JPS63153473A - Acceleration detector - Google Patents

Acceleration detector

Info

Publication number
JPS63153473A
JPS63153473A JP30197986A JP30197986A JPS63153473A JP S63153473 A JPS63153473 A JP S63153473A JP 30197986 A JP30197986 A JP 30197986A JP 30197986 A JP30197986 A JP 30197986A JP S63153473 A JPS63153473 A JP S63153473A
Authority
JP
Japan
Prior art keywords
magnetic
coils
acceleration
coil
spherical body
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
JP30197986A
Other languages
Japanese (ja)
Inventor
Takeshi Yasukawa
安川 武
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP30197986A priority Critical patent/JPS63153473A/en
Publication of JPS63153473A publication Critical patent/JPS63153473A/en
Pending legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Abstract

PURPOSE:To eliminate mechanical wear, etc., by composing coil assemblies of detection coils which detect the displacement of a magnetic spherical body and ferromagnetic fluid and exciting coils which apply constant magnetic fields to the detection coils, and holding the spherical body in the center of a container by holding coils. CONSTITUTION:Coil assemblies 4 and the inverse of 4, and 4A and the inverse of 4A are composed of couples of detection coils which detect variation in magnetic resistance due to the position shift of the magnetic spherical body 3 and exciting coils which apply constant magnetic fields to the detection coils. The holding coils 5 and the inverse of 5, and 5A and the inverse of 5A are arranged distantly from the coil assemblies respectively and hold the magnetic spherical body 3 by excitation. A G sensor supplies the constant magnetic fields to the detection coils during operation by the exciting coils and detect the variation in the magnetic reluctance of a magnetic circuit due to the displace ment of the magnetic spherical body and magnetic fluid caused on the center axis in the presence of parallel acceleration differentially by the detection coils to detect the direction and magnitude of the acceleration.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、例えば車載用やロボット用等の各種の機械
に装着される加速度検出装置(以下、Gセンサと称する
。)に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to an acceleration detection device (hereinafter referred to as a G sensor) that is mounted on various types of machines, such as vehicles and robots.

〔従来の技術〕[Conventional technology]

従来のGセンサに於ては、−りに振り子穴又はボール式
のものが用いられている。この振シ子又はポール全加速
度の作用体として利用して加速度を検出している。
In conventional G sensors, a pendulum hole or ball type is used. Acceleration is detected using this pendulum or pole as an effector of total acceleration.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来のGセンサは以上のように構成されているので、作
用体がかなり重近大となり且つ大型化し、しかも機械的
な磨耗部分が存在するのでこの部分の磨耗が作用体の重
量の増大につれて顕著となるために寿命を著るしく縮め
、さらに、構造的に複給仕して小型軽量化が困難である
と共に高価となるなどの問題点があった。
Since the conventional G sensor is constructed as described above, the effecting body is quite heavy, large and large, and there is a mechanically worn part, so the wear of this part becomes more noticeable as the weight of the effecting body increases. As a result, the service life is significantly shortened, and furthermore, the structure requires multiple servings, making it difficult to reduce the size and weight, and making it expensive.

この発明は上記のような問題点を解消するためになされ
たもので、簡単な構造で非接触式に加速度を検出できる
Gセンサを得ることを目的とする。
This invention was made to solve the above-mentioned problems, and aims to provide a G sensor that has a simple structure and can detect acceleration in a non-contact manner.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係るGセンサは、強磁性流体中に磁性球体を
浮遊させ、強磁性流体を封入している密閉容器の中心軸
線上でその2つの両側に、検出コイルと励磁コイルとか
ら各々集合構成された4つのコイル集合体及び4つの保
持コイルを配設したものである。
The G sensor according to the present invention has a magnetic sphere suspended in a ferromagnetic fluid, and has a detection coil and an excitation coil assembled on both sides of a closed container enclosing the ferromagnetic fluid on the central axis of the container. 4 coil assemblies and 4 holding coils are arranged.

〔作 用〕[For production]

この発明におけるGセンサは、励磁コイルによの変位に
より生じる磁気回路の磁気抵抗の変化を検出コイルによ
)差動検出して、その加速度の方向及び大きさを検出す
る。
The G sensor according to the present invention differentially detects a change in magnetic resistance of a magnetic circuit caused by a displacement caused by an excitation coil (using a detection coil), and detects the direction and magnitude of the acceleration.

〔実施例〕〔Example〕

以下、この発明の実施例を図について説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図乃至!3図はこの発明の一実施例を示す正面図で
ある。同図に於て、1は非磁性体から成る密閉容器、2
はこの密閉容器1中に封入された強磁性流体、3はこの
強磁性流体2中に浮遊状態に置かれた磁性球体である。
Figure 1~! FIG. 3 is a front view showing an embodiment of the present invention. In the figure, 1 is a closed container made of non-magnetic material, 2
is a ferromagnetic fluid sealed in this closed container 1, and 3 is a magnetic sphere placed in a floating state in this ferromagnetic fluid 2.

4,4,4A、4Aは、例えば密閉容器1の相直交する
左右及び上下の2つの中心軸線X−又、Y−Y上で密閉
容器1の2つの両側に配設され、磁性球体3の位置変化
に伴う磁気抵抗の変化を検出する4個の検出コイル及び
不図示の電源に接続され上記検出コイルに定磁場を与え
る4個の励磁コイルの各対が集合構成された4個のコイ
ル集合体である。5.5.5A。
4, 4, 4A, 4A are arranged on two sides of the closed container 1, for example, on the two orthogonal left and right and upper and lower central axes X- and Y-Y of the closed container 1, and A set of four coils each consisting of four detection coils that detect changes in magnetic resistance due to position changes and four excitation coils that are connected to a power source (not shown) and provide a constant magnetic field to the detection coils. It is the body. 5.5.5A.

5Aは同じく中心軸線X−X、Y−Y上でコイル集合体
4,4,4A、τiとは各々離隔して配設され、不図示
の電源に接続されて励磁によシ上記磁性球体3を保持す
るための4個の保持コイルである。
Similarly, the magnetic sphere 3 is arranged separately from the coil assemblies 4, 4, 4A, and τi on the central axes X-X and Y-Y, and is connected to a power source (not shown) for excitation. There are four holding coils to hold the

か\る構成のGセンサは例えば車載されているものとす
る。
It is assumed that the G sensor having the above configuration is mounted on a vehicle, for example.

次に動作について説明する。通常、加速度Gが作用して
いない無加速度時には、第1図に示す如く通電により発
生する4個の保持コイル5.5゜5A、5Aの磁力の作
用と強磁性流体2から受ける浮力の作用で磁性球体3は
、密閉容器1の中心位置に保持されている。このため、
x−x、y−Y軸線上のコイル集合体4.4,4A、4
Aの検出コイルの磁気回路は全く対称的でsb、その磁
気抵抗は各々等しくなるためX−X、Y−Y軸線上のコ
イル集合体4,4,4A、4Aの検出コイルの差動出力
は零となる。
Next, the operation will be explained. Normally, when there is no acceleration when no acceleration G is acting, the magnetic force of the four holding coils 5.5° 5A, 5A generated by energization and the buoyant force received from the ferromagnetic fluid 2 are applied as shown in Figure 1. The magnetic sphere 3 is held at the center of the closed container 1. For this reason,
Coil assembly on x-x, y-Y axis 4.4, 4A, 4
The magnetic circuit of the detection coil A is completely symmetrical, sb, and its magnetic resistance is equal, so the differential output of the detection coils of the coil assemblies 4, 4, 4A, and 4A on the X-X and Y-Y axes is as follows. It becomes zero.

次に、中心軸線X−又と平行に例えば右方向にGが作用
すると第2図に示す如く、磁性球体3はGの方向とは逆
の方向に変位する。その結果、図示左方では強磁性流体
2の密度が減少するため左側コイル集合体7の検出コイ
ル側の磁気回路における磁気抵抗は増加し、右側コイル
集合体4の検出コイル側の磁気回路における磁気抵抗F
it−iとんど変化しない。従って、両コイル集合体4
.4の励磁コイルの励磁によシ上記各磁気回路に磁場が
与えられているので電磁誘導によシ上記2個のコイル集
合体7.4の検出コイルには誘導電圧差による差動出力
電圧が生じる。この差動出力電圧は磁性球体3の変位量
に伴なう強磁性流体2の変位量に比例すること\なるた
め、この差動出力電圧によシ(左/右)方向のGの大き
さが検出できると共にその極性からGの方向が検出可能
となる。
Next, when a force of G acts parallel to the central axis X, for example in the right direction, the magnetic sphere 3 is displaced in a direction opposite to the direction of G, as shown in FIG. As a result, on the left side of the figure, the density of the ferromagnetic fluid 2 decreases, so the magnetic resistance in the magnetic circuit on the detection coil side of the left coil assembly 7 increases, and the magnetic resistance in the magnetic circuit on the detection coil side of the right coil assembly 4 increases. Resistance F
it-i hardly ever changes. Therefore, both coil assemblies 4
.. Since a magnetic field is applied to each of the above-mentioned magnetic circuits due to the excitation of the excitation coil 7.4, a differential output voltage due to the induced voltage difference is generated in the detection coil of the above two coil assembly 7.4 due to electromagnetic induction. arise. Since this differential output voltage is proportional to the amount of displacement of the ferromagnetic fluid 2 due to the amount of displacement of the magnetic sphere 3, the magnitude of G in the left/right direction depends on this differential output voltage. can be detected, and the direction of G can also be detected from its polarity.

又、中心軸線Y−Yと平行に例えば上方向にGが作用す
ると第3図に示す如く磁性球体3はG方向と逆の下方向
に変位する。その結果、下方向での強磁性流体2の密度
は減少し、下側コイル集合体4Aの検出コイル側の磁気
回路における磁気抵抗は増加し、上側コイル集合体4A
の検出コイル側の磁気回路における磁気抵抗はほとんど
変化しない。従って、両コイル集合体4A、4Aの励磁
コイルの励磁により上記各磁気回路に磁場が与えられて
いるので両コイル集合体4A、4Aの検出コイルには誘
導電圧差によシ差動出力電圧が生じる。との差動出力電
圧の大きさによシ(上/下)方向のGが検出でき、又、
その極性によシGの方向が検出可能となる。かくして本
例に於ては、上下左右の4方向のG検出を可能とするG
センサが実現されるわけである。
Further, when G is applied parallel to the central axis Y-Y, for example in an upward direction, the magnetic sphere 3 is displaced downward in the opposite direction to the G direction, as shown in FIG. As a result, the density of the ferromagnetic fluid 2 in the downward direction decreases, the magnetic resistance in the magnetic circuit on the detection coil side of the lower coil assembly 4A increases, and the magnetic resistance in the magnetic circuit on the detection coil side of the lower coil assembly 4A increases.
The magnetic resistance in the magnetic circuit on the detection coil side hardly changes. Therefore, since a magnetic field is applied to each magnetic circuit by the excitation of the excitation coils of both coil assemblies 4A, 4A, a differential output voltage is generated in the detection coils of both coil assemblies 4A, 4A due to the induced voltage difference. arise. G in the horizontal (up/down) direction can be detected depending on the magnitude of the differential output voltage between the
The direction of G can be detected depending on its polarity. Thus, in this example, the G
This is how the sensor is realized.

なお、上記実施例に於て、強磁性流体2の透磁率が磁性
球体3の透磁率より略10倍以上の値をとることが望ま
しい。
In the above embodiment, it is desirable that the magnetic permeability of the ferromagnetic fluid 2 is approximately 10 times or more greater than the magnetic permeability of the magnetic spheres 3.

第4図乃至第6図はこの発明の第2実施例を示した正面
図である。同図に於て、その特徴とする所は、磁性球体
3の重量全軽減して、磁性球体3の密閉容器1内壁面に
与える倫撃を緩和すべく磁性球体3の表層部のみ全磁性
体3aで形成し、その内部を非磁性体の軽金属(例えば
アルミニウム等)又はプラスチック等の軽い物質3bで
形成したものである。その他の構成及び作用については
第1実施例と同様であるので、その説明全省略する。
4 to 6 are front views showing a second embodiment of the present invention. In the figure, the feature is that only the surface layer of the magnetic sphere 3 is made entirely of magnetic material in order to reduce the total weight of the magnetic sphere 3 and reduce the impact of the magnetic sphere 3 on the inner wall surface of the sealed container 1. 3a, and the inside thereof is made of a light material 3b such as a non-magnetic light metal (for example, aluminum) or plastic. Since the other configurations and operations are the same as those in the first embodiment, the explanation thereof will be omitted entirely.

第7図乃至第9図はこの発明の第3実施例を示す正面図
である。同図に於て、この実施例の特徴とする所は密閉
容器1の内壁部の内で磁性球体3が衝突する内壁面の一
部にゴム等のクッション部材6.百、6A、6Aを四方
に設け、Gセンサの耐久性の向上を計ったものである。
7 to 9 are front views showing a third embodiment of the present invention. In the figure, the feature of this embodiment is that a cushion member 6, such as rubber, is provided on a part of the inner wall surface of the closed container 1 against which the magnetic sphere 3 collides. 100, 6A, and 6A are provided on all sides to improve the durability of the G sensor.

その他の構成要素及び作用については第1実施例と同様
である。
Other components and operations are the same as in the first embodiment.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば励磁コイルによシ検出
コイルに磁場を与え、加速度の作用下で強磁性流体及び
その中の磁性球体が変位し、その変位によシ検出コイル
による検出値に出力差を生じるように構成したので、構
造的に簡単にでき、小型軽量化できると共に部品点数も
少なく低コスト化できると共に非接触式検出であるので
信頼性も高く且つ機械的磨耗や劣化を□生じることもな
く耐久性の向上したものが得られる効果がある。
As described above, according to the present invention, a magnetic field is applied to the detection coil by the excitation coil, the ferromagnetic fluid and the magnetic sphere therein are displaced under the action of acceleration, and the detected value by the detection coil is determined by the displacement. Since it is configured to produce an output difference between the two, it is structurally simple and can be made smaller and lighter, with fewer parts and lower costs.Since it is non-contact detection, it is highly reliable and prevents mechanical wear and deterioration. □There is an effect that a product with improved durability can be obtained without causing any damage.

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

第1図乃至第3図はこの発明の第1実施例を示す各状態
の正面図、第4図乃至第6図はこの発明の第2実施例を
示す各状態の正面図、第7図乃至第9図はこの発明の第
3実施例を示す各状態の正面図である。 図中、lは密閉容器、2は強磁性流体、3は磁性球体、
4,4,4A、TIはコイル集合体、5゜T、5A、5
ズは保持コイル。 なお、図中、同一符号は同一、又は相当部分を示す。
1 to 3 are front views in each state showing a first embodiment of the invention, FIGS. 4 to 6 are front views in each state showing a second embodiment of the invention, and FIGS. FIG. 9 is a front view of the third embodiment of the present invention in various states. In the figure, l is a closed container, 2 is a ferromagnetic fluid, 3 is a magnetic sphere,
4, 4, 4A, TI is a coil assembly, 5°T, 5A, 5
is a holding coil. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.

Claims (4)

【特許請求の範囲】[Claims] (1) 非磁性体からなる密閉容器と、該密閉容器内に
封入された強磁性流体と、該強磁性流体中に浮遊状態に
置かれた磁性球体と、上記密閉容器の相直交する中心軸
線上で上記密閉容器の2つの両側に配置され、加速度の
作用下での上記磁性球体や強磁性流体の変位を検出する
検出コイル及び該検出コイルに定磁場を与えるための励
磁コイルから各々集合構成された4個のコイル集合体及
び通常時は励磁により上記磁性球体を上記密閉容器の中
心に保持するための4個の保持コイルとを備えた加速度
検出装置。
(1) An airtight container made of a non-magnetic material, a ferromagnetic fluid sealed in the airtight container, a magnetic sphere suspended in the ferromagnetic fluid, and orthogonal central axes of the airtight container. A detection coil arranged on two sides of the closed container on a line and configured to detect the displacement of the magnetic sphere or ferromagnetic fluid under the action of acceleration, and an excitation coil for applying a constant magnetic field to the detection coil. An acceleration detecting device comprising four coil aggregates having a magnetic sphere and four holding coils for holding the magnetic sphere at the center of the closed container by excitation during normal times.
(2) 上記強磁性流体の透磁率は上記磁性球体の透磁
率に対し略10倍以上の値であることを特徴とする特許
請求の範囲第1項記載の加速度検出装置。
(2) The acceleration detection device according to claim 1, wherein the magnetic permeability of the ferromagnetic fluid is approximately 10 times or more greater than the magnetic permeability of the magnetic sphere.
(3) 上記磁性球体は表層部のみ磁性体で構成されて
いることを特徴とする特許請求の範囲第1項記載の加速
度検出装置。
(3) The acceleration detection device according to claim 1, wherein only the surface layer of the magnetic sphere is made of a magnetic material.
(4) 上記密閉容器の内壁部の一部がクツシヨン部材
で構成されていることを特徴とする特許請求の範囲第1
項記載の加速度検出装置。
(4) Claim 1, wherein a part of the inner wall of the airtight container is made of a cushion member.
Acceleration detection device described in Section 2.
JP30197986A 1986-12-17 1986-12-17 Acceleration detector Pending JPS63153473A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30197986A JPS63153473A (en) 1986-12-17 1986-12-17 Acceleration detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30197986A JPS63153473A (en) 1986-12-17 1986-12-17 Acceleration detector

Publications (1)

Publication Number Publication Date
JPS63153473A true JPS63153473A (en) 1988-06-25

Family

ID=17903426

Family Applications (1)

Application Number Title Priority Date Filing Date
JP30197986A Pending JPS63153473A (en) 1986-12-17 1986-12-17 Acceleration detector

Country Status (1)

Country Link
JP (1) JPS63153473A (en)

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