JPS60162920A - Resolver device using magnetism sensing element - Google Patents

Resolver device using magnetism sensing element

Info

Publication number
JPS60162920A
JPS60162920A JP1874084A JP1874084A JPS60162920A JP S60162920 A JPS60162920 A JP S60162920A JP 1874084 A JP1874084 A JP 1874084A JP 1874084 A JP1874084 A JP 1874084A JP S60162920 A JPS60162920 A JP S60162920A
Authority
JP
Japan
Prior art keywords
signal
magnetically sensitive
function generator
sensing elements
magnetism sensing
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
JP1874084A
Other languages
Japanese (ja)
Inventor
Seishi Miyazaki
清史 宮崎
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.)
Nidec Sankyo Corp
Original Assignee
Nidec Sankyo 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 Nidec Sankyo Corp filed Critical Nidec Sankyo Corp
Priority to JP1874084A priority Critical patent/JPS60162920A/en
Publication of JPS60162920A publication Critical patent/JPS60162920A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D1/00Measuring arrangements giving results other than momentary value of variable, of general application
    • G01D1/16Measuring arrangements giving results other than momentary value of variable, of general application giving a value which is a function of two or more values, e.g. product or ratio

Abstract

PURPOSE:To drive a resolver device efficiently with a little electric power by providing a magnet rotor, two magnetism sensing elements, and a function generator which sends out a sin and a cos signal, and processing respective output signals by a multiplier and an adder. CONSTITUTION:Two magnetism sensing elements 21 and 22 are arranged at an interval of an electric angle pi/2 or its odd multiple in a magnetic field established by the magnet roller 23 magnetized to 2n (n; integer more than 1) in the circumferential direction of rotation, and they are driven by the common DC power source 24. The function generator 28, on the other hand, generates the sin signal and cos signal which have a phase difference of the electric angle pi/2, those output signals and output signals of the magnetism sensing elements 21 and 22 are multiplied by two sets of multipliers 25 and 26 respectively, and their outputs are added together by an operational amplifier 27 which constitutes an adding circuit. Thus, precise detection is attained.

Description

【発明の詳細な説明】 本発明は、磁気感応素子を用いたレゾルバ−装置に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a resolver device using a magnetically sensitive element.

従来、回転角度を検出する手段の一つであるレゾルバ−
装置の例として第1図及び第2図に示されているような
方式のものが知られている。
Conventionally, resolvers are one of the means of detecting rotation angles.
As an example of the apparatus, the system shown in FIGS. 1 and 2 is known.

第1図において、符号1.2はステータコイルであって
、これらステータコイル1.2は互いに90’隔てて配
置されており、一方のステータコイル1にはcos信号
発生器6からcosωtなる信号がアンプ4を介して加
えられ、他方のステータコイル2にはsin信号発生器
7からsinωtなる信号がアンプ5を介して加えられ
るようになっている。また、ロータ8がわにはロータコ
イル3が設けられており、ロータコイル3から出力信号
を得るようになっている。上記二つのステータコイル1
.2に加えられるCO8信号及びsin信号は電気的に
90°の位相差を有している。ロータコイル3からは、
ロータの位置が絶対零点よりθ°だけ移相された2次出
力波形が得られ、これによりロータ8の回転角度を検出
することができる。
In FIG. 1, reference numeral 1.2 denotes a stator coil, these stator coils 1.2 are arranged 90' apart from each other, and one stator coil 1 receives a signal cosωt from a cos signal generator 6. A signal sinωt is applied to the other stator coil 2 from a sin signal generator 7 via an amplifier 5. Further, a rotor coil 3 is provided beside the rotor 8, and an output signal is obtained from the rotor coil 3. Above two stator coils 1
.. The CO8 signal and the sine signal that are applied to the signal line 2 have an electrical phase difference of 90°. From rotor coil 3,
A secondary output waveform in which the rotor position is phase-shifted by θ° from the absolute zero point is obtained, and thereby the rotation angle of the rotor 8 can be detected.

第2図の例は、検出コイルを用いることなく磁気感応素
子を用いたものであって、回転円周方向に着磁されたマ
グネットロータ13の磁界内に二つの磁気感応素子11
.12を電気角でπ/2隔てて配置し、一方の磁気感応
素子11にはCQ3信号発生器14からcosωtなる
信号を、他方の磁気感応素子12にはsin信号発生器
15からsinωtなる信号をそれぞれ加え、互いに直
列に接続された磁気感応素子11.12の出力端からロ
ータの回転角度に応じた信号を取り出すようになってい
る。
The example shown in FIG. 2 uses magnetic sensing elements without using a detection coil, and two magnetic sensing elements 11 are placed in the magnetic field of a magnet rotor 13 magnetized in the circumferential direction of rotation.
.. 12 are arranged at an electrical angle of π/2 apart, one magnetically sensitive element 11 receives a signal cosωt from a CQ3 signal generator 14, and the other magnetically sensitive element 12 receives a signal sinωt from a sine signal generator 15. In addition, a signal corresponding to the rotation angle of the rotor is extracted from the output ends of magnetically sensitive elements 11 and 12 connected in series with each other.

上記何れの従来例にせよ、cos信号発生器及びsin
信号発生器によって発生させたcos信号及びsin信
号をコイル又は磁気感応素子に通電させるものであるた
めに比較的大きな電力が必要であると共に、アンプが必
要である。また、コイル又は磁気感応素子を比較的高い
周波数(10Kllz乃至50Kllz程度)で駆動す
るため、駆動回路からステータまでの長さを長くすると
、波形が歪んだり周波数特性を持ったりして効率の良い
駆動を行うことが難しく、また、外部ノイズが乗り易い
という問題点もあった。
In any of the above conventional examples, the cos signal generator and the sin
Since the cosine signal and the sine signal generated by the signal generator are used to energize a coil or a magnetically sensitive element, a relatively large amount of power is required, and an amplifier is also required. In addition, since the coil or magnetic sensing element is driven at a relatively high frequency (approximately 10Kllz to 50Kllz), if the length from the drive circuit to the stator is increased, the waveform may be distorted or have frequency characteristics, making it difficult to drive efficiently. There was also the problem that it was difficult to carry out this process, and external noise was easily picked up.

本発明の目的は、磁気感応素子を用いたレゾルバ−装置
において、磁気感応素子をcos信号等で直接駆動する
必要がなく、検出した信号を回路内部のみで演算処理す
ることを可能にすることにより、僅かな電力で足り、効
率良く駆動することが可能であり、かつ、外部ノイズの
影響を受け難い磁気感応素子を用いたレゾルバ−装置を
提供することにある。
An object of the present invention is to provide a resolver device using a magnetically sensitive element by eliminating the need to directly drive the magnetically sensitive element with a cosine signal or the like, and by making it possible to perform arithmetic processing on the detected signal only within the circuit. Another object of the present invention is to provide a resolver device using a magnetically sensitive element that requires only a small amount of electric power, can be driven efficiently, and is not easily affected by external noise.

本発明の特徴は、2n(nは1以上の整数)極に着磁さ
れたマグネットロータと、このマグネットロータによっ
て生ずる磁界内に電気角π/2またはその奇数倍隔てて
配置した2個の磁気感応素子と、電気角π/2の位相差
を有するsin信号及びcos信号を発生する関数発生
器と、この関数発生器の各出力信号と上記2個の磁気感
応素子の各出力信号とをそれぞれ乗算する2組の乗算器
と、この乗算器の各出力信号を加算する加算器とを具備
することにある。
The present invention is characterized by a magnet rotor magnetized to 2n (n is an integer greater than or equal to 1) poles, and two magnets arranged at an electrical angle of π/2 or an odd multiple thereof in the magnetic field generated by the magnet rotor. a sensing element, a function generator that generates a sine signal and a cosine signal having a phase difference of electrical angle π/2, and each output signal of this function generator and each output signal of the two magnetic sensing elements, respectively. The present invention is provided with two sets of multipliers for multiplication and an adder for adding the respective output signals of the multipliers.

以下、第3図に示された実施例を参照しながら本発明を
説明する。
The invention will now be described with reference to the embodiment shown in FIG.

第3図において、符号23はマグネットロータであって
、同マグネットロータ23は回転円周方向に2n(nは
1以上の整数)極に着磁されている。ロータマグネット
23によって生ずる磁界内には2個の磁気感応素子21
.22が電気角でπ/2またはその奇数倍隔てて配置さ
れており、各磁気感応素子21.22は共通の磁気感応
素子駆動用直流電源24によって駆動されるようになっ
ている。上記各磁気感応素子21.22はロータマグネ
ット23の位相を検出するものであって、ロータマグネ
ット23の回転に伴い一方の磁気感応素子にはcosθ
の信号が、他方の磁気感応素子にはsinθの信号が発
生するようになっている。磁気感応素子21の出力は乗
算器25に入力され、他方の磁気感応素子22の出力は
乗算器26に入力されるようになっている。乗算器25
は、磁気感応素子21からの信号と関数発生器28によ
って作られたcosωを信号とを乗算し、また乗算器2
6は、磁気感応素子22からの信号と関数発生器28に
よって作られたsinωを信号とを乗算するようになっ
ている。関数発生器28によって作られるcosωを信
号とsinωを信号は数K11zから数十K II z
の周波数になっており、また、上記双方の信号は電気角
でπ/2の位相差を有している。各乗算器25.26の
出力は演算増幅器27を含む加算器=5− 路によって加算され、この加算信号が検出信号として出
力されるようになっている。
In FIG. 3, reference numeral 23 denotes a magnet rotor, and the magnet rotor 23 is magnetized to have 2n (n is an integer greater than or equal to 1) poles in the rotational circumferential direction. Two magnetically sensitive elements 21 are located within the magnetic field generated by the rotor magnet 23.
.. 22 are arranged at electrical angles of π/2 or an odd multiple thereof, and each magnetically sensitive element 21, 22 is driven by a common DC power source 24 for driving the magnetically sensitive element. Each of the magnetic sensing elements 21 and 22 detects the phase of the rotor magnet 23, and as the rotor magnet 23 rotates, one of the magnetic sensing elements 21 and 22 has cosθ.
A signal of sin θ is generated in the other magnetic sensing element. The output of the magnetically sensitive element 21 is input to a multiplier 25, and the output of the other magnetically sensitive element 22 is inputted to a multiplier 26. Multiplier 25
multiplies the signal from the magnetically sensitive element 21 and the signal by cosω generated by the function generator 28, and also multiplies the signal from the multiplier 2
6 multiplies the signal from the magnetically sensitive element 22 and the signal by sin ω generated by the function generator 28 . The cos ω signal and sin ω signal generated by the function generator 28 range from several K11z to several tens of K II z
Furthermore, both of the above signals have a phase difference of π/2 in electrical angle. The outputs of each multiplier 25 and 26 are added by a 5-way adder including an operational amplifier 27, and this added signal is output as a detection signal.

いま、磁気感応素子21にはcosθの信号が、他方の
磁気感応素子22にはsinθの信号が発生したとする
。上記cosθの信号は乗算器25において関数発生器
28からのcosωtの信号と乗算され、一方、上記s
inθの信号は乗算器26において関数発生器28から
のsinωもの信号と乗算される。各乗算器25.26
における乗算結果は演算増幅器27を含む加算器で加算
され、その結果が検出信号Foutとして出力される。
Now, suppose that a cos θ signal is generated in the magnetically sensitive element 21, and a sin θ signal is generated in the other magnetically sensitive element 22. The above cos θ signal is multiplied by the cos ωt signal from the function generator 28 in the multiplier 25, while the above s
The in θ signal is multiplied by a sin ω signal from a function generator 28 in a multiplier 26 . Each multiplier 25.26
The multiplication results in are added by an adder including an operational amplifier 27, and the result is output as a detection signal Fout.

以上の演算動作を式で示すと、Fout= cosωt
 −cosθ+sinωtψsinθ−工(cos (
ωt−θ) + cos (ωを一θ))+工(cos
 (ωを一θ)−cos(ωt+θ))= cos (
ωを一θ) となる。上記の式から明らかなように、出力Fontは
マグネットロータ23の回動角θで位相変調された出力
となり、これによりレゾルバ−動作が行われることにな
る。
Expressing the above calculation operation in a formula, Fout= cosωt
−cosθ+sinωtψsinθ− 工(cos (
ωt-θ) + cos (ω to one θ)) + k (cos
(ω minus θ) − cos (ωt + θ)) = cos (
ω is one θ). As is clear from the above equation, the output Font is an output phase-modulated by the rotation angle θ of the magnet rotor 23, and thereby a resolver operation is performed.

なお、出力信号Fon tは、関数発生器28からの6
− cosωを信号を基準としてθ°だけずれた信号である
から、例えば上記ずれ角θ°内に存在するクロックパル
スをカウントすることにより絶対角度θを表すデジタル
出力を得ることができる。またマグネットロータの回転
数を検出する場合には、位相検出器によりθの変化を検
出し、その変化周波数を読み取ることにより回転数を算
出することができる。
Note that the output signal Font_t is 6 from the function generator 28.
- Since the signal is shifted by θ° with cosω as the reference signal, a digital output representing the absolute angle θ can be obtained, for example, by counting the clock pulses existing within the deviation angle θ°. Furthermore, when detecting the rotational speed of the magnet rotor, the rotational speed can be calculated by detecting a change in θ using a phase detector and reading the frequency of the change.

磁気感応素子としては、ホール素子や磁気抵抗素子(M
R素子)を利用することができる。
As a magnetic sensing element, a Hall element and a magnetoresistive element (M
R element) can be used.

本発明によれば、次のような効果がある。According to the present invention, there are the following effects.

(1)高い精度を必要とするcos信号及びsin信号
で磁気感応素子を駆動する必要がないから、位置検出信
号の周波数特性は磁気感応素子のみの周波数特性で決ま
り、精度の良い検出を行うことができる。
(1) Since it is not necessary to drive the magnetically sensitive element with cosine and sine signals that require high precision, the frequency characteristics of the position detection signal are determined by the frequency characteristics of the magnetically sensitive element alone, allowing highly accurate detection. I can do it.

(2)比較的大きな電流を駆動するアンプを必要としな
い。
(2) There is no need for an amplifier that drives a relatively large current.

(3)駆動回路部分と磁気感応素子との間には高い周波
数の駆動電流は流れないから、駆動回路と磁気感応素子
とを繋ぐ線が長くても検出信号が干渉されることがなく
、また、外部ノイズが乗ることもない。
(3) Since no high-frequency drive current flows between the drive circuit and the magnetically sensitive element, the detection signal will not be interfered with even if the wire connecting the drive circuit and the magnetically sensitive element is long. , there is no external noise.

(4)磁気感応素子を除く他の回路部分は、関数発生器
、乗算器、加算器でなる演算回路であり、磁気感応素子
の駆動回路部分がないから、消費電力が少なくなると共
に、IC化する場合は、駆動用ピンのない小さいチップ
のICを得ることができる。
(4) The other circuit parts except the magnetically sensitive element are arithmetic circuits consisting of a function generator, multiplier, and adder, and there is no drive circuit part for the magnetically sensitive element, so power consumption is reduced and it can be integrated into an IC. In this case, a small chip IC without drive pins can be obtained.

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

第1図は従来のレゾルバ−装置の一例を示す回路図、第
2図は従来のレゾルバ−装置の別の例を示す回路図、第
3図は本発明の実施例を示す回路図である。 21.22・・磁気感応素子 23・・マグネットロー
タ 25.26・・乗算器 27・・加算回路を構成す
る演算増幅器 28・・関数発生器 11
FIG. 1 is a circuit diagram showing an example of a conventional resolver device, FIG. 2 is a circuit diagram showing another example of the conventional resolver device, and FIG. 3 is a circuit diagram showing an embodiment of the present invention. 21.22... Magnetic sensing element 23... Magnet rotor 25.26... Multiplier 27... Operational amplifier constituting the adding circuit 28... Function generator 11

Claims (1)

【特許請求の範囲】[Claims] 2n(nは1以上の整数)極に着磁されたマグネットロ
ータと、このマグネットロータによって生ずる磁界内に
電気角π/2またはその奇数倍隔てて配置した2個の磁
気感応素子と、電気角π/2の位相差を有するsin信
号及びcos信号を発生する関数発生器と、この関数発
生器の各出力信号と上記2個の磁気感応素子の各出力信
号とをそれぞれ乗算する2組の乗算器と、この乗算器の
各出力信号を加算する加算器とを具備することを特徴と
する磁気感応素子を用いたレゾルバ−装置。
A magnet rotor magnetized to 2n (n is an integer greater than or equal to 1) poles, two magnetic sensing elements arranged in the magnetic field generated by the magnet rotor with an electrical angle of π/2 or an odd multiple thereof, and an electrical angle of π/2 or an odd multiple thereof. A function generator that generates a sine signal and a cosine signal having a phase difference of π/2, and two sets of multipliers that multiply each output signal of this function generator and each output signal of the two magnetically sensitive elements, respectively. 1. A resolver device using a magnetically sensitive element, characterized in that it comprises a multiplier and an adder for adding up each output signal of the multiplier.
JP1874084A 1984-02-03 1984-02-03 Resolver device using magnetism sensing element Pending JPS60162920A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1874084A JPS60162920A (en) 1984-02-03 1984-02-03 Resolver device using magnetism sensing element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1874084A JPS60162920A (en) 1984-02-03 1984-02-03 Resolver device using magnetism sensing element

Publications (1)

Publication Number Publication Date
JPS60162920A true JPS60162920A (en) 1985-08-24

Family

ID=11980059

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1874084A Pending JPS60162920A (en) 1984-02-03 1984-02-03 Resolver device using magnetism sensing element

Country Status (1)

Country Link
JP (1) JPS60162920A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6276607U (en) * 1985-10-31 1987-05-16
JPS62242817A (en) * 1986-04-15 1987-10-23 Sanyo Denki Co Ltd Resolver using pulse encoder
JPS631921A (en) * 1986-06-23 1988-01-06 Tamagawa Seiki Co Ltd Angle converter
US7098653B2 (en) * 2001-12-07 2006-08-29 Stoneridge Control Devices, Inc. Phase angle determining circuit
JP2008267907A (en) * 2007-04-18 2008-11-06 Ihi Corp Device and method for measuring rotational balance of high-speed rotor
JP2010022150A (en) * 2008-07-11 2010-01-28 Toshiba Corp Microcomputer, motor control system, and method for converting resolver signal into digital signal

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6276607U (en) * 1985-10-31 1987-05-16
JPS62242817A (en) * 1986-04-15 1987-10-23 Sanyo Denki Co Ltd Resolver using pulse encoder
JPS631921A (en) * 1986-06-23 1988-01-06 Tamagawa Seiki Co Ltd Angle converter
US7098653B2 (en) * 2001-12-07 2006-08-29 Stoneridge Control Devices, Inc. Phase angle determining circuit
JP2008267907A (en) * 2007-04-18 2008-11-06 Ihi Corp Device and method for measuring rotational balance of high-speed rotor
JP2010022150A (en) * 2008-07-11 2010-01-28 Toshiba Corp Microcomputer, motor control system, and method for converting resolver signal into digital signal

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