[go: up one dir, main page]

JPS60104202A - Displacement quantity detecting device - Google Patents

Displacement quantity detecting device

Info

Publication number
JPS60104202A
JPS60104202A JP21210783A JP21210783A JPS60104202A JP S60104202 A JPS60104202 A JP S60104202A JP 21210783 A JP21210783 A JP 21210783A JP 21210783 A JP21210783 A JP 21210783A JP S60104202 A JPS60104202 A JP S60104202A
Authority
JP
Japan
Prior art keywords
magnet
displacement
coil
movable part
current
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.)
Granted
Application number
JP21210783A
Other languages
Japanese (ja)
Other versions
JPH047444B2 (en
Inventor
Akitoshi Kamei
亀井 明敏
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.)
Tokyo Seimitsu Co Ltd
Original Assignee
Tokyo Seimitsu 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 Tokyo Seimitsu Co Ltd filed Critical Tokyo Seimitsu Co Ltd
Priority to JP21210783A priority Critical patent/JPS60104202A/en
Publication of JPS60104202A publication Critical patent/JPS60104202A/en
Publication of JPH047444B2 publication Critical patent/JPH047444B2/ja
Granted legal-status Critical Current

Links

Landscapes

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

Abstract

PURPOSE:To prevent generation of a measuring error, and to raise an accuracy by providing a coil and a magnet so as to be opposed to each other among a basic part, the first movable member and the second movable member, so that a direction and a current value of a current flowing to the oil can be controlled. CONSTITUTION:The first coil 13 and the first magnet 14 of E-type are provided between an arm 31 of the first movable part 4 and the second movable part 8. Each wire of the first coil 13 is combined so as to cut a magnetic flux of the magnet 14, when the first movable part 4 is displaced in the X direction. Also, the second coil 15 and the second magnet 16 are provided between the second movable part 8 and an arm 30 of a basic part 1. In such a structure, when a current is supplied to the coils 13, 15, a power is generated between the magnet and the coil, and magnitude of its power is proportional to magnitude of the flowing current. In this way, by controlling a current value, no measuring error is generated, and the measuring accuracy can be raised.

Description

【発明の詳細な説明】 この発明は三次元座標測定機等に用いられる三次元変位
検出装置(プローブ)の必要とする任意の軸と方向に測
定力を発生させ更に同一機構を用いて所定の軸の動きを
機械的原点にクランプする機構に係るものである。
Detailed Description of the Invention This invention generates a measuring force in any axis and direction required by a three-dimensional displacement detection device (probe) used in a three-dimensional coordinate measuring machine, etc., and further uses the same mechanism to generate a measuring force in a specified direction. This relates to a mechanism that clamps the movement of an axis to a mechanical origin.

三次元変位検出装置は三次元空間の全方向に検出方向を
持っているため、接触子が自由の状態即ち接触していな
い状態では、機械的原点の位置(中心)にあって、何れ
の方向にも測定力を持っていない。今接触によって一方
向に変位が与えられるとこの変位の逆方向即ち中心へ向
って復元しようとする力が発生し、これが測定力として
働く。手動測定により作業者が常に被測定物に接触させ
測定する場合は何の支障も生じないがNG副制御より自
動的に測定を行なう場合法の様な不都合を生しる。
The three-dimensional displacement detection device has detection directions in all directions in three-dimensional space, so when the contact is free, that is, not in contact, it is at the mechanical origin (center) and cannot be detected in any direction. It also does not have the ability to measure. When a displacement is applied in one direction due to contact, a force is generated in the opposite direction of this displacement, that is, toward the center, and this acts as a measuring force. If the worker constantly contacts the object to be measured by manual measurement, no problem will occur, but if the measurement is performed automatically using the NG sub-control, a similar problem will occur.

即し第1図に示す様な被測定物Wを自動測定する場合、
三次元座標測定機に付けられた三次元変位検出型の接触
子は、設露1値の軌跡(点線)を描く様にNG副制御れ
る。第1図のAからBの様な状態の場合接触子は被測定
物に接触し三次元変位検出型に変位を与え誤差が有るこ
とが検出される。しかし第1図BからCの状態の場合接
触子は設露1」二のJ法を示す空間を通過するだけで被
測定物に接触しない。この時三次元変位検出器は機械的
原点を保ち被測定物のN法誤差は零であることを示して
しまう。この様な誤りを防ぐ為には三次元変位検出器と
被測定物の位置関係を判断し接触子に測定力を与えて予
想される誤差範囲をカバー出来る景だけ接触子先端位置
を変位させればよい。原点位置が変ることなく任意方向
に測定力を加えろ方法が本発明の要点である。
Therefore, when automatically measuring the object W to be measured as shown in Fig. 1,
The three-dimensional displacement detection type contact attached to the three-dimensional coordinate measuring machine is subjected to NG sub-control so as to draw a locus (dotted line) of one value of the installed dew. In the case of states A to B in FIG. 1, the contactor contacts the object to be measured and causes a displacement in the three-dimensional displacement detection type, and it is detected that there is an error. However, in the conditions shown in FIG. 1 B to C, the contact only passes through the space showing the J method of the dew installation and does not come into contact with the object to be measured. At this time, the three-dimensional displacement detector maintains the mechanical origin and indicates that the N method error of the object to be measured is zero. To prevent such errors, judge the positional relationship between the three-dimensional displacement detector and the object to be measured, apply measuring force to the contact, and displace the tip of the contact only to cover the expected error range. Bye. The key point of the present invention is a method of applying measuring force in any direction without changing the origin position.

第2図に本発明の基になる三次元変位検出器の概要を示
す。x、y、z各軸の変位検出ユニットは基本的には同
一機構の物で測定部の先端にある接触子に与えられた変
位はフィラーを経て順次各ユニットに伝えられそれぞれ
x、y。
FIG. 2 shows an outline of the three-dimensional displacement detector on which the present invention is based. The displacement detection units for each of the x, y, and z axes basically have the same mechanism, and the displacement applied to the contact at the tip of the measuring section is sequentially transmitted to each unit via the filler, and the displacement is transmitted to each unit sequentially to detect x, y, respectively.

Z直交座標系の一軸方向の変位成分のみ検出する様に構
成されている。各ユニットの機構は同一なのでX軸につ
いて説明ずろ。
It is configured to detect only a displacement component in one axis direction of the Z orthogonal coordinate system. Since the mechanism of each unit is the same, I will explain about the X axis.

第3図はX軸の内部構造を示す。基礎部1をベースにし
て1組の平行バネ2.3により第1可動部材4を吊し、
3の先に測定軸12を設は更にフィラーを経て接触子9
が接続される。基礎部1をベースにして別の1組の平行
バネ6.7は平行バネ2.3に平行に取付けられて第2
司動部8を吊している。平行バネ2.3及び6.7は捩
れ方向に対して強い剛性を有しX方向以外の変位を生じ
ない機構となっている。基礎部1から伸びた腕30と第
2可動部8の間には機械的ストッパー10を設け、また
第1可動部4から伸びた腕31と第2可動部8の同には
1Mfi的ストッパー5を設け、このストッパーを常に
接触状態に付勢するためのスプリング32.33を設け
ている。このIll構により測定部の接触子9の位置は
非接触時に於いては常に定位置にあり安定な機械的原点
を得られろ。基礎部1の腕30と第1可動部4の腕31
の間には相対変位を検出する直線変位検出器11が設け
られ機械的原点にある時出力信号が零になる様に設定さ
れる。
FIG. 3 shows the internal structure of the X-axis. The first movable member 4 is suspended by a pair of parallel springs 2.3 based on the foundation part 1,
A measuring shaft 12 is installed at the tip of 3, and then the contact 9 is connected through a filler.
is connected. Another set of parallel springs 6.7 is mounted parallel to the parallel springs 2.3 on the basis of the foundation part 1, and a second set of parallel springs 6.7
The driving section 8 is suspended. The parallel springs 2.3 and 6.7 have strong rigidity in the torsional direction and are designed to prevent displacement in directions other than the X direction. A mechanical stopper 10 is provided between the arm 30 extending from the base part 1 and the second movable part 8, and a 1Mfi stopper 5 is provided between the arm 31 extending from the first movable part 4 and the second movable part 8. , and springs 32 and 33 are provided to always bias the stopper into contact. Due to this Ill structure, the position of the contactor 9 of the measuring section is always at a fixed position during non-contact, and a stable mechanical origin can be obtained. Arm 30 of the base part 1 and arm 31 of the first movable part 4
A linear displacement detector 11 for detecting relative displacement is provided between the two, and is set so that the output signal is zero when at the mechanical origin.

このような構造おいて接触子9に右方向変位が与えられ
ると第1司動部4はスプリング32の力に抗して右に変
位し、逆に左方向変位が与えられると第1可動部4はス
トッパー5を左へ押し、スプリング33を伸して第2可
動部8を左へ変位させる。変位量は直線検出N11によ
り出力される。接触子9が被測定物より離れ、変位入力
がなくなると再びスプリング32あるいは33の力によ
り機械的原点に復帰し、直線検出器11の出力も零にな
る。
In such a structure, when the contactor 9 is displaced to the right, the first movable portion 4 is displaced to the right against the force of the spring 32, and conversely, when the contactor 9 is displaced to the left, the first movable portion 4 is displaced to the right. 4 pushes the stopper 5 to the left, stretches the spring 33, and displaces the second movable part 8 to the left. The amount of displacement is output by linear detection N11. When the contactor 9 separates from the object to be measured and the displacement input disappears, it returns to the mechanical origin again by the force of the spring 32 or 33, and the output of the linear detector 11 also becomes zero.

次に本発明の第1の目的である測定力発生機構について
説明する。第3図において第1可動部4の腕31と第2
可動部8との間に第1コイル13及びE型の第一磁石1
4を設ける。第1コイル13の各線は第1可動部4がX
方向に変位したとき、磁石14の磁束を切る様に組み合
わされる。
Next, the measuring force generating mechanism, which is the first object of the present invention, will be explained. In FIG. 3, the arm 31 of the first movable part 4 and the second
A first coil 13 and an E-type first magnet 1 are placed between the movable part 8 and the movable part 8.
4 will be provided. Each wire of the first coil 13 is
When displaced in the direction, the magnetic flux of the magnet 14 is cut.

乙のm 構自体は音響用スピーカーのボイスコイル部分
と同様である。同様に第2可動部8と基礎部1の腕30
との間に第2コイル15及び第2磁石16を設ける。
The structure itself is similar to the voice coil part of an acoustic speaker. Similarly, the second movable part 8 and the arm 30 of the base part 1
A second coil 15 and a second magnet 16 are provided between the two.

乙のような構造においてコイル13.15に電流を供給
する装置を設け(図示せず)電流の方向、電流の大きさ
を設定する。コイル13,15に正流を供給すると磁石
とコイルの間には力が発生し、その方向は磁石の極性と
電流の方向により決定され、反発力或いは吸引力となる
。力の大きさは流れる電流の大きさに比例する。今、第
1コイル13に反発力を発生させろ方向に電流を流す。
In the structure shown in B, a device (not shown) for supplying current to the coils 13 and 15 is provided to set the direction and magnitude of the current. When a positive current is supplied to the coils 13 and 15, a force is generated between the magnet and the coil, the direction of which is determined by the polarity of the magnet and the direction of the current, and becomes a repulsive force or an attractive force. The magnitude of the force is proportional to the magnitude of the flowing current. Now, a current is applied to the first coil 13 in a direction to generate a repulsive force.

電流値を増加すると反発力が増大し、ストッパー5を接
触状態に付勢しているスプリング32の力より大きくな
ったとき第1可動部4は右方向へ移動し、これに連なる
フィラー、接触子9も右へ移動する。スプリング32は
伸びてコイル13の反発力と平衡に達したところで第1
可動部4は停止する。この時のコイル13の反発力が右
方向の測定力として働く。なお第1可動部4が右に動く
とき反作用により第2可動部8を左に動かず力が作用す
るが第2可動部8はスプリング33により右方向に付勢
されているので動くことはない。
As the current value increases, the repulsive force increases, and when it becomes greater than the force of the spring 32 that urges the stopper 5 into contact, the first movable part 4 moves to the right, and the filler and contactor that are connected to it move to the right. 9 also moves to the right. When the spring 32 stretches and reaches equilibrium with the repulsive force of the coil 13, the first
The movable part 4 stops. The repulsive force of the coil 13 at this time acts as a measuring force in the right direction. Note that when the first movable part 4 moves to the right, a reaction force acts on the second movable part 8 without moving it to the left, but the second movable part 8 is biased rightward by the spring 33, so it does not move. .

左方向の測定力を発生させる場合は、第2コイル15に
反発力を発生する方向に電流を流し第2可動部を左方へ
変位させる。第1可動部4及びこれに連なるフィラー、
接触子9はストッパー5を介してスプリング32で結合
されているので左方へ変位する。なお磁石およびコイル
の位置を右に取付けた場合には吸引力を発生させて測定
力とすれば同じ動作となる。以上説明したように任意の
方向に測定力を加え接触子位置を変位させることが可能
であるからNC制御信号より接触子の移動方向の信号を
得て移動方向に接触子を変位させて使用することが出来
る。
When generating a measuring force in the left direction, a current is applied to the second coil 15 in a direction that generates a repulsive force to displace the second movable portion to the left. A first movable part 4 and a filler connected thereto,
Since the contactor 9 is coupled with the spring 32 via the stopper 5, it is displaced to the left. Note that if the magnet and coil are mounted on the right side, the same operation will occur if an attractive force is generated and used as the measuring force. As explained above, it is possible to displace the position of the contact by applying a measuring force in any direction, so it is used by obtaining a signal in the moving direction of the contact from the NC control signal and displacing the contact in the moving direction. I can do it.

本装置の槽造としては第3図に示す他、磁石の大型化に
より可動部重量が増大して測定部の動きを悪化させる心
配のある場合は第4図のごとく第1磁石14、第2磁石
16とも基礎部1よりの腕部30に取付けても動作およ
び効率は同じである。
The structure of the tank for this device is shown in Figure 3. In addition, if there is a concern that the weight of the movable part will increase due to the enlargement of the magnet and worsen the movement of the measuring part, as shown in Figure 4, the first magnet 14, the second magnet 14, Even if the magnet 16 is attached to the arm portion 30 from the base portion 1, the operation and efficiency are the same.

次に本発明の第2の目的である同一機構を用いたクラン
プ機構について説明する。第5図においてXY平面上に
置かれた被測定物を三次元変位検出装置をX軸にそって
(−)方向(図では左方向)に移動し接触させ測定する
場合を例示する。三次元変位検出装置の原点がXoの所
で接触子9が被測定物Wの■の点で接触した後更に−a
JiX軸方向に移動した場合、三次元変位検出装置内の
可動部は変位を生じる。乙の時相ずる変位量はY軸方向
に変位が生じない場合には−aと逆方向のΔ1となるが
一般には被測定物と接触子の間の接触角、摩擦係数、各
軸相互の測定力の不均一性等によりX軸方向変位O1Y
軸変位のみΔ4を示すまでの間の任意の変位を生じ一定
とならない。Z軸変位を含む場合は更に複雑になる。実
際の測定の於ては指定する特定の軸方向変位を検知する
必要があり、乙の為にはそれ以外の軸方向変位を生じな
い様にするクランプ装置が必要となる。本発明において
はクランプ装置を特に設けることなく前記した測定力発
生用の磁石及びコイルを用いて、コイルに吸引力が発す
る方向に電流を流し、可動部の動きを制限することが可
能である。
Next, a clamp mechanism using the same mechanism, which is the second object of the present invention, will be explained. In FIG. 5, a case is illustrated in which the three-dimensional displacement detection device is moved along the X axis in the (-) direction (to the left in the figure) and brought into contact with the object to be measured placed on the XY plane. After the contact 9 contacts the object to be measured W at point ■ at the point where the origin of the three-dimensional displacement detection device is Xo, further -a
When moving in the JiX axis direction, the movable part within the three-dimensional displacement detection device causes displacement. If there is no displacement in the Y-axis direction, the amount of time-synchronized displacement of B will be Δ1 in the opposite direction to -a, but in general, it is determined by the contact angle between the object to be measured and the contact, the coefficient of friction, and the mutual relationship between each axis. X-axis direction displacement O1Y due to non-uniformity of measurement force, etc.
Only the shaft displacement causes arbitrary displacement until it shows Δ4 and is not constant. It becomes even more complicated when Z-axis displacement is included. In actual measurement, it is necessary to detect a specific specified axial displacement, and for this purpose a clamping device is required to prevent any other axial displacement from occurring. In the present invention, it is possible to restrict the movement of the movable part by using the above-mentioned measuring force generating magnet and coil without particularly providing a clamping device, and by passing current through the coil in the direction in which the attractive force is generated.

以」二詳述したように本発明は三次元変位検出装置のX
YZ各軸ユニットにそれぞれ2つの磁石および電磁コイ
ルを設け、所望する軸の2つの電磁コイルを選択的に吸
引あるいは反発させまたその電流値を制御することによ
って、その軸を変位さゼで測定力を発生させると共に、
同一機構を用いて所望の軸を機械的原点にクランプする
ようにしたものであって、特に自動測定に際して測定誤
差を生ぜしめず、高精度の測定が可能となった。
As described in detail below, the present invention is a three-dimensional displacement detection device.
Two magnets and electromagnetic coils are provided in each YZ axis unit, and by selectively attracting or repelling the two electromagnetic coils of the desired axis and controlling the current value, it is possible to measure force by displacing that axis. As well as generating
The same mechanism is used to clamp the desired axis to the mechanical origin, making it possible to perform highly accurate measurements without causing measurement errors, especially during automatic measurements.

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

第1図は測定力を付与しない状態におけるNC測定の場
合の測定位置の説明図、第2図は本発明を内蔵する三次
元変位検出器の外観図、第3図は本発明の一実施例を示
す正面図、第4図は他の実施例正面図、第5図は軸をク
ランプしない状態におけるXY平面上での測定値のバラ
ツキを示す説明図。 1:基礎部 2.3.6.7:平行バネ4:第1可動部
 5、lO:ストツパ 8:第2可動部 9:接触子 ll:直線検出型13:
第1コイル 14:第1磁石 15:第2コイル16:
第2磁石 特許出願人 株式会社東京精密
Fig. 1 is an explanatory diagram of the measurement position in the case of NC measurement without applying a measuring force, Fig. 2 is an external view of a three-dimensional displacement detector incorporating the present invention, and Fig. 3 is an embodiment of the present invention. FIG. 4 is a front view of another embodiment, and FIG. 5 is an explanatory diagram showing variations in measured values on the XY plane in a state where the shaft is not clamped. 1: Foundation part 2.3.6.7: Parallel spring 4: First movable part 5, lO: Stopper 8: Second movable part 9: Contactor ll: Linear detection type 13:
First coil 14: First magnet 15: Second coil 16:
Second magnet patent applicant Tokyo Seimitsu Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] (1)基礎部に対し、2組の平行バネによって関連され
た第1、第2の可動部材と第1可動部材に取付けられた
測定部によって構成された定方向の変位検出装置におい
て基礎部、第1可動部祠、第2可動部材の同1こ相対し
てフィル、磁石を設け、:1イルに流ず電流の方向、T
I電流値制御可能とし、この電流の方向、電流値を制御
することにより任意の方向に測定力を発生させ或いは任
意の軸方向変位をクランプすることを可能にした変位量
検出装置。 (21qti許請求の範囲第1項の記載:ζおいて変位
量検出装置を3ケ用いて変位方向xyz軸の座標系を構
成したことを特徴とする変位量検出装置。
(1) In a fixed-direction displacement detection device configured with first and second movable members related to each other by two sets of parallel springs and a measurement unit attached to the first movable member, the base part; A fill and a magnet are provided opposite the same one of the first movable member and the second movable member.
A displacement detection device that is capable of controlling an I current value, and is capable of generating a measuring force in any direction or clamping any axial displacement by controlling the direction and value of this current. (21qti Claim 1: A displacement detection device characterized in that a coordinate system of xyz axes in the displacement direction is constructed using three displacement detection devices in ζ.
JP21210783A 1983-11-10 1983-11-10 Displacement quantity detecting device Granted JPS60104202A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21210783A JPS60104202A (en) 1983-11-10 1983-11-10 Displacement quantity detecting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21210783A JPS60104202A (en) 1983-11-10 1983-11-10 Displacement quantity detecting device

Publications (2)

Publication Number Publication Date
JPS60104202A true JPS60104202A (en) 1985-06-08
JPH047444B2 JPH047444B2 (en) 1992-02-12

Family

ID=16616991

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21210783A Granted JPS60104202A (en) 1983-11-10 1983-11-10 Displacement quantity detecting device

Country Status (1)

Country Link
JP (1) JPS60104202A (en)

Also Published As

Publication number Publication date
JPH047444B2 (en) 1992-02-12

Similar Documents

Publication Publication Date Title
US11867666B2 (en) Measuring system, measuring arrangement and method for determining measuring signals during a penetration movement of a penetration body into a surface of a test body
JPH0586845B2 (en)
CN103543613B (en) A kind of moving-iron type is without the six-freedom-degree maglev motion platform of cable
US6922905B2 (en) Probe head for a coordinate measuring apparatus
JPH11264776A (en) Testing device
JP2017201258A (en) Fatigue test method and fatigue test apparatus
US9267987B2 (en) Apparatus for testing wafers
Ghalamestani et al. Magnetostriction measurement by using dual heterodyne laser interferometers
JPS60104202A (en) Displacement quantity detecting device
JPH05332766A (en) Copying probe
JPH0334660Y2 (en)
JP2018179619A (en) Probe unit and printed wiring board inspection device
KR102002814B1 (en) Extensometer for sit(structural integrity test) of nuclear power plants
JPH08201010A (en) Probe for measuring apparatus
JP4402112B2 (en) Flat direct drive with position measuring system
CN115615299A (en) Valve with position detection device
JP2686200B2 (en) Friction force measuring method and measuring apparatus therefor
JP4139612B2 (en) Precision machining stage equipment
JPH0421050Y2 (en)
JP2011133317A (en) Displacement measurement apparatus
JPS60119402A (en) Tactile sense device
US2956212A (en) Transducing apparatus
JPH1047944A (en) Position detector
JPH10148204A (en) Actuator
JP2642818B2 (en) Position measuring device