JPS6190895A - Force sensor transformation matrix detection method - Google Patents
Force sensor transformation matrix detection methodInfo
- Publication number
- JPS6190895A JPS6190895A JP59210435A JP21043584A JPS6190895A JP S6190895 A JPS6190895 A JP S6190895A JP 59210435 A JP59210435 A JP 59210435A JP 21043584 A JP21043584 A JP 21043584A JP S6190895 A JPS6190895 A JP S6190895A
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- transformation matrix
- force sensor
- sensor
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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は、ロボットに装着場れる6軸力センサ(即ち力
の3成分とトルクの3成分を検出できる)における歪′
成圧と力(力とトルクを総称して“力″と示す)との関
係を示す変換行列を自動的に検出する検出方法に関する
。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention is directed to the measurement of strain in a six-axis force sensor (that is, capable of detecting three components of force and three components of torque) mounted on a robot.
The present invention relates to a detection method for automatically detecting a transformation matrix indicating the relationship between forming pressure and force (force and torque are collectively referred to as "force").
力センサはロボットに装着され、その該当部分の力と歪
電圧との関係を見出す。歪電圧と力との関係は、一義的
に決定逼れるものであす、el、式上は、次式となる。A force sensor is attached to the robot to find the relationship between force and strain voltage at the relevant part. The relationship between strain voltage and force is uniquely determined, el, and the equation is as follows.
F=(B)V ・・・・・・・・・・・・(1
)ある。〔B〕 は、FとVとの関係を示す定数であ
り、一般に変換行列と呼ばれる。FとVとは共にベクト
ルで表現できる。F=(B)V ・・・・・・・・・・・・(1
)be. [B] is a constant indicating the relationship between F and V, and is generally called a transformation matrix. Both F and V can be expressed as vectors.
変換行列〔B〕 を求める従来例には、U S P。A conventional example of calculating the transformation matrix [B] is USP.
4094192 r Method andAonar
atus for SixDegrpe ofFree
dom Farce Sensing J がある0
この従来例の測定装置を第1図に示す。ベース1に力セ
ンサ2を固定して取付ける。力センサ2の移動部3にケ
ーブル4を取付け、このケーブル4の先端に滑車を介し
て分銅5をつり下げる。かかる装置で、分銅5の1爆を
変えたり、ケーブル4の取付方間を変えたりする。これ
によって、を換行列に必要なデータを得、変換行列の算
出を行う0
この従来例は、変換行列を求める有力な方法であるが、
多くの労力と時間を必要とする問題点を持つ。4094192 r Method and Aonar
atus for Six Degrees of Free
dom There is Farce Sensing J0
This conventional measuring device is shown in FIG. The force sensor 2 is fixed and attached to the base 1. A cable 4 is attached to the moving part 3 of the force sensor 2, and a weight 5 is suspended from the tip of the cable 4 via a pulley. With such a device, the number of strokes of the weight 5 can be changed, and the way in which the cable 4 is attached can be changed. By doing this, we obtain the data necessary for the transformation matrix and calculate the transformation matrix. This conventional example is an effective method for calculating the transformation matrix, but
It has problems that require a lot of effort and time.
本発明は、ロピノト自体に力センサを装着したままで変
換行列の検出を可能とした力センサの変換行列の検出方
法を提供することを目的とする。SUMMARY OF THE INVENTION An object of the present invention is to provide a method for detecting a transformation matrix of a force sensor, which makes it possible to detect a transformation matrix while the force sensor is attached to the lopinoto itself.
本発明は、ロゲットに力センサと標準ワークを装着して
異る姿勢を取らすことが、力センサに対して多くの独立
な力(力ととルク)を加えたことと同等になることに層
目してな嘔れた。肌ち、口♂ソトに力センサ及び適切な
標準ワークを装着妊せた状態で、ある条件に基づき、首
を振らして数種の異る姿勢を取らすだけで自動的に変換
行列を検出するようにした。The present invention shows that attaching a force sensor and a standard workpiece to a logget and taking different postures is equivalent to applying many independent forces (force and torque) to the force sensor. I was disgusted by the layers. A force sensor and an appropriate standard workpiece are attached to the skin and mouth of a pregnant woman, and the transformation matrix is automatically detected by simply shaking the head and assuming several different postures based on certain conditions. I decided to do so.
第2図は、本発明の詳細な説明図である。アーム11は
ロビノトの一部を構成するアームである。FIG. 2 is a detailed explanatory diagram of the present invention. Arm 11 is an arm that constitutes a part of Robinoto.
アーム11の先端とハンド部13との間に、力センサ1
2を取付ける。この力センサ12は、歪ゲージであり、
ハンド部13に加わった力に感応して力対応の歪電圧を
発生する。ここで、力とは、力とトルクとの両者を云う
。この力は、6次元ベクトルとなる。A force sensor 1 is installed between the tip of the arm 11 and the hand portion 13.
Install 2. This force sensor 12 is a strain gauge,
In response to the force applied to the hand portion 13, a strain voltage corresponding to the force is generated. Here, force refers to both force and torque. This force becomes a six-dimensional vector.
ベースの座標軸(ob Xb7bzb)と力センサ1
2の座標軸(Os ”3 7.−Z、 ) とは第
2図に示す如く異なる。Base coordinate axis (ob Xb7bzb) and force sensor 1
As shown in FIG. 2, it is different from the coordinate axes of No.
力センサ12の構成を第3図に示す。外部部材21と内
部部材nと薄板部材nとエリ成る。外部部材21はアー
ム部11の先端部に固定し、内部部材nはバンド部13
に固定する。薄板部材22は、内部部材%と外部部材2
1とを連結する。この薄板部材四の一部に歪ゲージ冴を
取付ける。The configuration of the force sensor 12 is shown in FIG. It consists of an outer member 21, an inner member n, and a thin plate member n. The external member 21 is fixed to the tip of the arm part 11, and the internal member n is fixed to the band part 13.
Fixed to. The thin plate member 22 has an inner member% and an outer member 2
Connect with 1. A strain gauge is attached to a part of this thin plate member 4.
この構成で、ハンド部13に力が加わると、それに連結
した内部部材乙に力が伝わり、連結板24を介して歪ゲ
ージあがたわむ。この歪み対応の電圧が歪グージムの出
力端子を現われ、電圧の検出となる。ここで、薄板部の
数、寸法、取付位置、及び歪ゲージの貼付ける枚数位置
等を適切に定めることによって、力と歪電圧との関係が
一義的に定まる。従って、歪電圧の太き塔から力を検出
できる。この力と歪電圧との関係を定めるのが、変換行
列〔B〕 である。With this configuration, when a force is applied to the hand portion 13, the force is transmitted to the internal member B connected thereto, and the strain gauge is deflected via the connecting plate 24. A voltage corresponding to this distortion appears at the output terminal of the distortion goojim, resulting in voltage detection. Here, the relationship between force and strain voltage is uniquely determined by appropriately determining the number, dimensions, and mounting positions of the thin plate parts, the number of strain gauges to be attached, and the like. Therefore, force can be detected from the thick tower of strain voltage. The transformation matrix [B] determines the relationship between this force and strain voltage.
(1)変換行列〔B〕 を求めるための前提事項。(1) Prerequisites for finding the transformation matrix [B].
力センサ12の歪電圧Vは、厳密には、V=vo−vd
・・・・・・・・・・・・(2)で規定できる。Strictly speaking, the strain voltage V of the force sensor 12 is V=vo-vd
・・・・・・・・・・・・It can be specified by (2).
ここで、■、は、力センサ12に力が加わらない(内部
重量も力とみなす)時の発生電圧である。このVNは、
n次元ベクトルとなる。Here, ■ is the voltage generated when no force is applied to the force sensor 12 (internal weight is also considered as force). This VN is
It becomes an n-dimensional vector.
voは、力センサ12に力(内部重量も力とみなす)が
、実際に加わった時に発生する電圧である。この電圧v
oもn次元ベクトルとなる。但し、n≧6である。vo is a voltage generated when force (internal weight is also considered as force) is actually applied to the force sensor 12. This voltage v
o is also an n-dimensional vector. However, n≧6.
力Fは、力センサ12に加わる力であり、センサ座標本
で考える。この力Fは、力・トルクより成り、6次元ベ
クトルとなる。The force F is a force applied to the force sensor 12, and is considered in terms of sensor coordinates. This force F consists of force and torque and becomes a six-dimensional vector.
更に、力Fと歪電圧Vとは、線形な関係にあるものとす
る。この結果、
F=〔B)V ・・・・・・・・・・・・(3)
が成立する。ここで、CBIは、6行n列の行列となる
。Furthermore, it is assumed that the force F and the strain voltage V have a linear relationship. As a result, F=[B)V ・・・・・・・・・・・・(3)
holds true. Here, CBI is a matrix of 6 rows and n columns.
(2) 電圧vdを求めるための手順。(2) Procedure for determining voltage vd.
内部重量は無視して考えられない。しかし、内部重量W
in、内部重量の重心位置din(図2で示した’s
”s ’s ”sで示芒れるセンサ座標系(以後
S系と称す)で表わされた値)とは設計図面等を利用し
て事前に求まる故、既知と考えてよい。Internal weight cannot be ignored. However, the internal weight W
in, the center of gravity position din of the internal weight ('s shown in Figure 2)
The value expressed in the sensor coordinate system (hereinafter referred to as the S system) indicated by s is determined in advance using a design drawing or the like, so it can be considered to be known.
内部重量Winを取り除いた時の歪ゲージ電圧vdを求
めたいが+ W inはセンサの一部であり取除くこと
はできない。そこで、以下の方法をとる。I would like to find the strain gauge voltage vd when the internal weight Win is removed, but +Win is part of the sensor and cannot be removed. Therefore, we will take the following method.
力センサ−2をロゴノドのアーム部11の先端に取付け
る。更に、先センサー2の先端には何もつけない。従っ
て、実際のロゴノド動作系である第2図の如きハンド部
13の取付けはしない。The force sensor 2 is attached to the tip of the arm portion 11 of the logo nose. Furthermore, do not attach anything to the tip of the tip sensor 2. Therefore, the hand portion 13 as shown in FIG. 2, which is the actual logo-nod operation system, is not attached.
そこで、センサ座標系の座ml111z、を下向き、即
ち重力の方向を向くようにロゴノドを操作する。座標軸
2、が重力方向になった条件下で、力センサ−2で歪電
圧を測定する。この歪電圧をvd owとする。Therefore, the robot is operated so that the position ml111z of the sensor coordinate system faces downward, that is, toward the direction of gravity. The strain voltage is measured by the force sensor 2 under the condition that the coordinate axis 2 is in the direction of gravity. Let this strain voltage be vdow.
次に、センサ座標系の座標軸2 を上向きの姿勢とし、
この姿勢のもとで力センサ−2で歪電圧を測定する。こ
の歪電圧を■。、とする。Next, set the coordinate axis 2 of the sensor coordinate system in an upward posture,
Under this posture, the force sensor 2 measures the strain voltage. ■ This distortion voltage. , and so on.
VdowとV u p とより、電圧Vd は、次式
で求める。From Vdow and V up , voltage Vd is determined by the following equation.
”a = (’dow + ”up )/2 −−−
(4)この下向き、上向きとは、姿勢を重力方向に関し
て反転するとの考え方であり、これにより、力センサに
710わる内部重量に工って生じる刀とトルクとのそれ
ぞれの正負が反転し相殺されて零となる。今、下向き姿
勢時の重力方向の単位ベクトルを”dow (S系表示
)、上向き姿勢時の重力方向の単位ベクトルをUu、
(S系表示〕とする。但し、いずれも、センサ座標系で
考える。この場合、u do W=u up
”””””” (5)となる。そこで、力F1.トルク
F2は、となる。"a = ('dow + "up)/2 ---
(4) These downward and upward directions are based on the concept of reversing the posture with respect to the direction of gravity, so that the positive and negative of the sword and torque generated by the internal weight of the force sensor are reversed and canceled out. becomes zero. Now, the unit vector in the direction of gravity when facing downward is "dow" (S system display), and the unit vector in the direction of gravity when facing upward is Uu.
(S-system display). However, both are considered in the sensor coordinate system. In this case, u do W=u up
”””””” (5). Therefore, force F1. The torque F2 is as follows.
従って、(4)式は正しく 、(4)式より電圧vdが
求まることとなる。Therefore, equation (4) is correct, and voltage vd can be found from equation (4).
(3)歪電圧Vと力Fとを求めるための手順。(3) Procedure for determining strain voltage V and force F.
第2図で示したノ・ンド部13の代りに、標準ワークを
力センサ12に取付ける。第4図に標準ワークを取付け
た際の斜視図を示す。標準ワーク31は、重量Wst
、センサ座標系のもとての重心位置datとする。この
W、j l d3tは共に、既知とする。A standard workpiece is attached to the force sensor 12 in place of the grip section 13 shown in FIG. Figure 4 shows a perspective view of the standard workpiece installed. The standard workpiece 31 has a weight Wst
, the original center of gravity position dat of the sensor coordinate system. It is assumed that both W and j l d3t are known.
内部重量Winに対してW、tなる標準ワーク13を付
加したこととなるから、両者の重量Wは、W=Wi n
+ ”st −・−・・(8)となる。Since the standard workpiece 13 W and t are added to the internal weight Win, the weight W of both is W=Win
+ ”st −・−・・(8).
一方、重心位置d(S系表示)は、
d = (Win’ d in + Wst ”、0
/(Wt n+Wat ) ・・・(9)となる。On the other hand, the center of gravity position d (S system display) is d = (Win' d in + Wst'', 0
/(Wt n+Wat ) (9).
ここで、第2図に示す如く、アーム11のベースの座標
系(’b Xb Ybzb)において、重力方向を
示す単位ベクトルをi、とする。このi、は既知である
。Here, as shown in FIG. 2, in the coordinate system ('b Xb Ybzb) of the base of the arm 11, the unit vector indicating the direction of gravity is defined as i. This i is known.
センサ座標系での重心方向を示す単位ベクトルを13と
する。センサ座標系での各座標軸方向の単位ベクトルを
f 、g 、hとする。この条件下では、下式が成立つ
。Let 13 be the unit vector indicating the direction of the center of gravity in the sensor coordinate system. Let f , g , and h be unit vectors in each coordinate axis direction in the sensor coordinate system. Under this condition, the following formula holds true.
”s =” ’ g 、’ )T’ y b ・” ・
・・”’ (io)さて、力センサの内部重量と標準ワ
ークの重量の双方を考慮したもとでの力・トルクはまと
めてFとすると。"s ="' g , ' ) T' y b ・” ・
..."' (io) Now, let's say that the force and torque are collectively F when considering both the internal weight of the force sensor and the weight of the standard workpiece.
となる。ここで、Fは、センナ座標系として表示し、ト
ルクとは、センサ座標系での原点まわりのトルクとする
。Fは6次元ベクトルである。becomes. Here, F is expressed as a sensor coordinate system, and torque is torque around the origin in the sensor coordinate system. F is a six-dimensional vector.
ベクトルFの6要素は、力のx、y、z軸成分。The six elements of vector F are the x, y, and z axis components of force.
トルクの!、7.Z軸成分を云う。Of torque! ,7. Refers to the Z-axis component.
一方、歪電圧Vは、(2)より求まる。即ち、実際の歪
電圧voを求め、このvoから電圧vdを差引けば、■
を求めることができる。On the other hand, the strain voltage V can be found from (2). That is, by finding the actual strain voltage vo and subtracting the voltage vd from this vo, we get ■
can be found.
(4)菱撲行夕11 CB 〕を求めるための手順。(4) Procedure for finding 11 CB].
以上の(3)項で述べた工程は、1つの姿勢と1つの標
準ワークのもとての1つの測定例である。実際には、姿
勢を変化妊せ、標準ワークを変化(重量や重心位置の変
化)畑せたそれぞれの条件のもとで測定することとなる
。The process described in item (3) above is an example of measurement using one posture and one standard workpiece. In reality, measurements are taken under various conditions, including changing the posture and changing the standard workpiece (changes in weight and center of gravity position).
そこで、(姿勢al lワークb、)、(姿勢IL2
rワークb2)、・・・、(姿勢amlワークbm)の
もとてそれぞれ測定を行うと、
が得られることとなる。02)式を行列でまとめると、
・・・・・・・・・03)
となる。ここで、〔Fl、F2.・・・、Fm〕は6行
m列の行列、〔B〕は6行n列の行列、(Vl + F
2 + ”’ 、V曜は5行m列の行列となる。但し、
m≧5.n≧6である。また、F、 、F2.・・・、
Fmの中には少なくとも6個の独立なベクトルを含むこ
ととする。Therefore, (posture al l work b,), (posture IL2
If measurements are made for each of r workpieces b2), . . . (posture aml workpiece bm), the following will be obtained. 02) When formulas are summarized in a matrix, it becomes...03). Here, [Fl, F2. ..., Fm] is a matrix with 6 rows and m columns, [B] is a matrix with 6 rows and n columns, (Vl + F
2 + "', V day is a matrix of 5 rows and m columns. However,
m≧5. n≧6. Also, F, , F2. ...,
It is assumed that Fm includes at least six independent vectors.
03)式は、CFl + ”2 + ”’ + Fm]
をCFI、CV+。03) The formula is CFL + "2 + "' + Fm]
CFI, CV+.
F2.・・・、vm〕をCVI とおくと、CF)=
(B)〔v〕 ・・・・・・・・・ 04)となる
。従って、
jB:]m=F :] 〔V 〕” ・・・・・・
・・・ α5)となる。但し、
〔V〕*=〔v)T〔〔v〕〔v)T〕−1・・・・・
・・・・(16)である。05)式より、変換行列〔B
〕を求めることができる。F2. ..., vm] as CVI, CF)=
(B) [v] ......04). Therefore, jB:]m=F:] [V]” ・・・・・・
... α5). However, [V]*=[v)T[[v][v)T]-1...
...(16). From formula 05), the transformation matrix [B
] can be found.
(5)変形例。(5) Modification example.
以上の実施例は、姿勢及びワークの異なるセット(例え
ば6個のセット)による方法であったが、他の方法もあ
りうる。第5図に示す如く、z3軸上に重心を持つワー
ク34をセンサ12に取付け、種々の姿勢をとらせる。Although the above embodiments are methods using different postures and different sets of workpieces (for example, six sets), other methods are also possible. As shown in FIG. 5, a workpiece 34 having its center of gravity on the z3 axis is attached to the sensor 12 and is made to take various postures.
姿勢の例を第6図に示す。An example of the posture is shown in FIG.
第6図は、5個の姿勢であり、(a)は下向き、(b)
はx′、軸回りに+451′の傾斜、(C)はx’軸軸
回に−45゜の傾斜、(d)はy′5軸囲軸回+45°
の傾斜、(C)はy’軸軸回に一45°の傾斜を示す。Figure 6 shows five postures, (a) facing downward, (b)
is an inclination of +451' around the x' axis, (C) is an inclination of -45° around the x' axis, (d) is an inclination of +45° around the y'5 axis.
The inclination of (C) shows the inclination of -45° around the y' axis.
いずれも、ベース系の座標軸で考えている。即ち、01
)−x′b−y′、−3′5座標系は、ベース系の対応
するx、y・2軸とxシ。In both cases, we consider the coordinate axes of the base system. That is, 01
)-x'b-y', -3'5 coordinate system is the base system's corresponding x, y, two axes and x-shi.
yb、”b軸との姿勢を同一とし、原点oGがセンサ系
の原点0 と一致略せるような構成の座標系とする。The coordinate system has the same attitude as the yb and b axes, and the origin oG can coincide with the origin 0 of the sensor system.
以上の第6図の5つの姿勢のもとで、それぞれの力’
+ Fb + ”C+ Fd r Fe を測定する
。この5個は独立したベクトルとなる。1つのワークで
は姿勢を父えるだけでは最大5個の独立したベクトルし
か取れないが、本方式では、6個の独立したベクトルを
必要とする。そこで第7図に示すように、ワーク34の
代りに、z3軸上に重心のないワーク35を力センサ1
2に取付ける。次に、z3軸囲りのモーメントが零でな
い工うな姿勢をとらせ ゛る。この姿勢で6個目の独立
したベクトルであるする(但し、m=6)。Under the five postures shown in Figure 6 above, each force'
+ Fb + "C+ Fd r Fe. These five vectors are independent vectors. For one workpiece, only a maximum of five independent vectors can be obtained just by determining the posture, but with this method, six independent vectors can be obtained. Therefore, as shown in FIG.
Attach to 2. Next, have them assume a posture in which the moment around the z-3 axis is not zero. In this attitude, it is assumed that the vector is the 6th independent vector (however, m=6).
そこで、03)式にFa−Ffを代入し、対応する歪ゲ
ージの電圧v、 、 Vb、 、・、 v(を”l *
F2 r ”’vmに代入すれば、05)式より〔B
〕を得ることができる。Therefore, by substituting Fa-Ff into equation 03), the voltage of the corresponding strain gauge v, , Vb, , ·, v( is expressed as "l *
By substituting F2 r ”'vm, we get [B
] can be obtained.
(6) 他の変形例。(6) Other variations.
前述の例は一例であり、ワークの種類やワークの数及び
姿勢の種類や姿勢の敬は、最低6個の独立したFを含ん
でいるとの条件芒え満たせば、どの様に選んでもかまわ
ない。従って、〔B〕 を算出する時の条件、例えば
(イ)ワークのSaの変更を少なくしたい(ロ)ワーク
の姿勢はできるだけ下向き姿勢に近くしたい
(・′)梢1隻の良い〔B〕を得たい
等の各要求に応じて適切な組合せを選べばよい。The above example is just an example, and the types of workpieces, the number of workpieces, the types of postures, and the postures may be selected in any way as long as the condition that they contain at least 6 independent F's is satisfied. do not have. Therefore, the conditions when calculating [B] are, for example, (a) the change in Sa of the workpiece should be minimized (b) the posture of the workpiece should be as close to the downward position as possible (・') a good [B] of one treetop. An appropriate combination can be selected according to each request such as what one wants to obtain.
また、姿勢を説明する便宜上、O′、−x′、−y′5
−z′。Also, for convenience of explaining the posture, O', -x', -y'5
−z′.
座標系を定義したが、必要に応じて他の座標系であって
もよい。Although a coordinate system has been defined, other coordinate systems may be used as necessary.
本発明によれば、変換行列を専用装置を使用することな
(o+yット自身を利用して検出できることとなった。According to the present invention, the transformation matrix can be detected using o+yt itself without using a dedicated device.
算出時間、労力の低下を生むこととなった。This resulted in a reduction in calculation time and labor.
第1図は従来例図、第2図は本発明の実施例図、第3図
は力センサの構成側図、第4図は標準ワークを取り付け
た場合の図、第5図は他の標準ワークを取り付けた場合
の図、第6図は測定モードを示す図、第7図は他の測定
モードを示す図である。
10・・・ロゲットのベース部、11・・・7−ム部、
12・・・力センサ、13・・・ハント部。
代理人 弁理士 秋 本 正 実
第1図
第2図
第3囚
第4図
第5図
第6図
2ら
↑
第7図Figure 1 is a diagram of a conventional example, Figure 2 is a diagram of an embodiment of the present invention, Figure 3 is a side view of the structure of the force sensor, Figure 4 is a diagram of a standard workpiece attached, and Figure 5 is a diagram of another standard workpiece. FIG. 6 is a diagram showing a case where a workpiece is attached, FIG. 6 is a diagram showing a measurement mode, and FIG. 7 is a diagram showing another measurement mode. 10... Base part of loggett, 11... 7-m part,
12...force sensor, 13...hunt part. Agent Patent Attorney Tadashi Akimoto Figure 1 Figure 2 Figure 3 Prisoner Figure 4 Figure 6 Figure 6 2 et al.↑ Figure 7
Claims (1)
ンサであって、該センサがハンド部に印加する力@F@
に感応し、@F@=〔B〕@V@(但し、〔B〕は変換
行列)なる関係の歪電圧@V@を発生する特性とする時
の変換行列〔B〕を検出する検出方法において、 ロボットアームの先端部に装着した力センサの先端に重
さ、重心位置の既知の種々の標準ワークを次々に取付け
、この標準ワークの取付けのもとでの力センサの歪電圧
@V@N及び力・トルクより成る力@F@を求め、該得
られた@V@と@F@とから変換行列〔B〕を検出して
なる力センサの変換行列検出方法。 2、ロボットアームとハンド部との間に装着される力セ
ンサであって、該センサがハンド部に印加する力@F@
に感応し、@F@=〔B〕@V@(但し、〔B〕は変換
行列)なる関係の歪電圧@V@を発生する特性とする時
の変換行列〔B〕を検出する検出方法において、 ロボットアームの先端部に装着した力センサの先端に少
くとも2個の標準ワークをそれぞれ取付けると共に該標
準ワークの姿勢を次々に変化させての力センサの歪電圧
@V@、及び力・トルクより成る力@F@を求め、該得
られた@V@と@F@とから変換行列〔B〕を検出して
なる力センサの変換行列検出方法。[Claims] 1. A force sensor installed between a robot arm and a hand section, which sensor applies a force @F@ to the hand section.
A detection method for detecting the transformation matrix [B] when the characteristic is to generate a distortion voltage @V@ with the relationship @F@ = [B] @V@ (where [B] is a transformation matrix). In this process, various standard workpieces with known weights and center of gravity positions are successively attached to the tip of the force sensor attached to the tip of the robot arm, and the strain voltage of the force sensor @V@ with the standard workpieces attached is A method for detecting a transformation matrix of a force sensor, in which a force @F@ consisting of N and force/torque is determined, and a transformation matrix [B] is detected from the obtained @V@ and @F@. 2. A force sensor installed between the robot arm and the hand section, which measures the force @F@ that the sensor applies to the hand section.
A detection method for detecting the transformation matrix [B] when the characteristic is to generate a distortion voltage @V@ with the relationship @F@ = [B] @V@ (where [B] is a transformation matrix). At least two standard workpieces are attached to the tip of a force sensor attached to the tip of a robot arm, and the postures of the standard workpieces are successively changed to measure the strain voltage @V@ of the force sensor and the force A method for detecting a transformation matrix for a force sensor, in which a force @F@ consisting of torque is determined, and a transformation matrix [B] is detected from the obtained @V@ and @F@.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59210435A JPS6190895A (en) | 1984-10-09 | 1984-10-09 | Force sensor transformation matrix detection method |
| US06/784,502 US4620436A (en) | 1984-10-09 | 1985-10-04 | Method and apparatus for calibrating transformation matrix of force sensor |
| KR1019850007359A KR890000736B1 (en) | 1984-10-07 | 1985-10-07 | Method and apparatus for calibrating transformation matrix of force sensor |
| DE8585112676T DE3573473D1 (en) | 1984-10-09 | 1985-10-07 | Method for calibrating transformation matrix of a force sensor |
| EP85112676A EP0177919B1 (en) | 1984-10-09 | 1985-10-07 | Method for calibrating transformation matrix of a force sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59210435A JPS6190895A (en) | 1984-10-09 | 1984-10-09 | Force sensor transformation matrix detection method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6190895A true JPS6190895A (en) | 1986-05-09 |
Family
ID=16589277
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59210435A Pending JPS6190895A (en) | 1984-10-07 | 1984-10-09 | Force sensor transformation matrix detection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6190895A (en) |
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009522017A (en) * | 2005-12-30 | 2009-06-11 | インテュイティブ サージカル インコーポレイテッド | Modular force sensor |
| JP2013160669A (en) * | 2012-02-07 | 2013-08-19 | Seiko Epson Corp | Sensor device, sensor module, force detector, and robot |
| JP2014041038A (en) * | 2012-08-22 | 2014-03-06 | Seiko Epson Corp | Sensor device, sensor module, force detector, and robot |
| JP2014074587A (en) * | 2012-10-02 | 2014-04-24 | Nissho Denki Kk | Multi-component force measurement method |
| JP2018077248A (en) * | 2018-01-10 | 2018-05-17 | セイコーエプソン株式会社 | Sensor device, sensor module, force detection device and robot |
| JP2022134578A (en) * | 2021-03-03 | 2022-09-15 | 凸版印刷株式会社 | Triaxial load measurement system, triaxial load measurement method, and program |
| JP2022168639A (en) * | 2021-04-26 | 2022-11-08 | 株式会社トライフォース・マネジメント | Calibration method of force sensor |
| US11571264B2 (en) | 2007-12-18 | 2023-02-07 | Intuitive Surgical Operations, Inc. | Force sensor temperature compensation |
| US11650111B2 (en) | 2007-12-18 | 2023-05-16 | Intuitive Surgical Operations, Inc. | Ribbed force sensor |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57136133A (en) * | 1981-02-18 | 1982-08-23 | Hitachi Ltd | Calibrating method for component detector |
-
1984
- 1984-10-09 JP JP59210435A patent/JPS6190895A/en active Pending
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57136133A (en) * | 1981-02-18 | 1982-08-23 | Hitachi Ltd | Calibrating method for component detector |
Cited By (12)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009522017A (en) * | 2005-12-30 | 2009-06-11 | インテュイティブ サージカル インコーポレイテッド | Modular force sensor |
| JP2012157744A (en) * | 2005-12-30 | 2012-08-23 | Intuitive Surgical Inc | Modular force sensor |
| US11571264B2 (en) | 2007-12-18 | 2023-02-07 | Intuitive Surgical Operations, Inc. | Force sensor temperature compensation |
| US11650111B2 (en) | 2007-12-18 | 2023-05-16 | Intuitive Surgical Operations, Inc. | Ribbed force sensor |
| JP2013160669A (en) * | 2012-02-07 | 2013-08-19 | Seiko Epson Corp | Sensor device, sensor module, force detector, and robot |
| JP2014041038A (en) * | 2012-08-22 | 2014-03-06 | Seiko Epson Corp | Sensor device, sensor module, force detector, and robot |
| US9410856B2 (en) | 2012-08-22 | 2016-08-09 | Seiko Epson Corporation | Sensor device, sensor module, force detection device, and robot |
| US9677953B2 (en) | 2012-08-22 | 2017-06-13 | Seiko Epson Corporation | Sensor device, sensor module, force detection device, and robot |
| JP2014074587A (en) * | 2012-10-02 | 2014-04-24 | Nissho Denki Kk | Multi-component force measurement method |
| JP2018077248A (en) * | 2018-01-10 | 2018-05-17 | セイコーエプソン株式会社 | Sensor device, sensor module, force detection device and robot |
| JP2022134578A (en) * | 2021-03-03 | 2022-09-15 | 凸版印刷株式会社 | Triaxial load measurement system, triaxial load measurement method, and program |
| JP2022168639A (en) * | 2021-04-26 | 2022-11-08 | 株式会社トライフォース・マネジメント | Calibration method of force sensor |
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