JPH0266407A - Control circuit for magnetic resolver - Google Patents

Control circuit for magnetic resolver

Info

Publication number
JPH0266407A
JPH0266407A JP21889288A JP21889288A JPH0266407A JP H0266407 A JPH0266407 A JP H0266407A JP 21889288 A JP21889288 A JP 21889288A JP 21889288 A JP21889288 A JP 21889288A JP H0266407 A JPH0266407 A JP H0266407A
Authority
JP
Japan
Prior art keywords
signal
phase
period
stator
magnetic resolver
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
JP21889288A
Other languages
Japanese (ja)
Other versions
JPH0643901B2 (en
Inventor
Yutaka Ono
裕 小野
Yoichi Kikukawa
要一 菊川
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa 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 Yokogawa Electric Corp filed Critical Yokogawa Electric Corp
Priority to JP21889288A priority Critical patent/JPH0643901B2/en
Publication of JPH0266407A publication Critical patent/JPH0266407A/en
Publication of JPH0643901B2 publication Critical patent/JPH0643901B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To omit an R/D converter and to obtain an inexpensive detector by executing operation by means of an operational amplifier and a phase difference counter to detect a rotational angle. CONSTITUTION:The frequency of a clock from a clock generator 10 is divided by a frequency divider 11, supplied to the coils 9081, 9082 of a resolver 900 as a sine wave through an LPF 11 and then supplied to coils 9091, 9092 as a cosine wave through a phase adjusting means 14. Respective differences between the coils 9081, 9082 and between the coils 9091, 9092 are added by an adder 19 and a phase having the same phase as an excited sine wave is subtracted from the added value by the adder 19 through a phase adjusting means 16 to obtain a sine wave whose phase is shifted from the excited sine wave by the rotational angle of the resolver. The phase difference is measured by a phase difference counter 23 through comparator 21, 22 to use it as a commutation control signal and the period of an output from the comparator 22 is measured by a period counter 24 to calculate a rotating position.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は磁気レゾルバのインタフェイス(以下、1/F
とする)となる磁気レゾルバの制御回路に関するもので
ある。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magnetic resolver interface (hereinafter referred to as 1/F
The present invention relates to a control circuit for a magnetic resolver.

[従来の技術] 従来の磁気レゾルバのI/Fとしては、R/Dコンバー
タ(レゾルバ/デジタル コンバータ)がある。
[Prior Art] An example of a conventional magnetic resolver I/F is an R/D converter (resolver/digital converter).

「発明が解決しようとする課題] しかし、R/Dコンバータは複雑なアナログICとデジ
タルICが混載されているため、非常に高価になるとい
う問題点かある0例えば、R/Dコンバータは1ビツト
あたり約3000円かかるため、12ビツトのR/Dコ
ンバータを構成するには36000円もかかることにな
る。
``Problem to be solved by the invention'' However, since the R/D converter is a combination of complex analog IC and digital IC, there is a problem that it becomes very expensive. For example, the R/D converter has a 1-bit Since it costs about 3,000 yen per unit, it will cost 36,000 yen to construct a 12-bit R/D converter.

本発明はこのような問題点を解決するためになされたも
のであり、低コストで磁気レゾルバのインタフェイスを
構成できる磁気レゾルバの制御回路を実現することを目
的とする。
The present invention has been made to solve these problems, and an object of the present invention is to realize a magnetic resolver control circuit that can configure a magnetic resolver interface at low cost.

[課題を解決するための手段] 本発明は、 ロータとステータにパルスモータと同様な歯を有し、ス
テータの各突極にはコイルが巻かれた磁気レゾルバと、 前記ステータの一部の突極に巻かれたコイルを正弦波の
交流電圧で励磁する信号源と、この正弦波の交流電圧の
振幅と位相を調整して余弦波の交流電圧を生成するとと
もに前記突極間の取り付け位置の誤差を電気的に除去し
、生成した余弦波の交流電圧で前記ステータの他の突極
に巻かれたコイルを励磁する第1の調整手段と、正弦波
で励磁されたコイルに流れる電流に比例した電圧どうし
と余弦波で励磁されたコイルに流れる電流に比例した電
圧どうしを減算する減算手段と、 前記正弦波の交流電圧の振幅と位相を調整する第2の調
整手段と、 前記減算手段でとった減算信号どうしを加算して前記ロ
ータの回転角で位相が変調される検出信号を算出し、こ
の検出信号に前記第2の調整手段で調整した信号を加算
して検出信号を補正する加算手段と、 補正後の検出信号と前記信号源の発生信号の位相差をと
って前記磁気レゾルバの1歯内における回転位置を検出
する位相差カウンタと、前記補正後の検出信号の周期を
計測する周期カウンタと、 この周期カウンタの計測周期と前記信号源の発生信号の
周期の差を一定周期ごとに算出し、この差を積算して磁
気レゾルバの回転位置を算出する位置算出手段、 を具備した磁気レゾルバの制御回路である。
[Means for Solving the Problems] The present invention includes a magnetic resolver having teeth similar to those of a pulse motor on a rotor and a stator, and a coil wound around each salient pole of the stator; A signal source that excites a coil wound around a pole with a sinusoidal alternating voltage; and a signal source that adjusts the amplitude and phase of this sinusoidal alternating voltage to generate a cosine-wave alternating voltage; a first adjusting means for electrically removing the error and exciting a coil wound around the other salient pole of the stator with the generated cosine wave AC voltage; subtracting means for subtracting the voltages proportional to the current flowing through the coil excited by the cosine wave from each other; a second adjusting means for adjusting the amplitude and phase of the sine wave AC voltage; Addition of adding together the obtained subtraction signals to calculate a detection signal whose phase is modulated by the rotation angle of the rotor, and correcting the detection signal by adding the signal adjusted by the second adjustment means to this detection signal. means; a phase difference counter that detects a rotational position within one tooth of the magnetic resolver by taking a phase difference between the corrected detection signal and the signal generated by the signal source; and a phase difference counter that measures the period of the corrected detection signal. A period counter; and a position calculation means for calculating the difference between the measurement period of the period counter and the period of the signal generated by the signal source every fixed period, and calculating the rotational position of the magnetic resolver by integrating the differences. This is a control circuit for a magnetic resolver.

[実施例] 以下、図面を用いて本発明を説明する。[Example] Hereinafter, the present invention will be explained using the drawings.

まず、磁気レゾルバ部分の構成を説明する。First, the configuration of the magnetic resolver section will be explained.

第1図は本発明にかかる制御回路に用いる磁気レゾルバ
の構成例を示した図であり、(a)は正面図、(b)は
<a>図のZl−21部分の断面図である。
FIG. 1 is a diagram showing an example of the configuration of a magnetic resolver used in a control circuit according to the present invention, in which (a) is a front view, and (b) is a sectional view of the Zl-21 portion in Figure <a>.

図で、901,902は磁性体材料で構成された2枚の
円板状のステータ部材である。ステータ部材901と9
02には、90゛の回転角を隔てた位置ごとに突#19
03 〜9034と9041〜9044が形成されてい
る。これらの突極の先端には一定ビッチpbで歯905
が形成されている。
In the figure, 901 and 902 are two disk-shaped stator members made of magnetic material. Stator members 901 and 9
02, there is a protrusion #19 at each position separated by a rotation angle of 90°.
03 to 9034 and 9041 to 9044 are formed. The tips of these salient poles have teeth 905 with a constant pitch pb.
is formed.

同一ステータ部材で、隣り合う突極の歯の位相は(1/
 2 ) p bずつずれている。
In the same stator member, the phase of the teeth of adjacent salient poles is (1/
2) It is shifted by p b.

ステータ部材901と902は非磁性体部材906を挿
入して積み重ねられてステータ907を構成している。
Stator members 901 and 902 are stacked with a non-magnetic member 906 inserted therein to form a stator 907.

このとき、ステータの隣り合う突極の歯の位相が(1/
 4 ) P bだけずれるように積み重ねられている
0例えば、突[!9031と9041の歯の位相は(1
/ 4 ) p bずれている。
At this time, the phase of the teeth of adjacent salient poles of the stator is (1/
4) 0 stacked so that they are shifted by P b For example, [! The phase of teeth 9031 and 9041 is (1
/ 4) p b is off.

9081は突極9031と9033に巻かれたコイル、
9082は突極9032と9034に巻かれたコイルで
ある。コイル9081と9082により、1相のコイル
を構成している。ステータ部材902にも同様にコイル
9091と9092が巻かれている。
9081 is a coil wound around salient poles 9031 and 9033,
9082 is a coil wound around salient poles 9032 and 9034. Coils 9081 and 9082 constitute a one-phase coil. Coils 9091 and 9092 are similarly wound around the stator member 902.

910はステータ部材901,902の外側に配置され
たロータである。ロータ910には、歯905と対向し
ていて、この歯とほぼ同一ピッチの歯911か形成され
ている。
910 is a rotor arranged outside the stator members 901 and 902. Teeth 911 are formed on the rotor 910, facing the teeth 905 and having substantially the same pitch as the teeth.

第2図は本発明にかかる磁気レゾルバの制御回路の一実
施例の構成図である。
FIG. 2 is a configuration diagram of an embodiment of a magnetic resolver control circuit according to the present invention.

図で、900は第1図に示した磁気レゾルバ部分である
In the figure, 900 is the magnetic resolver portion shown in FIG.

10は磁気レゾルバのコイルの駆動信号源となっている
タロツク発生器、11はクロック発生器10の発生タロ
ツクを分周する分周器、12は分周したクロックの低周
波成分を抽出するローパスフィルタ(以下、LPFとす
る)、13は抽出した信号を波形整形するコンパレータ
である。整形された信号はEs1nωtなる交流電圧(
E:電圧の振幅、ω:角速度、t:時間)となってコイ
ル908 と9082を駆動する。
Reference numeral 10 denotes a tarlock generator that serves as a driving signal source for the coil of the magnetic resolver, 11 a frequency divider that divides the frequency of the tarlock generated by the clock generator 10, and 12 a low-pass filter that extracts the low frequency component of the divided clock. (hereinafter referred to as LPF), 13 is a comparator that shapes the waveform of the extracted signal. The shaped signal is an AC voltage (Es1nωt) (
E: amplitude of voltage, ω: angular velocity, t: time) to drive the coils 908 and 9082.

14は位相調整手段であり、交流電圧 Es1nωtの位相を90°ずらして Ecosωtなる交流電圧にするとともに、ステータ部
材901と902(sinコアとcosコア)の取り付
け位置の機械的誤差を電気的に補正する。交流電圧Ec
osωtによりコイル9091と9092が励磁される
14 is a phase adjustment means, which shifts the phase of AC voltage Es1nωt by 90 degrees to make AC voltage Ecosωt, and electrically corrects mechanical errors in the mounting positions of stator members 901 and 902 (sin core and cos core). do. AC voltage Ec
Coils 9091 and 9092 are excited by osωt.

15と16は交流電圧Es1n6Jtの振幅と位相を調
整する振幅調整手段と位相調整手段である。
15 and 16 are amplitude adjusting means and phase adjusting means for adjusting the amplitude and phase of the AC voltage Es1n6Jt.

このような調整により、交流電圧Es1nωtのキャリ
ア成分がキャンセルされる。
By such adjustment, the carrier component of the AC voltage Es1nωt is canceled.

17はコイル908 と9082に流れる電流の差をと
り差に比例した電圧を出力する減算器、18はコイル9
09 と9092に流れる電流の差をとり差に比例した
電圧を出力する減算器である。
17 is a subtractor that calculates the difference between the currents flowing through the coils 908 and 9082 and outputs a voltage proportional to the difference; 18 is the coil 9;
This is a subtracter that takes the difference between the currents flowing through 09 and 9092 and outputs a voltage proportional to the difference.

19は減算器17と18でとった減算値を加え、この加
算信号に位相調整手段16を通過した信号を加算して加
算信号を補正する加算器である。ここで、補正した加算
信号は位相が磁気レゾルバのロータの回転角度θで変調
される信号 Ksin(ωt+θ)であるくに:定数)。
An adder 19 adds the subtracted values obtained by the subtracters 17 and 18, and adds the signal passed through the phase adjustment means 16 to this added signal to correct the added signal. Here, the corrected addition signal is a signal Ksin (ωt+θ) whose phase is modulated by the rotation angle θ of the rotor of the magnetic resolver (constant).

20は加算器19の補正信号の特定周波数成分を取り出
すバンドパスフィルタ(以下、BPFとする)、21.
22は分周器11とBPF20の出力を波形整形するコ
ンパレータである。
20 is a band pass filter (hereinafter referred to as BPF) for extracting a specific frequency component of the correction signal of the adder 19; 21.
22 is a comparator that shapes the waveforms of the outputs of the frequency divider 11 and BPF 20.

23はコンパレータ21と22で整形した信号の位相差
をタロツク発生器10のクロックでカウントする位相差
カウンタである。
A phase difference counter 23 counts the phase difference between the signals shaped by the comparators 21 and 22 using the clock of the tarlock generator 10.

24はコンパレータ22による整形信号の周期をクロッ
ク発生器10のクロックで計測する周期カウンタである
24 is a period counter that measures the period of the shaped signal produced by the comparator 22 using the clock of the clock generator 10.

25は位置算出手段であり、周期カウンタ24で計測し
た周期をもとにロータ910の1回転中の回転位置を算
出する。
A position calculating means 25 calculates the rotational position of the rotor 910 during one rotation based on the period measured by the period counter 24.

このような実施例の動作を説明する。The operation of such an embodiment will be explained.

交流信号Es1nωtとEcosωtの間には相対的な
電気角の誤差が含まれているため、コイル908 .9
08  と909 .9092は交流電圧Es1n(ω
t+ΔA)とEcosωtで駆動される(八〇は電気角
の誤差)。
Since a relative electrical angle error is included between the AC signals Es1nωt and Ecosωt, the coils 908 . 9
08 and 909. 9092 is the AC voltage Es1n(ω
t+ΔA) and Ecosωt (80 is the electrical angle error).

ロータ910がθだけ回転したときは、コイル908 
.908 .909 .9092に流れ1   2  
  す る電流I  、I  、I  、I  は次のとおりに
なる。
When the rotor 910 rotates by θ, the coil 908
.. 908. 909. Flow to 9092 1 2
The currents I , I , I , and I are as follows.

181=1□  (1+mcos (θ+δA))xs
  i  n  (ωt+ΔA )  01g2= I
□  (1mc o s (θ十δA))xsin(ω
t+Δ^) ■ 191=IO(1+ms i nθ)cosωt  ■
192=Io (1−m5 i nθ)cosωt  
■m:定数 ここで、δAはsinコアとCOSコアの取り付け位置
の相対的な機械誤差である。
181=1□ (1+mcos (θ+δA))xs
i n (ωt+ΔA) 01g2=I
□ (1mcos (θ0δA))xsin(ω
t+Δ^) ■ 191=IO(1+ms i nθ) cosωt ■
192=Io (1-m5 inθ)cosωt
■m: constant Here, δA is a relative mechanical error in the mounting positions of the sin core and the COS core.

減算器17.18と加算器19により、■式−■式+■
式−■式の演算を行って次式に示す演算値v1を算出す
る。
By the subtractor 17.18 and the adder 19, ■Formula-■Formula+■
The calculation of equation - (2) is performed to calculate the calculation value v1 shown in the following equation.

含まれたキャリア成分である。It is a carrier component included.

位相調整手段14は、0式の電気角を調整して、Δ^=
δA にすることにより、0式の右辺第2項を0にする。
The phase adjustment means 14 adjusts the electrical angle of the 0 type, so that Δ^=
By setting δA, the second term on the right side of equation 0 is set to 0.

更に、この信号に交流電圧Es1nωを振幅と位相を調
整した信号−esinωtを加算することにより、残留
キャリア成分を打ち消す。
Further, by adding to this signal a signal -esinωt obtained by adjusting the amplitude and phase of the AC voltage Es1nω, the residual carrier component is canceled.

位相差カウンタ23は、キャリア成分を打ち消した信号
θ と励磁信号θ1の位相差をタロツク発生器10の発
生タロツクで計測する。励磁信号θ1の360°の電気
角はロータ910の1歯ピッチ分に相当するため、位相
差カウンタ23で計測した位相差はロータ910の1歯
ピツチ内の回転位置に相当する。計測した位相差をアド
レスポインタとしてs t n(1iが格納されたRO
Mの値を読み出し、読み出しデータにより磁気レゾルバ
が回転を検出しているモータの転流制御を行う。
The phase difference counter 23 measures the phase difference between the carrier component canceled signal θ and the excitation signal θ1 using the tarlock generated by the tarlock generator 10. Since the 360° electrical angle of the excitation signal θ1 corresponds to one tooth pitch of the rotor 910, the phase difference measured by the phase difference counter 23 corresponds to the rotational position within one tooth pitch of the rotor 910. The measured phase difference is used as an address pointer and the RO in which s t n (1i is stored) is
The value of M is read out, and commutation control of the motor whose rotation is detected by the magnetic resolver is performed based on the read data.

周期カウンタ24は、信号θ。の周期をクロック発生器
10の発生クロックで計測する。
The period counter 24 receives a signal θ. The period of is measured using the clock generated by the clock generator 10.

位置算出手段25は、周期カウンタ24の計測周期をも
とに、位相が変調された信号θ。と励磁信号θ1の周期
の差を一定周期ごとにとる。
The position calculation means 25 generates a signal θ whose phase is modulated based on the measurement period of the period counter 24. The difference between the periods of the excitation signal θ1 and the excitation signal θ1 is determined at regular intervals.

ロータ910の回転角θはvtになるため(v:定数)
、変調された信号は Es1n(ω十v)tの形になる。このため、変調され
た信号の周期は回転角θによって変わる。
Since the rotation angle θ of the rotor 910 is vt (v: constant)
, the modulated signal has the form Es1n(ω+v)t. Therefore, the period of the modulated signal changes depending on the rotation angle θ.

従って、変調された信号Es1n(ω+v)tと励磁信
号Es1nωtの周期の差をとって積算するとロータ9
10の1回転中の回転位置が求められる。
Therefore, if the difference in period between the modulated signal Es1n(ω+v)t and the excitation signal Es1nωt is calculated and integrated, the rotor 9
The rotational position of 10 during one rotation is determined.

例えば、励磁信号θ1の1周期の計測カウントに要する
クロツク数が4096、磁気レゾルバのロータの歯数が
124の場合は、位置算出手段25は、次式から回転位
置を算出する。
For example, if the number of clocks required to count one period of the excitation signal θ1 is 4096 and the number of teeth of the rotor of the magnetic resolver is 124, the position calculating means 25 calculates the rotational position from the following equation.

P二Σ (p△丁Aイ − 4oqb)P: 回申艮イ
九士、 しA−′rAi:尤1ト目うJむ月夙基弓この
場合は、ロータが1回転すると、 124x4096=507904 の個数のクロックが検出される。
P2Σ (p△choAi - 4oqb) P: 1st rotation, 124x4096= 507,904 clocks are detected.

[効果] 本発明によれば次の効果が得られる。[effect] According to the present invention, the following effects can be obtained.

■OPアンプを複数個設けた回路構成であるなめ、R/
Dコンバータに比べて低コストになる。
■It has a circuit configuration with multiple OP amplifiers, and R/
Lower cost than D converter.

■信号検出力感が位相変調方式であるため、容易にデジ
タル・′インタフェイスを構成でき、また位置検出と磁
気レゾルバが回転を検出するモータの転流制御も可能に
なる。
■Since the signal detection force sensing is a phase modulation method, it is easy to configure a digital interface, and it also enables position detection and commutation control of the motor whose rotation is detected by the magnetic resolver.

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

第1図は本発明にかかる回路に用い、る磁気レゾルバの
構成例を示した図、第2図は本発明にかかる回路の一実
施例の構成図である。 10・・・クロック発生器、14.16・・・位相調整
手段、15・・・振幅調整手段、17.18・・・減算
器、19・・・加算器、23・・・位相差カウンタ、2
4・・・周期カウンタ、25・・・位置算出手段。
FIG. 1 is a diagram showing a configuration example of a magnetic resolver used in a circuit according to the present invention, and FIG. 2 is a configuration diagram of an embodiment of the circuit according to the present invention. 10... Clock generator, 14.16... Phase adjustment means, 15... Amplitude adjustment means, 17.18... Subtractor, 19... Adder, 23... Phase difference counter, 2
4... Period counter, 25... Position calculation means.

Claims (1)

【特許請求の範囲】 ロータとステータにパルスモータと同様な歯を有し、ス
テータの各突極にはコイルが巻かれた磁気レゾルバと、 前記ステータの一部の突極に巻かれたコイルを正弦波の
交流電圧で励磁する信号源と、 この正弦波の交流電圧の振幅と位相を調整して余弦波の
交流電圧を生成するとともに前記突極間の取り付け位置
の誤差を電気的に除去し、生成した余弦波の交流電圧で
前記ステータの他の突極に巻かれたコイルを励磁する第
1の調整手段と、正弦波で励磁されたコイルに流れる電
流に比例した電圧どうしと余弦波で励磁されたコイルに
流れる電流に比例した電圧どうしを減算する減算手段と
、 前記正弦波の交流電圧の振幅と位相を調整する第2の調
整手段と、 前記減算手段でとつた減算信号どうしを加算して前記ロ
ータの回転角で位相が変調される検出信号を算出し、こ
の検出信号に前記第2の調整手段で調整した信号を加算
して検出信号を補正する加算手段と、 補正後の検出信号と前記信号源の発生信号の位相差をと
って前記磁気レゾルバの1歯内における回転位置を検出
する位相差カウンタと、 前記補正後の検出信号の周期を計測する周期カウンタと
、 この周期カウンタの計測周期と前記信号源の発生信号の
周期の差を一定周期ごとに算出し、この差を積算して磁
気レゾルバの回転位置を算出する位置算出手段、 を具備した磁気レゾルバの制御回路。
[Claims] A magnetic resolver having teeth similar to a pulse motor on a rotor and a stator, a coil wound around each salient pole of the stator, and a coil wound around some of the salient poles of the stator. A signal source is excited by a sinusoidal alternating voltage, and the amplitude and phase of the sinusoidal alternating voltage are adjusted to generate a cosine-wave alternating voltage, and errors in the mounting positions between the salient poles are electrically removed. , a first adjusting means for exciting a coil wound around another salient pole of the stator with the generated cosine wave alternating current voltage; a subtracting means for subtracting voltages proportional to the current flowing through the excited coil; a second adjusting means for adjusting the amplitude and phase of the sine wave AC voltage; and adding the subtracted signals obtained by the subtracting means. adding means for calculating a detection signal whose phase is modulated by the rotation angle of the rotor, and correcting the detection signal by adding the signal adjusted by the second adjustment means to the detection signal; a phase difference counter that detects a rotational position within one tooth of the magnetic resolver by taking a phase difference between a signal and a signal generated by the signal source; a period counter that measures the period of the corrected detection signal; A control circuit for a magnetic resolver, comprising: position calculation means for calculating the difference between the measurement period of the signal and the period of the signal generated by the signal source at regular intervals, and calculating the rotational position of the magnetic resolver by integrating the differences.
JP21889288A 1988-09-01 1988-09-01 Magnetic resolver control circuit Expired - Fee Related JPH0643901B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21889288A JPH0643901B2 (en) 1988-09-01 1988-09-01 Magnetic resolver control circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21889288A JPH0643901B2 (en) 1988-09-01 1988-09-01 Magnetic resolver control circuit

Publications (2)

Publication Number Publication Date
JPH0266407A true JPH0266407A (en) 1990-03-06
JPH0643901B2 JPH0643901B2 (en) 1994-06-08

Family

ID=16726940

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21889288A Expired - Fee Related JPH0643901B2 (en) 1988-09-01 1988-09-01 Magnetic resolver control circuit

Country Status (1)

Country Link
JP (1) JPH0643901B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04127891A (en) * 1990-09-18 1992-04-28 Yokogawa Electric Corp Motor drive system
JP2001114116A (en) * 1999-10-19 2001-04-24 Alps Electric Co Ltd Rotation angle detecting device
JP2017201292A (en) * 2016-04-28 2017-11-09 ルネサスエレクトロニクス株式会社 Control device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04127891A (en) * 1990-09-18 1992-04-28 Yokogawa Electric Corp Motor drive system
JP2001114116A (en) * 1999-10-19 2001-04-24 Alps Electric Co Ltd Rotation angle detecting device
JP2017201292A (en) * 2016-04-28 2017-11-09 ルネサスエレクトロニクス株式会社 Control device

Also Published As

Publication number Publication date
JPH0643901B2 (en) 1994-06-08

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