JPH0641889B2 - Torque detector - Google Patents
Torque detectorInfo
- Publication number
- JPH0641889B2 JPH0641889B2 JP60086759A JP8675985A JPH0641889B2 JP H0641889 B2 JPH0641889 B2 JP H0641889B2 JP 60086759 A JP60086759 A JP 60086759A JP 8675985 A JP8675985 A JP 8675985A JP H0641889 B2 JPH0641889 B2 JP H0641889B2
- Authority
- JP
- Japan
- Prior art keywords
- torque
- temperature
- magnetic layer
- detection
- magnetic
- 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.)
- Expired - Lifetime
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L3/00—Measuring torque, work, mechanical power, or mechanical efficiency, in general
- G01L3/02—Rotary-transmission dynamometers
- G01L3/04—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft
- G01L3/10—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating
- G01L3/101—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating involving magnetic or electromagnetic means
- G01L3/102—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating involving magnetic or electromagnetic means involving magnetostrictive means
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L3/00—Measuring torque, work, mechanical power, or mechanical efficiency, in general
- G01L3/02—Rotary-transmission dynamometers
- G01L3/04—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft
- G01L3/10—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating
- G01L3/101—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating involving magnetic or electromagnetic means
- G01L3/105—Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating involving magnetic or electromagnetic means involving inductive means
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Power Steering Mechanism (AREA)
- Force Measurement Appropriate To Specific Purposes (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は磁歪式トルク検出装置に係わり,特に温度変
化の激しい環境下でも高精度のトルク検出を行ない得る
ようにしたトルク検出装置に関するものである。Description: TECHNICAL FIELD The present invention relates to a magnetostrictive torque detection device, and more particularly to a torque detection device capable of performing highly accurate torque detection even in an environment where the temperature changes drastically. is there.
トルクは回転駆動系の制御を行なう場合の基本量であ
り、回転駆動系ではその検出は非接触であることが望ま
しい。最近,アモルフアス金属の磁気ひずみ特性を利用
し,直接非接触でトルクを検出するトルク検出装置が提
案されている。この従来のトルク検出装置を第3図,第
4図,第5図に従つて説明する。一般に磁性材に応力を
加えるとその磁気特性が変化することは知られており,
例えば,アモルフアス金属では引張応力によつて透磁率
は増加し,圧縮応力によつて透磁率は減少する。ところ
で第3図に示すように受動軸(1)にトルクTを印加する
と,中心軸(2)に対し±45゜方向に応力±σが生じる。
つまり中心軸(2)に対し+45゜の角度をもつ線上に引張
応力σが発生し,−45゜の角度をもつ線上に圧縮応力−
σが生じる。従つて受動軸(1)の外周に高磁歪材からな
る磁性層を固着し,トルクが加わつたときの磁気ひずみ
効果を利用すればトルクの検出が可能となる。第4図は
この原理を利用した従来のトルク検出装置の構造図であ
る。(3a),(3b)は細長い形状の磁性材(例えばアモルフ
アス金属)からなる磁性層であり,互いに中心軸(2)に
対して対称の角度をなすよう受動軸(1)の表面に固着さ
れている。図では応力感度が最も大きい±45゜方向の場
合を示している。(4)はこの磁性層(3a),(3b)に対向す
る位置に,かつ受動軸(1)と所定のギヤツプを隔てて設
けられたコイルボビン,(5),(6)はこのコイルボビンに
巻回された検出コイルであり,トルク印加時に生じる上
記磁性層(3a),(3b)の透磁率変化をインダクタンス変化
として電気信号に変換する。第5図は従来のトルク検出
装置の電気回路図の一例である。(7a)は上記磁性層(3
a),(3b)をそれぞれ磁心とした検出コイル(5),(6)をコ
レクタ巻線として構成したプツシユプル型自励発振回路
であり,トランジスタ(71a),(72a),抵抗(73a),(74
a),コンデンサ(75a),(76a)により構成されている。こ
こでトランジスタ(71a),(72a)の導通時間は,磁心の透
磁率が変化すると,コレクタ巻線のインダクタンスが変
化するために,その透磁率の変化に応じて変化する。従
つてそのデユーテイ比は,検出コイル(5),(6)の磁心と
なる各磁性層(3a),(3b)の透磁率の相対的な変化によつ
て変わる。The torque is a basic amount for controlling the rotary drive system, and it is desirable that the torque is detected in the rotary drive system in a non-contact manner. Recently, there has been proposed a torque detection device that directly utilizes non-contact torque detection by utilizing the magnetostrictive characteristics of amorphous metal. This conventional torque detecting device will be described with reference to FIGS. 3, 4, and 5. It is generally known that the magnetic properties of magnetic materials change when stress is applied,
For example, in an amorphous metal, the tensile stress increases the magnetic permeability, and the compressive stress decreases the magnetic permeability. By the way, as shown in FIG. 3, when torque T is applied to the passive shaft (1), stress ± σ is generated in the direction of ± 45 ° with respect to the central shaft (2).
In other words, tensile stress σ is generated on the line with an angle of + 45 ° with respect to the central axis (2), and compressive stress − on the line with an angle of −45 °.
σ occurs. Therefore, the torque can be detected by fixing the magnetic layer made of high magnetostrictive material on the outer circumference of the passive shaft (1) and utilizing the magnetostrictive effect when the torque is applied. FIG. 4 is a structural diagram of a conventional torque detecting device using this principle. (3a) and (3b) are magnetic layers made of elongated magnetic material (for example, amorphous metal), which are fixed to the surface of the passive shaft (1) so as to form symmetric angles with respect to the central axis (2). ing. The figure shows the case where the stress sensitivity is the maximum ± 45 °. (4) is a coil bobbin provided at a position facing the magnetic layers (3a) and (3b) and separated from the passive shaft (1) by a predetermined gear, and (5) and (6) are wound around this coil bobbin. The rotated detection coil converts the change in magnetic permeability of the magnetic layers (3a) and (3b) that occurs when torque is applied into an electric signal as a change in inductance. FIG. 5 is an example of an electric circuit diagram of a conventional torque detection device. (7a) is the magnetic layer (3
This is a push-pull type self-excited oscillation circuit in which detection coils (5) and (6) with a) and (3b) as magnetic cores are used as collector windings, and transistors (71a), (72a), resistors (73a), (74
a), capacitors (75a) and (76a). Here, the conduction time of the transistors (71a), (72a) changes according to the change of the magnetic permeability because the inductance of the collector winding changes when the magnetic permeability of the magnetic core changes. Therefore, the duty ratio changes depending on the relative change in the magnetic permeability of the magnetic layers (3a) and (3b) that are the magnetic cores of the detection coils (5) and (6).
(8a)は上記発振回路(7a)の各コレクタ信号を矩形波に整
形する波形整形回路であり,抵抗(81a),(82a),(83
a),(84a),オペアンプ(85a),(86a)により構成され
る。(9a)は波形整形された各矩形波信号をデユーテイ比
に対応した直流レベルにする積分回路であり,抵抗(91
a),(92a),コンデンサ(93a),(94a)により構成され
る。(10a)は差動増幅回路であり,抵抗(101a),(102
a),(103a),(104a),オペアンプ(105a)により構成され
る。なお第5図中のVccは回路駆動用の駆動電源であ
る。さて,第5図においてトルクが印加されていない時
には,上記2つの磁性層(3a),(3b)の透磁率は等しいの
で,発振回路(7a)の各コレクタ信号はデユーテイ比50
%の信号となり,差動増幅回路(10a)に入力力される2
つの上記積分された直流レベルは等しく,従つて出力は
零となる。トルクが印加されると,上記のようにトルク
量に比例して一方の磁性層の透磁率が大きく,他方が小
さくなるので,上記発振回路(7a)のコレクタ信号のデユ
ーテイ比が変化し(一方のコレクタ信号のデユーテイ比
は50%より大,他方は50%より小となる),差動増
幅器(10a)の出力には,トルク量に比例したレベルの信
号があらわれる。またトルクの印加方向が変われば,上
記磁性層(3a),(3b)の透磁率が前とは逆に変化するの
で,差動増幅器(10a)の出力には符号が反対の出力信号
が得られ,トルク印加方向も判別することができる。Reference numeral (8a) is a waveform shaping circuit for shaping each collector signal of the oscillation circuit (7a) into a rectangular wave, and resistors (81a), (82a), (83
a), (84a), operational amplifier (85a), (86a). (9a) is an integrator circuit that sets each rectangular wave signal whose waveform is shaped to a DC level corresponding to the duty ratio.
It consists of a), (92a), capacitors (93a), and (94a). (10a) is a differential amplifier circuit, which includes resistors (101a), (102a)
It is composed of a), (103a), (104a), and operational amplifier (105a). Note that Vcc in FIG. 5 is a drive power supply for driving the circuit. Now, in FIG. 5, when no torque is applied, since the magnetic permeability of the two magnetic layers (3a) and (3b) is equal, each collector signal of the oscillator circuit (7a) has a duty ratio of 50.
% Signal, which is input to the differential amplifier circuit (10a) 2
The two integrated DC levels are equal, and therefore the output is zero. When torque is applied, the magnetic permeability of one magnetic layer increases and the other decreases in proportion to the amount of torque as described above, so the duty ratio of the collector signal of the oscillator circuit (7a) changes (one The duty ratio of the collector signal is larger than 50% and the other is smaller than 50%), and a signal having a level proportional to the torque amount appears in the output of the differential amplifier (10a). If the direction of torque application changes, the magnetic permeability of the magnetic layers (3a) and (3b) changes in the opposite direction to the previous one, so the output signal of the differential amplifier (10a) has the opposite sign. The torque application direction can also be determined.
〔発明が解決しようとする問題点〕 しかし上記従来装置では,周囲温度が変化した場合に
は,受動軸(1)と磁性層(3a),(3b)の熱膨張係数が等し
い理想的な場合を除いては,トルクによる応力以外に受
動軸と磁性層の熱膨張係数の差によつてバイアス的な引
張り,又は圧縮応力が加わることになり,これが温度に
よつて変化する。トルク出力は上記したように,2つの
磁性層部の透磁率変化を差動で検出しているので,熱膨
張係数の差によるバイアス応力の変化は2つの磁性層部
で同様に加わるので零点の変動はひきおこさないが,バ
イアス応力量の変動となり,応力−透磁率変化感度が変
わり,トルク出力感度が変化するという問題点があつ
た。これを補正する手段としては,トルク検出装置の近
傍にサーミスタなどの温度センサを配設して周囲温度を
検出し,それによつてトルク出力を補正する方法が考え
られる。しかしこの方法では,周囲温度変化と磁性層の
固着された受動軸の温度変化との間に時間遅れ等が生じ
たりして,かならずしも一致せず,適正な補正ができな
いという問題がある。[Problems to be Solved by the Invention] However, in the above-mentioned conventional device, when the ambient temperature changes, in the ideal case where the passive shaft (1) and the magnetic layers (3a) and (3b) have the same thermal expansion coefficient. In addition to the stress due to torque, bias-like tensile or compressive stress is applied due to the difference in thermal expansion coefficient between the passive shaft and the magnetic layer, which changes with temperature. As described above, since the torque output differentially detects the change in the magnetic permeability of the two magnetic layer portions, the change in the bias stress due to the difference in the coefficient of thermal expansion is similarly applied to the two magnetic layer portions, so that the zero point Although it does not fluctuate, it causes a change in the amount of bias stress, changes the sensitivity of stress-permeability change, and changes the torque output sensitivity. As a means for correcting this, a method of arranging a temperature sensor such as a thermistor near the torque detection device to detect the ambient temperature and correcting the torque output accordingly can be considered. However, in this method, there is a problem that a time delay or the like occurs between the ambient temperature change and the temperature change of the passive shaft to which the magnetic layer is fixed, so that they do not always match and proper correction cannot be performed.
この発明は上記のような問題を解決するためになされた
ものであり,周囲温度が変化した場合にも正確なトルク
出力が得られるトルク検出装置を得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 obtain a torque detection device that can obtain an accurate torque output even when the ambient temperature changes.
この発明に係るトルク検出装置は,受動軸に軸の温度検
出用の磁性層を固着して,非接触で軸の温度を検出する
とともに,上記検出された温度信号によつて,温度に応
じてトルク信号を補正するようにしたものである。The torque detecting device according to the present invention has a magnetic layer for detecting the temperature of the shaft fixed to the passive shaft to detect the temperature of the shaft in a non-contact manner, and according to the detected temperature signal, the temperature is detected according to the temperature. The torque signal is corrected.
この発明における受動軸の温度検出部は,ほぼトルク検
出部と同様の構成をとるが,軸に固着する温度検出用の
磁性層は,トルクに対しては感応しないように十分細長
い形状にして軸長手方向に平行に固着し,この温度検出
部の信号によつて温度補正信号を導出し,トルク出力感
度のゲインを温度に応じて調整する。The temperature detecting portion of the passive shaft according to the present invention has substantially the same structure as the torque detecting portion, but the magnetic layer for temperature detection fixed to the shaft has a sufficiently elongated shape so as not to be sensitive to torque. It is fixed in parallel with the longitudinal direction, a temperature correction signal is derived from the signal of this temperature detection unit, and the gain of the torque output sensitivity is adjusted according to the temperature.
以下,この発明の一実施例を図について説明する。第1
図はこの発明の一実施例を示す構造図,第2図はその電
気回路路図であり,上記第3図,第4図,第5図と同一
または相当部分には同一符号を付している。第1図にお
いて,(11)は受動軸(1)の温度検出用の磁性層であり,
細長い形状をしており,軸(1)の中心軸(2)の方向に平行
に固着されている。材質としては,トルク検出部に使用
した磁性材と同様のものが望ましいが、特にそれに限定
されるものではない。(12)はこの磁性層(11)に対向する
位置のコイルボビン(13)に巻回された温度検出用のコイ
ルであり,(14)は上記磁性層(11)をはずれた位置のコイ
ルボビン(13)に巻回された温度検出用のコイルである。An embodiment of the present invention will be described below with reference to the drawings. First
FIG. 1 is a structural view showing an embodiment of the present invention, FIG. 2 is an electric circuit diagram thereof, and the same or corresponding parts as in FIG. 3, FIG. 4 and FIG. There is. In FIG. 1, (11) is a magnetic layer for detecting the temperature of the passive shaft (1),
It has an elongated shape and is fixed parallel to the direction of the central axis (2) of the axis (1). The material is preferably the same as the magnetic material used for the torque detection unit, but is not particularly limited thereto. (12) is a coil for temperature detection wound around a coil bobbin (13) facing the magnetic layer (11), and (14) is a coil bobbin (13) located off the magnetic layer (11). ) Is a coil for temperature detection which is wound around.
第2図において,(7b)は温度検出用の磁性層(11)を磁心
とした検出コイル(12)と磁性層(11)をはずして配設され
た検出コイル(14)をコレクタ巻線として構成したプツシ
ユプル型自励発振回路であり,上記トルク検出部の発振
回路と同様トランジスタ(71b),(72b),抵抗(73b),(74
b),コンデンサ(75b),(76b)により構成されている。(8
b),(9b),(10b)は上記トルク検出部と同様のそれぞれ
波形整形回路,積分回路,差動増幅回路であり,これら
により,軸(1)の温度検出部が構成される。(15)は加算
回路,(16)は除算回路であり,ゲインコントロールを行
なう。In FIG. 2, (7b) is a detection coil (12) having a magnetic layer (11) for temperature detection as a magnetic core and a detection coil (14) arranged without the magnetic layer (11) as a collector winding. This is a push-pull type self-excited oscillating circuit configured, and transistors (71b), (72b), resistors (73b), (74
b), capacitors (75b) and (76b). (8
Reference numerals b), (9b), and (10b) denote a waveform shaping circuit, an integrating circuit, and a differential amplifier circuit, respectively, which are similar to the torque detecting unit, and these constitute a temperature detecting unit for the shaft (1). (15) is an adder circuit, and (16) is a divider circuit for gain control.
さて周囲温度が変化すると,それに応じて受動軸(1)の
温度も変化し,受動軸(1)に固着された磁性層(11)は,
軸材との熱膨張係数の違いによつて温度変化に比例した
応力を受けてその透磁率が変化する。この磁性層(11)に
近接して検出コイル(12)が巻回されているので,この検
出コイル(12)は温度変化に対応してそのインダクタンス
が変化する。一方,検出コイル(14)は磁性層(11)をはず
して巻回されているので,温度が変化してもそのインダ
クタンスは変らない。従つて,温度が変化した場合には
一方の検出コイルのインダクタンスのみ変化することに
なるので,上記プツシユプル発振回路(7b)の発振信号の
デユーテイ比が変化し,軸(1)の温度に対応した出力信
号Vb=k×ΔTが得られる(ただし,k:材料,回路な
どによる定数,ΔT:基準温度からの温度変化量)。こ
の温度信号Vbは加算回路(15)によつて温度補正信号Vd=
(1+ΔT)kに変換され,除算回路(16)からなるゲイ
ンコントロール回路に入力される。一方,温度補正され
ないトルク信号Vaは,基準温度からの温度変化量をΔ
T,基準温度時のトルク信号をVTとするとVa=(1+△
T)VTとあらわされ,これが除算回路(16)のもう一つの
入力となる。従つて,除算回路(16)の出力は となり,温度に依存しない出力信号が得られる。いうま
でもなく温度検出用の磁性層(11)は,十分細長い形状で
軸長手方向に平行に固着されるので,トルクによる±45
゜方向の応力に対してはほとんど感応せず,温度変化に
よつて生ずる軸長手方向の応力による信号のみが得られ
るものである。When the ambient temperature changes, the temperature of the passive shaft (1) also changes accordingly, and the magnetic layer (11) fixed to the passive shaft (1) becomes
Due to the difference in the coefficient of thermal expansion with the shaft material, the magnetic permeability changes due to the stress proportional to the temperature change. Since the detection coil (12) is wound close to the magnetic layer (11), the inductance of the detection coil (12) changes according to the temperature change. On the other hand, since the detection coil (14) is wound without the magnetic layer (11), its inductance does not change even if the temperature changes. Therefore, when the temperature changes, only the inductance of one of the detection coils changes, so the duty ratio of the oscillation signal of the push-pull oscillator circuit (7b) changes and the temperature of the axis (1) is changed. An output signal V b = k × ΔT is obtained (where k is a constant due to the material and circuit, ΔT is the amount of temperature change from the reference temperature). This temperature signal V b is converted by the adder circuit (15) into a temperature correction signal V d =
It is converted into (1 + ΔT) k and input to the gain control circuit composed of the division circuit (16). On the other hand, the torque signal V a that is not temperature-corrected is the amount of temperature change from the reference temperature Δ
If the torque signal at T and the reference temperature is V T , then V a = (1 + △
T) V T , which is the other input of the division circuit (16). Therefore, the output of the division circuit (16) is And an output signal independent of temperature is obtained. Needless to say, the magnetic layer (11) for temperature detection has a sufficiently elongated shape and is fixed in parallel with the longitudinal direction of the shaft.
It is almost insensitive to the stress in the ° direction, and only the signal due to the stress in the longitudinal direction of the shaft generated by the temperature change is obtained.
なお,上記実施例では検出コイル(14)は磁性層(11)部を
はずした軸外周に巻回したが,温度に感応しない磁心を
用いていればどこに配設してもよく,例えば受動軸(1)
上でなく,回路基板上に設けてもよい。また,上記実施
例ではトルク検出部,温度検出部とも,トルク検出,温
度検出はプツシユプル発振回路を用いたデユーテイ比変
化を検出する方法をとつているが,励磁コイル,検出コ
イルを用いて透磁率変化を検出する方式とすることもで
きる。Although the detection coil (14) is wound around the outer circumference of the shaft without the magnetic layer (11) in the above embodiment, it may be arranged anywhere if a magnetic core insensitive to temperature is used. (1)
It may be provided on the circuit board instead of above. Further, in the above-described embodiment, both the torque detection unit and the temperature detection unit adopt the method of detecting the duty ratio change using the push-pull oscillation circuit for the torque detection and the temperature detection, but the magnetic permeability is determined by using the exciting coil and the detecting coil. It is also possible to adopt a method of detecting a change.
以上のようにこの発明によれば,受動軸上に固着した磁
性材によつて軸温度が非接触で検出でき,この信号によ
つて温度補正をするので,周囲温度変化にかかわらず正
確なトルク信号を得ることができる。As described above, according to the present invention, since the shaft temperature can be detected in a non-contact manner by the magnetic material fixed on the passive shaft and the temperature is corrected by this signal, the accurate torque can be obtained regardless of the ambient temperature change. You can get a signal.
第1図はこの発明の一実施例によるトルク検出装置を示
す構造図であり,第2図はその電気回路図,第3図はト
ルク検出の原理を説明するための図,第4図は従来のト
ルク検出装置を示す構造図であり,第5図はその電気回
路図である。 図において,(1)は受動軸,(3a),(3b)はトルク検出用
の磁性層,(5),(6)はトルク検出用コイル,(7a)はトル
ク検出用のプツシユプル発振回路,(7b)は軸温度検出用
のプツシユプル発振回路,(8a),(8b)は波形整形回路,
(9a),(9b)は積分回路,(10a),(10b)は差動増幅回路,
(11)は軸温度検出用の磁性層,(12),(14)は軸温度検出
用コイル,(15)は加算回路,(16)は除算回路である。 なお,各図中同一符号は同一または相当部分を示す。FIG. 1 is a structural diagram showing a torque detection device according to an embodiment of the present invention, FIG. 2 is an electric circuit diagram thereof, FIG. 3 is a diagram for explaining the principle of torque detection, and FIG. FIG. 5 is a structural diagram showing the torque detection device of FIG. 5, and FIG. 5 is an electric circuit diagram thereof. In the figure, (1) is a passive shaft, (3a) and (3b) are magnetic layers for torque detection, (5) and (6) are coils for torque detection, (7a) is a push-pull oscillation circuit for torque detection, (7b) is a push-pull oscillator for shaft temperature detection, (8a), (8b) is a waveform shaping circuit,
(9a) and (9b) are integration circuits, (10a) and (10b) are differential amplification circuits,
(11) is a magnetic layer for detecting the shaft temperature, (12) and (14) are coils for detecting the shaft temperature, (15) is an adding circuit, and (16) is a dividing circuit. The same reference numerals in each figure indicate the same or corresponding parts.
Claims (1)
着し,該受動軸へのトルク印加時に生じる上記磁性層の
透磁率変化をこの磁性層の外周に巻回した検出コイルに
よつて検出してトルク信号を検出するトルク検出装置に
おいて,上記受動軸上に,かつ受動軸の中心軸に平行に
固着された細長い磁性層と,この磁性層の外周に巻回さ
れた検出コイルとにより構成された,上記受動軸の温度
に応じた信号を出力する受動軸温度検出回路を備え,こ
の検出回路の出力信号により上記トルク信号を補正する
ことを特徴とするトルク検出装置。1. A detection coil having a magnetic layer fixed to the outer circumference of a passive shaft that receives a torque, and a change in magnetic permeability of the magnetic layer caused when torque is applied to the passive shaft is detected by a detection coil wound around the outer circumference of the magnetic layer. In a torque detection device for detecting a torque signal by detecting, a slender magnetic layer fixed on the passive shaft and parallel to the central axis of the passive shaft, and a detection coil wound around the outer circumference of the magnetic layer. A torque detection device comprising a passive shaft temperature detection circuit configured to output a signal according to the temperature of the passive shaft, and correcting the torque signal by an output signal of the detection circuit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60086759A JPH0641889B2 (en) | 1985-04-23 | 1985-04-23 | Torque detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60086759A JPH0641889B2 (en) | 1985-04-23 | 1985-04-23 | Torque detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61245033A JPS61245033A (en) | 1986-10-31 |
| JPH0641889B2 true JPH0641889B2 (en) | 1994-06-01 |
Family
ID=13895671
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60086759A Expired - Lifetime JPH0641889B2 (en) | 1985-04-23 | 1985-04-23 | Torque detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0641889B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2009107751A1 (en) * | 2008-02-28 | 2009-09-03 | 本田技研工業株式会社 | Magneto-strictive torque sensor, method for manufacturing the same, and electric power steering device |
Families Citing this family (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63101838U (en) * | 1986-12-22 | 1988-07-02 | ||
| JPH0754273B2 (en) * | 1987-12-26 | 1995-06-07 | 大同特殊鋼株式会社 | Torxense |
| EP0480912A3 (en) * | 1987-12-28 | 1992-07-01 | Kubota Ltd. | Torque measuring device |
| JPH07117463B2 (en) * | 1987-12-28 | 1995-12-18 | 株式会社クボタ | Torque measuring device |
| JPH0227539U (en) * | 1988-08-12 | 1990-02-22 | ||
| JPH02136726A (en) * | 1988-11-17 | 1990-05-25 | Kubota Ltd | torque measuring device |
| JP2661728B2 (en) * | 1988-11-17 | 1997-10-08 | 株式会社クボタ | Torque measuring device |
| US5137128A (en) * | 1990-06-20 | 1992-08-11 | Mitsubishi Denki K.K. | Magnetic particle type electromagnetic clutch with torque detector |
| SE9102121D0 (en) * | 1991-07-08 | 1991-07-08 | Skf Nova Ab | SENSOR SYSTEM |
| JP4886264B2 (en) * | 2005-10-05 | 2012-02-29 | 本田技研工業株式会社 | Magnetostrictive torque sensor and electric power steering device using the same |
| CN108519180A (en) * | 2018-03-31 | 2018-09-11 | 天津大学 | A Torque Measurement Method Based on Electroplated Nickel Elastic Shaft |
-
1985
- 1985-04-23 JP JP60086759A patent/JPH0641889B2/en not_active Expired - Lifetime
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2009107751A1 (en) * | 2008-02-28 | 2009-09-03 | 本田技研工業株式会社 | Magneto-strictive torque sensor, method for manufacturing the same, and electric power steering device |
| JP2009204533A (en) * | 2008-02-28 | 2009-09-10 | Honda Motor Co Ltd | Magnetostrictive torque sensor, its manufacturing method, and electric power steering device |
| GB2470152A (en) * | 2008-02-28 | 2010-11-10 | Honda Motor Co Ltd | Magneto-strictive torque sensor, method for manufacturing the same, and electric power steering device |
| GB2470152B (en) * | 2008-02-28 | 2011-12-28 | Honda Motor Co Ltd | Magnetostrictive torque sensor and manufacturing method thereof, and electric power steering system |
| US8181538B2 (en) | 2008-02-28 | 2012-05-22 | Honda Motor Co., Ltd. | Magnestostrictive torque sensor and manufacturing method thereof, and electric power steering system |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61245033A (en) | 1986-10-31 |
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