に反比例する。従って、この
種の加速度センサは、この電圧値で受けた加速度を検出
する。
This acceleration sensor is installed on an object to be measured for acceleration and measures the acceleration by the inertial force of the weight 3. That is, the acceleration received by the base 5 acts on the piezoelectric body 1 as an inertial force of the weight 3, and in response to this, the piezoelectric effect of the piezoelectric body 1 is exerted.
Is charged. The amount of electric charge charged in the piezoelectric body 1 is proportional to the strain of the piezoelectric body when a voltage is applied to the piezoelectric body 1, the mass of the weight 3, and the acceleration. At this time, the electrode 2
The voltage generated at both ends of is proportional to the charge generated in the piezoelectric body 1 and inversely proportional to the capacitance of the piezoelectric body 1. Therefore, this type of acceleration sensor detects the acceleration received at this voltage value.

【0004】なお、装置の検出感度は圧電体1の性能で
定まる。すなわち、重り3からの慣性力が圧電体1に加
えられたときに発生する電化量は、圧電歪量が大きけれ
ば大きいほど、また、圧電体1の静電容量が小さければ
小さいほど、高感度(高分解能)な装置とでき、装置の
小型化も容易に行える。
The detection sensitivity of the device is determined by the performance of the piezoelectric body 1. That is, as the amount of electrification generated when the inertial force from the weight 3 is applied to the piezoelectric body 1, the greater the amount of piezoelectric strain and the smaller the capacitance of the piezoelectric body 1, the higher the sensitivity. (High resolution) device can be obtained, and the device can be easily downsized.

【0005】[0005]

【発明が解決しようとする課題】上記のようにこの種の
圧電加速度センサの性能は、圧電体の圧電歪量で定まる
ため、高性能な装置とするためには圧電歪量の大きい圧
電体を用いる必要がある。
As described above, since the performance of this type of piezoelectric acceleration sensor is determined by the amount of piezoelectric strain of the piezoelectric body, a piezoelectric body having a large amount of piezoelectric strain should be used for a high performance device. Must be used.

【0006】本発明は、かかる問題点を解決するために
なされたものであり、加えられる加速度が小さい場合で
も大きな電圧で検出できる高感度な圧電加速度センサを
提供することを目的としている。
The present invention has been made to solve the above problems, and an object of the present invention is to provide a highly sensitive piezoelectric acceleration sensor capable of detecting a large voltage even when the applied acceleration is small.

【0007】[0007]

【課題を解決するための手段】本発明に係わる圧電加速
度センサは、多数の空孔が形成された多孔質圧電材質を
用いて形成した圧電歪量の大きな圧電体を使用して構成
したことを特徴とする。
A piezoelectric acceleration sensor according to the present invention is constructed by using a piezoelectric body having a large piezoelectric strain formed by using a porous piezoelectric material having a large number of holes. Characterize.

【0008】[0008]

【実施例】以下、本発明の一実施例を図面を用いて説明
する。本発明における装置の構成は、圧電体1が異なる
だけで従来の技術として説明した図1に示す構成と同様
であり、ここでは重複した説明は省略する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. The configuration of the device according to the present invention is the same as the configuration shown in FIG. 1 described as a conventional technique except that the piezoelectric body 1 is different, and the duplicate description is omitted here.

【0009】次に本発明における圧電体1について説明
する。本発明における圧電体1は、多数の空孔が形成さ
れた多孔質圧電材質を用いて形成される。そして、その
製造方法は、ジルコン酸チタン酸鉛(PZT)等の圧電
材料の粉末とメタクリル樹脂等の有機材料の粉末とを適
当な比で混合して成形,焼成し、電界を印加して分極し
て製造する。
Next, the piezoelectric body 1 of the present invention will be described. The piezoelectric body 1 according to the present invention is formed by using a porous piezoelectric material having a large number of holes. Then, the manufacturing method is as follows. Powder of a piezoelectric material such as lead zirconate titanate (PZT) and powder of an organic material such as methacrylic resin are mixed at an appropriate ratio, molded, fired, and polarized by applying an electric field. And manufacture.

【0010】以下、これを詳細に説明する。例えば平均
粒径1.2μmのジルコン酸チタン酸鉛(PZT)の粉
末と、平均粒径30μmのメタクリル樹脂粉末(例え
ば、ポリメタクリル酸メチルの重合物)を適当な比率で
混合する。この混合比により、製造される多孔質圧電材
質の全体積に占める空孔の比率(以下、これを空孔率と
言う)が定まり、その圧電歪量も定まる。そして、成
形,焼成を行い、1kV/mm程度の電界を印加し、分
極して本発明の圧電体1が得られる。
This will be described in detail below. For example, a lead zirconate titanate (PZT) powder having an average particle diameter of 1.2 μm and a methacrylic resin powder (for example, a polymer of polymethylmethacrylate) having an average particle diameter of 30 μm are mixed at an appropriate ratio. This mixing ratio determines the ratio of pores to the total volume of the manufactured porous piezoelectric material (hereinafter referred to as porosity), and the amount of piezoelectric strain. Then, the piezoelectric body 1 of the present invention is obtained by molding and firing, applying an electric field of about 1 kV / mm and polarization.

【0011】図2は、空孔率と圧電歪量との関係を示す
図であり、図に示すように、多孔質とすることにより必
ず圧電歪量が増大し、圧電歪量は空孔率に依存すること
が解る。また、図3は空孔率と比誘電率との関係を示す
図で、空孔率が増加すればするほど、比誘電率すなわち
静電容量は小さくなり、静電容量が空孔率に依存してい
ることが解る。
FIG. 2 is a diagram showing the relationship between the porosity and the piezoelectric strain amount. As shown in the figure, the piezoelectric strain amount is always increased by making it porous, and the piezoelectric strain amount is the porosity. It turns out that it depends on. FIG. 3 is a diagram showing the relationship between the porosity and the relative permittivity. As the porosity increases, the relative permittivity, that is, the capacitance decreases, and the capacitance depends on the porosity. You can see what you are doing.

【0012】こうして得られた圧電体1で図1に示すよ
うな圧電加速度センサを構成すれば、圧電体1の圧電歪
量を大きくでき、従来の装置では検出できなかった小さ
な加速度の検出も可能となり、また、加速度の微小な相
違も検出できる高感度な装置とできる。
By constructing a piezoelectric acceleration sensor as shown in FIG. 1 with the piezoelectric body 1 thus obtained, the amount of piezoelectric strain of the piezoelectric body 1 can be increased, and a small acceleration which cannot be detected by the conventional device can be detected. In addition, a highly sensitive device capable of detecting a minute difference in acceleration can be obtained.

【0013】なお上記実施例では、圧電体1の圧電材料
としてジルコン酸チタン酸鉛を用い、多孔質を形成する
有機材料としてメタクリル樹脂粉末を用いた例で説明し
ているが、例えばチタン酸鉛,チタン酸バリウム等を用
いることができ、多孔質を形成する材料として他の有機
材料を用いても良い。
In the above embodiment, lead zirconate titanate is used as the piezoelectric material of the piezoelectric body 1 and methacryl resin powder is used as the organic material for forming the porosity. , Barium titanate or the like can be used, and other organic materials may be used as the material for forming the porosity.

【0014】[0014]

【発明の効果】本発明は以上説明したように、多数の空
孔が形成された多孔質圧電材質を用いて形成した圧電体
を用い装置を構成することで、高感度な圧電加速度セン
サが得られるという効果がある。
As described above, according to the present invention, a highly sensitive piezoelectric acceleration sensor can be obtained by constructing an apparatus using a piezoelectric body formed by using a porous piezoelectric material having a large number of holes. There is an effect that is.

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

【図1】圧電加速度センサの構成例を示すブロック図で
ある。
FIG. 1 is a block diagram showing a configuration example of a piezoelectric acceleration sensor.

【図2】空孔率と圧電効果との関係を示す図である。FIG. 2 is a diagram showing a relationship between a porosity and a piezoelectric effect.

【図3】空孔率と比誘電率との関係を示す図である。FIG. 3 is a diagram showing the relationship between porosity and relative permittivity.

【符号の説明】 1 圧電体 2 電極 3 重り 4 ケース 5 ベース 6 リード線[Explanation of symbols] 1 piezoelectric body 2 electrode 3 weight 4 case 5 base 6 lead wire

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 加速度を測定する測定対象物に設置され
るベース上に、その両端に取り出し電極が設けられた圧
電体を介して慣性物体を取り付けて成り、受けた加速度
により慣性物体からの慣性力が圧電体に作用して圧電効
果(piezoelectric effect)によ
り圧電体にチャージされる電荷量を検出して加速度を測
定する圧電加速度センサにおいて、 装置に使用する圧電体に、 例えばジルコン酸チタン酸鉛,チタン酸鉛,チタン酸バ
リウム等の圧電材料を用いて、多数の空孔が形成された
多孔質圧電材質で構成した圧電体を使用することを特徴
とする圧電加速度センサ。
1. An inertial object is mounted on a base, which is installed on an object to be measured whose acceleration is to be measured, through a piezoelectric body having extraction electrodes provided at both ends thereof, and the inertial force from the inertial object is generated by the received acceleration. In a piezoelectric acceleration sensor that measures the acceleration by detecting the amount of charge that is charged in the piezoelectric body due to the force acting on the piezoelectric body due to the piezoelectric effect, the piezoelectric body used in the device may be, for example, lead zirconate titanate. A piezoelectric acceleration sensor characterized by using a piezoelectric body made of a porous piezoelectric material in which a large number of holes are formed by using a piezoelectric material such as lead titanate or barium titanate.
JP16334292A 1992-06-01 1992-06-01 Piezoelectric acceleration sensor Pending JPH05333045A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16334292A JPH05333045A (en) 1992-06-01 1992-06-01 Piezoelectric acceleration sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16334292A JPH05333045A (en) 1992-06-01 1992-06-01 Piezoelectric acceleration sensor

Publications (1)

Publication Number Publication Date
JPH05333045A true JPH05333045A (en) 1993-12-17

Family

ID=15772056

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16334292A Pending JPH05333045A (en) 1992-06-01 1992-06-01 Piezoelectric acceleration sensor

Country Status (1)

Country Link
JP (1) JPH05333045A (en)

Similar Documents

Publication Publication Date Title
US6854330B2 (en) Accelerometer and methods thereof
Xie et al. Flexible and active self-powered pressure, shear sensors based on freeze casting ceramic–polymer composites
Banno Recent developments of piezoelectric ceramic products and composites of synthetic rubber and piezoelectric ceramic particles
Hillenbrand et al. Piezoelectricity in cellular electret films
Suzuki et al. A silicon electrostatic ultrasonic transducer
US20200408619A1 (en) Mechanical-stress sensor and manufacturing method
Pondrom et al. Energy harvesting with single-layer and stacked piezoelectret films
Waller et al. Corona poling of PZT ceramics and flexible piezoelectric composites
US5700359A (en) Method of polarizing at least one large area sheet of ferroelectric material
JP2002513263A (en) Acoustic element
Morten et al. PZT‐based Thick Films and the Development of a Piezoelectric Pressure Sensor
CN100437052C (en) shock sensor
JPH05333045A (en) Piezoelectric acceleration sensor
JPH05296861A (en) Piezoelectric pressure sensor
JPS5911841B2 (en) electret sensing device
US5869761A (en) Impact sensor
Collins The thermal pulsing technique applied to polymer electrets
JPH04115165A (en) Acceleration sensor
Alfaifi et al. Mems humidity sensors
US4390800A (en) Electret device
US4458161A (en) Electret device
JPH0252599A (en) Ultrasonic transducer and its manufacture
JP6513286B2 (en) Capacitive structure and method of determining charge amount using capacitive structure
US4455494A (en) Electret device
US5486320A (en) Method of depolarizing a ferroelectric material using electrical means and its application to obtain a ferroelectric material of reinforced dielectric strength