JPH0357962A - Rotary data detection circuit - Google Patents

Rotary data detection circuit

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Publication number
JPH0357962A
JPH0357962A JP19476789A JP19476789A JPH0357962A JP H0357962 A JPH0357962 A JP H0357962A JP 19476789 A JP19476789 A JP 19476789A JP 19476789 A JP19476789 A JP 19476789A JP H0357962 A JPH0357962 A JP H0357962A
Authority
JP
Japan
Prior art keywords
signal
magnetic field
circuit
field detection
detection signal
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
JP19476789A
Other languages
Japanese (ja)
Other versions
JP2805089B2 (en
Inventor
Yuji Miura
三浦 有二
Yuuichi Nanae
裕一 名苗
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.)
Sony Corp
Original Assignee
Sony Corp
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Filing date
Publication date
Application filed by Sony Corp filed Critical Sony Corp
Priority to JP19476789A priority Critical patent/JP2805089B2/en
Publication of JPH0357962A publication Critical patent/JPH0357962A/en
Application granted granted Critical
Publication of JP2805089B2 publication Critical patent/JP2805089B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To detect the rotary data of a rotary body with high detection accuracy by detecting the non-equilibrium voltage contained in a magnetic field detection signal and changing a reference level corresponding to the detection result. CONSTITUTION:A clamp circuit 15 clamping a magnetic field detection signal SMO10 at the first and second clamp levels VCP1, VCP2 to send out a magnetic field detection clamp signal SMO11, an integration circuit 14 integrating the signal SMO11 to send out the non-equilibrium detection signal SOFF1 corresponding to the non-equilibrium voltage contained in the signal SMO101 and a binarizing circuit 8 comparing the signal SMO10 on the second reference level VREF1 to send out a binarization signal SB10 are provided. The non-equlibrium voltage contained in the signal SMO10 is detected in the circuits 15, 14 and, in the circuit 8, the reference level VREF1 binarizing the signal SMO10 corresponding to the detection result SOFF2 thereof is changed to make it possible to always send out the signal SB10 having desired duty regardless of the presence of the non- equilibrium voltage in the signal SMO10.

Description

【発明の詳細な説明】 A産業上の利用分野 本発明は回転情報検出回路に関し、例えばビデオテーブ
のキャブスタンモー夕の回転速度を検出するものに適用
して好適なものである.B発明の概要 本発明は、回転情報検出回路において、磁界検出信号に
含まれる不平衡電圧を検出すると共に、その検出結果に
応じて磁界検出信号を2値化する基準レベルを変化させ
るようにしたことにより、磁界検出信号中の不平衡電圧
の有無に係わらず、常に所望のデューティを有する2 
{!化信号を得ることができる. C従来の技術 従来、例えばビデオテープレコーダにおいては、キャプ
スタンモータを所望の回転速度で安定に駆動するため、
磁気抵抗素子構威の回転速度検出回路を用いてキャプス
タンモータの回転速度を検出し、この検出結果に基づい
てサーボループを形戒するキャプスタンサーボ回路が用
いられている.すなわち、第4図に示すように、このキ
ャプスタンサーボ回路1においては、キャプスタンモー
タ2の回転速度を回転速度検出回路3で検出し、この結
果得られる回転速度検出信号SFを続く周波数電圧変換
回路4に送出する. 周波数電圧変換回路4は、入力される回転速度検出信号
SFに応じた回転速度検出電圧Svを発生し、この回転
速度検出電圧Svをメカニカル制御回路(図示せず)か
ら供給されるキャプスタンモータ制御信号Sl4と共に
加算回路5に入力して加算し、この加算信号SADDで
キャブスタンモータ2を駆動制御することにより、全体
として速度サーボルーブを形威し、かくして、キャプス
タンモータ2を所望の回転速度で安定に駆動し得るよう
になされている。
DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a rotational information detection circuit, and is suitable for application to, for example, a circuit for detecting the rotational speed of a cab stan motor of a video tape. B Summary of the Invention The present invention detects an unbalanced voltage included in a magnetic field detection signal in a rotation information detection circuit, and changes a reference level for binarizing the magnetic field detection signal in accordance with the detection result. By doing so, regardless of the presence or absence of an unbalanced voltage in the magnetic field detection signal, the
{! It is possible to obtain the converted signal. C. Prior Art Conventionally, in a video tape recorder, for example, in order to stably drive a capstan motor at a desired rotational speed,
A capstan servo circuit is used that detects the rotation speed of the capstan motor using a rotation speed detection circuit with a magnetoresistive element structure, and controls the servo loop based on this detection result. That is, as shown in FIG. 4, in this capstan servo circuit 1, the rotation speed of the capstan motor 2 is detected by a rotation speed detection circuit 3, and the rotation speed detection signal SF obtained as a result is subjected to a subsequent frequency-voltage conversion. Send to circuit 4. The frequency-voltage conversion circuit 4 generates a rotational speed detection voltage Sv according to the inputted rotational speed detection signal SF, and uses this rotational speed detection voltage Sv to control a capstan motor supplied from a mechanical control circuit (not shown). By inputting the signal Sl4 to the adding circuit 5 and adding it together, and driving and controlling the cabstan motor 2 with this added signal SADD, a speed servo loop is formed as a whole, and thus the capstan motor 2 is driven at the desired rotation speed. It is designed to be able to drive stably.

ここで回転速度検出回路3は、第5図に示すように、キ
ャプスタンモータ2の回転軸の円周方向に順次磁界方向
が異なる磁石をリング状に300〜400ピツチで着磁
した回転磁石部6、その回転磁石部6に当接して配置さ
れ、磁気抵抗特性がそれぞれ90゜異なる2端子磁気抵
抗素子7A及び7Bを直列に組み合わせてなる磁界検出
部7及びその出力信号5MOを2値化する2 {!化回
路部8から構戒されている. この磁界検出部7の2端子磁気抵抗素子7A及び7Bに
は、電圧値5〔■〕でなるti電圧VCCが印加されて
おり、これによりキャプスタンモータ2が1回転すると
、各磁気抵抗素子7A及び7Bの接続中点aからは、電
圧値2.5(V)を中心?圧とする300〜400周期
分の正弦波状でなる磁界検出信号SN。が送出される. 実際上磁界検出部7から送出される磁界検出信号SN。
Here, as shown in FIG. 5, the rotational speed detection circuit 3 is a rotating magnet section in which magnets with different magnetic field directions are magnetized in a ring shape at 300 to 400 pitches in the circumferential direction of the rotating shaft of the capstan motor 2. 6. Binarize the magnetic field detection unit 7 and its output signal 5MO, which is made up of a series combination of two-terminal magnetoresistive elements 7A and 7B that are placed in contact with the rotating magnet unit 6 and have magnetoresistive characteristics different by 90° from each other. 2 {! It has been warned against by the System Circuit Department 8. A ti voltage VCC having a voltage value of 5 [■] is applied to the two-terminal magnetic resistance elements 7A and 7B of the magnetic field detection unit 7, and when the capstan motor 2 rotates once, each magnetic resistance element 7A And from the connection midpoint a of 7B, the voltage value is centered at 2.5 (V)? The magnetic field detection signal SN has a sinusoidal waveform of 300 to 400 cycles. is sent. A magnetic field detection signal SN actually sent out from the magnetic field detection section 7.

は、演算増幅器構戒でなる2値化回路8Aの非反転入力
端に入力されている. この2値化回路8Aは、反転入力端に電源電圧VCCを
第1及び第2の抵抗R1及びR2で分圧してなる電圧値
2.5 C V )の基準電圧V■,が入力されている
. かくして、この2値化回路8Aからは、正弦波状でなる
磁界検出信号SI4。(第6図(A))を基準電圧V 
IEFに基づいて2値化してなる2値化信号Sl  (
第6図(B))が回転速度検出信号S,として送出され
る。
is input to the non-inverting input terminal of the binarization circuit 8A consisting of an operational amplifier. This binarization circuit 8A has a reference voltage V, which has a voltage value of 2.5 C V ) obtained by dividing the power supply voltage VCC by the first and second resistors R1 and R2, input to the inverting input terminal. .. Thus, the binarization circuit 8A generates a magnetic field detection signal SI4 having a sinusoidal waveform. (Figure 6(A)) as the reference voltage V
Binarized signal Sl (
6(B)) is sent out as the rotational speed detection signal S.

このようにして、このキャプスタンサーボ回路lにおい
ては、例えば回転速度検出信号S,の立上り周期をカウ
ントしたり、その周期によって、キャプスタンモータ2
の回転速度をデイジタル的に検出し得、またこの回転速
度検出信号SFを例えば周波数電圧変換回路4内のロー
バスフィルタを通じて平滑化することにより、回転速度
検出電圧Svを発生し得るようになされている.D発明
が解決しようとする問題点 ところでかかる構戒の回転速度検出回路3の磁界検出部
7においては、各磁気抵抗素子7A及び7Bの製造上の
問題や素子自体の磁気抵抗特性の問題等の点から、所定
範囲内における磁気抵抗特性のばらつきが許容されてい
る. このため、磁界検出部7から出力される磁界検出信号S
.。1には、第7図(A)に示すように、不平衡電圧V
。,Fが生じるおそれがあった.このように、磁界検出
信号SI4。,に不平衡電圧V 6,,が生じると、第
7図(B)に示すように、回転速度検出回路3から送出
される2値化信号S1のデューテイが変化し、回転速度
検出信号SFをローパスフィルタを通じて平滑化して、
回転速度検出電圧Svを発生するキャプスタンサーボ回
路tでは、回転速度検出電圧Svに不平衡電圧V。.に
応じた誤差が生じ、その結果キャブス?ンモータ2の回
転速度を正しく検出できなくなる問題があった。
In this way, in this capstan servo circuit 1, for example, the rising cycle of the rotational speed detection signal S is counted, and the capstan motor 2 is
The rotation speed of the rotation speed detection signal SF is smoothed through a low-pass filter in the frequency-voltage conversion circuit 4, for example, to generate the rotation speed detection voltage Sv. There is. D Problems to be Solved by the Invention By the way, in the magnetic field detection section 7 of the rotational speed detection circuit 3 of this construction, there are problems in manufacturing the respective magnetoresistive elements 7A and 7B, problems in the magnetoresistive characteristics of the elements themselves, etc. From this point, variations in magnetoresistive characteristics within a predetermined range are allowed. Therefore, the magnetic field detection signal S output from the magnetic field detection section 7
.. . 1, as shown in FIG. 7(A), an unbalanced voltage V
. , F could occur. In this way, the magnetic field detection signal SI4. When an unbalanced voltage V 6, , occurs in , as shown in FIG. 7(B), the duty of the binary signal S1 sent from the rotation speed detection circuit 3 changes, causing the rotation speed detection signal SF to change. Smoothed through a low-pass filter,
In the capstan servo circuit t that generates the rotational speed detection voltage Sv, an unbalanced voltage V is applied to the rotational speed detection voltage Sv. .. An error occurs depending on the result, and the result is Cavs? There was a problem that the rotational speed of the motor 2 could not be detected correctly.

また2値化信号S.の立上り周期及び又は立下り周期に
基づいて、キャブスタンモータ2の回転速度をデイジタ
ル的に検出するキャプスタンサーボ回路1では、2値化
信号S■のデューテイが変化すると回転速度の検出精度
が著しく劣化する問題があった。
Also, the binary signal S. In the capstan servo circuit 1, which digitally detects the rotational speed of the cabstan motor 2 based on the rise period and/or fall period of There was a problem with deterioration.

またさらに、磁界検出部7を2端子磁気抵抗素子7A及
び7Bに代え、正弦波状の第1の磁界検出信号Ssoz
  (第8図(A))に加えて、この第1の磁界検出信
号Sl4。2に対して90度位相の異なる余弦波状の第
2の磁界検出信号S..S  (第8図(A))を出力
し得るようになされた4端子磁気抵抗素子を用い、週倍
の周波数でなる回転速度検出信号を得る回転速度検出回
路においても、例えば、第2の磁界検出信号S.4。、
に不平衡電圧VOFFIが生じると、第8図(B)に示
すように、2{lI化信号Soのデューテイが変化し、
この結果、キャプスタンモータ2の回転速度を正しく検
出できなくなる問題があった. このような問題を解決するため、従来磁界検出部7から
送出される磁界検出信号SMOを結合用コンデンサC,
を介して2値化回路8に入力するように構戒し、これに
より不平衡電圧V REFの影響を排除するようになさ
れた回転速度検出回路が提案されている. ところがこのようにすると、キャプスタンモータ2が静
止状態から定常回転状態に立ち上る際には、回転速度が
遅いため磁界検出信号S,4。自体が直流的に変動し、
2値化信号として出力されないという問題があり、解決
策としては未だ不十分であった. 本発明は以上の点を考慮してなされたもので、静止状態
から定常回転状態まで、高い検出情度で回転体の回転情
報を検出し得る回転情報検出回路を提案しようとするも
のである. E問題点を解決するための手段 かかる問題点を解決するため本発明においては、?転体
2の周囲に、回転方向に順次異なる磁界を発生する回転
磁石部6を配置すると共に、回転磁石部6に当接するよ
うに磁界検出部1lを配置し、回転体2の回転に応じて
磁界検出部1lから送出される正弦波状の磁界検出信号
SMO+。を2値化してなる2値化信号S■。に基づい
て回転体2の回転情報を得る回転情報検出回路10にお
いて、磁界検出信号SNOI。を、その磁界検出信号S
8。.の中心レベルの上下に設定した第1及び第2のク
ランプレベルVCPI及びvcptでクランプして磁界
検出クランプ信号3H011を送出するクランプ回路1
5と、磁界検出クランプ信号SNOI1を積分してその
磁界検出クランプ信号SMOIIの平均値を算出し、磁
界検出信号S.。,。に含まれる不平衡電圧v0,■。
Furthermore, the magnetic field detection section 7 is replaced with two-terminal magnetic resistance elements 7A and 7B, and a sinusoidal first magnetic field detection signal Ssoz
In addition to the first magnetic field detection signal Sl4.2 (FIG. 8(A)), a cosine-shaped second magnetic field detection signal S. .. In a rotational speed detection circuit that uses a four-terminal magnetic resistance element capable of outputting S (FIG. 8(A)) and obtains a rotational speed detection signal with a frequency twice as high as a week, for example, the second magnetic field Detection signal S. 4. ,
When an unbalanced voltage VOFFI occurs in , the duty of the 2{lI signal So changes as shown in FIG. 8(B),
As a result, there was a problem that the rotational speed of the capstan motor 2 could not be detected correctly. In order to solve such problems, conventionally, the magnetic field detection signal SMO sent from the magnetic field detection section 7 is connected to a coupling capacitor C,
A rotational speed detection circuit has been proposed in which the unbalanced voltage V REF is inputted to the binarization circuit 8 via the rotation speed detection circuit 8, thereby eliminating the influence of the unbalanced voltage V REF. However, in this case, when the capstan motor 2 rises from a stationary state to a steady rotation state, the rotation speed is slow, so the magnetic field detection signal S,4 is generated. itself fluctuates like a direct current,
There was a problem that the signal was not output as a binary signal, and this was still an insufficient solution. The present invention has been made in consideration of the above points, and aims to propose a rotation information detection circuit that can detect rotation information of a rotating body with high detection sensitivity from a stationary state to a steady rotation state. EMeans for solving the problem In order to solve the problem, the present invention includes: A rotating magnet section 6 that sequentially generates different magnetic fields in the rotational direction is arranged around the rolling body 2, and a magnetic field detection section 1l is arranged so as to come into contact with the rotating magnet section 6. A sinusoidal magnetic field detection signal SMO+ is sent out from the magnetic field detection section 1l. Binarized signal S■ is obtained by binarizing. In the rotation information detection circuit 10 that obtains rotation information of the rotating body 2 based on the magnetic field detection signal SNOI. , its magnetic field detection signal S
8. .. Clamp circuit 1 that clamps at first and second clamp levels VCPI and vcpt set above and below the center level of and sends out a magnetic field detection clamp signal 3H011.
5 and the magnetic field detection clamp signal SNOI1 to calculate the average value of the magnetic field detection clamp signal SMOII. . ,. Unbalanced voltage v0,■ included in.

に応じた不平衡検出信号S。F■(S0,。)を送出す
る積分回路14と、磁界検出信号S.4。1。
unbalance detection signal S according to. An integrating circuit 14 that sends out F■ (S0,.) and a magnetic field detection signal S. 4.1.

を、第1の基準レベル■■,に不平衡検出信号S OF
FIを加えてなる第2の基準レベル■1■で比較して2
値化信号S■。を送出する2値化回路8とを設けるよう
にした。
, the unbalance detection signal S OF is set to the first reference level
Second standard level by adding FI■1■Compared with 2
Valued signal S■. A binarization circuit 8 for transmitting .

?作用 クランプ回路15及び積分回路14において磁界検出信
号SNOI。に含まれる不平衡電圧V。,■。
? The magnetic field detection signal SNOI is applied to the clamping circuit 15 and the integrating circuit 14 . The unbalanced voltage V contained in ,■.

を検出し、また2{直化回路8において、その検出結果
S。,nに応じて磁界検出信号SNI)l。を2値化す
る基準レベルV■■を変化させるようにしたことにより
、磁界検出信号3,401。中の不平衡電圧VOFF+
。の有無に係わらず、常に所望のデューテイを有する2
値化信号S■。を送出し得る。
is detected, and the detection result S is detected in the 2{direction circuit 8. , n, the magnetic field detection signal SNI)l. By changing the reference level V■■ for binarizing the magnetic field detection signal 3,401. unbalanced voltage VOFF+
. 2, which always has the desired duty regardless of the presence or absence of
Valued signal S■. can be sent.

G実施例 以下図面について、本発明の一実施例を詳述する. 第5図との対応部分に同一符号を付して示す第l図にお
いて、10は全体として本発明による回転速度検出回路
を示し、いわゆる4端子磁気抵抗素子構戒でなる磁界検
出部11の第1の出力端11Aから送出される第1の磁
界検出信号SMOI。が、2kl!化回路部8に入力さ
れると共に、不平衡電圧検出回路部12に入力される。
G. Embodiment An embodiment of the present invention will be described in detail below with reference to the drawings. In FIG. 1, in which parts corresponding to those in FIG. The first magnetic field detection signal SMOI is sent out from the output terminal 11A of 1. But, 2kl! The voltage is input to the unbalanced voltage detection circuit section 8 as well as to the unbalanced voltage detection circuit section 12 .

この磁界検出部l1は、第1、第2、第3及び第4の磁
気抵抗素子MRI、MR2、MR3及びMR4をブリッ
ジ接続してなり、キャプスタンモータ2(第4図)の回
転軸に装着した回転磁石部6(第5図)に当接した状態
で、第1及び第3の磁気抵抗素子MHI及びMR3の磁
気抵抗特性に対して、第2及び第4の磁気抵抗素子MR
2及びMR4の磁気抵抗特性が90゜異なるように配置
されている. なお第1及び第4の磁気抵抗素子MHI及びMR4の接
続中点aは、電圧値5〔V〕の電源電圧■CCに接続さ
れ、また第2及び第3の磁気抵抗素子MR2及びMR3
の接続中点Cは接地されている. これにより、第1及び第2の磁気抵抗素子MR1及びM
R2の接続中点bでなる第1の出力端11Aからは、キ
ャプスタンモータ2の1回転分に応して、電圧値2.5
(V)を中心電圧とする300〜400周期分の正弦波
状でなる第1の磁界検出信号SMOI。が送出される. ?たこれに対して、第3及び第4の磁気抵抗素子MR3
及びMR4の接続中点dでなる第2の出力端11Bから
は、第1の磁界検出信号S.。,。に対して90”位相
の異なる余弦波状の第2の磁界検出信号S.4。2。が
送出される。
This magnetic field detection unit l1 is formed by bridge-connecting first, second, third, and fourth magnetoresistive elements MRI, MR2, MR3, and MR4, and is mounted on the rotating shaft of the capstan motor 2 (Fig. 4). With respect to the magnetoresistive characteristics of the first and third magnetoresistive elements MHI and MR3, the second and fourth magnetoresistive elements MR
2 and MR4 are arranged so that their magnetoresistive characteristics differ by 90°. Note that the connection midpoint a of the first and fourth magnetoresistive elements MHI and MR4 is connected to the power supply voltage CC with a voltage value of 5 [V], and the connection point a of the second and third magnetoresistive elements MR2 and MR3 is
The middle point C of the connection is grounded. As a result, the first and second magnetoresistive elements MR1 and M
From the first output terminal 11A formed at the connection midpoint b of R2, a voltage value of 2.5 is generated corresponding to one rotation of the capstan motor 2.
The first magnetic field detection signal SMOI has a sinusoidal waveform of 300 to 400 cycles with (V) as the center voltage. is sent. ? On the other hand, the third and fourth magnetoresistive elements MR3
A first magnetic field detection signal S. . ,. A second magnetic field detection signal S.4.2 in the form of a cosine wave having a phase difference of 90'' with respect to the second magnetic field detection signal S.4.2.

この実施例の場合不平衡電圧検出回路部l2においては
、第1の磁界検出信号S,4。,。が演算増幅器構成の
バッファ回路13に入力され、その出力が抵抗RIOを
通じて、抵抗Rll及びコンデンサCOOでなる積分回
路l4に送出される.ここでこの抵抗RIO及び積分回
路14の抵抗Rllの接続中点eは、クランプ回路15
に接続されている。
In this embodiment, the unbalanced voltage detection circuit section l2 receives the first magnetic field detection signal S,4. ,. is input to a buffer circuit 13 having an operational amplifier configuration, and its output is sent through a resistor RIO to an integrating circuit 14 consisting of a resistor Rll and a capacitor COO. Here, the connection midpoint e of this resistor RIO and the resistor Rll of the integrating circuit 14 is the clamp circuit 15
It is connected to the.

このクランプ回路15は、電源VCC及びアース間を第
1〜第3の抵抗R12、R13及びR14の直列回路で
接続し、第1の抵抗R12と、第2及び第3の抵抗R1
3及びR14とで分圧して得られる第1のクランプ電圧
■。■が、演算増幅器構威のバツファ回路15A及び逆
極性で接続されたダイオードD1を通して接続中点eに
印加され?いる. また第1及び第2の抵抗R12及びR13と、第3の抵
抗R14とで分圧して得られる第2のクランプ電圧vc
ptが、演算増幅器構或のバッファ回路15B及び順極
性で接続されたダイオードD2を通じて接続中点eに印
加されている.なお実際上第1及び第2のクランプ電圧
■,■及びVCPRは、所定範囲内で許容されている磁
気抵抗特性のばらつきから逆算して、磁界検出部l1に
おいて発生する可能性のある不平it圧VOFF+を、
中心電圧として電圧{j! 2.5 (V ) ニ対し
て加算及び減算した電圧値に設定されている.従って、
バツファ回路13より送出される第1の磁界検出信号3
H01。は、第1のクランプ電圧VCPl以下のレベル
及び第2のクランプ電圧vcpt以上のレベルでクラン
プされ、この結果得られる磁界検出クランプ信号S.。
This clamp circuit 15 connects the power supply VCC and the ground with a series circuit of first to third resistors R12, R13, and R14, and includes a first resistor R12 and a second and third resistor R1.
3 and R14 to obtain the first clamp voltage (2). ? is applied to the connection midpoint e through the buffer circuit 15A of the operational amplifier structure and the diode D1 connected with opposite polarity? There is. Further, a second clamp voltage vc obtained by dividing the voltage by the first and second resistors R12 and R13 and the third resistor R14
pt is applied to the connection point e through a buffer circuit 15B having an operational amplifier structure and a diode D2 connected with forward polarity. In fact, the first and second clamp voltages ■, ■ and VCPR are calculated backward from the variations in magnetoresistive characteristics allowed within a predetermined range, and are calculated based on the undesired pressure that may occur in the magnetic field detection section l1. VOFF+,
The voltage {j! 2.5 (V) It is set to the voltage value added and subtracted from 2.5 (V). Therefore,
First magnetic field detection signal 3 sent out from buffer circuit 13
H01. is clamped at a level below the first clamp voltage VCPl and above the second clamp voltage vcpt, and the resulting magnetic field detection clamp signal S. .

.が、積分回路14に人力される. この積分回路14においては、磁界検出クランプ信号S
MOI1を積分して、当該磁界検出クランプ?号S.。
.. is manually input to the integrating circuit 14. In this integrating circuit 14, the magnetic field detection clamp signal S
Integrate MOI1 and select the relevant magnetic field detection clamp? No.S. .

.の平均値を求め、これを第lの不平衡電圧検出信号S
。,■として、演算増幅器構或のレベルシフト回路16
の非反転入力端に送出する.このレベルシフト回路l6
は、抵抗R15によって負帰還されると共に、電源V。
.. and calculate the average value of the lth unbalanced voltage detection signal S
. , ■, a level shift circuit 16 having an operational amplifier structure.
Send it to the non-inverting input terminal of . This level shift circuit l6
is negatively fed back by the resistor R15, and the power supply V.

及びアース間を第1及び第2の抵抗R16及びR17の
直列回路で接続し、この結果得−られる所定のレベルシ
フト電圧V,イが反転入力端に印加されている.これに
より、レベルシフト回路16において所定のレベルにシ
フトされた第2の不平衡電圧検出信号S。2■は、2値
化回路部8の2値化回路8Aの反転入力端に入力され、
このようにして、この2値化回路部8においては第lの
磁界検出信号S8。1。を、電圧値2.5(V)の基準
電圧V虞EFに対して、第2の不平′#電圧検出信号S
。,■を加えた第2の基準電圧V■,1と比較して、2
値化信号S■。を得るようになされている。
and ground are connected by a series circuit of first and second resistors R16 and R17, and a predetermined level shift voltage V,i obtained as a result is applied to the inverting input terminal. As a result, the second unbalanced voltage detection signal S is shifted to a predetermined level in the level shift circuit 16. 2■ is input to the inverting input terminal of the binarization circuit 8A of the binarization circuit section 8,
In this way, in this binarization circuit section 8, the lth magnetic field detection signal S8.1 is generated. , the second complaint '#voltage detection signal S
. ,■ compared with the second reference voltage V■,1, which is 2
Valued signal S■. It is made to obtain.

以上の構成において、例えば第2図(A)に示すように
、磁界検出部11から送出される第1の磁界検出信号S
MOIOに不平衡電圧が存在しない場?には、不平衡電
圧検出部12の積分回路14から送出される第1の不平
衡電圧検出信号S。,■(第2図(B))は0レベルと
なる。
In the above configuration, for example, as shown in FIG. 2(A), the first magnetic field detection signal S sent out from the magnetic field detection section 11
If there is no unbalanced voltage in MOIO? , the first unbalanced voltage detection signal S sent out from the integrating circuit 14 of the unbalanced voltage detection section 12. , ■ (Figure 2 (B)) is at the 0 level.

これにより、2値化回路部8においては、第1の磁界検
出信号Sl.IO+。を電圧値2.5(V)でなる第2
の基準電圧V1■と比較し、この結果、第2図(C)に
示すようにデューテイが50%の2値化信号S■。が送
出される。
As a result, in the binarization circuit unit 8, the first magnetic field detection signal Sl. IO+. The second voltage is 2.5 (V).
The result is a binary signal S■ with a duty of 50%, as shown in FIG. 2(C). is sent.

またこれに対して、例えば第3図(A)に示すように、
磁界検出部11から送出される第1の磁界検出信号Sx
。.に不平衡電圧V。2■。が存在する場合には、積分
回路l4からその不平衡電圧VOF■。に応じた第1の
不平衡電圧検出信号SOFFI。(第3図(B))が送
出される.これにより、2値化回路部8においては、第
1の磁界検出信号S.4。1。を電圧値2.5(V)で
なる基準電圧■■,に対して、第1の不平衡電圧検出信
号S。,■。に応じた電圧値を加えた第2の基準電圧■
■.で比較し、この結果、第3図(C)に示すようにデ
ューテイが50%の2値化信号S■。
In addition, on the other hand, as shown in FIG. 3(A), for example,
The first magnetic field detection signal Sx sent out from the magnetic field detection section 11
. .. unbalanced voltage V. 2■. If there is an unbalanced voltage VOF■ from the integrating circuit l4. A first unbalanced voltage detection signal SOFFI according to the first unbalanced voltage detection signal SOFFI. (Figure 3 (B)) is sent. As a result, in the binarization circuit unit 8, the first magnetic field detection signal S. 4.1. The first unbalanced voltage detection signal S with respect to the reference voltage ■■, which has a voltage value of 2.5 (V). ,■. The second reference voltage with the voltage value added according to ■
■. The result is a binary signal S■ with a duty of 50%, as shown in FIG. 3(C).

?送出される。? Sent out.

このようにして、この実施例による回転速度検出回路1
0の場合、磁界検出部l1から送出される第1の磁界検
出信号SMOI。に不平衡電圧V。,Fが存在する場合
でも、この不平衡電圧■。,,を検出すると共に、検出
された不平衡電圧V OFFに応じた第2の基準電圧■
1■と第1の磁界検出信号S,4。1。を比較して2値
化信号S■。を得るようにしたことにより、不平衡電圧
V。2Fの有無に係わらず、常にデューテイが50%の
2値化信号S■。
In this way, the rotational speed detection circuit 1 according to this embodiment
In the case of 0, the first magnetic field detection signal SMOI is sent out from the magnetic field detection unit l1. unbalanced voltage V. , F, this unbalanced voltage ■. , , and a second reference voltage corresponding to the detected unbalanced voltage V OFF.
1■ and the first magnetic field detection signal S, 4.1. Compare the values to obtain a binary signal S■. By obtaining the unbalanced voltage V. A binary signal S■ whose duty is always 50% regardless of the presence or absence of 2F.

を送出することかできる. なお実際上磁界検出部11から送出される第2の磁界検
出信号SMO!0についても、回転速度検出回路10と
同様に処理すれば、2値化信号S■。
It is possible to send . Note that the second magnetic field detection signal SMO! actually sent out from the magnetic field detection section 11! 0 is also processed in the same manner as in the rotational speed detection circuit 10, resulting in a binary signal S■.

に対して90度位相が遅れ、常にデューテイが50%の
2値化信号を送出することかできる.また、この回転速
度検出回路10の場合、磁界検出部11から送出される
第1の磁界検出信号SN。1。を所定のクランプ電圧■
。■及びVer■でクランプして、不平衡電圧V。7■
。を検出するよ?にしたことにより、静止状態から定常
回転状態に立ち上る過程においても、精度良く不平衡電
圧VOFFI。を検出することができる.以上の構成に
よれば、磁界検出部11から送出される第1の磁界検出
信号S8。,。中の不平衡電圧VOFF+。の有無に係
わらず、常にデューテイが50%の2値化信号S■。を
送出し得、かくして、静止状態から定常回転状態まで、
高い検出精度で回転速度を検出し得る回転速度検出回路
10を実現できる。
It is possible to transmit a binary signal with a 90 degree phase delay and a duty of 50%. Further, in the case of this rotational speed detection circuit 10, the first magnetic field detection signal SN sent out from the magnetic field detection section 11. 1. the given clamp voltage■
. Unbalanced voltage V by clamping at ■ and Ver■. 7■
. Will it detect? As a result, the unbalanced voltage VOFFI can be accurately controlled even in the process of rising from a stationary state to a steady rotation state. can be detected. According to the above configuration, the first magnetic field detection signal S8 is sent out from the magnetic field detection section 11. ,. unbalanced voltage VOFF+ inside. The binary signal S■ always has a duty of 50% regardless of the presence or absence of the signal. Thus, from a stationary state to a steady rotation state,
It is possible to realize the rotational speed detection circuit 10 that can detect rotational speed with high detection accuracy.

なお上述の実施例においては、本発明をビデオテープレ
コーダのキャブスタンモータの回転速度を検出するもの
に適用した場合について述べたが、これに限らず、回転
ドラム駆動モータや磁気ディスク装置のスピンドルモー
タ等、他のモータの回転速度を検出するものにも通用し
得、さらにモータに限らず、歯車やベルト等を介してモ
ータから回転駆動されるもの等、種々の回転体の回転′
速度を検出する場合に広く適用して好適なものである.
また上述の実施例においては、磁界検出信号から、常に
デューテイが50%の2値化信号を発生する場合につい
て述べたが、これに限らず、デューテイは必要に応じて
種々選択し得、常に所望のデューテイを有する2値化信
号を発生するようにしても上述の実施例と同様の効果を
実現できる.さらに上述の実施例においては、回転体の
回転速度を検出する場合について述べたが、本発明はこ
れに限らず、回転数等他の回転情報を検出する場合にも
広く適用して好適なものである。
In the above-described embodiment, the present invention is applied to detecting the rotational speed of the cab stan motor of a video tape recorder, but the present invention is not limited to this, and can be applied to a rotary drum drive motor or a spindle motor of a magnetic disk device. It can also be used to detect the rotational speed of other motors, such as those that detect the rotational speed of other motors.
It is widely applicable and suitable for detecting speed.
Furthermore, in the above embodiment, a case has been described in which a binary signal with a duty of 50% is always generated from the magnetic field detection signal, but the duty is not limited to this, and various duties can be selected as necessary, and the duty is always generated as desired. The same effect as in the above embodiment can be achieved by generating a binary signal having a duty of . Further, in the above-described embodiment, the case where the rotational speed of a rotating body is detected is described, but the present invention is not limited to this, but can be widely applied and suitable for detecting other rotational information such as the number of rotations. It is.

H発明の効果 上述のように本発明によれば、磁界検出信号に含まれる
不平衡電圧を検出し、その検出結果に応じて磁界検出信
号を2値化する基準レベルを変化させるようにしたこと
により、磁界検出信号中の不平′&T!圧の有無に係わ
らず、常に所望のデューテイを有する2値化信号を送出
し得、かくするにつき、静止状熊から定常回転状態まで
、高い検出精度で回転情報を検出し得る回転情報検出回
路を実現できる。
H Effects of the Invention As described above, according to the present invention, the unbalanced voltage included in the magnetic field detection signal is detected, and the reference level for binarizing the magnetic field detection signal is changed according to the detection result. Due to this, the complaint in the magnetic field detection signal '&T! A rotation information detection circuit that can always send a binary signal with a desired duty regardless of the presence or absence of pressure, and can detect rotation information with high detection accuracy from a stationary state to a steady rotation state. realizable.

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

第1図は本発明の一実施例による回転速度検出回路を示
す接続図、第2図及び第3図はその動作の説明に供する
信号波形図、第4図は回転速度検出回路が用いられるキ
ャプスタンサーボ回路を示すブロック図、第5図は従来
の回転速度検出回路を示す接続図、第6図〜第8図はそ
の動作の説明に供する信号波形図である。 1・・・・・・キャプスタンサーボ回路、2・・・・・
・キャプスクンモータ、3、10・・・・・・回転速度
検出回路、4・・・・・・周波数電圧変換回路、5・・
・・・・加算回路、6・・・・・・回転磁石部、7、1
1・・・・・・磁界検出部、8・・・・・・2{1!!
化回路部、12・・・・・・不平衡電圧検出部、14・
・・・・・積分回路、15・・・・・・クランプ回路。
FIG. 1 is a connection diagram showing a rotational speed detection circuit according to an embodiment of the present invention, FIGS. 2 and 3 are signal waveform diagrams for explaining its operation, and FIG. 4 is a capacitor in which the rotational speed detection circuit is used. FIG. 5 is a block diagram showing a stun servo circuit, FIG. 5 is a connection diagram showing a conventional rotational speed detection circuit, and FIGS. 6 to 8 are signal waveform diagrams for explaining its operation. 1... Capstan servo circuit, 2...
・Capsun motor, 3, 10... Rotation speed detection circuit, 4... Frequency voltage conversion circuit, 5...
... Addition circuit, 6 ... Rotating magnet section, 7, 1
1... Magnetic field detection section, 8...2 {1! !
circuit section, 12... unbalanced voltage detection section, 14.
...Integrator circuit, 15...Clamp circuit.

Claims (1)

【特許請求の範囲】 回転体の周囲に、回転方向に順次異なる磁界を発生する
回転磁石部を配置すると共に、上記回転磁石部に当接す
るように磁界検出部を配置し、上記回転体の回転に応じ
て上記磁界検出部から送出される正弦波状の磁界検出信
号を2値化してなる2値化信号に基づいて上記回転体の
回転情報を得る回転情報検出回路において、 上記磁界検出信号を、当該磁界検出信号の中心レベルの
上下に設定した第1及び第2のクランプレベルでクラン
プして磁界検出クランプ信号を送出するクランプ回路と
、 上記磁界検出クランプ信号を積分して当該磁界検出クラ
ンプ信号の平均値を算出し、上記磁界検出信号に含まれ
る不平衡電圧に応じた不平衡検出信号を送出する積分回
路と、 上記磁界検出信号を、第1の基準レベルに上記不平衡検
出信号を加えてなる第2の基準レベルで比較して2値化
信号を送出する2値化回路とを具え、上記磁界検出信号
中の上記不平衡電圧の有無に係わらず、常に所望のデュ
ーティを有する上記2値化信号を得るようにした ことを特徴とする回転情報検出回路。
[Claims] A rotating magnet section that sequentially generates different magnetic fields in the rotational direction is arranged around the rotating body, and a magnetic field detection section is arranged so as to come into contact with the rotating magnet section, and the rotation of the rotating body is In a rotation information detection circuit that obtains rotation information of the rotating body based on a binary signal obtained by binarizing a sinusoidal magnetic field detection signal sent from the magnetic field detection section in response to the above, the magnetic field detection signal is A clamp circuit that outputs a magnetic field detection clamp signal by clamping at first and second clamp levels set above and below the center level of the magnetic field detection signal; an integrating circuit that calculates an average value and sends out an unbalanced detection signal according to the unbalanced voltage included in the magnetic field detection signal; and a binarization circuit that sends out a binarized signal by making a comparison at a second reference level of 1. A rotation information detection circuit characterized in that a rotation signal is obtained.
JP19476789A 1989-07-26 1989-07-26 Rotation information detection circuit Expired - Fee Related JP2805089B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19476789A JP2805089B2 (en) 1989-07-26 1989-07-26 Rotation information detection circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19476789A JP2805089B2 (en) 1989-07-26 1989-07-26 Rotation information detection circuit

Publications (2)

Publication Number Publication Date
JPH0357962A true JPH0357962A (en) 1991-03-13
JP2805089B2 JP2805089B2 (en) 1998-09-30

Family

ID=16329904

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19476789A Expired - Fee Related JP2805089B2 (en) 1989-07-26 1989-07-26 Rotation information detection circuit

Country Status (1)

Country Link
JP (1) JP2805089B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008249452A (en) * 2007-03-30 2008-10-16 Tdk Corp Magnetic detector

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008249452A (en) * 2007-03-30 2008-10-16 Tdk Corp Magnetic detector

Also Published As

Publication number Publication date
JP2805089B2 (en) 1998-09-30

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