JPH02253131A - Measuring instrument - Google Patents

Measuring instrument

Info

Publication number
JPH02253131A
JPH02253131A JP1075767A JP7576789A JPH02253131A JP H02253131 A JPH02253131 A JP H02253131A JP 1075767 A JP1075767 A JP 1075767A JP 7576789 A JP7576789 A JP 7576789A JP H02253131 A JPH02253131 A JP H02253131A
Authority
JP
Japan
Prior art keywords
measured
force
physical quantities
electromotive force
acceleration
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
JP1075767A
Other languages
Japanese (ja)
Inventor
Takeshi Uematsu
武 上松
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.)
Nippon Electric Industry Co Ltd
Original Assignee
Nippon Electric Industry 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 Nippon Electric Industry Co Ltd filed Critical Nippon Electric Industry Co Ltd
Priority to JP1075767A priority Critical patent/JPH02253131A/en
Publication of JPH02253131A publication Critical patent/JPH02253131A/en
Pending legal-status Critical Current

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  • Force Measurement Appropriate To Specific Purposes (AREA)

Abstract

PURPOSE:To simultaneously measure respective components in three-dimensonal directions and various physical quantities by operating and converting an external force to an acceleration, a velocity, a frequency, or the like based on the electromotive force of a piezoelectric element which is displaced together with a body to be measured. CONSTITUTION:A body 2 to be measured is supported in a reference body 1, which is formed into a regularly hexahedral hollow box with materials having rigidity, by plural piezoelectric elements 3. Plural piezoelectric elements 3 are arranged in each of three x-axis, y-axis, and z-axis directions; and when the reference body 1 is oscillated by reception of a specific external force F, elements 3 generate the electromotive force corresponding to the extent of displacement due to expansion and contraction while expanding and contracting in accordance with the displacement of the body 2 to be measured. An operating part 4 uses a prescribed conversion formula to perform prescribed operation based on the electromotive force outputted from piezoelectric elements 3 and calculates various physical quantities acting on the body 2 to be measured in a certain direction, and measured force, acceleration, velocity, frequency and their numerical values or the like are displayed on a display part 5.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、ノj、加速度、速度、振動数等の各種物理
量を測定することができる測定装置にかかり、特にその
物理量を三次元方向についてそれぞれ同時に測定するこ
とができる新規の測定装置に関するものである。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a measuring device capable of measuring various physical quantities such as vibration, acceleration, velocity, and frequency, and particularly to a measuring device that can measure the physical quantities in three-dimensional directions. The present invention relates to a new measuring device that can perform simultaneous measurements.

〔従来の技術〕[Conventional technology]

従来より、各種物理量、即ち例えば力、加速度速度、振
動数等を測定するだめの手段として各種測定装置が開発
され、使用されている。
2. Description of the Related Art Conventionally, various measuring devices have been developed and used as means for measuring various physical quantities, such as force, acceleration velocity, vibration frequency, and the like.

〔解決しようとする課題〕[Problem to be solved]

ところで、通常このような測定装置にあっては、一般に
1個の装置で1つの方向及び1種の物理量のみしか測定
が行えず、不便である。また、このような測定装置は、
一般に大型で重量の嵩むものが多く、その分製造コスト
も高い等の欠点がある。
By the way, such a measuring device is generally inconvenient because it can only measure one direction and one type of physical quantity with one device. In addition, such a measuring device
In general, many of them are large and heavy, and their manufacturing costs are correspondingly high.

そこで、この発明は、上記した従来の欠点に鑑み、1個
のもので同時に三次元方向ついての各成分の測定が可能
であると共に、各種の物理量を測定することができ、し
かも軽量小型化を図ることが容易な測定装置を提供する
ことを目的とするものである。
Therefore, in view of the above-mentioned drawbacks of the conventional technology, the present invention is capable of simultaneously measuring each component in three-dimensional directions with a single device, and also being able to measure various physical quantities, while being lightweight and compact. The purpose of this invention is to provide a measuring device that is easy to measure.

〔課題を解決するための手段〕[Means to solve the problem]

即ち、この発明は、絶対座標系に対し通常静止している
と共に外力が作用すると運動するように取付けられた静
止体と、互いに直交する各方向毎に配置された圧電素子
によって前記静止体のケーシング内部に支持された一定
質量の被測定体と、この被測定体の変位動作と共に変位
する圧電素子から出力される起電力を人力し、これに基
づいて所定の変換式を用いて演算を行い、前記外力を被
測定体の所定方向における分力、加速度、速度振動数等
の物理量に演算・変換する演算部とを備えたものである
That is, the present invention provides a stationary body which is normally stationary with respect to an absolute coordinate system and is attached to move when an external force is applied, and a casing of the stationary body by means of piezoelectric elements arranged in each direction orthogonal to each other. The electromotive force output from an internally supported measured object with a constant mass and a piezoelectric element that is displaced along with the displacement movement of the measured object is manually generated, and based on this, calculations are performed using a predetermined conversion formula. The apparatus includes a calculation section that calculates and converts the external force into physical quantities such as component force, acceleration, and velocity frequency in a predetermined direction of the object to be measured.

〔作用〕[Effect]

この発明の測定装置は、外力の作用によって被測定体が
運動変位すると、その変位動作に伴って各圧電素子に特
定の力が作用してこの圧電素子に起電力が発生し、この
発生した起電力を人力した演算部が所定の変換式を用い
て演算を行い、これによって被測定物の特定方向に作用
する力、加速度、速度、振動数等の物理量を算出する。
In the measuring device of the present invention, when the object to be measured undergoes a movement displacement due to the action of an external force, a specific force acts on each piezoelectric element along with the displacement movement, and an electromotive force is generated in the piezoelectric element. A calculation unit using human power performs calculations using a predetermined conversion formula, thereby calculating physical quantities such as force, acceleration, velocity, and frequency that act on the object to be measured in a specific direction.

〔実施例〕〔Example〕

以下、この発明の一実施例について添イて1図面を参照
しながら説明する。
An embodiment of the present invention will be described below with reference to the accompanying drawings.

第1図はこの発明に係る測定装置を示すものであり、こ
の測定装置は、基準体1と、被測定体2と、圧電素子3
と、演算部4と1表示部5とから構成されている。
FIG. 1 shows a measuring device according to the present invention, which includes a reference body 1, a measured body 2, and a piezoelectric element 3.
It is composed of a calculation section 4 and a display section 5.

基準体1は、第2図に示すように剛性を有する材質のも
のを用いて正六面体の中空箱状に形成されており、地球
(絶対座標系)に対し通常は静止した状態となるように
据え付けられているが、外力の作用によって運動するよ
うになっている。
As shown in Figure 2, the reference body 1 is made of a rigid material and is shaped like a regular hexahedral hollow box, and is designed so that it is normally stationary with respect to the earth (absolute coordinate system). Although it is fixed, it is made to move by the action of an external force.

被測定体2は、各種物理量を観測するため外力の作用に
よって基準体I内へ振動変位させるものであり、質量M
の球状のものが使用されており、次に説明する圧電素子
3によって基準体1内方に支持されている。
The object to be measured 2 is vibrated and displaced into the reference object I by the action of an external force in order to observe various physical quantities, and has a mass M.
A spherical member is used, and is supported inside the reference body 1 by a piezoelectric element 3, which will be described next.

圧電素子3は、外力の作用により被測定体2の変位動作
に伴って伸縮しながらその伸縮変位量に応じ起電力を発
生するものであり、この実施例では第2図に示すように
、三次元的な各方向、即ちx、  y、  zの3方向
にそれぞれ2個づつ都合6個配置されており、それぞれ
演算部4の入力端と接続されている。即ち、この実施例
の圧電素子3は、X方向に沿って第1.第2圧電素子3
a、3bとX方向に沿って第3.第4圧電素子3c、3
dと2方向に沿って第5.第6圧電素子3e、3fとか
ら構成されている。なお、この発明の圧電素子としては
、例えばxyzの3方向についてそれぞれ1個づつ都合
3個のもので構成することも可能である。
The piezoelectric element 3 expands and contracts with the displacement of the object to be measured 2 due to the action of an external force, and generates an electromotive force according to the amount of expansion and contraction. In this embodiment, as shown in FIG. A total of six sensors are arranged, two in each of the original three directions, that is, x, y, and z, and each is connected to the input end of the calculation section 4. That is, the piezoelectric element 3 of this embodiment has the first . Second piezoelectric element 3
a, 3b and the third along the X direction. Fourth piezoelectric element 3c, 3
d and the fifth along two directions. It is composed of sixth piezoelectric elements 3e and 3f. Note that the piezoelectric element of the present invention may be configured with a total of three piezoelectric elements, for example, one in each of the three directions of x, y, and z.

演算部4は、圧電素子3から出力される起電力に基づい
て後に説明する所定の変換式を用いて所定の演算を行い
被測定体2の一定方向に作用する各種物理量を算出する
ようになっており、この実施例ではマイクロコンピュー
タが使用されている。
The calculation unit 4 calculates various physical quantities acting on the object to be measured 2 in a certain direction by performing predetermined calculations based on the electromotive force output from the piezoelectric element 3 using a predetermined conversion formula that will be explained later. A microcomputer is used in this embodiment.

表示部5は、演算部4によって算出された各種物理量の
データを表示させるものであり、画面上にその測定した
物理量の種類、即ち力、加速度。
The display unit 5 displays data on various physical quantities calculated by the calculation unit 4, and displays the types of measured physical quantities, ie, force and acceleration, on the screen.

速度1振動数とその数値等とを表示させるようになって
いる。
The speed 1 vibration frequency and its numerical value are displayed.

次に、この実施例の測定装置における圧電素子から発生
ずる起電力に基づいて各種物理量を算出するときの算出
方法について説明する。
Next, a calculation method for calculating various physical quantities based on the electromotive force generated from the piezoelectric element in the measuring device of this embodiment will be explained.

まず、第2図に示すように、基準体1が特定の力Fを受
は振動したときに、その力Fを受けて変位する被測定体
2の変位量を(fイ (t)、ry(t)、f、(t)
)で表すことができるものとする。ここで、説明を簡単
にするために1つの成分、即ぢX成分についてその変位
を調べて見る。
First, as shown in FIG. 2, when the reference body 1 vibrates under a specific force F, the amount of displacement of the measured body 2 that is displaced by the force F is expressed as (f(t)), ry (t), f, (t)
). Here, in order to simplify the explanation, we will examine the displacement of one component, namely the X component.

即ち、第3図において、力FのX成分F、によって第1
.第2圧電素子3a、3bには抵抗力Rが発生するが、
その抵抗力Rは、Xの函数R(x)として表すことがで
きる。そこで、この抵抗力R(x)をティラー展開して
、 R(!1l=cOX +c I父+C2父+・・・・・
・+C+、x ”’+−−・−・− となるが、一般に近似的には第2項までで充分であり、
したがって次式のように表すことができ、即ち、 Rfxl 〜CoX + [: + x       
   、、、 、、・■となる。
That is, in FIG. 3, the X component F of the force F causes the first
.. A resistance force R is generated in the second piezoelectric elements 3a and 3b, but
The resistance force R can be expressed as a function of X, R(x). Therefore, by developing this resistance R(x) with a tiller, R(!1l=cOX +c I father + C2 father +...
・+C+, x ”'+−−・−・− However, generally up to the second term is sufficient approximately,
Therefore, it can be expressed as the following formula, that is, Rfxl ~ CoX + [: + x
, , , , ・■.

今ここで、第4図のように被測定体3のX方向での変位
量fイを0とするような新しい座標系(以下これを絶対
座標系とよぶ)o−x’ を設けたとき、それらの間に
は次式で示すような関係式、即ち座標変換式が成立する
Now, if we set up a new coordinate system (hereinafter referred to as the absolute coordinate system) o-x' in which the amount of displacement f of the object to be measured 3 in the X direction is 0, as shown in Fig. 4. , a relational expression as shown in the following expression, that is, a coordinate transformation expression is established between them.

x  =x+fウ          ・・・・・・■
ここで、この座標変換式■において、時間tについて2
階微分を行うと次式が得られる。
x = x + f ・・・・・・■
Here, in this coordinate transformation formula (■), for time t, 2
By performing step differentiation, the following equation is obtained.

父° −父+78          ・・・・・・■
ところで、一般に第4図に示すような関係にある質量m
の被測定体2については次のような運動方式が成立して
おり、即ち、 m父′+2C大+2kx=O−−−−−−■(但し、k
は弾性定数、Cは減衰係数)ここで0式を0式へ代入し
て、 mx−4−2cx+2kx= −m?t+   +++
・・・■この0式を変形すると、 父+2ε文+w n’ x =−? +1    ””
”■”(但し、ここでε−C/m、ω2=2に7m)と
ころで、一般に■°のような微分方程式にあっては、そ
の一般解χ(被測定体の変位)はx =a −exp 
 [−αt  〕  ・ 5in(βを十ψ)のような
函数形をしており、減衰函数であるため、この実施例の
場合、特殊解のみを完えればよい。
Father ° − Father + 78 ・・・・・・■
By the way, in general, the mass m has the relationship shown in Figure 4.
The following motion method has been established for the measured object 2, that is, m father' + 2 C large + 2 k x = O
(elastic constant, C is damping coefficient) Here, substituting the 0 expression into the 0 expression, mx-4-2cx+2kx= -m? t+ +++
...■If you transform this 0 expression, father + 2ε sentence + w n' x = -? +1 ””
"■" (However, here ε-C/m, ω2 = 2, 7m) By the way, in general, for a differential equation like ■°, the general solution χ (displacement of the measured object) is x = a -exp
It has a function form such as [−αt]·5in (β is 10ψ) and is an attenuation function, so in the case of this embodiment, only the special solution needs to be completed.

ところで、変位fイをフーリエ展開すると、f X= 
党Ci6 exp  [int〕        −−
−−−−■したがって、 (++= −免n 2・Ch−exp C1ntlここ
で、ah−−n2Co      ・・・・・・■と置
くと、 いま、ここでf II8の第n項? Xnについて考え
てみると、■′の式において、 父、+2ε文。+ ωIl’xI+=−?jjha7 
° eXp  I:inl、  ]  −−−−−、■
(、“、■式より) ここで、xl、= a ・exp  [iBt 〕−■
とおくと、 ■、■を■に代入すると、 αβ2・ey、p  [i βt〕+21εαβ’ e
xp〔1βt 〕 + ω、  ’  a  争 ex
p   [’i  βt 〕ah′exp [i n 
t〕 整頓すると、 0≦tく■ のとき0式が成立するためには、 n−β でなければならない。
By the way, when the displacement f is subjected to Fourier expansion, f
Party Ci6 exp [int] --
−−−−■ Therefore, (++= -immune n 2・Ch-exp C1ntlHere, if we put ah−−n2Co ......■, now, here, f The nth term of II8? About Xn If you think about it, in the formula ■′, father, +2ε sentence.+ ωIl'xI+=-?jjha7
° eXp I:inl, ] -----,■
(from the formula, “, ■) Here, xl, = a ・exp [iBt ] − ■
Then, by substituting ■ and ■ into ■, αβ2・ey, p [i βt]+21εαβ' e
xp[1βt] + ω, 'a conflict ex
p ['i βt]ah'exp [i n
t] To put it in order, in order for the formula 0 to hold when 0≦t×■, it must be n−β.

したがって、このとき0式より an −a (−n2+2 εi n+rn2゜)・・
・・・・0が得られる。
Therefore, at this time, from equation 0, an -a (-n2+2 εi n+rn2°)...
...0 is obtained.

ところで、■式よりa、、−−n2c、、なので、とお
くと、■、■式から X n−αIl’ Ch。exp [int]α。・f
、、    (、−、■より)ところで、変位Xは x、=f)、α、°「8゜ f8・ゑα、 ・・・・・・■ 従って、振動する被測定体2の速度は、文−Lα、す。
By the way, from the formula (■), a,, --n2c,, so if we set, then from the formula (■) and (■), X n-αIl' Ch. exp [int] α.・f
,, (from ,−,■) By the way, the displacement Sentence-Lα, Su.

(t) + fiα。f、(t)また、このときの加速
度は、 父=2fia、?、(t)+fiα。¥、 (1)十j
δ。r、(t) また、このときの被測定体2に作用する力F8は、Fx
=m−父 m [2fian・i、(L) +立αhYX(t)−t−云d。f、(t)〕以上、X
成分について求めてきたが、y、  z各成分について
も同様に求められる。
(t) + fiα. f, (t) Also, the acceleration at this time is Father=2fia,? , (t)+fiα. ¥, (1) 10j
δ. r, (t) Also, the force F8 acting on the measured object 2 at this time is Fx
=m-father m [2fian・i, (L) + tachiαhYX(t)-t-yund. f, (t)] or more, X
Although we have calculated this for each component, the y and z components can also be calculated in the same way.

また、このときの合成された速度Vは、V−・ ×2+
、2+22 から、またこれら各成分について合成された加速度αに
ついても、 α−「・「’+ V ’+ 、p ’−から、さらに、
これらの各成分について合成された力Fは、 F−さ「〒−”十F y’−1−F g’から、求めら
れる。
Also, the combined speed V at this time is V-・×2+
, 2+22, and also for the acceleration α synthesized for each of these components, α−"・'+ V '+, p'-,
The combined force F for each of these components can be found from

〔効果〕〔effect〕

以上説明してきたように、この発明に係る測定装置によ
れば、被測定体が運動変位すると、その変位動作に伴っ
て圧電素子から起電力が発生し、この発生した起電力に
基づいて演算部が所定の演算を行い、被測定体に作用す
るカ、加速度、速度振動数等の物理量を三次元での各成
分毎に算出できるため、大型で特殊な、かつ高価な装置
を使用しなくても簡単に測定することができる。
As explained above, according to the measuring device according to the present invention, when the object to be measured undergoes a movement displacement, an electromotive force is generated from the piezoelectric element along with the displacement operation, and the calculation unit uses the generated electromotive force to generate an electromotive force. performs predetermined calculations and can calculate physical quantities such as force, acceleration, and velocity frequency acting on the object to be measured for each three-dimensional component, so there is no need to use large, special, and expensive equipment. can also be easily measured.

また、この発明に係る測定装置によれば、圧電素子から
発生ずる起電力のみを用いて各種の物理量を測定するこ
とができ、極めて実用的である。
Further, according to the measuring device according to the present invention, various physical quantities can be measured using only the electromotive force generated from the piezoelectric element, which is extremely practical.

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

第1図はこの発明に係る測定装置の構成を示すブロック
図、第2図はこの発明に係る測定装置に使用する基準体
とこの基準体内に圧電素子によって取付けられた被測定
体を示す斜視図、第3図及び第4図はそれぞれこの発明
に係る測定装置の作用を説明するための説明図である。 1 ・・・基準体、   3 用圧電素子2 ・・・被
測定体、  4 ・・・演算部。
FIG. 1 is a block diagram showing the configuration of a measuring device according to the present invention, and FIG. 2 is a perspective view showing a reference body used in the measuring device according to the present invention and a measured object attached to the reference body by a piezoelectric element. , FIG. 3, and FIG. 4 are explanatory diagrams for explaining the operation of the measuring device according to the present invention, respectively. 1... Reference body, 3 Piezoelectric element 2... Measured object, 4... Arithmetic unit.

Claims (1)

【特許請求の範囲】 1、絶対座標系に対し通常静止していると共に外力が作
用すると運動するように取付けられた静止体と、 互いに直交する各方向毎に配置された圧電素子によって
前記静止体のケーシング内部に支持された一定質量の被
測定体と、 この被測定体の変位動作と共に変位する圧電素子から出
力される起電力を入力し、これに基づいて所定の変換式
を用いて演算を行い、前記外力を被測定体の所定方向に
おける分力、加速度、速度振動数等の物理量に演算・変
換する演算部とを備えたことを特徴とする測定装置。
[Claims] 1. A stationary body that is normally stationary with respect to an absolute coordinate system and is attached to move when an external force is applied, and the stationary body is fixed by piezoelectric elements arranged in each direction orthogonal to each other. An object to be measured with a constant mass supported inside the casing of the device and the electromotive force output from a piezoelectric element that is displaced along with the displacement movement of this object to be measured are input, and calculations are performed using a predetermined conversion formula based on this input. A measuring device comprising: a calculating section that calculates and converts the external force into physical quantities such as component force, acceleration, velocity frequency, etc. in a predetermined direction of the object to be measured.
JP1075767A 1989-03-28 1989-03-28 Measuring instrument Pending JPH02253131A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1075767A JPH02253131A (en) 1989-03-28 1989-03-28 Measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1075767A JPH02253131A (en) 1989-03-28 1989-03-28 Measuring instrument

Publications (1)

Publication Number Publication Date
JPH02253131A true JPH02253131A (en) 1990-10-11

Family

ID=13585691

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1075767A Pending JPH02253131A (en) 1989-03-28 1989-03-28 Measuring instrument

Country Status (1)

Country Link
JP (1) JPH02253131A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7753899B2 (en) 2003-06-20 2010-07-13 Livedo Corporation Disposable absorbent article
WO2016170848A1 (en) * 2015-04-20 2016-10-27 学校法人早稲田大学 Multiaxial force sensor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7753899B2 (en) 2003-06-20 2010-07-13 Livedo Corporation Disposable absorbent article
WO2016170848A1 (en) * 2015-04-20 2016-10-27 学校法人早稲田大学 Multiaxial force sensor

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